Sample records for air-ice co2 fluxes

  1. Air-ice CO2 fluxes and pCO2 dynamics in the Arctic coastal area (Amundsen Gulf, Canada)

    NASA Astrophysics Data System (ADS)

    Geilfus, Nicolas-Xavier; Tison, Jean Louis; Carnat, Gauthier; Else, Brent; Borges, Alberto V.; Thomas, Helmuth; Shadwick, Elizabeth; Delille, Bruno

    2010-05-01

    Sea ice covers about 7% of the Earth surface at its maximum seasonal extent. For decades sea ice was assumed to be an impermeable and inert barrier for air - sea exchange of CO2 so that global climate models do not include CO2 exchange between the oceans and the atmosphere in the polar regions. However, uptake of atmospheric CO2 by sea ice cover was recently reported raising the need to further investigate pCO2 dynamics in the marine cryosphere realm and related air-ice CO2 fluxes. In addition, budget of CO2 fluxes are poorly constrained in high latitudes continental shelves [Borges et al., 2006]. We report measurements of air-ice CO2 fluxes above the Canadian continental shelf and compare them to previous measurements carried out in Antarctica. We carried out measurements of pCO2 within brines and bulk ice, and related air-ice CO2 fluxes (chamber method) in Antarctic first year pack ice ("Sea Ice Mass Balance in Antarctica -SIMBA" drifting station experiment September - October 2007) and in Arctic first year land fast ice ("Circumpolar Flaw Lead" - CFL, April - June 2008). These 2 experiments were carried out in contrasted sites. SIMBA was carried out on sea ice in early spring while CFL was carried out in from the middle of the winter to the late spring while sea ice was melting. Both in Arctic and Antarctic, no air-ice CO2 fluxes were detected when sea ice interface was below -10°C. Slightly above -10°C, fluxes toward the atmosphere were observed. In contrast, at -7°C fluxes from the atmosphere to the ice were significant. The pCO2 of the brine exhibits a same trend in both hemispheres with a strong decrease of the pCO2 anti-correlated with the increase of sea ice temperature. The pCO2 shifted from a large over-saturation at low temperature to a marked under-saturation at high temperature. These air-ice CO2 fluxes are partly controlled by the permeability of the air-ice interface, which depends of the temperature of this one. Moreover, air-ice CO2 fluxes are

  2. Effects of sea-ice and biogeochemical processes and storms on under-ice water fCO2 during the winter-spring transition in the high Arctic Ocean: Implications for sea-air CO2 fluxes

    NASA Astrophysics Data System (ADS)

    Fransson, Agneta; Chierici, Melissa; Skjelvan, Ingunn; Olsen, Are; Assmy, Philipp; Peterson, Algot K.; Spreen, Gunnar; Ward, Brian

    2017-07-01

    We performed measurements of carbon dioxide fugacity (fCO2) in the surface water under Arctic sea ice from January to June 2015 during the Norwegian young sea ICE (N-ICE2015) expedition. Over this period, the ship drifted with four different ice floes and covered the deep Nansen Basin, the slopes north of Svalbard, and the Yermak Plateau. This unique winter-to-spring data set includes the first winter-time under-ice water fCO2 observations in this region. The observed under-ice fCO2 ranged between 315 µatm in winter and 153 µatm in spring, hence was undersaturated relative to the atmospheric fCO2. Although the sea ice partly prevented direct CO2 exchange between ocean and atmosphere, frequently occurring leads and breakup of the ice sheet promoted sea-air CO2 fluxes. The CO2 sink varied between 0.3 and 86 mmol C m-2 d-1, depending strongly on the open-water fractions (OW) and storm events. The maximum sea-air CO2 fluxes occurred during storm events in February and June. In winter, the main drivers of the change in under-ice water fCO2 were dissolution of CaCO3 (ikaite) and vertical mixing. In June, in addition to these processes, primary production and sea-air CO2 fluxes were important. The cumulative loss due to CaCO3 dissolution of 0.7 mol C m-2 in the upper 10 m played a major role in sustaining the undersaturation of fCO2 during the entire study. The relative effects of the total fCO2 change due to CaCO3 dissolution was 38%, primary production 26%, vertical mixing 16%, sea-air CO2 fluxes 16%, and temperature and salinity insignificant.

  3. CO2 flux over young and snow-covered Arctic pack ice in winter and spring

    NASA Astrophysics Data System (ADS)

    Nomura, Daiki; Granskog, Mats A.; Fransson, Agneta; Chierici, Melissa; Silyakova, Anna; Ohshima, Kay I.; Cohen, Lana; Delille, Bruno; Hudson, Stephen R.; Dieckmann, Gerhard S.

    2018-06-01

    Rare CO2 flux measurements from Arctic pack ice show that two types of ice contribute to the release of CO2 from the ice to the atmosphere during winter and spring: young, thin ice with a thin layer of snow and older (several weeks), thicker ice with thick snow cover. Young, thin sea ice is characterized by high salinity and high porosity, and snow-covered thick ice remains relatively warm ( > -7.5 °C) due to the insulating snow cover despite air temperatures as low as -40 °C. Therefore, brine volume fractions of these two ice types are high enough to provide favorable conditions for gas exchange between sea ice and the atmosphere even in mid-winter. Although the potential CO2 flux from sea ice decreased due to the presence of the snow, the snow surface is still a CO2 source to the atmosphere for low snow density and thin snow conditions. We found that young sea ice that is formed in leads without snow cover produces CO2 fluxes an order of magnitude higher than those in snow-covered older ice (+1.0 ± 0.6 mmol C m-2 day-1 for young ice and +0.2 ± 0.2 mmol C m-2 day-1 for older ice).

  4. Climate change impacts on sea-air fluxes of CO2 in three Arctic seas: a sensitivity study using Earth observation

    NASA Astrophysics Data System (ADS)

    Land, P. E.; Shutler, J. D.; Cowling, R. D.; Woolf, D. K.; Walker, P.; Findlay, H. S.; Upstill-Goddard, R. C.; Donlon, C. J.

    2013-12-01

    We applied coincident Earth observation data collected during 2008 and 2009 from multiple sensors (RA2, AATSR and MERIS, mounted on the European Space Agency satellite Envisat) to characterise environmental conditions and integrated sea-air fluxes of CO2 in three Arctic seas (Greenland, Barents, Kara). We assessed net CO2 sink sensitivity due to changes in temperature, salinity and sea ice duration arising from future climate scenarios. During the study period the Greenland and Barents seas were net sinks for atmospheric CO2, with integrated sea-air fluxes of -36 ± 14 and -11 ± 5 Tg C yr-1, respectively, and the Kara Sea was a weak net CO2 source with an integrated sea-air flux of +2.2 ± 1.4 Tg C yr-1. The combined integrated CO2 sea-air flux from all three was -45 ± 18 Tg C yr-1. In a sensitivity analysis we varied temperature, salinity and sea ice duration. Variations in temperature and salinity led to modification of the transfer velocity, solubility and partial pressure of CO2 taking into account the resultant variations in alkalinity and dissolved organic carbon (DOC). Our results showed that warming had a strong positive effect on the annual integrated sea-air flux of CO2 (i.e. reducing the sink), freshening had a strong negative effect and reduced sea ice duration had a small but measurable positive effect. In the climate change scenario examined, the effects of warming in just over a decade of climate change up to 2020 outweighed the combined effects of freshening and reduced sea ice duration. Collectively these effects gave an integrated sea-air flux change of +4.0 Tg C in the Greenland Sea, +6.0 Tg C in the Barents Sea and +1.7 Tg C in the Kara Sea, reducing the Greenland and Barents sinks by 11% and 53%, respectively, and increasing the weak Kara Sea source by 81%. Overall, the regional integrated flux changed by +11.7 Tg C, which is a 26% reduction in the regional sink. In terms of CO2 sink strength, we conclude that the Barents Sea is the most

  5. Climatological mean and decadal change in surface ocean pCO 2, and net sea-air CO 2 flux over the global oceans

    NASA Astrophysics Data System (ADS)

    Takahashi, Taro; Sutherland, Stewart C.; Wanninkhof, Rik; Sweeney, Colm; Feely, Richard A.; Chipman, David W.; Hales, Burke; Friederich, Gernot; Chavez, Francisco; Sabine, Christopher; Watson, Andrew; Bakker, Dorothee C. E.; Schuster, Ute; Metzl, Nicolas; Yoshikawa-Inoue, Hisayuki; Ishii, Masao; Midorikawa, Takashi; Nojiri, Yukihiro; Körtzinger, Arne; Steinhoff, Tobias; Hoppema, Mario; Olafsson, Jon; Arnarson, Thorarinn S.; Tilbrook, Bronte; Johannessen, Truls; Olsen, Are; Bellerby, Richard; Wong, C. S.; Delille, Bruno; Bates, N. R.; de Baar, Hein J. W.

    2009-04-01

    A climatological mean distribution for the surface water pCO 2 over the global oceans in non-El Niño conditions has been constructed with spatial resolution of 4° (latitude) ×5° (longitude) for a reference year 2000 based upon about 3 million measurements of surface water pCO 2 obtained from 1970 to 2007. The database used for this study is about 3 times larger than the 0.94 million used for our earlier paper [Takahashi et al., 2002. Global sea-air CO 2 flux based on climatological surface ocean pCO 2, and seasonal biological and temperature effects. Deep-Sea Res. II, 49, 1601-1622]. A time-trend analysis using deseasonalized surface water pCO 2 data in portions of the North Atlantic, North and South Pacific and Southern Oceans (which cover about 27% of the global ocean areas) indicates that the surface water pCO 2 over these oceanic areas has increased on average at a mean rate of 1.5 μatm y -1 with basin-specific rates varying between 1.2±0.5 and 2.1±0.4 μatm y -1. A global ocean database for a single reference year 2000 is assembled using this mean rate for correcting observations made in different years to the reference year. The observations made during El Niño periods in the equatorial Pacific and those made in coastal zones are excluded from the database. Seasonal changes in the surface water pCO 2 and the sea-air pCO 2 difference over four climatic zones in the Atlantic, Pacific, Indian and Southern Oceans are presented. Over the Southern Ocean seasonal ice zone, the seasonality is complex. Although it cannot be thoroughly documented due to the limited extent of observations, seasonal changes in pCO 2 are approximated by using the data for under-ice waters during austral winter and those for the marginal ice and ice-free zones. The net air-sea CO 2 flux is estimated using the sea-air pCO 2 difference and the air-sea gas transfer rate that is parameterized as a function of (wind speed) 2 with a scaling factor of 0.26. This is estimated by inverting

  6. Effect of Sampling Depth on Air-Sea CO2 Flux Estimates in River-Stratified Arctic Coastal Waters

    NASA Astrophysics Data System (ADS)

    Miller, L. A.; Papakyriakou, T. N.

    2015-12-01

    In summer-time Arctic coastal waters that are strongly influenced by river run-off, extreme stratification severely limits wind mixing, making it difficult to effectively sample the surface 'mixed layer', which can be as shallow as 1 m, from a ship. During two expeditions in southwestern Hudson Bay, off the Nelson, Hayes, and Churchill River estuaries, we confirmed that sampling depth has a strong impact on estimates of 'surface' pCO2 and calculated air-sea CO2 fluxes. We determined pCO2 in samples collected from 5 m, using a typical underway system on the ship's seawater supply; from the 'surface' rosette bottle, which was generally between 1 and 3 m; and using a niskin bottle deployed at 1 m and just below the surface from a small boat away from the ship. Our samples confirmed that the error in pCO2 derived from typical ship-board versus small-boat sampling at a single station could be nearly 90 μatm, leading to errors in the calculated air-sea CO2 flux of more than 0.1 mmol/(m2s). Attempting to extrapolate such fluxes over the 6,000,000 km2 area of the Arctic shelves would generate an error approaching a gigamol CO2/s. Averaging the station data over a cruise still resulted in an error of nearly 50% in the total flux estimate. Our results have implications not only for the design and execution of expedition-based sampling, but also for placement of in-situ sensors. Particularly in polar waters, sensors are usually deployed on moorings, well below the surface, to avoid damage and destruction from drifting ice. However, to obtain accurate information on air-sea fluxes in these areas, it is necessary to deploy sensors on ice-capable buoys that can position the sensors in true 'surface' waters.

  7. Carbon Dioxide Transfer Through Sea Ice: Modelling Flux in Brine Channels

    NASA Astrophysics Data System (ADS)

    Edwards, L.; Mitchelson-Jacob, G.; Hardman-Mountford, N.

    2010-12-01

    For many years sea ice was thought to act as a barrier to the flux of CO2 between the ocean and atmosphere. However, laboratory-based and in-situ observations suggest that while sea ice may in some circumstances reduce or prevent transfer (e.g. in regions of thick, superimposed multi-year ice), it may also be highly permeable (e.g. thin, first year ice) with some studies observing significant fluxes of CO2. Sea ice covered regions have been observed to act both as a sink and a source of atmospheric CO2 with the permeability of sea ice and direction of flux related to sea ice temperature and the presence of brine channels in the ice, as well as seasonal processes such as whether the ice is freezing or thawing. Brine channels concentrate dissolved inorganic carbon (DIC) as well as salinity and as these dense waters descend through both the sea ice and the surface ocean waters, they create a sink for CO2. Calcium carbonate (ikaite) precipitation in the sea ice is thought to enhance this process. Micro-organisms present within the sea ice will also contribute to the CO2 flux dynamics. Recent evidence of decreasing sea ice extent and the associated change from a multi-year ice to first-year ice dominated system suggest the potential for increased CO2 flux through regions of thinner, more porous sea ice. A full understanding of the processes and feedbacks controlling the flux in these regions is needed to determine their possible contribution to global CO2 levels in a future warming climate scenario. Despite the significance of these regions, the air-sea CO2 flux in sea ice covered regions is not currently included in global climate models. Incorporating this carbon flux system into Earth System models requires the development of a well-parameterised sea ice-air flux model. In our work we use the Los Alamos sea ice model, CICE, with a modification to incorporate the movement of CO2 through brine channels including the addition of DIC processes and ice algae production to

  8. Arctic Ocean CO2 uptake: an improved multiyear estimate of the air-sea CO2 flux incorporating chlorophyll a concentrations

    NASA Astrophysics Data System (ADS)

    Yasunaka, Sayaka; Siswanto, Eko; Olsen, Are; Hoppema, Mario; Watanabe, Eiji; Fransson, Agneta; Chierici, Melissa; Murata, Akihiko; Lauvset, Siv K.; Wanninkhof, Rik; Takahashi, Taro; Kosugi, Naohiro; Omar, Abdirahman M.; van Heuven, Steven; Mathis, Jeremy T.

    2018-03-01

    We estimated monthly air-sea CO2 fluxes in the Arctic Ocean and its adjacent seas north of 60° N from 1997 to 2014. This was done by mapping partial pressure of CO2 in the surface water (pCO2w) using a self-organizing map (SOM) technique incorporating chlorophyll a concentration (Chl a), sea surface temperature, sea surface salinity, sea ice concentration, atmospheric CO2 mixing ratio, and geographical position. We applied new algorithms for extracting Chl a from satellite remote sensing reflectance with close examination of uncertainty of the obtained Chl a values. The overall relationship between pCO2w and Chl a was negative, whereas the relationship varied among seasons and regions. The addition of Chl a as a parameter in the SOM process enabled us to improve the estimate of pCO2w, particularly via better representation of its decline in spring, which resulted from biologically mediated pCO2w reduction. As a result of the inclusion of Chl a, the uncertainty in the CO2 flux estimate was reduced, with a net annual Arctic Ocean CO2 uptake of 180 ± 130 Tg C yr-1. Seasonal to interannual variation in the CO2 influx was also calculated.

  9. First estimates of the contribution of CaCO3 precipitation to the release of CO2 to the atmosphere during young sea ice growth

    NASA Astrophysics Data System (ADS)

    Geilfus, N.-X.; Carnat, G.; Dieckmann, G. S.; Halden, N.; Nehrke, G.; Papakyriakou, T.; Tison, J.-L.; Delille, B.

    2013-01-01

    report measurements of pH, total alkalinity, air-ice CO2 fluxes (chamber method), and CaCO3 content of frost flowers (FF) and thin landfast sea ice. As the temperature decreases, concentration of solutes in the brine skim increases. Along this gradual concentration process, some salts reach their solubility threshold and start precipitating. The precipitation of ikaite (CaCO3.6H2O) was confirmed in the FF and throughout the ice by Raman spectroscopy and X-ray analysis. The amount of ikaite precipitated was estimated to be 25 µmol kg-1 melted FF, in the FF and is shown to decrease from 19 to 15 µmol kg-1 melted ice in the upper part and at the bottom of the ice, respectively. CO2 release due to precipitation of CaCO3 is estimated to be 50 µmol kg-1 melted samples. The dissolved inorganic carbon (DIC) normalized to a salinity of 10 exhibits significant depletion in the upper layer of the ice and in the FF. This DIC loss is estimated to be 2069 µmol kg-1 melted sample and corresponds to a CO2 release from the ice to the atmosphere ranging from 20 to 40 mmol m-2 d-1. This estimate is consistent with flux measurements of air-ice CO2 exchange. Our measurements confirm previous laboratory findings that growing young sea ice acts as a source of CO2 to the atmosphere. CaCO3 precipitation during early ice growth appears to promote the release of CO2 to the atmosphere; however, its contribution to the overall release by newly formed ice is most likely minor.

  10. Spatio-temporal visualization of air-sea CO2 flux and carbon budget using volume rendering

    NASA Astrophysics Data System (ADS)

    Du, Zhenhong; Fang, Lei; Bai, Yan; Zhang, Feng; Liu, Renyi

    2015-04-01

    This paper presents a novel visualization method to show the spatio-temporal dynamics of carbon sinks and sources, and carbon fluxes in the ocean carbon cycle. The air-sea carbon budget and its process of accumulation are demonstrated in the spatial dimension, while the distribution pattern and variation of CO2 flux are expressed by color changes. In this way, we unite spatial and temporal characteristics of satellite data through visualization. A GPU-based direct volume rendering technique using half-angle slicing is adopted to dynamically visualize the released or absorbed CO2 gas with shadow effects. A data model is designed to generate four-dimensional (4D) data from satellite-derived air-sea CO2 flux products, and an out-of-core scheduling strategy is also proposed for on-the-fly rendering of time series of satellite data. The presented 4D visualization method is implemented on graphics cards with vertex, geometry and fragment shaders. It provides a visually realistic simulation and user interaction for real-time rendering. This approach has been integrated into the Information System of Ocean Satellite Monitoring for Air-sea CO2 Flux (IssCO2) for the research and assessment of air-sea CO2 flux in the China Seas.

  11. Seasonal variation of air-sea CO2 fluxes in the Terra Nova Bay of the Ross Sea, Antarctica, based on year-round pCO2 observations

    NASA Astrophysics Data System (ADS)

    Zappa, C. J.; Rhee, T. S.; Kwon, Y. S.; Choi, T.; Yang, E. J.; Kim, J.

    2017-12-01

    The polar oceans are rapidly changing in response to climate variability. In particular, augmented inflow of glacial melt water and shrinking sea-ice extent impacts the polar coastal oceans, which may in turn shift the biogeochemistry into an unprecedented paradigm not experienced previously. Nonetheless, most research in the polar oceans is limited to the summer season. Here, we present the first direct observations of ocean and atmospheric pCO2 measured near the coast of Terra Nova Bay in the Ross Sea, Antarctica, ongoing since February, 2015 at Jang Bogo Station. The coastal area is covered by landfast sea-ice from spring to fall while continually exposed to the atmosphere during summer season only. The pCO2 in seawater swung from 120 matm in February to 425 matm in early October. Although sea-ice still covers the coastal area, pCO2 already started decreasing after reaching the peak in October. In November, the pCO2 suddenly dropped as much as 100 matm in a week. This decrease of pCO2 continued until late February when the sea-ice concentration was minimal. With growing sea ice, the pCO2 increased logarithmically reaching the atmospheric concentration in June/July, depending on the year, and continued to increase until October. Daily mean air-sea CO2 flux in the coastal area widely varied from -70 mmol m-2 d-1 to 20 mmol m-2 d-1. Based on these observations of pCO2 in Terra Nova Bay, the annual uptake of CO2 is 8 g C m-2, estimated using the fraction of sea-ice concentration estimated from AMSR2 microwave emission imagery. Extrapolating to all polynyas surrounding Antarctica, we expect the annual uptake of 8 Tg C in the atmosphere. This is comparable to the amount of CO2 degassed into the atmosphere south of the Antarctic Polar Front (62°S).

  12. Air-water CO2 Fluxes In Seasonal Hypoxia-influenced Green Bay, Lake Michigan

    NASA Astrophysics Data System (ADS)

    Lin, P.; Klump, J. V.; Guo, L.

    2016-02-01

    Increasing anthropogenic nutrient enrichment has led to seasonal hypoxia in Green Bay, the largest freshwater estuary in the Laurentian Great Lakes, but change in carbon dynamics associated with the development of hypoxia remains poorly understood. Variations in alkalinity, abundance of carbon species, and air-water CO2 fluxes were quantified under contrasting hypoxic conditions during summer 2014. Green Bay was characterized with high pH (average 8.62 ± 0.16 in August), high DIC concentrations (2113 - 3213 µmol/kg) and high pCO2 in the water column. pCO2 was mostly >700 µatm in June, resulting in a net CO2 source to the air, while pCO2 was mostly <650 µatm in August when hypoxic conditions occurred in Green Bay. In central Green Bay, pCO2 was the highest during both sampling months, accompanying by low dissolved oxygen (DO) and lower pH in the water column. In August, pCO2 was inversely correlated with DOC concentration and increased with DOC/DOP ratio, suggesting a control by organic matter on air-water CO2 dynamics and consumption of DO in Green Bay. Positive CO2 fluxes to the atmosphere during August were only observed in northern bay but a CO2 sink was found in southern Green Bay ( 40% of study area) with high biological production and terrestrial DOM. Daily CO2 flux ranged from 10.9 to 48.5 mmol-C m-2 d-1 in June with an average of 18.29 ± 7.44 mmol-C m-2 d-1, whereas it varied from 1.82 ± 1.18 mmol m-2 d-1 in the north to -2.05 ± 1.89 mmol m-2 d-1 in the south of Green Bay in August. Even though strong biological production reduced the CO2 emission, daily CO2 fluxes from Green Bay to the air were as high as 7.4 × 107 mole-C in June and 4.6 × 106 mole-C in August, suggesting a significant role of high-DIC lakes in global CO2 budget and cycling.

  13. Surface Water pCO2 Variations and Sea-Air CO2 Fluxes During Summer in the Eastern Canadian Arctic

    NASA Astrophysics Data System (ADS)

    Burgers, T. M.; Miller, L. A.; Thomas, H.; Else, B. G. T.; Gosselin, M.; Papakyriakou, T.

    2017-12-01

    Based on a 2 year data set, the eastern Canadian Arctic Archipelago and Baffin Bay appear to be a modest summertime sink of atmospheric CO2. We measured surface water CO2 partial pressure (pCO2), salinity, and temperature throughout northern Baffin Bay, Nares Strait, and Lancaster Sound from the CCGS Amundsen during its 2013 and 2014 summer cruises. Surface water pCO2 displayed considerable variability (144-364 μatm) but never exceeded atmospheric concentrations, and average calculated CO2 fluxes in 2013 and 2014 were -12 and -3 mmol C m-2 d-1 (into the ocean), respectively. Ancillary measurements of chlorophyll a reveal low summertime productivity in surface waters. Based on total alkalinity and stable oxygen isotopes (δ18O) data, a strong riverine signal in northern Nares Strait coincided with relatively high surface pCO2, whereas areas of sea-ice melt occur with low surface pCO2. Further assessments, extending the seasonal observation period, are needed to properly constrain both seasonal and annual CO2 fluxes in this region.

  14. Mapping of the air-sea CO2 flux in the Arctic Ocean and its adjacent seas: Basin-wide distribution and seasonal to interannual variability

    NASA Astrophysics Data System (ADS)

    Yasunaka, Sayaka; Murata, Akihiko; Watanabe, Eiji; Chierici, Melissa; Fransson, Agneta; van Heuven, Steven; Hoppema, Mario; Ishii, Masao; Johannessen, Truls; Kosugi, Naohiro; Lauvset, Siv K.; Mathis, Jeremy T.; Nishino, Shigeto; Omar, Abdirahman M.; Olsen, Are; Sasano, Daisuke; Takahashi, Taro; Wanninkhof, Rik

    2016-09-01

    We produced 204 monthly maps of the air-sea CO2 flux in the Arctic north of 60°N, including the Arctic Ocean and its adjacent seas, from January 1997 to December 2013 by using a self-organizing map technique. The partial pressure of CO2 (pCO2) in surface water data were obtained by shipboard underway measurements or calculated from alkalinity and total inorganic carbon of surface water samples. Subsequently, we investigated the basin-wide distribution and seasonal to interannual variability of the CO2 fluxes. The 17-year annual mean CO2 flux shows that all areas of the Arctic Ocean and its adjacent seas were net CO2 sinks. The estimated annual CO2 uptake by the Arctic Ocean was 180 TgC yr-1. The CO2 influx was strongest in winter in the Greenland/Norwegian Seas (>15 mmol m-2 day-1) and the Barents Sea (>12 mmol m-2 day-1) because of strong winds, and strongest in summer in the Chukchi Sea (∼10 mmol m-2 day-1) because of the sea-ice retreat. In recent years, the CO2 uptake has increased in the Greenland/Norwegian Sea and decreased in the southern Barents Sea, owing to increased and decreased air-sea pCO2 differences, respectively.

  15. Comparison of Sea-Air CO2 Flux Estimates Using Satellite-Based Versus Mooring Wind Speed Data

    NASA Astrophysics Data System (ADS)

    Sutton, A. J.; Sabine, C. L.; Feely, R. A.; Wanninkhof, R. H.

    2016-12-01

    The global ocean is a major sink of anthropogenic CO2, absorbing approximately 27% of CO2 emissions since the beginning of the industrial revolution. Any variation or change in the ocean CO2 sink has implications for future climate. Observations of sea-air CO2 flux have relied primarily on ship-based underway measurements of partial pressure of CO2 (pCO2) combined with satellite, model, or multi-platform wind products. Direct measurements of ΔpCO2 (seawater - air pCO2) and wind speed from moored platforms now allow for high-resolution CO2 flux time series. Here we present a comparison of CO2 flux calculated from moored ΔpCO2 measured on four moorings in different biomes of the Pacific Ocean in combination with: 1) Cross-Calibrated Multi-Platform (CCMP) winds or 2) wind speed measurements made on ocean reference moorings excluded from the CCMP dataset. Preliminary results show using CCMP winds overestimates CO2 flux on average by 5% at the Kuroshio Extension Observatory, Ocean Station Papa, WHOI Hawaii Ocean Timeseries Station, and Stratus. In general, CO2 flux seasonality follows patterns of seawater pCO2 and SST with periods of CO2 outgassing during summer and CO2 uptake during winter at these locations. Any offsets or seasonal biases in CCMP winds could impact global ocean sink estimates using this data product. Here we present patterns and trends between the two CO2 flux estimates and discuss the potential implications for tracking variability and change in global ocean CO2 uptake.

  16. The Effect of Breaking Waves on CO_2 Air-Sea Fluxes in the Coastal Zone

    NASA Astrophysics Data System (ADS)

    Gutiérrez-Loza, Lucía; Ocampo-Torres, Francisco J.; García-Nava, Héctor

    2018-03-01

    The influence of wave-associated parameters controlling turbulent CO_2 fluxes through the air-sea interface is investigated in a coastal region. A full year of high-quality data of direct estimates of air-sea CO_2 fluxes based on eddy-covariance measurements is presented. The study area located in Todos Santos Bay, Baja California, Mexico, is a net sink of CO_2 with a mean flux of -1.3 μmol m^{-2}s^{-1} (-41.6 mol m^{-2}yr^{-1} ). The results of a quantile-regression analysis computed between the CO_2 flux and, (1) wind speed, (2) significant wave height, (3) wave steepness, and (4) water temperature, suggest that the significant wave height is the most correlated parameter with the magnitude of the flux but the behaviour of the relation varies along the probability distribution function, with the slopes of the regression lines presenting both positive and negative values. These results imply that the presence of surface waves in coastal areas is the key factor that promotes the increase of the flux from and into the ocean. Further analysis suggests that the local characteristics of the aqueous and atmospheric layers might determine the direction of the flux.

  17. Air-water gas exchange and CO2 flux in a mangrove-dominated estuary

    USGS Publications Warehouse

    Ho, David T.; Ferrón, Sara; Engel, Victor C.; Larsen, Laurel G.; Barr, Jordan G.

    2014-01-01

    Mangrove forests are highly productive ecosystems, but the fate of mangrove-derived carbon remains uncertain. Part of that uncertainty stems from the fact that gas transfer velocities in mangrove-surrounded waters are not well determined, leading to uncertainty in air-water CO2 fluxes. Two SF6 tracer release experiments were conducted to determine gas transfer velocities (k(600) = 8.3 ± 0.4 and 8.1 ± 0.6 cm h−1), along with simultaneous measurements of pCO2 to determine the air-water CO2 fluxes from Shark River, Florida (232.11 ± 23.69 and 171.13 ± 20.28 mmol C m−2 d−1), an estuary within the largest contiguous mangrove forest in North America. The gas transfer velocity results are consistent with turbulent kinetic energy dissipation measurements, indicating a higher rate of turbulence and gas exchange than predicted by commonly used wind speed/gas exchange parameterizations. The results have important implications for carbon fluxes in mangrove ecosystems.

  18. A flux-gradient system for simultaneous measurement of the CH4, CO2, and H2O fluxes at a lake-air interface.

    PubMed

    Xiao, Wei; Liu, Shoudong; Li, Hanchao; Xiao, Qitao; Wang, Wei; Hu, Zhenghua; Hu, Cheng; Gao, Yunqiu; Shen, Jing; Zhao, Xiaoyan; Zhang, Mi; Lee, Xuhui

    2014-12-16

    Inland lakes play important roles in water and greenhouse gas cycling in the environment. This study aims to test the performance of a flux-gradient system for simultaneous measurement of the fluxes of water vapor, CO2, and CH4 at a lake-air interface. The concentration gradients over the water surface were measured with an analyzer based on the wavelength-scanned cavity ring-down spectroscopy technology, and the eddy diffusivity was measured with a sonic anemometer. Results of a zero-gradient test indicate a flux measurement precision of 4.8 W m(-2) for water vapor, 0.010 mg m(-2) s(-1) for CO2, and 0.029 μg m(-2) s(-1) for CH4. During the 620 day measurement period, 97%, 69%, and 67% of H2O, CO2, and CH4 hourly fluxes were higher in magnitude than the measurement precision, which confirms that the flux-gradient system had adequate precision for the measurement of the lake-air exchanges. This study illustrates four strengths of the flux-gradient method: (1) the ability to simultaneously measure the flux of H2O, CO2, and CH4; (2) negligibly small density corrections; (3) the ability to resolve small CH4 gradient and flux; and (4) continuous and noninvasive operation. The annual mean CH4 flux (1.8 g CH4 m(-2) year(-1)) at this hypereutrophic lake was close to the median value for inland lakes in the world (1.6 g CH4 m(-2) year(-1)). The system has adequate precision for CH4 flux for broad applications but requires further improvement to resolve small CO2 flux in many lakes.

  19. Seasonal and spatial variations in surface pCO2 and air-sea CO2 flux in the Chesapeake Bay

    NASA Astrophysics Data System (ADS)

    Cai, W. J.; Chen, B.

    2017-12-01

    Bay-wide observations of surface water partial pressure of carbon dioxide (pCO2) were conducted in May, June, August, and October 2016 to study the spatial and seasonal variations in surface pCO2 and to estimate air-sea CO2 flux in the Chesapeake Bay. Overall, high surface pCO2 in the upper-bay decreased downstream rapidly below the atmospheric value near the bay bridge in the mid-bay and then increased slightly to the lower-bay where pCO2 approached the atmospheric level. Over the course of a year, pCO2 was higher than 1000 µatm in the upper bay and the highest pCO2 (2500 µatm) was observed in August. Significant biologically-induced pCO2 undersaturation was observed at the upper part of the mid-bay in August with pCO2 as low as 50 µatm and oversaturated DO% of 200%. In addition to biological control, vertical mixing and upwelling controlled by wind direction and tidal stage played an important role in controlling surface pCO2 in the mid-bay as is evidenced by co-occurrence of high pCO2 with low temperature and low oxygen or high salinity from the subsurface. These physical processes occurred regularly and in short time scale of hours, suggesting they must be considered in the assessment of annual air-sea CO2 flux. Seasonally, the upper-bay acted as a source for atmospheric CO2 over the course of a year. The boundary of upper and mid bay transited from a CO2 source to a sink from May to August and was a source again in October due to strong biological production in summer. In contrast, the mid-bay represented as a CO2 source with large temporal variation due to dynamic hydrographic settings. The lower-bay transited from a weak sink in May to equilibrated with the atmosphere from June to August, while became a source again in October. Moreover, the CO2 flux could be reversed very quickly under episodic severe weather events. Thus further research, including the influence of severe weather and subsequent bloom, is needed to get better understanding of the carbon

  20. Deriving a sea surface climatology of CO2 fugacity in support of air-sea gas flux studies

    NASA Astrophysics Data System (ADS)

    Goddijn-Murphy, L. M.; Woolf, D. K.; Land, P. E.; Shutler, J. D.; Donlon, C.

    2014-07-01

    Climatologies, or long-term averages, of essential climate variables are useful for evaluating models and providing a baseline for studying anomalies. The Surface Ocean Carbon Dioxide (CO2) Atlas (SOCAT) has made millions of global underway sea surface measurements of CO2 publicly available, all in a uniform format and presented as fugacity, fCO2. fCO2 is highly sensitive to temperature and the measurements are only valid for the instantaneous sea surface temperature (SST) that is measured concurrent with the in-water CO2 measurement. To create a climatology of fCO2 data suitable for calculating air-sea CO2 fluxes it is therefore desirable to calculate fCO2 valid for climate quality SST. This paper presents a method for creating such a climatology. We recomputed SOCAT's fCO2 values for their respective measurement month and year using climate quality SST data from satellite Earth observation and then extrapolated the resulting fCO2 values to reference year 2010. The data were then spatially interpolated onto a 1° × 1° grid of the global oceans to produce 12 monthly fCO2 distributions for 2010. The partial pressure of CO2 (pCO2) is also provided for those who prefer to use pCO2. The CO2 concentration difference between ocean and atmosphere is the thermodynamic driving force of the air-sea CO2 flux, and hence the presented fCO2 distributions can be used in air-sea gas flux calculations together with climatologies of other climate variables.

  1. Synoptic evaluation of carbon cycling in Beaufort Sea during summer: contrasting river inputs, ecosystem metabolism and air-sea CO2 fluxes

    NASA Astrophysics Data System (ADS)

    Forest, A.; Coupel, P.; Else, B.; Nahavandian, S.; Lansard, B.; Raimbault, P.; Papakyriakou, T.; Gratton, Y.; Fortier, L.; Tremblay, J.-É.; Babin, M.

    2013-10-01

    The accelerated decline in Arctic sea ice combined with an ongoing trend toward a more dynamic atmosphere is modifying carbon cycling in the Arctic Ocean. A critical issue is to understand how net community production (NCP; the balance between gross primary production and community respiration) responds to changes and modulates air-sea CO2 fluxes. Using data collected as part of the ArcticNet-Malina 2009 expedition in southeastern Beaufort Sea (Arctic Ocean), we synthesize information on sea ice, wind, river, water column properties, metabolism of the planktonic food web, organic carbon fluxes and pools, as well as air-sea CO2 exchange, with the aim of identifying indices of ecosystem response to environmental changes. Data were analyzed to develop a non-steady-state carbon budget and an assessment of NCP against air-sea CO2 fluxes. The mean atmospheric forcing was a mild upwelling-favorable wind (~5 km h-1) blowing from the N-E and a decaying ice cover (<80% concentration) was observed beyond the shelf, the latter being fully exposed to the atmosphere. We detected some areas where the surface mixed layer was net autotrophic owing to high rates of primary production (PP), but the ecosystem was overall net heterotrophic. The region acted nonetheless as a sink for atmospheric CO2 with a mean uptake rate of -2.0 ± 3.3 mmol C m-2d-1. We attribute this discrepancy to: (1) elevated PP rates (>600 mg C m-2d-1) over the shelf prior to our survey, (2) freshwater dilution by river runoff and ice melt, and (3) the presence of cold surface waters offshore. Only the Mackenzie River delta and localized shelf areas directly affected by upwelling were identified as substantial sources of CO2 to the atmosphere (>10mmol C m-2d-1). Although generally <100 mg C m-2d-1, daily PP rates cumulated to a total PP of ~437.6 × 103 t C, which was roughly twice higher than the organic carbon delivery by river inputs (~241.2 × 103 t C). Subsurface PP represented 37.4% of total PP for the

  2. Surface Ocean pCO2 Seasonality and Sea-Air CO2 Flux Estimates for the North American East Coast

    NASA Technical Reports Server (NTRS)

    Signorini, Sergio; Mannino, Antonio; Najjar, Raymond G., Jr.; Friedrichs, Marjorie A. M.; Cai, Wei-Jun; Salisbury, Joe; Wang, Zhaohui Aleck; Thomas, Helmuth; Shadwick, Elizabeth

    2013-01-01

    Underway and in situ observations of surface ocean pCO2, combined with satellite data, were used to develop pCO2 regional algorithms to analyze the seasonal and interannual variability of surface ocean pCO2 and sea-air CO2 flux for five physically and biologically distinct regions of the eastern North American continental shelf: the South Atlantic Bight (SAB), the Mid-Atlantic Bight (MAB), the Gulf of Maine (GoM), Nantucket Shoals and Georges Bank (NS+GB), and the Scotian Shelf (SS). Temperature and dissolved inorganic carbon variability are the most influential factors driving the seasonality of pCO2. Estimates of the sea-air CO2 flux were derived from the available pCO2 data, as well as from the pCO2 reconstructed by the algorithm. Two different gas exchange parameterizations were used. The SS, GB+NS, MAB, and SAB regions are net sinks of atmospheric CO2 while the GoM is a weak source. The estimates vary depending on the use of surface ocean pCO2 from the data or algorithm, as well as with the use of the two different gas exchange parameterizations. Most of the regional estimates are in general agreement with previous studies when the range of uncertainty and interannual variability are taken into account. According to the algorithm, the average annual uptake of atmospheric CO2 by eastern North American continental shelf waters is found to be between 3.4 and 5.4 Tg C/yr (areal average of 0.7 to 1.0 mol CO2 /sq m/yr) over the period 2003-2010.

  3. Synoptic evaluation of carbon cycling in the Beaufort Sea during summer: contrasting river inputs, ecosystem metabolism and air-sea CO2 fluxes

    NASA Astrophysics Data System (ADS)

    Forest, A.; Coupel, P.; Else, B.; Nahavandian, S.; Lansard, B.; Raimbault, P.; Papakyriakou, T.; Gratton, Y.; Fortier, L.; Tremblay, J.-É.; Babin, M.

    2014-05-01

    The accelerated decline in Arctic sea ice and an ongoing trend toward more energetic atmospheric and oceanic forcings are modifying carbon cycling in the Arctic Ocean. A critical issue is to understand how net community production (NCP; the balance between gross primary production and community respiration) responds to changes and modulates air-sea CO2 fluxes. Using data collected as part of the ArcticNet-Malina 2009 expedition in the southeastern Beaufort Sea (Arctic Ocean), we synthesize information on sea ice, wind, river, water column properties, metabolism of the planktonic food web, organic carbon fluxes and pools, as well as air-sea CO2 exchange, with the aim of documenting the ecosystem response to environmental changes. Data were analyzed to develop a non-steady-state carbon budget and an assessment of NCP against air-sea CO2 fluxes. During the field campaign, the mean wind field was a mild upwelling-favorable wind (~ 5 km h-1) from the NE. A decaying ice cover (< 80% concentration) was observed beyond the shelf, the latter being fully exposed to the atmosphere. We detected some areas where the surface mixed layer was net autotrophic owing to high rates of primary production (PP), but the ecosystem was overall net heterotrophic. The region acted nonetheless as a sink for atmospheric CO2, with an uptake rate of -2.0 ± 3.3 mmol C m-2 d-1 (mean ± standard deviation associated with spatial variability). We attribute this discrepancy to (1) elevated PP rates (> 600 mg C m-2 d-1) over the shelf prior to our survey, (2) freshwater dilution by river runoff and ice melt, and (3) the presence of cold surface waters offshore. Only the Mackenzie River delta and localized shelf areas directly affected by upwelling were identified as substantial sources of CO2 to the atmosphere (> 10 mmol C m-2 d-1). Daily PP rates were generally < 100 mg C m-2 d-1 and cumulated to a total PP of ~ 437.6 × 103 t C for the region over a 35-day period. This amount was about twice the

  4. The OceanFlux Greenhouse Gases methodology for deriving a sea surface climatology of CO2 fugacity in support of air-sea gas flux studies

    NASA Astrophysics Data System (ADS)

    Goddijn-Murphy, L. M.; Woolf, D. K.; Land, P. E.; Shutler, J. D.; Donlon, C.

    2015-07-01

    Climatologies, or long-term averages, of essential climate variables are useful for evaluating models and providing a baseline for studying anomalies. The Surface Ocean CO2 Atlas (SOCAT) has made millions of global underway sea surface measurements of CO2 publicly available, all in a uniform format and presented as fugacity, fCO2. As fCO2 is highly sensitive to temperature, the measurements are only valid for the instantaneous sea surface temperature (SST) that is measured concurrently with the in-water CO2 measurement. To create a climatology of fCO2 data suitable for calculating air-sea CO2 fluxes, it is therefore desirable to calculate fCO2 valid for a more consistent and averaged SST. This paper presents the OceanFlux Greenhouse Gases methodology for creating such a climatology. We recomputed SOCAT's fCO2 values for their respective measurement month and year using monthly composite SST data on a 1° × 1° grid from satellite Earth observation and then extrapolated the resulting fCO2 values to reference year 2010. The data were then spatially interpolated onto a 1° × 1° grid of the global oceans to produce 12 monthly fCO2 distributions for 2010, including the prediction errors of fCO2 produced by the spatial interpolation technique. The partial pressure of CO2 (pCO2) is also provided for those who prefer to use pCO2. The CO2 concentration difference between ocean and atmosphere is the thermodynamic driving force of the air-sea CO2 flux, and hence the presented fCO2 distributions can be used in air-sea gas flux calculations together with climatologies of other climate variables.

  5. Is CO2 ice permanent?

    NASA Technical Reports Server (NTRS)

    Lindner, Bernhard Lee

    1992-01-01

    Carbon dioxide ice has been inferred to exist at the south pole in summertime, but Earth based measurements in 1969 of water vapor in the Martian atmosphere suggest that all CO2 ice sublined from the southern polar cap and exposed underlying water ice. This implies that the observed summertime CO2 ice is of recent origin. It appears possible to construct an energy balance model that maintains seasonal CO2 ice at the south pole year round and still reasonably simulates the polar cap regression and atmospheric pressure data. This implies that the CO2 ice observed in the summertime south polar cap could be seasonal in origin, and that minor changes in climate could cause CO2 ice to completely vanish, as would appear to have happened in 1969. However, further research remains before it is certain whether the CO2 ice observed in the summertime south polar cap is seasonal or is part of a permanent reservoir.

  6. Air-sea CO2 flux pattern along the southern Bay of Bengal waters

    NASA Astrophysics Data System (ADS)

    Shanthi, R.; Poornima, D.; Naveen, M.; Thangaradjou, T.; Choudhury, S. B.; Rao, K. H.; Dadhwal, V. K.

    2016-12-01

    Physico-chemical observations made from January 2013 to March 2015 in coastal waters of the southwest Bay of Bengal show pronounced seasonal variation in physico-chemical parameters including total alkalinity (TA: 1927.390-4088.642 μmol kg-1), chlorophyll (0.13-19.41 μg l-1) and also calculated dissolved inorganic carbon (DIC: 1574.219-3790.954 μmol kg-1), partial pressure of carbon dioxide (pCO2: 155.520-1488.607 μatm) and air-sea CO2 flux (FCO2: -4.808 to 11.255 mmol Cm-2 d-1). Most of the physical parameters are at their maximum during summer due to the increased solar radiation at cloud free conditions, less or no riverine inputs, and lack of vertical mixing of water column which leads to the lowest nutrients concentration, dissolved oxygen (DO), biological production, pCO2 and negative flux of CO2 to the atmosphere. Chlorophyll and DO concentrations enhanced due to increased nutrients during premonsoon and monsoon season due to the vertical mixing of water column driven by the strong winds and external inputs at respective seasons. The constant positive loading of nutrients, TA, DIC, chlorophyll, pCO2 and FCO2 against atmospheric temperature (AT), lux, sea surface temperature (SST), pH and salinity observed in principal component analysis (PCA) suggested that physical and biological parameters play vital role in the seasonal distribution of pCO2 along the southwest Bay of Bengal. The annual variability of CO2 flux clearly depicted that the southwest Bay of Bengal switch from sink (2013) to source status in the recent years (2014 and 2015) and it act as significant source of CO2 to the atmosphere with a mean flux of 0.204 ± 1.449 mmol Cm-2 d-1.

  7. The impact of changing wind speeds on gas transfer and its effect on global air-sea CO2 fluxes

    NASA Astrophysics Data System (ADS)

    Wanninkhof, R.; Triñanes, J.

    2017-06-01

    An increase in global wind speeds over time is affecting the global uptake of CO2 by the ocean. We determine the impact of changing winds on gas transfer and CO2 uptake by using the recently updated, global high-resolution, cross-calibrated multiplatform wind product (CCMP-V2) and a fixed monthly pCO2 climatology. In particular, we assess global changes in the context of regional wind speed changes that are attributed to large-scale climate reorganizations. The impact of wind on global CO2 gas fluxes as determined by the bulk formula is dependent on several factors, including the functionality of the gas exchange-wind speed relationship and the regional and seasonal differences in the air-water partial pressure of CO2 gradient (ΔpCO2). The latter also controls the direction of the flux. Fluxes out of the ocean are influenced more by changes in the low-to-intermediate wind speed range, while ingassing is impacted more by changes in higher winds because of the regional correlations between wind and ΔpCO2. Gas exchange-wind speed parameterizations with a quadratic and third-order polynomial dependency on wind, each of which meets global constraints, are compared. The changes in air-sea CO2 fluxes resulting from wind speed trends are greatest in the equatorial Pacific and cause a 0.03-0.04 Pg C decade-1 increase in outgassing over the 27 year time span. This leads to a small overall decrease of 0.00 to 0.02 Pg C decade-1 in global net CO2 uptake, contrary to expectations that increasing winds increase net CO2 uptake.Plain Language SummaryThe effects of changing winds are isolated from the total change in trends in global <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> over the last 27 years. The overall effect of increasing winds over time has a smaller impact than expected as the impact in regions of outgassing is greater than for the regions acting as a <span class="hlt">CO</span><span class="hlt">2</span> sink.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AMT.....9.3687J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AMT.....9.3687J"><span>A new set-up for simultaneous high-precision measurements of <span class="hlt">CO</span><span class="hlt">2</span>, δ13C-<span class="hlt">CO</span><span class="hlt">2</span> and δ18O-<span class="hlt">CO</span><span class="hlt">2</span> on small <span class="hlt">ice</span> core samples</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jenk, Theo Manuel; Rubino, Mauro; Etheridge, David; Ciobanu, Viorela Gabriela; Blunier, Thomas</p> <p>2016-08-01</p> <p>Palaeoatmospheric records of carbon dioxide and its stable carbon isotope composition (δ13C) obtained from polar <span class="hlt">ice</span> cores provide important constraints on the natural variability of the carbon cycle. However, the measurements are both analytically challenging and time-consuming; thus only data exist from a limited number of sampling sites and time periods. Additional analytical resources with high analytical precision and throughput are thus desirable to extend the existing datasets. Moreover, consistent measurements derived by independent laboratories and a variety of analytical systems help to further increase confidence in the global <span class="hlt">CO</span><span class="hlt">2</span> palaeo-reconstructions. Here, we describe our new set-up for simultaneous measurements of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> mixing ratios and atmospheric δ13C and δ18O-<span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> extracted from <span class="hlt">ice</span> core samples. The centrepiece of the system is a newly designed needle cracker for the mechanical release of <span class="hlt">air</span> entrapped in <span class="hlt">ice</span> core samples of 8-13 g operated at -45 °C. The small sample size allows for high resolution and replicate sampling schemes. In our method, <span class="hlt">CO</span><span class="hlt">2</span> is cryogenically and chromatographically separated from the bulk <span class="hlt">air</span> and its isotopic composition subsequently determined by continuous flow isotope ratio mass spectrometry (IRMS). In combination with thermal conductivity measurement of the bulk <span class="hlt">air</span>, the <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio is calculated. The analytical precision determined from standard <span class="hlt">air</span> sample measurements over <span class="hlt">ice</span> is ±1.9 ppm for <span class="hlt">CO</span><span class="hlt">2</span> and ±0.09 ‰ for δ13C. In a laboratory intercomparison study with CSIRO (Aspendale, Australia), good agreement between <span class="hlt">CO</span><span class="hlt">2</span> and δ13C results is found for Law Dome <span class="hlt">ice</span> core samples. Replicate analysis of these samples resulted in a pooled standard deviation of <span class="hlt">2</span>.0 ppm for <span class="hlt">CO</span><span class="hlt">2</span> and 0.11 ‰ for δ13C. These numbers are good, though they are rather conservative estimates of the overall analytical precision achieved for single <span class="hlt">ice</span> sample measurements. Facilitated by the small sample requirement</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016CSR...119...68I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016CSR...119...68I"><span>Net sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and modelled p<span class="hlt">CO</span><span class="hlt">2</span> in the southwestern subtropical Atlantic continental shelf during spring 2010 and summer 2011</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ito, Rosane Gonçalves; Garcia, Carlos Alberto Eiras; Tavano, Virginia Maria</p> <p>2016-05-01</p> <p>Sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> over continental shelves vary substantially in time on both seasonal and sub-seasonal scales, driven primarily by variations in surface p<span class="hlt">CO</span><span class="hlt">2</span> due to several oceanic mechanisms. Furthermore, coastal zones have not been appropriately considered in global estimates of sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, despite their importance to ecology and to productivity. In this work, we aimed to improve our understanding of the role played by shelf waters in controlling sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by investigating the southwestern Atlantic Ocean (21-35°S) region, where physical, chemical and biological measurements were made on board the Brazilian R. V. Cruzeiro do Sul during late spring 2010 and early summer 2011. Features such as discharge from the La Plata River, intrusions of tropical waters on the outer shelf due to meandering and flow instabilities of the Brazil Current, and coastal upwelling in the Santa Marta Grande Cape and São Tomé Cape were detected by both in situ measurements and ocean colour and thermal satellite imagery. Overall, shelf waters in the study area were a source of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere, with an average of 1.<span class="hlt">2</span> mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> day-1 for the late spring and 11.<span class="hlt">2</span> mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> day-1 for the early summer cruises. The spatial variability in ocean p<span class="hlt">CO</span><span class="hlt">2</span> was associated with surface ocean properties (temperature, salinity and chlorophyll-a concentration) in both the slope and shelf waters. Empirical algorithms for predicting temperature-normalized surface ocean p<span class="hlt">CO</span><span class="hlt">2</span> as a function of surface ocean properties were shown to perform well in both shelf and slope waters, except (a) within cyclonic eddies produced by baroclinic instability of the Brazil Current as detected by satellite SST imagery and (b) in coastal upwelling regions. In these regions, surface ocean p<span class="hlt">CO</span><span class="hlt">2</span> values were higher as a result of upwelled <span class="hlt">CO</span><span class="hlt">2</span>-enriched subsurface waters. Finally, a p<span class="hlt">CO</span><span class="hlt">2</span> algorithm based on both sea surface temperature and surface chlorophyll-a was developed that enabled the spatial</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCD.....6.5037R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCD.....6.5037R"><span>Ikaite crystal distribution in Arctic winter sea <span class="hlt">ice</span> and implications for <span class="hlt">CO</span><span class="hlt">2</span> system dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rysgaard, S.; Søgaard, D. H.; Cooper, M.; Pućko, M.; Lennert, K.; Papakyriakou, T. N.; Wang, F.; Geilfus, N. X.; Glud, R. N.; Ehn, J.; McGinnnis, D. F.; Attard, K.; Sievers, J.; Deming, J. W.; Barber, D.</p> <p>2012-12-01</p> <p>The precipitation of ikaite (Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) in polar sea <span class="hlt">ice</span> is critical to the efficiency of the sea <span class="hlt">ice</span>-driven carbon pump and potentially important to the global carbon cycle, yet the spatial and temporal occurrence of ikaite within the <span class="hlt">ice</span> is poorly known. We report unique observations of ikaite in unmelted <span class="hlt">ice</span> and vertical profiles of ikaite abundance and concentration in sea <span class="hlt">ice</span> for the crucial season of winter. <span class="hlt">Ice</span> was examined from two locations: a 1 m thick land-fast <span class="hlt">ice</span> site and a 0.3 m thick polynya site, both in the Young Sound area (74° N, 20° W) of NE Greenland. Ikaite crystals, ranging in size from a few µm to 700 µm were observed to concentrate in the interstices between the <span class="hlt">ice</span> platelets in both granular and columnar sea <span class="hlt">ice</span>. In vertical sea-<span class="hlt">ice</span> profiles from both locations, ikaite concentration determined from image analysis, decreased with depth from surfaceice values of 700-900 µmol kg-1 <span class="hlt">ice</span> (~ 25 × 106 crystals kg-1) to bottom-layer values of 100-200 µmol kg-1 <span class="hlt">ice</span> (1-7 × 106 kg-1), all of which are much higher (4-10 times) than those reported in the few previous studies. Direct measurements of total alkalinity (TA) in surface layers fell within the same range as ikaite concentration whereas TA concentrations in bottom layers were twice as high. This depth-related discrepancy suggests interior <span class="hlt">ice</span> processes where ikaite crystals form in surface sea <span class="hlt">ice</span> layers and partly dissolved in bottom layers. From these findings and model calculations we relate sea <span class="hlt">ice</span> formation and melt to observed p<span class="hlt">CO</span><span class="hlt">2</span> conditions in polar surface waters, and hence, the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020044134','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020044134"><span>Sensitivity of Global Sea-<span class="hlt">Air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> to Gas Transfer Algorithms, Climatological Wind Speeds, and Variability of Sea Surface Temperature and Salinity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McClain, Charles R.; Signorini, Sergio</p> <p>2002-01-01</p> <p>Sensitivity analyses of sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> to gas transfer algorithms, climatological wind speeds, sea surface temperatures (SST) and salinity (SSS) were conducted for the global oceans and selected regional domains. Large uncertainties in the global sea-<span class="hlt">air</span> <span class="hlt">flux</span> estimates are identified due to different gas transfer algorithms, global climatological wind speeds, and seasonal SST and SSS data. The global sea-<span class="hlt">air</span> <span class="hlt">flux</span> ranges from -0.57 to -<span class="hlt">2</span>.27 Gt/yr, depending on the combination of gas transfer algorithms and global climatological wind speeds used. Different combinations of SST and SSS global fields resulted in changes as large as 35% on the oceans global sea-<span class="hlt">air</span> <span class="hlt">flux</span>. An error as small as plus or minus 0.<span class="hlt">2</span> in SSS translates into a plus or minus 43% deviation on the mean global <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. This result emphasizes the need for highly accurate satellite SSS observations for the development of remote sensing sea-<span class="hlt">air</span> <span class="hlt">flux</span> algorithms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5038955','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5038955"><span>A Sensitivity Analysis of the Impact of Rain on Regional and Global Sea-<span class="hlt">Air</span> <span class="hlt">Fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shutler, J. D.; Land, P. E.; Woolf, D. K.; Quartly, G. D.</p> <p>2016-01-01</p> <p>The global oceans are considered a major sink of atmospheric carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>). Rain is known to alter the physical and chemical conditions at the sea surface, and thus influence the transfer of <span class="hlt">CO</span><span class="hlt">2</span> between the ocean and atmosphere. It can influence gas exchange through enhanced gas transfer velocity, the direct export of carbon from the atmosphere to the ocean, by altering the sea skin temperature, and through surface layer dilution. However, to date, very few studies quantifying these effects on global net sea-<span class="hlt">air</span> <span class="hlt">fluxes</span> exist. Here, we include terms for the enhanced gas transfer velocity and the direct export of carbon in calculations of the global net sea-<span class="hlt">air</span> <span class="hlt">fluxes</span>, using a 7-year time series of monthly global climate quality satellite remote sensing observations, model and in-situ data. The use of a non-linear relationship between the effects of rain and wind significantly reduces the estimated impact of rain-induced surface turbulence on the rate of sea-<span class="hlt">air</span> gas transfer, when compared to a linear relationship. Nevertheless, globally, the rain enhanced gas transfer and rain induced direct export increase the estimated annual oceanic integrated net sink of <span class="hlt">CO</span><span class="hlt">2</span> by up to 6%. Regionally, the variations can be larger, with rain increasing the estimated annual net sink in the Pacific Ocean by up to 15% and altering monthly net <span class="hlt">flux</span> by > ± 50%. Based on these analyses, the impacts of rain should be included in the uncertainty analysis of studies that estimate net sea-<span class="hlt">air</span> <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> as the rain can have a considerable impact, dependent upon the region and timescale. PMID:27673683</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...852...75C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...852...75C"><span><span class="hlt">CO</span> Diffusion and Desorption Kinetics in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cooke, Ilsa R.; Öberg, Karin I.; Fayolle, Edith C.; Peeler, Zoe; Bergner, Jennifer B.</p> <p>2018-01-01</p> <p>The diffusion of species in icy dust grain mantles is a fundamental process that shapes the chemistry of interstellar regions; yet, measurements of diffusion in interstellar <span class="hlt">ice</span> analogs are scarce. Here we present measurements of <span class="hlt">CO</span> diffusion into <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at low temperatures (T = 11–23 K) using <span class="hlt">CO</span><span class="hlt">2</span> longitudinal optical phonon modes to monitor the level of mixing of initially layered <span class="hlt">ices</span>. We model the diffusion kinetics using Fick’s second law and find that the temperature-dependent diffusion coefficients are well fit by an Arrhenius equation, giving a diffusion barrier of 300 ± 40 K. The low barrier along with the diffusion kinetics through isotopically labeled layers suggest that <span class="hlt">CO</span> diffuses through <span class="hlt">CO</span><span class="hlt">2</span> along pore surfaces rather than through bulk diffusion. In complementary experiments, we measure the desorption energy of <span class="hlt">CO</span> from <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span> deposited at 11–50 K by temperature programmed desorption and find that the desorption barrier ranges from 1240 ± 90 K to 1410 ± 70 K depending on the <span class="hlt">CO</span><span class="hlt">2</span> deposition temperature and resultant <span class="hlt">ice</span> porosity. The measured CO–<span class="hlt">CO</span><span class="hlt">2</span> desorption barriers demonstrate that <span class="hlt">CO</span> binds equally well to <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">ices</span> when both are compact. The CO–<span class="hlt">CO</span><span class="hlt">2</span> diffusion–desorption barrier ratio ranges from 0.21 to 0.24 dependent on the binding environment during diffusion. The diffusion–desorption ratio is consistent with the above hypothesis that the observed diffusion is a surface process and adds to previous experimental evidence on diffusion in water <span class="hlt">ice</span> that suggests surface diffusion is important to the mobility of molecules within interstellar <span class="hlt">ices</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRC..120..471M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRC..120..471M"><span>Drivers of inorganic carbon dynamics in first-year sea <span class="hlt">ice</span>: A model study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moreau, Sébastien; Vancoppenolle, Martin; Delille, Bruno; Tison, Jean-Louis; Zhou, Jiayun; Kotovitch, Marie; Thomas, David N.; Geilfus, Nicolas-Xavier; Goosse, Hugues</p> <p>2015-01-01</p> <p>Sea <span class="hlt">ice</span> is an active source or a sink for carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), although to what extent is not clear. Here, we analyze <span class="hlt">CO</span><span class="hlt">2</span> dynamics within sea <span class="hlt">ice</span> using a one-dimensional halothermodynamic sea <span class="hlt">ice</span> model including gas physics and carbon biogeochemistry. The <span class="hlt">ice</span>-ocean <span class="hlt">fluxes</span>, and vertical transport, of total dissolved inorganic carbon (DIC) and total alkalinity (TA) are represented using fluid transport equations. Carbonate chemistry, the consumption, and release of <span class="hlt">CO</span><span class="hlt">2</span> by primary production and respiration, the precipitation and dissolution of ikaite (Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) and <span class="hlt">ice-air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, are also included. The model is evaluated using observations from a 6 month field study at Point Barrow, Alaska, and an <span class="hlt">ice</span>-tank experiment. At Barrow, results show that the DIC budget is mainly driven by physical processes, wheras brine-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, ikaite formation, and net primary production, are secondary factors. In terms of <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> exchanges, sea <span class="hlt">ice</span> is a net <span class="hlt">CO</span><span class="hlt">2</span> source and sink in winter and summer, respectively. The formulation of the <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> impacts the simulated near-surface <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>), but not the DIC budget. Because the simulated <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are limited by DIC stocks, and therefore <<span class="hlt">2</span> mmol m-<span class="hlt">2</span> d-1, we argue that the observed much larger <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from eddy covariance retrievals cannot be explained by a sea <span class="hlt">ice</span> direct source and must involve other processes or other sources of <span class="hlt">CO</span><span class="hlt">2</span>. Finally, the simulations suggest that near-surface TA/DIC ratios of ˜<span class="hlt">2</span>, sometimes used as an indicator of calcification, would rather suggest outgassing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1711342M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1711342M"><span>Drivers of inorganic carbon dynamics in first-year sea <span class="hlt">ice</span>: A model study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moreau, Sébastien; Vancoppenolle, Martin; Delille, Bruno; Tison, Jean-Louis; Zhou, Jiayun; Kotovich, Marie; Thomas, David; Geilfus, Nicolas-Xavier; Goosse, Hugues</p> <p>2015-04-01</p> <p>Sea <span class="hlt">ice</span> is an active source or a sink for carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), although to what extent is not clear. Here, we analyze <span class="hlt">CO</span><span class="hlt">2</span> dynamics within sea <span class="hlt">ice</span> using a one-dimensional halo-thermodynamic sea <span class="hlt">ice</span> model including gas physics and carbon biogeochemistry. The <span class="hlt">ice</span>-ocean <span class="hlt">fluxes</span>, and vertical transport, of total dissolved inorganic carbon (DIC) and total alkalinity (TA) are represented using fluid transport equations. Carbonate chemistry, the consumption and release of <span class="hlt">CO</span><span class="hlt">2</span> by primary production and respiration, the precipitation and dissolution of ikaite (Ca<span class="hlt">CO</span>3•6H<span class="hlt">2</span>O) and <span class="hlt">ice-air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, are also included. The model is evaluated using observations from a 6-month field study at Point Barrow, Alaska and an <span class="hlt">ice</span>-tank experiment. At Barrow, results show that the DIC budget is mainly driven by physical processes, wheras brine-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, ikaite formation, and net primary production, are secondary factors. In terms of <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> exchanges, sea <span class="hlt">ice</span> is a net <span class="hlt">CO</span><span class="hlt">2</span> source and sink in winter and summer, respectively. The formulation of the <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> impacts the simulated near-surface <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>), but not the DIC budget. Because the simulated <span class="hlt">ice</span>-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are limited by DIC stocks, and therefore < <span class="hlt">2</span> mmol m-<span class="hlt">2</span> day-1, we argue that the observed much larger <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from eddy covariance retrievals cannot be explained by a sea <span class="hlt">ice</span> direct source and must involve other processes or other sources of <span class="hlt">CO</span><span class="hlt">2</span>. Finally, the simulations suggest that near surface TA/DIC ratios of ~<span class="hlt">2</span>, sometimes used as an indicator of calcification, would rather suggest outgassing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CSR...162...27C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CSR...162...27C"><span>Diurnal variability of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at coastal zone of Taiwan based on eddy covariance observation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chien, Hwa; Zhong, Yao-Zhao; Yang, Kang-Hung; Cheng, Hao-Yuan</p> <p>2018-06-01</p> <p>In this study, we employed shore-based eddy covariance systems for a continuous measurement of the coastal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> near the northwestern coast of Taiwan from 2011 to 2015. To ensure the validity of the analysis, the data was selected and filtered with a footprint model and an empirical mode decomposition method. The results indicate that the nearshore <span class="hlt">air</span>-sea and <span class="hlt">air</span>-land <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> exhibited a significant diurnal variability and a substantial day-night difference. The net <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was -1.75 ± 0.98 μmol-C m-<span class="hlt">2</span> s-1, whereas the net <span class="hlt">air</span>-land <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was 0.54 ± 7.35 μmol-C m-<span class="hlt">2</span> s-1, which indicated that in northwestern Taiwan, the coastal water acts as a sink of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> but the coastal land acts as a source. The Random Forest Method was applied to hierarchize the influence of Chl-a, SST, DO, pH and U10 on <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The result suggests that the strength of the diurnal <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> is strongly influenced by the local wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008P%26SS...56.1300G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008P%26SS...56.1300G"><span>H-implantation in SO <span class="hlt">2</span> and <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garozzo, M.; Fulvio, D.; Gomis, O.; Palumbo, M. E.; Strazzulla, G.</p> <p>2008-07-01</p> <p><span class="hlt">Ices</span> in the solar system are observed on the surface of planets, satellites, comets and asteroids where they are continuously subordinate at particle <span class="hlt">fluxes</span> (cosmic ions, solar wind and charged particles caught in the magnetosphere of the planets) that deeply modify their physical and structural properties. Each incoming ion destroys molecular bonds producing fragments that, by recombination, form new molecules also different from the original ones. Moreover, if the incoming ion is reactive (H +, O n+ , S n+ , etc.), it can concur to the formation of new molecules. Those effects can be studied by laboratory experiments where, with some limitation, it is possible to reproduce the astrophysical environments of planetary <span class="hlt">ices</span>. In this work, we describe some experiments of 15-100 keV H + and He + implantation in pure sulfur dioxide (SO <span class="hlt">2</span>) at 16 and 80 K and carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span>) at 16 K <span class="hlt">ices</span> aimed to search for the formation of new molecules. Among other results we confirm that carbonic acid (H <span class="hlt">2</span><span class="hlt">CO</span> 3) is formed after H-implantation in <span class="hlt">CO</span> <span class="hlt">2</span>, vice versa H-implantation in SO <span class="hlt">2</span> at both temperatures does not produce measurable quantity of sulfurous acid (H <span class="hlt">2</span>SO 3). The results are discussed in the light of their relevance to the chemistry of some solar system objects, particularly of Io, the innermost of Jupiter's Galilean satellites, that exhibits a surface very rich in frost SO <span class="hlt">2</span> and it is continuously bombarded with H + ions caught in Jupiter's magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C13A0944M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C13A0944M"><span>Evaluation of changes in atmospheric and oceanic <span class="hlt">fluxes</span> during continental <span class="hlt">ice</span> sheet retreat</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martin, J.; Martin, E. E.; Deuerling, K. M.</p> <p>2017-12-01</p> <p>Extensive land areas were exposed across North America, Eurasia, and to a lesser extent Greenland as continental <span class="hlt">ice</span> sheets retreated following the last glacial maximum. A transect of watersheds from the coast to the western Greenland <span class="hlt">Ice</span> Sheet (GrIS) provides an opportunity to evaluate possible changes in oceanic solute <span class="hlt">fluxes</span> and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> exchange as <span class="hlt">ice</span> sheets retreat. We evaluate these <span class="hlt">fluxes</span> in one proglacial watershed (draining <span class="hlt">ice</span> sheet runoff) and four deglaciated watersheds (draining local precipitation and permafrost melt). Sr isotope ratios indicate bedrock near the coast has experienced greater weathering than near the <span class="hlt">ice</span> sheet. A mass balance model of the major element composition of stream water indicates weathering in deglaciated watersheds is dominated by carbonic acid dissolution of carbonate minerals near the <span class="hlt">ice</span> sheet that switches to carbonic acid alteration of silicate minerals near the coast. In addition, weathering by sulfuric acid, derived from oxidative dissolution of sulfide minerals, increases from the <span class="hlt">ice</span> sheet to the coast. These changes in the weathered minerals and weathering acids impact <span class="hlt">CO</span><span class="hlt">2</span> sequestration associated with weathering. Weathering consumes 350 to 550 µmol <span class="hlt">CO</span><span class="hlt">2</span>/L in watersheds near the <span class="hlt">ice</span> sheet, but close to the coast, consumes only 15 µmol <span class="hlt">CO</span><span class="hlt">2</span>/L in one watershed and sources 140 µmol <span class="hlt">CO</span><span class="hlt">2</span>/L to the atmosphere at another coastal watershed. The decreasing <span class="hlt">CO</span><span class="hlt">2</span> weathering sink from the GrIS to coast reflects decreased carbonic acid weathering and increased sulfuric acid weathering of carbonate minerals. The proglacial stream shows downstream variations in composition from mixing of two water sources, with only minor in-stream weathering, which consumes < 0.1 µmol <span class="hlt">CO</span><span class="hlt">2</span>/L. Discharge from the deglaciated watersheds is currently unknown but their higher solute concentrations and <span class="hlt">CO</span><span class="hlt">2</span> exchange than proglacial systems suggest deglaciated watersheds dominate atmospheric <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and oceanic solute <span class="hlt">fluxes</span>. These results</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850060100&hterms=Radon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DRadon','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850060100&hterms=Radon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DRadon"><span>Gas exchange and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the tropical Atlantic Ocean determined from Rn-222 and p<span class="hlt">CO</span><span class="hlt">2</span> measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smethie, W. M., Jr.; Takahashi, T.; Chipman, D. W.; Ledwell, J. R.</p> <p>1985-01-01</p> <p>The piston velocity for the tropical Atlantic Ocean has been determined from 29 radon profiles measured during the TTO Tropical Atlantic Study. By combining these data with the p<span class="hlt">CO</span><span class="hlt">2</span> data measured in the surface water and <span class="hlt">air</span> samples, the net <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> across the sea-<span class="hlt">air</span> interface has been calculated for the tropical Atlantic. The dependence of the piston velocity on wind speed is discussed, and possible causes for the high sea-to-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> observed in the equatorial zone are examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACPD...1422587Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACPD...1422587Z"><span>Constraining terrestrial ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by integrating models of biogeochemistry and atmospheric transport and data of surface carbon <span class="hlt">fluxes</span> and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Q.; Zhuang, Q.; Henze, D.; Bowman, K.; Chen, M.; Liu, Y.; He, Y.; Matsueda, H.; Machida, T.; Sawa, Y.; Oechel, W.</p> <p>2014-09-01</p> <p>Regional net carbon <span class="hlt">fluxes</span> of terrestrial ecosystems could be estimated with either biogeochemistry models by assimilating surface carbon <span class="hlt">flux</span> measurements or atmospheric <span class="hlt">CO</span><span class="hlt">2</span> inversions by assimilating observations of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations. Here we combine the ecosystem biogeochemistry modeling and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> inverse modeling to investigate the magnitude and spatial distribution of the terrestrial ecosystem <span class="hlt">CO</span><span class="hlt">2</span> sources and sinks. First, we constrain a terrestrial ecosystem model (TEM) at site level by assimilating the observed net ecosystem production (NEP) for various plant functional types. We find that the uncertainties of model parameters are reduced up to 90% and model predictability is greatly improved for all the plant functional types (coefficients of determination are enhanced up to 0.73). We then extrapolate the model to a global scale at a 0.5° × 0.5° resolution to estimate the large-scale terrestrial ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, which serve as prior for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> inversion. Second, we constrain the large-scale terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by assimilating the GLOBALVIEW-<span class="hlt">CO</span><span class="hlt">2</span> and mid-tropospheric <span class="hlt">CO</span><span class="hlt">2</span> retrievals from the Atmospheric Infrared Sounder (<span class="hlt">AIRS</span>) into an atmospheric transport model (GEOS-Chem). The transport inversion estimates that: (1) the annual terrestrial ecosystem carbon sink in 2003 is -<span class="hlt">2</span>.47 Pg C yr-1, which agrees reasonably well with the most recent inter-comparison studies of <span class="hlt">CO</span><span class="hlt">2</span> inversions (-<span class="hlt">2</span>.82 Pg C yr-1); (<span class="hlt">2</span>) North America temperate, Europe and Eurasia temperate regions act as major terrestrial carbon sinks; and (3) The posterior transport model is able to reasonably reproduce the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations, which are validated against Comprehensive Observation Network for TRace gases by <span class="hlt">AIr</span>Liner (CONTRAIL) <span class="hlt">CO</span><span class="hlt">2</span> concentration data. This study indicates that biogeochemistry modeling or atmospheric transport and inverse modeling alone might not be able to well quantify regional terrestrial carbon <span class="hlt">fluxes</span>. However, combining</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li class="active"><span>2</span></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_2 --> <div id="page_3" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="41"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23778238','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23778238"><span>An inorganic <span class="hlt">CO</span><span class="hlt">2</span> diffusion and dissolution process explains negative <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in saline/alkaline soils.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ma, Jie; Wang, Zhong-Yuan; Stevenson, Bryan A; Zheng, Xin-Jun; Li, Yan</p> <p>2013-01-01</p> <p>An 'anomalous' negative <span class="hlt">flux</span>, in which carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) enters rather than is released from the ground, was studied in a saline/alkaline soil. Soil sterilization disclosed an inorganic process of <span class="hlt">CO</span><span class="hlt">2</span> dissolution into (during the night) and out of (during the day) the soil solution, driven by variation in soil temperature. Experimental and modeling analysis revealed that pH and soil moisture were the most important determinants of the magnitude of this inorganic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. In the extreme cases of <span class="hlt">air</span>-dried saline/alkaline soils, this inorganic process was predominant. While the diurnal <span class="hlt">flux</span> measured was zero sum, leaching of the dissolved inorganic carbon in the soil solution could potentially effect net carbon ecosystem exchange. This finding implies that an inorganic module should be incorporated when dealing with the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of saline/alkaline land. Neglecting this inorganic <span class="hlt">flux</span> may induce erroneous or misleading conclusions in interpreting <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of these ecosystems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3685845','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3685845"><span>An inorganic <span class="hlt">CO</span><span class="hlt">2</span> diffusion and dissolution process explains negative <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in saline/alkaline soils</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ma, Jie; Wang, Zhong-Yuan; Stevenson, Bryan A.; Zheng, Xin-Jun; Li, Yan</p> <p>2013-01-01</p> <p>An ‘anomalous' negative <span class="hlt">flux</span>, in which carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) enters rather than is released from the ground, was studied in a saline/alkaline soil. Soil sterilization disclosed an inorganic process of <span class="hlt">CO</span><span class="hlt">2</span> dissolution into (during the night) and out of (during the day) the soil solution, driven by variation in soil temperature. Experimental and modeling analysis revealed that pH and soil moisture were the most important determinants of the magnitude of this inorganic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. In the extreme cases of <span class="hlt">air</span>-dried saline/alkaline soils, this inorganic process was predominant. While the diurnal <span class="hlt">flux</span> measured was zero sum, leaching of the dissolved inorganic carbon in the soil solution could potentially effect net carbon ecosystem exchange. This finding implies that an inorganic module should be incorporated when dealing with the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of saline/alkaline land. Neglecting this inorganic <span class="hlt">flux</span> may induce erroneous or misleading conclusions in interpreting <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of these ecosystems. PMID:23778238</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14..742J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14..742J"><span>In situ evaluation of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> gas transfer velocity in an inner estuary using eddy covariance - with a special focus on the importance of using reliable <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jørgensen, E. T.; Sørensen, L. L.; Jensen, B.; Sejr, M. K.</p> <p>2012-04-01</p> <p>The <span class="hlt">air</span>-sea exchange of <span class="hlt">CO</span><span class="hlt">2</span> or <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> is driven by the difference in the partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> in the water and the atmosphere (Δp<span class="hlt">CO</span><span class="hlt">2</span>), the solubility of <span class="hlt">CO</span><span class="hlt">2</span> (K0) and the gas transfer velocity (k) (Wanninkhof et al., 2009;Weiss, 1974) . Δp<span class="hlt">CO</span><span class="hlt">2</span> and K0 are determined with relatively high precision and it is estimated that the biggest uncertainty when modelling the <span class="hlt">air</span>-sea <span class="hlt">flux</span> is the parameterization of k. As an example; the estimated global <span class="hlt">air</span>-sea <span class="hlt">flux</span> increases by 70 % when using the parameterization by Wanninkhof and McGillis (1999) instead of Wanninkhof (1992) (Rutgersson et al., 2008). In coastal areas the uncertainty is even higher and only few studies have focused on determining transfer velocity for the coastal waters and even fewer on estuaries (Borges et al., 2004;Rutgersson et al., 2008). The transfer velocity (k600) of <span class="hlt">CO</span><span class="hlt">2</span> in the inner estuary of Roskilde Fjord, Denmark was investigated using eddy covariance <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (ECM) and directly measured Δp<span class="hlt">CO</span><span class="hlt">2</span> during May and June 2010. The data was strictly sorted to heighten the certainty of the results and the outcome was; DS1; using only ECM, and DS<span class="hlt">2</span>; including the inertial dissipation method (IDM). The inner part of Roskilde Fjord showed to be a very biological active <span class="hlt">CO</span><span class="hlt">2</span> sink and preliminary results showed that the average k600 was more than 10 times higher than transfer velocities from similar studies of other coastal areas. The much higher transfer velocities were estimated to be caused by the greater fetch and shallower water in Roskilde Fjord, which indicated that turbulence in both <span class="hlt">air</span> and water influence k600. The wind speed parameterization of k600 using DS1 showed some scatter but when including IDM the r<span class="hlt">2</span> of DS<span class="hlt">2</span> reached 0.93 with an exponential parameterization, where U10 was based on the Businger-Dyer relationships using friction velocity and atmospheric stability. This indicates that some of the uncertainties coupled with <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> calculated by the ECM are removed when including the IDM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25898645','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25898645"><span>[Partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span><span class="hlt">2</span> degassing <span class="hlt">fluxes</span> of Huayuankou and Xiaolangdi Station affected by Xiaolangdi Reservoir].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yong-ling; Yang, Xiao-lin; Zhang, Dong</p> <p>2015-01-01</p> <p>According to periodic sampling analysis per month in Xiaolangdi station and Huayuankou station from November 2011 to October 2012, combined with continuous sampling analysis of Xiaolangdi Reservoir during runoff and sediment control period in 2012, partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> (p<span class="hlt">CO</span><span class="hlt">2</span>) in surface water were calculated based on Henry's Law, p<span class="hlt">CO</span><span class="hlt">2</span> features and <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> degassing <span class="hlt">fluxes</span> of Huayuankou station and Xiaolangdi station affected by Xiaolangdi Reservoir were studied. The results were listed as follows, when Xiaolangdi Reservoir operated normally, p<span class="hlt">CO</span><span class="hlt">2</span> in surface water of Xiaolangdi station and Huayuankou station varied from 82 to 195 Pa and from 99 to 228 Pa, moreover, p<span class="hlt">CO</span><span class="hlt">2</span> in surface water from July to September were distinctly higher than those in other months; meanwhile, p<span class="hlt">CO</span>, in surface water from Huayuankou station were higher than that from Xiaolangdi station. During runoff and sediment control period of Xiaolangdi Reservoir, two hydrological stations commonly indicated that p<span class="hlt">CO</span><span class="hlt">2</span> in surface water during water draining were obviously lower than those during sediment releasing. Whether in the period of normal operation or runoff and sediment control, p<span class="hlt">CO</span><span class="hlt">2</span> in surface water had positive relations to DIC content in two hydrological stations. Since the Ep<span class="hlt">CO</span>,/AOU value was higher than the theoretical value of 0. 62, the biological aerobic respiration effect had distinct contribution to p<span class="hlt">CO</span><span class="hlt">2</span>. Throughout the whole year, <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> degassing <span class="hlt">fluxes</span> from Xiaolangdi station and Huayuankou station were 0.486 p.mol (m<span class="hlt">2</span> s) -l and 0.588 pmol (m<span class="hlt">2</span> x s)(-1) respectively; When Xiaolangdi Reservoir operated normally, <span class="hlt">air</span>-water <span class="hlt">CO</span>, degassing <span class="hlt">fluxes</span> in Huayuankou station were higher than that in Xiaolangdi station; during runoff and sediment control from Xiaolangdi Reservoir, two hydrological stations had one observation result in common, namely, <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> degassing <span class="hlt">fluxes</span> in the period of water draining were obviously lower than that in the period of sediment releasing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GBioC..30..983L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GBioC..30..983L"><span>Quantifying the drivers of ocean-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lauderdale, Jonathan M.; Dutkiewicz, Stephanie; Williams, Richard G.; Follows, Michael J.</p> <p>2016-07-01</p> <p>A mechanistic framework for quantitatively mapping the regional drivers of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at a global scale is developed. The framework evaluates the interplay between (1) surface heat and freshwater <span class="hlt">fluxes</span> that influence the potential saturated carbon concentration, which depends on changes in sea surface temperature, salinity and alkalinity, (<span class="hlt">2</span>) a residual, disequilibrium <span class="hlt">flux</span> influenced by upwelling and entrainment of remineralized carbon- and nutrient-rich waters from the ocean interior, as well as rapid subduction of surface waters, (3) carbon uptake and export by biological activity as both soft tissue and carbonate, and (4) the effect on surface carbon concentrations due to freshwater precipitation or evaporation. In a steady state simulation of a coarse-resolution ocean circulation and biogeochemistry model, the sum of the individually determined components is close to the known total <span class="hlt">flux</span> of the simulation. The leading order balance, identified in different dynamical regimes, is between the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> driven by surface heat <span class="hlt">fluxes</span> and a combination of biologically driven carbon uptake and disequilibrium-driven carbon outgassing. The framework is still able to reconstruct simulated <span class="hlt">fluxes</span> when evaluated using monthly averaged data and takes a form that can be applied consistently in models of different complexity and observations of the ocean. In this way, the framework may reveal differences in the balance of drivers acting across an ensemble of climate model simulations or be applied to an analysis and interpretation of the observed, real-world <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMPP21A1252A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMPP21A1252A"><span>Modelling the effects of <span class="hlt">ice</span>-sheet activity on <span class="hlt">CO</span><span class="hlt">2</span> outgassing by Icelandic volcanoes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Armitage, J. J.; Ferguson, D.; Petersen, K. D.; Creyts, T. T.</p> <p>2017-12-01</p> <p>Glacial cycles may play a significant role in mediating the <span class="hlt">flux</span> of magmatic <span class="hlt">CO</span><span class="hlt">2</span> between the Earth's mantle and atmosphere. In Iceland, it is thought that late-Pleistocene deglaciation led to a significant volcanic pulse, evidenced by increased post-glacial lava volumes and changes in melt chemistry consistent with depressurization. Investigating the extent to which glacial activity may have affected volcanic <span class="hlt">CO</span><span class="hlt">2</span> emissions from Iceland, and crucially over what timescale, requires detailed knowledge of how the magma system responded to the growth and collapse of the <span class="hlt">ice</span>-sheet before and after the LGM. To investigate this, we coupled a model of magma generation and transport with a history of <span class="hlt">ice</span>-sheet activity. Our results show that the emplacement and removal of the LGM <span class="hlt">ice</span>-sheet likely led to two significant pulses of magmatic <span class="hlt">CO</span><span class="hlt">2</span>. The first, and most significant of these, is associated with <span class="hlt">ice</span>-sheet growth and occurs as the magma system recovers from glacial loading. This recovery happens from the base of the melting region upwards, producing a pulse of <span class="hlt">CO</span><span class="hlt">2</span> rich magma that is predicted to reach the surface around 20 ka after the loading event, close in time to the LGM. The second peak in <span class="hlt">CO</span><span class="hlt">2</span> output occurs abruptly following deglaciation as a consequence of increased rates of melt generation and transport in the shallow mantle. Although these post-glacial melts are relatively depleted in <span class="hlt">CO</span><span class="hlt">2</span>, the increase in magma <span class="hlt">flux</span> leads to a short-lived period of elevated <span class="hlt">CO</span><span class="hlt">2</span> emissions. Our results therefore suggest a negative feedback, whereby <span class="hlt">ice</span>-sheet growth produces a delayed pulse of magmatic <span class="hlt">CO</span><span class="hlt">2</span>, which, in addition to increased geothermal heat <span class="hlt">flux</span>, may contribute towards driving deglaciation, which itself then causes further magmatism and <span class="hlt">CO</span><span class="hlt">2</span> outgassing. This model is consistent with the seismic structure of the asthenosphere below Iceland, and the established compositional and volumetric trends for sub- and post-glacial volcanism in Iceland. These trends show that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AMT.....9.5509Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AMT.....9.5509Y"><span>Comparison of two closed-path cavity-based spectrometers for measuring <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> by eddy covariance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Mingxi; Prytherch, John; Kozlova, Elena; Yelland, Margaret J.; Parenkat Mony, Deepulal; Bell, Thomas G.</p> <p>2016-11-01</p> <p>In recent years several commercialised closed-path cavity-based spectroscopic instruments designed for eddy covariance <span class="hlt">flux</span> measurements of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), methane (CH4), and water vapour (H<span class="hlt">2</span>O) have become available. Here we compare the performance of two leading models - the Picarro G2311-f and the Los Gatos Research (LGR) Fast Greenhouse Gas Analyzer (FGGA) at a coastal site. Both instruments can compute dry mixing ratios of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 based on concurrently measured H<span class="hlt">2</span>O, temperature, and pressure. Additionally, we used a high throughput Nafion dryer to physically remove H<span class="hlt">2</span>O from the Picarro airstream. Observed <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> from these two analysers, averaging about 12 and 0.12 mmol m-<span class="hlt">2</span> day-1 respectively, agree within the measurement uncertainties. For the purpose of quantifying dry <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> downstream of a long inlet, the numerical H<span class="hlt">2</span>O corrections appear to be reasonably effective and lead to results that are comparable to physical removal of H<span class="hlt">2</span>O with a Nafion dryer in the mean. We estimate the high-frequency attenuation of <span class="hlt">fluxes</span> in our closed-path set-up, which was relatively small ( ≤ 10 %) for <span class="hlt">CO</span><span class="hlt">2</span> and CH4 but very large for the more polar H<span class="hlt">2</span>O. The Picarro showed significantly lower noise and <span class="hlt">flux</span> detection limits than the LGR. The hourly <span class="hlt">flux</span> detection limit for the Picarro was about <span class="hlt">2</span> mmol m-<span class="hlt">2</span> day-1 for <span class="hlt">CO</span><span class="hlt">2</span> and 0.02 mmol m-<span class="hlt">2</span> day-1 for CH4. For the LGR these detection limits were about 8 and 0.05 mmol m-<span class="hlt">2</span> day-1. Using global maps of monthly mean <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> as reference, we estimate that the Picarro and LGR can resolve hourly <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from roughly 40 and 4 % of the world's oceans respectively. Averaging over longer timescales would be required in regions with smaller <span class="hlt">fluxes</span>. Hourly <span class="hlt">flux</span> detection limits of CH4 from both instruments are generally higher than the expected emissions from the open ocean, though the signal to noise of this measurement may improve closer to the coast.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140005809','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140005809"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Estimation Errors Associated with Moist Atmospheric Processes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parazoo, N. C.; Denning, A. S.; Kawa, S. R.; Pawson, S.; Lokupitiya, R.</p> <p>2012-01-01</p> <p>Vertical transport by moist sub-grid scale processes such as deep convection is a well-known source of uncertainty in <span class="hlt">CO</span><span class="hlt">2</span> source/sink inversion. However, a dynamical link between vertical transport, satellite based retrievals of column mole fractions of <span class="hlt">CO</span><span class="hlt">2</span>, and source/sink inversion has not yet been established. By using the same offline transport model with meteorological fields from slightly different data assimilation systems, we examine sensitivity of frontal <span class="hlt">CO</span><span class="hlt">2</span> transport and retrieved <span class="hlt">fluxes</span> to different parameterizations of sub-grid vertical transport. We find that frontal transport feeds off background vertical <span class="hlt">CO</span><span class="hlt">2</span> gradients, which are modulated by sub-grid vertical transport. The implication for source/sink estimation is two-fold. First, <span class="hlt">CO</span><span class="hlt">2</span> variations contained in moist poleward moving <span class="hlt">air</span> masses are systematically different from variations in dry equatorward moving <span class="hlt">air</span>. Moist poleward transport is hidden from orbital sensors on satellites, causing a sampling bias, which leads directly to small but systematic <span class="hlt">flux</span> retrieval errors in northern mid-latitudes. Second, differences in the representation of moist sub-grid vertical transport in GEOS-4 and GEOS-5 meteorological fields cause differences in vertical gradients of <span class="hlt">CO</span><span class="hlt">2</span>, which leads to systematic differences in moist poleward and dry equatorward <span class="hlt">CO</span><span class="hlt">2</span> transport and therefore the fraction of <span class="hlt">CO</span><span class="hlt">2</span> variations hidden in moist <span class="hlt">air</span> from satellites. As a result, sampling biases are amplified and regional scale <span class="hlt">flux</span> errors enhanced, most notably in Europe (0.43+/-0.35 PgC /yr). These results, cast from the perspective of moist frontal transport processes, support previous arguments that the vertical gradient of <span class="hlt">CO</span><span class="hlt">2</span> is a major source of uncertainty in source/sink inversion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1167255','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1167255"><span><span class="hlt">CO</span><span class="hlt">2</span> CH4 <span class="hlt">flux</span> <span class="hlt">Air</span> temperature Soil temperature and Soil moisture, Barrow, Alaska 2013 ver. 1</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Margaret Torn</p> <p>2015-01-14</p> <p>This dataset consists of field measurements of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span>, as well as soil properties made during 2013 in Areas A-D of Intensive Site 1 at the Next-Generation Ecosystem Experiments (NGEE) Arctic site near Barrow, Alaska. Included are i) measurements of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> made from June to September (ii) Calculation of corresponding Gross Primary Productivity (GPP) and CH4 exchange (transparent minus opaque) between atmosphere and the ecosystem (ii) Measurements of Los Gatos Research (LGR) chamber <span class="hlt">air</span> temperature made from June to September (ii) measurements of surface layer depth, type of surface layer, soil temperature and soil moisture from June to September.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApJ...801..118L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApJ...801..118L"><span><span class="hlt">CO</span> Diffusion into Amorphous H<span class="hlt">2</span>O <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lauck, Trish; Karssemeijer, Leendertjan; Shulenberger, Katherine; Rajappan, Mahesh; Öberg, Karin I.; Cuppen, Herma M.</p> <p>2015-03-01</p> <p>The mobility of atoms, molecules, and radicals in icy grain mantles regulates <span class="hlt">ice</span> restructuring, desorption, and chemistry in astrophysical environments. Interstellar <span class="hlt">ices</span> are dominated by H<span class="hlt">2</span>O, and diffusion on external and internal (pore) surfaces of H<span class="hlt">2</span>O-rich <span class="hlt">ices</span> is therefore a key process to constrain. This study aims to quantify the diffusion kinetics and barrier of the abundant <span class="hlt">ice</span> constituent <span class="hlt">CO</span> into H<span class="hlt">2</span>O-dominated <span class="hlt">ices</span> at low temperatures (15-23 K), by measuring the mixing rate of initially layered H<span class="hlt">2</span>O(:<span class="hlt">CO</span><span class="hlt">2</span>)/<span class="hlt">CO</span> <span class="hlt">ices</span>. The mixed fraction of <span class="hlt">CO</span> as a function of time is determined by monitoring the shape of the infrared <span class="hlt">CO</span> stretching band. Mixing is observed at all investigated temperatures on minute timescales and can be ascribed to <span class="hlt">CO</span> diffusion in H<span class="hlt">2</span>O <span class="hlt">ice</span> pores. The diffusion coefficient and final mixed fraction depend on <span class="hlt">ice</span> temperature, porosity, thickness, and composition. The experiments are analyzed by applying Fick’s diffusion equation under the assumption that mixing is due to <span class="hlt">CO</span> diffusion into an immobile H<span class="hlt">2</span>O <span class="hlt">ice</span>. The extracted energy barrier for <span class="hlt">CO</span> diffusion into amorphous H<span class="hlt">2</span>O <span class="hlt">ice</span> is ˜160 K. This is effectively a surface diffusion barrier. The derived barrier is low compared to current surface diffusion barriers in use in astrochemical models. Its adoption may significantly change the expected timescales for different <span class="hlt">ice</span> processes in interstellar environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApJ...816L..28F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApJ...816L..28F"><span>N<span class="hlt">2</span> and <span class="hlt">CO</span> Desorption Energies from Water <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fayolle, Edith C.; Balfe, Jodi; Loomis, Ryan; Bergner, Jennifer; Graninger, Dawn; Rajappan, Mahesh; Öberg, Karin I.</p> <p>2016-01-01</p> <p>The relative desorption energies of <span class="hlt">CO</span> and N<span class="hlt">2</span> are key to interpretations of observed interstellar <span class="hlt">CO</span> and N<span class="hlt">2</span> abundance patterns, including the well-documented <span class="hlt">CO</span> and N<span class="hlt">2</span>H+ anti-correlations in disks, protostars, and molecular cloud cores. Based on laboratory experiments on pure <span class="hlt">CO</span> and N<span class="hlt">2</span> <span class="hlt">ice</span> desorption, the difference between <span class="hlt">CO</span> and N<span class="hlt">2</span> desorption energies is small; the N<span class="hlt">2</span>-to-<span class="hlt">CO</span> desorption energy ratio is 0.93 ± 0.03. Interstellar <span class="hlt">ices</span> are not pure, however, and in this study we explore the effect of water <span class="hlt">ice</span> on the desorption energy ratio of the two molecules. We present temperature programmed desorption experiments of different coverages of 13<span class="hlt">CO</span> and 15N<span class="hlt">2</span> on porous and compact amorphous water <span class="hlt">ices</span> and, for reference, of pure <span class="hlt">ices</span>. In all experiments, 15N<span class="hlt">2</span> desorption begins a few degrees before the onset of 13<span class="hlt">CO</span> desorption. The 15N<span class="hlt">2</span> and 13<span class="hlt">CO</span> energy barriers are 770 and 866 K for the pure <span class="hlt">ices</span>, 1034-1143 K and 1155-1298 K for different submonolayer coverages on compact water <span class="hlt">ice</span>, and 1435 and 1575 K for ˜1 ML of <span class="hlt">ice</span> on top of porous water <span class="hlt">ice</span>. For all equivalent experiments, the N<span class="hlt">2</span>-to-<span class="hlt">CO</span> desorption energy ratio is consistently 0.9. Whenever <span class="hlt">CO</span> and N<span class="hlt">2</span> <span class="hlt">ice</span> reside in similar <span class="hlt">ice</span> environments (e.g., experience a similar degree of interaction with water <span class="hlt">ice</span>) their desorption temperatures should thus be within a few degrees of one another. A smaller N<span class="hlt">2</span>-to-<span class="hlt">CO</span> desorption energy ratio may be present in interstellar and circumstellar environments if the average <span class="hlt">CO</span> <span class="hlt">ice</span> molecules interacts more with water <span class="hlt">ice</span> compared to the average N<span class="hlt">2</span> molecules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002DSRII..49.1601T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002DSRII..49.1601T"><span>Global sea-<span class="hlt">air</span> <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> based on climatological surface ocean p<span class="hlt">CO</span> <span class="hlt">2</span>, and seasonal biological and temperature effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takahashi, Taro; Sutherland, Stewart C.; Sweeney, Colm; Poisson, Alain; Metzl, Nicolas; Tilbrook, Bronte; Bates, Nicolas; Wanninkhof, Rik; Feely, Richard A.; Sabine, Christopher; Olafsson, Jon; Nojiri, Yukihiro</p> <p></p> <p>Based on about 940,000 measurements of surface-water p<span class="hlt">CO</span> <span class="hlt">2</span> obtained since the International Geophysical Year of 1956-59, the climatological, monthly distribution of p<span class="hlt">CO</span> <span class="hlt">2</span> in the global surface waters representing mean non-El Niño conditions has been obtained with a spatial resolution of 4°×5° for a reference year 1995. The monthly and annual net sea-<span class="hlt">air</span> <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> has been computed using the NCEP/NCAR 41-year mean monthly wind speeds. An annual net uptake <span class="hlt">flux</span> of <span class="hlt">CO</span> <span class="hlt">2</span> by the global oceans has been estimated to be <span class="hlt">2.2</span> (+22% or -19%) Pg C yr -1 using the (wind speed) <span class="hlt">2</span> dependence of the <span class="hlt">CO</span> <span class="hlt">2</span> gas transfer velocity of Wanninkhof (J. Geophys. Res. 97 (1992) 7373). The errors associated with the wind-speed variation have been estimated using one standard deviation (about±<span class="hlt">2</span> m s -1) from the mean monthly wind speed observed over each 4°×5° pixel area of the global oceans. The new global uptake <span class="hlt">flux</span> obtained with the Wanninkhof (wind speed) <span class="hlt">2</span> dependence is compared with those obtained previously using a smaller number of measurements, about 250,000 and 550,000, respectively, and are found to be consistent within±0.<span class="hlt">2</span> Pg C yr -1. This estimate for the global ocean uptake <span class="hlt">flux</span> is consistent with the values of <span class="hlt">2</span>.0±0.6 Pg C yr -1 estimated on the basis of the observed changes in the atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> and oxygen concentrations during the 1990s (Nature 381 (1996) 218; Science 287 (2000) 2467). However, if the (wind speed) 3 dependence of Wanninkhof and McGillis (Res. Lett. 26 (1999) 1889) is used instead, the annual ocean uptake as well as the sensitivity to wind-speed variability is increased by about 70%. A zone between 40° and 60° latitudes in both the northern and southern hemispheres is found to be a major sink for atmospheric <span class="hlt">CO</span> <span class="hlt">2</span>. In these areas, poleward-flowing warm waters meet and mix with the cold subpolar waters rich in nutrients. The p<span class="hlt">CO</span> <span class="hlt">2</span> in the surface water is decreased by the cooling effect on warm waters and by the biological drawdown of p<span class="hlt">CO</span> <span class="hlt">2</span> in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28987084','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28987084"><span>Formation and decomposition of <span class="hlt">CO</span><span class="hlt">2</span>-filled <span class="hlt">ice</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Massani, B; Mitterdorfer, C; Loerting, T</p> <p>2017-10-07</p> <p>Recently it was shown that <span class="hlt">CO</span> <span class="hlt">2</span> -filled <span class="hlt">ice</span> is formed upon compression of <span class="hlt">CO</span> <span class="hlt">2</span> -clathrate hydrate. Here we show two alternative routes of its formation, namely, by decompression of <span class="hlt">CO</span> <span class="hlt">2</span> /<span class="hlt">ice</span> VI mixtures at 250 K and by isobaric heating of <span class="hlt">CO</span> <span class="hlt">2</span> /high-density amorphous <span class="hlt">ice</span> mixtures at 0.5-1.0 GPa above 200 K. Furthermore, we show that filled <span class="hlt">ice</span> may either transform into the clathrate at an elevated pressure or decompose to "empty" hexagonal <span class="hlt">ice</span> at ambient pressure and low temperature. This complements the literature studies in which decomposition to <span class="hlt">ice</span> VI was favoured at high pressures and low temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.147m4503M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.147m4503M"><span>Formation and decomposition of <span class="hlt">CO</span><span class="hlt">2</span>-filled <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Massani, B.; Mitterdorfer, C.; Loerting, T.</p> <p>2017-10-01</p> <p>Recently it was shown that <span class="hlt">CO</span><span class="hlt">2</span>-filled <span class="hlt">ice</span> is formed upon compression of <span class="hlt">CO</span><span class="hlt">2</span>-clathrate hydrate. Here we show two alternative routes of its formation, namely, by decompression of <span class="hlt">CO</span><span class="hlt">2</span>/<span class="hlt">ice</span> VI mixtures at 250 K and by isobaric heating of <span class="hlt">CO</span><span class="hlt">2</span>/high-density amorphous <span class="hlt">ice</span> mixtures at 0.5-1.0 GPa above 200 K. Furthermore, we show that filled <span class="hlt">ice</span> may either transform into the clathrate at an elevated pressure or decompose to "empty" hexagonal <span class="hlt">ice</span> at ambient pressure and low temperature. This complements the literature studies in which decomposition to <span class="hlt">ice</span> VI was favoured at high pressures and low temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.B23A0388H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.B23A0388H"><span>Solution for Minimizing Surface Heating Effect for Fast Open-Path <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Measurements in Cold Environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hupp, J. R.; Burba, G. G.; McDermitt, D. K.; Anderson, D. J.; Eckles, R. D.</p> <p>2010-12-01</p> <p>Open-path design of the high speed gas analyzers is a well-established configuration widely used for measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations. This configuration has advantages and deficiencies. Advantages include excellent frequency response, long-term stability, low sensitivity to window contamination, low-power pump-free operation, and infrequent calibration requirements. Deficiencies include susceptibility to precipitation and <span class="hlt">icing</span>, and a potential need for instrument surface heating correction in extremely cold environments. In spite of the deficiencies, open-path measurements often provide data coverage that would not have been possible using traditional closed-path approach. Data loss from precipitation and <span class="hlt">icing</span> may not always be prevented for the open-path instruments, while heating effect does not pose a problem for <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in warm environments. Even in cold environments, the impact of heating on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> is much smaller than other well-known effects, such as Webb-Pearman-Leuning terms, or frequency response corrections for closed-path analyzers. Nonetheless, instrument surface heating effect in cold environments could be addressed scientifically, via developing the theoretical corrections, and instrumentally, via measuring fast integrated <span class="hlt">air</span> temperature in the optical path, or via enclosing the open-path instrument into a low-power short-intake design. Here we provide an alternative way to minimize or eliminate open-path heating effect, achieved by minimizing or eliminating the temperature gradient between the instrument surface and ambient <span class="hlt">air</span>. Open-path low temperature controlled design is discussed in comparison with two other approaches (e.g., traditional open-path design and closed-path design) in terms of their field performance for Eddy Covariance <span class="hlt">flux</span> measurements in the cold. This study presents field data from a new open-path <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O gas analyzer, LI-7500A, based on the LI-7500 model modified to produce substantially less heat during</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B41B0407B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B41B0407B"><span>Field evaluation of open and closed-path <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> systems over asphalt surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bogoev, I.; Santos, E.</p> <p>2016-12-01</p> <p>Eddy covariance (EC) is a widely used method for quantifying surface <span class="hlt">fluxes</span> of heat, water vapor and carbon dioxide between ecosystems and the atmosphere. A typical EC system consists of an ultrasonic anemometer measuring the 3D wind vector and a fast-response infrared gas analyzer for sensing the water vapor and <span class="hlt">CO</span><span class="hlt">2</span> density in the <span class="hlt">air</span>. When using an open-path analyzer that detects the constituent's density in situ a correction for concurrent <span class="hlt">air</span> temperature and humidity fluctuations must be applied, Webb et al. (1980). In environments with small magnitudes of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> (<5µmol m-<span class="hlt">2</span> s-1) and in the presence of high sensible heat <span class="hlt">flux</span>, like wintertime over boreal forest, open-path <span class="hlt">flux</span> measurements have been challenging since the magnitude of the density corrections are as large as the uncorrected <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> itself. A new technology merging the sensing paths of the gas analyzer and the sonic anemometer has been recently developed. This new integrated instrument allows a direct measurement of <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio in the open <span class="hlt">air</span> and has the potential to improve the quality of the temperature related density corrections by synchronously measuring the sensible heat <span class="hlt">flux</span> in the optical path of the gas analyzer. We evaluate the performance and the accuracy of this new sensor over a large parking lot with an asphalt surface where the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are considered low and the interfering sensible heat <span class="hlt">fluxes</span> are above 200 Wm-<span class="hlt">2</span>. A <span class="hlt">co</span>-located closed-path EC system is used as a reference measurement to examine any systematic biases and apparent <span class="hlt">CO</span><span class="hlt">2</span> uptake observed with open-path sensors under high sensible heat <span class="hlt">flux</span> regimes. Half-hour mean and variance of <span class="hlt">CO</span><span class="hlt">2</span> and water vapor concentrations are evaluated. The relative spectral responses, covariances and corrected turbulent <span class="hlt">fluxes</span> using a common sonic anemometer are analyzed. The influence of sensor separation and frequency response attenuation on the density corrections is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010022991','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010022991"><span>BOREAS TF-3 Automated Chamber <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Data from the NSA-OBS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goulden, Michael L.; Crill, Patrick M.; Hall, Forrest G. (Editor); Conrad, Sara (Editor)</p> <p>2000-01-01</p> <p>The BOReal Ecosystem Atmosphere Study Tower <span class="hlt">Flux</span> (BOREAS TF-3) and Trace Gas Biogeochemistry (TGB-1) teams collected automated <span class="hlt">CO</span><span class="hlt">2</span> chamber <span class="hlt">flux</span> data in their efforts to fully describe the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at the Northern Study Area-Old Black Spruce (NSA-OBS) site. This data set contains <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> at the NSA-OBS site measured using automated chambers. In addition to reporting the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, it reports chamber <span class="hlt">air</span> temperature, moss temperature, and light levels during each measurement. The data set covers the period from 23-Sep-1995 through 26-Oct-1995 and from 28-May-1996 through 21-Oct-1996. The data are stored in tabular ASCII files.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B21C1972P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B21C1972P"><span>Implications for carbon processing beneath the Greenland <span class="hlt">Ice</span> Sheet from dissolved <span class="hlt">CO</span><span class="hlt">2</span> and CH4 concentrations of subglacial discharge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pain, A.; Martin, J.; Martin, E. E.</p> <p>2017-12-01</p> <p>Subglacial carbon processes are of increasing interest as warming induces <span class="hlt">ice</span> melting and increases <span class="hlt">fluxes</span> of glacial meltwater into proglacial rivers and the coastal ocean. Meltwater may serve as an atmospheric source or sink of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) or methane (CH4), depending on the magnitudes of subglacial organic carbon (OC) remineralization, which produces <span class="hlt">CO</span><span class="hlt">2</span> and CH4, and mineral weathering reactions, which consume <span class="hlt">CO</span><span class="hlt">2</span> but not CH4. We report wide variability in dissolved <span class="hlt">CO</span><span class="hlt">2</span> and CH4 concentrations at the beginning of the melt season (May-June 2017) between three sites draining land-terminating glaciers of the Greenland <span class="hlt">Ice</span> Sheet. Two sites, located along the Watson River in western Greenland, drain the Isunnguata and Russell Glaciers and contained 1060 and 400 ppm <span class="hlt">CO</span><span class="hlt">2</span>, respectively. In-situ <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements indicated that the Isunnguata was a source of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, while the Russell was a sink. Both sites had elevated CH4 concentrations, at 325 and 25 ppm CH4, respectively, suggesting active anaerobic OC remineralization beneath the <span class="hlt">ice</span> sheet. Dissolved <span class="hlt">CO</span><span class="hlt">2</span> and CH4 reached atmospheric equilibrium within <span class="hlt">2</span>.6 and 8.6 km downstream of Isunnguata and Russell discharge sites, respectively. These changes reflect rapid gas exchange with the atmosphere and/or <span class="hlt">CO</span><span class="hlt">2</span> consumption via instream mineral weathering. The third site, draining the Kiagtut Sermiat in southern Greenland, had about half atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations (250 ppm), but approximately atmospheric CH4 concentrations (<span class="hlt">2</span>.1 ppm). Downstream <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements indicated ingassing of <span class="hlt">CO</span><span class="hlt">2</span> over the entire 10-km length of the proglacial river. <span class="hlt">CO</span><span class="hlt">2</span> undersaturation may be due to more readily weathered lithologies underlying the Kiagtut Sermiat compared to Watson River sites, but low CH4 concentrations also suggest limited contributions of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 from OC remineralization. These results suggest that carbon processing beneath the Greenland <span class="hlt">Ice</span> Sheet may be more variable than previously recognized</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGeo...10.2699S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGeo...10.2699S"><span>Coccolithophore surface distributions in the North Atlantic and their modulation of the <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> from 10 years of satellite Earth observation data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shutler, J. D.; Land, P. E.; Brown, C. W.; Findlay, H. S.; Donlon, C. J.; Medland, M.; Snooke, R.; Blackford, J. C.</p> <p>2013-04-01</p> <p>Coccolithophores are the primary oceanic phytoplankton responsible for the production of calcium carbonate (Ca<span class="hlt">CO</span>3). These climatically important plankton play a key role in the oceanic carbon cycle as a major contributor of carbon to the open ocean carbonate pump (~50%) and their calcification can affect the atmosphere-to-ocean (<span class="hlt">air</span>-sea) uptake of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) through increasing the seawater partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> (p<span class="hlt">CO</span><span class="hlt">2</span>). Here we document variations in the areal extent of surface blooms of the globally important coccolithophore, Emiliania huxleyi, in the North Atlantic over a 10-year period (1998-2007), using Earth observation data from the Sea-viewing Wide Field-of-view Sensor (SeaWiFS). We calculate the annual mean sea surface areal coverage of E. huxleyi in the North Atlantic to be 474 000 ± 104 000 km<span class="hlt">2</span>, which results in a net Ca<span class="hlt">CO</span>3 carbon (Ca<span class="hlt">CO</span>3-C) production of 0.14-1.71 Tg Ca<span class="hlt">CO</span>3-C per year. However, this surface coverage (and, thus, net production) can fluctuate inter-annually by -54/+8% about the mean value and is strongly correlated with the El Niño/Southern Oscillation (ENSO) climate oscillation index (r=0.75, p<0.02). Our analysis evaluates the spatial extent over which the E. huxleyi blooms in the North Atlantic can increase the p<span class="hlt">CO</span><span class="hlt">2</span> and, thus, decrease the localised <span class="hlt">air</span>-sea <span class="hlt">flux</span> of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. In regions where the blooms are prevalent, the average reduction in the monthly <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> can reach 55%. The maximum reduction of the monthly <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the time series is 155%. This work suggests that the high variability, frequency and distribution of these calcifying plankton and their impact on p<span class="hlt">CO</span><span class="hlt">2</span> should be considered if we are to fully understand the variability of the North Atlantic <span class="hlt">air</span>-to-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>. We estimate that these blooms can reduce the annual N. Atlantic net sink atmospheric <span class="hlt">CO</span><span class="hlt">2</span> by between 3-28%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010022990','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010022990"><span>BOREAS TF-4 <span class="hlt">CO</span><span class="hlt">2</span> and CH4 Chamber <span class="hlt">Flux</span> Data from the SSA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anderson, Dean; Striegl, Robert; Wickland, Kimberly; Hall, Forrest G. (Editor); Conrad, Sara (Editor)</p> <p>2000-01-01</p> <p>The BOREAS TF-4 team measured <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 across the soil-<span class="hlt">air</span> interface in four ages of jack pine forest at the BOREAS SSA during August 1993 to March 1995. Gross and net <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">flux</span> of CH4 between soil and <span class="hlt">air</span> are presented for 24 chamber sites in mature jack pine forest, 20-year-old, 4-year-old, and clear cut areas. The data are stored in tabular ASCII files.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.8634D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.8634D"><span>Interannual variability of primary production and <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the Atlantic and Indian sectors of the Southern Ocean.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dufour, Carolina; Merlivat, Liliane; Le Sommer, Julien; Boutin, Jacqueline; Antoine, David</p> <p>2013-04-01</p> <p>As one of the major oceanic sinks of anthropogenic <span class="hlt">CO</span><span class="hlt">2</span>, the Southern Ocean plays a critical role in the climate system. However, due to the scarcity of observations, little is known about physical and biological processes that control <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and how these processes might respond to climate change. It is well established that primary production is one of the major drivers of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, consuming surface Dissolved Inorganic Carbon (DIC) during Summer. Southern Ocean primary production is though constrained by several limiting factors such as iron and light availability, which are both sensitive to mixed layer depth. Mixed layer depth is known to be affected by current changes in wind stress or freshwater <span class="hlt">fluxes</span> over the Southern Ocean. But we still don't know how primary production may respond to anomalous mixed layer depth neither how physical processes may balance this response to set the seasonal cycle of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. In this study, we investigate the impact of anomalous mixed layer depth on surface DIC in the Atlantic and Indian sectors of the Subantarctic zone of the Southern Ocean (60W-60E, 38S-55S) with a combination of in situ data, satellite data and model experiment. We use both a regional eddy permitting ocean biogeochemical model simulation based on NEMO-PISCES and data-based reconstruction of biogeochemical fields based on CARIOCA buoys and SeaWiFS data. A decomposition of the physical and biological processes driving the seasonal variability of surface DIC is performed with both the model data and observations. A good agreement is found between the model and the data for the amplitude of biological and <span class="hlt">air</span>-sea <span class="hlt">flux</span> contributions. The model data are further used to investigate the impact of winter and summer anomalies in mixed layer depth on surface DIC over the period 1990-2004. The relative changes of each physical and biological process contribution are quantified and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JMS...140...26M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JMS...140...26M"><span>Spatio-temporal dynamics of biogeochemical processes and <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the Western English Channel based on two years of FerryBox deployment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marrec, P.; Cariou, T.; Latimier, M.; Macé, E.; Morin, P.; Vernet, M.; Bozec, Y.</p> <p>2014-12-01</p> <p>From January 2011 to January 2013, a FerryBox system was installed on a Voluntary Observing Ship (VOS), which crossed the Western English Channel (WEC) between Roscoff (France) and Plymouth (UK) up to 3 times a day. The FerryBox continuously measured sea surface temperature (SST), sea surface salinity (SSS), dissolved oxygen (DO), fluorescence and partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> (from April 2012) along the ferry track. Sensors were calibrated based on 714 bimonthly surface samplings with precisions of 0.016 for SSS, 3.3 μM for DO, 0.40 μg L- 1 for Chlorophyll-a (Chl-a) (based on fluorescence measurements) and 5.<span class="hlt">2</span> μatm for p<span class="hlt">CO</span><span class="hlt">2</span>. Over the <span class="hlt">2</span> years of deployment (900 crossings), we reported 9% of data lost due to technical issues and quality checked data was obtained to allow investigation of the dynamics of biogeochemical processes related to <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the WEC. Based on this unprecedented high-frequency dataset, the physical structure of the WEC was assessed using SST anomalies and the presence of a thermal front was observed around the latitude 49.5°N, which divided the WEC in two main provinces: the seasonally stratified northern WEC (nWEC) and the all-year well-mixed southern WEC (sWEC). These hydrographical properties strongly influenced the spatial and inter-annual distributions of phytoplankton blooms, which were mainly limited by nutrients and light availability in the nWEC and the sWEC, respectively. <span class="hlt">Air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were also highly related to hydrographical properties of the WEC between late April and early September 2012, with the sWEC a weak source of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere of 0.9 mmol m- <span class="hlt">2</span> d- 1, whereas the nWEC acted as a sink for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> of 6.9 mmol m- <span class="hlt">2</span> d- 1. The study of short time-scale dynamics of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> revealed that an intense and short (less than 10 days) summer bloom in the nWEC contributed to 29% of the <span class="hlt">CO</span><span class="hlt">2</span> sink during the productive period, highlighting the necessity for high frequency observations in coastal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..1110845A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..1110845A"><span>Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> Over the Last 1000 Years: WAIS Divide <span class="hlt">Ice</span> Core Record</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahn, J.; Brook, E. J.</p> <p>2009-04-01</p> <p>How atmospheric <span class="hlt">CO</span><span class="hlt">2</span> varied over the last thousands years is of great interest because we may see not only natural, but also anthropogenic variations (Ruddiman, Climatic Change, 2003). The Law Dome <span class="hlt">ice</span> cores reveal decadal to centennial variations in <span class="hlt">CO</span><span class="hlt">2</span> over the last 2000 years (MacFarling Meure et al., Geophys. Res. Lett., 2006). However, these variations have not yet been well confirmed in other <span class="hlt">ice</span> core records. Here we use a newly drilled WAIS Divide <span class="hlt">ice</span> core, which is ideal for this purpose because WAIS Divide has relatively high snow accumulation rate and small gas age distribution that allow us to observe decadal <span class="hlt">CO</span><span class="hlt">2</span> variations with minimal damping. We have started an extensive study of <span class="hlt">CO</span><span class="hlt">2</span> in WAIS Divide core. So far we have obtained data for 960-1940 A.D. from the WDC05-A core drilled in 2005-2006. 344 <span class="hlt">ice</span> samples from 103 depths were analyzed and the standard error of the mean is ~0.8 ppm on average. Ancient <span class="hlt">air</span> in 8~12 g of bubbly <span class="hlt">ice</span> is liberated by crushing with steel pins at -35 °C and trapped in stainless steel tubes at -262 °C. <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio in the extracted <span class="hlt">air</span> is precisely determined using a gas chromatographic method. Details of the high-precision methods are described in Ahn et al. (J. of Glaciology, in press). Our new results show preindustrial atmospheric <span class="hlt">CO</span><span class="hlt">2</span> variability of ~ 10 ppm. The most striking feature of the record is a rapid atmospheric <span class="hlt">CO</span><span class="hlt">2</span> decrease of 7~8 ppm within ~20 years at ~ 1600 A.D. Considering the larger smoothing of gas records in the WAIS Divide relative to Law Dome, our results confirm the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> decrease of ~10 ppm in Law Dome records observed at this time. However, this event is not significant in the Dronning Maud Land <span class="hlt">ice</span> core (Siegenthaler et al., Tellus, 2005), probably due to more extensive smoothing of gas records in the core. Similar rapid changes of <span class="hlt">CO</span><span class="hlt">2</span> at other times in the WAIS Divide record need to be confirmed with higher resolution studies. We also found that our WAIS Divide <span class="hlt">CO</span><span class="hlt">2</span> data are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCD.....6.1015R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCD.....6.1015R"><span>Ikaite crystals in melting sea <span class="hlt">ice</span> - implications for p<span class="hlt">CO</span><span class="hlt">2</span> and pH levels in Arctic surface waters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rysgaard, S.; Glud, R. N.; Lennert, K.; Cooper, M.; Halden, N.; Leakey, R. J. G.; Hawthorne, F. C.; Barber, D.</p> <p>2012-03-01</p> <p>A major issue of Arctic marine science is to understand whether the Arctic Ocean is, or will be, a source or sink for <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange. This has been complicated by the recent discoveries of ikaite (Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) in Arctic and Antarctic sea <span class="hlt">ice</span>, which indicate that multiple chemical transformations occur in sea <span class="hlt">ice</span> with a possible effect on <span class="hlt">CO</span><span class="hlt">2</span> and pH conditions in surface waters. Here we report on biogeochemical conditions, microscopic examinations and x-ray diffraction analysis of single crystals from an actively melting 1.7 km<span class="hlt">2</span> (0.5-1 m thick) drifting <span class="hlt">ice</span> floe in the Fram Strait during summer. Our findings show that ikaite crystals are present throughout the sea <span class="hlt">ice</span> but with larger crystals appearing in the upper <span class="hlt">ice</span> layers. Ikaite crystals placed at elevated temperatures gradually disintegrated into smaller crystallites and dissolved. During our field campaign in late June, melt reduced the <span class="hlt">ice</span> flow thickness by ca. 0.<span class="hlt">2</span> m per week and resulted in an estimated 1.6 ppm decrease of p<span class="hlt">CO</span><span class="hlt">2</span> in the ocean surface mixed layer. This corresponds to an <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> uptake of 11 mmol m-<span class="hlt">2</span> sea <span class="hlt">ice</span> d-1 or to 3.5 ton km-<span class="hlt">2</span> <span class="hlt">ice</span> floe week-1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcSci..13..997P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcSci..13..997P"><span>The spatial and interannual dynamics of the surface water carbonate system and <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the outer shelf and slope of the Eurasian Arctic Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pipko, Irina I.; Pugach, Svetlana P.; Semiletov, Igor P.; Anderson, Leif G.; Shakhova, Natalia E.; Gustafsson, Örjan; Repina, Irina A.; Spivak, Eduard A.; Charkin, Alexander N.; Salyuk, Anatoly N.; Shcherbakova, Kseniia P.; Panova, Elena V.; Dudarev, Oleg V.</p> <p>2017-11-01</p> <p>The Arctic is undergoing dramatic changes which cover the entire range of natural processes, from extreme increases in the temperatures of <span class="hlt">air</span>, soil, and water, to changes in the cryosphere, the biodiversity of Arctic waters, and land vegetation. Small changes in the largest marine carbon pool, the dissolved inorganic carbon pool, can have a profound impact on the carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">flux</span> between the ocean and the atmosphere, and the feedback of this <span class="hlt">flux</span> to climate. Knowledge of relevant processes in the Arctic seas improves the evaluation and projection of carbon cycle dynamics under current conditions of rapid climate change. Investigation of the <span class="hlt">CO</span><span class="hlt">2</span> system in the outer shelf and continental slope waters of the Eurasian Arctic seas (the Barents, Kara, Laptev, and East Siberian seas) during 2006, 2007, and 2009 revealed a general trend in the surface water partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> (p<span class="hlt">CO</span><span class="hlt">2</span>) distribution, which manifested as an increase in p<span class="hlt">CO</span><span class="hlt">2</span> values eastward. The existence of this trend was defined by different oceanographic and biogeochemical regimes in the western and eastern parts of the study area; the trend is likely increasing due to a combination of factors determined by contemporary change in the Arctic climate, each change in turn evoking a series of synergistic effects. A high-resolution in situ investigation of the carbonate system parameters of the four Arctic seas was carried out in the warm season of 2007; this year was characterized by the next-to-lowest historic sea-<span class="hlt">ice</span> extent in the Arctic Ocean, on satellite record, to that date. The study showed the different responses of the seawater carbonate system to the environment changes in the western vs. the eastern Eurasian Arctic seas. The large, open, highly productive water area in the northern Barents Sea enhances atmospheric <span class="hlt">CO</span><span class="hlt">2</span> uptake. In contrast, the uptake of <span class="hlt">CO</span><span class="hlt">2</span> was strongly weakened in the outer shelf and slope waters of the East Siberian Arctic seas under the 2007 environmental conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5031984','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5031984"><span>A new frontier in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements using a highly portable DIAL laser system</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Queiβer, Manuel; Granieri, Domenico; Burton, Mike</p> <p>2016-01-01</p> <p>Volcanic <span class="hlt">CO</span><span class="hlt">2</span> emissions play a key role in the geological carbon cycle, and monitoring of volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> helps to forecast eruptions. The quantification of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> is challenging due to rapid dilution of magmatic <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">CO</span><span class="hlt">2</span>-rich ambient <span class="hlt">air</span> and the diffuse nature of many emissions, leading to large uncertainties in the global magmatic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> inventory. Here, we report measurements using a new DIAL laser remote sensing system for volcanic <span class="hlt">CO</span><span class="hlt">2</span> (<span class="hlt">CO</span><span class="hlt">2</span>DIAL). Two sites in the volcanic zone of Campi Flegrei (Italy) were scanned, yielding <span class="hlt">CO</span><span class="hlt">2</span> path-amount profiles used to compute <span class="hlt">fluxes</span>. Our results reveal a relatively high <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from Campi Flegrei, consistent with an increasing trend. Unlike previous methods, the <span class="hlt">CO</span><span class="hlt">2</span>DIAL is able to measure integrated <span class="hlt">CO</span><span class="hlt">2</span> path-amounts at distances up to 2000 m using virtually any solid surface as a reflector, whilst also being highly portable. This opens a new frontier in quantification of geological and anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. PMID:27652775</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ECSS..176....1M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ECSS..176....1M"><span>Temporal variability of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange in a low-emission estuary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mørk, Eva Thorborg; Sejr, Mikael Kristian; Stæhr, Peter Anton; Sørensen, Lise Lotte</p> <p>2016-07-01</p> <p>There is the need for further study of whether global estimates of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange in estuarine systems capture the relevant temporal variability and, as such, the temporal variability of bulk parameterized and directly measured <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> was investigated in the Danish estuary, Roskilde Fjord. The <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> showed large temporal variability across seasons and between days and that more than 30% of the net <span class="hlt">CO</span><span class="hlt">2</span> emission in 2013 was a result of two large fall and winter storms. The diurnal variability of Δp<span class="hlt">CO</span><span class="hlt">2</span> was up to 400 during summer changing the estuary from a source to a sink of <span class="hlt">CO</span><span class="hlt">2</span> within the day. Across seasons the system was suggested to change from a sink of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during spring to near neutral during summer and later to a source of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during fall. Results indicated that Roskilde Fjord was an annual low-emission estuary, with an estimated bulk parameterized release of 3.9 ± 8.7 mol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> y-1 during 2012-2013. It was suggested that the production-respiration balance leading to the low annual emission in Roskilde Fjord, was caused by the shallow depth, long residence time and high water quality in the estuary. In the data analysis the eddy covariance <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> samples were filtered according to the H<span class="hlt">2</span>Osbnd <span class="hlt">CO</span><span class="hlt">2</span> cross-sensitivity assessment suggested by Landwehr et al. (2014). This filtering reduced episodes of contradicting directions between measured and bulk parameterized <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchanges and changed the net <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange from an uptake to a release. The <span class="hlt">CO</span><span class="hlt">2</span> gas transfer velocity was calculated from directly measured <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and Δp<span class="hlt">CO</span><span class="hlt">2</span> and agreed to previous observations and parameterizations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009ApJ...690..486M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ApJ...690..486M"><span>Infrared Spectra and Thermodynamic Properties of <span class="hlt">Co</span><span class="hlt">2</span>/Methanol <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maté, Belén; Gálvez, Óscar; Herrero, Víctor J.; Escribano, Rafael</p> <p>2009-01-01</p> <p><span class="hlt">Ices</span> of mixtures of carbon dioxide and methanol have been studied in a range of temperatures relevant for star-forming regions, comets, polar caps of planets and satellites, and other solar system bodies. We have performed temperature-programmed desorption measurements and recorded IR spectra of various types of samples. The presence of two slightly different structures of <span class="hlt">CO</span><span class="hlt">2</span> is manifest. A distorted <span class="hlt">CO</span><span class="hlt">2</span> structure is characterized by bandshifts between 5 cm-1 (ν3) and 10 cm-1 (ν<span class="hlt">2</span>) with respect to normal <span class="hlt">CO</span><span class="hlt">2</span>. If the samples are heated above 130 K, the distorted <span class="hlt">CO</span><span class="hlt">2</span> sublimates and only the normal structure remains. The latter can stay trapped until the sublimation of crystalline methanol (150 K). The desorption energy (E d ~ 20 kJ mol-1) of <span class="hlt">CO</span><span class="hlt">2</span> from methanol <span class="hlt">ice</span>, and the specific adsorption surface area (6 m<span class="hlt">2</span> g-1) of amorphous CH3OH <span class="hlt">ice</span>, have been determined. <span class="hlt">CO</span><span class="hlt">2</span> does not penetrate into crystalline <span class="hlt">ice</span>. Whereas the desorption energy is similar to that of <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O samples, the specific surface of methanol is much smaller than that of amorphous solid water (ASW). The interaction of <span class="hlt">CO</span><span class="hlt">2</span> molecules with water and methanol is similar but <span class="hlt">ices</span> of CH3OH are much less porous than ASW. The inclusion of <span class="hlt">CO</span><span class="hlt">2</span> into previously formed <span class="hlt">ices</span> containing these two species would take place preferentially into ASW. However, in processes of simultaneous deposition, methanol <span class="hlt">ice</span> can admit a larger amount of <span class="hlt">CO</span><span class="hlt">2</span> than water <span class="hlt">ice</span>. <span class="hlt">CO</span><span class="hlt">2</span>/CH3OH <span class="hlt">ices</span> formed by simultaneous deposition admit two orders of magnitude more <span class="hlt">CO</span><span class="hlt">2</span> than sequentially deposited <span class="hlt">ices</span>. These findings can have direct relevance to the interpretation of observations from protostellar environments (e.g., RAFGL7009S) and comet nuclei.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002122','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002122"><span>Natural <span class="hlt">Air</span>-Sea <span class="hlt">Flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> in Simulations of the NASA-GISS Climate Model: Sensitivity to the Physical Ocean Model Formulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Romanou, A.; Gregg, Watson W.; Romanski, J.; Kelley, M.; Bleck, R.; Healy, R.; Nazarenko, L.; Russell, G.; Schmidt, G. A.; Sun, S.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150002122'); toggleEditAbsImage('author_20150002122_show'); toggleEditAbsImage('author_20150002122_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150002122_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150002122_hide"></p> <p>2013-01-01</p> <p>Results from twin control simulations of the preindustrial <span class="hlt">CO</span><span class="hlt">2</span> gas exchange (natural <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>) between the ocean and the atmosphere are presented here using the NASA-GISS climate model, in which the same atmospheric component (modelE<span class="hlt">2</span>) is coupled to two different ocean models, the Russell ocean model and HYCOM. Both incarnations of the GISS climate model are also coupled to the same ocean biogeochemistry module (NOBM) which estimates prognostic distributions for biotic and abiotic fields that influence the <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>. Model intercomparison is carried out at equilibrium conditions and model differences are contrasted with biases from present day climatologies. Although the models agree on the spatial patterns of the <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>, they disagree on the strength of the North Atlantic and Southern Ocean sinks mainly because of kinematic (winds) and chemistry (p<span class="hlt">CO</span><span class="hlt">2</span>) differences rather than thermodynamic (SST) ones. Biology/chemistry dissimilarities in the models stem from the different parameterizations of advective and diffusive processes, such as overturning, mixing and horizontal tracer advection and to a lesser degree from parameterizations of biogeochemical processes such as gravitational settling and sinking. The global meridional overturning circulation illustrates much of the different behavior of the biological pump in the two models, together with differences in mixed layer depth which are responsible for different SST, DIC and nutrient distributions in the two models and consequently different atmospheric feedbacks (in the wind, net heat and freshwater <span class="hlt">fluxes</span> into the ocean).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950045752&hterms=Parkinsons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DParkinsons','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950045752&hterms=Parkinsons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DParkinsons"><span>The role of sea <span class="hlt">ice</span> in <span class="hlt">2</span> x <span class="hlt">CO</span><span class="hlt">2</span> climate model sensitivity. Part 1: The total influence of sea <span class="hlt">ice</span> thickness and extent</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rind, D.; Healy, R.; Parkinson, C.; Martinson, D.</p> <p>1995-01-01</p> <p>As a first step in investigating the effects of sea <span class="hlt">ice</span> changes on the climate sensitivity to doubled atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, the authors use a standard simple sea <span class="hlt">ice</span> model while varying the sea <span class="hlt">ice</span> distributions and thicknesses in the control run. Thinner <span class="hlt">ice</span> amplifies the atmospheric temperature senstivity in these experiments by about 15% (to a warming of 4.8 C), because it is easier for the thinner <span class="hlt">ice</span> to be removed as the climate warms. Thus, its impact on sensitivity is similar to that of greater sea <span class="hlt">ice</span> extent in the control run, which provides more opportunity for sea <span class="hlt">ice</span> reduction. An experiment with sea <span class="hlt">ice</span> not allowed to change between the control and doubled <span class="hlt">CO</span><span class="hlt">2</span> simulations illustrates that the total effect of sea <span class="hlt">ice</span> on surface <span class="hlt">air</span> temperature changes, including cloud cover and water vapor feedbacks that arise in response to sea <span class="hlt">ice</span> variations, amounts to 37% of the temperature sensitivity to the <span class="hlt">CO</span><span class="hlt">2</span> doubling, accounting for 1.56 C of the 4.17 C global warming. This is about four times larger than the sea <span class="hlt">ice</span> impact when no feedbacks are allowed. The different experiments produce a range of results for southern high latitudes with the hydrologic budget over Antarctica implying sea level increases of varying magnitude or no change. These results highlight the importance of properly constraining the sea <span class="hlt">ice</span> response to climate perturbations, necessitating the use of more realistic sea <span class="hlt">ice</span> and ocean models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCry....6..901R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCry....6..901R"><span>Ikaite crystals in melting sea <span class="hlt">ice</span> - implications for p<span class="hlt">CO</span><span class="hlt">2</span> and pH levels in Arctic surface waters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rysgaard, S.; Glud, R. N.; Lennert, K.; Cooper, M.; Halden, N.; Leakey, R. J. G.; Hawthorne, F. C.; Barber, D.</p> <p>2012-08-01</p> <p>A major issue of Arctic marine science is to understand whether the Arctic Ocean is, or will be, a source or sink for <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange. This has been complicated by the recent discoveries of ikaite (a polymorph of Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) in Arctic and Antarctic sea <span class="hlt">ice</span>, which indicate that multiple chemical transformations occur in sea <span class="hlt">ice</span> with a possible effect on <span class="hlt">CO</span><span class="hlt">2</span> and pH conditions in surface waters. Here, we report on biogeochemical conditions, microscopic examinations and x-ray diffraction analysis of single crystals from a melting 1.7 km<span class="hlt">2</span> (0.5-1 m thick) drifting <span class="hlt">ice</span> floe in the Fram Strait during summer. Our findings show that ikaite crystals are present throughout the sea <span class="hlt">ice</span> but with larger crystals appearing in the upper <span class="hlt">ice</span> layers. Ikaite crystals placed at elevated temperatures disintegrated into smaller crystallites and dissolved. During our field campaign in late June, melt reduced the <span class="hlt">ice</span> floe thickness by 0.<span class="hlt">2</span> m per week and resulted in an estimated 3.8 ppm decrease of p<span class="hlt">CO</span><span class="hlt">2</span> in the ocean surface mixed layer. This corresponds to an <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> uptake of 10.6 mmol m-<span class="hlt">2</span> sea <span class="hlt">ice</span> d-1 or to 3.3 ton km-<span class="hlt">2</span> <span class="hlt">ice</span> floe week-1. This is markedly higher than the estimated primary production within the <span class="hlt">ice</span> floe of 0.3-1.3 mmol m-<span class="hlt">2</span> sea <span class="hlt">ice</span> d-1. Finally, the presence of ikaite in sea <span class="hlt">ice</span> and the dissolution of the mineral during melting of the sea <span class="hlt">ice</span> and mixing of the melt water into the surface oceanic mixed layer accounted for half of the estimated p<span class="hlt">CO</span><span class="hlt">2</span> uptake.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1514237M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1514237M"><span>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in alley-cropping systems composed of black locust and poplar trees, Germany</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Medinski, Tetiana; Freese, Dirk; Boehm, Christian</p> <p>2013-04-01</p> <p>The understanding of soil carbon dynamics after establishment of alley-cropping systems is crucial for mitigation of greenhouse <span class="hlt">CO</span><span class="hlt">2</span> gas. This study investigates soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in alley-cropping systems composed of strips of black locust (Robinia pseudoacacia L.) and poplar (Max 1) trees and adjacent to them crop strips (Lupinus). Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was measured monthly over a period from March to November 2012, using a LI-COR LI-8100A automated device. Concurrently with <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements, soil and <span class="hlt">air</span> temperature and soil moisture were recorded within 10 cm of each collar. Soil samples were collected nearby each soil collar for microbial C and hot water-extractable C analyses. At each study plot, root biomass was measured to a depth of 15 cm. In all vegetation types, soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> increased from May to August, showing a significant positive correlation with <span class="hlt">air</span> and soil temperature, which can be a reflection of increase in photosynthesis over the warm summer months. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was the highest in poplar followed by black locust and lupines. The relationships between <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, microbial biomass and hot water-extractable carbon were not straightforward. Among the measured parameters, root density was found to be the main factor to explain the higher <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in tree strips.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16..583M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16..583M"><span>Dynamics of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> based on FerryBox measurements and satellite-based prediction of p<span class="hlt">CO</span><span class="hlt">2</span> in the Western English Channel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marrec, Pierre; Thierry, Cariou; Eric, Mace; Pascal, Morin; Marc, Vernet; Yann, Bozec</p> <p>2014-05-01</p> <p>Since April 2012, we installed an autonomous FerryBox system on a Voluntary Observing Ship (VOS), which crosses the Western English Channel (WEC) between Roscoff and Plymouth on a daily basis. High-frequency data of sea surface temperature (SST), salinity (SSS), fluorescence, dissolved oxygen (DO) and partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> (p<span class="hlt">CO</span><span class="hlt">2</span>) were recorded for two years across the all-year mixed southern WEC (sWEC) and the seasonally stratified northern WEC (nWEC). These contrasting hydrographical provinces strongly influenced the spatio-temporal distributions of p<span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. During the productive period (from May to September), the nWEC acted as a sink for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> of -5.6 mmolC m-<span class="hlt">2</span> d-1 and -4.6 mmolC m-<span class="hlt">2</span> d-1, in 2012 and 2013, respectively. During the same period, the sWEC showed significant inter-annual variability degassing <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere in 2012 (1.4 mmolC m-<span class="hlt">2</span> d-1) and absorbing atmospheric <span class="hlt">CO</span><span class="hlt">2</span> in 2013 (-1.6 mmolC m-<span class="hlt">2</span> d-1). In 2012, high-frequency data revealed that an intense and short (less than 10 days) summer phytoplankton bloom in the nWEC contributed to 31% of the total <span class="hlt">CO</span><span class="hlt">2</span> drawdown during the productive period, highlighting the necessity of p<span class="hlt">CO</span><span class="hlt">2</span> high-frequency measurements in coastal ecosystems. Based on this multi-annual dataset, we developed p<span class="hlt">CO</span><span class="hlt">2</span> algorithms using multiple linear regression (MLR) based on SST, SSS, chlorophyll-a (Chl-a) concentration, time, latitude and mixed layer depth to predict p<span class="hlt">CO</span><span class="hlt">2</span> in the two hydrographical provinces of the WEC. MLR were performed based on more than 200,000 underway observations spanning the range from 150 to 480 µatm. The root mean square errors (RMSE) of the MLR fit to the data were 17.<span class="hlt">2</span> µatm and 21.5 µatm for the s WEC and the nWEC with correlation coefficient (r²) of 0.71 and 0.79, respectively. We applied these algorithms to satellite SST and Chl-a products and to modeled SSS estimates in the entire WEC. Based on these high-frequency and satellite approaches, we will discuss the main</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20140002146&hterms=climate+change+ocean&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dclimate%2Bchange%2Bocean','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20140002146&hterms=climate+change+ocean&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dclimate%2Bchange%2Bocean"><span>Monitoring Ocean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> from Space: GOSAT and OCO-<span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Crisp, David</p> <p>2012-01-01</p> <p>The ocean is a major component of the global carbon cycle, emitting over 330 billion tons of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) into the atmosphere each year, or about 10 times that emitted fossil fuel combustion and all other human activities [1, <span class="hlt">2</span>]. The ocean reabsorbs a comparable amount of <span class="hlt">CO</span><span class="hlt">2</span> each year, along with 25% of the <span class="hlt">CO</span><span class="hlt">2</span> emitted by these human activities. The nature and geographic distribution of the processes controlling these ocean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are still poorly constrained by observations. A better understanding of these processes is essential to predict how this important <span class="hlt">CO</span><span class="hlt">2</span> sink may evolve as the climate changes.While in situ measurements of ocean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> can be very precise, the sampling density is far too sparse to quantify ocean <span class="hlt">CO</span><span class="hlt">2</span> sources and sinks over much of the globe. One way to improve the spatial resolution, coverage, and sampling frequency is to make observations of the column averaged <span class="hlt">CO</span><span class="hlt">2</span> dry <span class="hlt">air</span> mole fraction, XCO<span class="hlt">2</span>, from space [4, 5, 6]. Such measurements could provide global coverage at high resolution (< 100 km) on monthly time scales. High precision (< 1 part per million, ppm) is essential to resolve the small, near-surface <span class="hlt">CO</span><span class="hlt">2</span> variations associated with ocean <span class="hlt">fluxes</span> and to better constrain the <span class="hlt">CO</span><span class="hlt">2</span> transport over the ocean. The Japanese Greenhouse gases Observing Satellite (GOSAT) and the NASA Orbiting Carbon Observatory (OCO) were first two space based sensors designed specifically for this task. GOSAT was successfully launched on January 23, 2009, and has been returning measurements of XCO<span class="hlt">2</span> since April 2009. The OCO mission was lost in February 2009, when its launch vehicle malfunctioned and failed to reach orbit. In early 2010, NASA authorized a re-flight of OCO, called OCO-<span class="hlt">2</span>, which is currently under development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMS...173...70C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMS...173...70C"><span><span class="hlt">Air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> for the Brazilian northeast continental shelf in a climatic transition region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carvalho, A. C. O.; Marins, R. V.; Dias, F. J. S.; Rezende, C. E.; Lefèvre, N.; Cavalcante, M. S.; Eschrique, S. A.</p> <p>2017-09-01</p> <p>Oceanographic cruises were carried out in October 2012 (3°S-5°S and 38,5°W-35,5°W) and in September 2014 (1°S-4°S and 43°W-37°W), measuring atmospheric and sea surface <span class="hlt">CO</span><span class="hlt">2</span> fugacity (f<span class="hlt">CO</span><span class="hlt">2</span>) underway in the northeast coast of Brazil. Sea surface water samples were also collected for chlorophyll a, nutrients and DOC analysis. During the second cruise, the sampling area covered a transition between semi-arid to more humid areas of the coast, with different hydrologic and rainfall regimes. The seawater f<span class="hlt">CO</span><span class="hlt">2</span>sw, in October 2012, was in average 400.9 ± 7.3μatm and 391.1 ± 6.3 μatm in September 2014. For the atmosphere, the f<span class="hlt">CO</span><span class="hlt">2</span><span class="hlt">air</span> in October 2012 was 375.8 ± <span class="hlt">2</span>.0 μatm and in September 2014, 368.9 ± <span class="hlt">2.2</span> μatm. The super-saturation of the seawater in relation to the atmosphere indicates a source of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere. The entire study area presents oligotrophic conditions. Despite the low concentrations, Chl a and nutrients presented significant influence on f<span class="hlt">CO</span><span class="hlt">2</span>sw, particularly in the westernmost and more humid part of the northeast coast, where river <span class="hlt">fluxes</span> are three orders of magnitude larger than eastern rivers and rainfall events are more intense and constant. f<span class="hlt">CO</span><span class="hlt">2</span>sw spatial distribution presented homogeneity along the same transect and longitudinal heterogeneity, between east and west, reinforcing the hypothesis of transition between two regions of different behaviour. The f<span class="hlt">CO</span><span class="hlt">2</span>sw at the eastern portion was controlled by parameters such as temperature and salinity. At the western portion, f<span class="hlt">CO</span><span class="hlt">2</span>sw was influenced by nutrient and Chl a. Calculated instantaneous <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> ranged from + 1.66 to + 7.24 mmol m- <span class="hlt">2</span> d- 1 in the first cruise and + 0.89 to + 14.62 mmol m- <span class="hlt">2</span> d- 1 in the second cruise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.C11C0384L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.C11C0384L"><span>Integrating Carbon <span class="hlt">Flux</span> Measurements with Hydrologic and Thermal Responses in a Low Centered <span class="hlt">Ice</span>-Wedge Polygon near Prudhoe Bay, AK</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Larson, T.; Young, M.; Caldwell, T. G.; Abolt, C.</p> <p>2014-12-01</p> <p>Substantial attention is being devoted to soil organic carbon (SOC) dynamics in Polar Regions, given the potential impacts of <span class="hlt">CO</span><span class="hlt">2</span> and methane (CH4) release into the atmosphere. In this study, which is part of a broader effort to quantify carbon loss pathways in patterned Arctic permafrost soils, CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements were recorded from a site approximately 30 km south of Deadhorse, Alaska and 1 km west of the Dalton Highway. Samples were collected in late July, 2014 using six static <span class="hlt">flux</span> chambers that were located within a single low-centered <span class="hlt">ice</span>-wedge polygon. Three <span class="hlt">flux</span> chambers were <span class="hlt">co</span>-located (within a 1 m triangle of each other) near the center of the polygon and three were <span class="hlt">co</span>-located (along a 1.5 m line) on the ridge adjacent to a trough. Soil in the center of the polygon was 100% water saturated, whereas water saturation measured on the ridge ranged between 25-50%. Depth to <span class="hlt">ice</span> table was approximately 50 cm near the center of the polygon and 40 cm at the ridge. Temperature depth probes were installed within the center and ridge of the polygon. Nine gas measurements were collected from each chamber over a 24 h period, stored in helium-purged Exetainer vials, shipped to a laboratory, and analyzed using gas chromatography. Measured cumulative methane <span class="hlt">fluxes</span> were linear over the 24 h period demonstrating constant methane production, but considerable spatial variability in <span class="hlt">flux</span> was observed (0.1 to 4.7 mg hr-1 m-<span class="hlt">2</span> in polygon center, and 0.003 to 0.36 mg hr-1m-<span class="hlt">2</span> on polygon ridge). Shallow soil temperatures varied between 1.3 and 9.8oC in the center and 0.6 to 7.5oC in the rim of the polygon. <span class="hlt">Air</span> temperatures varied between 1.3 and 4.6oC. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were greater than methane <span class="hlt">fluxes</span> and more consistent at each <span class="hlt">co</span>-location; ranging from 21.7 to 36.6 mg hr-1 m-<span class="hlt">2</span> near the polygon centers and 3.5 to 29.1 mg hr-1 m-<span class="hlt">2</span> in the drier polygon ridge. Results are consistent with previous observations that methanogenesis is favored in a water saturated active layer. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5400058','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5400058"><span>Revisiting the choice of the driving temperature for eddy covariance <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wohlfahrt, Georg; Galvagno, Marta</p> <p>2017-01-01</p> <p>So-called <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning algorithms are widely used to partition the net ecosystem <span class="hlt">CO</span><span class="hlt">2</span> exchange into the two component <span class="hlt">fluxes</span>, gross primary productivity and ecosystem respiration. Common <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning algorithms conceptualize ecosystem respiration to originate from a single source, requiring the choice of a corresponding driving temperature. Using a conceptual dual-source respiration model, consisting of an above- and a below-ground respiration source each driven by a corresponding temperature, we demonstrate that the typical phase shift between <span class="hlt">air</span> and soil temperature gives rise to a hysteresis relationship between ecosystem respiration and temperature. The hysteresis proceeds in a clockwise fashion if soil temperature is used to drive ecosystem respiration, while a counter-clockwise response is observed when ecosystem respiration is related to <span class="hlt">air</span> temperature. As a consequence, nighttime ecosystem respiration is smaller than daytime ecosystem respiration when referenced to soil temperature, while the reverse is true for <span class="hlt">air</span> temperature. We confirm these qualitative modelling results using measurements of day and night ecosystem respiration made with opaque chambers in a short-statured mountain grassland. Inferring daytime from nighttime ecosystem respiration or vice versa, as attempted by <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning algorithms, using a single-source respiration model is thus an oversimplification resulting in biased estimates of ecosystem respiration. We discuss the likely magnitude of the bias, options for minimizing it and conclude by emphasizing that the systematic uncertainty of gross primary productivity and ecosystem respiration inferred through <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning needs to be better quantified and reported. PMID:28439145</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B33C0620I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B33C0620I"><span>Analysis of uncertainties in GOSAT-inferred regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishizawa, M.; Shirai, T.; Maksyutov, S. S.; Yoshida, Y.; Morino, I.; Inoue, M.; Nakatsuru, T.; Uchino, O.; Mabuchi, K.</p> <p>2016-12-01</p> <p>Satellite-based <span class="hlt">CO</span><span class="hlt">2</span> measurements have potential for improving our understanding global carbon cycle because of more spatiotemporal coverage than those from ground-based observations. Since the Greenhouse gases Observing Satellite (GOSAT) was launched in January 2009, it has been measuring the column-average dry <span class="hlt">air</span>-mole function of <span class="hlt">CO</span><span class="hlt">2</span> (XCO<span class="hlt">2</span>) from the space. To utilize the GOSAT XCO<span class="hlt">2</span> for better <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates, several challenges should be overcome. Systematic errors (biases) in XCO<span class="hlt">2</span> retrievals are a major factor which leads to large differences among inverted <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Temporally variable data coverage and density are also taken into account when interpreting the estimated surface <span class="hlt">fluxes</span>. In this study, we employ an atmospheric inverse model to investigate the impacts of retrievals biases and temporally varying global distribution of GOSAT XCO<span class="hlt">2</span> on surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates. Inversions are performed for 2009-2013, with several subsets of the 5-year record of GOSAT XCO<span class="hlt">2</span> (v<span class="hlt">2</span>.21) and its bias-corrected XCO<span class="hlt">2</span>. GOSAT XCO<span class="hlt">2</span> data consist of three types: H-gain for vegetated lands, M-gain for bright surfaces (desert areas), and sun-glint for ocean surface. The results show that the global spatial distributions of estimated <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> depend on the subset of XCO<span class="hlt">2</span> used. M-gain XCO<span class="hlt">2</span> results in unrealistically high <span class="hlt">CO</span><span class="hlt">2</span> emissions in and around the Middle East, including the neighboring ocean regions. On the other hand, M-gain XCO<span class="hlt">2</span> causes compensating unrealistic uptakes far beyond M-gain regions in low latitudes, also partially contributing on the summer uptake in Europe. The joint inversions with both surface measurements and GOSAT XCO<span class="hlt">2</span> data obtain larger <span class="hlt">flux</span> gradient between the northern extra-tropics and the tropics than the inversion with surface measurements only for the first <span class="hlt">2</span> years. Recently, these North-South gradients seem to be gradually reducing as the tropics become a weaker source or turn into a sink, while the net emission strength in East Asia is increasing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28944134','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28944134"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from Javanese mud volcanism.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Queißer, M; Burton, M R; Arzilli, F; Chiarugi, A; Marliyani, G I; Anggara, F; Harijoko, A</p> <p>2017-06-01</p> <p>Studying the quantity and origin of <span class="hlt">CO</span> <span class="hlt">2</span> emitted by back-arc mud volcanoes is critical to correctly model fluid-dynamical, thermodynamical, and geochemical processes that drive their activity and to constrain their role in the global geochemical carbon cycle. We measured <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> of the Bledug Kuwu mud volcano on the Kendeng Fold and thrust belt in the back arc of Central Java, Indonesia, using scanning remote sensing absorption spectroscopy. The data show that the expelled gas is rich in <span class="hlt">CO</span> <span class="hlt">2</span> with a volume fraction of at least 16 vol %. A lower limit <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> of 1.4 kg s -1 (117 t d -1 ) was determined, in line with the <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> from the Javanese mud volcano LUSI. Extrapolating these results to mud volcanism from the whole of Java suggests an order of magnitude total <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> of 3 kt d -1 , comparable with the expected back-arc efflux of magmatic <span class="hlt">CO</span> <span class="hlt">2</span> . After discussing geochemical, geological, and geophysical evidence we conclude that the source of <span class="hlt">CO</span> <span class="hlt">2</span> observed at Bledug Kuwu is likely a mixture of thermogenic, biogenic, and magmatic <span class="hlt">CO</span> <span class="hlt">2</span> , with faulting controlling potential pathways for magmatic fluids. This study further demonstrates the merit of man-portable active remote sensing instruments for probing natural gas releases, enabling bottom-up quantification of <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRB..122.4191Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRB..122.4191Q"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from Javanese mud volcanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Queißer, M.; Burton, M. R.; Arzilli, F.; Chiarugi, A.; Marliyani, G. I.; Anggara, F.; Harijoko, A.</p> <p>2017-06-01</p> <p>Studying the quantity and origin of <span class="hlt">CO</span><span class="hlt">2</span> emitted by back-arc mud volcanoes is critical to correctly model fluid-dynamical, thermodynamical, and geochemical processes that drive their activity and to constrain their role in the global geochemical carbon cycle. We measured <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of the Bledug Kuwu mud volcano on the Kendeng Fold and thrust belt in the back arc of Central Java, Indonesia, using scanning remote sensing absorption spectroscopy. The data show that the expelled gas is rich in <span class="hlt">CO</span><span class="hlt">2</span> with a volume fraction of at least 16 vol %. A lower limit <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 1.4 kg s-1 (117 t d-1) was determined, in line with the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from the Javanese mud volcano LUSI. Extrapolating these results to mud volcanism from the whole of Java suggests an order of magnitude total <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 3 kt d-1, comparable with the expected back-arc efflux of magmatic <span class="hlt">CO</span><span class="hlt">2</span>. After discussing geochemical, geological, and geophysical evidence we conclude that the source of <span class="hlt">CO</span><span class="hlt">2</span> observed at Bledug Kuwu is likely a mixture of thermogenic, biogenic, and magmatic <span class="hlt">CO</span><span class="hlt">2</span>, with faulting controlling potential pathways for magmatic fluids. This study further demonstrates the merit of man-portable active remote sensing instruments for probing natural gas releases, enabling bottom-up quantification of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_4 --> <div id="page_5" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="81"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5586201','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5586201"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from Javanese mud volcanism</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Burton, M. R.; Arzilli, F.; Chiarugi, A.; Marliyani, G. I.; Anggara, F.; Harijoko, A.</p> <p>2017-01-01</p> <p>Abstract Studying the quantity and origin of <span class="hlt">CO</span><span class="hlt">2</span> emitted by back‐arc mud volcanoes is critical to correctly model fluid‐dynamical, thermodynamical, and geochemical processes that drive their activity and to constrain their role in the global geochemical carbon cycle. We measured <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of the Bledug Kuwu mud volcano on the Kendeng Fold and thrust belt in the back arc of Central Java, Indonesia, using scanning remote sensing absorption spectroscopy. The data show that the expelled gas is rich in <span class="hlt">CO</span><span class="hlt">2</span> with a volume fraction of at least 16 vol %. A lower limit <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 1.4 kg s−1 (117 t d−1) was determined, in line with the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from the Javanese mud volcano LUSI. Extrapolating these results to mud volcanism from the whole of Java suggests an order of magnitude total <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 3 kt d−1, comparable with the expected back‐arc efflux of magmatic <span class="hlt">CO</span><span class="hlt">2</span>. After discussing geochemical, geological, and geophysical evidence we conclude that the source of <span class="hlt">CO</span><span class="hlt">2</span> observed at Bledug Kuwu is likely a mixture of thermogenic, biogenic, and magmatic <span class="hlt">CO</span><span class="hlt">2</span>, with faulting controlling potential pathways for magmatic fluids. This study further demonstrates the merit of man‐portable active remote sensing instruments for probing natural gas releases, enabling bottom‐up quantification of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. PMID:28944134</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910070168&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DCO2%2BH2O','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910070168&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DCO2%2BH2O"><span>Studies of proton irradiated H<span class="hlt">2</span>O + <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O + <span class="hlt">CO</span> <span class="hlt">ices</span> and analysis of synthesized molecules</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moore, M. H.; Khanna, R.; Donn, B.</p> <p>1991-01-01</p> <p>Infrared spectra of H<span class="hlt">2</span>O + <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O + <span class="hlt">CO</span> <span class="hlt">ices</span> before and after proton irradiation showed that a major reaction in both mixtures was the interconversion of <span class="hlt">CO</span><span class="hlt">2</span> yields <span class="hlt">CO</span>. Radiation synthesized organic compounds such as carbonic acid were identified in the H<span class="hlt">2</span>O + <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. Different chemical pathways dominate in the H<span class="hlt">2</span>O + <span class="hlt">CO</span> <span class="hlt">ice</span> in which formaldehyde, methanol, ethanol, and methane were identified. Sublimed material was also analyzed using a mass spectrometer. Implications of these results are discussed in reference to comets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920004375','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920004375"><span>Quantification of UV stimulated <span class="hlt">ice</span> chemistry: <span class="hlt">CO</span> and <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anicich, V. G.; Arakelian, T.; Hanner, M. S.</p> <p>1991-01-01</p> <p>Recent laboratory experiments are presented that show that during photolysis of the pure <span class="hlt">ices</span> there is evidence of the interconversion of <span class="hlt">CO</span> to <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span><span class="hlt">2</span> to <span class="hlt">CO</span> using Lyman alpha (1216A) radiation. In addition, there is a substantial amount of another substance being produced. This substance is evident by its infrared absorption peak at 2235 cm(-1). It is believed that this new peak is due to carbon suboxide, C3O<span class="hlt">2</span>. <span class="hlt">CO</span> and <span class="hlt">CO</span><span class="hlt">2</span> have already been detected in comets, and C3O<span class="hlt">2</span> has been suggested as a cometary from radiation of <span class="hlt">CO</span>. Comparisons are made between our results at 1215A and proton radiation experiments and radiation at other wavelengths. The suggestion is that the processing of <span class="hlt">ices</span> is energy dependent, i.e., dependent on the type of radiation. Several difficult problems have to be solved before these radiation conversions can be quantified. The steps that we are taking to quantify the kinetics are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ECSS..166...13L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ECSS..166...13L"><span>Net ecosystem production, calcification and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> on a reef flat in Northeastern Brazil</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Longhini, Cybelle M.; Souza, Marcelo F. L.; Silva, Ananda M.</p> <p>2015-12-01</p> <p>The carbon cycle in coral reefs is usually dominated by the organic carbon metabolism and precipitation-dissolution of Ca<span class="hlt">CO</span>3, processes that control the <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>) in seawater and the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> through the <span class="hlt">air</span>-sea interface. In order to characterize these processes and the carbonate system, four sampling surveys were conducted at the reef flat of Coroa Vermelha during low tide (exposed flat). Net ecosystem production (NEP), net precipitation-dissolution of Ca<span class="hlt">CO</span>3 (G) and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> across the <span class="hlt">air</span>-water interface were calculated. The reef presented net autotrophy and calcification at daytime low tide. The NEP ranged from -8.7 to 31.6 mmol C m-<span class="hlt">2</span> h-1 and calcification from -13.1 to 26.0 mmol C m-<span class="hlt">2</span> h-1. The highest calcification rates occurred in August 2007, coinciding with the greater NEP rates. The daytime <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> varied from -9.7 to 22.6 μmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> h-1, but reached up to 13,900 μmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> h-1 during nighttime. Carbon dioxide influx to seawater was predominant in the reef flat during low tide. The regions adjacent to the reef showed a supersaturation of <span class="hlt">CO</span><span class="hlt">2</span>, acting as a source of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere (from -22.8 to -<span class="hlt">2</span>.6 mol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> h-1) in the reef flat during ebbing tide. Nighttime gas release to the atmosphere indicates a net <span class="hlt">CO</span><span class="hlt">2</span> release from the Coroa Vermelha reef flat within 24 h, and that these <span class="hlt">fluxes</span> can be important to carbon budget in coral reefs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24406807','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24406807"><span>Porosity and thermal collapse measurements of H<span class="hlt">2</span>O, CH3OH, <span class="hlt">CO</span><span class="hlt">2</span>, and H<span class="hlt">2</span>O:<span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Isokoski, K; Bossa, J-B; Triemstra, T; Linnartz, H</p> <p>2014-02-28</p> <p>The majority of astronomical and laboratory based studies of interstellar <span class="hlt">ices</span> have been focusing on <span class="hlt">ice</span> constituents. <span class="hlt">Ice</span> structure is a much less studied topic. Particularly the amount of porosity is an ongoing point of discussion. A porous <span class="hlt">ice</span> offers more surface area than a compact <span class="hlt">ice</span>, for reactions that are fully surface driven. In this paper we discuss the amount of compaction for four different <span class="hlt">ices</span>--H<span class="hlt">2</span>O, CH3OH, <span class="hlt">CO</span><span class="hlt">2</span> and mixed H<span class="hlt">2</span>O : <span class="hlt">CO</span><span class="hlt">2</span> = <span class="hlt">2</span> : 1--upon heating over an astronomically relevant temperature regime. Laser interference and Fourier transform infrared spectroscopy are used to confirm that for amorphous solid water the full signal loss of dangling OH bonds is not a proof for full compaction. These data are compared with the first compaction results for pure CH3OH, pure <span class="hlt">CO</span><span class="hlt">2</span> and mixed H<span class="hlt">2</span>O : <span class="hlt">CO</span><span class="hlt">2</span> = <span class="hlt">2</span> : 1 <span class="hlt">ice</span>. Here we find that thermal segregation benefits from a higher degree of porosity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A53L3379W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A53L3379W"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> and Concentrations in a Residential Area in the Southern Hemisphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weissert, L. F.; Salmond, J. A.; Turnbull, J. C.; Schwendenmann, L.</p> <p>2014-12-01</p> <p>While cities are generally major sources of anthropogenic carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) emissions, recent research has shown that parts of urban areas may also act as <span class="hlt">CO</span><span class="hlt">2</span> sinks due to <span class="hlt">CO</span><span class="hlt">2</span> uptake by vegetation. However, currently available results are related to a large degree of uncertainty due to the limitations of the applied methods and the limited number of studies available from urban areas, particularly from the southern hemisphere. In this study, we explore the potential of eddy covariance and tracer measurements (13C and 14C isotopes of <span class="hlt">CO</span><span class="hlt">2</span>) to quantify and partition <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations in a residential urban area in Auckland, New Zealand. Based on preliminary results from autumn and winter (March to July 2014) the residential area is a small source of <span class="hlt">CO</span><span class="hlt">2</span> (0.11 mol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> day-1). <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations follow a distinct diurnal cycle with a morning peak between 7:00 and 9:00 (max: 0.25 mol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> day-1/412 ppm) and midday low with negative <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (min: -0.17 mol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> day-1/392 ppm) between 10:00 and 15:00 local time, likely due to photosynthetic <span class="hlt">CO</span><span class="hlt">2</span> uptake by local vegetation. Soil <span class="hlt">CO</span><span class="hlt">2</span> efflux may explain that <span class="hlt">CO</span><span class="hlt">2</span> concentrations increase and remain high (401 ppm) throughout the night. Mean diurnal winter δ13C values are in anti-phase with <span class="hlt">CO</span><span class="hlt">2</span> concentrations and vary between -9.0 - -9.7‰. The depletion of δ13C compared to clean atmospheric <span class="hlt">air</span> (-8.<span class="hlt">2</span>‰) is likely a result of local <span class="hlt">CO</span><span class="hlt">2</span> sources dominated by gasoline combustion (appr. 60%) during daytime. A sector analysis (based on prevailing wind) of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations indicates lower <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations from the vegetation-dominated sector, further demonstrating the influence of vegetation on local <span class="hlt">CO</span><span class="hlt">2</span> concentrations. These results provide an insight into the temporal and spatial variability <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>/concentrations and potential <span class="hlt">CO</span><span class="hlt">2</span> sinks and sources from a city in the southern hemisphere and add valuable information to the global database of urban <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...1326529C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...1326529C"><span>Atmospheric inversion of the surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> with 13<span class="hlt">CO</span><span class="hlt">2</span> constraint</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, J. M.; Mo, G.; Deng, F.</p> <p>2013-10-01</p> <p>Observations of 13<span class="hlt">CO</span><span class="hlt">2</span> at 73 sites compiled in the GLOBALVIEW database are used for an additional constraint in a global atmospheric inversion of the surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> using <span class="hlt">CO</span><span class="hlt">2</span> observations at 210 sites for the 2002-2004 period for 39 land regions and 11 ocean regions. This constraint is implemented using the 13<span class="hlt">CO</span><span class="hlt">2</span>/<span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> ratio modeled with a terrestrial ecosystem model and an ocean model. These models simulate 13<span class="hlt">CO</span><span class="hlt">2</span> discrimination rates of terrestrial photosynthesis and respiration and ocean-atmosphere diffusion processes. In both models, the 13<span class="hlt">CO</span><span class="hlt">2</span> disequilibrium between <span class="hlt">fluxes</span> to and from the atmosphere is considered due to the historical change in atmospheric 13<span class="hlt">CO</span><span class="hlt">2</span> concentration. For the 2002-2004 period, the 13<span class="hlt">CO</span><span class="hlt">2</span> constraint on the inversion increases the total land carbon sink from 3.40 to 3.70 Pg C yr-1 and decreases the total oceanic carbon sink from 1.48 to 1.12 Pg C yr-1. The largest changes occur in tropical areas: a considerable decrease in the carbon source in the Amazon forest, and this decrease is mostly compensated by increases in the ocean region immediately west of the Amazon and the southeast Asian land region. Our further investigation through different treatments of the 13<span class="hlt">CO</span><span class="hlt">2</span>/<span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> ratio used in the inversion suggests that variable spatial distributions of the 13<span class="hlt">CO</span><span class="hlt">2</span> isotopic discrimination rate simulated by the models over land and ocean have considerable impacts on the spatial distribution of the inverted <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> over land and the inversion results are not sensitive to errors in the estimated disequilibria over land and ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017772','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017772"><span>Detection and monitoring of H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds on Mars</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Bell, J.F.; Calvin, W.M.; Ockert-Bell, M. E.; Crisp, D.; Pollack, James B.; Spencer, J.</p> <p>1996-01-01</p> <p>We have developed an observational scheme for the detection and discrimination of Mars atmospheric H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> clouds using ground-based instruments in the near infrared. We report the results of our cloud detection and characterization study using Mars near IR images obtained during the 1990 and 1993 oppositions. We focused on specific wavelengths that have the potential, based on previous laboratory studies of H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span>, of yielding the greatest degree of cloud detectability and compositional discriminability. We have detected and mapped absorption features at some of these wavelengths in both the northern and southern polar regions of Mars. Compositional information on the nature of these absorption features was derived from comparisons with laboratory <span class="hlt">ice</span> spectra and with a simplified radiative transfer model of a <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cloud overlying a bright surface. Our results indicate that both H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span> can be detected and distinguished in the polar hood clouds. The region near 3.00 ??m is most useful for the detection of water <span class="hlt">ice</span> clouds because there is a strong H<span class="hlt">2</span>O <span class="hlt">ice</span> absorption at this wavelength but only a weak <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> band. The region near 3.33 ??m is most useful for the detection of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds because there is a strong, relatively narrow <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> band at this wavelength but only broad "continuum" H<span class="hlt">2</span>O <span class="hlt">ice</span> absorption. Weaker features near <span class="hlt">2</span>.30 ??m could arise from <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at coarse grain sizes, or surface/dust minerals. Narrow features near <span class="hlt">2</span>.00 ??m, which could potentially be very diagnostic of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds, suffer from contamination by Mars atmospheric <span class="hlt">CO</span><span class="hlt">2</span> absorptions and are difficult to interpret because of the rather poor knowledge of surface elevation at high latitudes. These results indicate that future ground-based, Earth-orbital, and spacecraft studies over a more extended span of the seasonal cycle should yield substantial information on the style and timing of volatile transport on Mars, as well as a more detailed understanding of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7073379-reduction-air-pollutant-concentrations-indoor-ice-skating-rink','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7073379-reduction-air-pollutant-concentrations-indoor-ice-skating-rink"><span>Reduction of <span class="hlt">air</span> pollutant concentrations in an indoor <span class="hlt">ice</span>-skating rink</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lee, K.; Yanagisawa, Yukio; Spengler, J.D.</p> <p>1994-01-01</p> <p>High carbon monoxide and nitrogen dioxide concentrations were measured in an indoor <span class="hlt">ice</span>-skating rink with fuel-powered <span class="hlt">ice</span>-resurfacing equipment. In 22% to 33% of the measurements over 90-min segments, <span class="hlt">CO</span> concentrations exceeded 20 [mu]L/L as a 90-min average in the absence of rink ventilation. Average NO[sub <span class="hlt">2</span>] concentrations over 14 h were higher than 600 nL/L. Reduction of <span class="hlt">air</span> pollutant concentrations in the <span class="hlt">ice</span>-skating rink is necessary to prevent <span class="hlt">air</span>-pollutant-exposure-related health incidents. Various methods for reducing <span class="hlt">air</span> pollutants in an <span class="hlt">ice</span>-skating rink were evaluated by simultaneously measuring <span class="hlt">CO</span> and NO[sub <span class="hlt">2</span>] concentrations. Single pollution reduction attempts, such as extension of themore » exhaust pipe, reduction in the number of resurfacer operations, or use of an <span class="hlt">air</span> recirculation system, did not significantly reduce <span class="hlt">air</span> pollutant concentrations in the rink. Full operation of the mechanical ventilation system combined with reduced resurfacer operation was required to keep the <span class="hlt">air</span> pollutant levels in the skating rink below the recommended guidelines. This investigation showed that management of clean <span class="hlt">air</span> quality in an <span class="hlt">ice</span>-skating rink is practically difficult as long as fuel-powered resurfacing equipment is used. 16 refs., 3 figs., 5 tabs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940007582&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DCO2%2BH2O','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940007582&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DCO2%2BH2O"><span>An observational search for <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds on Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bell, James F., III; Calvin, Wendy M.; Pollack, James B.; Crisp, David</p> <p>1993-01-01</p> <p><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds were first directly identified on Mars by the Mariner 6 and 7 infrared spectrometer limb scans. These observations provided support for early theoretical modeling efforts of <span class="hlt">CO</span><span class="hlt">2</span> condensation. Mariner 9 IRIS temperature profiles of north polar hood clouds were interpreted as indicating that these clouds were composed of H<span class="hlt">2</span>O <span class="hlt">ice</span> at lower latitudes and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at higher latitudes. The role of <span class="hlt">CO</span><span class="hlt">2</span> condensation on Mars has recently received increased attention because (1) Kasting's model results indicated that <span class="hlt">CO</span><span class="hlt">2</span> cloud condensation limits the magnitude of the proposed early Mars <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O greenhouse, and (<span class="hlt">2</span>) Pollack el al.'s GCM results indicated that the formation of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds is favorable at all polar latitudes during the fall and winter seasons. These latter authors have shown that <span class="hlt">CO</span><span class="hlt">2</span> clouds play an important role in the polar energy balance, as the amount of <span class="hlt">CO</span><span class="hlt">2</span> contained in the polar caps is constrained by a balance between latent heat release, heat advected from lower latitudes, and thermal emission to space. The polar hood clouds reduce the amount of <span class="hlt">CO</span><span class="hlt">2</span> condensation on the polar caps because they reduce the net emission to space. There have been many extensive laboratory spectroscopic studies of H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span> and frosts. In this study, we use results from these and other sources to search for the occurrence of diagnostic <span class="hlt">CO</span><span class="hlt">2</span> (and H<span class="hlt">2</span>O) <span class="hlt">ice</span> and/or frost absorption features in ground based near-infrared imaging spectroscopic data of Mars. Our primary goals are (1) to try to confirm the previous direct observations of <span class="hlt">CO</span><span class="hlt">2</span> clouds on Mars; (<span class="hlt">2</span>) to determine the spatial extent, temporal variability, and composition (H<span class="hlt">2</span>O/<span class="hlt">CO</span><span class="hlt">2</span> ratio) of any clouds detected; and (3) through radiative transfer modeling, to try to determine the mean particle size and optical depth of polar hood clouds, thus, assessing their role in the polar heat budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JVGR..207..130C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JVGR..207..130C"><span>Diffuse <span class="hlt">CO</span> <span class="hlt">2</span> soil degassing and <span class="hlt">CO</span> <span class="hlt">2</span> and H <span class="hlt">2</span>S concentrations in <span class="hlt">air</span> and related hazards at Vulcano Island (Aeolian arc, Italy)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carapezza, M. L.; Barberi, F.; Ranaldi, M.; Ricci, T.; Tarchini, L.; Barrancos, J.; Fischer, C.; Perez, N.; Weber, K.; Di Piazza, A.; Gattuso, A.</p> <p>2011-10-01</p> <p>La Fossa crater on Vulcano Island is quiescent since 1890. Periodically it undergoes "crises" characterized by marked increase of temperature (T), gas output and concentration of magmatic components in the crater fumaroles (T may exceed 600 °C). During these crises, which so far did not lead to any eruptive reactivation, the diffuse <span class="hlt">CO</span> <span class="hlt">2</span> soil degassing also increases and in December 2005 an anomalous <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> of 1350 tons/day was estimated by 1588 measurements over a surface of 1.66 km <span class="hlt">2</span> extending from La Fossa crater to the inhabited zone of Vulcano Porto. The crater area and two other anomalously degassing sites (Levante Beach and Palizzi) have been periodically investigated from December 2004 to August 2010 for diffuse <span class="hlt">CO</span> <span class="hlt">2</span> soil <span class="hlt">flux</span>. They show a marked variation with time of the degassing rate, with synchronous maxima in December 2005. Carbon dioxide soil <span class="hlt">flux</span> and environmental parameters have been also continuously monitored for over one year by an automatic station at Vulcano Porto. In order to assess the hazard of the endogenous gas emissions, <span class="hlt">CO</span> <span class="hlt">2</span> and H <span class="hlt">2</span>S <span class="hlt">air</span> concentrations have been measured by Tunable Diode Laser profiles near the fumaroles of the crater rim and of the Levante Beach area, where also the viscous gas <span class="hlt">flux</span> has been estimated. In addition, <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">air</span> concentration has been measured both indoor and outdoor in an inhabited sector of Vulcano Porto. Results show that in some sites usually frequented by tourists there is a dangerous H <span class="hlt">2</span>S <span class="hlt">air</span> concentration and <span class="hlt">CO</span> <span class="hlt">2</span> exceeds the hazardous thresholds in some Vulcano houses. These zones should be immediately monitored for gas hazard should a new crisis arise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990115745&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DCO2%2BH2O','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990115745&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DCO2%2BH2O"><span>Laboratory IR Detection of H<span class="hlt">2</span>O, <span class="hlt">CO</span><span class="hlt">2</span> in Ion-Irradiated <span class="hlt">Ices</span> Relevant to Europa</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moore, Marla H.; Hudson, R. L.</p> <p>1999-01-01</p> <p>Hydrogen peroxide has been identified on Europa (Carlson et al. 1999) based in part on the 3.50 micron absorption feature observed in Galileo NIMS spectra. The observed feature was fitted with laboratory reflectance spectra of H<span class="hlt">2</span>O + H<span class="hlt">2</span>O<span class="hlt">2</span>. Since condensed phase molecules on Europa (H<span class="hlt">2</span>O, <span class="hlt">CO</span><span class="hlt">2</span>, SO<span class="hlt">2</span>, and H<span class="hlt">2</span>O<span class="hlt">2</span>) are bombarded with a significant <span class="hlt">flux</span> of energetic particles (H(+), O(n+), S(n+) and e-), we examined the proton irradiation of H<span class="hlt">2</span>O at 80 K and the conditions for the IR detection of H<span class="hlt">2</span>O<span class="hlt">2</span> near 3.5 microns. Contrary to expectations, H<span class="hlt">2</span>O<span class="hlt">2</span> was not detected if pure H<span class="hlt">2</span>O <span class="hlt">ice</span> was irradiated at 80 K. This was an unexpected result since, H<span class="hlt">2</span>O<span class="hlt">2</span> was detected if pure H<span class="hlt">2</span>O was irradiated at 18 K. We find, however, that if H<span class="hlt">2</span>O <span class="hlt">ice</span> contains either O<span class="hlt">2</span> or <span class="hlt">CO</span><span class="hlt">2</span> then H<span class="hlt">2</span>O<span class="hlt">2</span> is detected after irradiation at 80 K (Moore and Hudson, 1999). The source of O<span class="hlt">2</span> for the H<span class="hlt">2</span>O <span class="hlt">ice</span> on Europa could come from surface interactions with the tenuous oxygen atmosphere, or from the bombardment of the surface by O(n+).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V31E..03C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V31E..03C"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from diffuse degassing in Italy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cardellini, C.; Chiodini, G.; Frondini, F.; Caliro, S.</p> <p>2016-12-01</p> <p>Central and southern Italy are affected by an intense process of <span class="hlt">CO</span><span class="hlt">2</span> Earth degassing from both active volcanoes, and tectonically active areas. Regional scale studies, based on C mass balance of groundwater of regional aquifers in not volcanically active areas, highlighted the presence of two large <span class="hlt">CO</span><span class="hlt">2</span> degassing structures that, for magnitude and the geochemical-isotopic features, were related to a regional process of mantle degassing. Quantitative estimates provided a <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 9 Mt/y for the region (62000 km<span class="hlt">2</span>). Besides the magnitude of the process, a strong link between the deep <span class="hlt">CO</span><span class="hlt">2</span> degassing and the seismicity of the region and a strict correlation between migration of deep <span class="hlt">CO</span><span class="hlt">2</span>-rich fluids and the heat <span class="hlt">flux</span> have been highlighted. In addition, the region is also characterised by the presence of many cold gas emissions where deeply derived <span class="hlt">CO</span><span class="hlt">2</span> is released by vents and soil diffuse degassing areas. Both direct <span class="hlt">CO</span><span class="hlt">2</span> expulsion at the surface and C-rich groundwater are different manifestations of the same process, in fact, the deeply produced gas can be dissolved by groundwater or emitted directly to the atmosphere depending on the gas <span class="hlt">flux</span> rate, and the geological-structural and hydrogeological settings. Quantitative estimations of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are available only for a limited number ( 30) of the about 270 catalogued gas manifestations allowing an estimations of a <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 1.4 Mt/y. Summing the two estimates the non-volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from the region results globally relevant, being from <span class="hlt">2</span> to 10% of the estimated present-day global <span class="hlt">CO</span><span class="hlt">2</span> discharge from subaerial volcanoes. Large amounts of <span class="hlt">CO</span><span class="hlt">2</span> is also discharged by soil diffuse degassing in volcanic-hydrothermal systems. Specific surveys at Solfatara of Pozzuoli (Campi Flegrei Caldera) pointed out the relevance of this process. <span class="hlt">CO</span><span class="hlt">2</span> diffuse degassing at Solfatara, measured since 1998 shows a persistent <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of 1300 t/d (± 390 t/d), a <span class="hlt">flux</span> comparable to an erupting volcano. The quantification of diffuse <span class="hlt">CO</span><span class="hlt">2</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.1180C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.1180C"><span>On which timescales do gas transfer velocities control North Atlantic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> variability?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Couldrey, Matthew; Oliver, Kevin; Yool, Andrew; Halloran, Paul; Achterberg, Eric</p> <p>2016-04-01</p> <p>The North Atlantic is an important basin for the global ocean's uptake of anthropogenic and natural carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), but the mechanisms controlling this carbon <span class="hlt">flux</span> are not fully understood. The <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>, F, is the product of a gas transfer velocity, k, the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span>concentration gradient, Δp<span class="hlt">CO</span><span class="hlt">2</span>, and the temperature and salinity-dependent solubility coefficient, α. k is difficult to constrain, representing the dominant uncertainty in F on short (instantaneous to interannual) timescales. Previous work shows that in the North Atlantic, Δp<span class="hlt">CO</span><span class="hlt">2</span>and k both contribute significantly to interannual F variability, but that k is unimportant for multidecadal variability. On some timescale between interannual and multidecadal, gas transfer velocity variability and its associated uncertainty become negligible. Here, we quantify this critical timescale for the first time. Using an ocean model, we determine the importance of k, Δp<span class="hlt">CO</span><span class="hlt">2</span>and α on a range of timescales. On interannual and shorter timescales, both Δp<span class="hlt">CO</span><span class="hlt">2</span>and k are important controls on F. In contrast, pentadal to multidecadal North Atlantic <span class="hlt">flux</span> variability is driven almost entirely by Δp<span class="hlt">CO</span><span class="hlt">2</span>; k contributes less than 25%. Finally, we explore how accurately one can estimate North Atlantic F without a knowledge of non-seasonal k variability, finding it possible for interannual and longer timescales. These findings suggest that continued efforts to better constrain gas transfer velocities are necessary to quantify interannual variability in the North Atlantic carbon sink. However, uncertainty in k variability is unlikely to limit the accuracy of estimates of longer term <span class="hlt">flux</span> variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GBioC..30..787C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GBioC..30..787C"><span>On which timescales do gas transfer velocities control North Atlantic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> variability?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Couldrey, Matthew P.; Oliver, Kevin I. C.; Yool, Andrew; Halloran, Paul R.; Achterberg, Eric P.</p> <p>2016-05-01</p> <p>The North Atlantic is an important basin for the global ocean's uptake of anthropogenic and natural carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), but the mechanisms controlling this carbon <span class="hlt">flux</span> are not fully understood. The <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>, F, is the product of a gas transfer velocity, k, the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> concentration gradient, Δp<span class="hlt">CO</span><span class="hlt">2</span>, and the temperature- and salinity-dependent solubility coefficient, α. k is difficult to constrain, representing the dominant uncertainty in F on short (instantaneous to interannual) timescales. Previous work shows that in the North Atlantic, Δp<span class="hlt">CO</span><span class="hlt">2</span> and k both contribute significantly to interannual F variability but that k is unimportant for multidecadal variability. On some timescale between interannual and multidecadal, gas transfer velocity variability and its associated uncertainty become negligible. Here we quantify this critical timescale for the first time. Using an ocean model, we determine the importance of k, Δp<span class="hlt">CO</span><span class="hlt">2</span>, and α on a range of timescales. On interannual and shorter timescales, both Δp<span class="hlt">CO</span><span class="hlt">2</span> and k are important controls on F. In contrast, pentadal to multidecadal North Atlantic <span class="hlt">flux</span> variability is driven almost entirely by Δp<span class="hlt">CO</span><span class="hlt">2</span>; k contributes less than 25%. Finally, we explore how accurately one can estimate North Atlantic F without a knowledge of nonseasonal k variability, finding it possible for interannual and longer timescales. These findings suggest that continued efforts to better constrain gas transfer velocities are necessary to quantify interannual variability in the North Atlantic carbon sink. However, uncertainty in k variability is unlikely to limit the accuracy of estimates of longer-term <span class="hlt">flux</span> variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSAH23A..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSAH23A..06C"><span>On which timescales do gas transfer velocities control North Atlantic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> variability?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Couldrey, M.; Oliver, K. I. C.; Yool, A.; Halloran, P. R.; Achterberg, E. P.</p> <p>2016-02-01</p> <p>The North Atlantic is an important basin for the global ocean's uptake of anthropogenic and natural carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), but the mechanisms controlling this carbon <span class="hlt">flux</span> are not fully understood. The <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>, F, is the product of a gas transfer velocity, k, the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> concentration gradient, Δp<span class="hlt">CO</span><span class="hlt">2</span>, and the temperature and salinity-dependent solubility coefficient, α. k is difficult to constrain, representing the dominant uncertainty in F on short (instantaneous to interannual) timescales. Previous work shows that in the North Atlantic, Δp<span class="hlt">CO</span><span class="hlt">2</span> and k both contribute significantly to interannual F variability, but that k is unimportant for multidecadal variability. On some timescale between interannual and multidecadal, gas transfer velocity variability and its associated uncertainty become negligible. Here, we quantify this critical timescale for the first time. Using an ocean model, we determine the importance of k, Δp<span class="hlt">CO</span><span class="hlt">2</span> and α on a range of timescales. On interannual and shorter timescales, both Δp<span class="hlt">CO</span><span class="hlt">2</span> and k are important controls on F. In contrast, pentadal to multidecadal North Atlantic <span class="hlt">flux</span> variability is driven almost entirely by Δp<span class="hlt">CO</span><span class="hlt">2</span>; k contributes less than 25%. Finally, we explore how accurately one can estimate North Atlantic F without a knowledge of non-seasonal k variability, finding it possible for interannual and longer timescales. These findings suggest that continued efforts to better constrain gas transfer velocities are necessary to quantify interannual variability in the North Atlantic carbon sink. However, uncertainty in k variability is unlikely to limit the accuracy of estimates of longer term <span class="hlt">flux</span> variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.8661B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.8661B"><span>Oxygen in the Southern Ocean From Argo Floats: Determination of Processes Driving <span class="hlt">Air</span>-Sea <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bushinsky, Seth M.; Gray, Alison R.; Johnson, Kenneth S.; Sarmiento, Jorge L.</p> <p>2017-11-01</p> <p>The Southern Ocean is of outsized significance to the global oxygen and carbon cycles with relatively poor measurement coverage due to harsh winters and seasonal <span class="hlt">ice</span> cover. In this study, we use recent advances in the parameterization of <span class="hlt">air</span>-sea oxygen <span class="hlt">fluxes</span> to analyze 9 years of oxygen data from a recalibrated Argo oxygen data set and from <span class="hlt">air</span>-calibrated oxygen floats deployed as part of the Southern Ocean Carbon and Climate Observations and Modeling (SOCCOM) project. From this combined data set of 150 floats, we find a total Southern Ocean oxygen sink of -183 ± 80 Tmol yr-1 (positive to the atmosphere), greater than prior estimates. The uptake occurs primarily in the Polar-Frontal Antarctic Zone (PAZ, -94 ± 30 Tmol O<span class="hlt">2</span> yr-1) and Seasonal <span class="hlt">Ice</span> Zone (SIZ, -111 ± 9.3 Tmol O<span class="hlt">2</span> yr-1). This <span class="hlt">flux</span> is driven by wintertime ventilation, with a large portion of the <span class="hlt">flux</span> in the SIZ passing through regions with fractional sea <span class="hlt">ice</span>. The Subtropical Zone (STZ) is seasonally driven by thermal <span class="hlt">fluxes</span> and exhibits a net outgassing of 47 ± 29 Tmol O<span class="hlt">2</span> yr-1 that is likely driven by biological production. The Subantarctic Zone (SAZ) uptake is -25 ± 12 Tmol O<span class="hlt">2</span> yr-1. Total oxygen <span class="hlt">fluxes</span> were separated into a thermal and nonthermal component. The nonthermal <span class="hlt">flux</span> is correlated with net primary production and mixed layer depth in the STZ, SAZ, and PAZ, but not in the SIZ where seasonal sea <span class="hlt">ice</span> slows the <span class="hlt">air</span>-sea gas <span class="hlt">flux</span> response to the entrainment of deep, low-oxygen waters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1351785','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1351785"><span>Nonlinear <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> response to 7 years of experimentally induced permafrost thaw</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Mauritz, Marguerite; Bracho, Rosvel; Celis, Gerardo</p> <p></p> <p>Rapid Arctic warming is expected to increase global greenhouse gas concentrations as permafrost thaw exposes immense stores of frozen carbon (C) to microbial decomposition. Permafrost thaw also stimulates plant growth, which could offset C loss. Using data from 7 years of experimental <span class="hlt">Air</span> and Soil warming in moist acidic tundra, we show that Soil warming had a much stronger effect on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> than <span class="hlt">Air</span> warming. Soil warming caused rapid permafrost thaw and increased ecosystem respiration (R eco), gross primary productivity (GPP), and net summer <span class="hlt">CO</span> <span class="hlt">2</span> storage (NEE). Over 7 years R eco, GPP, and NEE also increasedmore » in Control (i.e., ambient plots), but this change could be explained by slow thaw in Control areas. In the initial stages of thaw, R eco, GPP, and NEE increased linearly with thaw across all treatments, despite different rates of thaw. As thaw in Soil warming continued to increase linearly, ground surface subsidence created saturated microsites and suppressed R eco, GPP, and NEE. However R eco and GPP remained high in areas with large Eriophorum vaginatum biomass. In general NEE increased with thaw, but was more strongly correlated with plant biomass than thaw, indicating that higher R eco in deeply thawed areas during summer months was balanced by GPP. Summer <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> across treatments fit a single quadratic relationship that captured the functional response of <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> to thaw, water table depth, and plant biomass. These results demonstrate the importance of indirect thaw effects on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span>: plant growth and water table dynamics. Nonsummer R eco models estimated that the area was an annual <span class="hlt">CO</span> <span class="hlt">2</span> source during all years of observation. As a result, nonsummer <span class="hlt">CO</span> <span class="hlt">2</span> loss in warmer, more deeply thawed soils exceeded the increases in summer GPP, and thawed tundra was a net annual <span class="hlt">CO</span> <span class="hlt">2</span> source.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1351785-nonlinear-co2-flux-response-nbsp-years-experimentally-induced-permafrost-thaw','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1351785-nonlinear-co2-flux-response-nbsp-years-experimentally-induced-permafrost-thaw"><span>Nonlinear <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> response to 7 years of experimentally induced permafrost thaw</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Mauritz, Marguerite; Bracho, Rosvel; Celis, Gerardo; ...</p> <p>2017-02-16</p> <p>Rapid Arctic warming is expected to increase global greenhouse gas concentrations as permafrost thaw exposes immense stores of frozen carbon (C) to microbial decomposition. Permafrost thaw also stimulates plant growth, which could offset C loss. Using data from 7 years of experimental <span class="hlt">Air</span> and Soil warming in moist acidic tundra, we show that Soil warming had a much stronger effect on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> than <span class="hlt">Air</span> warming. Soil warming caused rapid permafrost thaw and increased ecosystem respiration (R eco), gross primary productivity (GPP), and net summer <span class="hlt">CO</span> <span class="hlt">2</span> storage (NEE). Over 7 years R eco, GPP, and NEE also increasedmore » in Control (i.e., ambient plots), but this change could be explained by slow thaw in Control areas. In the initial stages of thaw, R eco, GPP, and NEE increased linearly with thaw across all treatments, despite different rates of thaw. As thaw in Soil warming continued to increase linearly, ground surface subsidence created saturated microsites and suppressed R eco, GPP, and NEE. However R eco and GPP remained high in areas with large Eriophorum vaginatum biomass. In general NEE increased with thaw, but was more strongly correlated with plant biomass than thaw, indicating that higher R eco in deeply thawed areas during summer months was balanced by GPP. Summer <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> across treatments fit a single quadratic relationship that captured the functional response of <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> to thaw, water table depth, and plant biomass. These results demonstrate the importance of indirect thaw effects on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span>: plant growth and water table dynamics. Nonsummer R eco models estimated that the area was an annual <span class="hlt">CO</span> <span class="hlt">2</span> source during all years of observation. As a result, nonsummer <span class="hlt">CO</span> <span class="hlt">2</span> loss in warmer, more deeply thawed soils exceeded the increases in summer GPP, and thawed tundra was a net annual <span class="hlt">CO</span> <span class="hlt">2</span> source.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28208232','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28208232"><span>Nonlinear <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> response to 7 years of experimentally induced permafrost thaw.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mauritz, Marguerite; Bracho, Rosvel; Celis, Gerardo; Hutchings, Jack; Natali, Susan M; Pegoraro, Elaine; Salmon, Verity G; Schädel, Christina; Webb, Elizabeth E; Schuur, Edward A G</p> <p>2017-09-01</p> <p>Rapid Arctic warming is expected to increase global greenhouse gas concentrations as permafrost thaw exposes immense stores of frozen carbon (C) to microbial decomposition. Permafrost thaw also stimulates plant growth, which could offset C loss. Using data from 7 years of experimental <span class="hlt">Air</span> and Soil warming in moist acidic tundra, we show that Soil warming had a much stronger effect on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> than <span class="hlt">Air</span> warming. Soil warming caused rapid permafrost thaw and increased ecosystem respiration (R eco ), gross primary productivity (GPP), and net summer <span class="hlt">CO</span> <span class="hlt">2</span> storage (NEE). Over 7 years R eco , GPP, and NEE also increased in Control (i.e., ambient plots), but this change could be explained by slow thaw in Control areas. In the initial stages of thaw, R eco , GPP, and NEE increased linearly with thaw across all treatments, despite different rates of thaw. As thaw in Soil warming continued to increase linearly, ground surface subsidence created saturated microsites and suppressed R eco , GPP, and NEE. However R eco and GPP remained high in areas with large Eriophorum vaginatum biomass. In general NEE increased with thaw, but was more strongly correlated with plant biomass than thaw, indicating that higher R eco in deeply thawed areas during summer months was balanced by GPP. Summer <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> across treatments fit a single quadratic relationship that captured the functional response of <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> to thaw, water table depth, and plant biomass. These results demonstrate the importance of indirect thaw effects on <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span>: plant growth and water table dynamics. Nonsummer R eco models estimated that the area was an annual <span class="hlt">CO</span> <span class="hlt">2</span> source during all years of observation. Nonsummer <span class="hlt">CO</span> <span class="hlt">2</span> loss in warmer, more deeply thawed soils exceeded the increases in summer GPP, and thawed tundra was a net annual <span class="hlt">CO</span> <span class="hlt">2</span> source. © 2017 John Wiley & Sons Ltd.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC24A..04P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC24A..04P"><span>Spatial and Temporal Variability of Surface Energy <span class="hlt">Fluxes</span> During Autumn <span class="hlt">Ice</span> Advance: Observations and Model Validation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Persson, O. P. G.; Blomquist, B.; Grachev, A. A.; Guest, P. S.; Stammerjohn, S. E.; Solomon, A.; Cox, C. J.; Capotondi, A.; Fairall, C. W.; Intrieri, J. M.</p> <p>2016-12-01</p> <p>From Oct 4 to Nov 5, 2015, the Office of Naval Research - sponsored Sea State cruise in the Beaufort Sea with the new National Science Foundation R/V Sikuliaq obtained extensive in-situ and remote sensing observations of the lower troposphere, the advancing sea <span class="hlt">ice</span>, wave state, and upper ocean conditions. In addition, a coupled atmosphere, sea <span class="hlt">ice</span>, upper-ocean model, based on the RASM model, was run at NOAA/PSD in a hindcast mode for this same time period, providing a 10-day simulation of the atmosphere/<span class="hlt">ice</span>/ocean evolution. Surface energy <span class="hlt">fluxes</span> quantitatively represent the <span class="hlt">air-ice</span>, <span class="hlt">air</span>-ocean, and <span class="hlt">ice</span>-ocean interaction processes, determining the cooling (warming) rate of the upper ocean and the growth (melting) rate of sea <span class="hlt">ice</span>. These <span class="hlt">fluxes</span> also impact the stratification of the lower troposphere and the upper ocean. In this presentation, both direct and indirect measurements of the energy <span class="hlt">fluxes</span> during Sea State will be used to explore the spatial and temporal variability of these <span class="hlt">fluxes</span> and the impacts of this variability on the upper ocean, <span class="hlt">ice</span>, and lower atmosphere during the autumn <span class="hlt">ice</span> advance. Analyses have suggested that these <span class="hlt">fluxes</span> are impacted by atmospheric synoptic evolution, proximity to existing <span class="hlt">ice</span>, <span class="hlt">ice</span>-relative wind direction, <span class="hlt">ice</span> thickness and snow depth. In turn, these <span class="hlt">fluxes</span> impact upper-ocean heat loss and timing of <span class="hlt">ice</span> formation, as well as stability in the lower troposphere and upper ocean, and hence heat transport to the free troposphere and ocean mixed-layer. Therefore, the atmospheric structure over the advancing first-year <span class="hlt">ice</span> differs from that over the nearby open water. Finally, these observational analyses will be used to provide a preliminary validation of the spatial and temporal variability of the surface energy <span class="hlt">fluxes</span> and the associated lower-tropospheric and upper-ocean structures in the simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080015856&hterms=Fuel+co2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFuel%2Bco2','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080015856&hterms=Fuel+co2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFuel%2Bco2"><span>Using <span class="hlt">CO</span><span class="hlt">2</span>:<span class="hlt">CO</span> Correlations to Improve Inverse Analyses of Carbon <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Palmer, Paul I.; Suntharalingam, Parvadha; Jones, Dylan B. A.; Jacob, Daniel J.; Streets, David G.; Fu, Qingyan; Vay, Stephanie A.; Sachse, Glen W.</p> <p>2006-01-01</p> <p>Observed correlations between atmospheric concentrations of <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> represent potentially powerful information for improving <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">flux</span> estimates through coupled <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">CO</span> inverse analyses. We explore the value of these correlations in improving estimates of regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in east Asia by using aircraft observations of <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> from the TRACE-P campaign over the NW Pacific in March 2001. Our inverse model uses regional <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> surface <span class="hlt">fluxes</span> as the state vector, separating biospheric and combustion contributions to <span class="hlt">CO</span><span class="hlt">2</span>. <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">CO</span> error correlation coefficients are included in the inversion as off-diagonal entries in the a priori and observation error covariance matrices. We derive error correlations in a priori combustion source estimates of <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> by propagating error estimates of fuel consumption rates and emission factors. However, we find that these correlations are weak because <span class="hlt">CO</span> source uncertainties are mostly determined by emission factors. Observed correlations between atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> concentrations imply corresponding error correlations in the chemical transport model used as the forward model for the inversion. These error correlations in excess of 0.7, as derived from the TRACE-P data, enable a coupled <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">CO</span> inversion to achieve significant improvement over a <span class="hlt">CO</span><span class="hlt">2</span>-only inversion for quantifying regional <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4015316','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4015316"><span>Siple Dome <span class="hlt">ice</span> reveals two modes of millennial <span class="hlt">CO</span><span class="hlt">2</span> change during the last <span class="hlt">ice</span> age</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ahn, Jinho; Brook, Edward J.</p> <p>2014-01-01</p> <p>Reconstruction of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during times of past abrupt climate change may help us better understand climate-carbon cycle feedbacks. Previous <span class="hlt">ice</span> core studies reveal simultaneous increases in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and Antarctic temperature during times when Greenland and the northern hemisphere experienced very long, cold stadial conditions during the last <span class="hlt">ice</span> age. Whether this relationship extends to all of the numerous stadial events in the Greenland <span class="hlt">ice</span> core record has not been clear. Here we present a high-resolution record of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> from the Siple Dome <span class="hlt">ice</span> core, Antarctica for part of the last <span class="hlt">ice</span> age. We find that <span class="hlt">CO</span><span class="hlt">2</span> does not significantly change during the short Greenlandic stadial events, implying that the climate system perturbation that produced the short stadials was not strong enough to substantially alter the carbon cycle. PMID:24781344</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70127620','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70127620"><span>Interannual observations and quantification of summertime H<span class="hlt">2</span>O <span class="hlt">ice</span> deposition on the Martian <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> south polar cap</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Brown, Adrian J.; Piqueux, Sylvain; Titus, Timothy N.</p> <p>2014-01-01</p> <p>The spectral signature of water <span class="hlt">ice</span> was observed on Martian south polar cap in 2004 by the Observatoire pour l'Mineralogie, l'Eau les Glaces et l'Activite (OMEGA) ( Bibring et al., 2004). Three years later, the OMEGA instrument was used to discover water <span class="hlt">ice</span> deposited during southern summer on the polar cap ( Langevin et al., 2007). However, temporal and spatial variations of these water <span class="hlt">ice</span> signatures have remained unexplored, and the origins of these water deposits remains an important scientific question. To investigate this question, we have used observations from the Compact Reconnaissance Imaging Spectrometer for Mars (CRISM) instrument on the Mars Reconnaissance Orbiter (MRO) spacecraft of the southern cap during austral summer over four Martian years to search for variations in the amount of water <span class="hlt">ice</span>. We report below that for each year we have observed the cap, the magnitude of the H<span class="hlt">2</span>O <span class="hlt">ice</span> signature on the southern cap has risen steadily throughout summer, particularly on the west end of the cap. The spatial extent of deposition is in disagreement with the current best simulations of deposition of water <span class="hlt">ice</span> on the south polar cap (Montmessin et al., 2007). This increase in water <span class="hlt">ice</span> signatures is most likely caused by deposition of atmospheric H<span class="hlt">2</span>O <span class="hlt">ice</span> and a set of unusual conditions makes the quantification of this transport <span class="hlt">flux</span> using CRISM close to ideal. We calculate a ‘minimum apparent‘ amount of deposition corresponding to a thin H<span class="hlt">2</span>O <span class="hlt">ice</span> layer of 0.<span class="hlt">2</span> mm (with 70% porosity). This amount of H<span class="hlt">2</span>O <span class="hlt">ice</span> deposition is 0.6–6% of the total Martian atmospheric water budget. We compare our ‘minimum apparent’ quantification with previous estimates. This deposition process may also have implications for the formation and stability of the southern <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cap, and therefore play a significant role in the climate budget of modern day Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PNAS..113.3453L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PNAS..113.3453L"><span>Antarctic <span class="hlt">ice</span> sheet sensitivity to atmospheric <span class="hlt">CO</span><span class="hlt">2</span> variations in the early to mid-Miocene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levy, Richard; Harwood, David; Florindo, Fabio; Sangiorgi, Francesca; Tripati, Robert; von Eynatten, Hilmar; Gasson, Edward; Kuhn, Gerhard; Tripati, Aradhna; DeConto, Robert; Fielding, Christopher; Field, Brad; Golledge, Nicholas; McKay, Robert; Naish, Timothy; Olney, Matthew; Pollard, David; Schouten, Stefan; Talarico, Franco; Warny, Sophie; Willmott, Veronica; Acton, Gary; Panter, Kurt; Paulsen, Timothy; Taviani, Marco; SMS Science Team; Acton, Gary; Askin, Rosemary; Atkins, Clifford; Bassett, Kari; Beu, Alan; Blackstone, Brian; Browne, Gregory; Ceregato, Alessandro; Cody, Rosemary; Cornamusini, Gianluca; Corrado, Sveva; DeConto, Robert; Del Carlo, Paola; Di Vincenzo, Gianfranco; Dunbar, Gavin; Falk, Candice; Field, Brad; Fielding, Christopher; Florindo, Fabio; Frank, Tracy; Giorgetti, Giovanna; Grelle, Thomas; Gui, Zi; Handwerger, David; Hannah, Michael; Harwood, David M.; Hauptvogel, Dan; Hayden, Travis; Henrys, Stuart; Hoffmann, Stefan; Iacoviello, Francesco; Ishman, Scott; Jarrard, Richard; Johnson, Katherine; Jovane, Luigi; Judge, Shelley; Kominz, Michelle; Konfirst, Matthew; Krissek, Lawrence; Kuhn, Gerhard; Lacy, Laura; Levy, Richard; Maffioli, Paola; Magens, Diana; Marcano, Maria C.; Millan, Cristina; Mohr, Barbara; Montone, Paola; Mukasa, Samuel; Naish, Timothy; Niessen, Frank; Ohneiser, Christian; Olney, Mathew; Panter, Kurt; Passchier, Sandra; Patterson, Molly; Paulsen, Timothy; Pekar, Stephen; Pierdominici, Simona; Pollard, David; Raine, Ian; Reed, Joshua; Reichelt, Lucia; Riesselman, Christina; Rocchi, Sergio; Sagnotti, Leonardo; Sandroni, Sonia; Sangiorgi, Francesca; Schmitt, Douglas; Speece, Marvin; Storey, Bryan; Strada, Eleonora; Talarico, Franco; Taviani, Marco; Tuzzi, Eva; Verosub, Kenneth; von Eynatten, Hilmar; Warny, Sophie; Wilson, Gary; Wilson, Terry; Wonik, Thomas; Zattin, Massimiliano</p> <p>2016-03-01</p> <p>Geological records from the Antarctic margin offer direct evidence of environmental variability at high southern latitudes and provide insight regarding <span class="hlt">ice</span> sheet sensitivity to past climate change. The early to mid-Miocene (23-14 Mya) is a compelling interval to study as global temperatures and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were similar to those projected for coming centuries. Importantly, this time interval includes the Miocene Climatic Optimum, a period of global warmth during which average surface temperatures were 3-4 °C higher than today. Miocene sediments in the ANDRILL-<span class="hlt">2</span>A drill core from the Western Ross Sea, Antarctica, indicate that the Antarctic <span class="hlt">ice</span> sheet (AIS) was highly variable through this key time interval. A multiproxy dataset derived from the core identifies four distinct environmental motifs based on changes in sedimentary facies, fossil assemblages, geochemistry, and paleotemperature. Four major disconformities in the drill core coincide with regional seismic discontinuities and reflect transient expansion of grounded <span class="hlt">ice</span> across the Ross Sea. They correlate with major positive shifts in benthic oxygen isotope records and generally coincide with intervals when atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were at or below preindustrial levels (˜280 ppm). Five intervals reflect <span class="hlt">ice</span> sheet minima and <span class="hlt">air</span> temperatures warm enough for substantial <span class="hlt">ice</span> mass loss during episodes of high (˜500 ppm) atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. These new drill core data and associated <span class="hlt">ice</span> sheet modeling experiments indicate that polar climate and the AIS were highly sensitive to relatively small changes in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during the early to mid-Miocene.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4822588','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4822588"><span>Antarctic <span class="hlt">ice</span> sheet sensitivity to atmospheric <span class="hlt">CO</span><span class="hlt">2</span> variations in the early to mid-Miocene</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Levy, Richard; Harwood, David; Florindo, Fabio; Sangiorgi, Francesca; Tripati, Robert; von Eynatten, Hilmar; Tripati, Aradhna; DeConto, Robert; Fielding, Christopher; Field, Brad; Golledge, Nicholas; McKay, Robert; Naish, Timothy; Olney, Matthew; Pollard, David; Schouten, Stefan; Talarico, Franco; Warny, Sophie; Willmott, Veronica; Acton, Gary; Panter, Kurt; Paulsen, Timothy; Taviani, Marco</p> <p>2016-01-01</p> <p>Geological records from the Antarctic margin offer direct evidence of environmental variability at high southern latitudes and provide insight regarding <span class="hlt">ice</span> sheet sensitivity to past climate change. The early to mid-Miocene (23–14 Mya) is a compelling interval to study as global temperatures and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were similar to those projected for coming centuries. Importantly, this time interval includes the Miocene Climatic Optimum, a period of global warmth during which average surface temperatures were 3–4 °C higher than today. Miocene sediments in the ANDRILL-<span class="hlt">2</span>A drill core from the Western Ross Sea, Antarctica, indicate that the Antarctic <span class="hlt">ice</span> sheet (AIS) was highly variable through this key time interval. A multiproxy dataset derived from the core identifies four distinct environmental motifs based on changes in sedimentary facies, fossil assemblages, geochemistry, and paleotemperature. Four major disconformities in the drill core coincide with regional seismic discontinuities and reflect transient expansion of grounded <span class="hlt">ice</span> across the Ross Sea. They correlate with major positive shifts in benthic oxygen isotope records and generally coincide with intervals when atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were at or below preindustrial levels (∼280 ppm). Five intervals reflect <span class="hlt">ice</span> sheet minima and <span class="hlt">air</span> temperatures warm enough for substantial <span class="hlt">ice</span> mass loss during episodes of high (∼500 ppm) atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. These new drill core data and associated <span class="hlt">ice</span> sheet modeling experiments indicate that polar climate and the AIS were highly sensitive to relatively small changes in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during the early to mid-Miocene. PMID:26903644</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26903644','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26903644"><span>Antarctic <span class="hlt">ice</span> sheet sensitivity to atmospheric <span class="hlt">CO</span><span class="hlt">2</span> variations in the early to mid-Miocene.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Levy, Richard; Harwood, David; Florindo, Fabio; Sangiorgi, Francesca; Tripati, Robert; von Eynatten, Hilmar; Gasson, Edward; Kuhn, Gerhard; Tripati, Aradhna; DeConto, Robert; Fielding, Christopher; Field, Brad; Golledge, Nicholas; McKay, Robert; Naish, Timothy; Olney, Matthew; Pollard, David; Schouten, Stefan; Talarico, Franco; Warny, Sophie; Willmott, Veronica; Acton, Gary; Panter, Kurt; Paulsen, Timothy; Taviani, Marco</p> <p>2016-03-29</p> <p>Geological records from the Antarctic margin offer direct evidence of environmental variability at high southern latitudes and provide insight regarding <span class="hlt">ice</span> sheet sensitivity to past climate change. The early to mid-Miocene (23-14 Mya) is a compelling interval to study as global temperatures and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were similar to those projected for coming centuries. Importantly, this time interval includes the Miocene Climatic Optimum, a period of global warmth during which average surface temperatures were 3-4 °C higher than today. Miocene sediments in the ANDRILL-<span class="hlt">2</span>A drill core from the Western Ross Sea, Antarctica, indicate that the Antarctic <span class="hlt">ice</span> sheet (AIS) was highly variable through this key time interval. A multiproxy dataset derived from the core identifies four distinct environmental motifs based on changes in sedimentary facies, fossil assemblages, geochemistry, and paleotemperature. Four major disconformities in the drill core coincide with regional seismic discontinuities and reflect transient expansion of grounded <span class="hlt">ice</span> across the Ross Sea. They correlate with major positive shifts in benthic oxygen isotope records and generally coincide with intervals when atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations were at or below preindustrial levels (∼280 ppm). Five intervals reflect <span class="hlt">ice</span> sheet minima and <span class="hlt">air</span> temperatures warm enough for substantial <span class="hlt">ice</span> mass loss during episodes of high (∼500 ppm) atmospheric <span class="hlt">CO</span><span class="hlt">2</span> These new drill core data and associated <span class="hlt">ice</span> sheet modeling experiments indicate that polar climate and the AIS were highly sensitive to relatively small changes in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during the early to mid-Miocene.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A42F..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A42F..07L"><span>Simultaneous assimilation of <span class="hlt">AIRS</span> and GOSAT <span class="hlt">CO</span><span class="hlt">2</span> observations with Ensemble Kalman filter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, J.; Kalnay, E.; Fung, I.; Kang, J.</p> <p>2012-12-01</p> <p>Lack of <span class="hlt">CO</span><span class="hlt">2</span> vertical information could lead to bias in the surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimation (Stephens et al., 2007). Liu et al. (2012) showed that assimilating <span class="hlt">AIRS</span> <span class="hlt">CO</span><span class="hlt">2</span> observations, which are sensitive to middle to upper troposphere <span class="hlt">CO</span><span class="hlt">2</span>, improves <span class="hlt">CO</span><span class="hlt">2</span> concentration, especially in the middle to upper troposphere. GOSAT is sensitive to <span class="hlt">CO</span><span class="hlt">2</span> over the whole column, but the spatial coverage is sparser than <span class="hlt">AIRS</span>. In this study, we assimilate <span class="hlt">AIRS</span> and GOSAT <span class="hlt">CO</span><span class="hlt">2</span> observations simultaneously along with surface flask <span class="hlt">CO</span><span class="hlt">2</span> observations and meteorology observations with Ensemble Kalman filter (EnKF) to constrain <span class="hlt">CO</span><span class="hlt">2</span> vertical profiles simulated by NCAR carbon-climate model. We will show the impact of assimilating <span class="hlt">AIRS</span> and GOSAT <span class="hlt">CO</span><span class="hlt">2</span> on the <span class="hlt">CO</span><span class="hlt">2</span> vertical gradient, seasonal cycle and spatial gradient by assimilating only GOSAT or <span class="hlt">AIRS</span> and comparing to the control experiment. The quality of <span class="hlt">CO</span><span class="hlt">2</span> analysis will be examined by validating against independent <span class="hlt">CO</span><span class="hlt">2</span> aircraft observations, and analyzing the relationship between <span class="hlt">CO</span><span class="hlt">2</span> analysis fields and major circulation, such as Madden Julian Oscillation. We will also discuss the deficiencies of the observation network in understanding the carbon cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A43H..07F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A43H..07F"><span>Evaluation of NASA's Carbon Monitoring System (CMS) <span class="hlt">Flux</span> Pilot: Terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fisher, J. B.; Polhamus, A.; Bowman, K. W.; Collatz, G. J.; Potter, C. S.; Lee, M.; Liu, J.; Jung, M.; Reichstein, M.</p> <p>2011-12-01</p> <p>NASA's Carbon Monitoring System (CMS) <span class="hlt">flux</span> pilot project combines NASA's Earth System models in land, ocean and atmosphere to track surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The system is constrained by atmospheric measurements of XCO<span class="hlt">2</span> from the Japanese GOSAT satellite, giving a "big picture" view of total <span class="hlt">CO</span><span class="hlt">2</span> in Earth's atmosphere. Combining two land models (CASA-Ames and CASA-GFED), two ocean models (ECCO<span class="hlt">2</span> and NOBM) and two atmospheric chemistry and inversion models (GEOS-5 and GEOS-Chem), the system brings together the stand-alone component models of the Earth System, all of which are run diagnostically constrained by a multitude of other remotely sensed data. Here, we evaluate the biospheric land surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (i.e., net ecosystem exchange, NEE) as estimated from the atmospheric <span class="hlt">flux</span> inversion. We compare against the prior bottom-up estimates (e.g., the CASA models) as well. Our evaluation dataset is the independently derived global wall-to-wall MPI-BGC product, which uses a machine learning algorithm and model tree ensemble to "scale-up" a network of in situ <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements from 253 globally-distributed sites in the FLUXNET network. The measurements are based on the eddy covariance method, which uses observations of <span class="hlt">co</span>-varying <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> (and water and energy) from instruments on towers extending above ecosystem canopies; the towers integrate <span class="hlt">fluxes</span> over large spatial areas (~1 km<span class="hlt">2</span>). We present global maps of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and differences between products, summaries of <span class="hlt">fluxes</span> by TRANSCOM region, country, latitude, and biome type, and assess the time series, including timing of minimum and maximum <span class="hlt">fluxes</span>. This evaluation shows both where the CMS is performing well, and where improvements should be directed in further work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A53E0229L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A53E0229L"><span>A Synthesized Model-Observation Approach to Constraining Gross Urban <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Using 14<span class="hlt">CO</span><span class="hlt">2</span> and carbonyl sulfide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>LaFranchi, B. W.; Campbell, J. E.; Cameron-Smith, P. J.; Bambha, R.; Michelsen, H. A.</p> <p>2013-12-01</p> <p>Urbanized regions are responsible for a disproportionately large percentage (30-40%) of global anthropogenic greenhouse gas (GHG) emissions, despite covering only <span class="hlt">2</span>% of the Earth's surface area [Satterthwaite, 2008]. As a result, policies enacted at the local level in these urban areas can, in aggregate, have a large global impact, both positive and negative. In order to address the scientific questions that are required to drive these policy decisions, methods are needed that resolve gross <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> components from the net <span class="hlt">flux</span>. Recent work suggests that the critical knowledge gaps in <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> could be addressed through the combined analysis of atmospheric carbonyl sulfide (COS) and radiocarbon in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> (14<span class="hlt">CO</span><span class="hlt">2</span>) [e.g. Campbell et al., 2008; Graven et al., 2009]. The 14<span class="hlt">CO</span><span class="hlt">2</span> approach relies on mass balance assumptions about atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and the large differences in 14<span class="hlt">CO</span><span class="hlt">2</span> abundance between fossil and natural sources of <span class="hlt">CO</span><span class="hlt">2</span> [Levin et al., 2003]. COS, meanwhile, is a potentially transformative tracer of photosynthesis because its variability in the atmosphere has been found to be influenced primarily by vegetative uptake, scaling linearly will gross primary production (GPP) [Kettle et al., 20027]. Taken together, these two observations provide constraints on two of the three main components of the <span class="hlt">CO</span><span class="hlt">2</span> budget at the urban scale: photosynthesis and fossil fuel emissions. The third component, respiration, can then be determined by difference if the net <span class="hlt">flux</span> is known. Here we present a general overview of our synthesized model-observation approach for improving surface <span class="hlt">flux</span> estimates of <span class="hlt">CO</span><span class="hlt">2</span> for the upwind fetch of a ~30m tower located in Livermore, CA, USA, a suburb (pop. ~80,000) at the eastern edge of the San Francisco Bay Area. Additionally, we will present initial results from a one week observational intensive, which includes continuous <span class="hlt">CO</span><span class="hlt">2</span>, CH4, <span class="hlt">CO</span>, SO<span class="hlt">2</span>, NOx, and O3 observations in addition to measurements of 14<span class="hlt">CO</span><span class="hlt">2</span> and COS from <span class="hlt">air</span> samples</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B51I1941B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B51I1941B"><span>A Spatial-Temporal Comparison of Lake Mendota <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> and Collection Methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baldocchi, A. K.; Reed, D. E.; Desai, A. R.; Loken, L. C.; Schramm, P.; Stanley, E. H.</p> <p>2017-12-01</p> <p>Monitoring of carbon <span class="hlt">fluxes</span> at the lake/atmosphere interface can help us determine baselines from which to understand responses in both space and time that may result from our warming climate or increasing nutrient inputs. Since recent research has shown lakes to be hotspots of global carbon cycling, it is important to quantify carbon sink and source dynamics as well as to verify observations between multiple methods in the context of long-term data collection efforts. Here we evaluate a new method for measuring space and time variation in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> based on novel speedboat-based collection method of aquatic greenhouse gas concentrations and a <span class="hlt">flux</span> computation and interpolation algorithm. Two-hundred and forty-nine consecutive days of spatial <span class="hlt">flux</span> maps over the 2016 open <span class="hlt">ice</span> period were compared to ongoing eddy covariance tower <span class="hlt">flux</span> measurements on the shore of Lake Mendota, Wisconsin US using a <span class="hlt">flux</span> footprint analysis. Spatial and temporal alignments of the <span class="hlt">fluxes</span> from these two observational datasets revealed both similar trends from daily to seasonal timescales as well as biases between methods. For example, throughout the Spring carbon <span class="hlt">fluxes</span> showed strong correlation although off by an order of magnitude. Isolating physical patterns of agreement between the two methods of the lake/atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> allows us to pinpoint where biology and physical drivers contribute to the global carbon cycle and help improve modelling of lakes and utilize lakes as leading indicators of climate change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70028279','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70028279"><span><span class="hlt">CO</span><span class="hlt">2</span> jets formed by sublimation beneath translucent slab <span class="hlt">ice</span> in Mars' seasonal south polar <span class="hlt">ice</span> cap</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kieffer, H.H.; Christensen, P.R.; Titus, T.N.</p> <p>2006-01-01</p> <p>The martian polar caps are among the most dynamic regions on Mars, growing substantially in winter as a significant fraction of the atmosphere freezes out in the form of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. Unusual dark spots, fans and blotches form as the south-polar seasonal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cap retreats during spring and summer. Small radial channel networks are often associated with the location of spots once the <span class="hlt">ice</span> disappears. The spots have been proposed to be simply bare, defrosted ground; the formation of the channels has remained uncertain. Here we report infrared and visible observations that show that the spots and fans remain at <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> temperatures well into summer, and must be granular materials that have been brought up to the surface of the <span class="hlt">ice</span>, requiring a complex suite of processes to get them there. We propose that the seasonal <span class="hlt">ice</span> cap forms an impermeable, translucent slab of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> that sublimates from the base, building up high-pressure gas beneath the slab. This gas levitates the <span class="hlt">ice</span>, which eventually ruptures, producing high-velocity <span class="hlt">CO</span> <span class="hlt">2</span> vents that erupt sand-sized grains in jets to form the spots and erode the channels. These processes are unlike any observed on Earth. ?? 2006 Nature Publishing Group.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.B43H0528Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.B43H0528Y"><span>Effects of a holiday week on urban soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>: an intensive study in Xiamen, southeastern China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ye, H.; Wang, K.; Chen, F.</p> <p>2012-12-01</p> <p>To study the effects of a holiday period on urban soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, <span class="hlt">CO</span><span class="hlt">2</span> efflux from grassland soil in a traditional park in the city of Xiamen was measured hourly from 28th Sep to 11th Oct, a period that included China's National Day holiday week in 2009. The results of this study revealed that: a) The urban soil <span class="hlt">CO</span><span class="hlt">2</span> emissions were higher before and after the holiday week and lower during the National Day holiday reflecting changes in the traffic cycles; b) A diurnal cycle where the soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> decreased from early morning to noon was associated with <span class="hlt">CO</span><span class="hlt">2</span> uptake by vegetation which strongly offset vehicle <span class="hlt">CO</span><span class="hlt">2</span> emissions. The soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> increased from night to early morning, associated with reduced <span class="hlt">CO</span><span class="hlt">2</span> uptake by vegetation; c) During the National Day holiday week in 2009, lower rates of soil respiration were measured after Mid-Autumn Day than earlier in the week, and this was related to a reduced level of human activities and vehicle traffic, reducing the <span class="hlt">CO</span><span class="hlt">2</span> concentration in the <span class="hlt">air</span>. Urban holidays have a clear effect on soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> through the interactions between vehicle, visitor and vegetation <span class="hlt">CO</span><span class="hlt">2</span> emissions which indirectly control the use of carbon by plant roots, the rhizosphere and soil microorganisms. Consequently, appropriate traffic controls and tourism travel plans can have positive effects on the soil carbon store and may improve local <span class="hlt">air</span> quality.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27811286','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27811286"><span>Observed Arctic sea-<span class="hlt">ice</span> loss directly follows anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emission.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Notz, Dirk; Stroeve, Julienne</p> <p>2016-11-11</p> <p>Arctic sea <span class="hlt">ice</span> is retreating rapidly, raising prospects of a future <span class="hlt">ice</span>-free Arctic Ocean during summer. Because climate-model simulations of the sea-<span class="hlt">ice</span> loss differ substantially, we used a robust linear relationship between monthly-mean September sea-<span class="hlt">ice</span> area and cumulative carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span> ) emissions to infer the future evolution of Arctic summer sea <span class="hlt">ice</span> directly from the observational record. The observed linear relationship implies a sustained loss of 3 ± 0.3 square meters of September sea-<span class="hlt">ice</span> area per metric ton of <span class="hlt">CO</span> <span class="hlt">2</span> emission. On the basis of this sensitivity, Arctic sea <span class="hlt">ice</span> will be lost throughout September for an additional 1000 gigatons of <span class="hlt">CO</span> <span class="hlt">2</span> emissions. Most models show a lower sensitivity, which is possibly linked to an underestimation of the modeled increase in incoming longwave radiation and of the modeled transient climate response. Copyright © 2016, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/467708-measurements-co-sub-fluxes-bubbles-from-tower-during-asgasex','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/467708-measurements-co-sub-fluxes-bubbles-from-tower-during-asgasex"><span>Measurements of <span class="hlt">CO</span>{sub <span class="hlt">2</span>} <span class="hlt">fluxes</span> and bubbles from a tower during ASGASEX</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Leeuw, G. de; Kunz, G.J.; Larsen, S.E.</p> <p>1994-12-31</p> <p>The <span class="hlt">Air</span>-Sea Gas Exchange experiment ASGASEX was conducted from August 30 until October 1st from the Meetpost Noordwijk (MPN), a research tower in the North Sea at 9 km from the Dutch coast. The objective of ASGASEX was a study of parameters affecting the <span class="hlt">air</span>-sea exchange of gases, and a comparison of experimental methods to derive the exchange coefficient for <span class="hlt">CO</span>{sub <span class="hlt">2</span>}. A detailed description of the ASGASEX experiment is presented in Oost. The authors` contribution to ASGASEX was a micro-meteorological package to measure the <span class="hlt">fluxes</span> of <span class="hlt">CO</span>{sub <span class="hlt">2</span>}, momentum, heat and water vapor, and an instrument to measure themore » size distribution of bubbles just below the sea surface. In this contribution the authors report preliminary results from the <span class="hlt">CO</span>{sub <span class="hlt">2</span>} <span class="hlt">flux</span> measurements and the bubble measurements. The latter was made as part of a larger study on the influence of bubbles on gas exchange in cooperation with the University of Southampton and the University of Galway.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006ThApC..84..117V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006ThApC..84..117V"><span>Temporal dynamics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and profiles over a Central European city</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vogt, R.; Christen, A.; Rotach, M. W.; Roth, M.; Satyanarayana, A. N. V.</p> <p>2006-02-01</p> <p>In Summer 2002 eddy covariance <span class="hlt">flux</span> measurements of <span class="hlt">CO</span><span class="hlt">2</span> were performed over a dense urban surface. The month-long measurements were carried out in the framework of the Basel Urban Boundary Layer Experiment (BUBBLE). Two Li7500 open path analysers were installed at z/z H = 1.0 and <span class="hlt">2.2</span> above a street canyon with z H the average building height of 14.6 m and z the height above street level. Additionally, profiles of <span class="hlt">CO</span><span class="hlt">2</span> concentration were sampled at 10 heights from street level up to <span class="hlt">2</span> z H . The minimum and maximum of the average diurnal course of <span class="hlt">CO</span><span class="hlt">2</span> concentration at <span class="hlt">2</span> z H were 362 and 423 ppmv in late afternoon and early morning, respectively. Daytime <span class="hlt">CO</span><span class="hlt">2</span> concentrations were not correlated to local sources, e.g. the minimum occurred together with the maximum in traffic load. During night-time <span class="hlt">CO</span><span class="hlt">2</span> is in general accumulated, except when inversion development is suppressed by frontal passages. <span class="hlt">CO</span><span class="hlt">2</span> concentrations were always decreasing with height and correspondingly, the <span class="hlt">fluxes</span> on average always directed upward. At z/z H = <span class="hlt">2.2</span> low values of about 3 µmol m-<span class="hlt">2</span> s-1 were measured during the second half of the night. During daytime average values reached up to 14 µmol m-<span class="hlt">2</span> s-1. The <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are well correlated with the traffic load, with their maxima occurring together in late afternoon. Daytime minimum <span class="hlt">CO</span><span class="hlt">2</span> concentrations fell below regional background values. Besides vertical mixing and entrainment, it is suggested that this is also due to advection of rural <span class="hlt">air</span> with reduced <span class="hlt">CO</span><span class="hlt">2</span> concentration. Comparison with other urban observations shows a large range of differences among urban sites in terms of both <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8085Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8085Q"><span>A practical <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> remote sensing technique</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Queisser, Manuel; Burton, Mike</p> <p>2017-04-01</p> <p>An accurate quantification of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from both natural and anthropogenic sources is of great interest in various areas of the Earth, environmental and atmospheric sciences. As emitted excess <span class="hlt">CO</span><span class="hlt">2</span> quickly dilutes into the 400 ppm ambient <span class="hlt">CO</span><span class="hlt">2</span> concentration and degassing often occurs diffusively, measuring <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> is challenging. Therefore, <span class="hlt">fluxes</span> are usually derived from grids of in-situ measurements, which are labour intensive measurements. Other than a safe measurement distance, remote sensing offers quick, spatially integrated and thus a more thorough measurement of gas <span class="hlt">fluxes</span>. Active remote sensing combines these merits with operation independent of sunlight or clear sky conditions. Due to their weight and size, active remote sensing platforms for <span class="hlt">CO</span><span class="hlt">2</span>, such as LIDAR, cannot easily be applied in the field or transported overseas. Moreover, their complexity requires a rather lengthy setup procedure to be undertaken by skilled personal. To meet the need for a rugged, practical <span class="hlt">CO</span><span class="hlt">2</span> remote sensing technique to scan volcanic plumes, we have developed the <span class="hlt">CO</span><span class="hlt">2</span> LIDAR. It measures 1-D column densities of <span class="hlt">CO</span><span class="hlt">2</span> with sufficient sensitivity to reveal the contribution of magmatic <span class="hlt">CO</span><span class="hlt">2</span>. The <span class="hlt">CO</span><span class="hlt">2</span> LIDAR has been mounted inside a small aircraft and used to measure atmospheric column <span class="hlt">CO</span><span class="hlt">2</span> concentrations between the aircraft and the ground. It was further employed on the ground, measuring <span class="hlt">CO</span><span class="hlt">2</span> emissions from mud volcanism. During the measurement campaign the <span class="hlt">CO</span><span class="hlt">2</span> LIDAR demonstrated reliability, portability, quick set-up time (10 to 15 min) and platform independence. This new technique opens the possibility of rapid, comprehensive surveys of point source, open-vent <span class="hlt">CO</span><span class="hlt">2</span> emissions, as well as emissions from more diffuse sources such as lakes and fumarole fields. Currently, within the proof-of-concept ERC project CarbSens, a further reduction in size, weight and operational complexity is underway with the goal to commercialize the platform. Areas of potential applications include fugitive</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950025364','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950025364"><span><span class="hlt">CO</span><span class="hlt">2</span> (dry <span class="hlt">ice</span>) cleaning system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barnett, Donald M.</p> <p>1995-01-01</p> <p>Tomco Equipment Company has participated in the dry <span class="hlt">ice</span> (solid carbon dioxide, <span class="hlt">CO</span><span class="hlt">2</span>) cleaning industry for over ten years as a pioneer in the manufacturer of high density, dry <span class="hlt">ice</span> cleaning pellet production equipment. For over four years Tomco high density pelletizers have been available to the dry <span class="hlt">ice</span> cleaning industry. Approximately one year ago Tomco introduced the DI-250, a new dry <span class="hlt">ice</span> blast unit making Tomco a single source supplier for sublimable media, particle blast, cleaning systems. This new blast unit is an all pneumatic, single discharge hose device. It meters the insertion of 1/8 inch diameter (or smaller), high density, dry <span class="hlt">ice</span> pellets into a high pressure, propellant gas stream. The dry <span class="hlt">ice</span> and propellant streams are controlled and mixed from the blast cabinet. From there the mixture is transported to the nozzle where the pellets are accelerated to an appropriate blasting velocity. When directed to impact upon a target area, these dry <span class="hlt">ice</span> pellets have sufficient energy to effectively remove most surface coatings through dry, abrasive contact. The meta-stable, dry <span class="hlt">ice</span> pellets used for <span class="hlt">CO</span><span class="hlt">2</span> cleaning, while labeled 'high density,' are less dense than alternate, abrasive, particle blast media. In addition, after contacting the target surface, they return to their equilibrium condition: a superheated gas state. Most currently used grit blasting media are silicon dioxide based, which possess a sharp tetrahedral molecular structure. Silicon dioxide crystal structures will always produce smaller sharp-edged replicas of the original crystal upon fracture. Larger, softer dry <span class="hlt">ice</span> pellets do not share the same sharp-edged crystalline structures as their non-sublimable counterparts when broken. In fact, upon contact with the target surface, dry <span class="hlt">ice</span> pellets will plastically deform and break apart. As such, dry <span class="hlt">ice</span> cleaning is less harmful to sensitive substrates, workers and the environment than chemical or abrasive cleaning systems. Dry <span class="hlt">ice</span> cleaning system</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BGeo...14.5189J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BGeo...14.5189J"><span>Year-round CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> dynamics in two contrasting freshwater ecosystems of the subarctic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jammet, Mathilde; Dengel, Sigrid; Kettner, Ernesto; Parmentier, Frans-Jan W.; Wik, Martin; Crill, Patrick; Friborg, Thomas</p> <p>2017-11-01</p> <p>Lakes and wetlands, common ecosystems of the high northern latitudes, exchange large amounts of the climate-forcing gases methane (CH4) and carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) with the atmosphere. The magnitudes of these <span class="hlt">fluxes</span> and the processes driving them are still uncertain, particularly for subarctic and Arctic lakes where direct measurements of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> emissions are often of low temporal resolution and are rarely sustained throughout the entire year. Using the eddy covariance method, we measured surface-atmosphere exchange of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> during <span class="hlt">2</span>.5 years in a thawed fen and a shallow lake of a subarctic peatland complex. Gas exchange at the fen exhibited the expected seasonality of a subarctic wetland with maximum CH4 emissions and <span class="hlt">CO</span><span class="hlt">2</span> uptake in summer, as well as low but continuous emissions of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> throughout the snow-covered winter. The seasonality of lake <span class="hlt">fluxes</span> differed, with maximum <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> rates recorded at spring thaw. During the <span class="hlt">ice</span>-free seasons, we could identify surface CH4 emissions as mostly ebullition events with a seasonal trend in the magnitude of the release, while a net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> indicated photosynthetic activity. We found correlations between surface CH4 emissions and surface sediment temperature, as well as between diel <span class="hlt">CO</span><span class="hlt">2</span> uptake and diel solar input. During spring, the breakdown of thermal stratification following <span class="hlt">ice</span> thaw triggered the degassing of both CH4 and <span class="hlt">CO</span><span class="hlt">2</span>. This spring burst was observed in <span class="hlt">2</span> consecutive years for both gases, with a large inter-annual variability in the magnitude of the CH4 degassing. On the annual scale, spring emissions converted the lake from a small <span class="hlt">CO</span><span class="hlt">2</span> sink to a <span class="hlt">CO</span><span class="hlt">2</span> source: 80 % of total annual carbon emissions from the lake were emitted as <span class="hlt">CO</span><span class="hlt">2</span>. The annual total carbon exchange per unit area was highest at the fen, which was an annual sink of carbon with respect to the atmosphere. Continuous respiration during the winter partly counteracted the fen summer sink by accounting for, as both CH4 and <span class="hlt">CO</span><span class="hlt">2</span>, 33</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRG..122.1615H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRG..122.1615H"><span>Effect of hydroperiod on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at the <span class="hlt">air</span>-water interface in the Mediterranean coastal wetlands of Doñana</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huertas, I. Emma; Flecha, Susana; Figuerola, Jordi; Costas, Eduardo; Morris, Edward P.</p> <p>2017-07-01</p> <p>Wetlands are productive ecosystems that play an important role in the Earth's carbon cycle and thus global carbon budgets. Climate variability affects amount of material entering and the metabolic balance of wetlands, thereby modifying carbon dynamics. This study presents spatiotemporal changes in <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> exchange in the vast wetlands of Doñana (Spain) in relation to different hydrological cycles. Water sources feeding Doñana, including groundwater and streams, ultimately depend on the fluctuating balance between annual precipitation and evapotranspiration. Hence, in order to examine the contribution of the rainfall pattern to the emission/capture of <span class="hlt">CO</span><span class="hlt">2</span> by a range of aquatic habitats in Doñana, we took monthly measurements during severely wet, dry, and normal hydrological years (2010-2013). During wet hydrological cycles, <span class="hlt">CO</span><span class="hlt">2</span> outgassing from flooded marshes markedly decreased in comparison to that observed during subsequent dry-normal cycles, with mean values of 25.84 ± 19 and 5.<span class="hlt">2</span> ± 8 mmol m-<span class="hlt">2</span> d-1, respectively. Under drier meteorological conditions, <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> also diminished in permanent floodplains and ponds, which even behaved as mild sinks for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> during certain periods. Increased inputs of dissolved <span class="hlt">CO</span><span class="hlt">2</span> from the underground aquifer and the stream following periods of high rainfall are believed to be behind this pattern. Large lagoons with a managed water supply from an adjacent estuary took up atmospheric <span class="hlt">CO</span><span class="hlt">2</span> nearly permanently. Regional <span class="hlt">air</span>-water carbon transport was 15.<span class="hlt">2</span> GgC yr-1 under wet and 1.24 GgC yr-1 under dry meteorological conditions, well below the estimated net primary production for Doñana wetlands, indicating that the ecosystem acts as a large <span class="hlt">CO</span><span class="hlt">2</span> sink.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PrOce.141..153Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PrOce.141..153Z"><span>The impact of dissolved organic carbon and bacterial respiration on p<span class="hlt">CO</span><span class="hlt">2</span> in experimental sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, J.; Kotovitch, M.; Kaartokallio, H.; Moreau, S.; Tison, J.-L.; Kattner, G.; Dieckmann, G.; Thomas, D. N.; Delille, B.</p> <p>2016-02-01</p> <p>Previous observations have shown that the partial pressure of carbon dioxide (p<span class="hlt">CO</span><span class="hlt">2</span>) in sea <span class="hlt">ice</span> brines is generally higher in Arctic sea <span class="hlt">ice</span> compared to those from the Antarctic sea <span class="hlt">ice</span>, especially in winter and early spring. We hypothesized that these differences result from the higher dissolved organic carbon (DOC) content in Arctic seawater: Higher concentrations of DOC in seawater would be reflected in a greater DOC incorporation into sea <span class="hlt">ice</span>, enhancing bacterial respiration, which in turn would increase the p<span class="hlt">CO</span><span class="hlt">2</span> in the <span class="hlt">ice</span>. To verify this hypothesis, we performed an experiment using two series of mesocosms: one was filled with seawater (SW) and the other one with seawater with an addition of filtered humic-rich river water (SWR). The addition of river water increased the DOC concentration of the water from a median of 142 μmol Lwater-1 in SW to 249 μmol Lwater-1 in SWR. Sea <span class="hlt">ice</span> was grown in these mesocosms under the same physical conditions over 19 days. Microalgae and protists were absent, and only bacterial activity has been detected. We measured the DOC concentration, bacterial respiration, total alkalinity and p<span class="hlt">CO</span><span class="hlt">2</span> in sea <span class="hlt">ice</span> and the underlying seawater, and we calculated the changes in dissolved inorganic carbon (DIC) in both media. We found that bacterial respiration in <span class="hlt">ice</span> was higher in SWR: median bacterial respiration was 25 nmol C Lice-1 h-1 compared to 10 nmol C Lice-1 h-1 in SW. p<span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">ice</span> was also higher in SWR with a median of 430 ppm compared to 356 ppm in SW. However, the differences in p<span class="hlt">CO</span><span class="hlt">2</span> were larger within the <span class="hlt">ice</span> interiors than at the surfaces or the bottom layers of the <span class="hlt">ice</span>, where exchanges at the <span class="hlt">air-ice</span> and <span class="hlt">ice</span>-water interfaces might have reduced the differences. In addition, we used a model to simulate the differences of p<span class="hlt">CO</span><span class="hlt">2</span> and DIC based on bacterial respiration. The model simulations support the experimental findings and further suggest that bacterial growth efficiency in the <span class="hlt">ice</span> might approach 0.15 and 0.<span class="hlt">2</span>. It is thus credible</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1364062','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1364062"><span>Radiocarbon in Ecosystem Respiration and Soil Pore-Space <span class="hlt">CO</span><span class="hlt">2</span> with Surface Gas <span class="hlt">Flux</span>, <span class="hlt">Air</span> Temperature, and Soil Temperature and Moisture, Barrow, Alaska, 2012-2014</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lydia Vaughn; Margaret Torn; Rachel Porras</p> <p></p> <p>Dataset includes Delta14C measurements made from <span class="hlt">CO</span><span class="hlt">2</span> that was collected and purified in 2012-2014 from surface soil chambers, soil pore space, and background atmosphere. In addition to 14<span class="hlt">CO</span><span class="hlt">2</span> data, dataset includes <span class="hlt">co</span>-located measurements of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span>, soil and <span class="hlt">air</span> temperature, and soil moisture. Measurements and field samples were taken from intensive study site 1 areas A, B, and C, and the site 0 and AB transects, from specified positions in high-centered, flat-centered, and low centered polygons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoRL..4311726A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoRL..4311726A"><span>A comparison of <span class="hlt">CO</span><span class="hlt">2</span> dynamics and <span class="hlt">air</span>-water <span class="hlt">fluxes</span> in a river-dominated estuary and a mangrove-dominated marine estuary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akhand, Anirban; Chanda, Abhra; Manna, Sudip; Das, Sourav; Hazra, Sugata; Roy, Rajdeep; Choudhury, S. B.; Rao, K. H.; Dadhwal, V. K.; Chakraborty, Kunal; Mostofa, K. M. G.; Tokoro, T.; Kuwae, Tomohiro; Wanninkhof, Rik</p> <p>2016-11-01</p> <p>The fugacity of <span class="hlt">CO</span><span class="hlt">2</span> (f<span class="hlt">CO</span><span class="hlt">2</span> (water)) and <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> were compared between a river-dominated anthropogenically disturbed open estuary, the Hugli, and a comparatively pristine mangrove-dominated semiclosed marine estuary, the Matla, on the east coast of India. Annual mean salinity of the Hugli Estuary (≈7.1) was much less compared to the Matla Estuary (≈20.0). All the stations of the Hugli Estuary were highly supersaturated with <span class="hlt">CO</span><span class="hlt">2</span> (annual mean 2200 µatm), whereas the Matla was marginally oversaturated (annual mean 530 µatm). During the postmonsoon season, the outer station of the Matla Estuary was under saturated with respect to <span class="hlt">CO</span><span class="hlt">2</span> and acted as a sink. The annual mean <span class="hlt">CO</span><span class="hlt">2</span> emission from the Hugli Estuary (32.4 mol C m-<span class="hlt">2</span> yr-1) was 14 times higher than the Matla Estuary (<span class="hlt">2</span>.3 mol C m-<span class="hlt">2</span> yr-1). <span class="hlt">CO</span><span class="hlt">2</span> efflux rate from the Hugli Estuary has increased drastically in the last decade, which is attributed to increased runoff from the river-dominated estuary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009BGD.....6.3481Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009BGD.....6.3481Z"><span>Conditional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> analysis of a managed grassland with the aid of stable isotopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zeeman, M. J.; Tuzson, B.; Emmenegger, L.; Knohl, A.; Buchmann, N.; Eugster, W.</p> <p>2009-04-01</p> <p>Short statured managed ecosystems, such as agricultural grasslands, exhibit high temporal changes in carbon dioxide assimilation and respiration <span class="hlt">fluxes</span> for which measurements of the net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, e.g. by using the eddy covariance (EC) method, give only limited insight. We have therefore adopted a recently proposed concept for conditional EC <span class="hlt">flux</span> analysis of forest to grasslands, in order to identify and quantify daytime sub-canopy respiration <span class="hlt">fluxes</span>. To validate the concept, high frequency (≈5 Hz) stable carbon isotope analyis of <span class="hlt">CO</span><span class="hlt">2</span> was used. We made eddy covariance measurements of <span class="hlt">CO</span><span class="hlt">2</span> and its isotopologues during four days in August 2007, using a novel quantum cascade laser absorption spectrometer, capable of high time resolution stable isotope analysis. The effects of a grass cut during the measurement period could be detected and resulted in a sub-canopy source conditional <span class="hlt">flux</span> classification, for which the isotope composition of the <span class="hlt">CO</span><span class="hlt">2</span> could be confirmed to be of a respiration source. However, the conditional <span class="hlt">flux</span> method did not work for an undisturbed grassland canopy. We attribute this to the <span class="hlt">flux</span> measurement height that was chosen well above the roughness sublayer, where the natural isotopic tracer (δ13C) of respiration was too well mixed with background <span class="hlt">air</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150001279','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150001279"><span>Quantifying the Observability of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Uncertainty in Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> Records Using Products from Nasa's Carbon Monitoring <span class="hlt">Flux</span> Pilot Project</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ott, Lesley; Pawson, Steven; Collatz, Jim; Watson, Gregg; Menemenlis, Dimitris; Brix, Holger; Rousseaux, Cecile; Bowman, Kevin; Bowman, Kevin; Liu, Junjie; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150001279'); toggleEditAbsImage('author_20150001279_show'); toggleEditAbsImage('author_20150001279_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150001279_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150001279_hide"></p> <p>2014-01-01</p> <p>NASAs Carbon Monitoring System (CMS) <span class="hlt">Flux</span> Pilot Project (FPP) was designed to better understand contemporary carbon <span class="hlt">fluxes</span> by bringing together state-of-the art models with remote sensing datasets. Here we report on simulations using NASAs Goddard Earth Observing System Model, version 5 (GEOS-5) which was used to evaluate the consistency of two different sets of observationally constrained land and ocean <span class="hlt">fluxes</span> with atmospheric <span class="hlt">CO</span><span class="hlt">2</span> records. Despite the strong data constraint, the average difference in annual terrestrial biosphere <span class="hlt">flux</span> between the two land (NASA Ames CASA and CASA-GFED) models is 1.7 Pg C for 2009-2010. Ocean models (NOBM and ECCO<span class="hlt">2</span>-Darwin) differ by 35 in their global estimates of carbon <span class="hlt">flux</span> with particularly strong disagreement in high latitudes. Based upon combinations of terrestrial and ocean <span class="hlt">fluxes</span>, GEOS-5 reasonably simulated the seasonal cycle observed at northern hemisphere surface sites and by the Greenhouse gases Observing SATellite (GOSAT) while the model struggled to simulate the seasonal cycle at southern hemisphere surface locations. Though GEOS-5 was able to reasonably reproduce the patterns of XCO<span class="hlt">2</span> observed by GOSAT, it struggled to reproduce these aspects of <span class="hlt">AIRS</span> observations. Despite large differences between land and ocean <span class="hlt">flux</span> estimates, resulting differences in atmospheric mixing ratio were small, typically less than 5 ppmv at the surface and 3 ppmv in the XCO<span class="hlt">2</span> column. A statistical analysis based on the variability of observations shows that <span class="hlt">flux</span> differences of these magnitudes are difficult to distinguish from natural variability, regardless of measurement platform.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACP....1413281T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACP....1413281T"><span>A joint data assimilation system (Tan-Tracker) to simultaneously estimate surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and 3-D atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations from observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tian, X.; Xie, Z.; Liu, Y.; Cai, Z.; Fu, Y.; Zhang, H.; Feng, L.</p> <p>2014-12-01</p> <p> precision for both <span class="hlt">CO</span><span class="hlt">2</span> concentrations and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, mainly due to the simultaneous estimation of <span class="hlt">CO</span><span class="hlt">2</span> concentrations and CFs in our Tan-Tracker data assimilation system. A experiment for assimilating the real dry-<span class="hlt">air</span> column <span class="hlt">CO</span><span class="hlt">2</span> retrievals (XCO<span class="hlt">2</span>) from the Japanese Greenhouse Gases Observation Satellite (GOSAT) further demonstrates its potential wide applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.B51E0337M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.B51E0337M"><span>Expanding Spatial and Temporal Coverage of Arctic CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murphy, P.; Oechel, W. C.; Moreaux, V.; Losacco, S.; Zona, D.</p> <p>2013-12-01</p> <p>Carbon storage and exchange in Arctic ecosystems is the subject of intensive study focused on determining rates, controls, and mechanisms of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The Arctic contains more than 1 Gt of Carbon in the upper meter of soil, both in the active layer and permafrost (Schuur et al., 2008; Tarnocai et al., 2009). However, the annual pattern and controls on the release of CH4 is inadequately understood in Arctic tundra ecosystems. Annual methane budgets are poorly understood, and very few studies measure <span class="hlt">fluxes</span> through the freeze-up cycle during autumn months (Mastepanov et al., 2008; Mastepanov et al., 2010; Sturtevant et al., 2012). There is no known, relatively continuous, CH4 <span class="hlt">flux</span> record for the Arctic. Clearly, the datasets that currently exist for budget calculations and model parameterization and verification are inadequate. This is likely due to the difficult nature of <span class="hlt">flux</span> measurements in the Arctic. In September 2012, we initiated a research project towards continuous methane <span class="hlt">flux</span> measurements along a latitudinal transect in Northern Alaska. The eddy-covariance (EC) technique is challenging in such extreme weather conditions due to the effects of <span class="hlt">ice</span> formation and precipitation on instrumentation, including gas analyzers and sonic anemometers. The challenge is greater in remote areas of the Arctic, when low power availability and limited communication can lead to delays in data retrieval or data loss. For these reasons, a combination of open- and closed-path gas analyzers, and several sonic anemometers (including one with heating), have been installed on EC towers to allow for cross-comparison and cross-referencing of calculated <span class="hlt">fluxes</span>. Newer instruments for fast CH4 <span class="hlt">flux</span> determination include: the Los Gatos Research Fast Greenhouse Gas Analyzer and the Li-Cor LI-7700. We also included the self-heated Metek Class-A uSonic-3 Anemometer as a new instrument. Previously existing instruments used for comparison include the Li-Cor LI-7500; Li-Cor LI-7200</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016LPICo1926.6099P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016LPICo1926.6099P"><span>Laboratory Investigations of Physical State of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> on Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Portyankina, G.; Merrison, J.; Iversen, J. J.; Yoldi, Z.; Hansen, C. J.; Aye, K.-M.; Pommeroll, A.</p> <p>2016-09-01</p> <p>We used Environmental Wind Tunnel to simulate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> condensation under the conditions of the martian polar areas. We find that under conditions usual for martian fall and winter, <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> always deposits from atmosphere as a translucent slab.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMPP34C..08T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMPP34C..08T"><span>Role of Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> in the <span class="hlt">Ice</span> Ages (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Toggweiler, J. R.</p> <p>2010-12-01</p> <p><span class="hlt">Ice</span> cores from Antarctica provide our most highly resolved records of glacial-interglacial climate change. They feature big transitions every 100,000 years or so in which Antarctica warms by up to 10 deg. C while the level of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> rises by up to 100 ppm. We have no other records like these from any other location, so the assumption is often made that the Earth's mean temperature varies like the temperatures in Antarctica. The striking <span class="hlt">co</span>-variation between the two records is taken to mean 1) that there is a causal relationship between the global temperature and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">2</span>) that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> is a powerful agent of climate change during the <span class="hlt">ice</span> ages. The problem is that the mechanism most often invoked to explain the <span class="hlt">CO</span><span class="hlt">2</span> variations operates right next to Antarctica and, as such, provides a fairly direct way to explain the temperature variations in Antarctica as well. If so, Antarctic temperatures go up and down for the same reason that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> goes up and down, in which case no causation can be inferred. Climate models suggest that the 100-ppm <span class="hlt">CO</span><span class="hlt">2</span> increases during the big transitions did not increase surface temperatures by more than <span class="hlt">2</span> deg. C. This is not nearly enough to explain the observed variability. A better reason for thinking that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> is important is that its temporal variations are concentrated in the 100,000-yr band. In my presentation I will argue that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> is important because it has the longest time scale in the system. We observe empirically that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> remains low for 50,000 years during the second half of each 100,000-yr cycle. The northern <span class="hlt">ice</span> sheets become especially large toward the ends of these intervals, and it is large <span class="hlt">ice</span> sheets that make the Earth especially cold. This leads me to conclude that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> is important because of its slow and persistent influence on the northern <span class="hlt">ice</span> sheets over the second half of each 100,000-yr cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1210618A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1210618A"><span>Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and abrupt climate change on submillennial timescales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahn, Jinho; Brook, Edward</p> <p>2010-05-01</p> <p>How atmospheric <span class="hlt">CO</span><span class="hlt">2</span> varies and is controlled on various time scales and under various boundary conditions is important for understanding how the carbon cycle and climate change are linked. Ancient <span class="hlt">air</span> preserved in <span class="hlt">ice</span> cores provides important information on past variations in atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. In particular, concentration records for intervals of abrupt climate change may improve understanding of mechanisms that govern atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. We present new multi-decadal <span class="hlt">CO</span><span class="hlt">2</span> records that cover Greenland stadial 9 (between Dansgaard-Oeschger (DO) events 8 and 9) and the abrupt cooling event at 8.<span class="hlt">2</span> ka. The <span class="hlt">CO</span><span class="hlt">2</span> records come from Antarctic <span class="hlt">ice</span> cores but are well synchronized with Greenland <span class="hlt">ice</span> core records using new high-resolution CH4 records,precisely defining the timing of <span class="hlt">CO</span><span class="hlt">2</span> change with respect to abrupt climate events in Greenland. Previous work showed that during stadial 9 (40~38 ka), <span class="hlt">CO</span><span class="hlt">2</span> rose by about 15~20 ppm over around <span class="hlt">2</span>,000 years, and at the same time temperatures in Antarctica increased. Dust proxies indicate a decrease in dust <span class="hlt">flux</span> over the same period. With more detailed data and better age controls we now find that approximately half of the <span class="hlt">CO</span><span class="hlt">2</span> increase during stadial 9 occurred abruptly, over the course of decades to a century at ~39.6 ka. The step increase of <span class="hlt">CO</span><span class="hlt">2</span> is synchronous with a similar step increase of Antarctic isotopic temperature and a small abrupt change in CH4, and lags after the onset of decrease in dust <span class="hlt">flux</span> by ~400 years. New atmospheric <span class="hlt">CO</span><span class="hlt">2</span> records at the well-known ~8.<span class="hlt">2</span> ka cooling event were obtained from Siple Dome <span class="hlt">ice</span> core, Antarctica. Our preliminary <span class="hlt">CO</span><span class="hlt">2</span> data span 900 years and include 19 data points within the 8.<span class="hlt">2</span> ka cooling event, which persisted for ~160 years (Thomas et al., Quarternary Sci. Rev., 2007). We find that <span class="hlt">CO</span><span class="hlt">2</span> increased by <span class="hlt">2</span>~4 ppm during that cooling event. Further analyses will improve the resolution and better constrain the <span class="hlt">CO</span><span class="hlt">2</span> variability during other times in the early Holocene to determine if the variations observed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JGRD..11210301G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JGRD..11210301G"><span>Retrieval of average <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by combining in situ <span class="hlt">CO</span><span class="hlt">2</span> measurements and backscatter lidar information</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gibert, Fabien; Schmidt, Martina; Cuesta, Juan; Ciais, Philippe; Ramonet, Michel; Xueref, IrèNe; Larmanou, Eric; Flamant, Pierre Henri</p> <p>2007-05-01</p> <p>The present paper deals with a boundary layer budgeting method which makes use of observations from various in situ and remote sensing instruments to infer regional average net ecosystem exchange (NEE) of <span class="hlt">CO</span><span class="hlt">2</span>. Measurements of <span class="hlt">CO</span><span class="hlt">2</span> within and above the atmospheric boundary layer (ABL) by in situ sensors, in conjunction with a precise knowledge of the change in ABL height by lidar and radiosoundings, enable to infer diurnal and seasonal NEE variations. Near-ground in situ <span class="hlt">CO</span> measurements are used to discriminate natural and anthropogenic contributions of <span class="hlt">CO</span><span class="hlt">2</span> diurnal variations in the ABL. The method yields mean NEE that amounts to 5 μmol m-<span class="hlt">2</span> s-1 during the night and -20 μmol m-<span class="hlt">2</span> s-1 in the middle of the day between May and July. A good agreement is found with the expected NEE accounting for a mixed wheat field and forest area during winter season, representative of the mesoscale ecosystems in the Paris area according to the trajectory of an <span class="hlt">air</span> column crossing the landscape. Daytime NEE is seen to follow the vegetation growth and the change in the ratio diffuse/direct radiation. The <span class="hlt">CO</span><span class="hlt">2</span> vertical mixing <span class="hlt">flux</span> during the rise of the atmospheric boundary layer is also estimated and seems to be the main cause of the large decrease of <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio in the morning. The outcomes on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimate are compared to eddy-covariance measurements on a barley field. The importance of various sources of error and uncertainty on the retrieval is discussed. These errors are estimated to be less than 15%; the main error resulted from anthropogenic emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3594177','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3594177"><span>Responses of Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> to Short-Term Experimental Warming in Alpine Steppe Ecosystem, Northern Tibet</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lu, Xuyang; Fan, Jihui; Yan, Yan; Wang, Xiaodan</p> <p>2013-01-01</p> <p>Soil carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) emission is one of the largest <span class="hlt">fluxes</span> in the global carbon cycle. Therefore small changes in the size of this <span class="hlt">flux</span> can have a large effect on atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations and potentially constitute a powerful positive feedback to the climate system. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the alpine steppe ecosystem of Northern Tibet and their responses to short-term experimental warming were investigated during the growing season in 2011. The results showed that the total soil <span class="hlt">CO</span><span class="hlt">2</span> emission <span class="hlt">fluxes</span> during the entire growing season were 55.82 and 104.31 g C m-<span class="hlt">2</span> for the control and warming plots, respectively. Thus, the soil <span class="hlt">CO</span><span class="hlt">2</span> emission <span class="hlt">fluxes</span> increased 86.86% with the <span class="hlt">air</span> temperature increasing 3.74°C. Moreover, the temperature sensitivity coefficient (Q 10) of the control and warming plots were <span class="hlt">2</span>.10 and 1.41, respectively. The soil temperature and soil moisture could partially explain the temporal variations of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The relationship between the temporal variation of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and the soil temperature can be described by exponential equation. These results suggest that warming significantly promoted soil <span class="hlt">CO</span><span class="hlt">2</span> emission in the alpine steppe ecosystem of Northern Tibet and indicate that this alpine ecosystem is very vulnerable to climate change. In addition, soil temperature and soil moisture are the key factors that controls soil organic matter decomposition and soil <span class="hlt">CO</span><span class="hlt">2</span> emission, but temperature sensitivity significantly decreases due to the rise in temperature. PMID:23536854</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23536854','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23536854"><span>Responses of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to short-term experimental warming in alpine steppe ecosystem, Northern Tibet.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lu, Xuyang; Fan, Jihui; Yan, Yan; Wang, Xiaodan</p> <p>2013-01-01</p> <p>Soil carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) emission is one of the largest <span class="hlt">fluxes</span> in the global carbon cycle. Therefore small changes in the size of this <span class="hlt">flux</span> can have a large effect on atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations and potentially constitute a powerful positive feedback to the climate system. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the alpine steppe ecosystem of Northern Tibet and their responses to short-term experimental warming were investigated during the growing season in 2011. The results showed that the total soil <span class="hlt">CO</span><span class="hlt">2</span> emission <span class="hlt">fluxes</span> during the entire growing season were 55.82 and 104.31 g C m(-<span class="hlt">2</span>) for the control and warming plots, respectively. Thus, the soil <span class="hlt">CO</span><span class="hlt">2</span> emission <span class="hlt">fluxes</span> increased 86.86% with the <span class="hlt">air</span> temperature increasing 3.74°C. Moreover, the temperature sensitivity coefficient (Q 10) of the control and warming plots were <span class="hlt">2</span>.10 and 1.41, respectively. The soil temperature and soil moisture could partially explain the temporal variations of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The relationship between the temporal variation of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and the soil temperature can be described by exponential equation. These results suggest that warming significantly promoted soil <span class="hlt">CO</span><span class="hlt">2</span> emission in the alpine steppe ecosystem of Northern Tibet and indicate that this alpine ecosystem is very vulnerable to climate change. In addition, soil temperature and soil moisture are the key factors that controls soil organic matter decomposition and soil <span class="hlt">CO</span><span class="hlt">2</span> emission, but temperature sensitivity significantly decreases due to the rise in temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013TCD.....7.6075R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013TCD.....7.6075R"><span>Dynamic ikaite production and dissolution in sea <span class="hlt">ice</span> - control by temperature, salinity and p<span class="hlt">CO</span><span class="hlt">2</span> conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rysgaard, S.; Wang, F.; Galley, R. J.; Grimm, R.; Lemes, M.; Geilfus, N.-X.; Chaulk, A.; Hare, A. A.; Crabeck, O.; Else, B. G. T.; Campbell, K.; Papakyriakou, T.; Sørensen, L. L.; Sievers, J.; Notz, D.</p> <p>2013-12-01</p> <p>Ikaite is a hydrous calcium carbonate mineral (Ca<span class="hlt">CO</span>3 · 6H<span class="hlt">2</span>O). It is only found in a metastable state, and decomposes rapidly once removed from near-freezing water. Recently, ikaite crystals have been found in sea <span class="hlt">ice</span> and it has been suggested that their precipitation may play an important role in <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange in <span class="hlt">ice</span>-covered seas. Little is known, however, of the spatial and temporal dynamics of ikaite in sea <span class="hlt">ice</span>. Here we present evidence for highly dynamic ikaite precipitation and dissolution in sea <span class="hlt">ice</span> grown at an out-door pool of the Sea-<span class="hlt">ice</span> Environmental Research Facility (SERF). During the experiment, ikaite precipitated in sea <span class="hlt">ice</span> with temperatures below -3 °C, creating three distinct zones of ikaite concentrations: (1) a mm to cm thin surface layer containing frost flowers and brine skim with bulk concentrations of > 2000 μmol kg-1, (<span class="hlt">2</span>) an internal layer with concentrations of 200-400 μmol kg-1 and (3) a~bottom layer with concentrations of < 100 μmol kg-1. Snowfall events caused the sea <span class="hlt">ice</span> to warm, dissolving ikaite crystals under acidic conditions. Manual removal of the snow cover allowed the sea <span class="hlt">ice</span> to cool and brine salinities to increase, resulting in rapid ikaite precipitation. The modeled (FREZCHEM) ikaite concentrations were in the same order of magnitude as observations and suggest that ikaite concentration in sea <span class="hlt">ice</span> increase with decreasing temperatures. Thus, varying snow conditions may play a key role in ikaite precipitation and dissolution in sea <span class="hlt">ice</span>. This will have implications for <span class="hlt">CO</span><span class="hlt">2</span> exchange with the atmosphere and ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C33B1201H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C33B1201H"><span>The Impact of Moisture Intrusions from Lower Latitudes on Arctic Net Surface Radiative <span class="hlt">Fluxes</span> and Sea <span class="hlt">Ice</span> Growth in Fall and Winter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hegyi, B. M.; Taylor, P. C.</p> <p>2017-12-01</p> <p>The fall and winter seasons mark an important period in the evolution of Arctic sea <span class="hlt">ice</span>, where energy is transferred away from the surface to facilitate the cooling of the surface and the growth of Arctic sea <span class="hlt">ice</span> extent and thickness. Climatologically, these seasons are characterized by distinct periods of increased and reduced surface cooling and sea <span class="hlt">ice</span> growth. Periods of reduced sea <span class="hlt">ice</span> growth and surface cooling are associated with cloudy conditions and the transport of warm and moist <span class="hlt">air</span> from lower latitudes, termed moisture intrusions. In the research presented, we explore the regional and Arctic-wide impact of moisture intrusions on the surface net radiative <span class="hlt">fluxes</span> and sea <span class="hlt">ice</span> growth for each fall and winter season from 2000/01-2015/16, utilizing MERRA<span class="hlt">2</span> reanalysis data, PIOMAS sea <span class="hlt">ice</span> thickness data, and daily CERES radiative <span class="hlt">flux</span> data. Consistent with previous studies, we find that positive anomalies in downwelling longwave surface <span class="hlt">flux</span> are associated with increased temperature and water vapor content in the atmospheric column contained within the moisture intrusions. Interestingly, there are periods of increased downwelling LW <span class="hlt">flux</span> anomalies that persist for one week or longer (i.e. longer than synoptic timescales) that are associated with persistent poleward <span class="hlt">flux</span> of warm, moist <span class="hlt">air</span> from lower latitudes. These persistent anomalies significantly reduce the regional growth of Arctic sea <span class="hlt">ice</span>, and may in part explain the interannual variability of fall and winter Arctic sea <span class="hlt">ice</span> growth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4646773','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4646773"><span>High geothermal heat <span class="hlt">flux</span> measured below the West Antarctic <span class="hlt">Ice</span> Sheet</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fisher, Andrew T.; Mankoff, Kenneth D.; Tulaczyk, Slawek M.; Tyler, Scott W.; Foley, Neil</p> <p>2015-01-01</p> <p>The geothermal heat <span class="hlt">flux</span> is a critical thermal boundary condition that influences the melting, flow, and mass balance of <span class="hlt">ice</span> sheets, but measurements of this parameter are difficult to make in <span class="hlt">ice</span>-covered regions. We report the first direct measurement of geothermal heat <span class="hlt">flux</span> into the base of the West Antarctic <span class="hlt">Ice</span> Sheet (WAIS), below Subglacial Lake Whillans, determined from the thermal gradient and the thermal conductivity of sediment under the lake. The heat <span class="hlt">flux</span> at this site is 285 ± 80 mW/m<span class="hlt">2</span>, significantly higher than the continental and regional averages estimated for this site using regional geophysical and glaciological models. Independent temperature measurements in the <span class="hlt">ice</span> indicate an upward heat <span class="hlt">flux</span> through the WAIS of 105 ± 13 mW/m<span class="hlt">2</span>. The difference between these heat <span class="hlt">flux</span> values could contribute to basal melting and/or be advected from Subglacial Lake Whillans by flowing water. The high geothermal heat <span class="hlt">flux</span> may help to explain why <span class="hlt">ice</span> streams and subglacial lakes are so abundant and dynamic in this region. PMID:26601210</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26601210','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26601210"><span>High geothermal heat <span class="hlt">flux</span> measured below the West Antarctic <span class="hlt">Ice</span> Sheet.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fisher, Andrew T; Mankoff, Kenneth D; Tulaczyk, Slawek M; Tyler, Scott W; Foley, Neil</p> <p>2015-07-01</p> <p>The geothermal heat <span class="hlt">flux</span> is a critical thermal boundary condition that influences the melting, flow, and mass balance of <span class="hlt">ice</span> sheets, but measurements of this parameter are difficult to make in <span class="hlt">ice</span>-covered regions. We report the first direct measurement of geothermal heat <span class="hlt">flux</span> into the base of the West Antarctic <span class="hlt">Ice</span> Sheet (WAIS), below Subglacial Lake Whillans, determined from the thermal gradient and the thermal conductivity of sediment under the lake. The heat <span class="hlt">flux</span> at this site is 285 ± 80 mW/m(<span class="hlt">2</span>), significantly higher than the continental and regional averages estimated for this site using regional geophysical and glaciological models. Independent temperature measurements in the <span class="hlt">ice</span> indicate an upward heat <span class="hlt">flux</span> through the WAIS of 105 ± 13 mW/m(<span class="hlt">2</span>). The difference between these heat <span class="hlt">flux</span> values could contribute to basal melting and/or be advected from Subglacial Lake Whillans by flowing water. The high geothermal heat <span class="hlt">flux</span> may help to explain why <span class="hlt">ice</span> streams and subglacial lakes are so abundant and dynamic in this region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080023465','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080023465"><span>A Preliminary Study of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Measurements by Lidar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gibert, Fabien; Koch, Grady J.; Beyon, Jeffrey Y.; Hilton, T.; Davis, Kenneth J.; Andrews, Arlyn; Ismail, Syed; Singh, Upendra N.</p> <p>2008-01-01</p> <p>A mechanistic understanding of the global carbon cycle requires quantification of terrestrial ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at regional scales. In this paper, we analyze the potential of a Doppler DIAL system to make <span class="hlt">flux</span> measurements of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> using the eddy-covariance and boundary layer budget methods and present results from a ground based experiment. The goal of this study is to put <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> point measurements in a mesoscale context. In June 2007, a field experiment combining a <span class="hlt">2</span>-m Doppler Heterodyne Differential Absorption Lidar (HDIAL) and in-situ sensors of a 447-m tall tower (WLEF) took place in Wisconsin. The HDIAL measures simultaneously: 1) <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio, <span class="hlt">2</span>) atmosphere structure via aerosol backscatter and 3) radial velocity. We demonstrate how to synthesize these data into regional <span class="hlt">flux</span> estimates. Lidar-inferred <span class="hlt">fluxes</span> are compared with eddy-covariance <span class="hlt">fluxes</span> obtained in-situ at 396m AGL from the tower. In cases where the lidar was not yet able to measure the <span class="hlt">fluxes</span> with acceptable precision, we discuss possible modifications to improve system performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000038180&hterms=dependency&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddependency','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000038180&hterms=dependency&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddependency"><span>The Role of Sea <span class="hlt">Ice</span> in <span class="hlt">2</span> x <span class="hlt">CO</span><span class="hlt">2</span> Climate Model Sensitivity. Part <span class="hlt">2</span>; Hemispheric Dependencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rind, D.; Healy, R.; Parkinson, C.; Martinson, D.</p> <p>1997-01-01</p> <p>How sensitive are doubled <span class="hlt">CO</span><span class="hlt">2</span> simulations to GCM control-run sea <span class="hlt">ice</span> thickness and extent? This issue is examined in a series of 10 control-run simulations with different sea <span class="hlt">ice</span> and corresponding doubled <span class="hlt">CO</span><span class="hlt">2</span> simulations. Results show that with increased control-run sea <span class="hlt">ice</span> coverage in the Southern Hemisphere, temperature sensitivity with climate change is enhanced, while there is little effect on temperature sensitivity of (reasonable) variations in control-run sea <span class="hlt">ice</span> thickness. In the Northern Hemisphere the situation is reversed: sea <span class="hlt">ice</span> thickness is the key parameter, while (reasonable) variations in control-run sea <span class="hlt">ice</span> coverage are of less importance. In both cases, the quantity of sea <span class="hlt">ice</span> that can be removed in the warmer climate is the determining factor. Overall, the Southern Hemisphere sea <span class="hlt">ice</span> coverage change had a larger impact on global temperature, because Northern Hemisphere sea <span class="hlt">ice</span> was sufficiently thick to limit its response to doubled <span class="hlt">CO</span><span class="hlt">2</span>, and sea <span class="hlt">ice</span> changes generally occurred at higher latitudes, reducing the sea <span class="hlt">ice</span>-albedo feedback. In both these experiments and earlier ones in which sea <span class="hlt">ice</span> was not allowed to change, the model displayed a sensitivity of -0.02 C global warming per percent change in Southern Hemisphere sea <span class="hlt">ice</span> coverage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060044030&hterms=SLP&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSLP','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060044030&hterms=SLP&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSLP"><span>Ross sea <span class="hlt">ice</span> motion, area <span class="hlt">flux</span>, and deformation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>kwok, Ron</p> <p>2005-01-01</p> <p>The sea <span class="hlt">ice</span> motion, area export, and deformation of the Ross Sea <span class="hlt">ice</span> cover are examined with satellite passive microwave and RADARSAT observations. The record of high-resolution synthetic aperture radar (SAR) data, from 1998 and 2000, allows the estimation of the variability of <span class="hlt">ice</span> deformation at the small scale (10 km) and to assess the quality of the longer record of passive microwave <span class="hlt">ice</span> motion. Daily and subdaily deformation fields and RADARSAT imagery highlight the variability of motion and deformation in the Ross Sea. With the passive microwave <span class="hlt">ice</span> motion, the area export at a <span class="hlt">flux</span> gate positioned between Cape Adare and Land Bay is estimated. Between 1992 and 2003, a positive trend can be seen in the winter (March-November) <span class="hlt">ice</span> area <span class="hlt">flux</span> that has a mean of 990 x 103 km<span class="hlt">2</span> and ranges from a low of 600 x 103 km<span class="hlt">2</span> in 1992 to a peak of 1600 x 103 km<span class="hlt">2</span> in 2001. In the mean, the southern Ross Sea produces almost twice its own area of sea <span class="hlt">ice</span> during the winter. Cross-gate sea level pressure (SLP) gradients explain 60% of the variance in the <span class="hlt">ice</span> area <span class="hlt">flux</span>. A positive trend in this gradient, from reanalysis products, suggests a 'spinup' of the Ross Sea Gyre over the past 12 yr. In both the NCEP-NCAR and ERA-40 surface pressure fields, longer-term trends in this gradient and mean SLP between 1979 and 2002 are explored along with positive anomalies in the monthly cross-gate SLP gradient associated with the positive phase of the Southern Hemisphere annular mode and the extrapolar Southern Oscillation.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS54A..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS54A..06S"><span>Evolution of Summer Ocean Mixed Layer Heat Content and Ocean/<span class="hlt">Ice</span> <span class="hlt">Fluxes</span> in the Arctic Ocean During the Last Decade</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stanton, T. P.; Shaw, W. J.</p> <p>2014-12-01</p> <p>Since 2002, a series of 28 Autonomous Ocean <span class="hlt">Flux</span> Buoys have been deployed in the Beaufort Sea and from the North Pole Environmental Observatory. These long-term <span class="hlt">ice</span>-deployed instrument systems primarily measure vertical turbulent <span class="hlt">fluxes</span> of heat, salt and momentum at a depth of <span class="hlt">2</span> - 6 m below the ocean/<span class="hlt">ice</span> interface, while concurrently measuring current profile every <span class="hlt">2</span>m down to approximately 40-50m depth, within the seasonal pycnocline. Additional sensors have been added to measure local <span class="hlt">ice</span> melt rates acoustically, and finescale thermal structure from the eddy correlation <span class="hlt">flux</span> sensor up into the <span class="hlt">ice</span> to resolve summer near-surface heating. The AOFB buoys have typically been <span class="hlt">co</span>-located with <span class="hlt">Ice</span> Tethered Profilers, that measure the upper ocean T/S structure and <span class="hlt">ice</span> mass balance instruments. Comparisons of near-surface heat <span class="hlt">fluxes</span>, heat content and vertical structure over the last decade will be made for buoys in the Beaufort Sea and Transpolar Drift between the North Pole and Spitzbergen. The effects of enhanced basal melting from <span class="hlt">ice</span>/albedo feedbacks can be clearly seen in the low <span class="hlt">ice</span> concentration summer conditions found more recently in the Beaufort Sea, while there are less pronounced effects of enhanced summer surface heating in the higher <span class="hlt">ice</span> concentrations still found in the transpolar drift.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Icar..302..175A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Icar..302..175A"><span>Mesospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds on Mars observed by Planetary Fourier Spectrometer onboard Mars Express</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aoki, S.; Sato, Y.; Giuranna, M.; Wolkenberg, P.; Sato, T. M.; Nakagawa, H.; Kasaba, Y.</p> <p>2018-03-01</p> <p>We have investigated mesospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds on Mars through analysis of near-infrared spectra acquired by Planetary Fourier Spectrometer (PFS) onboard the Mars Express (MEx) from MY 27 to MY 32. With the highest spectral resolution achieved thus far in the relevant spectral range among remote-sensing experiments orbiting Mars, PFS enables precise identification of the scattering peak of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at the bottom of the 4.3 μm <span class="hlt">CO</span><span class="hlt">2</span> band. A total of 111 occurrences of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cloud features have been detected over the period investigated. Data from the OMEGA imaging spectrometer onboard MEx confirm all of PFS detections from times when OMEGA operated simultaneously with PFS. The spatial and seasonal distributions of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds detected by PFS are consistent with previous observations by other instruments. We find <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds between Ls = 0° and 140° in distinct longitudinal corridors around the equatorial region (± 20°N). Moreover, <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds were preferentially detected at the observational LT range between 15-16 h in MY 29. However, observational biases prevent from distinguishing local time dependency from inter-annual variation. PFS also enables us to investigate the shape of mesospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cloud spectral features in detail. In all cases, peaks were found between 4.240 and 4.265 μm. Relatively small secondary peaks were occasionally observed around 4.28 μm (8 occurrences). These spectral features cannot be reproduced using our radiative transfer model, which may be because the available <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> refractive indices are inappropriate for the mesospheric temperatures of Mars, or because of the assumption in our model that the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> crystals are spherical and composed by pure <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005IAUS..235P.168B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005IAUS..235P.168B"><span>The behavior of N<span class="hlt">2</span> and O<span class="hlt">2</span> in pure, mixed or layered <span class="hlt">CO</span> <span class="hlt">ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bisschop, Suzanne E.; Fraser, Helen J.; Fuchs, Guido; Öberg, Karin I.; Acharyya, Kinsuk; van Broekhuizen, Fleur; Schlemmer, Stephan; van Dishoeck, Ewine F.</p> <p></p> <p>N<span class="hlt">2</span> and O<span class="hlt">2</span> are molecules that are predicted to be abundant in dense molecular clouds. Both molecules are difficult to detect as neither has a dipole moment. The chemical abundance of N<span class="hlt">2</span> is mostly inferred from its daughter species N<span class="hlt">2</span>H+, but was recently detected in the ISM for the first time, with an abundance of 3.3 × 10-7 (Knauth et al 2004). Searches for the submillimeter lines of O<span class="hlt">2</span> have given upper limits for the abundance of ≤ <span class="hlt">2</span>.6 10-7 for star forming clouds and ≤ 3 10-6 for cold dark clouds (Goldsmith et al. 2000). Pontoppidan et al. (2003) deduced from the <span class="hlt">CO</span> line profile that <span class="hlt">CO</span> is present in both H<span class="hlt">2</span>O poor and H<span class="hlt">2</span>O rich <span class="hlt">ice</span> layers, so it follows that N<span class="hlt">2</span> is likely to be present in a H<span class="hlt">2</span>O poor <span class="hlt">ice</span> layer. In many cold and protostellar cores N<span class="hlt">2</span>H+ is found to anti-correlate with HCO+ and <span class="hlt">CO</span> (Bergin et al. 2001; Jørgensen et al. 2004). Models by, for example Bergin & Langer (1997), assume this is due to the balance between freeze-out and evaporation, where ratios for the binding energy for N<span class="hlt">2</span> compared to <span class="hlt">CO</span> of 0.50-0.70 are used. To model these processes, and reproduce the observed abundances of each species it is important to determine empirically the binding energies, sticking probabilities and desorption kinetics of model <span class="hlt">ice</span> systems containing <span class="hlt">CO</span>, N<span class="hlt">2</span> and O<span class="hlt">2</span>. It seems that these quantities depend on the degree to which N<span class="hlt">2</span> and O<span class="hlt">2</span> mix with <span class="hlt">CO</span>. Therefore, <span class="hlt">CO</span> and N<span class="hlt">2</span> <span class="hlt">ices</span> were studied extensively in a Ultra High Vacuum (UHV) experiment (P ~ 1 × 10-10 Torr) (Oberg et al. 2005; Bisschop et al submitted)). <span class="hlt">Ice</span> samples were deposited at 14 K on a polycrystalline gold sample, mounted in the UHV chamber, covering morphologies from pure <span class="hlt">CO</span> and N<span class="hlt">2</span>, and 1:1 mixtures, to 1/1 layers of both <span class="hlt">CO</span> over N<span class="hlt">2</span> and N<span class="hlt">2</span> over <span class="hlt">CO</span>, and layers of 40 L of <span class="hlt">CO</span> (1 L ≈ 1 monolayer) covered with 5 to 50 L of N<span class="hlt">2</span>. The <span class="hlt">ices</span> were studied using a combination of Reflection Absorption Infrared Spectroscopy (RAIRS) and Temperature Programmed Desorption (TPD), at a ramp-rate of 0.1 K min-1. The TPD</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GSL.....4....9S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GSL.....4....9S"><span>Implications of overestimated anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions on East Asian and global land <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> inversion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saeki, Tazu; Patra, Prabir K.</p> <p>2017-12-01</p> <p>Measurement and modelling of regional or country-level carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">fluxes</span> are becoming critical for verification of the greenhouse gases emission control. One of the commonly adopted approaches is inverse modelling, where <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (emission: positive <span class="hlt">flux</span>, sink: negative <span class="hlt">flux</span>) from the terrestrial ecosystems are estimated by combining atmospheric <span class="hlt">CO</span><span class="hlt">2</span> measurements with atmospheric transport models. The inverse models assume anthropogenic emissions are known, and thus the uncertainties in the emissions introduce systematic bias in estimation of the terrestrial (residual) <span class="hlt">fluxes</span> by inverse modelling. Here we show that the <span class="hlt">CO</span><span class="hlt">2</span> sink increase, estimated by the inverse model, over East Asia (China, Japan, Korea and Mongolia), by about 0.26 PgC year-1 (1 Pg = 1012 g) during 2001-2010, is likely to be an artifact of the anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions increasing too quickly in China by 1.41 PgC year-1. Independent results from methane (CH4) inversion suggested about 41% lower rate of East Asian CH4 emission increase during 2002-2012. We apply a scaling factor of 0.59, based on CH4 inversion, to the rate of anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emission increase since the anthropogenic emissions of both <span class="hlt">CO</span><span class="hlt">2</span> and CH4 increase linearly in the emission inventory. We find no systematic increase in land <span class="hlt">CO</span><span class="hlt">2</span> uptake over East Asia during 1993-2010 or 2000-2009 when scaled anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions are used, and that there is a need of higher emission increase rate for 2010-2012 compared to those calculated by the inventory methods. High bias in anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions leads to stronger land sinks in global land-ocean <span class="hlt">flux</span> partitioning in our inverse model. The corrected anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions also produce measurable reductions in the rate of global land <span class="hlt">CO</span><span class="hlt">2</span> sink increase post-2002, leading to a better agreement with the terrestrial biospheric model simulations that include <span class="hlt">CO</span><span class="hlt">2</span>-fertilization and climate effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRC..120..777M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRC..120..777M"><span>Invisible polynyas: Modulation of fast <span class="hlt">ice</span> thickness by ocean heat <span class="hlt">flux</span> on the Canadian polar shelf</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melling, Humfrey; Haas, Christian; Brossier, Eric</p> <p>2015-02-01</p> <p>Although the Canadian polar shelf is dominated by thick fast <span class="hlt">ice</span> in winter, areas of young <span class="hlt">ice</span> or open water do recur annually at locations within and adjacent to the fast <span class="hlt">ice</span>. These polynyas are detectable by eye and sustained by wind or tide-driven <span class="hlt">ice</span> divergence and ocean heat <span class="hlt">flux</span>. Our <span class="hlt">ice</span>-thickness surveys by drilling and towed electromagnetic sounder reveal that visible polynyas comprise only a subset of thin-<span class="hlt">ice</span> coverage. Additional area in the coastal zone, in shallow channels and in fjords is covered by thin <span class="hlt">ice</span> which is too thick to be discerned by eye. Our concurrent surveys by CTD reveal correlation between thin fast <span class="hlt">ice</span> and above-freezing seawater beneath it. We use winter time series of <span class="hlt">air</span> and ocean temperatures and <span class="hlt">ice</span> and snow thicknesses to calculate the ocean-to-<span class="hlt">ice</span> heat <span class="hlt">flux</span> as 15 and 22 W/m<span class="hlt">2</span> at locations with thin <span class="hlt">ice</span> in Penny Strait and South Cape Fjord, respectively. Near-surface seawater above freezing is not a sufficient condition for ocean heat to reach the <span class="hlt">ice</span>; kinetic energy is needed to overcome density stratification. The ocean's isolation from wind under fast <span class="hlt">ice</span> in winter leaves tides as the only source. Two tidal mechanisms driving ocean heat <span class="hlt">flux</span> are discussed: diffusion via turbulence generated by shear at the under-<span class="hlt">ice</span> and benthic boundaries, and the internal hydraulics of flow over topography. The former appears dominant in channels and the coastal zone and the latter in some silled fjords where and when the layering of seawater density permits hydraulically critical flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1431413','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1431413"><span>Sniffle: a step forward to measure in situ <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> with the floating chamber technique</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ribas-Ribas, Mariana; Kilcher, Levi F.; Wurl, Oliver</p> <p></p> <p>Understanding how the ocean absorbs anthropogenic <span class="hlt">CO</span> <span class="hlt">2</span> is critical for predicting climate change. We designed Sniffle, a new autonomous drifting buoy with a floating chamber, to measure gas transfer velocities and <span class="hlt">air</span>-sea <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> with high spatiotemporal resolution. Currently, insufficient in situ data exist to verify gas transfer parameterizations at low wind speeds (<4 m s -1), which leads to underestimation of gas transfer velocities and, therefore, of <span class="hlt">air</span>-sea <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span>. The Sniffle is equipped with a sensor to consecutively measure aqueous and atmospheric p<span class="hlt">CO</span> <span class="hlt">2</span> and to monitor increases or decreases of <span class="hlt">CO</span> <span class="hlt">2</span> inside themore » chamber. During autonomous operation, a complete cycle lasts 40 minutes, with a new cycle initiated after flushing the chamber. The Sniffle can be deployed for up to 15 hours at wind speeds up to 10 m s -1. Floating chambers often overestimate <span class="hlt">fluxes</span> because they create additional turbulence at the water surface. We correct <span class="hlt">fluxes</span> by measuring turbulence with two acoustic Doppler velocimeters, one positioned directly under the floating chamber and the other positioned sideways, to compare artificial disturbance caused by the chamber and natural turbulence. The first results of deployment in the North Sea during the summer of 2016 demonstrate that the new drifting buoy is a useful tool that can improve our understanding of gas transfer velocity with in situ measurements. At low and moderate wind speeds and different conditions, the results obtained indicate that the observed tidal basin was acting as a source of atmospheric <span class="hlt">CO</span> <span class="hlt">2</span>. Wind speed and turbulence alone could not fully explain the variance in gas transfer velocity. We suggest therefore, that other factors like surfactants, rain or tidal current will have an impact on gas transfer parameterizations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1431413-sniffle-step-forward-measure-situ-co2-fluxes-floating-chamber-technique','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1431413-sniffle-step-forward-measure-situ-co2-fluxes-floating-chamber-technique"><span>Sniffle: a step forward to measure in situ <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> with the floating chamber technique</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ribas-Ribas, Mariana; Kilcher, Levi F.; Wurl, Oliver</p> <p>2018-01-09</p> <p>Understanding how the ocean absorbs anthropogenic <span class="hlt">CO</span> <span class="hlt">2</span> is critical for predicting climate change. We designed Sniffle, a new autonomous drifting buoy with a floating chamber, to measure gas transfer velocities and <span class="hlt">air</span>-sea <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> with high spatiotemporal resolution. Currently, insufficient in situ data exist to verify gas transfer parameterizations at low wind speeds (<4 m s -1), which leads to underestimation of gas transfer velocities and, therefore, of <span class="hlt">air</span>-sea <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span>. The Sniffle is equipped with a sensor to consecutively measure aqueous and atmospheric p<span class="hlt">CO</span> <span class="hlt">2</span> and to monitor increases or decreases of <span class="hlt">CO</span> <span class="hlt">2</span> inside themore » chamber. During autonomous operation, a complete cycle lasts 40 minutes, with a new cycle initiated after flushing the chamber. The Sniffle can be deployed for up to 15 hours at wind speeds up to 10 m s -1. Floating chambers often overestimate <span class="hlt">fluxes</span> because they create additional turbulence at the water surface. We correct <span class="hlt">fluxes</span> by measuring turbulence with two acoustic Doppler velocimeters, one positioned directly under the floating chamber and the other positioned sideways, to compare artificial disturbance caused by the chamber and natural turbulence. The first results of deployment in the North Sea during the summer of 2016 demonstrate that the new drifting buoy is a useful tool that can improve our understanding of gas transfer velocity with in situ measurements. At low and moderate wind speeds and different conditions, the results obtained indicate that the observed tidal basin was acting as a source of atmospheric <span class="hlt">CO</span> <span class="hlt">2</span>. Wind speed and turbulence alone could not fully explain the variance in gas transfer velocity. We suggest therefore, that other factors like surfactants, rain or tidal current will have an impact on gas transfer parameterizations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900048282&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dphysical%2Bdependence','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900048282&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dphysical%2Bdependence"><span>The physical and infrared spectral properties of <span class="hlt">CO</span><span class="hlt">2</span> in astrophysical <span class="hlt">ice</span> analogs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sandford, S. A.; Allamandola, L. J.</p> <p>1990-01-01</p> <p>Results of measurements of the infrared spectroscopic and condensation-vaporization properties of <span class="hlt">CO</span><span class="hlt">2</span> in pure and mixed <span class="hlt">ices</span> are presented. Detailed examination of five infrared <span class="hlt">CO</span><span class="hlt">2</span> bands, <span class="hlt">2</span>.20, <span class="hlt">2</span>.78, 4.27, 15.<span class="hlt">2</span>, and 4.39 microns, shows that the peak position, FWHM, and profile of the bands provide important information about the composition, formation, and subsequent thermal history of the <span class="hlt">ices</span>. Absorption coefficients and their temperature dependence for all five <span class="hlt">CO</span><span class="hlt">2</span> bands are determined. The temperature dependence variation is found to be less than 15 percent from 10 to 150 K, i.e., the temperature at which H<span class="hlt">2</span>O <span class="hlt">ice</span> sublimes. The number of parameters associated with the physical behavior of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">CO</span><span class="hlt">2</span>- and H<span class="hlt">2</span>O-rich <span class="hlt">ices</span>, including surface binding energies, and condensation and sublimation temperatures, are determined under experimental conditions. The implications of the data obtained for cometary models are considered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.B53C0683C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.B53C0683C"><span>Coupling of N<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from agriculture in Michigan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cui, M.; Tang, J.; Hastings, M. G.; Gelfand, I.; Tao, L.; Sun, K.</p> <p>2012-12-01</p> <p><span class="hlt">CO</span><span class="hlt">2</span> has been known to cause global warming, and N<span class="hlt">2</span>O is the largest contributor to the greenhouse gas burden of cropping systems in the United States due to application of fertilizer. In our study, <span class="hlt">fluxes</span> of N<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> were measured at two maize fields and one reference grassland from Kellogg Biological Station in Southwest Michigan. Here we compared two measuring systems, traditional GC method and LGR/Li-Cor system. Our initial results show that the two measuring systems are consistent (N<span class="hlt">2</span>O slope=0.96, R<span class="hlt">2</span>=0.96; and <span class="hlt">CO</span><span class="hlt">2</span> slope= 1.03, R<span class="hlt">2</span>=0.86 measuring from the same chamber). Measurements done in pairs of chambers suggest great spatial variations, despite that the chambers were only 0.5 meter apart. The two systems are still comparable by averaging 8 pairs of chambers distributed within one site. Increase of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were observed the second day after fertilization, but no significant change of N<span class="hlt">2</span>O <span class="hlt">fluxes</span> was shown. After artificial rainfall, boosting N<span class="hlt">2</span>O <span class="hlt">fluxes</span> and further increase in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were demonstrated. Our result indicates that precipitation is necessary before a prominent N<span class="hlt">2</span>O peak. In our LGR/Li-Cor system, <span class="hlt">CO</span> was also measured from chambers. Interesting <span class="hlt">CO</span> <span class="hlt">fluxes</span> were shown in our experiment. Soil, which is usually considered as a <span class="hlt">CO</span> sink, emits <span class="hlt">CO</span> in some chambers during our measurement, which is probably related to the nationwide forest fires and lack of precipitation during the period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRC..121.1229W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRC..121.1229W"><span>On the calculation of <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> in the presence of temperature and salinity gradients</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Woolf, D. K.; Land, P. E.; Shutler, J. D.; Goddijn-Murphy, L. M.; Donlon, C. J.</p> <p>2016-02-01</p> <p>The presence of vertical temperature and salinity gradients in the upper ocean and the occurrence of variations in temperature and salinity on time scales from hours to many years complicate the calculation of the <span class="hlt">flux</span> of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) across the sea surface. Temperature and salinity affect the interfacial concentration of aqueous <span class="hlt">CO</span><span class="hlt">2</span> primarily through their effect on solubility with lesser effects related to saturated vapor pressure and the relationship between fugacity and partial pressure. The effects of temperature and salinity profiles in the water column and changes in the aqueous concentration act primarily through the partitioning of the carbonate system. Climatological calculations of <span class="hlt">flux</span> require attention to variability in the upper ocean and to the limited validity of assuming "constant chemistry" in transforming measurements to climatological values. Contrary to some recent analysis, it is shown that the effect on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of a cool skin on the sea surface is large and ubiquitous. An opposing effect on calculated <span class="hlt">fluxes</span> is related to the occurrence of warm layers near the surface; this effect can be locally large but will usually coincide with periods of low exchange. A salty skin and salinity anomalies in the upper ocean also affect <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> calculations, though these haline effects are generally weaker than the thermal effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.2190Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.2190Q"><span>Development of a laser remote sensing instrument to measure sub-aerial volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Queisser, Manuel; Burton, Mike</p> <p>2016-04-01</p> <p>A thorough quantification of volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> would lead to an enhanced understanding of the role of volcanoes in the geological carbon cycle. This would enable a more subtle understanding of human impact on that cycle. Furthermore, variations in volcanic <span class="hlt">CO</span><span class="hlt">2</span> emissions are a key to understanding volcanic processes such as eruption phenomenology. However, measuring <span class="hlt">fluxes</span> of volcanic <span class="hlt">CO</span><span class="hlt">2</span> is challenging as volcanic <span class="hlt">CO</span><span class="hlt">2</span> concentrations are modest compared with the ambient <span class="hlt">CO</span><span class="hlt">2</span> concentration (~400 ppm) . Volcanic <span class="hlt">CO</span><span class="hlt">2</span> quickly dilutes with the background <span class="hlt">air</span>. For Mt. Etna (Italy), for instance, 1000 m downwind from the crater, dispersion modelling yields a signal of ~4 ppm only. It is for this reason that many magmatic <span class="hlt">CO</span><span class="hlt">2</span> concentration measurements focus on in situ techniques, such as direct sampling Giggenbach bottles, chemical sensors, IR absorption spectrometers or mass spectrometers. However, emission rates are highly variable in time and space. Point measurements fail to account for this variability. Inferring 1-D or <span class="hlt">2</span>-D gas concentration profiles, necessary to estimate gas <span class="hlt">fluxes</span>, from point measurements may thus lead to erroneous <span class="hlt">flux</span> estimations. Moreover, in situ probing is time consuming and, since many volcanoes emit toxic gases and are dangerous as mountains, may raise safety concerns. In addition, degassing is often diffuse and spatially extended, which makes a measurement approach with spatial coverage desirable. There are techniques that allow to indirectly retrieve <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from correlated SO<span class="hlt">2</span> concentrations and <span class="hlt">fluxes</span>. However, they still rely on point measurements of <span class="hlt">CO</span><span class="hlt">2</span> and are prone to errors of SO<span class="hlt">2</span> <span class="hlt">fluxes</span> due to light dilution and depend on blue sky conditions. Here, we present a new remote sensing instrument, developed with the ERC project <span class="hlt">CO</span><span class="hlt">2</span>Volc, which measures 1-D column amounts of <span class="hlt">CO</span><span class="hlt">2</span> in the atmosphere with sufficient sensitivity to reveal the contribution of magmatic <span class="hlt">CO</span><span class="hlt">2</span>. Based on differential absorption LIDAR (DIAL) the instrument measures</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN12C..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN12C..01H"><span>Evaluation of Deep Learning Models for Predicting <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halem, M.; Nguyen, P.; Frankel, D.</p> <p>2017-12-01</p> <p>Artificial neural networks have been employed to calculate surface <span class="hlt">flux</span> measurements from station data because they are able to fit highly nonlinear relations between input and output variables without knowing the detail relationships between the variables. However, the accuracy in performing neural net estimates of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from observations of <span class="hlt">CO</span><span class="hlt">2</span> and other atmospheric variables is influenced by the architecture of the neural model, the availability, and complexity of interactions between physical variables such as wind, temperature, and indirect variables like latent heat, and sensible heat, etc. We evaluate two deep learning models, feed forward and recurrent neural network models to learn how they each respond to the physical measurements, time dependency of the measurements of <span class="hlt">CO</span><span class="hlt">2</span> concentration, humidity, pressure, temperature, wind speed etc. for predicting the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. In this paper, we focus on a) building neural network models for estimating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> based on DOE data from tower Atmospheric Radiation Measurement data; b) evaluating the impact of choosing the surface variables and model hyper-parameters on the accuracy and predictions of surface <span class="hlt">flux</span>; c) assessing the applicability of the neural network models on estimate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> by using OCO-<span class="hlt">2</span> satellite data; d) studying the efficiency of using GPU-acceleration for neural network performance using IBM Power AI deep learning software and packages on IBM Minsky system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...854...13P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...854...13P"><span>Modeling <span class="hlt">CO</span>, <span class="hlt">CO</span><span class="hlt">2</span>, and H<span class="hlt">2</span>O <span class="hlt">Ice</span> Abundances in the Envelopes of Young Stellar Objects in the Magellanic Clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pauly, Tyler; Garrod, Robin T.</p> <p>2018-02-01</p> <p>Massive young stellar objects (MYSOs) in the Magellanic Clouds show infrared absorption features corresponding to significant abundances of <span class="hlt">CO</span>, <span class="hlt">CO</span><span class="hlt">2</span>, and H<span class="hlt">2</span>O <span class="hlt">ice</span> along the line of sight, with the relative abundances of these <span class="hlt">ices</span> differing between the Magellanic Clouds and the Milky Way. <span class="hlt">CO</span> <span class="hlt">ice</span> is not detected toward sources in the Small Magellanic Cloud, and upper limits put its relative abundance well below sources in the Large Magellanic Cloud and the Milky Way. We use our gas-grain chemical code MAGICKAL, with multiple grain sizes and grain temperatures, and further expand it with a treatment for increased interstellar radiation field intensity to model the elevated dust temperatures observed in the MCs. We also adjust the elemental abundances used in the chemical models, guided by observations of H II regions in these metal-poor satellite galaxies. With a grid of models, we are able to reproduce the relative <span class="hlt">ice</span> fractions observed in MC MYSOs, indicating that metal depletion and elevated grain temperature are important drivers of the MYSO envelope <span class="hlt">ice</span> composition. Magellanic Cloud elemental abundances have a subgalactic <span class="hlt">C/O</span> ratio, increasing H<span class="hlt">2</span>O <span class="hlt">ice</span> abundances relative to the other <span class="hlt">ices</span>; elevated grain temperatures favor <span class="hlt">CO</span><span class="hlt">2</span> production over H<span class="hlt">2</span>O and <span class="hlt">CO</span>. The observed shortfall in <span class="hlt">CO</span> in the Small Magellanic Cloud can be explained by a combination of reduced carbon abundance and increased grain temperatures. The models indicate that a large variation in radiation field strength is required to match the range of observed LMC abundances. CH3OH abundance is found to be enhanced in low-metallicity models, providing seed material for complex organic molecule formation in the Magellanic Clouds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43C2468M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43C2468M"><span>Constraints on Southern Ocean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> and Seasonality from Atmospheric Vertical Gradients Observed on Multiple Airborne Campaigns</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McKain, K.; Sweeney, C.; Stephens, B. B.; Long, M. C.; Jacobson, A. R.; Basu, S.; Chatterjee, A.; Weir, B.; Wofsy, S. C.; Atlas, E. L.; Blake, D. R.; Montzka, S. A.; Stern, R.</p> <p>2017-12-01</p> <p>The Southern Ocean plays an important role in the global carbon cycle and climate system, but net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> into the Southern Ocean is difficult to measure and model because it results from large opposing and seasonally-varying <span class="hlt">fluxes</span> due to thermal forcing, biological uptake, and deep-water mixing. We present an analysis to constrain the seasonal cycle of net <span class="hlt">CO</span><span class="hlt">2</span> exchange with the Southern Ocean, and the magnitude of summer uptake, using the vertical gradients in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> observed during three aircraft campaigns in the southern polar region. The O<span class="hlt">2</span>/N<span class="hlt">2</span> Ratio and <span class="hlt">CO</span><span class="hlt">2</span> Airborne Southern Ocean Study (ORCAS) was an airborne campaign that intensively sampled the atmosphere at 0-13 km altitude and 45-75 degrees south latitude in the austral summer (January-February) of 2016. The global airborne campaigns, the HIAPER Pole-to-Pole Observations (HIPPO) study and the Atmospheric Tomography Mission (ATom), provide additional measurements over the Southern Ocean from other seasons and multiple years (2009-2011, 2016-2017). Derivation of <span class="hlt">fluxes</span> from measured vertical gradients requires robust estimates of the residence time of <span class="hlt">air</span> in the polar tropospheric domain, and of the contribution of long-range transport from northern latitudes outside the domain to the <span class="hlt">CO</span><span class="hlt">2</span> gradient. We use diverse independent approaches to estimate both terms, including simulations using multiple transport and <span class="hlt">flux</span> models, and observed gradients of shorter-lived tracers with specific sources regions and well-known loss processes. This study demonstrates the utility of aircraft profile measurements for constraining large-scale <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> for the Southern Ocean, in contrast to those derived from the extrapolation of sparse ocean and atmospheric measurements and uncertain <span class="hlt">flux</span> parameterizations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.C13C0833H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.C13C0833H"><span>A New Fast, Reliable Technique for the Sampling of Dissolved Inorganic Carbon in Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, Y.; Wang, F.; Rysgaard, S.; Barber, D. G.</p> <p>2015-12-01</p> <p>For a long time, sea <span class="hlt">ice</span> was considered to act as a lid over seawater preventing <span class="hlt">CO</span><span class="hlt">2</span> exchange between the atmosphere and ocean. Recent observations suggest that sea <span class="hlt">ice</span> can be an active source or a sink for <span class="hlt">CO</span><span class="hlt">2</span>, although its magnitude is not very clear. The direct measurements on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> based on the chamber method and eddy covariance often do not agree with each other. It is therefore important to measure the dissolved inorganic carbon (DIC) stock in sea <span class="hlt">ice</span> precisely in order to better understand the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> through sea <span class="hlt">ice</span>. The challenges in sea <span class="hlt">ice</span> DIC sampling is how to melt the <span class="hlt">ice</span> core without being exposed to the <span class="hlt">air</span> gaining or losing <span class="hlt">CO</span><span class="hlt">2</span>. A common practice is to seal the <span class="hlt">ice</span> core in a self-prepared gas-tight plastic bag and suck the <span class="hlt">air</span> out of the bag gently using a syringe (together with a needle) through a valve mounted on one side of the bag. However, this method is time consuming (takes up to several minutes to suck the <span class="hlt">air</span> out) and very often there is large headspace found in the bag after the <span class="hlt">ice</span> melts due to the imperfect bag-preparation, which might affect the DIC concentration in melt <span class="hlt">ice</span>-water. We developed a new technique by using a commercially available plastic bag with a vacuum sealer to seal the <span class="hlt">ice</span> core. In comparison to syringe-based method, this technique is fast and easy to operate; it takes less than 10 seconds to vacuum and seal the bag all in one button with no headspace left in the bag. Experimental tests with replicate <span class="hlt">ice</span> cores sealed by those two methods showed that there is no difference in the DIC concentration measured after these two methods, suggesting that there is no loss of DIC during the course of vacuum sealing. In addition, a time series experiment on DIC in melt <span class="hlt">ice</span>-water stored in the new bag shows that when the samples were not poisoned, the DIC concentration remains unchanged for at least 3 days in the bag; while poisoned by HgCl<span class="hlt">2</span>, there is no change in DIC for at least 21 days, indicating that this new bag is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A34B..03F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A34B..03F"><span>Estimating regional <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> using GOSAT XCO<span class="hlt">2</span> and XCH4 observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fraser, A. C.; Palmer, P. I.; Feng, L.; Parker, R.; Boesch, H.; Cogan, A. J.</p> <p>2012-12-01</p> <p>We infer regional monthly surface <span class="hlt">flux</span> estimates for <span class="hlt">CO</span><span class="hlt">2</span> and CH4, June 2009-December 2010, from proxy dry-<span class="hlt">air</span> column-averaged mole fractions of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 from the Greenhouse gases Observing SATellite (GOSAT) using an ensemble Kalman Filter combined with the GEOS-Chem chemistry transport model. We compare these <span class="hlt">flux</span> estimates with estimates inferred from in situ surface mole fraction measurements and from combining in situ and GOSAT measurements in order to quantify the added value of GOSAT data above the conventional surface measurement network. We find that the error reduction, a measure of how much the posterior <span class="hlt">fluxes</span> are being informed by the assimilated data, at least doubles when GOSAT measurements are used versus the surface only inversions, with the exception of regions that are well covered by the surface network at the spatial and temporal resolution of our <span class="hlt">flux</span> estimation calculation. We have incorporated a new online bias correction scheme to account for GOSAT biases. We report global and regional <span class="hlt">flux</span> estimates inferred from GOSAT and/or in situ measurements. While the global posterior <span class="hlt">fluxes</span> from GOSAT and in situ measurements agree, we find significant differences in the regional <span class="hlt">fluxes</span>, particularly over the tropics. We evaluate the posterior <span class="hlt">fluxes</span> by comparing them against independent surface mole fraction, column, and aircraft measurements using the GEOS-Chem model as an intermediary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007BGD.....4.2279K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007BGD.....4.2279K"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> determination by closed-chamber methods can be seriously biased by inappropriate application of linear regression</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kutzbach, L.; Schneider, J.; Sachs, T.; Giebels, M.; Nykänen, H.; Shurpali, N. J.; Martikainen, P. J.; Alm, J.; Wilmking, M.</p> <p>2007-07-01</p> <p>Closed (non-steady state) chambers are widely used for quantifying carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">fluxes</span> between soils or low-stature canopies and the atmosphere. It is well recognised that covering a soil or vegetation by a closed chamber inherently disturbs the natural <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by altering the concentration gradients between the soil, the vegetation and the overlying <span class="hlt">air</span>. Thus, the driving factors of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are not constant during the closed chamber experiment, and no linear increase or decrease of <span class="hlt">CO</span><span class="hlt">2</span> concentration over time within the chamber headspace can be expected. Nevertheless, linear regression has been applied for calculating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in many recent, partly influential, studies. This approach was justified by keeping the closure time short and assuming the concentration change over time to be in the linear range. Here, we test if the application of linear regression is really appropriate for estimating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using closed chambers over short closure times and if the application of nonlinear regression is necessary. We developed a nonlinear exponential regression model from diffusion and photosynthesis theory. This exponential model was tested with four different datasets of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements (total number: 1764) conducted at three peatland sites in Finland and a tundra site in Siberia. The <span class="hlt">flux</span> measurements were performed using transparent chambers on vegetated surfaces and opaque chambers on bare peat surfaces. Thorough analyses of residuals demonstrated that linear regression was frequently not appropriate for the determination of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by closed-chamber methods, even if closure times were kept short. The developed exponential model was well suited for nonlinear regression of the concentration over time c(t) evolution in the chamber headspace and estimation of the initial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at closure time for the majority of experiments. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates by linear regression can be as low as 40% of the <span class="hlt">flux</span> estimates of exponential regression for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BGeo...14.5727K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BGeo...14.5727K"><span>Low p<span class="hlt">CO</span><span class="hlt">2</span> under sea-<span class="hlt">ice</span> melt in the Canada Basin of the western Arctic Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosugi, Naohiro; Sasano, Daisuke; Ishii, Masao; Nishino, Shigeto; Uchida, Hiroshi; Yoshikawa-Inoue, Hisayuki</p> <p>2017-12-01</p> <p>In September 2013, we observed an expanse of surface water with low <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>sea) (< 200 µatm) in the Chukchi Sea of the western Arctic Ocean. The large undersaturation of <span class="hlt">CO</span><span class="hlt">2</span> in this region was the result of massive primary production after the sea-<span class="hlt">ice</span> retreat in June and July. In the surface of the Canada Basin, salinity was low (< 27) and p<span class="hlt">CO</span><span class="hlt">2</span>sea was closer to the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> equilibrium (˜ 360 µatm). From the relationships between salinity and total alkalinity, we confirmed that the low salinity in the Canada Basin was due to the larger fraction of meltwater input (˜ 0.16) rather than the riverine discharge (˜ 0.1). Such an increase in p<span class="hlt">CO</span><span class="hlt">2</span>sea was not so clear in the coastal region near Point Barrow, where the fraction of riverine discharge was larger than that of sea-<span class="hlt">ice</span> melt. We also identified low p<span class="hlt">CO</span><span class="hlt">2</span>sea (< 250 µatm) in the depth of 30-50 m under the halocline of the Canada Basin. This subsurface low p<span class="hlt">CO</span><span class="hlt">2</span>sea was attributed to the advection of Pacific-origin water, in which dissolved inorganic carbon is relatively low, through the Chukchi Sea where net primary production is high. Oxygen supersaturation (> 20 µmol kg-1) in the subsurface low p<span class="hlt">CO</span><span class="hlt">2</span>sea layer in the Canada Basin indicated significant net primary production undersea and/or in preformed condition. If these low p<span class="hlt">CO</span><span class="hlt">2</span>sea layers surface by wind mixing, they will act as additional <span class="hlt">CO</span><span class="hlt">2</span> sinks; however, this is unlikely because intensification of stratification by sea-<span class="hlt">ice</span> melt inhibits mixing across the halocline.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.14501003D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.14501003D"><span>Investigating cosmic rays and <span class="hlt">air</span> shower physics with <span class="hlt">IceCube/Ice</span>Top</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dembinski, Hans</p> <p>2017-06-01</p> <p><span class="hlt">Ice</span>Cube is a cubic-kilometer detector in the deep <span class="hlt">ice</span> at South Pole. Its square-kilometer surface array, <span class="hlt">Ice</span>Top, is located at 2800 m altitude. <span class="hlt">Ice</span>Top is large and dense enough to cover the cosmic-ray energy spectrum from PeV to EeV energies with a remarkably small systematic uncertainty, thanks to being close to the shower maximum. The experiment offers new insights into hadronic physics of <span class="hlt">air</span> showers by observing three components: the electromagnetic signal at the surface, GeV muons in the periphery of the showers, and TeV muons in the deep <span class="hlt">ice</span>. The cosmic-ray <span class="hlt">flux</span> is measured with the surface signal. The mass composition is extracted from the energy loss of TeV muons observed in the deep <span class="hlt">ice</span> in coincidence with signals at the surface. The muon lateral distribution is obtained from GeV muons identified in surface signals in the periphery of the shower. The energy spectrum of the most energetic TeV muons is also under study, as well as special events with laterally separated TeV muon tracks which originate from high-pT TeV muons. A combination of all these measurements opens the possibility to perform powerful new tests of hadronic interaction models used to simulate <span class="hlt">air</span> showers. The latest results will be reviewed from this perspective.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005616','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005616"><span>Comparing Global Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> and Transport Models with Remote Sensing (and Other) Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kawa, S. R.; Collatz, G. J.; Pawson, S.; Wennberg, P. O.; Wofsy, S. C.; Andrews, A. E.</p> <p>2010-01-01</p> <p>We report recent progress derived from comparison of global <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and transport models with new remote sensing and other sources of <span class="hlt">CO</span><span class="hlt">2</span> data including those from satellite. The overall objective of this activity is to improve the process models that represent our understanding of the workings of the atmospheric carbon cycle. Model estimates of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">flux</span> and atmospheric transport processes are required for initial constraints on inverse analyses, to connect atmospheric observations to the location of surface sources and sinks, to provide the basic framework for carbon data assimilation, and ultimately for future projections of carbon-climate interactions. Models can also be used to test consistency within and between <span class="hlt">CO</span><span class="hlt">2</span> data sets under varying geophysical states. Here we focus on simulated <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from terrestrial vegetation and atmospheric transport mutually constrained by analyzed meteorological fields from the Goddard Modeling and Assimilation Office for the period 2000 through 2009. Use of assimilated meteorological data enables direct model comparison to observations across a wide range of scales of variability. The biospheric <span class="hlt">fluxes</span> are produced by the CASA model at 1x1 degrees on a monthly mean basis, modulated hourly with analyzed temperature and sunlight. Both physiological and biomass burning <span class="hlt">fluxes</span> are derived using satellite observations of vegetation, burned area (as in GFED-3), and analyzed meteorology. For the purposes of comparison to <span class="hlt">CO</span><span class="hlt">2</span> data, fossil fuel and ocean <span class="hlt">fluxes</span> are also included in the transport simulations. In this presentation we evaluate the model's ability to simulate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and mixing ratio variability in comparison to remote sensing observations from TCCON, GOSAT, and <span class="hlt">AIRS</span> as well as relevant in situ observations. Examples of the influence of key process representations are shown from both forward and inverse model comparisons. We find that the model can resolve much of the synoptic, seasonal, and interannual</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.C21A0064F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.C21A0064F"><span>Measurements of Turbulent <span class="hlt">Fluxes</span> over Sea <span class="hlt">Ice</span> Region in the Sea of Okhotsk.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fujisaki, A.; Yamaguchi, H.; Toyota, T.; Futatsudera, A.; Miyanaga, M.</p> <p>2007-12-01</p> <p>The measurements of turbulent <span class="hlt">fluxes</span> over sea <span class="hlt">ice</span> area were done in the southern part of the Sea of Okhotsk, during the cruises of the <span class="hlt">ice</span>-breaker P/V 'Soya' in 2000-2005. The <span class="hlt">air-ice</span> drag coefficients CDN were 3.57×10-3 over small floes \\left(diameter:φ=20- 100m\\right), 3.38×10-3 over medium floes \\left(φ=100-500m\\right), and <span class="hlt">2</span>.12×10-3 over big floes \\left( φ=500m-<span class="hlt">2</span>km\\right), which showed a decrease with the increase of floe size. This is because the smaller floes contribue to the roughness of sea-<span class="hlt">ice</span> area by their edges more than the larger ones. The average CDN values showed a gradual upslope with <span class="hlt">ice</span> concentration, which is simply due to the rougher surface of sea <span class="hlt">ice</span> than that of open water, while they showed a slight decline at <span class="hlt">ice</span> concentration 100%, which is possibly due to the lack of freeboard effect of lateral side of floes. We also compared the relation between the roughness length zM and the friction velocity u* with the model developed in the previous study. The zM-u* relation well corresponded with the model results, while the range of zM we obtained was larger than those obtained at the <span class="hlt">Ice</span> Station Weddell and during the Surface Heat Budget of the Arctic Ocean project. The sensible heat transfer coefficients CHN were 1.35×10-3 at 80-90% <span class="hlt">ice</span> concentration, and 0.95×10-3 at 100% <span class="hlt">ice</span> concentration, which are comparable with the results of the past reaserches. On the other hand, we obtained a maximum CHN value of <span class="hlt">2</span>.39×10-3at 20-50% <span class="hlt">ice</span> concentration, and <span class="hlt">2</span>.35×10-3 over open water, which are more than twice as the typical value of 1.0×10-3 over open water. These large CHN values are due to the significant upward sensible heat <span class="hlt">flux</span> during the measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.A53B1167B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.A53B1167B"><span>Firn-<span class="hlt">air</span> Properties and Influences at the West Antarctic <span class="hlt">Ice</span> Sheet Divide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Battle, M. O.; Severinghaus, J. P.; Montzka, S. A.; Sofen, E. D.; Tans, P. P.</p> <p>2007-12-01</p> <p>In December 2005, we collected samples of firn <span class="hlt">air</span> from a pair of dedicated boreholes drilled at the West Antarctic <span class="hlt">Ice</span> Sheet Divide (WAIS-D), immediately adjacent to the WAIS-D deep <span class="hlt">ice</span> coring effort currently underway at 79° 28'S, 112° 7'W at an elevation of ~1800m. The site is characterized by moderate temperatures (annual mean of -31°C) and moderate accumulation (24 cm/yr <span class="hlt">ice</span>-equivalent). These samples were analyzed for a wide variety of atmospheric species by laboratories at the Scripps Institution of Oceanography, NOAA-ESRL, University of Colorado/INSTAAR, UC Irvine and Penn. State University. In this presentation, we focus on general properties of the firn <span class="hlt">air</span> at this site and the influences on its composition, as inferred from concentration data for <span class="hlt">CO</span><span class="hlt">2</span>, CH4, and a range of halogenated species, as well as the stable isotope ratios of N<span class="hlt">2</span> and several noble gases. Preliminary analyses indicate the presence of a shallow convective zone (a few meters or less), a diffusive region extending down to roughly 65m and a lock-in zone from 65m to the firn-<span class="hlt">ice</span> transition at 76.5m. There is also evidence of a thermally-driven seasonal cycle in composition in the upper 25m of the firn. Modeling studies indicate that the accumulation rate at this site is low enough that the downward advection of <span class="hlt">air</span> accompanying firn compression has a very small influence on the firn <span class="hlt">air</span> profile. <span class="hlt">Air</span> at the bottom of the diffusive column has a <span class="hlt">CO</span><span class="hlt">2</span>-based age of 10-15 years (depending on the definition of "mean age"), while the <span class="hlt">air</span> at the firn-<span class="hlt">ice</span> transition is ~38 years old. Concentrations of halogenated species in the samples collected imply atmospheric histories that are generally consistent with those derived from direct atmospheric measurements and from firn <span class="hlt">air</span> collected at other sites. Additional properties of the <span class="hlt">air</span>, and their controlling processes will also be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.473..860H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.473..860H"><span>Characterization of thin film <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> through the infrared ν1 + ν3 combination mode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Jiao; Vidali, Gianfranco</p> <p>2018-01-01</p> <p>Carbon dioxide is abundant in <span class="hlt">ice</span> mantles of dust grains; some is found in the pure crystalline form as inferred from the double peak splitting of the bending profile at about 650 cm-1. To study how <span class="hlt">CO</span><span class="hlt">2</span> segregates into the pure form from water-rich mixtures of <span class="hlt">ice</span> mantles and how it then crystallizes, we used Reflection Absorption InfraRed Spectroscopy to study the structural change of pure <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> as a function of both <span class="hlt">ice</span> thickness and temperature. We found that the ν1 + ν3 combination mode absorption profile at 3708 cm-1 provides an excellent probe to quantify the degree of crystallinity in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. We also found that between 20 and 30 K, there is an ordering transition that we attribute to reorientation of <span class="hlt">CO</span><span class="hlt">2</span> molecules, while the diffusion of <span class="hlt">CO</span><span class="hlt">2</span> becomes significant at much higher temperatures. In the formation of pure crystalline <span class="hlt">CO</span><span class="hlt">2</span> in interstellar medium <span class="hlt">ices</span>, the rate limiting process is the diffusion/segregation of <span class="hlt">CO</span><span class="hlt">2</span> molecules in the <span class="hlt">ice</span> instead of the phase transition from amorphous to crystalline after clusters/islands of <span class="hlt">CO</span><span class="hlt">2</span> are formed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.8639K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.8639K"><span>Net drainage effects on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of a permafrost ecosystem through eddy-covariance measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kittler, Fanny; Burjack, Ina; Zimov, Nikita; Zimov, Sergey; Heimann, Martin; Göckede, Mathias</p> <p>2015-04-01</p> <p>Permafrost landscapes in the Northern high latitudes with their massive organic carbon stocks are critically important for the global carbon cycle, yet feedback processes with the atmosphere under future climate conditions are uncertain. To improve the understanding of mechanisms and drivers dominating permafrost carbon cycling, we established a continuous observation program in moist tussock tundra ecosystem near Cherskiy in North-eastern Siberia (68.75°N, 161.33°E). The experiment has been designed to monitor carbon cycle <span class="hlt">fluxes</span> at different scales with different approaches, including e.g. the eddy-covariance technique, and their environmental drivers. Recent observations started mid July 2013 and are still ongoing, while 'historic' measurements are available for the period 2002-2005. Since 2004 part of the observation area has been disturbed by a drainage ditch ring, altering the soil water conditions in the surrounding area in a way that is expected for degrading <span class="hlt">ice</span>-rich permafrost under a warming climate. With parallel observations over the disturbed (drained) area and a reference area nearby, respectively, we aim to evaluate the disturbance effect on the carbon cycle budgets and the dominating biogeochemical mechanisms. Here, findings based on over 1.5 years of continuous eddy-covariance <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements (July 2013 - March 2015) for both observation areas are presented. Results show systematic shifts in the tundra ecosystem as a result of 10 years of disturbance in the drained area, with significant effects on biotic and abiotic site conditions as well as on the carbon cycle dynamics. Comparing the net budget <span class="hlt">fluxes</span> between both observations areas indicates a reduction of the net sink strength for <span class="hlt">CO</span><span class="hlt">2</span> of the drained ecosystem during the summer season in comparison to natural conditions, mostly caused by reduced <span class="hlt">CO</span><span class="hlt">2</span> uptake with low water levels in late summer. Regarding the long-term <span class="hlt">CO</span><span class="hlt">2</span> uptake dynamics of the disturbance regime (2005 vs. 2013/14) the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521483-chemical-evolution-co-ice-induced-soft-rays','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521483-chemical-evolution-co-ice-induced-soft-rays"><span>CHEMICAL EVOLUTION OF A <span class="hlt">CO</span> <span class="hlt">ICE</span> INDUCED BY SOFT X-RAYS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ciaravella, A.; Cecchi-Pestellini, C.; Jiménez-Escobar, A.</p> <p>2016-03-01</p> <p>We irradiated a pure carbon monoxide <span class="hlt">ice</span> with soft X-rays of energies up to 1.<span class="hlt">2</span> keV. The experiments were performed using the spherical grating monochromator beamline at the National Synchrotron Radiation Research Center in Taiwan, exploiting both monochromatic (at 0.3 and 0.55 keV) and broader energy (0.25–1.<span class="hlt">2</span> keV) <span class="hlt">fluxes</span>. The infrared spectra of the irradiated <span class="hlt">ices</span> showed the formation of a number of products such as polycarbon mono- and dioxides C{sub n}O{sub m}, and chains containing up to 10 carbon atoms. While a gentle increase in the energy absorbed by the <span class="hlt">ice</span> sample is reflected by an increase in themore » column densities of newly born species, such correlation breaks down at very high <span class="hlt">fluxes</span>. In this regime the production yield falls down sharply by about a factor of 100. The refractory residue obtained in the broad energy irradiation is a “compromise” between those obtained with proton irradiation of C{sub 3}O{sub <span class="hlt">2</span>} and <span class="hlt">CO</span> <span class="hlt">ices</span> in previous experiments. Finally, we discuss the possible implications for space chemistry.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24037377','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24037377"><span>Calving <span class="hlt">fluxes</span> and basal melt rates of Antarctic <span class="hlt">ice</span> shelves.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Depoorter, M A; Bamber, J L; Griggs, J A; Lenaerts, J T M; Ligtenberg, S R M; van den Broeke, M R; Moholdt, G</p> <p>2013-10-03</p> <p>Iceberg calving has been assumed to be the dominant cause of mass loss for the Antarctic <span class="hlt">ice</span> sheet, with previous estimates of the calving <span class="hlt">flux</span> exceeding <span class="hlt">2</span>,000 gigatonnes per year. More recently, the importance of melting by the ocean has been demonstrated close to the grounding line and near the calving front. So far, however, no study has reliably quantified the calving <span class="hlt">flux</span> and the basal mass balance (the balance between accretion and ablation at the <span class="hlt">ice</span>-shelf base) for the whole of Antarctica. The distribution of fresh water in the Southern Ocean and its partitioning between the liquid and solid phases is therefore poorly constrained. Here we estimate the mass balance components for all <span class="hlt">ice</span> shelves in Antarctica, using satellite measurements of calving <span class="hlt">flux</span> and grounding-line <span class="hlt">flux</span>, modelled <span class="hlt">ice</span>-shelf snow accumulation rates and a regional scaling that accounts for unsurveyed areas. We obtain a total calving <span class="hlt">flux</span> of 1,321 ± 144 gigatonnes per year and a total basal mass balance of -1,454 ± 174 gigatonnes per year. This means that about half of the <span class="hlt">ice</span>-sheet surface mass gain is lost through oceanic erosion before reaching the <span class="hlt">ice</span> front, and the calving <span class="hlt">flux</span> is about 34 per cent less than previous estimates derived from iceberg tracking. In addition, the fraction of mass loss due to basal processes varies from about 10 to 90 per cent between <span class="hlt">ice</span> shelves. We find a significant positive correlation between basal mass loss and surface elevation change for <span class="hlt">ice</span> shelves experiencing surface lowering and enhanced discharge. We suggest that basal mass loss is a valuable metric for predicting future <span class="hlt">ice</span>-shelf vulnerability to oceanic forcing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004GeCoA..68.1749P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004GeCoA..68.1749P"><span>Experimental evidence for carbonate precipitation and <span class="hlt">CO</span> <span class="hlt">2</span> degassing during sea <span class="hlt">ice</span> formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Papadimitriou, S.; Kennedy, H.; Kattner, G.; Dieckmann, G. S.; Thomas, D. N.</p> <p>2004-04-01</p> <p>Chemical and stable carbon isotopic modifications during the freezing of artificial seawater were measured in four 4 m 3 tank incubations. Three of the four incubations were inoculated with a nonaxenic Antarctic diatom culture. The 18 days of freezing resulted in 25 to 27 cm thick <span class="hlt">ice</span> sheets overlying the residual seawater. The <span class="hlt">ice</span> phase was characterized by a decrease in temperature from -1.9 to -<span class="hlt">2.2</span>°C in the under-<span class="hlt">ice</span> seawater down to -6.7°C in the upper 4 cm of the <span class="hlt">ice</span> sheet, with a concurrent increase in the salinity of the under-<span class="hlt">ice</span> seawater and brine inclusions of the <span class="hlt">ice</span> sheet as a result of physical concentration of major dissolved salts by expulsion from the solid <span class="hlt">ice</span> matrix. Measurements of pH, total dissolved inorganic carbon (C T) and its stable isotopic composition (δ 13C T) all exhibited changes, which suggest minimal effect by biological activity during the experiment. A systematic drop in pH and salinity-normalized C T by up to 0.37 pH SWS units and 376 μmol C kg -1 respectively at the lowest temperature and highest salinity part of the <span class="hlt">ice</span> sheet were coupled with an equally systematic 13C enrichment of the C T. Calculations based on the direct pH and C T measurements indicated a steady increase in the in situ concentration of dissolved carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span>(aq)) with time and increasing salinity within the <span class="hlt">ice</span> sheet, partly due to changes in the dissociation constants of carbonic acid in the low temperature-high salinity range within sea <span class="hlt">ice</span>. The combined effects of temperature and salinity on the solubility of <span class="hlt">CO</span> <span class="hlt">2</span> over the range of conditions encountered during this study was a slight net decrease in the equilibrium <span class="hlt">CO</span> <span class="hlt">2</span>(aq) concentration as a result of the salting-out overriding the increase in solubility with decreasing temperature. Hence, the increase in the in situ <span class="hlt">CO</span> <span class="hlt">2</span>(aq) concentration lead to saturation or supersaturation of the brine inclusions in the <span class="hlt">ice</span> sheet with respect to atmospheric p<span class="hlt">CO</span> <span class="hlt">2</span> (≈3.5 × 10 -4 atm). When all physico</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS33A1443Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS33A1443Y"><span>Diagnosing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and seasonality in the Arabian Sea as an Ocean-Dominated Margin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, W.; Dai, M.</p> <p>2017-12-01</p> <p>The Arabian Sea is a large marginal sea of the Indian Ocean characterized by highly predictable annual circulation cycle driven by Asian monsoon. The Arabian Sea is generally sources to atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. In this study, we applied the physical-biogeochemical coupled approach previously adopted for diagnosis of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Ocean-dominated margin (OceMar) to assesses the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and their seasonality in Arabian Sea using data collected during five US JGOFS Arabian Sea Process Study cruises (ttn-043, ttn-045, ttn-049, ttn-053, ttn-054) conducted from September 1994 to December 1995. The p<span class="hlt">CO</span><span class="hlt">2</span> estimated during the 5 cruises was 396±5μatm, 359±7 μatm, 373±7 μatm, 379±9 μatm and 387±12 μatm, respectively, which agreed well with the p<span class="hlt">CO</span><span class="hlt">2</span> observed during the cruises of 389±8 μatm, 361±6 μatm, 366±6 μatm, 371±8 μatm and 367±11 μatm from underway measurements. This strongly suggests that our semi-analytical diagnostic approach in the OceMar framework can evaluate the p<span class="hlt">CO</span><span class="hlt">2</span> in Arabian Sea. Our coupled diagnostic approach assumes that water mass mixing, biological response and <span class="hlt">air</span>-sea exchange under steady state over a similar time scale. This assumption should be justified at the region with intensified upwelling where decoupling between upwelling and biological response may occur, where only water mass mixing and <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange should be accounted for. This presentation will also examine the seasonality of the <span class="hlt">CO</span><span class="hlt">2</span> dynamics and its controls.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70020545','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70020545"><span>Winter <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 from subalpine soils in Rocky Mountain National Park, Colorado</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mast, M. Alisa; Wickland, Kimberly P.; Striegl, Robert G.; Clow, David W.</p> <p>1998-01-01</p> <p><span class="hlt">Fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 through a seasonal snowpack were measured in and adjacent to a subalpine wetland in Rocky Mountain National Park, Colorado. Gas diffusion through the snow was controlled by gas production or consumption in the soil and by physical snowpack properties. The snowpack insulated soils from cold midwinter <span class="hlt">air</span> temperatures allowing microbial activity to continue through the winter. All soil types studied were net sources of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere through the winter, whereas saturated soils in the wetland center were net emitters of CH4 and soils adjacent to the wetland were net CH4 consumers. Most sites showed similar temporal patterns in winter gas <span class="hlt">fluxes</span>; the lowest <span class="hlt">fluxes</span> occurred in early winter, and maximum <span class="hlt">fluxes</span> occurred at the onset of snowmelt. Temporal changes in <span class="hlt">fluxes</span> probably were related to changes in soil-moisture conditions and hydrology because soil temperatures were relatively constant under the snowpack. Average winter <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were 42.3, 31.<span class="hlt">2</span>, and 14.6 mmol m−<span class="hlt">2</span> d−1 over dry, moist, and saturated soils, respectively, which accounted for 8 to 23% of the gross annual <span class="hlt">CO</span><span class="hlt">2</span>emissions from these soils. Average winter CH4 <span class="hlt">fluxes</span> were −0.016, 0.274, and <span class="hlt">2</span>.87 mmol m−<span class="hlt">2</span> d−1over dry, moist, and saturated soils, respectively. Microbial activity under snow cover accounted for 12% of the annual CH4 consumption in dry soils and 58 and 12% of the annual CH4 emitted from moist and saturated soils, respectively. The observed ranges in <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> through snow indicated that winter <span class="hlt">fluxes</span> are an important part of the annual carbon budget in seasonally snow-covered terrains.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/4575','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/4575"><span>Quantitative comparison of in situ soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurement methods</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Jennifer D. Knoepp; James M. Vose</p> <p>2002-01-01</p> <p>Development of reliable regional or global carbon budgets requires accurate measurement of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. We conducted laboratory and field studies to determine the accuracy and comparability of methods commonly used to measure in situ soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Methods compared included <span class="hlt">CO</span><span class="hlt">2</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.C43A0587P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.C43A0587P"><span>Heat <span class="hlt">flux</span> variations over sea-<span class="hlt">ice</span> observed at the coastal area of the Sejong Station, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, S.; Choi, T.; Kim, S.</p> <p>2012-12-01</p> <p>This study presents variations of sensible heat <span class="hlt">flux</span> and latent heat <span class="hlt">flux</span> over sea-<span class="hlt">ice</span> observed in 2011 from the 10-m <span class="hlt">flux</span> tower located at the coast of the Sejong Station on King George Island, Antarctica. A period from June to November was divided into three parts: "Freezing", "Frozen", and "Melting" periods based on daily monitoring of sea state and hourly photos looking at the Marian Cove in front of the Sejong Station. The division of periods enabled us to look into the heat <span class="hlt">flux</span> variations depending on the sea-<span class="hlt">ice</span> conditions. Over freezing sea surface during the freezing period of late June, daily mean sensible heat <span class="hlt">flux</span> was -11.9 Wm-<span class="hlt">2</span> and daily mean latent heat <span class="hlt">flux</span> was +16.3 Wm-<span class="hlt">2</span>. Over the frozen sea-<span class="hlt">ice</span>, daily mean sensible heat <span class="hlt">flux</span> was -10.4 Wm-<span class="hlt">2</span> while daily mean latent heat <span class="hlt">flux</span> was +<span class="hlt">2</span>.4 Wm-<span class="hlt">2</span>. During the melting period of mid-October to early November, magnitudes of sensible heat <span class="hlt">flux</span> increased to -14.<span class="hlt">2</span> Wm-<span class="hlt">2</span> and latent heat <span class="hlt">flux</span> also increased to +13.5 Wm-<span class="hlt">2</span>. In short, latent heat <span class="hlt">flux</span> was usually upward over sea-<span class="hlt">ice</span> most of the time while sensible heat <span class="hlt">flux</span> was downward from atmosphere to sea-<span class="hlt">ice</span>. Magnitudes of the <span class="hlt">fluxes</span> were small but increased when freezing or melting of sea-<span class="hlt">ice</span> was occurring. Especially, latent heat <span class="hlt">flux</span> increased five to six times compared to that of "frozen" period implying that early melting of sea-<span class="hlt">ice</span> may cause five to six times larger supply of moisture to the atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A43H..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A43H..02B"><span>Optimization of <span class="hlt">CO</span><span class="hlt">2</span> Surface <span class="hlt">Flux</span> using GOSAT Total Column <span class="hlt">CO</span><span class="hlt">2</span>: First Results for 2009-2010</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Basu, S.; Houweling, S.</p> <p>2011-12-01</p> <p>Constraining surface <span class="hlt">flux</span> estimates of <span class="hlt">CO</span><span class="hlt">2</span> using satellite measurements has been one of the long-standing goals of the atmospheric inverse modeling community. We present the first results of inverting GOSAT total column <span class="hlt">CO</span><span class="hlt">2</span> measurements for obtaining global monthly <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> maps over one year (June 2009 to May 2010). We use the SRON RemoTeC retrieval of <span class="hlt">CO</span><span class="hlt">2</span> for our inversions. The SRON retrieval has been shown to have no bias when compared to TCCON total column measurements, and latitudinal gradients of the retrieved <span class="hlt">CO</span><span class="hlt">2</span> are consistent with gradients deduced from the surface flask network [Butz et al, 2011]. This makes this retrieval an ideal candidate for atmospheric inversions, which are highly sensitive to spurious gradients. Our inversion system is analogous to the CarbonTracker (CT) data assimilation system; it is initialized with the prior <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of CT, and uses the same atmospheric transport model, i.e., TM5. The two major differences are (a) we add GOSAT <span class="hlt">CO</span><span class="hlt">2</span> data to the inversion in addition to flask data, and (b) we use a 4DVAR optimization system instead of a Kalman filter. We compare inversions using (a) only GOSAT total column <span class="hlt">CO</span><span class="hlt">2</span> measurements, (b) only surface flask <span class="hlt">CO</span><span class="hlt">2</span> measurements, and (c) the joint data set of GOSAT and surface flask measurements. We validate GOSAT-only inversions against the NOAA surface flask network and joint inversions against CONTRAIL and other aircraft campaigns. We see that inverted <span class="hlt">fluxes</span> from a GOSAT-only inversion are consistent with <span class="hlt">fluxes</span> from a stations-only inversion, reaffirming the low biases in SRON retrievals. From the joint inversion, we estimate the amount of added constraints upon adding GOSAT total column measurements to existing surface layer measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B43J..06P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B43J..06P"><span>Responses of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> to Arctic Browning Events in a Range of High Latitude, Shrub-Dominated Ecosystems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phoenix, G. K.; Treharne, R.; Emberson, L.; Tømmervik, H. A.; Bjerke, J. W.</p> <p>2017-12-01</p> <p>Climatic and biotic extreme events can result in considerable damage to arctic vegetation, often at landscape and larger scale. These acute events therefore contribute to the browning observed in some arctic regions. It is of considerable concern, therefore, that such extreme events are increasing in frequency as part of climate change. However, despite the increasing importance of browning events, and the considerable impact they can have on ecosystems, to date there is little understanding of their impacts on ecosystem carbon <span class="hlt">fluxes</span>. To address this, the impacts of a number of different, commonly occurring, extreme events and their subsequent browning (vegetation damage) on key ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were assessed during the growing season at a range of event damaged sites of shrub dominated vegetation. Sites were located from the boreal to High Arctic (64˚N-79˚N) and had been previously been damaged by events of frost-drought, extreme winter warming, ground <span class="hlt">icing</span> and caterpillar (Epirrita autumnata) outbreaks. Plot-level <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of Ecosystem Exchange (NEE), Gross Primary Productivity (GPP) and Ecosystem Respiration (Reco) were assessed using vegetation chambers. At a sub-set of sites, NDVI (greenness) in <span class="hlt">flux</span> plots was also assessed by hand-held proximal sensor, allowing the relationship between NDVI of damage plots to <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> to be calculated. Despite the contrasting sites and drivers, damage had consistent, major impacts on all <span class="hlt">fluxes</span>. All sites showed reductions in GPP and NEE with increasing damage, despite efflux from Reco also declining with damage. When scaled to site-level, reductions of up to 81% of NEE, 51% of GPP and 37% of Reco were observed. In the plot-level NDVI-<span class="hlt">flux</span> relationship, NDVI was shown to explain up to 91% of variation in GPP, and therefore supports the use of NDVI for estimating changes in ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at larger scales in regions where browning has been driven by extreme events. This work is the first attempt to quantify the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.B31E0447B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.B31E0447B"><span>Assessing the impact of urban land cover composition on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Becker, K.; Hinkle, C.</p> <p>2013-12-01</p> <p>Urbanization is an ever increasing trend in global land use change, and has been identified as a key driver of <span class="hlt">CO</span><span class="hlt">2</span> emissions. Therefore, understanding how urbanization affects <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> across a range of climatic zones and development patterns is critical to projecting the impact of future land use on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> dynamics. A growing number of studies are applying the eddy covariance method to urban areas to quantify the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> dynamics of these systems. However, interpretation of eddy covariance data in these urban systems presents a challenge, particularly in areas with high heterogeneity due to a mixing of built and green space. Here we present a study aimed at establishing a relationship between land cover composition and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for a heterogeneous urban area of Orlando, FL. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> has been measured at this site for > 4 years using an open path eddy covariance system. Land cover at this site was classified into built and green space, and relative weight of both land covers were calculated for each 30 min <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurement using the Schuepp model and a source area based on +/- one standard deviation of wind direction. The results of this analysis established a relationship between built land cover and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> within the measured footprint of this urban area. These results, in combination with future projected land use data, will be a valuable resource for providing insight into the impact of future urbanization on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> dynamics in this region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A43A..03B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A43A..03B"><span>Seasonal Oxygen Supersaturation and <span class="hlt">Air</span>-Sea <span class="hlt">Fluxes</span> from Profiling Floats in the Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bushinsky, S. M.; Emerson, S. R.</p> <p>2016-02-01</p> <p>The Pacific Ocean is a heterogeneous basin that includes regions of strong <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to and from the atmosphere. The Kuroshio Extension (KE) is a current associated with the largest <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> into the Pacific Ocean, which extends across the Pacific basin between the subarctic and subtropical regions. The relative importance of the biological and physical processes controlling this sink is uncertain. The stoichiometric relationship between O<span class="hlt">2</span> and dissolved inorganic carbon during photosynthesis and respiration may allow in situ O<span class="hlt">2</span> measurements to help determine the processes driving this large <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. In this study, we used Argo profiling floats with modified oxygen sensors to estimate O<span class="hlt">2</span> <span class="hlt">fluxes</span> in several areas of the Pacific. In situ <span class="hlt">air</span> calibrations of these sensors allowed us to accurately measure <span class="hlt">air</span>-sea O<span class="hlt">2</span> differences, which largely control the <span class="hlt">flux</span> of O<span class="hlt">2</span> to and from the atmosphere. In this way, we determine <span class="hlt">air</span>-sea O<span class="hlt">2</span> <span class="hlt">fluxes</span> from profiling floats, which previously did not measure O<span class="hlt">2</span> accurately enough to make these calculations. To characterize different areas within the KE, we separated O<span class="hlt">2</span> measurements from floats into 3 regions based on geographical position and temperature-salinity relationships: North KE, Central KE, and South KE. We then used these regions and floats in the Alaska Gyre and subtropical South Pacific gyre to develop seasonal climatologies of ΔO<span class="hlt">2</span> and <span class="hlt">air</span>-sea <span class="hlt">flux</span>. Mean annual <span class="hlt">air</span>-sea oxygen <span class="hlt">fluxes</span> (positive <span class="hlt">fluxes</span> represent addition of O<span class="hlt">2</span> to the ocean) were calculated for the Alaska Gyre of -0.3 mol m-<span class="hlt">2</span> yr-1 (2012-2015), for the northern KE, central KE, and southern KE (2013-2015) of 6.8, 10.5, and 0.5 mol m-<span class="hlt">2</span> yr-1, respectively, and for the south subtropical Pacific (2014-2015) of 0.6 mol m-<span class="hlt">2</span> yr-1. The <span class="hlt">air</span>-sea <span class="hlt">flux</span> due to bubbles was greater than 50% of the total <span class="hlt">flux</span> for winter months and essential for determining the magnitude and, in some cases, direction of the cumulative mean annual <span class="hlt">flux</span>. Increases in solubility due to wintertime</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007BGeo....4.1005K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007BGeo....4.1005K"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> determination by closed-chamber methods can be seriously biased by inappropriate application of linear regression</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kutzbach, L.; Schneider, J.; Sachs, T.; Giebels, M.; Nykänen, H.; Shurpali, N. J.; Martikainen, P. J.; Alm, J.; Wilmking, M.</p> <p>2007-11-01</p> <p>Closed (non-steady state) chambers are widely used for quantifying carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">fluxes</span> between soils or low-stature canopies and the atmosphere. It is well recognised that covering a soil or vegetation by a closed chamber inherently disturbs the natural <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by altering the concentration gradients between the soil, the vegetation and the overlying <span class="hlt">air</span>. Thus, the driving factors of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are not constant during the closed chamber experiment, and no linear increase or decrease of <span class="hlt">CO</span><span class="hlt">2</span> concentration over time within the chamber headspace can be expected. Nevertheless, linear regression has been applied for calculating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in many recent, partly influential, studies. This approach has been justified by keeping the closure time short and assuming the concentration change over time to be in the linear range. Here, we test if the application of linear regression is really appropriate for estimating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using closed chambers over short closure times and if the application of nonlinear regression is necessary. We developed a nonlinear exponential regression model from diffusion and photosynthesis theory. This exponential model was tested with four different datasets of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements (total number: 1764) conducted at three peatlands sites in Finland and a tundra site in Siberia. Thorough analyses of residuals demonstrated that linear regression was frequently not appropriate for the determination of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by closed-chamber methods, even if closure times were kept short. The developed exponential model was well suited for nonlinear regression of the concentration over time c(t) evolution in the chamber headspace and estimation of the initial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at closure time for the majority of experiments. However, a rather large percentage of the exponential regression functions showed curvatures not consistent with the theoretical model which is considered to be caused by violations of the underlying model assumptions. Especially the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950028540&hterms=condensation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcondensation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950028540&hterms=condensation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcondensation"><span>The condensation and vaporization behavior of <span class="hlt">ices</span> containing SO<span class="hlt">2</span>, H<span class="hlt">2</span>S, and <span class="hlt">CO</span><span class="hlt">2</span>: Implications for Io</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sandford, Scott A.; Allamandola, Louis J.</p> <p>1993-01-01</p> <p>In an extension of previously reported work on <span class="hlt">ices</span> containing <span class="hlt">CO</span>, <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O, CH3OH, NH3, and H<span class="hlt">2</span>, measurements of the physical and infrared spectral properties of <span class="hlt">ices</span> containing molecules relevant to Jupiter's moon Io are presented. These include studies on <span class="hlt">ice</span> systems containing SO<span class="hlt">2</span>, H<span class="hlt">2</span>S, and <span class="hlt">CO</span><span class="hlt">2</span>. The condensation and sublimation behaviors of each <span class="hlt">ice</span> system and surface binding energies of their components are discussed. The surface binding energies can be used to calculate the residence times of the molecules on a surface as a function of temperature and thus represent important parameters for any calculation that attempts to model the transport of these molecules on Io's surface. The derived values indicate that SO<span class="hlt">2</span> frosts on Io are likely to anneal rapidly, resulting in less fluffy, 'glassy' <span class="hlt">ices</span> and that H<span class="hlt">2</span>S can be trapped in the SO<span class="hlt">2</span> <span class="hlt">ices</span> of Io during night-time hours provided that SO<span class="hlt">2</span> deposition rates are on the order of 5 micrometers/hr or larger.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850005139','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850005139"><span>Dynamics of coupled <span class="hlt">ice</span>-ocean system in the marginal <span class="hlt">ice</span> zone: Study of the mesoscale processes and of constitutive equations for sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hakkinen, S.</p> <p>1984-01-01</p> <p>This study is aimed at the modelling of mesoscale processed such as up/downwelling and <span class="hlt">ice</span> edge eddies in the marginal <span class="hlt">ice</span> zones. A <span class="hlt">2</span>-dimensional coupled <span class="hlt">ice</span>-ocean model is used for the study. The <span class="hlt">ice</span> model is coupled to the reduced gravity ocean model (f-plane) through interfacial stresses. The constitutive equations of the sea <span class="hlt">ice</span> are formulated on the basis of the Reiner-Rivlin theory. The internal <span class="hlt">ice</span> stresses are important only at high <span class="hlt">ice</span> concentrations (90-100%), otherwise the <span class="hlt">ice</span> motion is essentially free drift, where the <span class="hlt">air-ice</span> stress is balanced by the <span class="hlt">ice</span>-water stress. The model was tested by studying the upwelling dynamics. Winds parallel to the <span class="hlt">ice</span> edge with the <span class="hlt">ice</span> on the right produce upwilling because the <span class="hlt">air-ice</span> momentum <span class="hlt">flux</span> is much greater that <span class="hlt">air</span>-ocean momentum <span class="hlt">flux</span>, and thus the Ekman transport is bigger under the <span class="hlt">ice</span> than in the open water. The upwelling simulation was extended to include temporally varying forcing, which was chosen to vary sinusoidally with a 4 day period. This forcing resembles successive cyclone passings. In the model with a thin oceanic upper layer, <span class="hlt">ice</span> bands were formed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS24A..02V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS24A..02V"><span>Watershed-scale drivers of <span class="hlt">air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> exchanges in two lagoonal, North Carolina (USA) estuaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van Dam, B.; Crosswell, J.; Anderson, I. C.; Paerl, H. W.</p> <p>2017-12-01</p> <p>Riverine loading of nutrients and organic matter act in concert to modulate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in estuaries, yet quantitative relationships between these factors remain poorly defined. This study explored watershed-scale mechanisms responsible for the relatively low <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> observed in two microtidal, lagoonal estuaries. <span class="hlt">Air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were quantified with 74 high-resolution spatial surveys in the neighboring New River Estuary (NewRE) and Neuse River Estuary (NeuseRE), North Carolina, which experience a common climatology, but differ in marine versus riverine influence. Annually, both estuaries were relatively small sources of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere, 12.5 and 16.3 mmol C m<span class="hlt">2</span> d-1 in the NeuseRE and NewRE, respectively. Variations in riverine alkalinity and inorganic carbon loading caused zones of minimum buffering capacity to occur at different locations in each estuary, enhancing the sensitivity of estuarine inorganic C chemistry to acidification. Large-scale p<span class="hlt">CO</span><span class="hlt">2</span> variations were driven by changes in freshwater age (akin to residence time), which modulate nutrient and organic carbon supply and phytoplankton flushing. Greatest p<span class="hlt">CO</span><span class="hlt">2</span> under-saturation was observed at intermediate freshwater ages, between <span class="hlt">2</span>-3 weeks. Biological controls on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were obscured by variable inputs of river-borne <span class="hlt">CO</span><span class="hlt">2</span>, which drove <span class="hlt">CO</span><span class="hlt">2</span> degassing in the river-dominated NeuseRE. Internally produced <span class="hlt">CO</span><span class="hlt">2</span> exceeded river-borne <span class="hlt">CO</span><span class="hlt">2</span> in the marine-dominated NewRE, suggesting that net ecosystem heterotrophy, rather than riverine inputs, drove <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in this system. Although annual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were similar between systems, watershed-specific hydrologic factors led to disparate controls on internal carbonate chemistry, which can influence overall ecosystem health and response to future perturbation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRG..123..271V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRG..123..271V"><span>Watershed-Scale Drivers of <span class="hlt">Air</span>-Water <span class="hlt">CO</span><span class="hlt">2</span> Exchanges in Two Lagoonal North Carolina (USA) Estuaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van Dam, Bryce R.; Crosswell, Joseph R.; Anderson, Iris C.; Paerl, Hans W.</p> <p>2018-01-01</p> <p>Riverine loading of nutrients and organic matter act in concert to modulate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in estuaries, yet quantitative relationships between these factors remain poorly defined. This study explored watershed-scale mechanisms responsible for the relatively low <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> observed in two microtidal, lagoonal estuaries. <span class="hlt">Air</span>-water <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were quantified with 74 high-resolution spatial surveys in the neighboring New River Estuary (NewRE) and Neuse River Estuary (NeuseRE), North Carolina, which experience a common climatology but differ in marine versus riverine influence. Annually, both estuaries were relatively small sources of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere, 12.5 and 16.3 mmol C m-<span class="hlt">2</span> d-1 in the NeuseRE and NewRE, respectively. Large-scale p<span class="hlt">CO</span><span class="hlt">2</span> variations were driven by changes in freshwater age, which modulates nutrient and organic carbon supply and phytoplankton flushing. Greatest p<span class="hlt">CO</span><span class="hlt">2</span> undersaturation was observed at intermediate freshwater ages, between <span class="hlt">2</span> and 3 weeks. Biological controls on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were obscured by variable inputs of river-borne <span class="hlt">CO</span><span class="hlt">2</span>, which drove <span class="hlt">CO</span><span class="hlt">2</span> degassing in the river-dominated NeuseRE. Internally produced <span class="hlt">CO</span><span class="hlt">2</span> exceeded river-borne <span class="hlt">CO</span><span class="hlt">2</span> in the marine-dominated NewRE, suggesting that net ecosystem heterotrophy, rather than riverine inputs, drove <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in this system. Variations in riverine alkalinity and inorganic carbon loading caused zones of minimum buffering capacity to occur at different locations in each estuary, enhancing the sensitivity of estuarine inorganic C chemistry to acidification. Although annual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were similar between systems, watershed-specific hydrologic factors led to disparate controls on internal carbonate chemistry, which can influence ecosystem biogeochemical cycling, trophic state, and response to future perturbations.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P43C2897W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P43C2897W"><span>Sea <span class="hlt">Ice</span> as a Sink for <span class="hlt">CO</span><span class="hlt">2</span> and Biogeochemical Material: a Novel Sampling Method and Astrobiological Applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilner, J.; Hofmann, A.; Hand, K. P.</p> <p>2017-12-01</p> <p>Accurately modelling the intensification of greenhouse gas effects in the polar regions ("polar amplification") necessitates a thorough understanding of the geochemical balance between atmospheric, sea <span class="hlt">ice</span>, and oceanic layers. Sea <span class="hlt">ice</span> is highly permeable to <span class="hlt">CO</span><span class="hlt">2</span> and therefore represents a major sink of oceanic <span class="hlt">CO</span><span class="hlt">2</span> in winter and of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> in summer, sinks that are typically either poorly constrained in or fully absent from global climate models. We present a novel method for sampling both trapped and dissolved gases (<span class="hlt">CO</span><span class="hlt">2</span>, CH4 and δ13CH4) in sea <span class="hlt">ice</span> with a Picarro 2132-i Methane Analyzer, taking the following sampling considerations into account: minimization of water and <span class="hlt">air</span> contamination, full headspace sampling, prevention of inadvertent sample bag double-puncturing, and ease of use. This method involves melting of vacuum-sealed <span class="hlt">ice</span> cores to evacuate trapped gases to the headspace and sampling the headspace gas with a blunt needle sheathed by a beveled puncturing needle. A gravity catchment tube prevents input of dangerous levels of liquid water to the Picarro cavity. Subsequent ultrasonic degassing allows for dissolved gas measurement. We are in the process of using this method to sample gases trapped and dissolved in Arctic autumn sea <span class="hlt">ice</span> cores and atmospheric samples collected during the 2016 Polarstern Expedition and during a May 2017 field campaign north of Barrow, Alaska. We additionally employ this method, together with inductively coupled plasma mass spectrometry (ICP-MS), to analyze the transfer of potential biogeochemical signatures of underlying hydrothermal plumes to sea <span class="hlt">ice</span>. This has particular relevance to Europa and Enceladus, where hypothetical hydrothermal plumes may deliver seafloor chemicals to the overlying <span class="hlt">ice</span> shell. Hence, we are presently investigating the entrainment of methane and other hydrothermal material in sea <span class="hlt">ice</span> cores collected along the Gakkel Ridge that may serve as biosignatures of methanogenic organisms in seafloor</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.5627S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.5627S"><span>Variability and trends in surface seawater p<span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the Pacific Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sutton, A. J.; Wanninkhof, R.; Sabine, C. L.; Feely, R. A.; Cronin, M. F.; Weller, R. A.</p> <p>2017-06-01</p> <p>Variability and change in the ocean sink of anthropogenic carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) have implications for future climate and ocean acidification. Measurements of surface seawater <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>) and wind speed from moored platforms are used to calculate high-resolution <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> time series. Here we use the moored <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to examine variability and its drivers over a range of time scales at four locations in the Pacific Ocean. There are significant surface seawater p<span class="hlt">CO</span><span class="hlt">2</span>, salinity, and wind speed trends in the North Pacific subtropical gyre, especially during winter and spring, which reduce <span class="hlt">CO</span><span class="hlt">2</span> uptake over the 10 year record of this study. Starting in late 2013, elevated seawater p<span class="hlt">CO</span><span class="hlt">2</span> values driven by warm anomalies cause this region to be a net annual <span class="hlt">CO</span><span class="hlt">2</span> source for the first time in the observational record, demonstrating how climate forcing can influence the timing of an ocean region shift from <span class="hlt">CO</span><span class="hlt">2</span> sink to source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22518917-first-infrared-band-strengths-amorphous-co-sub-overlooked-component-interstellar-ices','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22518917-first-infrared-band-strengths-amorphous-co-sub-overlooked-component-interstellar-ices"><span>FIRST INFRARED BAND STRENGTHS FOR AMORPHOUS <span class="hlt">CO</span>{sub <span class="hlt">2</span>}, AN OVERLOOKED COMPONENT OF INTERSTELLAR <span class="hlt">ICES</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gerakines, Perry A.; Hudson, Reggie L., E-mail: Reggie.Hudson@NASA.gov</p> <p>2015-08-01</p> <p>Solid carbon dioxide (<span class="hlt">CO</span>{sub <span class="hlt">2</span>}) has long been recognized as a component of both interstellar and solar system <span class="hlt">ices</span>, but a recent literature search has revealed significant qualitative and quantitative discrepancies in the laboratory spectra on which the abundances of extraterrestrial <span class="hlt">CO</span>{sub <span class="hlt">2</span>} are based. Here we report new infrared (IR) spectra of amorphous <span class="hlt">CO</span>{sub <span class="hlt">2</span>}-<span class="hlt">ice</span> along with band intensities (band strengths) of four mid-IR absorptions, the first such results in the literature. A possible thickness dependence for amorphous-<span class="hlt">CO</span>{sub <span class="hlt">2</span>} IR band shapes and positions also is investigated, and the three discordant reports of amorphous <span class="hlt">CO</span>{sub <span class="hlt">2</span>} spectra in themore » literature are addressed. Applications of our results are discussed with an emphasis on laboratory investigations and results from astronomical observations. A careful comparison with earlier work shows that the IR spectra calculated from several databases for <span class="hlt">CO</span>{sub <span class="hlt">2</span>} <span class="hlt">ices</span>, all <span class="hlt">ices</span> being made near 10 K, are not for amorphous <span class="hlt">CO</span>{sub <span class="hlt">2</span>}, but rather for crystalline <span class="hlt">CO</span>{sub <span class="hlt">2</span>} or crystalline-amorphous mixtures.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApJ...807...29Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApJ...807...29Y"><span>Systematic Variations in <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">Ice</span> Abundance Ratios in Nearby Galaxies Found with AKARI Near-infrared Spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamagishi, M.; Kaneda, H.; Ishihara, D.; Oyabu, S.; Onaka, T.; Shimonishi, T.; Suzuki, T.</p> <p>2015-07-01</p> <p>We report <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios in seven nearby star-forming galaxies based on the AKARI near-infrared (<span class="hlt">2</span>.5-5.0 μm) spectra. The <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios show clear variations between 0.05 and 0.<span class="hlt">2</span> with the averaged value of 0.14 ± 0.01. The previous study on M82 revealed that the <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios strongly correlate with the intensity ratios of the hydrogen recombination Brα line to the polycyclic aromatic hydrocarbon (PAH) 3.3 μm feature. In the present study, however, we find no correlation for the seven galaxies as a whole due to systematic differences in the relation between <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance and Brα/PAH 3.3 μm intensity ratios from galaxy to galaxy. This result suggests that there is another parameter that determines the <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios in a galaxy in addition to the Brα/PAH 3.3 μm ratios. We find that the <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios positively correlate with the specific star formation rates of the galaxies. From these results, we conclude that <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">ice</span> abundance ratios tend to be high in young star-forming galaxies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GBioC..30.1509B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GBioC..30.1509B"><span>The role of metabolism in modulating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in boreal lakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bogard, Matthew J.; del Giorgio, Paul A.</p> <p>2016-10-01</p> <p>Lake <span class="hlt">CO</span><span class="hlt">2</span> emissions are increasingly recognized as an important component of the global <span class="hlt">CO</span><span class="hlt">2</span> cycle, yet the origin of these emissions is not clear, as specific contributions from metabolism and in-lake cycling, versus external inputs, are not well defined. To assess the coupling of lake metabolism with <span class="hlt">CO</span><span class="hlt">2</span> concentrations and <span class="hlt">fluxes</span>, we estimated steady state ratios of gross primary production to respiration (GPP:R) and rates of net ecosystem production (NEP = GPP-R) from surface water O<span class="hlt">2</span> dynamics (concentration and stable isotopes) in 187 boreal lakes spanning long environmental gradients. Our findings suggest that internal metabolism plays a dominant role in regulating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in most lakes, but this pattern only emerges when examined at a resolution that accounts for the vastly differing relationships between lake metabolism and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. <span class="hlt">Fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> exceeded those from NEP in over half the lakes, but unexpectedly, these effects were most common and typically largest in a subset ( 30% of total) of net autotrophic lakes that nevertheless emitted <span class="hlt">CO</span><span class="hlt">2</span>. Equally surprising, we found no environmental characteristics that distinguished this category from the more common net heterotrophic, <span class="hlt">CO</span><span class="hlt">2</span> outgassing lakes. Excess <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> relative to NEP were best predicted by catchment structure and hydrologic properties, and we infer from a combination of methods that both catchment inputs and internal anaerobic processes may have contributed this excess <span class="hlt">CO</span><span class="hlt">2</span>. Together, our findings show that the link between lake metabolism and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> is often strong but can vary widely across the boreal biome, having important implications for catchment-wide C budgets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70118551','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70118551"><span>Structure, spectroscopy and dynamics of layered H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ices</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>,; Plattner, Nuria; Meuwly, Markus</p> <p>2012-01-01</p> <p>Molecular dynamics simulations of structural, spectroscopic and dynamical properties of mixed water–carbon dioxide (H<span class="hlt">2</span>O–<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">ices</span> are discussed over temperature ranges relevant to atmospheric and astrophysical conditions. The simulations employ multipolar force fields to represent electrostatic interactions which are essential for spectroscopic and dynamical investigations. It is found that at the water/<span class="hlt">CO</span><span class="hlt">2</span> interface the water surface acts as a template for the <span class="hlt">CO</span><span class="hlt">2</span> component. The rotational reorientation times in both bulk phases agree well with experimental observations. A pronounced temperature effect on the <span class="hlt">CO</span><span class="hlt">2</span> reorientation time is observed between 100 K and 200 K. At the interface, water reorientation times are nearly twice as long compared to water in the bulk. The spectroscopy of such <span class="hlt">ices</span> is rich in the far-infrared region of the spectrum and can be related to translational and rotational modes. Furthermore, spectroscopic signatures mediated across the water/<span class="hlt">CO</span><span class="hlt">2</span> interface are found in this frequency range (around 440 cm−1). These results will be particularly important for new airborne experiments such as planned for SOFIA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000070381&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsonar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000070381&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsonar"><span>Variability of Fram Strait <span class="hlt">Ice</span> <span class="hlt">Flux</span> and North Atlantic Oscillation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kwok, Ron</p> <p>1999-01-01</p> <p>An important term in the mass balance of the Arctic Ocean sea <span class="hlt">ice</span> is the <span class="hlt">ice</span> export. We estimated the winter sea <span class="hlt">ice</span> export through the Fram Strait using <span class="hlt">ice</span> motion from satellite passive microwave data and <span class="hlt">ice</span> thickness data from moored upward looking sonars. The average winter area <span class="hlt">flux</span> over the 18-year record (1978-1996) is 670,000 square km, approximately 7% of the area of the Arctic Ocean. The winter area <span class="hlt">flux</span> ranges from a minimum of 450,000 sq. km in 1984 to a maximum of 906,000 sq km in 1995. The daily, monthly and interannual variabilities of the <span class="hlt">ice</span> area <span class="hlt">flux</span> are high. There is an upward trend in the <span class="hlt">ice</span> area <span class="hlt">flux</span> over the 18-year record. The average winter volume <span class="hlt">flux</span> over the winters of October 1990 through May 1995 is 1745 cubic km ranging from a low of 1375 cubic km in 1990 to a high of 2791 cubic km in 1994. The sea-level pressure gradient across the Fram Strait explains more than 80% of the variance in the <span class="hlt">ice</span> <span class="hlt">flux</span> over the 18-year record. We use the coefficients from the regression of the time-series of area <span class="hlt">flux</span> versus pressure gradient across the Fram Strait and <span class="hlt">ice</span> thickness data to estimate the summer area and volume <span class="hlt">flux</span>. The average 12-month area <span class="hlt">flux</span> and volume <span class="hlt">flux</span> are 919,000 sq km and 2366 cubic km. We find a significant correlation (R =0.86) between the area <span class="hlt">flux</span> and positive phases of the North Atlantic Oscillation (NAO) index over the months of December through March. Correlation between our six years of volume <span class="hlt">flux</span> estimates and the NAO index gives R =0.56. During the high NAO years, a more intense Icelandic low increases the gradient in the sea-level pressure by almost 1 mbar across the Fram Strait thus increasing the atmospheric forcing on <span class="hlt">ice</span> transport. Correlation is reduced during the negative NAO years because of decreased dominance of this large-scale atmospheric pattern on the sea-level pressure gradient across the Fram Strait. Additional information is contained in the original.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoRL..42.5442L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoRL..42.5442L"><span>Observed platelet <span class="hlt">ice</span> distributions in Antarctic sea <span class="hlt">ice</span>: An index for ocean-<span class="hlt">ice</span> shelf heat <span class="hlt">flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Langhorne, P. J.; Hughes, K. G.; Gough, A. J.; Smith, I. J.; Williams, M. J. M.; Robinson, N. J.; Stevens, C. L.; Rack, W.; Price, D.; Leonard, G. H.; Mahoney, A. R.; Haas, C.; Haskell, T. G.</p> <p>2015-07-01</p> <p>Antarctic sea <span class="hlt">ice</span> that has been affected by supercooled <span class="hlt">Ice</span> Shelf Water (ISW) has a unique crystallographic structure and is called platelet <span class="hlt">ice</span>. In this paper we synthesize platelet <span class="hlt">ice</span> observations to construct a continent-wide map of the winter presence of ISW at the ocean surface. The observations demonstrate that, in some regions of coastal Antarctica, supercooled ISW drives a negative oceanic heat <span class="hlt">flux</span> of -30 Wm-<span class="hlt">2</span> that persists for several months during winter, significantly affecting sea <span class="hlt">ice</span> thickness. In other regions, particularly where the thinning of <span class="hlt">ice</span> shelves is believed to be greatest, platelet <span class="hlt">ice</span> is not observed. Our new data set includes the longest <span class="hlt">ice</span>-ocean record for Antarctica, which dates back to 1902 near the McMurdo <span class="hlt">Ice</span> Shelf. These historical data indicate that, over the past 100 years, any change in the volume of very cold surface outflow from this <span class="hlt">ice</span> shelf is less than the uncertainties in the measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820009925','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820009925"><span>Sensitivity of a climatologically-driven sea <span class="hlt">ice</span> model to the ocean heat <span class="hlt">flux</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parkinson, C. L.; Good, M. R.</p> <p>1982-01-01</p> <p>Ocean heat <span class="hlt">flux</span> sensitivity was studied on a numerical model of sea <span class="hlt">ice</span> covering the Weddell Sea region of the southern ocean. The model is driven by mean monthly climatological atmospheric variables. For each model run, the ocean heat <span class="hlt">flux</span> is uniform in both space and time. Ocean heat <span class="hlt">fluxes</span> below 20 W m to the minus <span class="hlt">2</span> power do not provide sufficient energy to allow the <span class="hlt">ice</span> to melt to its summertime thicknesses and concentrations by the end of the 14 month simulation, whereas ocean heat <span class="hlt">fluxes</span> of 30 W m to the minus <span class="hlt">2</span> power and above result in too much <span class="hlt">ice</span> melt, producing the almost total disappearance of <span class="hlt">ice</span> in the Weddell Sea by the end of the 14 months. These results are dependent on the atmospheric forcing fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900061679&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DCO2%2BH2O','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900061679&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DCO2%2BH2O"><span>The volume- and surface-binding energies of <span class="hlt">ice</span> systems containing <span class="hlt">CO</span>, <span class="hlt">CO</span><span class="hlt">2</span>, and H<span class="hlt">2</span>O</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sandford, Scott A.; Allamandola, Louis J.</p> <p>1990-01-01</p> <p>Laboratory-measured, temperature-dependent sticking efficiencies are presently used to derive the surface-binding energies of <span class="hlt">CO</span> and <span class="hlt">CO</span><span class="hlt">2</span> on H<span class="hlt">2</span>O-rich <span class="hlt">ices</span>, with a view to determining the condensation and vaporization properties of these systems as well as to the measured energies' implications for both cometary behavior and the evolution of interstellar <span class="hlt">ices</span>. The molecular volume and the surface binding energies are not found to be necessarily related on the basis of simple nearest-neighbor scaling in surface and bulk sites; this may be due to the physical constraints associated with matrix structure-associated physical constraints, which sometimes dominate the volume-binding energies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JGRD..108.8224W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JGRD..108.8224W"><span>Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in a boreal black spruce fire chronosequence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Chuankuan; Bond-Lamberty, Ben; Gower, Stith T.</p> <p>2003-02-01</p> <p>Understanding the effects of wildfire on the carbon (C) cycle of boreal forests is essential to quantifying the role of boreal forests in the global carbon cycle. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> (Rs), the second largest C <span class="hlt">flux</span> in boreal forests, is directly and indirectly affected by fire and is hypothesized to change during forest succession following fire. The overall objective of this study was to measure and model Rs for a black spruce (Picea mariana [Mill.] BSP) postfire chronosequence in northern Manitoba, Canada. The experiment design was a nested factorial that included two soil drainage classes (well and poorly drained) × seven postfire aged stands. Specific objectives were (1) to quantify the relationship between Rs and soil temperature for different aged boreal black spruce forests in well-drained and poorly drained soil conditions, (<span class="hlt">2</span>) to examine Rs dynamics along postfire successional stands, and (3) to estimate annual soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for these ecosystems. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was significantly affected by soil drainage class (p = 0.014) and stand age (p = 0.006). Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was positively correlated to soil temperature (R<span class="hlt">2</span> = 0.78, p < 0.001), but different models were required for each drainage class × aged stand combination. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was significantly greater at the well-drained than the poorly drained stands (p = 0.007) during growing season. Annual soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the 1998, 1995, 1989, 1981, 1964, 1930, and 1870 burned stands averaged 226, 412, 357, 413, 350, 274, and 244 g C m-<span class="hlt">2</span> yr-1 in the well-drained stands and 146, 380, 300, 303, 256, 233, and 264 g C m-<span class="hlt">2</span> yr-1 in the poorly drained stands. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> during the winter (from 1 November to 30 April) comprised from 5 to 19% of the total annual Rs. We speculate that the smaller soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the recently burned than the older stands is mainly caused by decreased root respiration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002JGRD..107.8224W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002JGRD..107.8224W"><span>Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in a boreal black spruce fire chronosequence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Chuankuan; Bond-Lamberty, Ben; Gower, Stith T.</p> <p>2002-02-01</p> <p>Understanding the effects of wildfire on the carbon (C) cycle of boreal forests is essential to quantifying the role of boreal forests in the global carbon cycle. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> (Rs), the second largest C <span class="hlt">flux</span> in boreal forests, is directly and indirectly affected by fire and is hypothesized to change during forest succession following fire. The overall objective of this study was to measure and model Rs for a black spruce (Picea mariana [Mill.] BSP) postfire chronosequence in northern Manitoba, Canada. The experiment design was a nested factorial that included two soil drainage classes (well and poorly drained) × seven postfire aged stands. Specific objectives were (1) to quantify the relationship between Rs and soil temperature for different aged boreal black spruce forests in well-drained and poorly drained soil conditions, (<span class="hlt">2</span>) to examine Rs dynamics along postfire successional stands, and (3) to estimate annual soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for these ecosystems. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was significantly affected by soil drainage class (p = 0.014) and stand age (p = 0.006). Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was positively correlated to soil temperature (R<span class="hlt">2</span> = 0.78, p < 0.001), but different models were required for each drainage class × aged stand combination. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was significantly greater at the well-drained than the poorly drained stands (p = 0.007) during growing season. Annual soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the 1998, 1995, 1989, 1981, 1964, 1930, and 1870 burned stands averaged 226, 412, 357, 413, 350, 274, and 244 g C m-<span class="hlt">2</span> yr-1 in the well-drained stands and 146, 380, 300, 303, 256, 233, and 264 g C m-<span class="hlt">2</span> yr-1 in the poorly drained stands. Soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> during the winter (from 1 November to 30 April) comprised from 5 to 19% of the total annual Rs. We speculate that the smaller soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the recently burned than the older stands is mainly caused by decreased root respiration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26324399','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26324399"><span>New ground-based lidar enables volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aiuppa, Alessandro; Fiorani, Luca; Santoro, Simone; Parracino, Stefano; Nuvoli, Marcello; Chiodini, Giovanni; Minopoli, Carmine; Tamburello, Giancarlo</p> <p>2015-09-01</p> <p>There have been substantial advances in the ability to monitor the activity of hazardous volcanoes in recent decades. However, obtaining early warning of eruptions remains challenging, because the patterns and consequences of volcanic unrests are both complex and nonlinear. Measuring volcanic gases has long been a key aspect of volcano monitoring since these mobile fluids should reach the surface long before the magma. There has been considerable progress in methods for remote and in-situ gas sensing, but measuring the <span class="hlt">flux</span> of volcanic <span class="hlt">CO</span><span class="hlt">2</span>-the most reliable gas precursor to an eruption-has remained a challenge. Here we report on the first direct quantitative measurements of the volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> using a newly designed differential absorption lidar (DIAL), which were performed at the restless Campi Flegrei volcano. We show that DIAL makes it possible to remotely obtain volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> time series with a high temporal resolution (tens of minutes) and accuracy (<30%). The ability of this lidar to remotely sense volcanic <span class="hlt">CO</span><span class="hlt">2</span> represents a major step forward in volcano monitoring, and will contribute improved volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> inventories. Our results also demonstrate the unusually strong degassing behavior of Campi Flegrei fumaroles in the current ongoing state of unrest.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4204Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4204Z"><span>Global <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> inversions from remote-sensing data with systematic errors using hierarchical statistical models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zammit-Mangion, Andrew; Stavert, Ann; Rigby, Matthew; Ganesan, Anita; Rayner, Peter; Cressie, Noel</p> <p>2017-04-01</p> <p>The Orbiting Carbon Observatory-<span class="hlt">2</span> (OCO-<span class="hlt">2</span>) satellite was launched on <span class="hlt">2</span> July 2014, and it has been a source of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> data since September 2014. The OCO-<span class="hlt">2</span> dataset contains a number of variables, but the one of most interest for <span class="hlt">flux</span> inversion has been the column-averaged dry-<span class="hlt">air</span> mole fraction (in units of ppm). These global level-<span class="hlt">2</span> data offer the possibility of inferring <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at Earth's surface and tracking those <span class="hlt">fluxes</span> over time. However, as well as having a component of random error, the OCO-<span class="hlt">2</span> data have a component of systematic error that is dependent on the instrument's mode, namely land nadir, land glint, and ocean glint. Our statistical approach to <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">flux</span> inversion starts with constructing a statistical model for the random and systematic errors with parameters that can be estimated from the OCO-<span class="hlt">2</span> data and possibly in situ sources from flasks, towers, and the Total Column Carbon Observing Network (TCCON). Dimension reduction of the <span class="hlt">flux</span> field is achieved through the use of physical basis functions, while temporal evolution of the <span class="hlt">flux</span> is captured by modelling the basis-function coefficients as a vector autoregressive process. For computational efficiency, <span class="hlt">flux</span> inversion uses only three months of sensitivities of mole fraction to changes in <span class="hlt">flux</span>, computed using MOZART; any residual variation is captured through the modelling of a stochastic process that varies smoothly as a function of latitude. The second stage of our statistical approach is to simulate from the posterior distribution of the basis-function coefficients and all unknown parameters given the data using a fully Bayesian Markov chain Monte Carlo (MCMC) algorithm. Estimates and posterior variances of the <span class="hlt">flux</span> field can then be obtained straightforwardly from this distribution. Our statistical approach is different than others, as it simultaneously makes inference (and quantifies uncertainty) on both the error components' parameters and the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. We compare it to more classical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70023234','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70023234"><span>High <span class="hlt">CO</span><span class="hlt">2</span> emissions through porous media: Transport mechanisms and implications for <span class="hlt">flux</span> measurement and fractionation</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Evans, William C.; Sorey, M.L.; Kennedy, B.M.; Stonestrom, David A.; Rogie, J.D.; Shuster, D.L.</p> <p>2001-01-01</p> <p>Diffuse emissions of <span class="hlt">CO</span><span class="hlt">2</span> are known to be large around some volcanoes and hydrothermal areas. Accumulation-chamber measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> are increasingly used to estimate the total magmatic or metamorphic <span class="hlt">CO</span><span class="hlt">2</span> released from such areas. To assess the performance of accumulation chamber systems at <span class="hlt">fluxes</span> one to three orders of magnitude higher than normally encountered in soil respiration studies, a test system was constructed in the laboratory where known <span class="hlt">fluxes</span> could be maintained through dry sand. Steady-state gas concentration profiles and fractionation effects observed in the 30-cm sand column nearly match those predicted by the Stefan-Maxwell equations, indicating that the test system was functioning successfully as a uniform porous medium. Eight groups of investigators tested their accumulation chamber equipment, all configured with continuous infrared gas analyzers (IRGA), in this system. Over a <span class="hlt">flux</span> range of ~ 200-12,000 g m-<span class="hlt">2</span> day-1, 90% of their 203 <span class="hlt">flux</span> measurements were 0-25% lower than the imposed <span class="hlt">flux</span> with a mean difference of - 12.5%. Although this difference would seem to be within the range of acceptability for many geologic investigations, some potential sources for larger errors were discovered. A steady-state pressure gradient of -20 Pa/m was measured in the sand column at a <span class="hlt">flux</span> of 11,200 g m-<span class="hlt">2</span> day-1. The derived permeability (50 darcies) was used in the dusty-gas model (DGM) of transport to quantify various diffusive and viscous <span class="hlt">flux</span> components. These calculations were used to demonstrate that accumulation chambers, in addition to reducing the underlying diffusive gradient, severely disrupt the steady-state pressure gradient. The resultant diversion of the net gas flow is probably responsible for the systematically low <span class="hlt">flux</span> measurements. It was also shown that the fractionating effects of a viscous <span class="hlt">CO</span><span class="hlt">2</span> efflux against a diffusive influx of <span class="hlt">air</span> will have a major impact on some important geochemical indicators, such as N<span class="hlt">2</span>/Ar, ??15N-N<span class="hlt">2</span>, and 4He/22</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A14G..06A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A14G..06A"><span>Studying emissions of <span class="hlt">CO</span><span class="hlt">2</span> in the Baltimore/Washington area using airborne measurements: source attribution, <span class="hlt">flux</span> quantification, and model comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahn, D.; Hansford, J. R.; Salawitch, R. J.; Ren, X.; Cohen, M.; Karion, A.; Whetstone, J. R.; Salmon, O. E.; Shepson, P. B.; Gurney, K. R.; Osterman, G. B.; Dickerson, R. R.</p> <p>2017-12-01</p> <p>We study emissions of <span class="hlt">CO</span><span class="hlt">2</span> in the Baltimore-Washington area using airborne in-situ measurements, obtained during the February 2015 <span class="hlt">Fluxes</span> of Greenhouse Gases in Maryland (FLAGG-MD) campaign. In this study, we attributed enhanced signals of <span class="hlt">CO</span><span class="hlt">2</span> to several power plants and two urban areas (Baltimore City and Washington, DC), using the NOAA HYSPLIT <span class="hlt">air</span> parcel trajectory model as well as the analysis of chemical ratios to quantify the source/receptor relationship. Then, the <span class="hlt">fluxes</span> of attributed <span class="hlt">CO</span><span class="hlt">2</span> are estimated using a mass balance approach. The uncertainty in the aircraft-based mass balance approach is estimated by conducting a detailed sensitivity analysis of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, considering factors such as the background mixing ratio of <span class="hlt">CO</span><span class="hlt">2</span>, wind direction and speed, PBL heights, the horizontal boundary, and vertical interpolation methods. Estimated <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> with estimated uncertainty ranges are then compared to output from various emissions data and models, such as CEMS, CarbonTracker, FFDAS, and ODIAC. Finally, column <span class="hlt">CO</span><span class="hlt">2</span> data over the Baltimore-Washington region observed by the OCO-<span class="hlt">2</span> satellite instrument are statistically compared to aircraft in-situ observations, to assess how well OCO-<span class="hlt">2</span> is able to quantify geographic and synoptic-scale variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110011454&hterms=Koch&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DKoch','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110011454&hterms=Koch&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DKoch"><span>Can <span class="hlt">CO</span><span class="hlt">2</span> Turbulent <span class="hlt">Flux</span> Be Measured by Lidar? A Preliminary Study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gilbert, Fabien; Koch, Grady; Beyon, Jeffrey Y.; Hilton, Timothy W.; Davis, Kenneth J.; Andrews, Arlyn; Flamant, Pierre H.; Singh, Upendra N.</p> <p>2011-01-01</p> <p>The vertical profiling of<span class="hlt">CO</span><span class="hlt">2</span> turbulent <span class="hlt">fluxes</span> in the atmospheric boundary layer (ABL) is investigated using a coherent differential absorption lidar (CDIAL) operated nearby a tall tower in Wisconsin during June 2007. A CDIAL can perform simultaneous range-resolved <span class="hlt">CO</span><span class="hlt">2</span> DIAL and velocity measurements. The lidar eddy covariance technique is presented. The aims of the study are (i) an assessment of performance and current limitation of available CDIAL for <span class="hlt">CO</span><span class="hlt">2</span> turbulent <span class="hlt">fluxes</span> and (ii) the derivation of instrument specifications to build a future CDIAL to perform accurate range-resolved <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Experimental lidar <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio and vertical velocity profiles are successfully compared with in situ sensors measurements. Time and space integral scales of turbulence in the ABL are addressed that result in limitation for time averaging and range accumulation. A first attempt to infer <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using an eddy covariance technique with currently available <span class="hlt">2</span>-mm CDIAL dataset is reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014BGD....1117543L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014BGD....1117543L"><span>Rapid establishment of the <span class="hlt">CO</span><span class="hlt">2</span> sink associated with Kerguelen's bloom observed during the KEOPS<span class="hlt">2</span>/OISO20 cruise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lo Monaco, C.; Metzl, N.; D'Ovidio, F.; Llort, J.; Ridame, C.</p> <p>2014-12-01</p> <p>Iron and light are the main factors limiting the biological pump of <span class="hlt">CO</span><span class="hlt">2</span> in the Southern Ocean. Iron fertilization experiments have demonstrated the potential for increased uptake of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, but little is known about the evolution of fertilized environnements. This paper presents observations collected in one of the largest phytoplankton bloom of the Southern Ocean sustained by iron originating from the Kerguelen Plateau. We first complement previous studies by investigating the mechanisms that control <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> over and downstream of the Kerguelen Plateau at the onset of the bloom based on measurements obtained in October-November 2011. These new observations show the rapid establishment of a strong <span class="hlt">CO</span><span class="hlt">2</span> sink in waters fertilized with iron as soon as vertical mixing is reduced. The magnitude of the <span class="hlt">CO</span><span class="hlt">2</span> sink was closely related to chlorophyll a and iron concentrations. Because iron concentration strongly depends on the distance from the iron source and the mode of delivery, we identified lateral advection as the main mechanism controlling <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> downtream the Kerguelen Plateau during the growing season. In the southern part of the bloom, situated over the Plateau (iron source), the <span class="hlt">CO</span><span class="hlt">2</span> sink was stronger and spatially more homogeneous than in the plume offshore. However, we also witnessed a substantial reduction in the uptake of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> over the Plateau following a strong winds event. Next, we used all the data available in this region in order to draw the seasonal evolution of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The <span class="hlt">CO</span><span class="hlt">2</span> sink is rapidly reduced during the course of the growing season, which we attribute to iron and silicic acid depletion. South of the Polar Front, where nutrients depletion is delayed, we suggest that the amplitude and duration of the <span class="hlt">CO</span><span class="hlt">2</span> sink is mainly controlled by vertical mixing. The impact of iron fertilization on <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> is revealed by comparing the uptake of <span class="hlt">CO</span><span class="hlt">2</span> integrated over the productive season in the bloom</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFMGC31B0184C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFMGC31B0184C"><span>Carbon Dioxide and Water Vapor <span class="hlt">Fluxes</span> at Reduced and Elevated <span class="hlt">CO</span><span class="hlt">2</span> Concentrations in Southern California Chaparral</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheng, Y.; Oechel, W. C.; Hastings, S. J.; Bryant, P. J.; Qian, Y.</p> <p>2003-12-01</p> <p>This research took two different approaches to measuring carbon and water vapor <span class="hlt">fluxes</span> at the plot level (<span class="hlt">2</span> x <span class="hlt">2</span> meter and 1 x 1 meter plots) to help understand and predict ecosystem responses to elevated <span class="hlt">CO</span><span class="hlt">2</span> concentrations and concomitant environmental changes. The first measurement approach utilized a <span class="hlt">CO</span><span class="hlt">2</span>-controlled, ambient lit, temperature controlled (<span class="hlt">CO</span><span class="hlt">2</span>LT) null-balance chamber system run in a chaparral ecosystem in southern California, with six different <span class="hlt">CO</span><span class="hlt">2</span> concentrations ranging from 250 to 750 ppm <span class="hlt">CO</span><span class="hlt">2</span> concentrations with 100 ppm difference between treatments. The second measurement approach used a free <span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> enrichment (FACE) system operated at 550 ppm <span class="hlt">CO</span><span class="hlt">2</span> concentration. These manipulations allowed the study of responses of naturally-growing chaparral to varying levels of <span class="hlt">CO</span><span class="hlt">2</span>, under both chamber and open <span class="hlt">air</span> conditions. There was a statistically significant <span class="hlt">CO</span><span class="hlt">2</span> effect on annual NEE (net ecosystem exchange) during the period of this study, 1997 to 2000. The effects of elevated <span class="hlt">CO</span><span class="hlt">2</span> on <span class="hlt">CO</span><span class="hlt">2</span> and water vapor <span class="hlt">flux</span> showed strong seasonal patterns. Elevated <span class="hlt">CO</span><span class="hlt">2</span> delayed the development of water stress, enhanced leaf-level photosynthesis, and decreased transpiration and conductance rates. These effects were observed regardless of water availability. Ecosystem <span class="hlt">CO</span><span class="hlt">2</span> sink strength and plant water status were significantly enhanced by elevated <span class="hlt">CO</span><span class="hlt">2</span> when water availability was restricted. Comparing the FACE treatment and the FACE control, the ecosystem was either a stronger sink or a weaker source to the atmosphere throughout the dry seasons, but there was no statistically significant difference during the wet seasons. Annual average leaf transpiration decreased with the increasing of the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration. Although leaf level water-use efficiency (WUE) increased with the growth <span class="hlt">CO</span><span class="hlt">2</span> concentration increase, annual evapotranspiration (ET) during these four years also increased with the increase of the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations. These results indicate that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/42020','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/42020"><span>Seasonal soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> under big sagebrush (Artemisia tridentata Nutt.)</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Michael C. Amacher; Cheryl L. Mackowiak</p> <p>2011-01-01</p> <p>Soil respiration is a major contributor to atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, but accurate landscape-scale estimates of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for many ecosystems including shrublands have yet to be established. We began a project to measure, with high spatial and temporal resolution, soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in a stand (11 x 25 m area) of big sagebrush (Artemisia tridentata Nutt.) at the Logan, Utah,...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C23A1212A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C23A1212A"><span>Responses of Basal Melting of Antarctic <span class="hlt">Ice</span> Shelves to the Climatic Forcing of the Last Glacial Maximum and <span class="hlt">CO</span><span class="hlt">2</span> Doubling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abe-Ouchi, A.; Obase, T.</p> <p>2017-12-01</p> <p>Basal melting of the Antarctic <span class="hlt">ice</span> shelves is an important factor in determining the stability of the Antarctic <span class="hlt">ice</span> sheet. This study used the climatic outputs of an atmosphere?ocean general circulation model to force a circumpolar ocean model that resolves <span class="hlt">ice</span> shelf cavity circulation to investigate the response of Antarctic <span class="hlt">ice</span> shelf melting to different climatic conditions, i.e., to an increase (doubling) of <span class="hlt">CO</span><span class="hlt">2</span> and the Last Glacial Maximum conditions. We also conducted sensitivity experiments to investigate the role of surface atmospheric change, which strongly affects sea <span class="hlt">ice</span> production, and the change of oceanic lateral boundary conditions. We found that the rate of change of basal melt due to climate warming is much greater (by an order of magnitude) than due to cooling. This is mainly because the intrusion of warm water onto the continental shelves, linked to sea <span class="hlt">ice</span> production and climate change, is crucial in determining the basal melt rate of many <span class="hlt">ice</span> shelves. Sensitivity experiments showed that changes of atmospheric heat <span class="hlt">flux</span> and ocean temperature are both important for warm and cold climates. The offshore wind change together with atmospheric heat <span class="hlt">flux</span> change strongly affected the production of sea <span class="hlt">ice</span> and high-density water, preventing warmer water approaching the <span class="hlt">ice</span> shelves under a colder climate. These results reflect the importance of both water mass formation in the Antarctic shelf seas and subsurface ocean temperature in understanding the long-term response to climate change of the melting of Antarctic <span class="hlt">ice</span> shelves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012E%26PSL.341..243F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012E%26PSL.341..243F"><span>The evolution of p<span class="hlt">CO</span><span class="hlt">2</span>, <span class="hlt">ice</span> volume and climate during the middle Miocene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Foster, Gavin L.; Lear, Caroline H.; Rae, James W. B.</p> <p>2012-08-01</p> <p>The middle Miocene Climatic Optimum (17-15 Ma; MCO) is a period of global warmth and relatively high <span class="hlt">CO</span><span class="hlt">2</span> and is thought to be associated with a significant retreat of the Antarctic <span class="hlt">Ice</span> Sheet (AIS). We present here a new planktic foraminiferal δ11B record from 16.6 to 11.8 Ma from two deep ocean sites currently in equilibrium with the atmosphere with respect to <span class="hlt">CO</span><span class="hlt">2</span>. These new data demonstrate that the evolution of global climate during the middle Miocene (as reflected by changes in the cyrosphere) was well correlated to variations in the concentration of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. What is more, within our sampling resolution (∼1 sample per 300 kyr) there is no evidence of hysteresis in the response of <span class="hlt">ice</span> volume to <span class="hlt">CO</span><span class="hlt">2</span> forcing during the middle Miocene, contrary to what is understood about the Antarctic <span class="hlt">Ice</span> Sheet from <span class="hlt">ice</span> sheet modelling studies. In agreement with previous data, we show that absolute levels of <span class="hlt">CO</span><span class="hlt">2</span> during the MCO were relatively modest (350-400 ppm) and levels either side of the MCO are similar or lower than the pre-industrial (200-260 ppm). These new data imply the presence of either a very dynamic AIS at relatively low <span class="hlt">CO</span><span class="hlt">2</span> during the middle Miocene or the advance and retreat of significant northern hemisphere <span class="hlt">ice</span>. Recent drilling on the Antarctic margin and shore based studies indicate significant retreat and advance beyond the modern limits of the AIS did occur during the middle Miocene, but the complete loss of the AIS was unlikely. Consequently, it seems that <span class="hlt">ice</span> volume and climate variations during the middle Miocene probably involved a more dynamic AIS than the modern but also some component of land-based <span class="hlt">ice</span> in the northern hemisphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A41B0088V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A41B0088V"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from a tropical neighborhood: sources and sinks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Velasco, E.; Roth, M.; Tan, S.; Quak, M.; Britter, R.; Norford, L.</p> <p>2011-12-01</p> <p>Cities are the main contributors to the <span class="hlt">CO</span><span class="hlt">2</span> rise in the atmosphere. The <span class="hlt">CO</span><span class="hlt">2</span> released from the various emission sources is typically quantified by a bottom-up aggregation process that accounts for emission factors and fossil fuel consumption data. This approach does not consider the heterogeneity and variability of the urban emission sources, and error propagation can result in large uncertainties. In this context, direct measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> that include all major and minor anthropogenic and natural sources and sinks from a specific district can be used to evaluate emission inventories. This study reports and compares <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> measured directly using the eddy covariance method with emissions estimated by emissions factors and activity data for a residential neighborhood of Singapore, a highly populated and urbanized tropical city. The <span class="hlt">flux</span> measurements were conducted during one year. No seasonal variability was found as a consequence of the constant climate conditions of tropical places; but a clear diurnal pattern with morning and late afternoon peaks in phase with the rush-hour traffic was observed. The magnitude of the <span class="hlt">fluxes</span> throughout daylight hours is modulated by the urban vegetation, which is abundant in terms of biomass but not of land-cover (15%). Even though the carbon uptake by vegetation is significant, it does not exceed the anthropogenic emissions and the monitored district is a net <span class="hlt">CO</span><span class="hlt">2</span> source of 20.3 ton km-<span class="hlt">2</span> day-1 on average. The carbon uptake by vegetation is investigated as the difference between the estimated emissions and the measured <span class="hlt">fluxes</span> during daytime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.B51D0296M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.B51D0296M"><span>Microbial imprint on soil-atmosphere H<span class="hlt">2</span>, COS, and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meredith, L. K.; Commane, R.; Munger, J. W.; Wofsy, S. C.; Prinn, R. G.</p> <p>2013-12-01</p> <p>Microorganisms drive large trace gas <span class="hlt">fluxes</span> between soil and atmosphere, but the signal can be difficult to detect and quantify in the presence of stronger exchange processes in an ecosystem. Partitioning methods are often needed to estimate trace gas budgets and to develop process-based models to explore the sensitivity of microbe-mediated <span class="hlt">fluxes</span>. In this study, we test the performance of trace gases with predominantly microbe-mediated soil <span class="hlt">fluxes</span> as a metric of the soil microbial uptake activity of other trace gases. Using simultaneous, collocated measurements at Harvard Forest, we consider three trace gases with microbe-mediated soil <span class="hlt">fluxes</span> of various importance relative to their other (mainly plant-mediated) ecosystem <span class="hlt">fluxes</span>: molecular hydrogen (H<span class="hlt">2</span>), carbonyl sulfide (COS), and carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>). These gases probe different aspects of the soil trace-gas microbiology. Soil H<span class="hlt">2</span> uptake is a redox reaction driving the energy metabolism of a portion of the microbial community, while soil <span class="hlt">CO</span><span class="hlt">2</span> respiration is a partial proxy for the overall soil microbial metabolism. In comparison, very little is understood about the microbiological and environmental drivers of soil COS uptake and emissions. In this study, we find that H<span class="hlt">2</span>, COS, and <span class="hlt">CO</span><span class="hlt">2</span> soil uptake rates are often correlated, but the relative soil uptake between gases is not constant, and is influenced by seasonality and local environmental conditions. We also consider how differences in the microbial communities and pathways involved in the soil <span class="hlt">fluxes</span> may explain differences in the observations. Our results are important for informing previous studies using tracer approaches. For example, H<span class="hlt">2</span> has been used to estimate COS soil uptake, which must be accounted for to use COS as a carbon cycle tracer. Furthermore, the global distribution of H<span class="hlt">2</span> deposition velocity has been inferred from net primary productivity (<span class="hlt">CO</span><span class="hlt">2</span>). Given that insufficient measurement frequency and spatial distribution exists to partition global net</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160010510','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160010510"><span>The Effect of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Cap Sublimation on Mars Atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Batterson, Courtney</p> <p>2016-01-01</p> <p>Sublimation of the polar <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> caps on Mars is an ongoing phenomenon that may be contributing to secular climate change on Mars. The transfer of <span class="hlt">CO</span><span class="hlt">2</span> between the surface and atmosphere via sublimation and deposition may alter atmospheric mass such that net atmospheric mass is increasing despite seasonal variations in <span class="hlt">CO</span><span class="hlt">2</span> transfer. My study builds on previous studies by Kahre and Haberle that analyze and compare data from the Phoenix and Viking Landers 1 and <span class="hlt">2</span> to determine whether secular climate change is happening on Mars. In this project, I use two years worth of temperature, pressure, and elevation data from the MSL Curiosity rover to create a program that allows for successful comparison of Curiosity pressure data to Viking Lander pressure data so a conclusion can be drawn regarding whether <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cap sublimation is causing a net increase in atmospheric mass and is thus contributing to secular climate change on Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A54D..06M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A54D..06M"><span>The Impact of Cloud Properties on Young Sea <span class="hlt">Ice</span> during Three Winter Storms at N-<span class="hlt">ICE</span>2015</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murphy, S. Y.; Walden, V. P.; Cohen, L.; Hudson, S. R.</p> <p>2017-12-01</p> <p>The impact of clouds on sea <span class="hlt">ice</span> varies significantly as cloud properties change. Instruments deployed during the Norwegian Young Sea <span class="hlt">Ice</span> field campaign (N-<span class="hlt">ICE</span>2015) are used to study how differing cloud properties influence the cloud radiative forcing at the sea <span class="hlt">ice</span> surface. N-<span class="hlt">ICE</span>2015 was the first campaign in the Arctic winter since SHEBA (1997/1998) to study the surface energy budget of sea <span class="hlt">ice</span> and the associated effects of cloud properties. Cloud characteristics, surface radiative and turbulent <span class="hlt">fluxes</span>, and meteorological properties were measured throughout the field campaign. Here we explore how cloud macrophysical and microphysical properties affect young, thin sea <span class="hlt">ice</span> during three winter storms from 31 January to 15 February 2015. This time period is of interest due to the varying surface and atmospheric conditions, which showcase the variety of conditions the newly-formed sea <span class="hlt">ice</span> can experience during the winter. This period was characterized by large variations in the <span class="hlt">ice</span> surface and near-surface <span class="hlt">air</span> temperatures, with highs near 0°C when warm, moist <span class="hlt">air</span> was advected into the area and lows reaching -40°C during clear, calm periods between storms. The advection of warm, moist <span class="hlt">air</span> into the area influenced the cloud properties and enhanced the downwelling longwave <span class="hlt">flux</span>. For most of the period, downwelling longwave <span class="hlt">flux</span> correlates closely with the <span class="hlt">air</span> temperature. However, at the end of the first storm, a drop in downwelling longwave <span class="hlt">flux</span> of about 50 Wm-<span class="hlt">2</span> was observed, independent of any change in surface or <span class="hlt">air</span> temperature or cloud fraction, indicating a change in cloud properties. Lidar data show an increase in cloud height during this period and a potential shift in cloud phase from <span class="hlt">ice</span> to mixed-phase. This study will describe the cloud properties during the three winter storms and discuss their impacts on surface energy budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRG..122.3238C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRG..122.3238C"><span>Grain Yield Observations Constrain Cropland <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Over Europe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Combe, M.; de Wit, A. J. W.; Vilà-Guerau de Arellano, J.; van der Molen, M. K.; Magliulo, V.; Peters, W.</p> <p>2017-12-01</p> <p>Carbon exchange over croplands plays an important role in the European carbon cycle over daily to seasonal time scales. A better description of this exchange in terrestrial biosphere models—most of which currently treat crops as unmanaged grasslands—is needed to improve atmospheric <span class="hlt">CO</span><span class="hlt">2</span> simulations. In the framework we present here, we model gross European cropland <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> with a crop growth model constrained by grain yield observations. Our approach follows a two-step procedure. In the first step, we calculate day-to-day crop carbon <span class="hlt">fluxes</span> and pools with the WOrld FOod STudies (WOFOST) model. A scaling factor of crop growth is optimized regionally by minimizing the final grain carbon pool difference to crop yield observations from the Statistical Office of the European Union. In a second step, we re-run our WOFOST model for the full European 25 × 25 km gridded domain using the optimized scaling factors. We combine our optimized crop <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> with a simple soil respiration model to obtain the net cropland <span class="hlt">CO</span><span class="hlt">2</span> exchange. We assess our model's ability to represent cropland <span class="hlt">CO</span><span class="hlt">2</span> exchange using 40 years of observations at seven European <span class="hlt">Flux</span>Net sites and compare it with carbon <span class="hlt">fluxes</span> produced by a typical terrestrial biosphere model. We conclude that our new model framework provides a more realistic and strongly observation-driven estimate of carbon exchange over European croplands. Its products will be made available to the scientific community through the ICOS Carbon Portal and serve as a new cropland component in the CarbonTracker Europe inverse model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011BGeo....8..505M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011BGeo....8..505M"><span>Changes in ocean circulation and carbon storage are decoupled from <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marinov, I.; Gnanadesikan, A.</p> <p>2011-02-01</p> <p>The spatial distribution of the <span class="hlt">air</span>-sea <span class="hlt">flux</span> of carbon dioxide is a poor indicator of the underlying ocean circulation and of ocean carbon storage. The weak dependence on circulation arises because mixing-driven changes in solubility-driven and biologically-driven <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> largely cancel out. This cancellation occurs because mixing driven increases in the poleward residual mean circulation result in more transport of both remineralized nutrients and heat from low to high latitudes. By contrast, increasing vertical mixing decreases the storage associated with both the biological and solubility pumps, as it decreases remineralized carbon storage in the deep ocean and warms the ocean as a whole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010BGD.....7.7985M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010BGD.....7.7985M"><span>Changes in ocean circulation and carbon storage are decoupled from <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marinov, I.; Gnanadesikan, A.</p> <p>2010-11-01</p> <p>The spatial distribution of the <span class="hlt">air</span>-sea <span class="hlt">flux</span> of carbon dioxide is a poor indicator of the underlying ocean circulation and of ocean carbon storage. The weak dependence on circulation arises because mixing-driven changes in solubility-driven and biologically-driven <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> largely cancel out. This cancellation occurs because mixing driven increases in the poleward residual mean circulation results in more transport of both remineralized nutrients and heat from low to high latitudes. By contrast, increasing vertical mixing decreases the storage associated with both the biological and solubility pumps, as it decreases remineralized carbon storage in the deep ocean and warms the ocean as a whole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23712111','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23712111"><span>Dynamics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and environmental responses in the rain-fed winter wheat ecosystem of the Loess Plateau, China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Wen; Liao, Yuncheng; Wen, Xiaoxia; Guo, Qiang</p> <p>2013-09-01</p> <p>Chinese Loess Plateau plays an important role in carbon balance of terrestrial ecosystems. Continuous measurement of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in cropland ecosystem is of great significance to accurately evaluate the carbon sequestration potential and to better explain the carbon cycle process in this region. By using the eddy covariance system we conducted a long-term (from Sep 2009 to Jun 2010) <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> measurement in the rain-fed winter wheat field of the Chinese Loess Plateau and elaborated the responses of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to environmental factors. The results show that the winter wheat ecosystem has distinct seasonal dynamics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The total net ecosystem <span class="hlt">CO</span><span class="hlt">2</span> exchange (NEE) of -218.9±11.5 gC m(-<span class="hlt">2</span>) in the growing season, however, after considering the harvested grain, the agro-ecosystem turned into a weak carbon sink (-36.<span class="hlt">2</span> gC m(-<span class="hlt">2</span>)). On the other hand, the responses of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to environmental factors depended on different growth stages of winter wheat and different ranges of environmental variables, suggesting that the variations in <span class="hlt">CO</span><span class="hlt">2</span> exchange were sensitive to the changes in controlling factors. Particularly, we found the pulse response of ecosystem respiration (Reco) to a large rainfall event, and the strong fluctuations of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> usually appeared after effective rainfall events (daily precipitation > 5 mm) during middle growing season. Such phenomenon also occurred in the case of the drastic changes in <span class="hlt">air</span> temperature and within 5 days after field management (e.g. tillage and plough). Copyright © 2013 The Authors. Published by Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20180002067','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20180002067"><span>The Impact of Prior Biosphere Models in the Inversion of Global Terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> by Assimilating OCO-<span class="hlt">2</span> Retrievals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Philip, Sajeev; Johnson, Matthew S.</p> <p>2018-01-01</p> <p>Atmospheric mixing ratios of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) are largely controlled by anthropogenic emissions and biospheric <span class="hlt">fluxes</span>. The processes controlling terrestrial biosphere-atmosphere carbon exchange are currently not fully understood, resulting in terrestrial biospheric models having significant differences in the quantification of biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Atmospheric transport models assimilating measured (in situ or space-borne) <span class="hlt">CO</span><span class="hlt">2</span> concentrations to estimate "top-down" <span class="hlt">fluxes</span>, generally use these biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> as a priori information. Most of the <span class="hlt">flux</span> inversion estimates result in substantially different spatio-temporal posteriori estimates of regional and global biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The Orbiting Carbon Observatory <span class="hlt">2</span> (OCO-<span class="hlt">2</span>) satellite mission dedicated to accurately measure column <span class="hlt">CO</span><span class="hlt">2</span> (XCO<span class="hlt">2</span>) allows for an improved understanding of global biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. OCO-<span class="hlt">2</span> provides much-needed <span class="hlt">CO</span><span class="hlt">2</span> observations in data-limited regions facilitating better global and regional estimates of "top-down" <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> through inversion model simulations. The specific objectives of our research are to: 1) conduct GEOS-Chem 4D-Var assimilation of OCO-<span class="hlt">2</span> observations, using several state-of-the-science biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> models as a priori information, to better constrain terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, and <span class="hlt">2</span>) quantify the impact of different biospheric model prior <span class="hlt">fluxes</span> on OCO-<span class="hlt">2</span>-assimilated a posteriori <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates. Here we present our assessment of the importance of these a priori <span class="hlt">fluxes</span> by conducting Observing System Simulation Experiments (OSSE) using simulated OCO-<span class="hlt">2</span> observations with known "true" <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43C2466P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43C2466P"><span>Assessing the Importance of Prior Biospheric <span class="hlt">Fluxes</span> on Inverse Model Estimates of <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Philip, S.; Johnson, M. S.; Potter, C. S.; Genovese, V. B.</p> <p>2017-12-01</p> <p>Atmospheric mixing ratios of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) are largely controlled by anthropogenic emissions and biospheric sources/sinks. The processes controlling terrestrial biosphere-atmosphere carbon exchange are currently not fully understood, resulting in models having significant differences in the quantification of biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Currently, atmospheric chemical transport models (CTM) and global climate models (GCM) use multiple different biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> models resulting in large differences in simulating the global carbon cycle. The Orbiting Carbon Observatory <span class="hlt">2</span> (OCO-<span class="hlt">2</span>) satellite mission was designed to allow for the improved understanding of the processes involved in the exchange of carbon between terrestrial ecosystems and the atmosphere, and therefore allowing for more accurate assessment of the seasonal/inter-annual variability of <span class="hlt">CO</span><span class="hlt">2</span>. OCO-<span class="hlt">2</span> provides much-needed <span class="hlt">CO</span><span class="hlt">2</span> observations in data-limited regions allowing for the evaluation of model simulations of greenhouse gases (GHG) and facilitating global/regional estimates of "top-down" <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. We conduct a 4-D Variation (4D-Var) data assimilation with the GEOS-Chem (Goddard Earth Observation System-Chemistry) CTM using 1) OCO-<span class="hlt">2</span> land nadir and land glint retrievals and <span class="hlt">2</span>) global in situ surface flask observations to constrain biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. We apply different state-of-the-science year-specific <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> models (e.g., NASA-CASA (NASA-Carnegie Ames Stanford Approach), CASA-GFED (Global Fire Emissions Database), Simple Biosphere Model version 4 (SiB-4), and LPJ (Lund-Postdam-Jena)) to assess the impact of "a priori" <span class="hlt">flux</span> predictions to "a posteriori" estimates. We will present the "top-down" <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates for the year 2015 using OCO-<span class="hlt">2</span> and in situ observations, and a complete indirect evaluation of the a priori and a posteriori <span class="hlt">flux</span> estimates using independent in situ observations. We will also present our assessment of the variability of "top-down" <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates when using different</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B22E..06O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B22E..06O"><span>Progress Toward Measuring <span class="hlt">CO</span><span class="hlt">2</span> Isotopologue <span class="hlt">Fluxes</span> <em>in situ</em> with the LLNL Miniature, Laser-based <span class="hlt">CO</span><span class="hlt">2</span> Sensor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Osuna, J. L.; Bora, M.; Bond, T.</p> <p>2015-12-01</p> <p>One method to constrain photosynthesis and respiration independently at the ecosystem scale is to measure the <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>­ isotopologues. Instrumentation is currently available to makes these measurements but they are generally costly, large, bench-top instruments. Here, we present progress toward developing a laser-based sensor that can be deployed directly to a canopy to passively measure <span class="hlt">CO</span><span class="hlt">2</span> isotopologue <span class="hlt">fluxes</span>. In this study, we perform initial proof-of-concept and sensor characterization tests in the laboratory and in the field to demonstrate performance of the Lawrence Livermore National Laboratory (LLNL) tunable diode laser <span class="hlt">flux</span> sensor. The results shown herein demonstrate measurement of bulk <span class="hlt">CO</span><span class="hlt">2</span> as a first step toward achieving <span class="hlt">flux</span> measurements of <span class="hlt">CO</span><span class="hlt">2</span> isotopologues. The sensor uses a Vertical Cavity Surface Emitting Laser (VCSEL) in the 2012 nm range. The laser is mounted in a multi-pass White Cell. In order to amplify the absorption signal of <span class="hlt">CO</span><span class="hlt">2</span> in this range we employ wave modulation spectroscopy, introducing an alternating current (AC) bias component where f is the frequency of modulation on the laser drive current in addition to the direct current (DC) emission scanning component. We observed a strong linear relationship (r<span class="hlt">2</span> = 0.998 and r<span class="hlt">2</span> = 0.978 at all and low <span class="hlt">CO</span><span class="hlt">2</span> concentrations, respectively) between the <span class="hlt">2</span>f signal and the <span class="hlt">CO</span><span class="hlt">2</span> concentration in the cell across the range of <span class="hlt">CO</span><span class="hlt">2</span> concentrations relevant for <span class="hlt">flux</span> measurements. We use this calibration to interpret <span class="hlt">CO</span><span class="hlt">2</span> concentration of a gas flowing through the White cell in the laboratory and deployed over a grassy field. We will discuss sensor performance in the lab and in situ as well as address steps toward achieving canopy-deployed, passive measurements of <span class="hlt">CO</span><span class="hlt">2</span> isotopologue <span class="hlt">fluxes</span>. This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344. LLNL-ABS-675788</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SolE....8.1017Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SolE....8.1017Q"><span>Increasing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at Pisciarelli, Campi Flegrei, Italy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Queißer, Manuel; Granieri, Domenico; Burton, Mike; Arzilli, Fabio; Avino, Rosario; Carandente, Antonio</p> <p>2017-09-01</p> <p>The Campi Flegrei caldera is located in the metropolitan area of Naples (Italy) and has been undergoing different stages of unrest since 1950, evidenced by episodes of significant ground uplift followed by minor subsidence, increasing and fluctuating emission strengths of water vapor and <span class="hlt">CO</span><span class="hlt">2</span> from fumaroles, and periodic seismic crises. We deployed a scanning laser remote-sensing spectrometer (LARSS) that measured path-integrated <span class="hlt">CO</span><span class="hlt">2</span> concentrations in the Pisciarelli area in May 2017. The resulting mean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> is 578 ± 246 t d-1. Our data suggest a significant increase in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at this site since 2015. Together with recent geophysical observations, this suggests a greater contribution of the magmatic source to the degassing and/or an increase in permeability at shallow levels. Thanks to the integrated path soundings, LARSS may help to give representative measurements from large regions containing different <span class="hlt">CO</span><span class="hlt">2</span> sources, including fumaroles, low-temperature vents, and degassing soils, helping to constrain the contribution of deep gases and their migration mechanisms towards the surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4078843','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4078843"><span>Evidence for elevated and spatially variable geothermal <span class="hlt">flux</span> beneath the West Antarctic <span class="hlt">Ice</span> Sheet</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Schroeder, Dustin M.; Blankenship, Donald D.; Young, Duncan A.; Quartini, Enrica</p> <p>2014-01-01</p> <p>Heterogeneous hydrologic, lithologic, and geologic basal boundary conditions can exert strong control on the evolution, stability, and sea level contribution of marine <span class="hlt">ice</span> sheets. Geothermal <span class="hlt">flux</span> is one of the most dynamically critical <span class="hlt">ice</span> sheet boundary conditions but is extremely difficult to constrain at the scale required to understand and predict the behavior of rapidly changing glaciers. This lack of observational constraint on geothermal <span class="hlt">flux</span> is particularly problematic for the glacier catchments of the West Antarctic <span class="hlt">Ice</span> Sheet within the low topography of the West Antarctic Rift System where geothermal <span class="hlt">fluxes</span> are expected to be high, heterogeneous, and possibly transient. We use airborne radar sounding data with a subglacial water routing model to estimate the distribution of basal melting and geothermal <span class="hlt">flux</span> beneath Thwaites Glacier, West Antarctica. We show that the Thwaites Glacier catchment has a minimum average geothermal <span class="hlt">flux</span> of ∼114 ± 10 mW/m<span class="hlt">2</span> with areas of high <span class="hlt">flux</span> exceeding 200 mW/m<span class="hlt">2</span> consistent with hypothesized rift-associated magmatic migration and volcanism. These areas of highest geothermal <span class="hlt">flux</span> include the westernmost tributary of Thwaites Glacier adjacent to the subaerial Mount Takahe volcano and the upper reaches of the central tributary near the West Antarctic <span class="hlt">Ice</span> Sheet Divide <span class="hlt">ice</span> core drilling site. PMID:24927578</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C12A..08C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C12A..08C"><span>Capturing the Petermann <span class="hlt">Ice</span> Island <span class="hlt">Flux</span> With the CI<span class="hlt">2</span>D3 Database</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crawford, A. J.; Crocker, G.; Mueller, D.; Saper, R.; Desjardins, L.; Carrieres, T.</p> <p>2017-12-01</p> <p>The Petermann Glacier <span class="hlt">ice</span> tongue lost >460 km<span class="hlt">2</span> of areal extent ( 38 Gt of mass) due to three large calving events in 2008, 2010 and 2012, as well as three previously unrecorded events in 2011 and 2012. Hundreds of <span class="hlt">ice</span> islands subsequently drifted south between Hall Basin and Newfoundland's Grand Banks, but no systematic data collection or analysis has been conducted for the full <span class="hlt">flux</span> of fragments prior to the present study. To accomplish this, the Canadian <span class="hlt">Ice</span> Service's extensive RADARSAT-1 and -<span class="hlt">2</span> synthetic aperture radar image archive was mined to create the Canadian <span class="hlt">Ice</span> Island Drift, Deterioration and Detection (CI<span class="hlt">2</span>D3) Database. Over 15000 fragments have been digitized in GIS software from 3200 SAR scenes. A unique characteristic of the database is the inclusion of the lineage (i.e., connecting repeat observations or mother-daughter fragments) for all tracked fragments with areas >0.25 km<span class="hlt">2</span>. This genealogical information was used to isolate <span class="hlt">ice</span> islands that were about to fracture in order to assess the environmental conditions and morphological characteristics that influence this deterioration mechanism. Fracture counts showed a significant relationship with sea <span class="hlt">ice</span> concentration (r = -0.56). However, variations in relative thickness played a large role in fracturing likelihood regardless of sea <span class="hlt">ice</span> conditions. The exceedance probability of the daughter fragment length was calculated, as is often conducted for offshore industry hazard assessment. Grounded <span class="hlt">ice</span> islands, which are hazards to seafloor installations and disturb benthic ecology, were recognized from their negligible drift speeds and two grounding hot-spots were identified along the Coburg and eastern Baffin island coasts. Petermann <span class="hlt">ice</span> islands have been noted to drift along specific isobaths due to the influence of bathymetry on ocean currents. 50% of observations occurred between the 100 and 300 m isobaths, and smaller <span class="hlt">ice</span> islands were observed more frequently in deeper regions. The CI<span class="hlt">2</span>D3 Database can</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16...26P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16...26P"><span>Volcanic <span class="hlt">CO</span><span class="hlt">2</span> mapping and <span class="hlt">flux</span> measurements at Campi Flegrei by Tunable Diode Laser absorption Spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pedone, Maria; Aiuppa, Alessandro; Giudice, Gaetano; Grassa, Fausto; Chiodini, Giovanni; Valenza, Mariano</p> <p>2014-05-01</p> <p>Near-infrared room-temperature Tunable Diode Lasers (TDL) have recently found increased usage in atmospheric chemistry and <span class="hlt">air</span> monitoring research, but applications in Volcanology are still limited to a few examples. Here, we explored the potentiality of a commercial infrared laser unit (GasFinder <span class="hlt">2</span>.0 from Boreal Laser Ltd) to measurement of volcanic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> emissions. Our field tests were conducted at Campi Flegrei (near Pozzuoli, Southern Italy), where the GasFinder was used (during three campaigns in October 2012, January 2013 and May 2013) to repeatedly measure the path-integrated concentrations of <span class="hlt">CO</span><span class="hlt">2</span> along cross-sections of the atmospheric plumes of the two main fumarolic fields in the area (Solfatara and Pisciarelli). By using ad-hoc designed field-set-up and a tomographic post-processing routine, we resolved, for each of the <span class="hlt">2</span> manifestations, the contour maps of <span class="hlt">CO</span><span class="hlt">2</span> concentrations in their atmospheric plumes, from the integration of which (and after multiplication by the plumes' transport speeds) the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were finally obtained [1]. The so-calculated <span class="hlt">fluxes</span> average of 490 tons/day, which agrees well with independent evaluations of Aiuppa et al. (2013) [<span class="hlt">2</span>] (460 tons/day on average), and support a significant contribution of fumaroles to the total <span class="hlt">CO</span><span class="hlt">2</span> budget. The cumulative (fumarole [this study] +soil [<span class="hlt">2</span>]) <span class="hlt">CO</span><span class="hlt">2</span> output from Campi Flegrei is finally evaluated at 1600 tons/day. The application of lasers to volcanic gas studies is still an emerging (though intriguing) research field, and requires more testing and validation experiments. We conclude that TDL technique may valuably assist <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> quantification at a number of volcanic targets worldwide. [1] Pedone M. et al. (2013) Gold2013:abs:5563, Goldschmidt Conference, session 11a. [<span class="hlt">2</span>] Aiuppa A. et al. (2013) Geochemistry Geophysics Geosystems. doi: 10.1002/ggge.20261. [3] Chiodini G. et al. (2010) Journal of Geophysical Research, Volume 115, B03205. doi:10.1029/2008JB006258.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.1656L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.1656L"><span><span class="hlt">Air</span> content and O<span class="hlt">2</span>/N<span class="hlt">2</span> tuned chronologies on local insolation signatures in the Vostok <span class="hlt">ice</span> core are similar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lipenkov, V.; Raynaud, D.; Loutre, M.-F.; Duval, P.; Lemieux-Dudon, B.</p> <p>2009-04-01</p> <p>An accurate chronology of <span class="hlt">ice</span> cores is needed for interpreting the paleoclimatic record and understanding the relation between insolation and climate. A new domain of research in this area has been initially stimulated by the work of M. Bender (2002) linking the record of O<span class="hlt">2</span>/N<span class="hlt">2</span> ratio in the <span class="hlt">air</span> trapped in the Vostok <span class="hlt">ice</span> with the local insolation. More recently, it has been proposed that the long-term changes in <span class="hlt">air</span> content, V, recorded in <span class="hlt">ice</span> from the high Antarctic plateau is also dominantly imprinted by the local summer insolation (Raynaud et al., 2007). The present paper presents a new V record from Vostok, which is compared with the published Vostok O<span class="hlt">2</span>/N<span class="hlt">2</span> record for the same period of time (150-400 ka BP) by using the same spectral analysis methods. The spectral differences between the two properties and the possible mechanisms linking them with insolation through the surface snow structure and the close-off processes are discussed. The main result of our study is that the two experimentally independent local insolation proxies lead to absolute (orbital) time scales, which agree together within a standard deviation of 0.6 ka. This result strongly adds credibility to the <span class="hlt">air</span> content of <span class="hlt">ice</span> and the O<span class="hlt">2</span> to N<span class="hlt">2</span> ratio of the <span class="hlt">air</span> trapped in <span class="hlt">ice</span> as equally reliable and complementary tools for accurate dating of existing and future deep <span class="hlt">ice</span> cores. References: M. Bender, Orbital tuning chronology for the Vostok climate record supported by trapped gas composition, Earth and Planetary Science Letters 204(2002) 275-289. D. Raynaud, V. Lipenkov, B. Lemieux-Dudon, P. Duval, M.F. Loutre, N. Lhomme, The local insolation signature of <span class="hlt">air</span> content in Antarctic <span class="hlt">ice</span>: a new step toward an absolute dating of <span class="hlt">ice</span> records, Earth and Planetary Science Letters 261(2007) 337-349.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=85598&Lab=NERL&keyword=control+AND+group+AND+experimental&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=85598&Lab=NERL&keyword=control+AND+group+AND+experimental&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>SOIL <span class="hlt">FLUXES</span> OF <span class="hlt">CO</span><span class="hlt">2</span>, <span class="hlt">CO</span>, NO AND N<span class="hlt">2</span>O FROM AN OLD-PASTURE AND FROM NATIVE SAVANNA IN BRAZIL</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>We compared <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>, <span class="hlt">CO</span>, NO and N<span class="hlt">2</span>O, soil microbial biomass, and N-mineralization rates in a 20-year old Brachiaria pasture and a native cerrado area (savanna in Central Brazil). In order to assess the spatial variability of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, we tested the relation between elect...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC54C..04H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC54C..04H"><span><span class="hlt">Ice</span> Surface Temperature Variability in the Polar Regions and the Relationships to <span class="hlt">2</span> Meter <span class="hlt">Air</span> Temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hoyer, J.; Madsen, K. S.; Englyst, P. N.</p> <p>2017-12-01</p> <p>Determining the surface and near surface <span class="hlt">air</span> temperature from models or observations in the Polar Regions is challenging due to the extreme conditions and the lack of in situ observations. The errors in near surface temperature products are typically larger than for other regions of the world, and the potential for using Earth Observations is large. As part of the EU project, EUSTACE, we have developed empirical models for the relationship between the satellite observed skin <span class="hlt">ice</span> temperatures and <span class="hlt">2</span>m <span class="hlt">air</span> temperatures. We use the Arctic and Antarctic Sea and sea <span class="hlt">ice</span> Surface Temperatures from thermal Infrared satellite sensors (AASTI) reanalysis to estimate daily surface <span class="hlt">air</span> temperature over land <span class="hlt">ice</span> and sea <span class="hlt">ice</span> for the Arctic and the Antarctic. Large efforts have been put into collecting and quality controlling in situ observations from various data portals and research projects. The reconstruction is independent of numerical weather prediction models and thus provides an important alternative to modelled <span class="hlt">air</span> temperature estimates. The new surface <span class="hlt">air</span> temperature data record has been validated against more than 58.000 independent in situ measurements for the four surface types: Arctic sea <span class="hlt">ice</span>, Greenland <span class="hlt">ice</span> sheet, Antarctic sea <span class="hlt">ice</span> and Antarctic <span class="hlt">ice</span> sheet. The average correlations are 92-97% and average root mean square errors are 3.1-3.6°C for the four surface types. The root mean square error includes the uncertainty of the in-situ measurement, which ranges from 0.5 to <span class="hlt">2</span>°C. A comparison with ERA-Interim shows a consistently better performance of the satellite based <span class="hlt">air</span> temperatures than the ERA-Interim for the Greenland <span class="hlt">ice</span> sheet, when compared against observations not used in any of the two estimates. This is encouraging and demonstrates the values of these products. In addition, the procedure presented here works on satellite observations that are available in near real time and this opens up for a near real time estimation of the surface <span class="hlt">air</span> temperature over</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27363345','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27363345"><span>Grazing effects on ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> differ among temperate steppe types in Eurasia.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hou, Longyu; Liu, Yan; Du, Jiancai; Wang, Mingya; Wang, Hui; Mao, Peisheng</p> <p>2016-07-01</p> <p>Grassland ecosystems play a critical role in regulating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> into and out of the Earth's surface. Whereas previous studies have often addressed single <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> separately, few have addressed the relation among and controls of multiple <span class="hlt">CO</span><span class="hlt">2</span> sub-<span class="hlt">fluxes</span> simultaneously. In this study, we examined the relation among and controls of individual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (i.e., GEP, NEP, SR, ER, CR) in three contrasting temperate steppes of north China, as affected by livestock grazing. Our findings show that climatic controls of the seasonal patterns in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were both individual <span class="hlt">flux</span>- and steppe type-specific, with significant grazing impacts observed for canopy respiration only. In contrast, climatic controls of the annual patterns were only individual <span class="hlt">flux</span>-specific, with minor grazing impacts on the individual <span class="hlt">fluxes</span>. Grazing significantly reduced the mean annual soil respiration rate in the typical and desert steppes, but significantly enhanced both soil and canopy respiration in the meadow steppe. Our study suggests that a reassessment of the role of livestock grazing in regulating GHG exchanges is imperative in future studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120016605','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120016605"><span>Laboratory Spectra of <span class="hlt">CO</span><span class="hlt">2</span> Vibrational Modes in Planetary <span class="hlt">Ice</span> Analogs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>White, Douglas; Mastrapa, Rachel M.; Sandford, Scott</p> <p>2012-01-01</p> <p>Laboratory spectra have shown that <span class="hlt">CO</span><span class="hlt">2</span> is a powerful diagnostic tool for analyzing infrared data from remote observations, as it has been detected on icy moons in the outer Solar System as well as dust grain surfaces in the interstellar medium (ISM). IR absorption band profiles of <span class="hlt">CO</span><span class="hlt">2</span> within <span class="hlt">ice</span> mixtures containing H<span class="hlt">2</span>O and CH3OH change with respect to temperature and mixture ratios. In this particular study, the <span class="hlt">CO</span><span class="hlt">2</span> asymmetric stretching mode near 4.3 m (2350 cm (exp-1)), overtone mode near 1.97 m (5080 cm (exp-1)), and the combination bands near <span class="hlt">2</span>.7 m (3700 cm (exp-1)), <span class="hlt">2</span>.8 m (3600 cm (exp-1)), and <span class="hlt">2</span>.02 m (4960 cm (exp -1)), are systematically observed in different mixtures with H<span class="hlt">2</span>O and CH3OH in temperature ranges from 15K to 150 K. Additionally, some high-temperature deposits (T greater than 50 K) of H<span class="hlt">2</span>O, CH3OH, and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> mixtures were performed. These data may then be used to interpret infrared observational data obtained from icy surfaces in the outer Solar System and beyond.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920001603','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920001603"><span>Optical properties of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> and <span class="hlt">CO</span><span class="hlt">2</span> snow from ultraviolet to infrared: Application to frost deposits and clouds on Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hansen, Gary B.; Warren, Stephen G.; Leovy, Conway B.</p> <p>1991-01-01</p> <p>Researchers found that it is possible to grow large clear samples of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at Mars-like temperatures of 150-170K if a temperature controlled refrigerator is connected to an isolated two-phase pure <span class="hlt">CO</span><span class="hlt">2</span> system. They designed a chamber for transmission measurements whose optical path between the 13mm diameter window is adjustable from 1.6mm to 107mm. This will allow measurements of linear absorption down to less than 0.01 cm (exp -1). A preliminary transmission spectrum of a thick sample of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> in the near infrared was obtained. Once revised optical constants have been determined as a function of wavelength and temperature, they can be applied to spectral reflectance/emissivity models for <span class="hlt">CO</span><span class="hlt">2</span> snow surfaces, both pure and contaminated with dust and water <span class="hlt">ice</span>, using previously established approaches. It will be useful, also, to develop an infrared scattering-emission cloud radiance model (especially as viewed from near the limb) in order to develop a strategy for the identification of <span class="hlt">CO</span><span class="hlt">2</span> cloud layers by the atmospheric infrared radiometer instrument on the Mars Observer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013TCry....7..707R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013TCry....7..707R"><span>Ikaite crystal distribution in winter sea <span class="hlt">ice</span> and implications for <span class="hlt">CO</span><span class="hlt">2</span> system dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rysgaard, S.; Søgaard, D. H.; Cooper, M.; Pućko, M.; Lennert, K.; Papakyriakou, T. N.; Wang, F.; Geilfus, N. X.; Glud, R. N.; Ehn, J.; McGinnis, D. F.; Attard, K.; Sievers, J.; Deming, J. W.; Barber, D.</p> <p>2013-04-01</p> <p>The precipitation of ikaite (Ca<span class="hlt">CO</span>3 ⋅ 6H<span class="hlt">2</span>O) in polar sea <span class="hlt">ice</span> is critical to the efficiency of the sea <span class="hlt">ice</span>-driven carbon pump and potentially important to the global carbon cycle, yet the spatial and temporal occurrence of ikaite within the <span class="hlt">ice</span> is poorly known. We report unique observations of ikaite in unmelted <span class="hlt">ice</span> and vertical profiles of ikaite abundance and concentration in sea <span class="hlt">ice</span> for the crucial season of winter. <span class="hlt">Ice</span> was examined from two locations: a 1 m thick land-fast <span class="hlt">ice</span> site and a 0.3 m thick polynya site, both in the Young Sound area (74° N, 20° W) of NE Greenland. Ikaite crystals, ranging in size from a few μm to 700 μm, were observed to concentrate in the interstices between the <span class="hlt">ice</span> platelets in both granular and columnar sea <span class="hlt">ice</span>. In vertical sea <span class="hlt">ice</span> profiles from both locations, ikaite concentration determined from image analysis, decreased with depth from surface-<span class="hlt">ice</span> values of 700-900 μmol kg-1 <span class="hlt">ice</span> (~25 × 106 crystals kg-1) to values of 100-200 μmol kg-1 <span class="hlt">ice</span> (1-7 × 106 crystals kg-1) near the sea <span class="hlt">ice</span>-water interface, all of which are much higher (4-10 times) than those reported in the few previous studies. Direct measurements of total alkalinity (TA) in surface layers fell within the same range as ikaite concentration, whereas TA concentrations in the lower half of the sea <span class="hlt">ice</span> were twice as high. This depth-related discrepancy suggests interior <span class="hlt">ice</span> processes where ikaite crystals form in surface sea <span class="hlt">ice</span> layers and partly dissolve in layers below. Melting of sea <span class="hlt">ice</span> and dissolution of observed concentrations of ikaite would result in meltwater with a p<span class="hlt">CO</span><span class="hlt">2</span> of <15 μatm. This value is far below atmospheric values of 390 μatm and surface water concentrations of 315 μatm. Hence, the meltwater increases the potential for seawater uptake of <span class="hlt">CO</span><span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.7939Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.7939Z"><span>Application of Relaxed Eddy Accumulation (REA) method to estimate <span class="hlt">CO</span><span class="hlt">2</span> and CH4 surface <span class="hlt">fluxes</span> in the city of Krakow, southern Poland.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zimnoch, Miroslaw; Gorczyca, Zbigniew; Pieniazek, Katarzyna; Jasek, Alina; Chmura, Lukasz; Rozanski, Kazimierz</p> <p>2013-04-01</p> <p>There is a growing interest in the recent years in studies aimed at quantifying carbon cycling in urban centres. Worldwide migration of human population from rural to urban areas and corresponding growth of extensive urban agglomerations and megacities leads to intensification of anthropogenic emissions of carbon and strong disruption of natural carbon cycle on these areas. Therefore, a deeper understanding of the carbon "metabolism" of such regions is required. Apart of better quantification of surface carbon <span class="hlt">fluxes</span>, also a thorough understanding of the functioning of biosphere under strong anthropogenic influence is needed. Nowadays, covariance methods are widely applied for studying gas exchange between the atmosphere and the Earth's surface. Relaxed Eddy Accumulation method (REA), combined with the <span class="hlt">CO</span><span class="hlt">2</span> and CH4 CRDS analyser allows simultaneous measurements of surface <span class="hlt">fluxes</span> of carbon dioxide and methane within the chosen footprint of the detection system, thus making possible thorough characterisation of the overall exchange of those gases between the atmosphere and the urban surface across diverse spatial and temporal scales. Here we present preliminary results of the study aimed at quantifying surface <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 in Krakow, southern Poland. The REA system for <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> measurements has been installed on top of a 20m high tower mounted on the roof of the faculty building, close to the city centre of Krakow. The sensors were installed ca 42 m above the local ground. Gill Windmaster-Pro sonic anemometer was coupled with self-made system, designed by the Poznan University of Life Sciences, Poland, for collecting <span class="hlt">air</span> samples in two pairs of 10-liter Tedlar bags, and with Picarro G2101-i CRDS analyser. The <span class="hlt">air</span> was collected in 30-min intervals. The <span class="hlt">CO</span><span class="hlt">2</span> and CH4 mixing ratios in these cumulative downdraft and updraft <span class="hlt">air</span> samples were determined by the CRDS analyser after each sampling interval. Based on the measured mixing ratios difference and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22522230-systematic-variations-co-sub-sub-ice-abundance-ratios-nearby-galaxies-found-akari-near-infrared-spectroscopy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22522230-systematic-variations-co-sub-sub-ice-abundance-ratios-nearby-galaxies-found-akari-near-infrared-spectroscopy"><span>SYSTEMATIC VARIATIONS IN <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ICE</span> ABUNDANCE RATIOS IN NEARBY GALAXIES FOUND WITH AKARI NEAR-INFRARED SPECTROSCOPY</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Yamagishi, M.; Kaneda, H.; Ishihara, D.</p> <p>2015-07-01</p> <p>We report <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios in seven nearby star-forming galaxies based on the AKARI near-infrared (<span class="hlt">2</span>.5–5.0 μm) spectra. The <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios show clear variations between 0.05 and 0.<span class="hlt">2</span> with the averaged value of 0.14 ± 0.01. The previous study on M82 revealed that the <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios strongly correlate with the intensity ratios of the hydrogen recombination Brα line to the polycyclic aromatic hydrocarbon (PAH) 3.3 μm feature. In the present study, however, we find no correlation for the seven galaxies as a whole due to systematic differences in themore » relation between <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance and Brα/PAH 3.3 μm intensity ratios from galaxy to galaxy. This result suggests that there is another parameter that determines the <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios in a galaxy in addition to the Brα/PAH 3.3 μm ratios. We find that the <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios positively correlate with the specific star formation rates of the galaxies. From these results, we conclude that <span class="hlt">CO</span>{sub <span class="hlt">2</span>}/H{sub <span class="hlt">2</span>}O <span class="hlt">ice</span> abundance ratios tend to be high in young star-forming galaxies.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P53H..07W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P53H..07W"><span>Mass <span class="hlt">Fluxes</span> of <span class="hlt">Ice</span> and Oxygen Across the Entire Lid of Lake Vostok from Observations of Englacial Radiowave Attenuation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Winebrenner, D. P.; Kintner, P. M. S.; MacGregor, J. A.</p> <p>2017-12-01</p> <p>Over deep Antarctic subglacial lakes, spatially varying <span class="hlt">ice</span> thickness and the pressure-dependent melting point of <span class="hlt">ice</span> result in areas of melting and accretion at the <span class="hlt">ice</span>-water interface, i.e., the lake lid. These <span class="hlt">ice</span> mass <span class="hlt">fluxes</span> drive lake circulation and, because basal Antarctic <span class="hlt">ice</span> contains <span class="hlt">air</span>-clathrate, affect the input of oxygen to the lake, with implications for subglacial life. Inferences of melting and accretion from radar-layer tracking and geodesy are limited in spatial coverage and resolution. Here we develop a new method to estimate rates of accretion, melting, and the resulting oxygen input at a lake lid, using airborne radar data over Lake Vostok together with <span class="hlt">ice</span>-temperature and chemistry data from the Vostok <span class="hlt">ice</span> core. Because the lake lid is a coherent reflector of known reflectivity (at our radar frequency), we can infer depth-averaged radiowave attenuation in the <span class="hlt">ice</span>, with spatial resolution 1 km along flight lines. Spatial variation in attenuation depends mostly on variation in <span class="hlt">ice</span> temperature near the lid, which in turn varies strongly with <span class="hlt">ice</span> mass <span class="hlt">flux</span> at the lid. We model <span class="hlt">ice</span> temperature versus depth with <span class="hlt">ice</span> mass <span class="hlt">flux</span> as a parameter, thus linking that <span class="hlt">flux</span> to (observed) depth-averaged attenuation. The resulting map of melt- and accretion-rates independently reproduces features known from earlier studies, but now covers the entire lid. We find that accretion is dominant when integrated over the lid, with an <span class="hlt">ice</span> imbalance of 0.05 to 0.07 km3 a-1, which is robust against uncertainties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.H23D1006B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.H23D1006B"><span>Multi-channel Auto-dilution System for Remote Continuous Monitoring of High Soil-<span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barr, J. L.; Amonette, J. E.</p> <p>2008-12-01</p> <p>We describe a novel field instrument that takes input from up to 27 soil <span class="hlt">flux</span> chambers and measures <span class="hlt">flux</span> using the steady-state method. <span class="hlt">CO</span><span class="hlt">2</span> concentrations are determined with an infrared gas analyzer (IRGA, 0- 3000 ppmv range) with corrections for temperature, barometric pressure, and moisture content. The concentrations are monitored during data collection and, if they exceed the range of the IRGA, a stepped dilution program is automatically implemented that allows up to 50-fold dilution of the incoming gas stream with N<span class="hlt">2</span> supplied by boil-off from a large dewar. The upper concentration limit of the system with dilution is extended to at least 150,000 ppmv <span class="hlt">CO</span><span class="hlt">2</span>. The data are stored on a datalogger having a cellular modem connection that allows remote control of the system as well as transmittal of data. The system is designed to operate for six weeks with no on-site maintenance required. Longer periods are possible with modifications to allow on-site generation of N<span class="hlt">2</span> from <span class="hlt">air</span>. Example data from a recent <span class="hlt">CO</span><span class="hlt">2</span> test injection at the Zero- Emission Research and Technology (ZERT) field site in Bozeman, MT are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CorRe..32..239W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CorRe..32..239W"><span>Spatiotemporal variations in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in a fringing reef simulated using a novel carbonate system dynamics model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Watanabe, A.; Yamamoto, T.; Nadaoka, K.; Maeda, Y.; Miyajima, T.; Tanaka, Y.; Blanco, A. C.</p> <p>2013-03-01</p> <p>A carbonate system dynamics (CSD) model was developed in a fringing reef on the east coast of Ishigaki Island, southwest Japan, by incorporating organic and inorganic carbon <span class="hlt">fluxes</span> (photosynthesis and calcification), <span class="hlt">air</span>-sea gas exchanges, and benthic cover of coral and seagrass into a three-dimensional hydrodynamic model. The CSD model could reproduce temporal variations in dissolved inorganic carbon (DIC) and total alkalinity in coral zones, but not in seagrass meadows. The poor reproduction in seagrass meadows can be attributed to significant contributions of submarine groundwater discharge as well as misclassification of remotely sensed megabenthos in this area. In comparison with offshore areas, the reef acted as a <span class="hlt">CO</span><span class="hlt">2</span> sink during the observation period when it was averaged over 24 h. The CSD model also indicated large spatiotemporal differences in the carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) sink/source, possibly related to hydrodynamic features such as effective offshore seawater exchange and neap/spring tidal variation. This suggests that the data obtained from a single point observation may lead to misinterpretation of the overall trend and thus should be carefully considered. The model analysis also showed that the advective <span class="hlt">flux</span> of DIC from neighboring grids is several times greater than local biological <span class="hlt">flux</span> of DIC and is three orders of magnitude greater than the <span class="hlt">air</span>-sea gas <span class="hlt">flux</span> at the coral zone. Sensitivity tests in which coral or seagrass covers were altered revealed that the <span class="hlt">CO</span><span class="hlt">2</span> sink potential was much more sensitive to changes in coral cover than seagrass cover.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B33C0609S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B33C0609S"><span>Decadal trends in regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> estimated from atmospheric inversions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saeki, T.; Patra, P. K.</p> <p>2016-12-01</p> <p>Top-down approach (or atmospheric inversion) using atmospheric transport models and <span class="hlt">CO</span><span class="hlt">2</span> observations are an effective way to optimize surface <span class="hlt">fluxes</span> at subcontinental scales and monthly time intervals. We used the CCSR/NIES/FRCGC AGCM-based Chemistry Transport Model (JAMSTEC's ACTM) and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations at NOAA, CSIRO, JMA, NIES, NIES-MRI sites from Obspack GLOBALVIEW-<span class="hlt">CO</span><span class="hlt">2</span> data product (2013) for estimating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> for the period of 1990-2011. Carbon <span class="hlt">fluxes</span> were estimated for 84 partitions (54 lands + 30 oceans) of the globe by using a Bayesian synthesis inversion framework. A priori <span class="hlt">fluxes</span> are (1) atmosphere-ocean exchange from Takahashi et al. (2009), (<span class="hlt">2</span>) 3-hourly terrestrial biosphere <span class="hlt">fluxes</span> (annually balanced) from CASA model, and (3) fossil fuel <span class="hlt">fluxes</span> from CDIAC global totals and EDGAR4.<span class="hlt">2</span> spatial distributions. Four inversion cases have been tested with 1) 21 sites (sites which have real data fraction of 90 % or more for 1989-2012), <span class="hlt">2</span>) 21 sites + CONTRAIL data, 3) 66 sites (over 70 % coverage), and 4) 157 sites. As a result of time-dependent inversions, mean total <span class="hlt">flux</span> (excluding fossil fuel) for the period 1990-2011 is estimated to be -3.09 ±0.16 PgC/yr (mean and standard deviation of the four cases), where land (incl. biomass burning and land use change) and ocean absorb an average rate of -1.80 ±0.18 and -1.29 ±0.08 PgC/yr, respectively. The average global total sink from 1991-2000 to 2001-2010 increases by about 0.5 PgC/yr, mainly due to the increase in northern and tropical land sinks (Africa, Boreal Eurasia, East Asia and Europe), while ocean sinks show no clear trend. Inversion with CONTRAIL data estimates large positive <span class="hlt">flux</span> anomalies in late 1997 associated with the 1997/98 El-Nino, while inversion without CONTARIL data between Japan and Australia fails to estimate such large anomalies. Acknowledgements. This work is supported by the Environment Research and Technology Development Fund (<span class="hlt">2</span>-1401) of the Ministry of the Environment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B21E1987B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B21E1987B"><span>Carbon Dioxide and Water Vapor Concentrations, <span class="hlt">Co</span>-spectra and <span class="hlt">Fluxes</span> from Latest Standardized Automated <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">Flux</span> Systems versus Established Analyzer Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burba, G. G.; Kathilankal, J. C.; Begashaw, I.; Franzen, D.; Welles, J.; McDermitt, D. K.</p> <p>2017-12-01</p> <p>Spatial and temporal <span class="hlt">flux</span> data coverage have improved significantly in recent years, due to standardization, automation and management of data collection, and better handling of the generated data. With more stations and networks, larger data streams from each station, and smaller operating budgets, modern tools are required to effectively and efficiently handle the entire process.These tools should produce standardized verifiable datasets, and provide a way to cross-share the standardized data with external collaborators to leverage available funding, and promote data analyses and publications. In 2015, new open-path and enclosed <span class="hlt">flux</span> measurement systems1 were developed, based on established gas analyzer models<span class="hlt">2</span>,3, with the goal of improving stability in the presence of contamination, refining temperature control and compensation, and providing more accurate gas concentration measurements. In 2017, the new open-path system was further refined to simplify hardware configuration, and to reduce power consumption and cost. Additionally, all new systems incorporate complete automated on-site <span class="hlt">flux</span> calculations using EddyPro® Software4 run by a weatherized remotely-accessible microcomputer to provide standardized traceable data sets for <span class="hlt">fluxes</span> and supporting variables. This presentation will describe details and results from the field tests of the new <span class="hlt">flux</span> systems, in comparison to older models and reference instruments. References:1 Burba G., W. Miller, I. Begashaw, G. Fratini, F. Griessbaum, J. Kathilankal, L. Xu, D. Franz, E. Joseph, E. Larmanou, S. Miller, D. Papale, S. Sabbatini, T. Sachs, R. Sakai, D. McDermitt, 2017. Comparison of <span class="hlt">CO</span><span class="hlt">2</span> Concentrations, <span class="hlt">Co</span>-spectra and <span class="hlt">Flux</span> Measurements between Latest Standardized Automated <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O <span class="hlt">Flux</span> Systems and Older Gas Analysers. 10th ICDC Conference, Switzerland: 21-25/08 <span class="hlt">2</span> Metzger, S., G. Burba, S. Burns, P. Blanken, J. Li, H. Luo, R. Zulueta, 2016. Optimization of an enclosed gas analyzer sampling system for measuring eddy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.7189B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.7189B"><span>The impact of transport model differences on <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">flux</span> estimates from OCO-<span class="hlt">2</span> retrievals of column average <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Basu, Sourish; Baker, David F.; Chevallier, Frédéric; Patra, Prabir K.; Liu, Junjie; Miller, John B.</p> <p>2018-05-01</p> <p>We estimate the uncertainty of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates in atmospheric inversions stemming from differences between different global transport models. Using a set of observing system simulation experiments (OSSEs), we estimate this uncertainty as represented by the spread between five different state-of-the-art global transport models (ACTM, LMDZ, GEOS-Chem, PCTM and TM5), for both traditional in situ <span class="hlt">CO</span><span class="hlt">2</span> inversions and inversions of XCO<span class="hlt">2</span> estimates from the Orbiting Carbon Observatory <span class="hlt">2</span> (OCO-<span class="hlt">2</span>). We find that, in the absence of relative biases between in situ <span class="hlt">CO</span><span class="hlt">2</span> and OCO-<span class="hlt">2</span> XCO<span class="hlt">2</span>, OCO-<span class="hlt">2</span> estimates of terrestrial <span class="hlt">flux</span> for TRANSCOM-scale land regions can be more robust to transport model differences than corresponding in situ <span class="hlt">CO</span><span class="hlt">2</span> inversions. This is due to a combination of the increased spatial coverage of OCO-<span class="hlt">2</span> samples and the total column nature of OCO-<span class="hlt">2</span> estimates. We separate the two effects by constructing hypothetical in situ networks with the coverage of OCO-<span class="hlt">2</span> but with only near-surface samples. We also find that the transport-driven uncertainty in <span class="hlt">fluxes</span> is comparable between well-sampled northern temperate regions and poorly sampled tropical regions. Furthermore, we find that spatiotemporal differences in sampling, such as between OCO-<span class="hlt">2</span> land and ocean soundings, coupled with imperfect transport, can produce differences in <span class="hlt">flux</span> estimates that are larger than <span class="hlt">flux</span> uncertainties due to transport model differences. This highlights the need for sampling with as complete a spatial and temporal coverage as possible (e.g., using both land and ocean retrievals together for <span style="" class="text">OCO-<span class="hlt">2</span>) to minimize the impact of selective sampling. Finally, our annual and monthly estimates of transport-driven uncertainties can be used to evaluate the robustness of conclusions drawn from real OCO-<span class="hlt">2</span> and in situ <span class="hlt">CO</span><span class="hlt">2</span> inversions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A13B2066N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A13B2066N"><span>14<span class="hlt">CO</span> in Antarctic Glacial <span class="hlt">Ice</span> as a Tracer of Changes in Atmospheric OH Abundance from 1880 AD to Present</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neff, P. D.; Petrenko, V. V.; Hmiel, B.; Smith, A. W.; Buizert, C.; Etheridge, D. M.; Murray, L. T.; Dyonisius, M.</p> <p>2017-12-01</p> <p>OH is the main tropospheric oxidant and determines the lifetime of methane and most other trace gases in the atmosphere, thereby controlling the amount of greenhouse warming that these gases can produce. Changes in [OH] in response to large changes in reactive trace gas emissions (which may occur in the future) are uncertain. Measurements of 14C-containing carbon monoxide (14<span class="hlt">CO</span>) and other tracers such as methyl chloroform over the last ≈25 years have been successfully used to monitor changes in average OH concentration ([OH]), but there are no observational constraints on [OH] further back in time. Reconstructions of 14<span class="hlt">CO</span> from <span class="hlt">ice</span> cores could in principle provide such constraints but are complicated by in-situ production of 14<span class="hlt">CO</span> by cosmic rays directly in the <span class="hlt">ice</span>. Recent work in Antarctica and Greenland shows that this in-situ component would be relatively small and can be accurately corrected for at sites with very high snow accumulation rates. We propose to sample firn-<span class="hlt">air</span> and shallow <span class="hlt">ice</span> to ≈230 m depth at Law Dome, Antarctica (site DE-08, 1.<span class="hlt">2</span> m a-1 <span class="hlt">ice</span>-equivalent snow accumulation), extracting trapped <span class="hlt">air</span> from the <span class="hlt">ice</span> cores on-site using a new large-volume <span class="hlt">ice</span> melting system. 14<span class="hlt">CO</span> will be analyzed in firn and <span class="hlt">ice</span> core <span class="hlt">air</span> samples, and accurate corrections made for the in-situ cosmogenic 14<span class="hlt">CO</span> component in the ice—allowing for the atmospheric 14<span class="hlt">CO</span> history to be reconstructed. This 14<span class="hlt">CO</span> history will be interpreted with the aid of a chemistry-transport model to place the first observational constraints on the variability of Southern Hemisphere [OH] since ≈1880 AD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A44A..06N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A44A..06N"><span>Imposing strong constraints on tropical terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using passenger aircraft based measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Niwa, Y.; Machida, T.; Sawa, Y.; Matsueda, H.; Schuck, T. J.; Brenninkmeijer, C. A.; Imasu, R.; Satoh, M.</p> <p>2011-12-01</p> <p>Better understanding of the global and regional carbon budget is needed to perform a reliable prediction of future climate with an earth system model. However, the reliability of <span class="hlt">CO</span><span class="hlt">2</span> source/sink estimation by inverse modeling, which is one of the promising methods to estimate regional carbon budget, is limited because of sparse observational data coverage. Very few observational data are available in tropics. Therefore, especially the reconstruction of tropical terrestrial <span class="hlt">fluxes</span> has considerable uncertainties. In this study, regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> for 2006-2008 are estimated by inverse modeling using the Comprehensive Observation Network for Trace gases by Airliner (CONTRAIL) in addition to the surface measurement dataset of GLOBALVIEW-<span class="hlt">CO</span><span class="hlt">2</span>. CONTRAIL is a recently established <span class="hlt">CO</span><span class="hlt">2</span> measurement network using in-situ measurement instruments on board commercial aircraft. Five CONTRAIL aircraft travel back and forth between Japan and many areas: Europe, North America, Southeast Asia, South Asia, and Australia. The Bayesian synthesis approach is used to estimate monthly <span class="hlt">fluxes</span> for 42 regions using NICAM-TM simulations with existing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> datasets and monthly mean observational data. It is demonstrated that the aircraft data have great impact on estimated tropical terrestrial <span class="hlt">fluxes</span>. By adding the aircraft data to the surface data, the analyzed uncertainty of tropical <span class="hlt">fluxes</span> has been reduced by 15 % and more than 30 % uncertainty reduction rate is found in Southeast and South Asia. Specifically, for annual net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, nearly neutral <span class="hlt">fluxes</span> of Indonesia, which is estimated using the surface dataset alone, turn to positive <span class="hlt">fluxes</span>, i.e. carbon sources. In Indonesia, a remarkable carbon release during the severe drought period of October-December in 2006 is estimated, which suggests that biosphere respiration or biomass burning was larger than the prior <span class="hlt">fluxes</span>. Comparison of the optimized atmospheric <span class="hlt">CO</span><span class="hlt">2</span> with independent aircraft measurements of CARIBIC tends to validate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B53G0599C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B53G0599C"><span>Year-round Regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> from Boreal and Tundra Ecosystems in Alaska</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Commane, R.; Lindaas, J.; Benmergui, J. S.; Luus, K. A.; Chang, R. Y. W.; Daube, B. C.; Euskirchen, E. S.; Henderson, J.; Karion, A.; Miller, J. B.; Miller, S. M.; Parazoo, N.; Randerson, J. T.; Sweeney, C.; Tans, P. P.; Thoning, K. W.; Veraverbeke, S.; Miller, C. E.; Wofsy, S. C.</p> <p>2016-12-01</p> <p>High-latitude ecosystems could release large amounts of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) to the atmosphere in a warmer climate. We derive temporally and spatially resolved year-round <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Alaska from a synthesis of airborne and tower <span class="hlt">CO</span><span class="hlt">2</span> observations in 2012-2014. We find that tundra ecosystems were net sources of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. We discuss these <span class="hlt">flux</span> estimates in the context of long-term <span class="hlt">CO</span><span class="hlt">2</span> measurements at Barrow, AK, to asses the long term trend in carbon <span class="hlt">fluxes</span> in the Arctic. Many Earth System Models incorrectly simulate net carbon uptake in Alaska presently. Our results imply that annual net emission of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere may have increased markedly in this region of the Arctic in response to warming climate, supporting the view that climate-carbon feedback is strongly positive in the high Arctic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24489821','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24489821"><span>The response of Antarctic sea <span class="hlt">ice</span> algae to changes in pH and <span class="hlt">CO</span><span class="hlt">2</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McMinn, Andrew; Müller, Marius N; Martin, Andrew; Ryan, Ken G</p> <p>2014-01-01</p> <p>Ocean acidification substantially alters ocean carbon chemistry and hence pH but the effects on sea <span class="hlt">ice</span> formation and the <span class="hlt">CO</span><span class="hlt">2</span> concentration in the enclosed brine channels are unknown. Microbial communities inhabiting sea <span class="hlt">ice</span> ecosystems currently contribute 10-50% of the annual primary production of polar seas, supporting overwintering zooplankton species, especially Antarctic krill, and seeding spring phytoplankton blooms. Ocean acidification is occurring in all surface waters but the strongest effects will be experienced in polar ecosystems with significant effects on all trophic levels. Brine algae collected from McMurdo Sound (Antarctica) sea <span class="hlt">ice</span> was incubated in situ under various carbonate chemistry conditions. The carbon chemistry was manipulated with acid, bicarbonate and bases to produce a p<span class="hlt">CO</span><span class="hlt">2</span> and pH range from 238 to 6066 µatm and 7.19 to 8.66, respectively. Elevated p<span class="hlt">CO</span><span class="hlt">2</span> positively affected the growth rate of the brine algal community, dominated by the unique <span class="hlt">ice</span> dinoflagellate, Polarella glacialis. Growth rates were significantly reduced when pH dropped below 7.6. However, when the pH was held constant and the p<span class="hlt">CO</span><span class="hlt">2</span> increased, growth rates of the brine algae increased by more than 20% and showed no decline at p<span class="hlt">CO</span><span class="hlt">2</span> values more than five times current ambient levels. We suggest that projected increases in seawater p<span class="hlt">CO</span><span class="hlt">2</span>, associated with OA, will not adversely impact brine algal communities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060032490&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsonar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060032490&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsonar"><span>Combined Satellite - and ULS-Derived Sea-<span class="hlt">Ice</span> <span class="hlt">Flux</span> in the Weddell Sea</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Drinkwater, M.; Liu, X.; Harms, S.</p> <p>2000-01-01</p> <p>Several years of daily microwave satellite <span class="hlt">ice</span>-drift are combined with moored Upward Looking Sonar (ULS) <span class="hlt">ice</span>-drafts into an <span class="hlt">ice</span> volume <span class="hlt">flux</span> record at points along a <span class="hlt">flux</span> gate across the Weddell Sea, Antarctica.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.P31A0118B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.P31A0118B"><span>Landscape Evolution and the Reincarnation of the Residual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Cap of Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Byrne, S.; Zuber, M.</p> <p>2006-12-01</p> <p>Observations of the southern residual <span class="hlt">CO</span><span class="hlt">2</span> cap of Mars reveal a wide range of landforms including flat-floored quasi-circular pits with steep walls (dubbed Swiss-cheese features). Interannual comparisons show that these depressions are expanding laterally at rates of ~<span class="hlt">2</span>m/yr to ~4m/yr, prompting suggestions of climate change. The residual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cap is up to 10m thick and underlain by an involatile basement, it also contains layers roughly <span class="hlt">2</span>m thick representing different accumulation episodes in the recent past. Changes in the appearance of the residual <span class="hlt">ice</span> between the Mariner 9 and Viking missions indicate that the top-most layer was deposited in that time-frame, soon after the global dust storm of 1971. The spatial density of the Swiss-cheese features, and the rate at which they expand, mean that it is unlikely that any part of the residual <span class="hlt">ice</span> cap is older than a few centuries. Given this, we may ask: how can there be a residual cap present today for us to observe? To answer this and other questions we have developed a model to examine the evolution of a <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> landscape. This model reproduces the morphologies and expansion rates seen in the actual residual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> cap. Our model results indicate that the fate of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> surfaces is controlled by their surface roughness. Surface roughness always increases with time, which results in an unstable situation. When the surface roughness exceeds a critical point small pits can begin to develop. The walls of these pits rapidly steepen and begin retreating which enlarges and deepens the pit. This situation always occurs even if the surface of the <span class="hlt">CO</span><span class="hlt">2</span> slab has a high enough albedo to have a net mass gain each year. Once these pits begin expanding they quickly erode the entire <span class="hlt">ice</span> slab. When the underlying non-<span class="hlt">CO</span><span class="hlt">2</span> material is exposed, it will not frost over again if Mars were to repeat like clockwork every year. We conclude that interannual climatic variability is actually a requirement for the continued existence of a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC21D1126A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC21D1126A"><span>Sensitivity of Great Lakes <span class="hlt">Ice</span> Cover to <span class="hlt">Air</span> Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Austin, J. A.; Titze, D.</p> <p>2016-12-01</p> <p><span class="hlt">Ice</span> cover is shown to exhibit a strong linear sensitivity to <span class="hlt">air</span> temperature. Upwards of 70% of <span class="hlt">ice</span> cover variability on all of the Great Lakes can be explained in terms of <span class="hlt">air</span> temperature, alone, and nearly 90% of <span class="hlt">ice</span> cover variability can be explained in some lakes. <span class="hlt">Ice</span> cover sensitivity to <span class="hlt">air</span> temperature is high, and a difference in seasonally-averaged (Dec-May) <span class="hlt">air</span> temperature on the order of 1°C to <span class="hlt">2</span>°C can be the difference between a low-<span class="hlt">ice</span> year and a moderate- to high- <span class="hlt">ice</span> year. The total amount of seasonal <span class="hlt">ice</span> cover is most influenced by <span class="hlt">air</span> temperatures during the meteorological winter, contemporaneous with the time of <span class="hlt">ice</span> formation. <span class="hlt">Air</span> temperature conditions during the pre-winter conditioning period and during the spring melting period were found to have less of an impact on seasonal <span class="hlt">ice</span> cover. This is likely due to the fact that there is a negative feedback mechanism when heat loss goes toward cooling the lake, but a positive feedback mechanism when heat loss goes toward <span class="hlt">ice</span> formation. <span class="hlt">Ice</span> cover sensitivity relationships were compared between shallow coastal regions of the Great Lakes and similarly shallow smaller, inland lakes. It was found that the sensitivity to <span class="hlt">air</span> temperature is similar between these coastal regions and smaller lakes, but that the absolute amount of <span class="hlt">ice</span> that forms varies significantly between small lakes and the Great Lakes, and amongst the Great Lakes themselves. The Lake Superior application of the ROMS three-dimensional hydrodynamic numerical model verifies a deterministic linear relationship between <span class="hlt">air</span> temperature and <span class="hlt">ice</span> cover, which is also strongest around the period of <span class="hlt">ice</span> formation. When the Lake Superior bathymetry is experimentally adjusted by a constant vertical multiplier, average lake depth is shown to have a nonlinear relationship with seasonal <span class="hlt">ice</span> cover, and this nonlinearity may be associated with a nonlinear increase in the lake-wide volume of the surface mixed layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015A%26A...584A..14M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015A%26A...584A..14M"><span>UV photoprocessing of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>: a complete quantification of photochemistry and photon-induced desorption processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martín-Doménech, R.; Manzano-Santamaría, J.; Muñoz Caro, G. M.; Cruz-Díaz, G. A.; Chen, Y.-J.; Herrero, V. J.; Tanarro, I.</p> <p>2015-12-01</p> <p>Context. <span class="hlt">Ice</span> mantles that formed on top of dust grains are photoprocessed by the secondary ultraviolet (UV) field in cold and dense molecular clouds. UV photons induce photochemistry and desorption of <span class="hlt">ice</span> molecules. Experimental simulations dedicated to <span class="hlt">ice</span> analogs under astrophysically relevant conditions are needed to understand these processes. Aims: We present UV-irradiation experiments of a pure <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> analog. Calibration of the quadrupole mass spectrometer allowed us to quantify the photodesorption of molecules to the gas phase. This information was added to the data provided by the Fourier transform infrared spectrometer on the solid phase to obtain a complete quantitative study of the UV photoprocessing of an <span class="hlt">ice</span> analog. Methods: Experimental simulations were performed in an ultra-high vacuum chamber. <span class="hlt">Ice</span> samples were deposited onto an infrared transparent window at 8K and were subsequently irradiated with a microwave-discharged hydrogen flow lamp. After irradiation, <span class="hlt">ice</span> samples were warmed up until complete sublimation was attained. Results: Photolysis of <span class="hlt">CO</span><span class="hlt">2</span> molecules initiates a network of photon-induced chemical reactions leading to the formation of <span class="hlt">CO</span>, <span class="hlt">CO</span>3, O<span class="hlt">2</span>, and O3. During irradiation, photon-induced desorption of <span class="hlt">CO</span> and, to a lesser extent, O<span class="hlt">2</span> and <span class="hlt">CO</span><span class="hlt">2</span> took place through a process called indirect desorption induced by electronic transitions, with maximum photodesorption yields (Ypd) of ~1.<span class="hlt">2</span> × 10-<span class="hlt">2</span> molecules incident photon-1, ~9.3 × 10-4 molecules incident photon-1, and ~1.1 × 10-4 molecules incident photon-1, respectively. Conclusions: Calibration of mass spectrometers allows a direct quantification of photodesorption yields instead of the indirect values that were obtained from infrared spectra in most previous works. Supplementary information provided by infrared spectroscopy leads to a complete quantification, and therefore a better understanding, of the processes taking place in UV-irradiated <span class="hlt">ice</span> mantles. Appendix A is available in</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BVol...75..757M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BVol...75..757M"><span>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> baseline in an urban monogenetic volcanic field: the Auckland Volcanic Field, New Zealand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazot, Agnès; Smid, Elaine R.; Schwendenmann, Luitgard; Delgado-Granados, Hugo; Lindsay, Jan</p> <p>2013-11-01</p> <p>The Auckland Volcanic Field (AVF) is a dormant monogenetic basaltic field located in Auckland, New Zealand. Though soil gas <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are routinely used to monitor volcanic regions, there have been no published studies of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> or soil gas <span class="hlt">CO</span><span class="hlt">2</span> concentrations in the AVF to date or many other monogenetic fields worldwide. We measured soil gas <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and soil gas <span class="hlt">CO</span><span class="hlt">2</span> concentrations in 2010 and 2012 in varying settings, seasons, and times of day to establish a baseline soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and to determine the major sources of and controlling influences on Auckland's soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements varied from 0 to 203 g m-<span class="hlt">2</span> day-1, with an average of 27.1 g m-<span class="hlt">2</span> day-1. Higher <span class="hlt">fluxes</span> were attributed to varying land use properties (e.g., landfill). Using a graphical statistical approach, two populations of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were identified. Isotope analyses of δ13<span class="hlt">CO</span><span class="hlt">2</span> confirmed that the source of <span class="hlt">CO</span><span class="hlt">2</span> in the AVF is biogenic with no volcanic component. These data may be used to assist with eruption forecasting in the event of precursory activity in the AVF, and highlight the importance of knowing land use history when assessing soil gas <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in urban environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70021683','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70021683"><span>Estimating lake-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> exchange</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Anderson, D.E.; Striegl, Robert G.; Stannard, D.I.; Michmerhuizen, C.M.; McConnaughey, T.A.; LaBaugh, J.W.</p> <p>1999-01-01</p> <p>Lake-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was directly measured above a small, woodland lake using the eddy covariance technique and compared with <span class="hlt">fluxes</span> deduced from changes in measured lake-water <span class="hlt">CO</span><span class="hlt">2</span> storage and with <span class="hlt">flux</span> predictions from boundary-layer and surface-renewal models. Over a 3-yr period, lake-atmosphere exchanges of <span class="hlt">CO</span><span class="hlt">2</span> were measured over 5 weeks in spring, summer, and fall. Observed springtime <span class="hlt">CO</span><span class="hlt">2</span> efflux was large (<span class="hlt">2.3-2</span>.7 ??mol m-<span class="hlt">2</span> s-1) immediately after lake-thaw. That efflux decreased exponentially with time to less than 0.<span class="hlt">2</span> ??mol m-<span class="hlt">2</span> s-1 within <span class="hlt">2</span> weeks. Substantial interannual variability was found in the magnitudes of springtime efflux, surface water <span class="hlt">CO</span><span class="hlt">2</span> concentrations, lake <span class="hlt">CO</span><span class="hlt">2</span> storage, and meteorological conditions. Summertime measurements show a weak diurnal trend with a small average downward <span class="hlt">flux</span> (-0.17 ??mol m-<span class="hlt">2</span> s-1) to the lake's surface, while late fall <span class="hlt">flux</span> was trendless and smaller (-0.0021 ??mol m-<span class="hlt">2</span> s-1). Large springtime efflux afforded an opportunity to make direct measurement of lake-atmosphere <span class="hlt">fluxes</span> well above the detection limits of eddy covariance instruments, facilitating the testing of different gas <span class="hlt">flux</span> methodologies and <span class="hlt">air</span>-water gas-transfer models. Although there was an overall agreement in <span class="hlt">fluxes</span> determined by eddy covariance and those calculated from lake-water storage change in <span class="hlt">CO</span><span class="hlt">2</span>, agreement was inconsistent between eddy covariance <span class="hlt">flux</span> measurements and <span class="hlt">fluxes</span> predicted by boundary-layer and surface-renewal models. Comparison of measured and modeled transfer velocities for <span class="hlt">CO</span><span class="hlt">2</span>, along with measured and modeled cumulative <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, indicates that in most instances the surface-renewal model underpredicts actual <span class="hlt">flux</span>. Greater underestimates were found with comparisons involving homogeneous boundary-layer models. No physical mechanism responsible for the inconsistencies was identified by analyzing coincidentally measured environmental variables.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.C21C0359C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.C21C0359C"><span>Buried <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> traces in South Polar Layered Deposits of Mars detected by radar sounder</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Castaldo, L.; Mège, D.; Orosei, R.; Séjourné, A.</p> <p>2014-12-01</p> <p>SHARAD (SHAllow RADar) is the subsurface sounding radar provided by the Italian Space Agency (ASI) as a facility instrument to NASA's 2005 Mars Reconnaissance Orbiter (MRO). The Reduced Data Record of SHARAD data covering the area of the South Polar Layered Deposits (SPLD), has been used. The elaboration and interpretation of the data, aimed to estimate electromagnetic properties of surface layers, has been performed in terms of permittivity. The theory of electromagnetic scattering from fractal surfaces, and the estimation of geometric parameters from topographic data by Mars Orbiter Laser Altimeter (MOLA) which was one of five instruments on board the Mars Global Surveyor (MGS) spacecraft, has been used. A deep analysis of inversion has been made on all Mars and extended to the South Polar Caps in order to extract the area with a permittivity constant of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. Several corrections have been applied to the data, moreover the calibration of the signal requires the determination of a constant that takes into account the power gain due to the radar system and the surface in order to compensate the power losses due to the orbitographic phenomena. The determination of regions with high probability of buried <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> in the first layer of the Martian surface, is obtained extracting the real part of the permittivity constant of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> (~<span class="hlt">2</span>), estimated by other means. The permittivity of <span class="hlt">CO</span><span class="hlt">2</span><span class="hlt">ice</span> is extracted from the Global Permittivity Map of Mars using the global standard deviation of itself as following: ɛ<span class="hlt">CO</span><span class="hlt">2</span><span class="hlt">ice=ɛCO</span><span class="hlt">2</span><span class="hlt">ice</span>+ Σ (1)where Σ=±std(ɛMapMars)/<span class="hlt">2</span>Figure 1(a) shows the south polar areas where the values of the permittivity point to the possibility of a <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> layer. Figure 1(b) is the corresponding geologic map. The comparison between the two maps indicates that the area with probable buried <span class="hlt">CO</span><span class="hlt">2</span> overlaps Hesperian and Amazonian polar units (Hp, Hesperian plains-forming deposits marked by narrow sinuous, anabranching ridges and irregular depressions, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1255257-co2-fluxing-collapses-metal-mobility-magmatic-vapour','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1255257-co2-fluxing-collapses-metal-mobility-magmatic-vapour"><span><span class="hlt">CO</span> <span class="hlt">2</span>-<span class="hlt">fluxing</span> collapses metal mobility in magmatic vapour</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>van Hinsberg, V. J.; Berlo, K.; Migdisov, A. A.; ...</p> <p>2016-05-18</p> <p>Magmatic systems host many types of ore deposits, including world-class deposits of copper and gold. Magmas are commonly an important source of metals and ore-forming fluids in these systems. In many magmatic-hydrothermal systems, low-density aqueous fluids, or vapours, are significant metal carriers. Such vapours are water-dominated shallowly, but <span class="hlt">fluxing</span> of <span class="hlt">CO</span> <span class="hlt">2</span>-rich vapour exsolved from deeper magma is now recognised as ubiquitous during open-system magma degassing. Furthermore, we show that such <span class="hlt">CO</span> <span class="hlt">2</span>-<span class="hlt">fluxing</span> leads to a sharp drop in element solubility, up to a factor of 10,000 for Cu, and thereby provides a highly efficient, but as yet unrecognised mechanismmore » for metal deposition.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070025049&hterms=chemical+reactions&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dchemical%2Breactions','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070025049&hterms=chemical+reactions&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dchemical%2Breactions"><span>Ab initio Quantum Chemical Studies of Reactions in Astrophysical <span class="hlt">Ices</span>. Reactions Involving CH3OH, <span class="hlt">CO</span><span class="hlt">2</span>, <span class="hlt">CO</span>, HNCO in H<span class="hlt">2</span><span class="hlt">CO</span>/NH3/H<span class="hlt">2</span>O <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Woon, David E.</p> <p>2006-01-01</p> <p>While reactions between closed shell molecules generally involve prohibitive barriers in the gas phase, prior experimental and theoretical studies have demonstrated that some of these reactions are significantly enhanced when confined within an icy grain mantle and can occur efficiently at temperatures below 100 K with no additional energy processing. The archetypal case is the reaction of formaldehyde (H<span class="hlt">2</span><span class="hlt">CO</span>) and ammonia (NH3) to yield hydroxymethylamine (NH<span class="hlt">2</span>CH<span class="hlt">2</span>OH). In the present work we have characterized reactions involving methanol (CH3OH), carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), carbon monoxide (<span class="hlt">CO</span>), and isocyanic acid (HNCO) in search of other favorable cases. Most of the emphasis is on CH3OH, which was investigated in the two-body reaction with one H<span class="hlt">2</span><span class="hlt">CO</span> and the three-body reaction with two H<span class="hlt">2</span><span class="hlt">CO</span> molecules. The addition of a second H<span class="hlt">2</span><span class="hlt">CO</span> to the product of the reaction between CH3OH and H<span class="hlt">2</span><span class="hlt">CO</span> was also considered as an alternative route to longer polyoxymethylene polymers of the -CH<span class="hlt">2</span>O- form. The reaction between HNCO and NH3 was studied to determine if it can compete against the barrierless charge transfer process that yields OCN(-) and NH4(+). Finally, the H<span class="hlt">2</span><span class="hlt">CO</span> + NH3 reaction was revisited with additional benchmark calculations that confirm that little or no barrier is present when it occurs in <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001JGR...10632139N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001JGR...10632139N"><span>Turbulent aerosol <span class="hlt">fluxes</span> over the Arctic Ocean: <span class="hlt">2</span>. Wind-driven sources from the sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nilsson, E. D.; Rannik, Ü.; Swietlicki, E.; Leck, C.; Aalto, P. P.; Zhou, J.; Norman, M.</p> <p>2001-12-01</p> <p>An eddy-covariance <span class="hlt">flux</span> system was successfully applied over open sea, leads and <span class="hlt">ice</span> floes during the Arctic Ocean Expedition in July-August 1996. Wind-driven upward aerosol number <span class="hlt">fluxes</span> were observed over open sea and leads in the pack <span class="hlt">ice</span>. These particles must originate from droplets ejected into the <span class="hlt">air</span> at the bursting of small <span class="hlt">air</span> bubbles at the water surface. The source <span class="hlt">flux</span> F (in 106 m-<span class="hlt">2</span> s-1) had a strong dependency on wind speed, log>(F>)=0.20U¯-1.71 and 0.11U¯-1.93, over the open sea and leads, respectively (where U¯ is the local wind speed at about 10 m height). Over the open sea the wind-driven aerosol source <span class="hlt">flux</span> consisted of a film drop mode centered at ˜100 nm diameter and a jet drop mode centered at ˜1 μm diameter. Over the leads in the pack <span class="hlt">ice</span>, a jet drop mode at ˜<span class="hlt">2</span> μm diameter dominated. The jet drop mode consisted of sea-salt, but oxalate indicated an organic contribution, and bacterias and other biogenic particles were identified by single particle analysis. Particles with diameters less than -100 nm appear to have contributed to the <span class="hlt">flux</span>, but their chemical composition is unknown. Whitecaps were probably the bubble source at open sea and on the leads at high wind speed, but a different bubble source is needed in the leads owing to their small fetch. Melting of <span class="hlt">ice</span> in the leads is probably the best candidate. The <span class="hlt">flux</span> over the open sea was of such a magnitude that it could give a significant contribution to the condensation nuclei (CCN) population. Although the <span class="hlt">flux</span> from the leads were roughly an order of magnitude smaller and the leads cover only a small fraction of the pack <span class="hlt">ice</span>, the local source may till be important for the CCN population in Arctic fogs. The primary marine aerosol source will increase both with increased wind speed and with decreased <span class="hlt">ice</span> fraction and extent. The local CCN production may therefore increase and influence cloud or fog albedo and lifetime in response to greenhouse warming in the Arctic Ocean region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B41E0110R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B41E0110R"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> From Antarctic Dry Valley Soils: Determining the Source and Environmental Controls</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Risk, D. A.; Macintyre, C. M.; Shanhun, F.; Almond, P. C.; Lee, C.; Cary, C.</p> <p>2014-12-01</p> <p>Soils within the McMurdo Dry Valleys are known to respire carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), but considerable debate surrounds the contributing sources and mechanisms that drive temporal variability. While some of the <span class="hlt">CO</span><span class="hlt">2</span> is of biological origin, other known contributors to variability include geochemical sources within, or beneath, the soil column. The relative contribution from each of these sources will depend on seasonal and environmental drivers such as temperature and wind that exert influence on temporal dynamics. To supplement a long term <span class="hlt">CO</span><span class="hlt">2</span>­ surface <span class="hlt">flux</span> monitoring station that has now recorded <span class="hlt">fluxes</span> over three full annual cycles, in January 2014 an automated <span class="hlt">flux</span> and depth concentration monitoring system was installed in the Spaulding Pond area of Taylor Valley, along with standard meteorological sensors, to assist in defining source contributions through time. During two weeks of data we observed marked diel variability in <span class="hlt">CO</span><span class="hlt">2</span> concentrations within the profile (~100 ppm <span class="hlt">CO</span><span class="hlt">2</span> above or below atmospheric), and of <span class="hlt">CO</span><span class="hlt">2</span> moving across the soil surface. The pattern at many depths suggested an alternating diel-scale transition from source to sink that seemed clearly correlated with temperature-driven changes in the solubility of <span class="hlt">CO</span><span class="hlt">2</span> in water films. This <span class="hlt">CO</span><span class="hlt">2</span> solution storage <span class="hlt">flux</span> was very highly coupled to soil temperature. A small depth source of unknown origin also appeared to be present. A controlled laboratory soil experiment was conducted to confirm the magnitude of <span class="hlt">fluxes</span> into and out of soil water films, and confirmed the field results and temperature dependence. Ultimately, this solution storage <span class="hlt">flux</span> needs to be well understood if the small biological <span class="hlt">fluxes</span> from these soils are to be properly quantified and monitored for change. Here, we present results from the 2013/2014 field season and these supplementary experiments, placed in the context of 3 year long term continuous measurement of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> within the Dry Valleys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A41A2248P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A41A2248P"><span>An Improved Extraction and Analysis Technique for Determination of Carbon Monoxide Stable Isotopes and Mixing Ratios from <span class="hlt">Ice</span> Core and Atmospheric <span class="hlt">Air</span> Samples.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Place, P., Jr.; Petrenko, V. V.; Vimont, I.</p> <p>2017-12-01</p> <p>Carbon Monoxide (<span class="hlt">CO</span>) is an important atmospheric trace gas that affects the oxidative capacity of the atmosphere and contributes indirectly to anthropogenic radiative forcing. Carbon monoxide stable isotopes can also serve as a tracer for variations in biomass burning, particularly in the preindustrial atmosphere. A good understanding of the past variations in <span class="hlt">CO</span> mole fractions and isotopic composition can help improve the skill of chemical transport models and constrain biomass burning changes. <span class="hlt">Ice</span> cores may preserve a record of past atmospheric <span class="hlt">CO</span> for analysis and interpretation. To this end, a new extraction system has been developed for analysis of stable isotopes (δ13<span class="hlt">CO</span> and δC18O) of atmospheric carbon monoxide from <span class="hlt">ice</span> core and atmospheric <span class="hlt">air</span> samples. This system has been designed to measure relatively small sample sizes (80 cc STP of <span class="hlt">air</span>) to accommodate the limited availability of <span class="hlt">ice</span> core samples. Trapped <span class="hlt">air</span> is extracted from <span class="hlt">ice</span> core samples via melting in a glass vacuum chamber. This <span class="hlt">air</span> is expanded into a glass expansion loop and then compressed into the sample loop of a Reducing Gas Detector (Peak Laboratories, Peak Performer 1 RCP) for the <span class="hlt">CO</span> mole fraction measurement. The remaining sample gas will be expelled from the melt vessel into a larger expansion loop via headspace compression for isotopic analysis. The headspace compression will be accomplished by introduction of clean degassed water into the bottom of the melt vessel. Isotopic analysis of the sample gas is done utilizing the Schütze Reagent to convert the carbon monoxide to carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) which is then measured using continuous-flow isotope ratio mass spectrometry (Elementar Americas, IsoPrime 100). A series of cryogenic traps are used to purify the sample <span class="hlt">air</span>, capture the converted sample <span class="hlt">CO</span><span class="hlt">2</span>, and cryofocus the sample <span class="hlt">CO</span><span class="hlt">2</span> prior to injection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ESD.....8.1093P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ESD.....8.1093P"><span>The potential of using remote sensing data to estimate <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange in the Baltic Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parard, Gaëlle; Rutgersson, Anna; Parampil, Sindu Raj; Alexandre Charantonis, Anastase</p> <p>2017-12-01</p> <p>In this article, we present the first climatological map of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> over the Baltic Sea based on remote sensing data: estimates of p<span class="hlt">CO</span><span class="hlt">2</span> derived from satellite imaging using self-organizing map classifications along with class-specific linear regressions (SOMLO methodology) and remotely sensed wind estimates. The estimates have a spatial resolution of 4 km both in latitude and longitude and a monthly temporal resolution from 1998 to 2011. The <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are estimated using two types of wind products, i.e. reanalysis winds and satellite wind products, the higher-resolution wind product generally leading to higher-amplitude <span class="hlt">flux</span> estimations. Furthermore, the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were also estimated using two methods: the method of Wanninkhof et al. (2013) and the method of Rutgersson and Smedman (2009). The seasonal variation in <span class="hlt">fluxes</span> reflects the seasonal variation in p<span class="hlt">CO</span><span class="hlt">2</span> unvaryingly over the whole Baltic Sea, with high winter <span class="hlt">CO</span><span class="hlt">2</span> emissions and high p<span class="hlt">CO</span><span class="hlt">2</span> uptakes. All basins act as a source for the atmosphere, with a higher degree of emission in the southern regions (mean source of 1.6 mmol m-<span class="hlt">2</span> d-1 for the South Basin and 0.9 for the Central Basin) than in the northern regions (mean source of 0.1 mmol m-<span class="hlt">2</span> d-1) and the coastal areas act as a larger sink (annual uptake of -4.<span class="hlt">2</span> mmol m-<span class="hlt">2</span> d-1) than does the open sea (-4 mmol m-<span class="hlt">2</span> d-1). In its entirety, the Baltic Sea acts as a small source of 1.<span class="hlt">2</span> mmol m-<span class="hlt">2</span> d-1 on average and this annual uptake has increased from 1998 to 2012.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011epsc.conf..224K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011epsc.conf..224K"><span>On the size dependence of the scattering greenhouse effect of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kitzmann, D.; Patzer, A. B. C.; Rauer, H.</p> <p>2011-10-01</p> <p>In this contribution we study the potential greenhouse effect due to scattering of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds for atmospheric conditions of terrestrial extrasolar planets. Therefore, we calculate the scattering and absorption properties of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles using Mie theory for assumed particle size distributions with different effective radii and particle densities to determine the scattering and absorption characteristics of such clouds. Implications especially in view of a potential greenhouse warming of the planetary surface are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A32F..08C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A32F..08C"><span>Constraining the Stratosphere-Troposphere Exchange of Radiocarbon using <span class="hlt">Air</span>Core 14<span class="hlt">CO</span><span class="hlt">2</span> Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, H.</p> <p>2016-12-01</p> <p>Radiocarbon (14C) plays an important role in the carbon cycle studies to understand both natural and anthropogenic carbon <span class="hlt">fluxes</span>, but also in atmospheric chemistry to constrain hydroxyl radical (OH) concentrations in the atmosphere. Apart from the enormous 14C emissions from nuclear bomb testing in the 1950s and 1960s, radiocarbon is primarily produced in the upper atmosphere due to reactions of nitrogen nuclei with thermal neutrons that are induced by cosmic rays. 14C is quickly oxidized to 14<span class="hlt">CO</span>, which is then further oxidized to 14<span class="hlt">CO</span><span class="hlt">2</span> by OH. To this end, better understanding the radiocarbon source is very useful to advance the use of radiocarbon for these applications. However, upper atmospheric 14C observations have been very sparse to constrain the magnitude and the location of the 14C production as well as the transport of radiocarbon from the stratosphere to the troposphere. Recently we have successfully made stratospheric 14<span class="hlt">CO</span><span class="hlt">2</span> measurements using <span class="hlt">Air</span>Core samples from Sodankylä, Northern Finland, along with regular <span class="hlt">Air</span>Core profiles of <span class="hlt">CO</span><span class="hlt">2</span>, CH4, and <span class="hlt">CO</span> since 2013. In this study, we calculate the stratosphere-troposphere exchange of 14C using the correlation between 14<span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O, and the estimated N<span class="hlt">2</span>O loss rate. Besides this, we assess the impact of the mean age of <span class="hlt">air</span> on 14<span class="hlt">CO</span><span class="hlt">2</span> profiles. Furthermore, we will evaluate the influence of different cosmogenic 14C production scenarios and the uncertainties in the OH field on the seasonal cycles of radiocarbon and on the stratosphere-troposphere exchange.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.7685S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.7685S"><span>Concurrent <span class="hlt">CO</span><span class="hlt">2</span> and COS <span class="hlt">fluxes</span> across major biomes in Europe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spielmann, Felix M.; Kitz, Florian; Hammerle, Albin; Gerdel, Katharina; Ibrom, Andreas; Kolle, Olaf; Migliavacca, Mirco; Moreno, Gerardo; Noe, Steffen M.; Wohlfahrt, Georg</p> <p>2017-04-01</p> <p>The trace gas carbonyl sulfide (COS) has been proposed as a tracer for canopy gross primary production (GPP), canopy transpiration and stomatal conductance of plant canopies in the last few years. COS enters the plant leaf through the stomata and diffuses through the intercellular space, the cell wall, the plasma membrane and the cytosol like carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>). It is then catalyzed by the enzyme carbonic anhydrase in a one-way reaction to hydrogen sulfide and <span class="hlt">CO</span><span class="hlt">2</span>. This one-way <span class="hlt">flux</span> into the leaf makes COS a promising tracer for the GPP. However, this approach assumes that the ratio of the deposition velocities between COS and <span class="hlt">CO</span><span class="hlt">2</span> is constant, which must be determined in field experiments covering a wide variety of ecosystems. The overarching objective of this study was to quantify the relationship between the ecosystem-scale exchange of COS and <span class="hlt">CO</span><span class="hlt">2</span> and thus, to test for the potential of COS to be used as a universal tracer for the plant canopy <span class="hlt">CO</span><span class="hlt">2</span> exchange. Between spring 2015 and summer 2016 we set up our quantum cascade laser at different field sites across Europe. These sites included a managed temperate mountain grassland (AUT), a savanna (ESP), a temperate beech forest (DEN) and a hemiboreal forest (EST). On each of these sites, we conducted ecosystem scale eddy covariance and soil chamber measurements. Since the soil COS <span class="hlt">flux</span> contribution, especially in grass dominated ecosystems, could not be neglected, we had to derive the actual canopy COS <span class="hlt">fluxes</span> for all the measurement sites. Using these <span class="hlt">fluxes</span> we compared the ecosystem relative uptake (ERU) of the sites and searched for factors affecting its variability. We then used the influential factors to scale the ERU to be comparable under different field sites and conditions. Furthermore we also calculated the GPP using conventional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> partitioning and compared the results with the approach of using the leaf relative uptake.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20103140','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20103140"><span><span class="hlt">CO</span><span class="hlt">2</span> volume <span class="hlt">fluxes</span> outgassing from champagne glasses: the impact of champagne ageing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liger-Belair, Gérard; Villaume, Sandra; Cilindre, Clara; Jeandet, Philippe</p> <p>2010-02-15</p> <p>It was demonstrated that <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">fluxes</span> outgassing from a flute poured with a young champagne (elaborated in 2007) are much higher than those outgassing from the same flute poured with an older champagne (elaborated in the early 1990s). The difference in dissolved-<span class="hlt">CO</span>(<span class="hlt">2</span>) concentrations between the two types of champagne samples was found to be a crucial parameter responsible for differences in <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">fluxes</span> outgassing from one champagne to another. Nevertheless, it was shown that, for a given identical dissolved-<span class="hlt">CO</span>(<span class="hlt">2</span>) concentration in both champagne types, the <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">flux</span> outgassing from the flute poured with the old champagne is, in average, significantly lower than that outgassing from the flute poured with the young one. Therefore, <span class="hlt">CO</span>(<span class="hlt">2</span>) seems to "escape" more easily from the young champagne than from the older one. The diffusion coefficient of <span class="hlt">CO</span>(<span class="hlt">2</span>) in both champagne types was pointed as a key parameter to thoroughly determine in the future, in order to unravel our experimental observation. Copyright 2009 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A31O..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A31O..02S"><span>Interpreting OCO-<span class="hlt">2</span> Constrained <span class="hlt">CO</span><span class="hlt">2</span> Surface <span class="hlt">Flux</span> Estimates Through the Lens of Atmospheric Transport Uncertainty.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schuh, A. E.; Jacobson, A. R.; Basu, S.; Weir, B.; Baker, D. F.; Bowman, K. W.; Chevallier, F.; Crowell, S.; Deng, F.; Denning, S.; Feng, L.; Liu, J.</p> <p>2017-12-01</p> <p>The orbiting carbon observatory (OCO-<span class="hlt">2</span>) was launched in July 2014 and has collected three years of column mean <span class="hlt">CO</span><span class="hlt">2</span> (XCO<span class="hlt">2</span>) data. The OCO-<span class="hlt">2</span> model inter-comparison project (MIP) was formed to provide a means of analysis of results from many different atmospheric inversion modeling systems. Certain facets of the inversion systems, such as observations and fossil fuel <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were standardized to remove first order sources of difference between the systems. Nevertheless, large variations amongst the <span class="hlt">flux</span> results from the systems still exist. In this presentation, we explore one dimension of this uncertainty, the impact of different atmospheric transport fields, i.e. wind speeds and directions. Early results illustrate a large systematic difference between two classes of atmospheric transport, arising from winds in the parent GEOS-DAS (NASA-GMAO) and ERA-Interim (ECMWF) data assimilation models. We explore these differences and their effect on inversion-based estimates of surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> by using a combination of simplified inversion techniques as well as the full OCO-<span class="hlt">2</span> MIP suite of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20527160','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20527160"><span>[Characteristics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> before and in the heating period at urban complex underlying surface area].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jia, Qing-yu; Zhou, Guang-sheng; Wang, Yu; Liu, Xiao-mei</p> <p>2010-04-01</p> <p>Urban areas were significant contributors to global carbon dioxide emissions. The eddy covariance (EC) was used to measure carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) concentration and <span class="hlt">flux</span> data at urban area in Shenyang. This research analyzed the characteristics of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration and <span class="hlt">flux</span> in October 2008 to November 2008 period before and in the heating period. The results showed that the daily variation of <span class="hlt">CO</span><span class="hlt">2</span> concentration was two-peak curve. The first peak time appeared as same as sunrise time, while the second peak time impacted by vehicles and heating. The result of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> showed that urban atmospheric <span class="hlt">CO</span><span class="hlt">2</span> was net emissions, vegetation photosynthesis absorbed <span class="hlt">CO</span><span class="hlt">2</span> of traffic, the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> peak appeared at 17:15-18:15 in the heating period, <span class="hlt">CO</span><span class="hlt">2</span> emission increased 29.37 g x (m<span class="hlt">2</span> x d)(-1) in the heating period than that before the heating period; there was corresponding relationship between <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and the time when temperature peak and sensible heating <span class="hlt">flux</span> (Hc) turn positive. The results also indicated that atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration and its <span class="hlt">flux</span> were affected seriously by both wind direction and carbon sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/sir/2009/5061/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/sir/2009/5061/"><span>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> in the Amargosa Desert, Nevada, during El Nino 1998 and La Nina 1999</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Riggs, Alan C.; Stannard, David I.; Maestas, Florentino B.; Karlinger, Michael R.; Striegl, Robert G.</p> <p>2009-01-01</p> <p>Mean annual soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from normally bare mineral soil in the Amargosa Desert in southern Nevada, United States, measured with clear and opaque soil <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">flux</span> chambers (autochambers) were small - <5 millimoles per square meter per day - during both El Nino 1998 and La Nina 1999. The 1998 opaque-chamber <span class="hlt">flux</span> exceeded 1999 opaque-chamber <span class="hlt">flux</span> by an order of magnitude, whereas the 1998 clear-chamber <span class="hlt">flux</span> exceeded 1999 clear-chamber <span class="hlt">flux</span> by less than a factor of two. These data suggest that above-normal soil moisture stimulated increased metabolic activity, but that much of the extra <span class="hlt">CO</span><span class="hlt">2</span> produced was recaptured by plants. <span class="hlt">Fluxes</span> from warm moist soil were the largest sustained <span class="hlt">fluxes</span> measured, and their hourly pattern is consistent with enhanced soil metabolic activity at some depth in the soil and photosynthetic uptake of a substantial portion of the <span class="hlt">CO</span><span class="hlt">2</span> released. <span class="hlt">Flux</span> from cool moist soil was smaller than <span class="hlt">flux</span> from warm moist soil. <span class="hlt">Flux</span> from hot dry soil was intermediate between warm-moist and cool-moist <span class="hlt">fluxes</span>, and clear-chamber <span class="hlt">flux</span> was more than double the opaque-chamber <span class="hlt">flux</span>, apparently due to a chamber artifact stemming from a thermally controlled <span class="hlt">CO</span><span class="hlt">2</span> reservoir near the soil surface. There was no demonstrable metabolic contribution to the very small <span class="hlt">flux</span> from cool dry soil, which was dominated by diffusive up-<span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> from the water table and temperature-controlled <span class="hlt">CO</span><span class="hlt">2</span>-reservoir up- and down-<span class="hlt">fluxes</span>. These <span class="hlt">flux</span> patterns suggest that transfer of <span class="hlt">CO</span><span class="hlt">2</span> across the land surface is a complex process that is difficult to accurately measure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22445955','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22445955"><span>Responses of CH(4), <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O <span class="hlt">fluxes</span> to increasing nitrogen deposition in alpine grassland of the Tianshan Mountains.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Kaihui; Gong, Yanming; Song, Wei; He, Guixiang; Hu, Yukun; Tian, Changyan; Liu, Xuejun</p> <p>2012-06-01</p> <p>To assess the effects of nitrogen (N) deposition on greenhouse gas (GHG) <span class="hlt">fluxes</span> in alpine grassland of the Tianshan Mountains in central Asia, CH(4), <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O <span class="hlt">fluxes</span> were measured from June 2010 to May 2011. Nitrogen deposition tended to significantly increase CH(4) uptake, <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O emissions at sites receiving N addition compared with those at site without N addition during the growing season, but no significant differences were found for all sites outside the growing season. <span class="hlt">Air</span> temperature, soil temperature and water content were the important factors that influence <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O emissions at year-round scale, indicating that increased temperature and precipitation in the future will exert greater impacts on <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O emissions in the alpine grassland. In addition, plant coverage in July was also positively correlated with <span class="hlt">CO</span>(<span class="hlt">2</span>) and N(<span class="hlt">2</span>)O emissions under elevated N deposition rates. The present study will deepen our understanding of N deposition impacts on GHG balance in the alpine grassland ecosystem, and help us assess the global N effects, parameterize Earth System models and inform decision makers. Copyright © 2012 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.2333B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.2333B"><span>On the importance of high-frequency <span class="hlt">air</span>-temperature fluctuations for spectroscopic corrections of open-path carbon dioxide <span class="hlt">flux</span> measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bogoev, Ivan; Helbig, Manuel; Sonnentag, Oliver</p> <p>2015-04-01</p> <p>A growing number of studies report systematic differences in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates obtained with the two main types of gas analyzers: compared to eddy-covariance systems based on closed-path (CP) gas analyzers, systems with open-path (OP) gas analyzers systematically overestimate <span class="hlt">CO</span><span class="hlt">2</span> uptake during daytime periods with high positive sensible heat <span class="hlt">fluxes</span>, while patterns for differences in nighttime <span class="hlt">CO</span><span class="hlt">2</span> exchange are less obvious. These biases have been shown to correlate with the sign and the magnitude of the sensible heat <span class="hlt">flux</span> and to introduce large uncertainties when calculating annual <span class="hlt">CO</span><span class="hlt">2</span> budgets. In general, CP and OP gas analyzers commonly used to measure the <span class="hlt">CO</span><span class="hlt">2</span> density in the atmosphere operate on the principle of infrared light absorption approximated by Beer-Lambert's law. Non-dispersive interference-based optical filter elements are used to select spectral bands with strong attenuation of light transmission, characteristic to the gas of interest. The intensity of the light passing through the optical sensing path depends primarily on the amount of absorber gas in the measurement volume. Besides the density of the gas, barometric pressure and <span class="hlt">air</span> temperature are additional factors affecting the strength and the half-width of the absorption lines. These so-called spectroscopic effects are accounted for by measuring barometric pressure and <span class="hlt">air</span> temperature in the sensing path and scaling the light-intensity measurements before applying the calibration equation. This approach works well for CP gas analyzers with an intake tube that acts as a low-pass filter on fast <span class="hlt">air</span>-temperature fluctuations. Low-frequency response temperature sensors in the measurement cell are therefore sufficient to account for spectroscopic temperature effects. In contrast, OP gas analyzers are exposed to high-frequency <span class="hlt">air</span>-temperature fluctuations associated with the atmospheric surface-layer turbulent heat exchange. If not corrected adequately, these fast <span class="hlt">air</span>-temperature variations can cause</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRD..11711303N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRD..11711303N"><span>Imposing strong constraints on tropical terrestrial <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using passenger aircraft based measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Niwa, Yosuke; Machida, Toshinobu; Sawa, Yousuke; Matsueda, Hidekazu; Schuck, Tanja J.; Brenninkmeijer, Carl A. M.; Imasu, Ryoichi; Satoh, Masaki</p> <p>2012-06-01</p> <p>Because very few measurements of atmospheric carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) are available in the tropics, estimates of surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in tropical regions are beset with considerable uncertainties. To improve estimates of tropical terrestrial <span class="hlt">fluxes</span>, atmospheric <span class="hlt">CO</span><span class="hlt">2</span> inversion was performed using passenger aircraft based measurements of the Comprehensive Observation Network for Trace gases by Airliner (CONTRAIL) project in addition to the surface measurement data set of GLOBALVIEW-<span class="hlt">CO</span><span class="hlt">2</span>. Regional monthly <span class="hlt">fluxes</span> at the earth's surface were estimated using the Bayesian synthesis approach focusing on the period 2006-2008 using the Nonhydrostatic Icosahedral Atmospheric Model-based Transport Model (NICAM-TM). By adding the aircraft to the surface data, the posterior <span class="hlt">flux</span> errors were greatly reduced; specifically, error reductions of up to 64% were found for tropical Asia regions. This strong impact is closely related to efficient vertical transport in the tropics. The optimized surface <span class="hlt">fluxes</span> using the CONTRAIL data were evaluated by comparing the simulated atmospheric <span class="hlt">CO</span><span class="hlt">2</span> distributions with independent aircraft measurements of the Civil Aircraft for the Regular Investigation of the atmosphere Based on an Instrument Container (CARIBIC) project. The inversion with the CONTRAIL data yields the global carbon sequestration rates of <span class="hlt">2</span>.22 ± 0.28 Pg C yr-1 for the terrestrial biosphere and <span class="hlt">2</span>.24 ± 0.27 Pg C yr-1 for the oceans (the both are adjusted by riverine input of <span class="hlt">CO</span><span class="hlt">2</span>). For the first time the CONTRAIL <span class="hlt">CO</span><span class="hlt">2</span> measurements were used in an inversion system to identify the areas of greatest impact in terms of reducing <span class="hlt">flux</span> uncertainties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C52A..01N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C52A..01N"><span>Error estimates for <span class="hlt">ice</span> discharge calculated using the <span class="hlt">flux</span> gate approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Navarro, F. J.; Sánchez Gámez, P.</p> <p>2017-12-01</p> <p><span class="hlt">Ice</span> discharge to the ocean is usually estimated using the <span class="hlt">flux</span> gate approach, in which <span class="hlt">ice</span> <span class="hlt">flux</span> is calculated through predefined <span class="hlt">flux</span> gates close to the marine glacier front. However, published results usually lack a proper error estimate. In the <span class="hlt">flux</span> calculation, both errors in cross-sectional area and errors in velocity are relevant. While for estimating the errors in velocity there are well-established procedures, the calculation of the error in the cross-sectional area requires the availability of ground penetrating radar (GPR) profiles transverse to the <span class="hlt">ice</span>-flow direction. In this contribution, we use <span class="hlt">Ice</span>Bridge operation GPR profiles collected in Ellesmere and Devon Islands, Nunavut, Canada, to compare the cross-sectional areas estimated using various approaches with the cross-sections estimated from GPR <span class="hlt">ice</span>-thickness data. These error estimates are combined with those for <span class="hlt">ice</span>-velocities calculated from Sentinel-1 SAR data, to get the error in <span class="hlt">ice</span> discharge. Our preliminary results suggest, regarding area, that the parabolic cross-section approaches perform better than the quartic ones, which tend to overestimate the cross-sectional area for flight lines close to the central flowline. Furthermore, the results show that regional <span class="hlt">ice</span>-discharge estimates made using parabolic approaches provide reasonable results, but estimates for individual glaciers can have large errors, up to 20% in cross-sectional area.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6688K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6688K"><span>Comparison of Source Partitioning Methods for <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">Fluxes</span> Based on High Frequency Eddy Covariance Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klosterhalfen, Anne; Moene, Arnold; Schmidt, Marius; Ney, Patrizia; Graf, Alexander</p> <p>2017-04-01</p> <p>Source partitioning of eddy covariance (EC) measurements of <span class="hlt">CO</span><span class="hlt">2</span> into respiration and photosynthesis is routinely used for a better understanding of the exchange of greenhouse gases, especially between terrestrial ecosystems and the atmosphere. The most frequently used methods are usually based either on relations of <span class="hlt">fluxes</span> to environmental drivers or on chamber measurements. However, they often depend strongly on assumptions or invasive measurements and do usually not offer partitioning estimates for latent heat <span class="hlt">fluxes</span> into evaporation and transpiration. SCANLON and SAHU (2008) and SCANLON and KUSTAS (2010) proposed an promising method to estimate the contributions of transpiration and evaporation using measured high frequency time series of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">fluxes</span> - no extra instrumentation necessary. This method (SK10 in the following) is based on the spatial separation and relative strength of sources and sinks of <span class="hlt">CO</span><span class="hlt">2</span> and water vapor among the sub-canopy and canopy. Assuming that <span class="hlt">air</span> from those sources and sinks is not yet perfectly mixed before reaching EC sensors, partitioning is estimated based on the separate application of the <span class="hlt">flux</span>-variance similarity theory to the stomatal and non-stomatal components of the regarded <span class="hlt">fluxes</span>, as well as on additional assumptions on stomatal water use efficiency (WUE). The <span class="hlt">CO</span><span class="hlt">2</span> partitioning method after THOMAS et al. (2008) (TH08 in the following) also follows the argument that the dissimilarities of sources and sinks in and below a canopy affect the relation between H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> fluctuations. Instead of involving assumptions on WUE, TH08 directly screens their scattergram for signals of joint respiration and evaporation events and applies a conditional sampling methodology. In spite of their different main targets (H<span class="hlt">2</span>O vs. <span class="hlt">CO</span><span class="hlt">2</span>), both methods can yield partitioning estimates on both <span class="hlt">fluxes</span>. We therefore compare various sub-methods of SK10 and TH08 including own modifications (e.g., cluster analysis) to each other, to established</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.476...11T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.476...11T"><span><span class="hlt">CO</span><span class="hlt">2</span> condensation is a serious limit to the deglaciation of Earth-like planets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Turbet, Martin; Forget, Francois; Leconte, Jeremy; Charnay, Benjamin; Tobie, Gabriel</p> <p>2017-10-01</p> <p>It is widely believed that the carbonate-silicate cycle is the main agent, through volcanism, to trigger deglaciations by <span class="hlt">CO</span><span class="hlt">2</span> greenhouse warming on Earth and on Earth-like planets when they get in a frozen state. Here we use a 3D Global Climate Model to simulate the ability of planets initially completely frozen to escape from glaciation episodes by accumulating enough gaseous <span class="hlt">CO</span><span class="hlt">2</span>. The model includes <span class="hlt">CO</span><span class="hlt">2</span> condensation and sublimation processes and the water cycle. We find that planets with Earth-like characteristics (size, mass, obliquity, rotation rate, etc.) orbiting a Sun-like star may never be able to escape from a glaciation era, if their orbital distance is greater than ∼1.27 Astronomical Units (<span class="hlt">Flux</span> < 847 Wm-<span class="hlt">2</span> or 62% of the Solar constant), because <span class="hlt">CO</span><span class="hlt">2</span> would condense at the poles - here the cold traps - forming permanent <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> caps. This limits the amount of <span class="hlt">CO</span><span class="hlt">2</span> in the atmosphere and thus its greenhouse effect. Furthermore, our results indicate that for (1) high rotation rates (Prot < 24 h), (<span class="hlt">2</span>) low obliquity (obliquity <23.5°), (3) low background gas partial pressures (<1 bar), and (4) high water <span class="hlt">ice</span> albedo (H<span class="hlt">2</span>O albedo > 0.6), this critical limit could occur at a significantly lower equivalent distance (or higher insolation). For each possible configuration, we show that the amount of <span class="hlt">CO</span><span class="hlt">2</span> that can be trapped in the polar caps depends on the efficiency of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> to flow laterally as well as its gravitational stability relative to subsurface water <span class="hlt">ice</span>. We find that a frozen Earth-like planet located at 1.30 AU of a Sun-like star could store as much as 1.5, 4.5 and 15 bars of dry <span class="hlt">ice</span> at the poles, for internal heat <span class="hlt">fluxes</span> of 100, 30 and 10 mW m-<span class="hlt">2</span>, respectively. But these amounts are in fact lower limits. For planets with a significant water <span class="hlt">ice</span> cover, we show that <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> deposits should be gravitationally unstable. They get buried beneath the water <span class="hlt">ice</span> cover in geologically short timescales of ∼104 yrs, mainly controlled by the viscosity of water <span class="hlt">ice</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1355135-how-can-mountaintop-co2-observations-used-constrain-regional-carbon-fluxes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1355135-how-can-mountaintop-co2-observations-used-constrain-regional-carbon-fluxes"><span>How can mountaintop <span class="hlt">CO</span> <span class="hlt">2</span> observations be used to constrain regional carbon <span class="hlt">fluxes</span>?</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lin, John C.; Mallia, Derek V.; Wu, Dien; ...</p> <p>2017-05-03</p> <p>Despite the need for researchers to understand terrestrial biospheric carbon <span class="hlt">fluxes</span> to account for carbon cycle feedbacks and predict future <span class="hlt">CO</span> <span class="hlt">2</span> concentrations, knowledge of these <span class="hlt">fluxes</span> at the regional scale remains poor. This is particularly true in mountainous areas, where complex meteorology and lack of observations lead to large uncertainties in carbon <span class="hlt">fluxes</span>. Yet mountainous regions are often where significant forest cover and biomass are found – i.e., areas that have the potential to serve as carbon sinks. As <span class="hlt">CO</span> <span class="hlt">2</span> observations are carried out in mountainous areas, it is imperative that they are properly interpreted to yield informationmore » about carbon <span class="hlt">fluxes</span>. In this paper, we present <span class="hlt">CO</span> <span class="hlt">2</span> observations at three sites in the mountains of the western US, along with atmospheric simulations that attempt to extract information about biospheric carbon <span class="hlt">fluxes</span> from the <span class="hlt">CO</span> <span class="hlt">2</span> observations, with emphasis on the observed and simulated diurnal cycles of <span class="hlt">CO</span> <span class="hlt">2</span>. We show that atmospheric models can systematically simulate the wrong diurnal cycle and significantly misinterpret the <span class="hlt">CO</span> <span class="hlt">2</span> observations, due to erroneous atmospheric flows as a result of terrain that is misrepresented in the model. This problem depends on the selected vertical level in the model and is exacerbated as the spatial resolution is degraded, and our results indicate that a fine grid spacing of ~4 km or less may be needed to simulate a realistic diurnal cycle of <span class="hlt">CO</span> <span class="hlt">2</span> for sites on top of the steep mountains examined here in the American Rockies. In conclusion, in the absence of higher resolution models, we recommend coarse-scale models to focus on assimilating afternoon <span class="hlt">CO</span> <span class="hlt">2</span> observations on mountaintop sites over the continent to avoid misrepresentations of nocturnal transport and influence.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.5561L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.5561L"><span>How can mountaintop <span class="hlt">CO</span><span class="hlt">2</span> observations be used to constrain regional carbon <span class="hlt">fluxes</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, John C.; Mallia, Derek V.; Wu, Dien; Stephens, Britton B.</p> <p>2017-05-01</p> <p>Despite the need for researchers to understand terrestrial biospheric carbon <span class="hlt">fluxes</span> to account for carbon cycle feedbacks and predict future <span class="hlt">CO</span><span class="hlt">2</span> concentrations, knowledge of these <span class="hlt">fluxes</span> at the regional scale remains poor. This is particularly true in mountainous areas, where complex meteorology and lack of observations lead to large uncertainties in carbon <span class="hlt">fluxes</span>. Yet mountainous regions are often where significant forest cover and biomass are found - i.e., areas that have the potential to serve as carbon sinks. As <span class="hlt">CO</span><span class="hlt">2</span> observations are carried out in mountainous areas, it is imperative that they are properly interpreted to yield information about carbon <span class="hlt">fluxes</span>. In this paper, we present <span class="hlt">CO</span><span class="hlt">2</span> observations at three sites in the mountains of the western US, along with atmospheric simulations that attempt to extract information about biospheric carbon <span class="hlt">fluxes</span> from the <span class="hlt">CO</span><span class="hlt">2</span> observations, with emphasis on the observed and simulated diurnal cycles of <span class="hlt">CO</span><span class="hlt">2</span>. We show that atmospheric models can systematically simulate the wrong diurnal cycle and significantly misinterpret the <span class="hlt">CO</span><span class="hlt">2</span> observations, due to erroneous atmospheric flows as a result of terrain that is misrepresented in the model. This problem depends on the selected vertical level in the model and is exacerbated as the spatial resolution is degraded, and our results indicate that a fine grid spacing of ˜ 4 km or less may be needed to simulate a realistic diurnal cycle of <span class="hlt">CO</span><span class="hlt">2</span> for sites on top of the steep mountains examined here in the American Rockies. In the absence of higher resolution models, we recommend coarse-scale models to focus on assimilating afternoon <span class="hlt">CO</span><span class="hlt">2</span> observations on mountaintop sites over the continent to avoid misrepresentations of nocturnal transport and influence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/5413','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/5413"><span>Forest Floor <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> From Two Contrasting Ecosystems in the Southern Appalachians</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>James M. Vose; Barton D. Clinton; Verl Emrick</p> <p>1995-01-01</p> <p>We measured forest floor <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in two contrasting ecosystems (white pine plantation and northern hardwood ecosystems at low and high elevations, respectively) in May and September 1993 to quantify differences and determine factors regulating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. An automated IRGA based, flow through system was used with chambers...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6085685-co-sub-fluxes-tropical-atlantic-during-focal-cruises','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6085685-co-sub-fluxes-tropical-atlantic-during-focal-cruises"><span><span class="hlt">CO</span>/sub <span class="hlt">2</span>/ <span class="hlt">fluxes</span> in the tropical Atlantic during FOCAL cruises</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Andrie, C.; Oudot, C.; Genthon, C.</p> <p>1986-10-15</p> <p><span class="hlt">CO</span>/sub <span class="hlt">2</span>/ partial pressures in the atmosphere and in surface seawater have been measured in the equatorial Atlantic Ocean during Programme Francais Ocean-Climat en Atlantique Equatorial cruises extending from July 1982 to August 1984 along the 4/degree/W, 22/degree/W, and 35/degree/W meridians. Gas transfer coefficients based on recently reported field data combined with information deduced from wind tunnel experiments are used to compute the <span class="hlt">CO</span>/sub <span class="hlt">2</span>/ <span class="hlt">fluxes</span>. The global mean net <span class="hlt">flux</span> between 5/degree/N and 5/degree/S is equal to 1.05 mmol m/sup /minus/<span class="hlt">2</span>/ d/sup /minus/1/ and is from the ocean to the atmosphere. The escape of <span class="hlt">CO</span>/sub <span class="hlt">2</span>/ increases strongly frommore » the east to the west and is always lower in the north than in the south. The importance of wind speed, p<span class="hlt">CO</span>/sub <span class="hlt">2</span>/ in atmosphere, PCO/sub <span class="hlt">2</span>/ in surface seawater, and temperature on the <span class="hlt">flux</span> variability is discussed. The relative influence of the equatorial upwelling on one hand and of the advection and warming of surface waters on the other hand is studied in order to explain high partial pressure in seawater. 59 refs., 15 figs., 5 tabs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15..856N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15..856N"><span>Human Effects and Soil Surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Tropical Urban Green Areas, Singapore</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ng, Bernard; Gandois, Laure; Kai, Fuu Ming; Chua, Amy; Cobb, Alex; Harvey, Charles; Hutyra, Lucy</p> <p>2013-04-01</p> <p>Urban green spaces are appreciated for their amenity value, with increasing interest in the ecosystem services they could provide (e.g. climate amelioration and increasingly as possible sites for carbon sequestration). In Singapore, turfgrass occupies approximately 20% of the total land area and is readily found on both planned and residual spaces. This project aims at understanding carbon <span class="hlt">fluxes</span> in tropical urban green areas, including controls of soil environmental factors and the effect of urban management techniques. Given the large pool of potentially labile carbon, management regimes are recognised to have an influence on soil environmental factors (temperature and moisture), this would affect soil respiration and feedbacks to the greenhouse effect. A modified closed dynamic chamber method was employed to measure total soil respiration <span class="hlt">fluxes</span>. In addition to soil respiration rates, environmental factors such as soil moisture and temperature, and ambient <span class="hlt">air</span> temperature were monitored for the site in an attempt to evaluate their control on the observed <span class="hlt">fluxes</span>. Measurements of soil-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> exchanges are reported for four experimental plots within the Singtel-Kranji Radio Transmission Station (103o43'49E, 1o25'53N), an area dominated by Axonopus compressus. Different treatments such as the removal of turf, and application of clippings were effected as a means to determine the <span class="hlt">fluxes</span> from the various components (respiration of soil and turf, and decomposition of clippings), and to explore the effects of human intervention on observed effluxes. The soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> observed during the daylight hours ranges from <span class="hlt">2</span>.835 + 0.772 umol m-<span class="hlt">2</span> s-1 for the bare plot as compared to 6.654 + 1.134 umol m-<span class="hlt">2</span> s-1 for the turfed plot; this could be attributed to both autotrophic and heterotrophic respiration. Strong controls of both soil temperature and soil moisture are observed on measured soil <span class="hlt">fluxes</span>. On the base soils, <span class="hlt">fluxes</span> were positively correlated to soil</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.A51C0127L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.A51C0127L"><span>Modeling Global Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> and Transport Using NASA MERRA Reanalysis Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Y.; Kawa, S. R.; Collatz, G. J.</p> <p>2010-12-01</p> <p>We present our first results of <span class="hlt">CO</span><span class="hlt">2</span> surface biosphere <span class="hlt">fluxes</span> and global atmospheric <span class="hlt">CO</span><span class="hlt">2</span> transport using NASA’s new MERRA reanalysis data. MERRA is the Modern Era Retrospective-Analysis For Research And Applications based on the Goddard Global Modeling and Assimilation Office GEOS-5 data assimilation system. After some application testing and analysis, we have generated biospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at 3-hourly temporal resolution from an updated version of the CASA carbon cycle model using the 1x1.25-degree reanalysis data. The experiment covers a period of 9 years from 2000 -2008. The affects of US midwest crop (largely corn and soy) carbon uptake and removal by harvest are explicitly included in this version of CASA. Across the agricultural regions of the Midwest US, USDA crop yield data are used to scale vegetation <span class="hlt">fluxes</span> producing a strong sink in the growing season and a comparatively weaker source from respiration after harvest. Comparisons of the new <span class="hlt">fluxes</span> to previous ones generated using GEOS-4 data are provided. The Parameterized Chemistry/Transport Model (PCTM) is then used with the analyzed meteorology in offline <span class="hlt">CO</span><span class="hlt">2</span> transport. In the simulation of <span class="hlt">CO</span><span class="hlt">2</span> transport, we have a higher vertical resolution from MERRA (the lowest 56 of 72 levels are used in our simulation). A preliminary analysis of the <span class="hlt">CO</span><span class="hlt">2</span> simulation results is carried out, including diurnal, seasonal and latitudinal variability. We make comparisons of our simulation to continuous <span class="hlt">CO</span><span class="hlt">2</span> analyzer sites, especially those in agricultural regions. The results show that the model captures reasonably well the observed synoptic variability due to transport changes and biospheric <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....16.5665B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....16.5665B"><span>Separation of biospheric and fossil fuel <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> by atmospheric inversion of <span class="hlt">CO</span><span class="hlt">2</span> and 14<span class="hlt">CO</span><span class="hlt">2</span> measurements: Observation System Simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Basu, Sourish; Bharat Miller, John; Lehman, Scott</p> <p>2016-05-01</p> <p>National annual total <span class="hlt">CO</span><span class="hlt">2</span> emissions from combustion of fossil fuels are likely known to within 5-10 % for most developed countries. However, uncertainties are inevitably larger (by unknown amounts) for emission estimates at regional and monthly scales, or for developing countries. Given recent international efforts to establish emission reduction targets, independent determination and verification of regional and national scale fossil fuel <span class="hlt">CO</span><span class="hlt">2</span> emissions are likely to become increasingly important. Here, we take advantage of the fact that precise measurements of 14C in <span class="hlt">CO</span><span class="hlt">2</span> provide a largely unbiased tracer for recently added fossil-fuel-derived <span class="hlt">CO</span><span class="hlt">2</span> in the atmosphere and present an atmospheric inversion technique to jointly assimilate observations of <span class="hlt">CO</span><span class="hlt">2</span> and 14<span class="hlt">CO</span><span class="hlt">2</span> in order to simultaneously estimate fossil fuel emissions and biospheric exchange <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>. Using this method in a set of Observation System Simulation Experiments (OSSEs), we show that given the coverage of 14<span class="hlt">CO</span><span class="hlt">2</span> measurements available in 2010 (969 over North America, 1063 globally), we can recover the US national total fossil fuel emission to better than 1 % for the year and to within 5 % for most months. Increasing the number of 14<span class="hlt">CO</span><span class="hlt">2</span> observations to ˜ 5000 per year over North America, as recently recommended by the National Academy of Science (NAS) (Pacala et al., 2010), we recover monthly emissions to within 5 % for all months for the US as a whole and also for smaller, highly emissive regions over which the specified data coverage is relatively dense, such as for the New England states or the NY-NJ-PA tri-state area. This result suggests that, given continued improvement in state-of-the art transport models, a measurement program similar in scale to that recommended by the NAS can provide for independent verification of bottom-up inventories of fossil fuel <span class="hlt">CO</span><span class="hlt">2</span> at the regional and national scale. In addition, we show that the dual tracer inversion framework can detect and minimize biases in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CSR...156....1G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CSR...156....1G"><span>Spatial and temporal variability of seawater p<span class="hlt">CO</span><span class="hlt">2</span> within the Canadian Arctic Archipelago and Baffin Bay during the summer and autumn 2011</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Geilfus, N.-X.; Pind, M. L.; Else, B. G. T.; Galley, R. J.; Miller, L. A.; Thomas, H.; Gosselin, M.; Rysgaard, S.; Wang, F.; Papakyriakou, T. N.</p> <p>2018-03-01</p> <p>The partial pressure of <span class="hlt">CO</span><span class="hlt">2</span> in surface water (p<span class="hlt">CO</span><span class="hlt">2</span>sw) measured within the Canadian Arctic Archipelago (CAA) and Baffin Bay was highly variable with values ranging from strongly undersaturated (118 μatm) to slightly supersaturated (419 μatm) with respect to the atmospheric levels ( 386 μatm) during summer and autumn 2011. During summer, melting sea <span class="hlt">ice</span> contributed to cold and fresh surface water and enhanced the <span class="hlt">ice</span>-edge bloom, resulting in strong p<span class="hlt">CO</span><span class="hlt">2</span>sw undersaturation. Coronation Gulf was the only area with supersaturated p<span class="hlt">CO</span><span class="hlt">2</span>sw, likely due to warm <span class="hlt">CO</span><span class="hlt">2</span>-enriched freshwater input from the Coppermine River. During autumn, the entire CAA (including Coronation Gulf) was undersaturated, despite generally increasing p<span class="hlt">CO</span><span class="hlt">2</span>sw. Coronation Gulf was the one place where p<span class="hlt">CO</span><span class="hlt">2</span>sw decreased, likely due to seasonal reduction in discharge from the Coppermine River and the decreasing sea surface temperature. The seasonal summer-to-autumn increase in p<span class="hlt">CO</span><span class="hlt">2</span>sw across the archipelago is attributed in part to the continuous uptake of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> through both summer and autumn and to the seasonal deepening of the surface mixed layer, bringing <span class="hlt">CO</span><span class="hlt">2</span>-rich waters to the surface. These observations demonstrate how freshwater from sea <span class="hlt">ice</span> melt and rivers affect p<span class="hlt">CO</span><span class="hlt">2</span>sw differently. The general p<span class="hlt">CO</span><span class="hlt">2</span>sw undersaturation during summer-autumn 2011 throughout the CAA and Baffin Bay give an estimated net oceanic sink for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> over the study period of 11.4 mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> d-1, assuming no sea-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> exchange across the sea-<span class="hlt">ice</span> covered areas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...13.7267V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...13.7267V"><span>The role of vegetation in the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from a tropical urban neighbourhood</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Velasco, E.; Roth, M.; Tan, S. H.; Quak, M.; Nabarro, S. D. A.; Norford, L.</p> <p>2013-03-01</p> <p>Urban surfaces are usually net sources of <span class="hlt">CO</span><span class="hlt">2</span>. Vegetation can potentially have an important role in reducing the <span class="hlt">CO</span><span class="hlt">2</span> emitted by anthropogenic activities in cities, particularly when vegetation is extensive and/or evergreen. Negative daytime <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, for example have been observed during the growing season at suburban sites characterized by abundant vegetation and low population density. A direct and accurate estimation of carbon uptake by urban vegetation is difficult due to the particular characteristics of the urban ecosystem and high variability in tree distribution and species. Here, we investigate the role of urban vegetation in the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from a residential neighbourhood in Singapore using two different approaches. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> measured directly by eddy covariance are compared with emissions estimated from emissions factors and activity data. The latter includes contributions from vehicular traffic, household combustion, soil respiration and human breathing. The difference between estimated emissions and measured <span class="hlt">fluxes</span> should approximate the biogenic <span class="hlt">flux</span>. In addition, a tree survey was conducted to estimate the annual <span class="hlt">CO</span><span class="hlt">2</span> sequestration using allometric equations and an alternative model of the metabolic theory of ecology for tropical forests. Palm trees, banana plants and turfgrass were also included in the survey with their annual <span class="hlt">CO</span><span class="hlt">2</span> uptake obtained from published growth rates. Both approaches agree within <span class="hlt">2</span>% and suggest that vegetation captures 8% of the total emitted <span class="hlt">CO</span><span class="hlt">2</span> in the residential neighbourhood studied. A net uptake of 1.4 ton km-<span class="hlt">2</span> day-1 (510 ton km-<span class="hlt">2</span> yr-1 ) was estimated from the difference between the daily <span class="hlt">CO</span><span class="hlt">2</span> uptake by photosynthesis (3.95 ton km-<span class="hlt">2</span> ) and release by respiration (<span class="hlt">2</span>.55 ton km-<span class="hlt">2</span>). The study shows the importance of urban vegetation at the local scale for climate change mitigation in the tropics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918160M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918160M"><span>Application of a two-dimensional hydrodynamic model for calculating the <span class="hlt">CO</span>_{<span class="hlt">2</span>} and H_{<span class="hlt">2</span>}O <span class="hlt">fluxes</span> over complex terrain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukhartova, Yulia; Krupenko, Alexandr; Levashova, Natalia; Olchev, Alexandr</p> <p>2017-04-01</p> <p>Within the framework of the study a two dimensional hydrodynamic model of turbulent transfer of greenhouse gases was developed and applied for calculating the <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O turbulent <span class="hlt">fluxes</span> within the atmospheric surface layer over the heterogeneous land surface with mosaic vegetation and complex topography. The vegetation cover in the model is represented as the two-phase medium containing the elements of vegetation and the <span class="hlt">air</span>. The model is based on solving the system of averaged Navier-Stokes and continuity equations for the wind velocity components (⃗V = {V1,V<span class="hlt">2</span>}), using the 1.5-order closure scheme (Wilcox 1998, Wyngaard 2010). The system of the main equations includes also the diffusion and advection equations for turbulent transfer of sensible heat, <span class="hlt">CO</span><span class="hlt">2</span> concentration (Cs) and specific humidity (q) at soil - vegetation -atmosphere interface (Sogachev, Panferov 2006, Mukhartova et al. 2015, Mamkin et al. 2016): ( ) { ( )} ∂Vi+ ⃗V,∇ V = -1ṡ-∂-δP -∂- <span class="hlt">2</span>δ ¯e- K ṡ ∂Vi-+ ∂Vj- +gṡδTv+F , i,j = 1,<span class="hlt">2</span>, ∂t i ρ0 ∂xi ∂xj 3 ij ∂xj ∂xi T0 i div⃗V = 0, ∂T ( ) Tv γa ∂T 1 ( ) H ∂t-+ ⃗V ,∇ T+ γaṡT-ṡV<span class="hlt">2</span> = div (KT ṡ∇T )+ T-ṡKT ṡ∂x-+ρ-c- ⃗V,∇ δP -ρ-c-, 0 0 <span class="hlt">2</span> 0 p 0 p ∂Cs- (⃗ ) ∂q- (⃗ ) E- ∂t + V ,∇ Cs = div(KC ṡ∇Cs )+FC, ∂t+ V ,∇ q = div(Kv ṡ∇q )+ ρ , where x1,x<span class="hlt">2</span> - horizontal and vertical coordinates respectively, ρ0 - the density of dry <span class="hlt">air</span>, δP - the deviation of mean <span class="hlt">air</span> pressure from the hydrostatic distribution, ¯e - the turbulent kinetic energy, T - the temperature of the <span class="hlt">air</span>, δTv = T ṡ(1+ 0.61q) -T0 - the deviation of virtual temperature from the adiabatic temperature T0(x<span class="hlt">2</span>) for dry <span class="hlt">air</span>, Fi - the components of the viscous drag forces induced by the presence of vegetation, K,KT,KC,Kv - turbulent exchange coefficients for momentum, sensible heat, <span class="hlt">CO</span><span class="hlt">2</span>and H<span class="hlt">2</span>O respectively, γa = g/ cp, cp - the specific heat of the <span class="hlt">air</span> at constant atmospheric pressure, FC - the sources/sinks of <span class="hlt">CO</span><span class="hlt">2</span>in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APJAS..49..443P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APJAS..49..443P"><span>Heat <span class="hlt">flux</span> variations over sea <span class="hlt">ice</span> observed at the coastal area of the Sejong Station, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, Sang-Jong; Choi, Tae-Jin; Kim, Seong-Joong</p> <p>2013-08-01</p> <p>This study presents variations of sensible heat <span class="hlt">flux</span> and latent heat <span class="hlt">flux</span> over sea <span class="hlt">ice</span> observed in 2011 from the 10-m <span class="hlt">flux</span> tower located at the coast of the Sejong Station on King George Island, Antarctica. A period from July to September was selected as a sea <span class="hlt">ice</span> period based on daily record of sea state and hourly photos looking at the Marian Cove in front of the Sejong Station. For the sea <span class="hlt">ice</span> period, mean sensible heat <span class="hlt">flux</span> is about -11 Wm-<span class="hlt">2</span>, latent heat <span class="hlt">flux</span> is about +<span class="hlt">2</span> W m-<span class="hlt">2</span>, net radiation is -12 W m-<span class="hlt">2</span>, and residual energy is -3 W m-<span class="hlt">2</span> with clear diurnal variations. Estimated mean values of surface exchange coefficients for momentum, heat and moisture are 5.15 × 10-3, 1.19 × 10-3, and 1.87 × 10-3, respectively. The observed exchange coefficients of heat shows clear diurnal variations while those of momentum and moisture do not show diurnal variation. The parameterized exchange coefficients of heat and moisture produces heat <span class="hlt">fluxes</span> which compare well with the observed diurnal variations of heat <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4948307','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4948307"><span>Detecting regional patterns of changing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in Alaska</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Parazoo, Nicholas C.; Wofsy, Steven C.; Koven, Charles D.; Sweeney, Colm; Lawrence, David M.; Lindaas, Jakob; Chang, Rachel Y.-W.; Miller, Charles E.</p> <p>2016-01-01</p> <p>With rapid changes in climate and the seasonal amplitude of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) in the Arctic, it is critical that we detect and quantify the underlying processes controlling the changing amplitude of <span class="hlt">CO</span><span class="hlt">2</span> to better predict carbon cycle feedbacks in the Arctic climate system. We use satellite and airborne observations of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> with climatically forced <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> simulations to assess the detectability of Alaskan carbon cycle signals as future warming evolves. We find that current satellite remote sensing technologies can detect changing uptake accurately during the growing season but lack sufficient cold season coverage and near-surface sensitivity to constrain annual carbon balance changes at regional scale. Airborne strategies that target regular vertical profile measurements within continental interiors are more sensitive to regional <span class="hlt">flux</span> deeper into the cold season but currently lack sufficient spatial coverage throughout the entire cold season. Thus, the current <span class="hlt">CO</span><span class="hlt">2</span> observing network is unlikely to detect potentially large <span class="hlt">CO</span><span class="hlt">2</span> sources associated with deep permafrost thaw and cold season respiration expected over the next 50 y. Although continuity of current observations is vital, strategies and technologies focused on cold season measurements (active remote sensing, aircraft, and tall towers) and systematic sampling of vertical profiles across continental interiors over the full annual cycle are required to detect the onset of carbon release from thawing permafrost. PMID:27354511</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1259729-detecting-regional-patterns-changing-co2-flux-alaska','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1259729-detecting-regional-patterns-changing-co2-flux-alaska"><span>Detecting regional patterns of changing <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> in Alaska</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Parazoo, Nicholas C.; Commane, Roisin; Wofsy, Steven C.; ...</p> <p>2016-06-27</p> <p>With rapid changes in climate and the seasonal amplitude of carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span>) in the Arctic, it is critical that we detect and quantify the underlying processes controlling the changing amplitude of <span class="hlt">CO</span> <span class="hlt">2</span> to better predict carbon cycle feedbacks in the Arctic climate system. We use satellite and airborne observations of atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> with climatically forced <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> simulations to assess the detectability of Alaskan carbon cycle signals as future warming evolves. We find that current satellite remote sensing technologies can detect changing uptake accurately during the growing season but lack sufficient cold season coverage andmore » near-surface sensitivity to constrain annual carbon balance changes at regional scale. Airborne strategies that target regular vertical profile measurements within continental interiors are more sensitive to regional <span class="hlt">flux</span> deeper into the cold season but currently lack sufficient spatial coverage throughout the entire cold season. Thus, the current <span class="hlt">CO</span> <span class="hlt">2</span> observing network is unlikely to detect potentially large <span class="hlt">CO</span> <span class="hlt">2</span> sources associated with deep permafrost thaw and cold season respiration expected over the next 50 y. In conclusion, although continuity of current observations is vital, strategies and technologies focused on cold season measurements (active remote sensing, aircraft, and tall towers) and systematic sampling of vertical profiles across continental interiors over the full annual cycle are required to detect the onset of carbon release from thawing permafrost.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AtmEn..74...60L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AtmEn..74...60L"><span>Variability of <span class="hlt">CO</span><span class="hlt">2</span> concentrations and <span class="hlt">fluxes</span> in and above an urban street canyon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lietzke, Björn; Vogt, Roland</p> <p>2013-08-01</p> <p>The variability of <span class="hlt">CO</span><span class="hlt">2</span> concentrations and <span class="hlt">fluxes</span> in dense urban environments is high due to the inherent heterogeneity of these complex areas and their spatio-temporally variable anthropogenic sources. With a focus on micro- to local-scale <span class="hlt">CO</span><span class="hlt">2</span>-exchange processes, measurements were conducted in a street canyon in the city of Basel, Switzerland in 2010. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were sampled at the top of the canyon (19 m) and at 39 m while vertical <span class="hlt">CO</span><span class="hlt">2</span> concentration profiles were measured in the center and at a wall of the canyon. <span class="hlt">CO</span><span class="hlt">2</span> concentration distributions in the street canyon and exchange processes with the layers above show, apart from expected general diurnal patterns due mixing layer heights, a strong dependence on wind direction relative to the canyon. As a consequence of the resulting corkscrew-like canyon vortex, accumulation of <span class="hlt">CO</span><span class="hlt">2</span> inside the canyon is modulated with distinct distribution patterns. The evaluation of diurnal traffic data provides good explanations for the vertical and horizontal differences in <span class="hlt">CO</span><span class="hlt">2</span>-distribution inside the canyon. Diurnal <span class="hlt">flux</span> characteristics at the top of the canyon can almost solely be explained with traffic density expressed by the strong linear dependence. Even the diurnal course of the <span class="hlt">flux</span> at 39 m shows a remarkable relationship to traffic density for east wind conditions while, for west wind situations, a change toward source areas with lower emissions leads to a reduced <span class="hlt">flux</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P43D2905H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P43D2905H"><span>The Heat <span class="hlt">Flux</span> through the <span class="hlt">Ice</span> Shell on Europa, Constraints from Measurements in Terrestrial Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hruba, J.; Kletetschka, G.</p> <p>2017-12-01</p> <p>Heat transport across the <span class="hlt">ice</span> shell of Europa controls the thermal evolution of its interior. Such process involves energy sources that drive <span class="hlt">ice</span> resurfacing (1). More importantly, heat <span class="hlt">flux</span> through the <span class="hlt">ice</span> shell controls the thickness of the <span class="hlt">ice</span> (<span class="hlt">2</span>), that is poorly constrained between 1 km to 30+ km (3). Thin <span class="hlt">ice</span> would allow ocean water to be affected by radiation from space. Thick <span class="hlt">ice</span> would limit the heat ocean sources available to the rock-ocean interface at the ocean's bottom due to tidal dissipation and potential radioactive sources. The heat <span class="hlt">flux</span> structures control the development of geometrical configurations on the Europa's surface like double ridges, <span class="hlt">ice</span> diapirs, chaos regions because the rheology of <span class="hlt">ice</span> is temperature dependent (4).Analysis of temperature record of growing <span class="hlt">ice</span> cover over a pond and water below revealed the importance of solar radiation during the <span class="hlt">ice</span> growth. If there is no snow cover, a sufficient amount of solar radiation can penetrate through the <span class="hlt">ice</span> and heat the water below. Due to temperature gradient, there is a heat <span class="hlt">flux</span> from the water to the <span class="hlt">ice</span> (Qwi), which may reduce <span class="hlt">ice</span> growth at the bottom. Details and variables that constrain the heat <span class="hlt">flux</span> through the <span class="hlt">ice</span> can be utilized to estimate the <span class="hlt">ice</span> thickness. We show with this analog analysis provides the forth step towards measurement strategy on the surface of Europa. We identify three types of thermal profiles (5) and fourth with combination of all three mechanisms.References:(1) Barr, A. C., A. P. Showman, 2009, Heat transfer in Europa's icy shell, University of Arizona Press, p. 405-430.(<span class="hlt">2</span>) Ruiz, J., J. A. Alvarez-Gómez, R. Tejero, and N. Sánchez, 2007, Heat flow and thickness of a convective <span class="hlt">ice</span> shell on Europa for grain size-dependent rheologies: Icarus, v. 190, p. 145-154.(3) Billings, S. E., S. A. Kattenhorn, 2005, The great thickness debate: <span class="hlt">Ice</span> shell thickness models for Europa and comparisons with estimates based on flexure at ridges: Icarus, v. 177, p. 397-412.(4) Quick</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMNH41E..07Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMNH41E..07Z"><span>Marginal <span class="hlt">Ice</span> Zone Processes Observed from Unmanned Aerial Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zappa, C. J.</p> <p>2015-12-01</p> <p>Recent years have seen extreme changes in the Arctic. Marginal <span class="hlt">ice</span> zones (MIZ), or areas where the "<span class="hlt">ice</span>-albedo feedback" driven by solar warming is highest and <span class="hlt">ice</span> melt is extensive, may provide insights into the extent of these changes. Furthermore, MIZ play a central role in setting the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> balance making them a critical component of the global carbon cycle. Incomplete understanding of how the sea-<span class="hlt">ice</span> modulates gas <span class="hlt">fluxes</span> renders it difficult to estimate the carbon budget in MIZ. Here, we investigate the turbulent mechanisms driving mixing and gas exchange in leads, polynyas and in the presence of <span class="hlt">ice</span> floes using both field and laboratory measurements. Measurements from unmanned aerial systems (UAS) in the marginal <span class="hlt">ice</span> zone were made during <span class="hlt">2</span> experiments: 1) North of Oliktok Point AK in the Beaufort Sea were made during the Marginal <span class="hlt">Ice</span> Zone Ocean and <span class="hlt">Ice</span> Observations and Processes EXperiment (MIZOPEX) in July-August 2013 and <span class="hlt">2</span>) Fram Strait and Greenland Sea northwest of Ny-Ålesund, Svalbard, Norway during the <span class="hlt">Air-Sea-Ice</span> Physics and Biogeochemistry Experiment (ASIPBEX) April - May 2015. We developed a number of new payloads that include: i) hyperspectral imaging spectrometers to measure VNIR (400-1000 nm) and NIR (900-1700 nm) spectral radiance; ii) net longwave and net shortwave radiation for <span class="hlt">ice</span>-ocean albedo studies; iii) <span class="hlt">air-sea-ice</span> turbulent <span class="hlt">fluxes</span> as well as wave height, <span class="hlt">ice</span> freeboard, and surface roughness with a LIDAR; and iv) drone-deployed micro-drifters (DDµD) deployed from the UAS that telemeter temperature, pressure, and RH as it descends through the atmosphere and temperature and salinity of the upper meter of the ocean once it lands on the ocean's surface. Visible and IR imagery of melting <span class="hlt">ice</span> floes clearly defines the scale of the <span class="hlt">ice</span> floes. The IR imagery show distinct cooling of the skin sea surface temperature (SST) as well as an intricate circulation and mixing pattern that depends on the surface current, wind speed, and near</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11538596','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11538596"><span>Temperature of nitrogen <span class="hlt">ice</span> on Pluto and its implications for <span class="hlt">flux</span> measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tryka, K A; Brown, R H; Cruikshank, D P; Owen, T C; Geballe, T R; DeBergh, C</p> <p>1994-01-01</p> <p>Previous work by K.A. Tryka et al. (Science 261, 751-754, 1993) has shown that the profile of the <span class="hlt">2</span>.148-micrometers band of solid nitrogen can be used as a "thermometer" and determined the temperature of nitrogen <span class="hlt">ice</span> on Triton to be 38(+<span class="hlt">2</span>)-1 K. Here we reevaluate that data and refine the temperature value to 38 +/- 1 K. Applying the same technique to Pluto we determine that the temperature of the N<span class="hlt">2</span> <span class="hlt">ice</span> on that body is 40 +/- <span class="hlt">2</span> K. Using this result we have created a nonisothermal <span class="hlt">flux</span> model of the Pluto-Charon system. The model treats Pluto as a body with symmetric N<span class="hlt">2</span> polar caps and an equatorial region devoid of N<span class="hlt">2</span>. Comparison with the infrared and millimeter <span class="hlt">flux</span> measurements shows that the published <span class="hlt">fluxes</span> are consistent with models incorporating extensive N<span class="hlt">2</span> polar caps (down to +/- 15 degrees or +/- 20 degrees latitude) and an equatorial region with a bolometric albedo < or = 0.<span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950053532&hterms=pluto&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dpluto','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950053532&hterms=pluto&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dpluto"><span>Temperature of nitrogen <span class="hlt">ice</span> on Pluto and its implications for <span class="hlt">flux</span> measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tryka, Kimberly A.; Brown, Robert H.; Chruikshank, Dale P.; Owen, Tobias C.; Geballe, Thomas R.; Debergh, Catherine</p> <p>1994-01-01</p> <p>Previous work by K. A. Tryka et al. (1993) has shown that the profile of the <span class="hlt">2</span>.148-micron band of solid nitrogen can be used as a 'thermometer' and determined the tempertature of nitrogen <span class="hlt">ice</span> on Triton to be 38(sup +<span class="hlt">2</span>)(sub -1) K. Here we reevalute that data and refine the temperature value to 38 +/- 1 K. Applying the same technique to Pluto we determine that the temperature of the N<span class="hlt">2</span> <span class="hlt">ice</span> on that body is 40 +/- <span class="hlt">2</span> K. Using this result we have created a nonisothermal <span class="hlt">flux</span> model of the Pluto-Charon system. The model treats Pluto as a body with symmetric N<span class="hlt">2</span> polar caps and an equatorial region devoid of N<span class="hlt">2</span>. Comparison with the infrared and millimeter <span class="hlt">flux</span> measurements shows that the published <span class="hlt">fluxes</span> are consistent with models incorporating extensive N<span class="hlt">2</span> polar caps (down to +/- 15 deg ot +/- 20 deg latitude) and an equatorial region with a bolometric albedo less than or equal to 0.<span class="hlt">2</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940011426','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940011426"><span>Imaging radar studies of polar <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Carsey, Frank</p> <p>1993-01-01</p> <p>A vugraph format presentation is given. The following topics are discussed: scientific overview, radar data opportunities, sea <span class="hlt">ice</span> investigations, and <span class="hlt">ice</span> sheet investigations. The Sea <span class="hlt">Ice</span> Scientific Objectives are as follows: (1) to estimate globally the surface brine generation, heat <span class="hlt">flux</span>, and fresh water advection (as <span class="hlt">ice</span>); (<span class="hlt">2</span>) to monitor phasing of seasonal melt and freeze events and accurately estimate melt and growth rates; and (3) to develop improved treatment of momentum transfer and <span class="hlt">ice</span> mechanics in coupled <span class="hlt">air-sea-ice</span> models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.1398B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.1398B"><span>Top-down estimate of surface <span class="hlt">flux</span> in the Los Angeles Basin using a mesoscale inverse modeling technique: assessing anthropogenic emissions of <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> and their impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brioude, Jerome; Angevine, Wayne; Ahmadov, Ravan; Kim, Si Wan; Evan, Stephanie; McKeen, Stuart; Hsie, Eirh Yu; Frost, Greg; Neuman, Andy; Pollack, Ilana; Peischl, Jeff; Ryerson, Tom; Holloway, John; Brown, Steeve; Nowak, John; Roberts, Jim; Wofsy, Steeve; Santoni, Greg; Trainer, Michael</p> <p>2013-04-01</p> <p>We present top-down estimates of anthropogenic <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> at mesoscale using a Lagrangian model in combination with three different WRF model configurations, driven by data from aircraft flights during the CALNEX campaign in southern California in May-June 2010. The US EPA National Emission Inventory 2005 (NEI 2005) was the prior in the <span class="hlt">CO</span> and NOx inversion calculations. The <span class="hlt">flux</span> ratio inversion method, based on linear relationships between chemical species, was used to calculate the <span class="hlt">CO</span><span class="hlt">2</span> inventory without prior knowledge of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span>. The inversion was applied to each flight to estimate the variability of single-flight-based <span class="hlt">flux</span> estimates. In Los Angeles (LA) County, the uncertainties on <span class="hlt">CO</span> and NOx <span class="hlt">fluxes</span> were 10% and 15%, respectively. Compared with NEI 2005, the <span class="hlt">CO</span> posterior emissions were lower by 43% ± 6% in LA County and by 37% ± 10% in the South Coast <span class="hlt">Air</span> Basin (SoCAB). NOx posterior emissions were lower by 32% ± 10% in LA County and by 27% ± 15% in the SoCAB. NOx posterior emissions were 40% lower on weekends relative to weekdays. The <span class="hlt">CO</span><span class="hlt">2</span> posterior estimates were 183 ± 18 Tg yr-1 in SoCAB. A flight during ITCT in 2002 was used to estimate emissions in the LA Basin in 2002. From 2002 to 2010, the <span class="hlt">CO</span> and NOx posterior emissions decreased by 41% and 37%, respectively, in agreement with previous studies. Over the same time period, <span class="hlt">CO</span><span class="hlt">2</span> emissions increased by 10% ± 14% in LA County but decreased by 4% ± 10% in the SoCAB, a statistically insignificant change. Overall, the posterior estimates were in good agreement with the California <span class="hlt">Air</span> Resources Board (CARB) inventory, with differences of 15% or less. However, the posterior spatial distribution in the basin was significantly different from CARB for NOx emissions. WRF-Chem mesoscale chemical-transport model simulations allowed an evaluation of differences in chemistry using different inventory assumptions, including NEI 2005, CARB 2010 and the posterior inventories derived in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACP....13.3661B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACP....13.3661B"><span>Top-down estimate of surface <span class="hlt">flux</span> in the Los Angeles Basin using a mesoscale inverse modeling technique: assessing anthropogenic emissions of <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> and their impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brioude, J.; Angevine, W. M.; Ahmadov, R.; Kim, S.-W.; Evan, S.; McKeen, S. A.; Hsie, E.-Y.; Frost, G. J.; Neuman, J. A.; Pollack, I. B.; Peischl, J.; Ryerson, T. B.; Holloway, J.; Brown, S. S.; Nowak, J. B.; Roberts, J. M.; Wofsy, S. C.; Santoni, G. W.; Oda, T.; Trainer, M.</p> <p>2013-04-01</p> <p>We present top-down estimates of anthropogenic <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> at mesoscale using a Lagrangian model in combination with three different WRF model configurations, driven by data from aircraft flights during the CALNEX campaign in southern California in May-June 2010. The US EPA National Emission Inventory 2005 (NEI 2005) was the prior in the <span class="hlt">CO</span> and NOx inversion calculations. The <span class="hlt">flux</span> ratio inversion method, based on linear relationships between chemical species, was used to calculate the <span class="hlt">CO</span><span class="hlt">2</span> inventory without prior knowledge of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span>. The inversion was applied to each flight to estimate the variability of single-flight-based <span class="hlt">flux</span> estimates. In Los Angeles (LA) County, the uncertainties on <span class="hlt">CO</span> and NOx <span class="hlt">fluxes</span> were 10% and 15%, respectively. Compared with NEI 2005, the <span class="hlt">CO</span> posterior emissions were lower by 43% in LA County and by 37% in the South Coast <span class="hlt">Air</span> Basin (SoCAB). NOx posterior emissions were lower by 32% in LA County and by 27% in the SoCAB. NOx posterior emissions were 40% lower on weekends relative to weekdays. The <span class="hlt">CO</span><span class="hlt">2</span> posterior estimates were 183 Tg yr-1 in SoCAB. A flight during ITCT (Intercontinental Transport and Chemical Transformation) in 2002 was used to estimate emissions in the LA Basin in 2002. From 2002 to 2010, the <span class="hlt">CO</span> and NOx posterior emissions decreased by 41% and 37%, respectively, in agreement with previous studies. Over the same time period, <span class="hlt">CO</span><span class="hlt">2</span> emissions increased by 10% in LA County but decreased by 4% in the SoCAB, a statistically insignificant change. Overall, the posterior estimates were in good agreement with the California <span class="hlt">Air</span> Resources Board (CARB) inventory, with differences of 15% or less. However, the posterior spatial distribution in the basin was significantly different from CARB for NOx emissions. WRF-Chem mesoscale chemical-transport model simulations allowed an evaluation of differences in chemistry using different inventory assumptions, including NEI 2005, a gridded CARB inventory and the posterior</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ACPD...1231439B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ACPD...1231439B"><span>Top-down estimate of surface <span class="hlt">flux</span> in the Los Angeles Basin using a mesoscale inverse modeling technique: assessing anthropogenic emissions of <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> and their impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brioude, J.; Angevine, W. M.; Ahmadov, R.; Kim, S.-W.; Evan, S.; McKeen, S. A.; Hsie, E.-Y.; Frost, G. J.; Neuman, J. A.; Pollack, I. B.; Peischl, J.; Ryerson, T. B.; Holloway, J.; Brown, S. S.; Nowak, J. B.; Roberts, J. M.; Wofsy, S. C.; Santoni, G. W.; Trainer, M.</p> <p>2012-12-01</p> <p>We present top-down estimates of anthropogenic <span class="hlt">CO</span>, NOx and <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> at mesoscale using a Lagrangian model in combination with three different WRF model configurations, driven by data from aircraft flights during the CALNEX campaign in southern California in May-June 2010. The US EPA National Emission Inventory 2005 (NEI 2005) was the prior in the <span class="hlt">CO</span> and NOx inversion calculations. The <span class="hlt">flux</span> ratio inversion method, based on linear relationships between chemical species, was used to calculate the <span class="hlt">CO</span><span class="hlt">2</span> inventory without prior knowledge of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span>. The inversion was applied to each flight to estimate the variability of single-flight-based <span class="hlt">flux</span> estimates. In Los Angeles (LA) County, the uncertainties on <span class="hlt">CO</span> and NOx <span class="hlt">fluxes</span> were 10% and 15%, respectively. Compared with NEI 2005, the <span class="hlt">CO</span> posterior emissions were lower by 43% ± 6% in LA County and by 37% ± 10% in the South Coast <span class="hlt">Air</span> Basin (SoCAB). NOx posterior emissions were lower by 32% ± 10% in LA County and by 27% ± 15% in the SoCAB. NOx posterior emissions were 40% lower on weekends relative to weekdays. The <span class="hlt">CO</span><span class="hlt">2</span> posterior estimates were 183 ± 18 Tg yr-1 in SoCAB. A flight during ITCT in 2002 was used to estimate emissions in the LA Basin in 2002. From 2002 to 2010, the <span class="hlt">CO</span> and NOx posterior emissions decreased by 41% and 37%, respectively, in agreement with previous studies. Over the same time period, <span class="hlt">CO</span><span class="hlt">2</span> emissions increased by 10% ± 14% in LA County but decreased by 4% ± 10% in the SoCAB, a statistically insignificant change. Overall, the posterior estimates were in good agreement with the California <span class="hlt">Air</span> Resources Board (CARB) inventory, with differences of 15% or less. However, the posterior spatial distribution in the basin was significantly different from CARB for NOx emissions. WRF-Chem mesoscale chemical-transport model simulations allowed an evaluation of differences in chemistry using different inventory assumptions, including NEI 2005, CARB 2010 and the posterior inventories derived in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016QuRes..85...87C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016QuRes..85...87C"><span>Variability of 14C reservoir age and <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> in the Peru-Chile upwelling region during the past 12,000 years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carré, Matthieu; Jackson, Donald; Maldonado, Antonio; Chase, Brian M.; Sachs, Julian P.</p> <p>2016-01-01</p> <p>The variability of radiocarbon marine reservoir age through time and space limits the accuracy of chronologies in marine paleo-environmental archives. We report here new radiocarbon reservoir ages (ΔR) from the central coast of Chile ( 32°S) for the Holocene period and compare these values to existing reservoir age reconstructions from southern Peru and northern Chile. Late Holocene ΔR values show little variability from central Chile to Peru. Prior to 6000 cal yr BP, however, ΔR values were markedly increased in southern Peru and northern Chile, while similar or slightly lower-than-modern ΔR values were observed in central Chile. This extended dataset suggests that the early Holocene was characterized by a substantial increase in the latitudinal gradient of marine reservoir age between central and northern Chile. This change in the marine reservoir ages indicates that the early Holocene <span class="hlt">air</span>-sea <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> could have been up to five times more intense than in the late Holocene in the Peruvian upwelling, while slightly reduced in central Chile. Our results show that oceanic circulation changes in the Humboldt system during the Holocene have substantially modified the <span class="hlt">air</span>-sea carbon <span class="hlt">flux</span> in this region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999DPS....31.6105M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999DPS....31.6105M"><span>Trapping of CH4, <span class="hlt">CO</span>, and <span class="hlt">CO</span><span class="hlt">2</span> in Amorphous Water <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mastrapa, R. M. E.; Brown, R. H.; Anicich, V. G.; Cohen, B. A.; Dai, W.; Lunine, J. I.</p> <p>1999-09-01</p> <p>In this study, <span class="hlt">CO</span>, CH4, and <span class="hlt">CO</span><span class="hlt">2</span> were trapped in H<span class="hlt">2</span>O at temperatures as low as 20 K and pressures between 10-5 and 10-8 Torr. IR spectra were taken of each sample before sublimation to confirm the presence of volatiles. The samples were then heated at rates from 0.25 K/min to 1 K/min and the escape ranges were measured with a mass spectrometer. The volatiles escaped from the <span class="hlt">ice</span> mixtures in temperature ranges similar to those found in previous work (1, <span class="hlt">2</span>, 3), namely 48-52 K, 145-160 K, 170-185 K. H<span class="hlt">2</span>O is released from 150 K to 185 K. However, the temperature range of escape is strongly dependent on deposition temperature and heating rate. If the deposition temperature is below the point where the solid volatile rapidly sublimates in the ambient environment of our experiment, then the first range of volatile escape is centered around it's sublimation point, and there is little of the volatile remaining from 170-185 K. The location of the third escape range shifts to lower temperatures with slower sublimation rate. It was determined that 0.5 K/min is the ideal sample heating rate to determine these escape ranges. In our data, the infrared spectrum of <span class="hlt">CO</span> trapped in water <span class="hlt">ice</span> shows a splitting of the 2145 cm-1 solid <span class="hlt">CO</span> line into two bands at 2343 cm-1 and 2135 cm-1. These shifts are similar to those seen by Sandford, et al. (4). (1) Bar-Nun, A., G. Herman, D. Laufer, and M. L. Rappaport, (1985), Icarus, 63, 317-332. (<span class="hlt">2</span>) Bar-Nun, A., J. Dror, E. Kochavi, and D. Laufer, (1987), Physical Review B, 35, no. 5, 2427-2435. (3) Hudson, R. L., and B. Donn, (1991), Icarus, 94, 326-332. (4) Sandford, S. A., L. J. Allamandola, A. G. G. M. Tielens, and G. J. Valero, (1988), Astrophysical Journal, 329, 498-510.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970021275','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970021275"><span>Low p<span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Air</span>-Polarized <span class="hlt">CO</span><span class="hlt">2</span> Concentrator Development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schubert, Franz H.</p> <p>1997-01-01</p> <p>Life Systems completed a Ground-based Space Station Experiment Development Study Program which verifies through testing the performance and applicability of the electrochemical <span class="hlt">Air</span>-Polarized Carbon Dioxide Concentrator (APC) process technology for space missions requiring low (i.e., less than 3 mm Hg) <span class="hlt">CO</span><span class="hlt">2</span> partial pressure (p<span class="hlt">CO</span><span class="hlt">2</span>) in the cabin atmosphere. Required test hardware was developed and testing was accomplished at an approximate one-person capacity <span class="hlt">CO</span><span class="hlt">2</span> removal level. Initially, two five-cell electrochemical modules using flight-like 0.5 sq ft cell hardware were tested individually, following by their testing at the integrated APC system level. Testing verified previously projected performance and established a database for sizing of APC systems. A four person capacity APC system was sized and compared with four candidate <span class="hlt">CO</span><span class="hlt">2</span> removal systems. At its weight of 252 lb, a volume of 7 cu ft and a power consumption of 566 W while operating at <span class="hlt">2.2</span> mm Hg p<span class="hlt">CO</span><span class="hlt">2</span>, the APC was surpassed only by an Electrochemical Depolarized <span class="hlt">CO</span><span class="hlt">2</span> Concentrator (EDC) (operating with H<span class="hlt">2</span>), when compared on a total equivalent basis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/48404','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/48404"><span>Diffusional <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> through snow: Spatial and temporal variability among alpine-subalpine sites</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Richard A. Sommerfeld; William J. Massman; Robert C. Musselman</p> <p>1996-01-01</p> <p>Three alpine and three subalpine sites were monitored for up to 4 years to acquire data on the temporal and spatial variability of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> through snowpacks. We conclude that the snow formed a passive cap which controlled the concentration of <span class="hlt">CO</span><span class="hlt">2</span> at the snow-soil interface, while the <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> into the atmosphere was controlled by <span class="hlt">CO</span><span class="hlt">2</span> production in the soil....</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987ClDy....1...87B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987ClDy....1...87B"><span>The influence of continental <span class="hlt">ice</span>, atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, and land albedo on the climate of the last glacial maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Broccoli, A. J.; Manabe, S.</p> <p>1987-02-01</p> <p>The contributions of expanded continental <span class="hlt">ice</span>, reduced atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, and changes in land albedo to the maintenance of the climate of the last glacial maximum (LGM) are examined. A series of experiments is performed using an atmosphere-mixed layer ocean model in which these changes in boundary conditions are incorporated either singly or in combination. The model used has been shown to produce a reasonably realistic simulation of the reduced temperature of the LGM (Manabe and Broccoli 1985b). By comparing the results from pairs of experiments, the effects of each of these environmental changes can be determined. Expanded continental <span class="hlt">ice</span> and reduced atmospheric <span class="hlt">CO</span><span class="hlt">2</span> are found to have a substantial impact on global mean temperature. The <span class="hlt">ice</span> sheet effect is confined almost exclusively to the Northern Hemisphere, while lowered <span class="hlt">CO</span><span class="hlt">2</span> cools both hemispheres. Changes in land albedo over <span class="hlt">ice</span>-free areas have only a minor thermal effect on a global basis. The reduction of <span class="hlt">CO</span><span class="hlt">2</span> content in the atmosphere is the primary contributor to the cooling of the Southern Hemisphere. The model sensitivity to both the <span class="hlt">ice</span> sheet and <span class="hlt">CO</span><span class="hlt">2</span> effects is characterized by a high latitude amplification and a late autumn and early winter maximum. Substantial changes in Northern Hemisphere tropospheric circulation are found in response to LGM boundary conditions during winter. An amplified flow pattern and enhanced westerlies occur in the vicinity of the North American and Eurasian <span class="hlt">ice</span> sheets. These alterations of the tropospheric circulation are primarily the result of the <span class="hlt">ice</span> sheet effect, with reduced <span class="hlt">CO</span><span class="hlt">2</span> contributing only a slight amplification of the <span class="hlt">ice</span> sheet-induced pattern.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998PhDT.........8T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998PhDT.........8T"><span><span class="hlt">CO-ices</span> in embedded Young Stellar Objects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Teixeira, Teresa Cláeira V. S.</p> <p>1998-09-01</p> <p> significance of the results is discussed. Excellent fits to the nonpolar component of the <span class="hlt">CO-ices</span> along the observed lines-of-sight are produced with ion irradiated pure <span class="hlt">CO</span> <span class="hlt">ices</span>. The possible origin of the ion irradiation is discussed, covering flares on the YSOs, cosmic rays and X-ray and UV processing. Predictions are made for the abundance of <span class="hlt">CO</span><span class="hlt">2</span> and methanol in the mantles. Furthermore, a comparison is made between the results of observations of <span class="hlt">CO</span> and H<span class="hlt">2</span> O <span class="hlt">ices</span> towards the Taurus and Ophiuchus dark clouds. The column densities of the <span class="hlt">ices</span> are compared with the visual extinction, Av, through the clouds, and with the 1.3mm continuum emission from the YSOs. The inclusion of the objects in Taurus observed in this work resulted in the appearance of a discontinuity in the relation between the water-<span class="hlt">ice</span> column density and Av, at the value of Av for which the optical depth at 3 microns (the wavelength of the water-<span class="hlt">ice</span> absorption feature) is unity. Finally, all the observations and results discussed throughout the thesis are brought together to address their implications in the current understanding of the conditions in Taurus and Ophiuchus. Thesis and published paper available at http://www.obs.aau.dk/~tct/</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70188140','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70188140"><span>Historical patterns of acidification and increasing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> associated with Florida springs</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Barrera, Kira E.; Robbins, Lisa L.</p> <p>2017-01-01</p> <p>Florida has one of the highest concentrations of springs in the world, with many discharging into rivers and predominantly into eastern Gulf of Mexico coast, and they likely influence the hydrochemistry of these adjacent waters; however, temporal and spatial trends have not been well studied. We present over 20 yr of hydrochemical, seasonally sampled data to identify temporal and spatial trends of pH, alkalinity, partial pressure of carbon dioxide (p<span class="hlt">CO</span><span class="hlt">2</span>), and <span class="hlt">CO</span><span class="hlt">2</span><span class="hlt">flux</span> from five first-order-magnitude (springs that discharge greater than <span class="hlt">2</span>.83 m3 s−1) coastal spring groups fed by the Floridan Aquifer System that ultimately discharge into the Gulf of Mexico. All spring groups had p<span class="hlt">CO</span><span class="hlt">2</span> levels (averages 3174.3–6773.<span class="hlt">2</span> μatm) that were much higher than atmospheric levels of <span class="hlt">CO</span><span class="hlt">2</span> and demonstrated statistically significant temporal decreases in pH and increases in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, p<span class="hlt">CO</span><span class="hlt">2</span>, and alkalinity. Total carbon <span class="hlt">flux</span> emissions increased from each of the spring groups by between 3.48 × 107 and <span class="hlt">2</span>.856 × 108 kg C yr−1 over the time period. By 2013 the Springs Groups in total emitted more than 1.1739 × 109 kg C yr−1. Increases in alkalinity and p<span class="hlt">CO</span><span class="hlt">2</span> varied from 90.9 to 347.6 μmol kg−1 and 1262.3 to 2666.7 μatm, respectively. Coastal data show higher <span class="hlt">CO</span><span class="hlt">2</span> evasion than the open Gulf of Mexico, which suggests spring water influences nearshore waters. The results of this study have important implications for spring water quality, dissolution of the Florida carbonate platform, and identification of the effect and partitioning of carbon <span class="hlt">fluxes</span> to and within coastal and marine ecosystems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS24A..04D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS24A..04D"><span>Diagnosis of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> in the Coastal Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dai, M.; Cao, Z.; Yang, W.; Guo, X.; Yin, Z.; Zhao, Y.</p> <p>2017-12-01</p> <p>Coastal ocean carbon is an important component of the global carbon cycle. However, its mechanistic-based conceptualization, a prerequisite of coastal carbon modeling and its inclusion in the Earth System Model, remains difficult due to the highest variability in both time and space. Here we show that the inter-seasonal change of the global coastal p<span class="hlt">CO</span><span class="hlt">2</span> is more determined by non-temperature factors such as biological drawdown and water mass mixing, the latter of which features the dynamic boundary processes of the coastal ocean at both land-margin and margin-open ocean interfaces. Considering these unique features, we resolve the coastal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> using a semi-analytical approach coupling physics-biogeochemistry and carbon-nutrients and conceptualize the coastal carbon cycle into Ocean-dominated Margins (OceMar) and River-dominated Ocean Margins (RiOMar). The diagnostic result of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the South China Sea basin and the Arabian Sea as OceMars and in the Pearl River Plume as a RioMar is consistent with field observations. Our mechanistic-based diagnostic approach therefore helps better understand and model coastal carbon cycle yet the stoichiometry of carbon-nutrients coupling needs scrutiny when applying our approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43D2493M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43D2493M"><span>Remarkable separability of the circulation response to Arctic sea <span class="hlt">ice</span> loss and greenhouse gas forcing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McCusker, K. E.; Kushner, P. J.; Fyfe, J. C.; Sigmond, M.; Kharin, V. V.; Bitz, C. M.</p> <p>2017-12-01</p> <p>Arctic sea <span class="hlt">ice</span> loss has an important effect on local climate through increases in ocean to atmosphere heat <span class="hlt">flux</span> and associated feedbacks, and may influence midlatitude climate by changing large-scale circulation that can enhance or counter changes that are due to greenhouse gases. The extent to which climate change in a warming world can be understood as greenhouse gas-induced changes that are modulated by Arctic sea <span class="hlt">ice</span> loss depends on how additive the responses to the separate influences are. Here we use a novel sea <span class="hlt">ice</span> nudging methodology in the Canadian Earth System Model, which has a fully coupled ocean, to isolate the effects of Arctic sea <span class="hlt">ice</span> loss and doubled atmospheric carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) to determine their additivity and sensitivity to mean state. We find that the separate effects of Arctic sea <span class="hlt">ice</span> loss and doubled <span class="hlt">CO</span><span class="hlt">2</span> are remarkably additive and relatively insensitive to mean climate state. This separability is evident in several thermodynamic and dynamic fields throughout most of the year, from hemispheric to synoptic scales. The extent to which the regional response to sea <span class="hlt">ice</span> loss sometimes agrees with and sometimes cancels the response to <span class="hlt">CO</span><span class="hlt">2</span> is quantified. In this model, Arctic sea <span class="hlt">ice</span> loss enhances the <span class="hlt">CO</span><span class="hlt">2</span>-induced surface <span class="hlt">air</span> temperature changes nearly everywhere and zonal wind changes over the Pacific sector, whereas sea <span class="hlt">ice</span> loss counters <span class="hlt">CO</span><span class="hlt">2</span>-induced sea level pressure changes nearly everywhere over land and zonal wind changes over the Atlantic sector. This separability of the response to Arctic sea <span class="hlt">ice</span> loss from the response to <span class="hlt">CO</span><span class="hlt">2</span> doubling gives credence to the body of work in which Arctic sea <span class="hlt">ice</span> loss is isolated from the forcing that modified it, and might provide a means to better interpret the diverse array of modeling and observational studies of Arctic change and influence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B53I..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B53I..03W"><span>Warming trumps <span class="hlt">CO</span><span class="hlt">2</span>: future climate conditions suppress carbon <span class="hlt">fluxes</span> in two dominant boreal tree species</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Way, D.; Dusenge, M. E.; Madhavji, S.</p> <p>2017-12-01</p> <p>Increases in <span class="hlt">CO</span><span class="hlt">2</span> are expected to raise <span class="hlt">air</span> temperatures in northern latitudes by up to 8 °C by the end of the century. Boreal forests in these regions play a large role in the global carbon cycle, and the responses of boreal tree species to climate drivers will thus have considerable impacts on the trajectory of future <span class="hlt">CO</span><span class="hlt">2</span> increases. We grew two dominant North American boreal tree species at a range of future climate conditions to assess how carbon <span class="hlt">fluxes</span> were altered by high <span class="hlt">CO</span><span class="hlt">2</span> and warming. Black spruce (Picea mariana) and tamarack (Larix laricina) were grown from seed under either ambient (400 ppm) or elevated <span class="hlt">CO</span><span class="hlt">2</span> concentrations (750 ppm) and either ambient temperatures, moderate warming (ambient +4 °C), or extreme warming (ambient +8 °C) for six months. We measured temperature responses of net photosynthesis, maximum rates of Rubisco carboxylation (Vcmax) and electron transport (Jmax) and dark respiration to determine acclimation to the climate treatments. Overall, growth temperature had a strong effect on carbon <span class="hlt">fluxes</span>, while there were no significant effects of growth <span class="hlt">CO</span><span class="hlt">2</span>. In both species, the photosynthetic thermal optimum increased and maximum photosynthetic rates were reduced in warm-grown seedlings, but the strength of these changes varied between species. Vcmax and Jmax were also reduced in warm-grown seedlings, and this correlated with reductions in leaf N concentrations. Warming increased the activation energy for Vcmax and the thermal optimum for Jmax in both species. Respiration acclimated to elevated growth temperatures, but there were no treatment effects on the Q10 of respiration (the increase in respiration for a 10 °C increase in leaf temperature). Our results show that climate warming is likely to reduce carbon <span class="hlt">fluxes</span> in these boreal conifers, and that photosynthetic parameters used to model photosynthesis in dynamic global vegetation models acclimate to increased temperatures, but show little response to elevated <span class="hlt">CO</span><span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA258067','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA258067"><span>Sediment <span class="hlt">Flux</span>, East Greenland Margin</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1991-09-17</p> <p>D.. T 0ATE [3. AEORT TYPE AND ý -<span class="hlt">2</span>-’S .’:<span class="hlt">2</span>,E.i 09/17/91 Final Oct. . 1988 - Seot.l. 1991 4. TITLE AND SU.3TITLE S. F*.i1CjG . AU • 12..5 Sediment <span class="hlt">Flux</span>...and s le ,; its ditribution is unlimited. 13. ABSTRACT (Maximum <span class="hlt">2</span><span class="hlt">CO</span> words) We investigated sediment <span class="hlt">flux</span> across an <span class="hlt">ice</span>-dominated, high latitude...investigated an area off the East Greenland margin where the world’s second largest <span class="hlt">ice</span> sheet still exists and where information on the extent of glaciation on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.6547Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.6547Y"><span><span class="hlt">Air</span>-sea interaction regimes in the sub-Antarctic Southern Ocean and Antarctic marginal <span class="hlt">ice</span> zone revealed by icebreaker measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Lisan; Jin, Xiangze; Schulz, Eric W.; Josey, Simon A.</p> <p>2017-08-01</p> <p>This study analyzed shipboard <span class="hlt">air</span>-sea measurements acquired by the icebreaker Aurora Australis during its off-winter operation in December 2010 to May 2012. Mean conditions over 7 months (October-April) were compiled from a total of 22 ship tracks. The icebreaker traversed the water between Hobart, Tasmania, and the Antarctic continent, providing valuable in situ insight into two dynamically important, yet poorly sampled, regimes: the sub-Antarctic Southern Ocean and the Antarctic marginal <span class="hlt">ice</span> zone (MIZ) in the Indian Ocean sector. The transition from the open water to the <span class="hlt">ice</span>-covered surface creates sharp changes in albedo, surface roughness, and <span class="hlt">air</span> temperature, leading to consequential effects on <span class="hlt">air</span>-sea variables and <span class="hlt">fluxes</span>. Major effort was made to estimate the <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> in the MIZ using the bulk <span class="hlt">flux</span> algorithms that are tuned specifically for the sea-<span class="hlt">ice</span> effects, while computing the <span class="hlt">fluxes</span> over the sub-Antarctic section using the COARE3.0 algorithm. The study evidenced strong sea-<span class="hlt">ice</span> modulations on winds, with the southerly airflow showing deceleration (convergence) in the MIZ and acceleration (divergence) when moving away from the MIZ. Marked seasonal variations in heat exchanges between the atmosphere and the <span class="hlt">ice</span> margin were noted. The monotonic increase in turbulent latent and sensible heat <span class="hlt">fluxes</span> after summer turned the MIZ quickly into a heat loss regime, while at the same time the sub-Antarctic surface water continued to receive heat from the atmosphere. The drastic increase in turbulent heat loss in the MIZ contrasted sharply to the nonsignificant and seasonally invariant turbulent heat loss over the sub-Antarctic open water.<abstract type="synopsis"><title type="main">Plain Language SummaryThe icebreaker Aurora Australis is a research and supply vessel that is regularly chartered by the Australian Antarctic Division during the southern summer to operate in waters between Hobart, Tasmania, and Antarctica. The vessel serves as the main lifeline to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22518575-ray-irradiation-sub-co-ice-mixtures-synchrotron-light','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22518575-ray-irradiation-sub-co-ice-mixtures-synchrotron-light"><span>X-RAY IRRADIATION OF H{sub <span class="hlt">2</span>}O + <span class="hlt">CO</span> <span class="hlt">ICE</span> MIXTURES WITH SYNCHROTRON LIGHT</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Jiménez-Escobar, A.; Ciaravella, A.; Micela, G.</p> <p>2016-03-20</p> <p>We irradiated a (4:1) mixture of water and carbon monoxide with soft X-rays of energies up to 1.<span class="hlt">2</span> keV. The experiments were performed using the spherical grating monochromator beamline at National Synchrotron Radiation Research Center in Taiwan. Both monochromatic (300 and 900 eV) and broader energy <span class="hlt">fluxes</span> (250–1200 eV) were employed. During the irradiation, the H{sub <span class="hlt">2</span>}O + <span class="hlt">CO</span> mixture was ionized, excited, and fragmented, producing a number of reactive species. The composition of the <span class="hlt">ice</span> has been monitored throughout both the irradiation and warm-up phases. We identified several products, which can be related through a plausible chemical reaction scheme. Such chemistrymore » is initiated by the injection of energetic photoelectrons that produce multiple ionization events generating a secondary electron cascade. The results have been discussed in light of a model for protoplanetary disks around young solar-type stars.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090025444','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090025444"><span>Turbulent <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Measurements by Lidar: Length Scales, Results and Comparison with In-Situ Sensors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gilbert, Fabien; Koch, Grady J.; Beyon, Jeffrey Y.; Hilton, Timothy W.; Davis, Kenneth J.; Andrews, Arlyn; Ismail, Syed; Singh, Upendra N.</p> <p>2009-01-01</p> <p>The vertical <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the atmospheric boundary layer (ABL) is investigated with a Doppler differential absorption lidar (DIAL). The instrument was operated next to the WLEF instrumented tall tower in Park Falls, Wisconsin during three days and nights in June 2007. Profiles of turbulent <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio and vertical velocity fluctuations are measured by in-situ sensors and Doppler DIAL. Time and space scales of turbulence are precisely defined in the ABL. The eddy-covariance method is applied to calculate turbulent <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> both by lidar and in-situ sensors. We show preliminary mean lidar <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements in the ABL with a time and space resolution of 6 h and 1500 m respectively. The <span class="hlt">flux</span> instrumental errors decrease linearly with the standard deviation of the <span class="hlt">CO</span><span class="hlt">2</span> data, as expected. Although turbulent fluctuations of <span class="hlt">CO</span><span class="hlt">2</span> are negligible with respect to the mean (0.1 %), we show that the eddy-covariance method can provide <span class="hlt">2</span>-h, 150-m range resolved <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates as long as the <span class="hlt">CO</span><span class="hlt">2</span> mixing ratio instrumental error is no greater than 10 ppm and the vertical velocity error is lower than the natural fluctuations over a time resolution of 10 s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1394139','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1394139"><span>Historical Carbon Dioxide Record from the Vostok <span class="hlt">Ice</span> Core (417,160 - <span class="hlt">2</span>,342 years BP)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Barnola, J. M. [CNRS, Saint Martin d'Heres Cedex, France; Raynaud, D. [CNRS, Saint Martin d'Heres Cedex, France; Lorius, C. [CNRS, Saint Martin d'Heres Cedex, France; Barkov, N. I.</p> <p>2003-01-01</p> <p>In January 1998, the collaborative <span class="hlt">ice</span>-drilling project between Russia, the United States, and France at the Russian Vostok station in East Antarctica yielded the deepest <span class="hlt">ice</span> core ever recovered, reaching a depth of 3,623 m (Petit et al. 1997, 1999). <span class="hlt">Ice</span> cores are unique with their entrapped <span class="hlt">air</span> inclusions enabling direct records of past changes in atmospheric trace-gas composition. Preliminary data indicate the Vostok <span class="hlt">ice</span>-core record extends through four climate cycles, with <span class="hlt">ice</span> slightly older than 400 kyr (Petit et al. 1997, 1999). Because <span class="hlt">air</span> bubbles do not close at the surface of the <span class="hlt">ice</span> sheet but only near the firn-<span class="hlt">ice</span> transition (that is, at ~90 m below the surface at Vostok), the <span class="hlt">air</span> extracted from the <span class="hlt">ice</span> is younger than the surrounding <span class="hlt">ice</span> (Barnola et al. 1991). Using semiempirical models of densification applied to past Vostok climate conditions, Barnola et al. (1991) reported that the age difference between <span class="hlt">air</span> and <span class="hlt">ice</span> may be ~6000 years during the coldest periods instead of ~4000 years, as previously assumed. <span class="hlt">Ice</span> samples were cut with a bandsaw in a cold room (at about -15°C) as close as possible to the center of the core in order to avoid surface contamination (Barnola et al. 1983). Gas extraction and measurements were performed with the "Grenoble analytical setup," which involved crushing the <span class="hlt">ice</span> sample (~40 g) under vacuum in a stainless steel container without melting it, expanding the gas released during the crushing in a pre-evacuated sampling loop, and analyzing the <span class="hlt">CO</span><span class="hlt">2</span> concentrations by gas chromatography (Barnola et al. 1983). The analytical system, except for the stainless steel container in which the <span class="hlt">ice</span> was crushed, was calibrated for each <span class="hlt">ice</span> sample measurement with a standard mixture of <span class="hlt">CO</span><span class="hlt">2</span> in nitrogen and oxygen. For further details on the experimental procedures and the dating of the successive <span class="hlt">ice</span> layers at Vostok, see Barnola et al. (1987, 1991), Lorius et al. (1985), and Petit et al. (1999).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9319M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9319M"><span><span class="hlt">CO</span><span class="hlt">2</span> and heat <span class="hlt">fluxes</span> in a recently clear-cut spruce forest in European Russia: experimental and modeling studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mamkin, Vadim; Kurbatova, Julia; Avilov, Vitaly; Mukhartova, Yulia; Krupenko, Alexander; Ivanov, Dmitry; Levashova, Natalia; Olchev, Alexander</p> <p>2017-04-01</p> <p>Ecosystem carbon dioxide, energy, and water <span class="hlt">fluxes</span> were measured using eddy covariance and portable chambers in a fresh clear-cut surrounded by a mixed spruce-birch-aspen forest in the boreal zone of European Russia. Measurements were initiated in spring 2016 following timber harvest and continued for seven months until the end of October. The influence of surrounding forest on <span class="hlt">air</span> flow and turbulent <span class="hlt">fluxes</span> within the clear-cut were examined using a process-based two-dimensional (<span class="hlt">2</span>D) hydrodynamic turbulent exchange model. Clear-cut was a permanent source of <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere. During the period the mean daily latent (LE) and sensible (H) heat <span class="hlt">fluxes</span> were very similar and the Bowen ratio (β=H/LE) averaged about 1.0. During the late spring and summer months the net ecosystem exchange of <span class="hlt">CO</span><span class="hlt">2</span> (NEE) remained slightly positive following onset of vegetation growth, while β was changing in the range from 0.6 to 4.0. There was strong diurnal variability in NEE, LE and H over the measurement period that was governed by solar radiation and temperature as well as the leaf area index (LAI) of regrown vegetation. Modeled vertical <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">fluxes</span> along a transect that crossed the clear-cut and coincided with the dominate wind direction showed that the clear-cut strongly influenced turbulent <span class="hlt">fluxes</span> within the atmospheric surface layer. Furthermore, modeled atmospheric dynamics suggested that the clear-cut had a large influence on turbulent <span class="hlt">fluxes</span> in the downwind forest, but little impact on the upwind side. An aggregated approach including field measurements and process-based models can be used to estimate energy, water and carbon dioxide <span class="hlt">fluxes</span> in non-uniform forest landscapes. This study was supported by a grant from the Russian Science Foundation (14-14-00956).</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1616784M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1616784M"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Monitoring at the Level of Field Agroecosystem in Moscow Region of Russia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meshalkina, Joulia; Mazirov, Ilya; Samardzic, Miljan; Yaroslavtsev, Alexis; Valentini, Riccardo; Vasenev, Ivan</p> <p>2014-05-01</p> <p>The Central Russia is still one of the less GHG-investigated European areas especially in case of agroecosystem-level carbon dioxide <span class="hlt">fluxes</span> monitoring by eddy covariance method. The eddy covariance technique is a statistical method to measure and calculate vertical turbulent <span class="hlt">fluxes</span> within atmospheric boundary layers. The major assumption of the metod is that measurements at a point can represent an entire upwind area. Eddy covariance researches, which could be considered as repeated for the same area, are very rare. The research has been carried out on the Precision Farming Experimental Field of the Russian Timiryazev State Agricultural University (Moscow, Russia) in 2013 under the support of RF Government grant No. 11.G34.31.0079. Arable derno-podzoluvisls have around 1 The results have shown high daily and seasonal dynamic of agroecosystem <span class="hlt">CO</span><span class="hlt">2</span> emission. Sowing activates soil microbiological activity and the average soil <span class="hlt">CO</span><span class="hlt">2</span> emission and adsorption are rising at the same time. <span class="hlt">CO</span><span class="hlt">2</span> streams are intensified after crop emerging from values of 3 to 7 μmol/s-m<span class="hlt">2</span> for emission, and from values of 5 to 20 μmol/s-m<span class="hlt">2</span> for adsorption. Stabilization of the flow has come at achieving plants height of 10-12 cm. The vegetation period is characterized by high average soil <span class="hlt">CO</span><span class="hlt">2</span> emission and adsorption at the same time, but the adsorption is significantly higher. The resulted <span class="hlt">CO</span><span class="hlt">2</span> absorption during the day is approximately <span class="hlt">2</span>-5 times higher than emissions at night. For example, in mid-June, the absorption value was about 0.45 mol/m<span class="hlt">2</span> during the day-time, and the emission value was about 0.1 mol/m<span class="hlt">2</span> at night. After harvesting <span class="hlt">CO</span><span class="hlt">2</span> emission is becoming essentially higher than adsorption. Autumn and winter data are fluctuate around zero, but for some periods a small predominance of <span class="hlt">CO</span><span class="hlt">2</span> emissions over the absorption may be observed. The daily dynamics of <span class="hlt">CO</span><span class="hlt">2</span> emissions depends on the <span class="hlt">air</span> temperature with the correlation coefficient changes between 0.4 and 0.8. Crop stage, agrotechnological</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Icar..282..118K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Icar..282..118K"><span>Experimental investigation of insolation-driven dust ejection from Mars' <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> caps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaufmann, E.; Hagermann, A.</p> <p>2017-01-01</p> <p>Mars' polar caps are - depending on hemisphere and season - partially or totally covered with <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. Icy surfaces such as the polar caps of Mars behave differently from surfaces covered with rock and soil when they are irradiated by solar light. The latter absorb and reflect incoming solar radiation within a thin layer beneath the surface. In contrast, <span class="hlt">ices</span> are partially transparent in the visible spectral range and opaque in the infrared. Due to this fact, the solar radiation can penetrate to a certain depth and raise the temperature of the <span class="hlt">ice</span> or dust below the surface. This may play an important role in the energy balance of icy surfaces in the solar system, as already noted in previous investigations. We investigated the temperature profiles inside <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> samples including a dust layer under Martian conditions. We have been able to trigger dust eruptions, but also demonstrated that these require a very narrow range of temperature and ambient pressure. We discuss possible implications for the understanding of phenomena such as arachneiform patterns or fan shaped deposits as observed in Mars' southern polar region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710530G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710530G"><span>Potentials and challenges associated with automated closed dynamic chamber measurements of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Görres, Carolyn-Monika; Kammann, Claudia; Ceulemans, Reinhart</p> <p>2015-04-01</p> <p>Soil respiration <span class="hlt">fluxes</span> are influenced by natural factors such as climate and soil type, but also by anthropogenic activities in managed ecosystems. As a result, soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> show a large intra- and interannual as well as intra- and intersite variability. Most of the available soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> data giving insights into this variability have been measured with manually closed static chambers, but technological advances in the past 15 years have also led to an increased use of automated closed chamber systems. The great advantage of automated chambers in comparison to manually operated chambers is the higher temporal resolution of the <span class="hlt">flux</span> data. This is especially important if we want to better understand the effects of short-term events, e.g. fertilization or heavy rainfall, on soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> variability. However, the chamber method is an invasive measurement method which can potentially alter soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and lead to biased measurement results. In the peer-reviewed literature, many papers compare the field performance and results of different closed static chamber designs, or compare manual chambers with automated chamber systems, to identify potential biases in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements, and thus help to reduce uncertainties in the <span class="hlt">flux</span> data. However, inter-comparisons of different automated closed dynamic chamber systems are still lacking. Here we are going to present a field comparison of the most-cited automated chamber system, the LI-8100A Automated Soil <span class="hlt">Flux</span> System, with the also commercially available Greenhouse Gas Monitoring System AGPS. Both measurement systems were installed side by side at a recently harvested poplar bioenergy plantation (POPFULL, http://uahost.uantwerpen.be/popfull/) from April 2014 until August 2014. The plantation provided optimal comparison conditions with a bare field situation after the harvest and a regrowing canopy resulting in a broad variety of microclimates. Furthermore, the plantation was planted in a double-row system with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22390636-iceveto-extended-pev-neutrino-astronomy-southern-hemisphere-icecube','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22390636-iceveto-extended-pev-neutrino-astronomy-southern-hemisphere-icecube"><span><span class="hlt">Ice</span>Veto: Extended PeV neutrino astronomy in the Southern Hemisphere with <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Auffenberg, Jan; Collaboration: IceCube Collaboration</p> <p></p> <p><span class="hlt">Ice</span>Cube, the world's largest high-energy neutrino observatory, built at the South Pole, recently reported evidence of an astrophysical neutrino <span class="hlt">flux</span> extending to PeV energies in the Southern Hemisphere. This observation raises the question of how the sensitivity in this energy range could be further increased. In the down-going sector, in <span class="hlt">Ice</span>Cube's case the Southern Hemisphere, backgrounds from atmospheric muons and neutrinos pose a challenge to the identification of an astrophysical neutrino <span class="hlt">flux</span>. The <span class="hlt">Ice</span>Cube analysis, that led to the evidence for astrophysical neutrinos, is based on an in-<span class="hlt">ice</span> veto strategy for background rejection. One possibility available to <span class="hlt">Ice</span>Cube is themore » concept of an extended surface detector, <span class="hlt">Ice</span>Veto, which could allow the rejection of a large fraction of atmospheric backgrounds, primarily for muons from cosmic ray (CR) <span class="hlt">air</span> showers as well as from neutrinos in the same <span class="hlt">air</span> showers. Building on the experience of <span class="hlt">IceTop/Ice</span>Cube, possibly the most cost-effective and sensitive way to build <span class="hlt">Ice</span>Veto is as an extension of the <span class="hlt">Ice</span>Top detector, with simple photomultiplier based detector modules for CR <span class="hlt">air</span> shower detection. Initial simulations and estimates indicate that such a veto detector will significantly increase the sensitivity to an astrophysical <span class="hlt">flux</span> of ν{sub μ} induced muon tracks in the Southern Hemisphere compared to current analyses. Here we present the motivation and capabilities based on initial simulations. Conceptual ideas for a simplified surface array will be discussed briefly.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013NatGe...6..457Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013NatGe...6..457Z"><span>Millennial-scale changes in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> levels linked to the Southern Ocean carbon isotope gradient and dust <span class="hlt">flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ziegler, Martin; Diz, Paula; Hall, Ian R.; Zahn, Rainer</p> <p>2013-06-01</p> <p>The rise in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations observed at the end of glacial periods has, at least in part, been attributed to the upwelling of carbon-rich deep water in the Southern Ocean. The magnitude of outgassing of dissolved <span class="hlt">CO</span><span class="hlt">2</span>, however, is influenced by the biological fixation of upwelled inorganic carbon and its transfer back to the deep sea as organic carbon. The efficiency of this biological pump is controlled by the extent of nutrient utilization, which can be stimulated by the delivery of iron by atmospheric dust particles. Changes in nutrient utilization should be reflected in the δ13C gradient between intermediate and deep waters. Here we use the δ13C values of intermediate- and bottom-dwelling foraminifera to reconstruct the carbon isotope gradient between thermocline and abyssal water in the subantarctic zone of the South Atlantic Ocean over the past 360,000 years. We find millennial-scale oscillations of the carbon isotope gradient that correspond to changes in dust <span class="hlt">flux</span> and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations as reported from Antarctic <span class="hlt">ice</span> cores. We interpret this correlation as a relationship between the efficiency of the biological pump and fertilization by dust-borne iron. As the correlation is exponential, we suggest that the sensitivity of the biological pump to dust-borne iron fertilization may be increased when the background dust <span class="hlt">flux</span> is low.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51M..01A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51M..01A"><span>North American <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> for 2007-2015 from NOAA's CarbonTracker-Lagrange Regional Inverse Modeling Framework</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrews, A. E.; Hu, L.; Thoning, K. W.; Nehrkorn, T.; Mountain, M. E.; Jacobson, A. R.; Michalak, A.; Dlugokencky, E. J.; Sweeney, C.; Worthy, D. E. J.; Miller, J. B.; Fischer, M. L.; Biraud, S.; van der Velde, I. R.; Basu, S.; Tans, P. P.</p> <p>2017-12-01</p> <p>CarbonTracker-Lagrange (CT-L) is a new high-resolution regional inverse modeling system for improved estimation of North American <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. CT-L uses footprints from the Stochastic Time-Inverted Lagrangian Transport (STILT) model driven by high-resolution (10 to 30 km) meteorological fields from the Weather Research and Forecasting (WRF) model. We performed a suite of synthetic-data experiments to evaluate a variety of inversion configurations, including (1) solving for scaling factors to an a priori <span class="hlt">flux</span> versus additive corrections, (<span class="hlt">2</span>) solving for <span class="hlt">fluxes</span> at 3-hrly resolution versus at coarser temporal resolution, (3) solving for <span class="hlt">fluxes</span> at 1o × 1o resolution versus at large eco-regional scales. Our framework explicitly and objectively solves for the optimal solution with a full error covariance matrix with maximum likelihood estimation, thereby enabling rigorous uncertainty estimates for the derived <span class="hlt">fluxes</span>. In the synthetic-data inversions, we find that solving for weekly scaling factors of a priori Net Ecosystem Exchange (NEE) at 1o × 1o resolution with optimization of diurnal cycles of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> yields faithful retrieval of the specified "true" <span class="hlt">fluxes</span> as those solved at 3-hrly resolution. In contrast, a scheme that does not allow for optimization of diurnal cycles of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> suffered from larger aggregation errors. We then applied the optimal inversion setup to estimate North American <span class="hlt">fluxes</span> for 2007-2015 using real atmospheric <span class="hlt">CO</span><span class="hlt">2</span> observations, multiple prior estimates of NEE, and multiple boundary values estimated from the NOAA's global Eulerian CarbonTracker (CarbonTracker) and from an empirical approach. Our derived North American land <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> show larger seasonal amplitude than those estimated from the CarbonTracker, removing seasonal biases in the CarbonTracker's simulated <span class="hlt">CO</span><span class="hlt">2</span> mole fractions. Independent evaluations using in-situ <span class="hlt">CO</span><span class="hlt">2</span> eddy covariance <span class="hlt">flux</span> measurements and independent aircraft profiles also suggest an improved estimation on North</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.3907W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.3907W"><span>Fram Strait: Atmospheric Forcing of The Sea <span class="hlt">Ice</span> <span class="hlt">Flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Widell, K.; Østerhus, S.; Gammelsrød, T.</p> <p></p> <p>Measuring the magnitude and variability of the <span class="hlt">ice</span> and freshwater <span class="hlt">flux</span> through Fram Strait is an important element in understanding climate variability in the Arctic. Since the major part of the <span class="hlt">ice</span> and freshwater that leaves the Arctic passes through Fram Strait, this passage can be considered a key area for estimating the net <span class="hlt">ice</span> production in the Arctic Ocean. In 1990, the Norwegian Polar Institute (NPI) started a monitoring program in the strait, most years by means of two moorings with Upward Looking Sonars (ULS) measuring <span class="hlt">ice</span> draft. From 1995 and on, these moorings were also equipped with Doppler Current Meters (DCM) to measure the <span class="hlt">ice</span> velocity. These measurements give an opportunity to investigate the different forces affecting <span class="hlt">ice</span> motion in the strait. Maximum correlation coefficient between atmospheric sea level pressure (from NCEP/NCAR reanalysed data) and southward <span class="hlt">ice</span> velocity is found when using the cross strait pressure difference along 80N between 10W and 5E (R = 0.72) consider- ing monthly means. Subtracting current velocity at 50 m depth (also measured by the DCM) from <span class="hlt">ice</span> velocity improves the correlation to R = 0.84. This gives insight in the relative importance of current and wind on the <span class="hlt">ice</span> motion, and indicates that pressure data can be used to make fairly good estimates of the <span class="hlt">ice</span> velocity in the strait. In combination with data on <span class="hlt">ice</span> thickness and <span class="hlt">ice</span> stream width, this result is used to calculate the <span class="hlt">ice</span> volume transport. By making assumptions on the parameters in- volved, the time series is extended back to 1948, the start of the pressure record. This time series will be presented and compared to literature, and annual and seasonal vari- ation of the <span class="hlt">ice</span> <span class="hlt">flux</span> will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUSM.U32A..01G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUSM.U32A..01G"><span>Measurement of Urban <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and water</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grimmond, S.; Crawford, B.; Offerle, B.; Hom, J.</p> <p>2006-05-01</p> <p>Measurements of surface-atmosphere <span class="hlt">fluxes</span> of carbon dioxide (FCO<span class="hlt">2</span>) and latent heat in urban environments are rare even though cities are a major source of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and users of water. In this paper, an overview of urban FCO<span class="hlt">2</span> measurements will be presented to illustrate how and where such measurements are being conducted and emerging results to date. Most of these studies have been conducted over short periods of time; few studies have considered annual sources/sinks. More investigations have been conducted, and are planned, in European cities than elsewhere, most commonly in areas of medium density urban development. The most dense urban sites are significant net sources of carbon. However, in areas where there is large amounts of vegetation present, there is a net sink of carbon during the summertime. In the second part of the presentation, more detailed attention will be directed to an ongoing measurement program in Baltimore, MD (part of the Baltimore Ecosystem Study). Eddy covariance instrumentation mounted on a tall-tower at 41.<span class="hlt">2</span> m has continuously measured local-scale <span class="hlt">fluxes</span> of carbon dioxide from a suburban environment since 2001. Several features make this particular study unique: 1) for an urban area, the study site is extensively vegetated, <span class="hlt">2</span>) the period of record (2001-2005) is among the longest available for urban FCO<span class="hlt">2</span> measurements, 3) both closed-path and open-path infrared gas analyzers are used for observations, and 4) several unique data quality control and gap-filling methods have been developed for use in an urban environment. Additionally, detailed surface datasets and GIS software are used to perform <span class="hlt">flux</span> source area analysis. Results from Baltimore indicate that FCO<span class="hlt">2</span> is very dependent on source area land-cover characteristics, particularly the proportion of vegetated and built surfaces. Over the course of a year, the urban surface is a strong net source of <span class="hlt">CO</span><span class="hlt">2</span>, though there is considerable inter-annual variability depending on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1917180Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1917180Q"><span>Land use and rainfall effect on soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in a Mediterranean agroforestry system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Quijano, Laura; Álvaro-Fuentes, Jorge; Lizaga, Iván; Navas, Ana</p> <p>2017-04-01</p> <p>Soils are the largest C reservoir of terrestrial ecosystems and play an important role in regulating the concentration of <span class="hlt">CO</span><span class="hlt">2</span> in the atmosphere. The exchange of <span class="hlt">CO</span><span class="hlt">2</span> between the atmosphere and soil controls the balance of C in soils. The <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> may be influenced by climate conditions and land use and cover change especially in the upper soil organic layer. Understanding C dynamics is important for maintaining C stocks to sustain and improve soil quality and to enhance sink C capacity of soils. This study focuses on the response of the <span class="hlt">CO</span><span class="hlt">2</span> emitted to rainfall events from different land uses (i.e. forest, abandoned cultivated soils and winter cereal cultivated soils) in a representative Mediterranean agroforestry ecosystem in the central part of the Ebro basin, NE Spain (30T 4698723N 646424E). A total of 30 measurement points with the same soil type (classified as Calcisols) were selected. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was measured in situ using a portable EGM-4 <span class="hlt">CO</span><span class="hlt">2</span> analyzer PPSystems connected to a dynamic chamber system (model CFX-1, PPSystems) weekly during autumn 2016. Eleven different rainfall events were measured at least 24 hours before (n=7) and after the rainfall event (n=4). Soil water content and temperature were measured at each sampling point within the first 5 cm. Soil samples were taken at the beginning of the experiment to determine soil organic carbon (SOC) content using a LECO RC-612. The mean SOC for forest, abandoned and cultivated soils were <span class="hlt">2</span>.5, <span class="hlt">2</span>.7 and 0.6 %, respectively. The results indicated differences in soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> between land uses. The field measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> show that before cereal sowing the highest values were recorded in the abandoned soils varying from 56.1 to 171.9 mg <span class="hlt">CO</span><span class="hlt">2</span>-C m-<span class="hlt">2</span> h-1 whereas after cereal sowing the highest values were recorded in cultivated soils ranged between 37.8 and 116.<span class="hlt">2</span> mg <span class="hlt">CO</span><span class="hlt">2</span>-C m-<span class="hlt">2</span> h-1 indicating the agricultural impact on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. In cultivated soils, lower mean <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were measured after direct seeding</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013DPS....4540005G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013DPS....4540005G"><span>The Radiolytic Destruction of Glycine Diluted in H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span>: Implications for Mars and Other Planetary Environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gerakines, Perry A.; Hudson, R. L.</p> <p>2013-10-01</p> <p>Future missions to Mars and other planetary surfaces will probe under the surfaces of these worlds for signs of organic chemistry. In previous studies we have shown that glycine and other amino acids have radiolytic destruction rates that depend on temperature and on dilution within an H<span class="hlt">2</span>O <span class="hlt">ice</span> matrix (Gerakines et al., 2012; Gerakines and Hudson 2013). In the new work presented here, we have examined the destruction of glycine diluted in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> at various concentrations and irradiated with protons at 0.8 MeV, typical of cosmic rays and solar energetic particles. Destruction rates for glycine were measured by infrared spectroscopy in situ, without removing or warming the <span class="hlt">ice</span> samples. New results on the half life of glycine in solid <span class="hlt">CO</span><span class="hlt">2</span> will be compared to those found in H<span class="hlt">2</span>O <span class="hlt">ice</span> matrices. The survivability of glycine in icy planetary surfaces rich in H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> will be discussed, and the implications for planetary science missions will be considered. References: Gerakines, P. A., Hudson, R. L., Moore, M. H., and Bell, J-L. (2012). In-situ Measurements of the Radiation Stability of Amino Acids at 15 - 140 K. Icarus, 220, 647-659. Gerakines, P. A. and Hudson, R. L. (2013). Glycine's Radiolytic Destruction in <span class="hlt">Ices</span>: First in situ Laboratory Measurements for Mars. Astrobiology, 13, 647-655.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=340834&Lab=NHEERL&keyword=Change+AND+climate&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=340834&Lab=NHEERL&keyword=Change+AND+climate&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>Nitrous oxide <span class="hlt">flux</span> under changing temperature and <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>We are investigating nitrous oxide <span class="hlt">flux</span> seasonal trends and response to temperature and <span class="hlt">CO</span><span class="hlt">2</span> increases in a boreal peatland. Peatlands located in boreal regions make up a third of global wetland area and are expected to have the highest temperature increases in response to climat...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCD.....6..505F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCD.....6..505F"><span>Quantification of ikaite in Antarctic sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, M.; Thomas, D. N.; Krell, A.; Nehrke, G.; Göttlicher, J.; Norman, L.; Riaux-Gobin, C.; Dieckmann, G. S.</p> <p>2012-02-01</p> <p>Calcium carbonate precipitation in sea <span class="hlt">ice</span> can increase p<span class="hlt">CO</span><span class="hlt">2</span> during precipitation in winter and decrease p<span class="hlt">CO</span><span class="hlt">2</span> during dissolution in spring. Ca<span class="hlt">CO</span>3 precipitation in sea <span class="hlt">ice</span> is thought to potentially drive significant <span class="hlt">CO</span><span class="hlt">2</span> uptake by the ocean. However, little is known about the quantitative spatial and temporal distribution of Ca<span class="hlt">CO</span>3 within sea <span class="hlt">ice</span>. This is the first quantitative study of hydrous calcium carbonate, as ikaite, in sea <span class="hlt">ice</span> and discusses its potential significance for the carbon cycle in polar oceans. <span class="hlt">Ice</span> cores and brine samples were collected from pack and land fast sea <span class="hlt">ice</span> between September and December 2007 during an expedition in the East Antarctic and another off Terre Adélie, Antarctica. Samples were analysed for Ca<span class="hlt">CO</span>3, Salinity, DOC, DON, Phosphate, and total alkalinity. A relationship between the measured parameters and Ca<span class="hlt">CO</span>3 precipitation could not be observed. We found calcium carbonate, as ikaite, mostly in the top layer of sea <span class="hlt">ice</span> with values up to 126 mg ikaite per liter melted sea <span class="hlt">ice</span>. This potentially represents a contribution between 0.12 and 9 Tg C to the annual carbon <span class="hlt">flux</span> in polar oceans. The horizontal distribution of ikaite in sea <span class="hlt">ice</span> was heterogenous. We also found the precipitate in the snow on top of the sea <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.B31H..08S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.B31H..08S"><span><span class="hlt">CO</span><span class="hlt">2</span>, CH4, and DOC <span class="hlt">Flux</span> During Long Term Thaw of High Arctic Tundra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stackhouse, B. T.; Vishnivetskaya, T. A.; Layton, A.; Bennett, P.; Mykytczuk, N.; Lau, C. M.; Whyte, L.; Onstott, T. C.</p> <p>2013-12-01</p> <p>Arctic regions are expected to experience temperature increases of >4° C by the end of this century. This warming is projected to cause a drastic reduction in the extent of permafrost at high northern latitudes, affecting an estimated 1000 Pg of SOC in the top 3 m. Determining the effects of this temperature change on <span class="hlt">CO</span><span class="hlt">2</span> and CH4 emissions is critical for defining source constraints to global climate models. To investigate this problem, 18 cores of 1 m length were collected in late spring 2011 before the thawing of the seasonal active layer from an <span class="hlt">ice</span>-wedge polygon near the McGill Arctic Research Station (MARS) on Axel Heiberg Island, Nunavut, Canada (N79°24, W90°45). Cores were collected from acidic soil (pH 5.5) with low SOC (~1%), summertime active layer depth between 40-70 cm (2010-2013), and sparse vegetation consisting primarily of small shrubs and sedges. Cores were progressively thawed from the surface over the course of 14 weeks to a final temperature of 4.5° C and held at that temperature for 15 months under the following conditions: in situ water saturation conditions versus fully water saturated conditions using artificial rain fall, surface light versus no surface light, cores from the polygon edge, and control cores with a permafrost table maintained at 70 cm depth. Core headspaces were measured weekly for <span class="hlt">CO</span><span class="hlt">2</span>, CH4, H<span class="hlt">2</span>, <span class="hlt">CO</span>, and O<span class="hlt">2</span> <span class="hlt">flux</span> during the 18 month thaw experiment. After ~20 weeks of thawing maximum, <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the polygon edge and dark treatment cores were 3.0×0.7 and 1.7×0.4 mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> hr-1, respectively. The <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the control, saturated, and in situ saturation cores reached maximums of 0.6×0.<span class="hlt">2</span>, 0.9×0.5, and 0.9×0.1 mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> hr-1, respectively. Field measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from an adjacent polygon during the mid-summer of 2011 to 2013 ranged from 0.3 to 3.7 mmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> hr-1. Cores from all treatments except water saturated were found to consistently oxidize CH4 at ~atmospheric concentrations (<span class="hlt">2</span> ppmv) with a maximum</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1306691-direct-capture-co2-from-ambient-air','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1306691-direct-capture-co2-from-ambient-air"><span>Direct capture of <span class="hlt">CO</span> <span class="hlt">2</span> from ambient <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sanz-Perez, Eloy S.; Murdock, Christopher R.; Didas, Stephanie A.</p> <p></p> <p>The increase in the global atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration resulting from over a century of combustion of fossil fuels has been associated with significant global climate change. With the global population increase driving continued increases in fossil fuel use, humanity’s primary reliance on fossil energy for the next several decades is assured. Traditional modes of carbon capture such as precombustion and postcombustion <span class="hlt">CO</span> <span class="hlt">2</span> capture from large point sources can help slow the rate of increase of the atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration, but only the direct removal of <span class="hlt">CO</span> <span class="hlt">2</span> from the <span class="hlt">air</span>, or “direct <span class="hlt">air</span> capture” (DAC), can actuallymore » reduce the global atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration. The past decade has seen a steep rise in the use of chemical sorbents that are cycled through sorption and desorption cycles for <span class="hlt">CO</span> <span class="hlt">2</span> removal from ultradilute gases such as <span class="hlt">air</span>. This Review provides a historical overview of the field of DAC, along with an exhaustive description of the use of chemical sorbents targeted at this application. Solvents and solid sorbents that interact strongly with <span class="hlt">CO</span> <span class="hlt">2</span> are described, including basic solvents, supported amine and ammonium materials, and metal-organic frameworks (MOFs), as the primary classes of chemical sorbents. Hypothetical processes for the deployment of such sorbents are discussed, as well as the limited array of technoeconomic analyses published on DAC. Overall, it is concluded that there are many new materials that could play a role in emerging DAC technologies. Furthermore, these materials need to be further investigated and developed with a practical sorbent-<span class="hlt">air</span> contacting process in mind if society is to make rapid progress in deploying DAC as a means of mitigating climate change.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1306691-direct-capture-co2-from-ambient-air','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1306691-direct-capture-co2-from-ambient-air"><span>Direct capture of <span class="hlt">CO</span> <span class="hlt">2</span> from ambient <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sanz-Perez, Eloy S.; Murdock, Christopher R.; Didas, Stephanie A.; ...</p> <p>2016-08-25</p> <p>The increase in the global atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration resulting from over a century of combustion of fossil fuels has been associated with significant global climate change. With the global population increase driving continued increases in fossil fuel use, humanity’s primary reliance on fossil energy for the next several decades is assured. Traditional modes of carbon capture such as precombustion and postcombustion <span class="hlt">CO</span> <span class="hlt">2</span> capture from large point sources can help slow the rate of increase of the atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration, but only the direct removal of <span class="hlt">CO</span> <span class="hlt">2</span> from the <span class="hlt">air</span>, or “direct <span class="hlt">air</span> capture” (DAC), can actuallymore » reduce the global atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration. The past decade has seen a steep rise in the use of chemical sorbents that are cycled through sorption and desorption cycles for <span class="hlt">CO</span> <span class="hlt">2</span> removal from ultradilute gases such as <span class="hlt">air</span>. This Review provides a historical overview of the field of DAC, along with an exhaustive description of the use of chemical sorbents targeted at this application. Solvents and solid sorbents that interact strongly with <span class="hlt">CO</span> <span class="hlt">2</span> are described, including basic solvents, supported amine and ammonium materials, and metal-organic frameworks (MOFs), as the primary classes of chemical sorbents. Hypothetical processes for the deployment of such sorbents are discussed, as well as the limited array of technoeconomic analyses published on DAC. Overall, it is concluded that there are many new materials that could play a role in emerging DAC technologies. Furthermore, these materials need to be further investigated and developed with a practical sorbent-<span class="hlt">air</span> contacting process in mind if society is to make rapid progress in deploying DAC as a means of mitigating climate change.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/43522','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/43522"><span>High-frequency pressure variations in the vicinity of a surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> chamber</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Eugene S. Takle; James R. Brandle; R. A. Schmidt; Rick Garcia; Irina V. Litvina; William J. Massman; Xinhua Zhou; Geoffrey Doyle; Charles W. Rice</p> <p>2003-01-01</p> <p>We report measurements of <span class="hlt">2</span>Hz pressure fluctuations at and below the soil surface in the vicinity of a surface-based <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> chamber. These measurements were part of a field experiment to examine the possible role of pressure pumping due to atmospheric pressure fluctuations on measurements of surface <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>. Under the moderate wind speeds, warm temperatures,...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4822021A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4822021A"><span>Modeling <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">ice</span> clouds with a Mars Global Climate Model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Audouard, Joachim; Määttänen, Anni; Listowski, Constantino; Millour, Ehouarn; Forget, Francois; Spiga, Aymeric</p> <p>2016-10-01</p> <p>Since the first claimed detection of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds by the Mariner campaign (Herr and Pimentel, 1970), more recent observations and modelling works have put new constraints concerning their altitude, region, time and mechanisms of formation (Clancy and Sandor, 1998; Montmessin et al., 2007; Colaprete et al., 2008; Määttänen et al., 2010; Vincendon et al., 2011; Spiga et al. 2012; Listowski et al. 2014). <span class="hlt">CO</span><span class="hlt">2</span> clouds are observed at the poles at low altitudes (< 20 km) during the winter and at high altitudes (60-110 km) in the equatorial regions during the first half of the year. However, Martian <span class="hlt">CO</span><span class="hlt">2</span> clouds's variability and dynamics remain somehow elusive.Towards an understanding of Martian <span class="hlt">CO</span><span class="hlt">2</span> clouds and especially of their precise radiative impact on the climate throughout the history of the planet, including their formation and evolution in a Global Climate Model (GCM) is necessary.Adapting the <span class="hlt">CO</span><span class="hlt">2</span> clouds microphysics modeling work of Listowski et al. (2013; 2014), we aim at implementing a complete <span class="hlt">CO</span><span class="hlt">2</span> clouds scheme in the GCM of the Laboratoire de Météorologie Dynamique (LMD, Forget et al., 1999). It covers <span class="hlt">CO</span><span class="hlt">2</span> microphysics, growth, evolution and dynamics with a methodology inspired from the water <span class="hlt">ice</span> clouds scheme recently included in the LMD GCM (Navarro et al., 2014).Two main factors control the formation and evolution of <span class="hlt">CO</span><span class="hlt">2</span> clouds in the Martian atmosphere: sufficient supersaturation of <span class="hlt">CO</span><span class="hlt">2</span> is needed and condensation nuclei must be available. Topography-induced gravity-waves (GW) are expected to propagate to the upper atmosphere where they produce cold pockets of supersaturated <span class="hlt">CO</span><span class="hlt">2</span> (Spiga et al., 2012), thus allowing the formation of clouds provided enough condensation nuclei are present. Such supersaturations have been observed by various instruments, in situ (Schofield et al., 1997) and from orbit (Montmessin et al., 2006, 2011; Forget et al., 2009).Using a GW-induced temperature profile and the 1-D version of the GCM, we simulate the formation of <span class="hlt">CO</span><span class="hlt">2</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915402S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915402S"><span>Results from twelve years of continuous monitoring of the soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at the Ketzin <span class="hlt">CO</span><span class="hlt">2</span> storage pilot site, Germany</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Szizybalski, Alexandra; Zimmer, Martin; Pilz, Peter; Liebscher, Axel</p> <p>2017-04-01</p> <p>Under the coordination of the GFZ German Research Centre for Geosciences the complete life-cycle of a geological storage site for <span class="hlt">CO</span><span class="hlt">2</span> has been investigated and studied in detail over the past 12 years at Ketzin near Berlin, Germany. The test site is located at the southern flank of an anticlinal structure. Beginning with an exploration phase in 2004, drilling of the first three wells took place in 2007. From June 2008 to August 2013 about 67 kt of <span class="hlt">CO</span><span class="hlt">2</span> were injected into Upper Triassic sandstones at a depth of 630 to 650 m overlain by more than 165 m of shaley cap rocks. A comprehensive operational and scientific monitoring program forms the central part of the Ketzin project targeting at the reservoir itself, its overburden or above-zone and the surface. The surface monitoring is done by continuous soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements. These already started in 2005, more than three years prior to the injection phase using a survey chamber from LI-COR Inc. Twenty sampling locations were selected in the area of the anticline covering about 3 x 3 km. In order to obtain information on seasonal trends, measurements are performed at least once a month. The data set obtained prior to the injection serves as a basis for comparison with all further measurements during the injection and storage operations [Zimmer et al., 2010]. To refine the monitoring network, eight automatic, permanent soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> stations were additionally installed in 2011 in the direct vicinity of the boreholes. Using this system, the <span class="hlt">CO</span><span class="hlt">2</span> soil <span class="hlt">flux</span> is measured on an hourly basis. Over the whole monitoring time, soil temperature and moisture are recorded simultaneously and soil samples down to 70 cm depth were studied for their structure, carbon and nitrogen content. ver the whole monitoring time. Both, diurnal and seasonal <span class="hlt">flux</span> variations can be detected and hence, provide a basis for interpretation of the measured data. Detailed analysis of the long-term monitoring at each station clearly reveals the influence</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25258295','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25258295"><span>Polygonal tundra geomorphological change in response to warming alters future <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> on the Barrow Peninsula.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lara, Mark J; McGuire, A David; Euskirchen, Eugenie S; Tweedie, Craig E; Hinkel, Kenneth M; Skurikhin, Alexei N; Romanovsky, Vladimir E; Grosse, Guido; Bolton, W Robert; Genet, Helene</p> <p>2015-04-01</p> <p>The landscape of the Barrow Peninsula in northern Alaska is thought to have formed over centuries to millennia, and is now dominated by <span class="hlt">ice</span>-wedge polygonal tundra that spans drained thaw-lake basins and interstitial tundra. In nearby tundra regions, studies have identified a rapid increase in thermokarst formation (i.e., pits) over recent decades in response to climate warming, facilitating changes in polygonal tundra geomorphology. We assessed the future impact of 100 years of tundra geomorphic change on peak growing season carbon exchange in response to: (i) landscape succession associated with the thaw-lake cycle; and (ii) low, moderate, and extreme scenarios of thermokarst pit formation (10%, 30%, and 50%) reported for Alaskan arctic tundra sites. We developed a 30 × 30 m resolution tundra geomorphology map (overall accuracy:75%; Kappa:0.69) for our ~1800 km² study area composed of ten classes; drained slope, high center polygon, flat-center polygon, low center polygon, coalescent low center polygon, polygon trough, meadow, ponds, rivers, and lakes, to determine their spatial distribution across the Barrow Peninsula. Land-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> data were collected for the summers of 2006-2010 at eighty-two sites near Barrow, across the mapped classes. The developed geomorphic map was used for the regional assessment of carbon <span class="hlt">flux</span>. Results indicate (i) at present during peak growing season on the Barrow Peninsula, <span class="hlt">CO</span><span class="hlt">2</span> uptake occurs at -902.3 10(6) gC-<span class="hlt">CO</span><span class="hlt">2</span> day(-1) (uncertainty using 95% CI is between -438.3 and -1366 10(6) gC-<span class="hlt">CO</span><span class="hlt">2</span> day(-1)) and CH4 <span class="hlt">flux</span> at 28.9 10(6) gC-CH4 day(-1) (uncertainty using 95% CI is between 12.9 and 44.9 10(6) gC-CH4 day(-1)), (ii) one century of future landscape change associated with the thaw-lake cycle only slightly alter <span class="hlt">CO</span><span class="hlt">2</span> and CH4 exchange, while (iii) moderate increases in thermokarst pits would strengthen both <span class="hlt">CO</span><span class="hlt">2</span> uptake (-166.9 10(6) gC-<span class="hlt">CO</span><span class="hlt">2</span> day(-1)) and CH4 <span class="hlt">flux</span> (<span class="hlt">2</span>.8 10(6) gC-CH4 day(-1)) with geomorphic change from low</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70192718','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70192718"><span>Polygonal tundra geomorphological change in response to warming alters future <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> on the Barrow Peninsula</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Lara, Mark J.; McGuire, A. David; Euskirchen, Eugénie S.; Tweedie, Craig E.; Hinkel, Kenneth M.; Skurikhin, Alexei N.; Romanovsky, Vladimir E.; Grosse, Guido; Bolton, W. Robert; Genet, Helene</p> <p>2015-01-01</p> <p>The landscape of the Barrow Peninsula in northern Alaska is thought to have formed over centuries to millennia, and is now dominated by <span class="hlt">ice</span>-wedge polygonal tundra that spans drained thaw-lake basins and interstitial tundra. In nearby tundra regions, studies have identified a rapid increase in thermokarst formation (i.e., pits) over recent decades in response to climate warming, facilitating changes in polygonal tundra geomorphology. We assessed the future impact of 100 years of tundra geomorphic change on peak growing season carbon exchange in response to: (i) landscape succession associated with the thaw-lake cycle; and (ii) low, moderate, and extreme scenarios of thermokarst pit formation (10%, 30%, and 50%) reported for Alaskan arctic tundra sites. We developed a 30 × 30 m resolution tundra geomorphology map (overall accuracy:75%; Kappa:0.69) for our ~1800 km² study area composed of ten classes; drained slope, high center polygon, flat-center polygon, low center polygon, coalescent low center polygon, polygon trough, meadow, ponds, rivers, and lakes, to determine their spatial distribution across the Barrow Peninsula. Land-atmosphere <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> data were collected for the summers of 2006–2010 at eighty-two sites near Barrow, across the mapped classes. The developed geomorphic map was used for the regional assessment of carbon <span class="hlt">flux</span>. Results indicate (i) at present during peak growing season on the Barrow Peninsula, <span class="hlt">CO</span><span class="hlt">2</span> uptake occurs at -902.3 106gC-<span class="hlt">CO</span><span class="hlt">2</span> day−1(uncertainty using 95% CI is between −438.3 and −1366 106gC-<span class="hlt">CO</span><span class="hlt">2</span> day−1) and CH4 <span class="hlt">flux</span> at 28.9 106gC-CH4 day−1(uncertainty using 95% CI is between 12.9 and 44.9 106gC-CH4 day−1), (ii) one century of future landscape change associated with the thaw-lake cycle only slightly alter <span class="hlt">CO</span><span class="hlt">2</span> and CH4 exchange, while (iii) moderate increases in thermokarst pits would strengthen both <span class="hlt">CO</span><span class="hlt">2</span>uptake (−166.9 106gC-<span class="hlt">CO</span><span class="hlt">2</span> day−1) and CH4 <span class="hlt">flux</span> (<span class="hlt">2</span>.8 106gC-CH4 day−1) with geomorphic change from</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1080961','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1080961"><span>Relationships between the Efficiencies of Photosystems I and II and Stromal Redox State in <span class="hlt">CO</span><span class="hlt">2</span>-Free <span class="hlt">Air</span> 1</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Harbinson, Jeremy; Foyer, Christine H.</p> <p>1991-01-01</p> <p>The responses of the efficiencies of photosystems I and II, stromal redox state (as indicated by NADP-malate dehydrogenase activation state), and activation of the Benson-Calvin cycle enzymes ribulose 1,5-bisphosphate carboxylase and fructose 1,6-bisphosphatase to varying irradiance were measured in pea (Pisum sativum L.) leaves operating close to the <span class="hlt">CO</span><span class="hlt">2</span> compensation point. A comparison of the relationships among these parameters obtained from leaves in <span class="hlt">air</span> was made with those obtained when the leaves were maintained in <span class="hlt">air</span> from which the <span class="hlt">CO</span><span class="hlt">2</span> had been removed. P700 was more oxidized at any measured irradiance in <span class="hlt">CO</span><span class="hlt">2</span>-free <span class="hlt">air</span> than in <span class="hlt">air</span>. The relationship between the quantum efficiencies of the photosystems in <span class="hlt">CO</span><span class="hlt">2</span>-free <span class="hlt">air</span> was distinctly curvilinear in contrast to the predominantly linear relationship obtained with leaves in <span class="hlt">air</span>. This nonlinearity may be consistent with the operation of cyclic electron flow around photosystem I because the quantum efficiency of photosystem II was much more restricted than the quantum efficiency of photosystem I. In <span class="hlt">CO</span><span class="hlt">2</span>-free <span class="hlt">air</span>, measured NADP-malate dehydrogenase activities varied considerably at low irradiances. However, at high irradiance the activity of the enzyme was low, implying that the stroma was oxidized. In contrast, fructose-1,6-bisphosphatase activities tended to increase with increasing electron <span class="hlt">flux</span> through the photosystems. Ribulose-1,5-bisphosphate carboxylase activity remained relatively constant with respect to irradiance in <span class="hlt">CO</span><span class="hlt">2</span>-free <span class="hlt">air</span>, with an activation state 50% of maximum. We conclude that, at the <span class="hlt">CO</span><span class="hlt">2</span> compensation point and high irradiance, low redox states are favored and that cyclic electron flow may be substantial. These two features may be the requirements necessary to trigger and maintain the dissipative processes in the thylakoid membrane. PMID:16668401</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3251141','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3251141"><span>Economic and energetic analysis of capturing <span class="hlt">CO</span><span class="hlt">2</span> from ambient <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>House, Kurt Zenz; Baclig, Antonio C.; Ranjan, Manya; van Nierop, Ernst A.; Wilcox, Jennifer; Herzog, Howard J.</p> <p>2011-01-01</p> <p>Capturing carbon dioxide from the atmosphere (“<span class="hlt">air</span> capture”) in an industrial process has been proposed as an option for stabilizing global <span class="hlt">CO</span><span class="hlt">2</span> concentrations. Published analyses suggest these <span class="hlt">air</span> capture systems may cost a few hundred dollars per tonne of <span class="hlt">CO</span><span class="hlt">2</span>, making it cost competitive with mainstream <span class="hlt">CO</span><span class="hlt">2</span> mitigation options like renewable energy, nuclear power, and carbon dioxide capture and storage from large <span class="hlt">CO</span><span class="hlt">2</span> emitting point sources. We investigate the thermodynamic efficiencies of commercial separation systems as well as trace gas removal systems to better understand and constrain the energy requirements and costs of these <span class="hlt">air</span> capture systems. Our empirical analyses of operating commercial processes suggest that the energetic and financial costs of capturing <span class="hlt">CO</span><span class="hlt">2</span> from the <span class="hlt">air</span> are likely to have been underestimated. Specifically, our analysis of existing gas separation systems suggests that, unless <span class="hlt">air</span> capture significantly outperforms these systems, it is likely to require more than 400 kJ of work per mole of <span class="hlt">CO</span><span class="hlt">2</span>, requiring it to be powered by <span class="hlt">CO</span><span class="hlt">2</span>-neutral power sources in order to be <span class="hlt">CO</span><span class="hlt">2</span> negative. We estimate that total system costs of an <span class="hlt">air</span> capture system will be on the order of $1,000 per tonne of <span class="hlt">CO</span><span class="hlt">2</span>, based on experience with as-built large-scale trace gas removal systems. PMID:22143760</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACP....13.7607C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACP....13.7607C"><span>Improved simulation of regional <span class="hlt">CO</span><span class="hlt">2</span> surface concentrations using GEOS-Chem and <span class="hlt">fluxes</span> from VEGAS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Z. H.; Zhu, J.; Zeng, N.</p> <p>2013-08-01</p> <p><span class="hlt">CO</span><span class="hlt">2</span> measurements have been combined with simulated <span class="hlt">CO</span><span class="hlt">2</span> distributions from a transport model in order to produce the optimal estimates of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> in inverse modeling. However, one persistent problem in using model-observation comparisons for this goal relates to the issue of compatibility. Observations at a single station reflect all underlying processes of various scales. These processes usually cannot be fully resolved by model simulations at the grid points nearest the station due to lack of spatial or temporal resolution or missing processes in the model. In this study the stations in one region were grouped based on the amplitude and phase of the seasonal cycle at each station. The regionally averaged <span class="hlt">CO</span><span class="hlt">2</span> at all stations in one region represents the regional <span class="hlt">CO</span><span class="hlt">2</span> concentration of this region. The regional <span class="hlt">CO</span><span class="hlt">2</span> concentrations from model simulations and observations were used to evaluate the regional model results. The difference of the regional <span class="hlt">CO</span><span class="hlt">2</span> concentration between observation and modeled results reflects the uncertainty of the large-scale <span class="hlt">flux</span> in the region where the grouped stations are. We compared the regional <span class="hlt">CO</span><span class="hlt">2</span> concentrations between model results with biospheric <span class="hlt">fluxes</span> from the Carnegie-Ames-Stanford Approach (CASA) and VEgetation-Global-Atmosphere-Soil (VEGAS) models, and used observations from GLOBALVIEW-<span class="hlt">CO</span><span class="hlt">2</span> to evaluate the regional model results. The results show the largest difference of the regionally averaged values between simulations with <span class="hlt">fluxes</span> from VEGAS and observations is less than 5 ppm for North American boreal, North American temperate, Eurasian boreal, Eurasian temperate and Europe, which is smaller than the largest difference between CASA simulations and observations (more than 5 ppm). There is still a large difference between two model results and observations for the regional <span class="hlt">CO</span><span class="hlt">2</span> concentration in the North Atlantic, Indian Ocean, and South Pacific tropics. The regionally averaged <span class="hlt">CO</span><span class="hlt">2</span> concentrations will be helpful for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.C23D..06F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.C23D..06F"><span>New <span class="hlt">ice</span> core records on the glacial/interglacial change in atmospheric δ13<span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, H.; Schmitt, J.; Schneider, R.; Elsig, J.; Lourantou, A.; Leuenberger, M.; Stocker, T. F.; Koehler, P.; Lavric, J.; Raynaud, D. P.; Chappellaz, J. A.</p> <p>2010-12-01</p> <p>The reconstruction of δ13<span class="hlt">CO</span><span class="hlt">2</span> using Antarctic <span class="hlt">ice</span> cores promises a deeper understanding on the causes of past atmospheric <span class="hlt">CO</span><span class="hlt">2</span> changes. Previous measurements on the Taylor Dome <span class="hlt">ice</span> core over the last 30,000 years (Smith et al., 1999) indicated marine processes to be dominating the significant δ13<span class="hlt">CO</span><span class="hlt">2</span> changes over the transition, whereas glacial δ13<span class="hlt">CO</span><span class="hlt">2</span> was only slightly depleted relative to the Holocene (Leuenberger et al., 1992; Smith et al., 1999). However, significant uncertainty and the low temporal resolution of the Taylor Dome δ13<span class="hlt">CO</span><span class="hlt">2</span> data prevented a more detailed interpretation. Recently, substantial improvements have been made in the analysis and the resolution of <span class="hlt">ice</span> core δ13<span class="hlt">CO</span><span class="hlt">2</span> records (Elsig et al., 2009; Lourantou et al., 2010). With these and new measurements presented here, three independent δ13<span class="hlt">CO</span><span class="hlt">2</span> data sets over the last glacial/interglacial transition have now been derived from the two EPICA and the Talos Dome <span class="hlt">ice</span> cores. Two of the methods use traditional dry extraction techniques with a reproducibility of 0.07-0.1‰. The third method uses a novel sublimation technique with a reproducibility of 0.05‰. Here we compare the data sets, their analytical setups and discuss their joint information as well as their differences. The three records provide a more detailed picture on the temporal evolution of δ13<span class="hlt">CO</span><span class="hlt">2</span> and confirm two pronounced isotope minima between 18-12,000 years BP in parallel to the two major phases of <span class="hlt">CO</span><span class="hlt">2</span> increase (Lourantou et al., 2010; Smith et al., 1999) as also reflected in marine sediments (Marchitto et al., 2007; Skinner et al., 2010). Accordingly, a release of old carbon from the deep ocean is most likely responsible for a large part of the long-term increase in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> in this time interval. However, the fast <span class="hlt">CO</span><span class="hlt">2</span> jumps at a round 12,000 and 14,000 years BP may be partly of terrestrial origin (Elsig, 2009; Köhler et al., 2010b). The new sublimation data set provides also unambiguous δ13<span class="hlt">CO</span><span class="hlt">2</span> data for clathrate <span class="hlt">ice</span> in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.2264C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.2264C"><span>METEOPOLE-<span class="hlt">FLUX</span>: an observatory of terrestrial water, energy, and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Toulouse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calvet, Jean-Christophe; Roujean, Jean-Louis; Zhang, Sibo; Maurel, William; Piguet, Bruno; Barrié, Joël; Bouhours, Gilles; Couzinier, Jacques; Garrouste, Olivier; Girres, Sandrine; Suquia, David; Tzanos, Diane</p> <p>2016-04-01</p> <p>The METEOPOLE-<span class="hlt">FLUX</span> project (http://www.cnrm.meteo.fr/spip.php?article874&lang=en) aims at monitoring a large suburban set-aside field in the city of Toulouse (43.572898 N, 1.374384 E). Since June 2012, these data contribute to the international effort to monitor terrestrial ecosystems (grasslands in particular), to the validation of land surface models, and to the near real time quality monitoring of operational weather forecast models. Various variables are monitored at a subhourly rate: wind speed, <span class="hlt">air</span> temperature, <span class="hlt">air</span> humidity, atmospheric pressure, precipitation, turbulent <span class="hlt">fluxes</span> (H, LE, <span class="hlt">CO</span><span class="hlt">2</span>), downwelling and upwelling solar and infrared radiation, downwelling and upwelling PAR, fraction of diffuse incoming PAR, presence of water intercepted by vegetation (rain, dew), soil moisture profile, soil temperature profile, surface albedo, transmissivity of PAR in vegetation canopy. Moreover, local observations are performed using remote sensing techniques: infrared radiometry, GNSS reflectometry, and multi-band surface reflectometry using an aerosol photometer from the AERONET network. Destructive measurements of LAI, green/brown above-ground biomass, and necromass are performed twice a year. This site is characterized by a large fraction of gravels and stones in the soil, ranging from 17% to 35% in the top soil layer (down to 0.6 m), and peaking at 81% at 0.7 m. The impact of gravels and stones on thermal and moisture <span class="hlt">fluxes</span> in the soil has not been much addressed in the past and is not represented in most land surface models. Their impact on the available water content for plant transpiration and plant growth is not much documented so far. The long term monitoring of this site will therefore improve the knowledge on land processes. The data will be used together with urban meteorological data to characterize the urban heat island. Finally, this site will be used for the CAL/VAL of various satellite products in conjunction with the SMOSMANIA soil moisture network</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013732','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013732"><span>Wave-<span class="hlt">Ice</span> and <span class="hlt">Air-Ice</span>-Ocean Interaction During the Chukchi Sea <span class="hlt">Ice</span> Edge Advance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Wave -<span class="hlt">Ice</span> and <span class="hlt">Air-Ice</span>-Ocean Interaction During the...Chukchi Sea in the late summer have potentially changed the impact of fall storms by creating wave fields in the vicinity of the advancing <span class="hlt">ice</span> edge. A...first) wave -<span class="hlt">ice</span> interaction field experiment that adequately documents the relationship of a growing pancake <span class="hlt">ice</span> cover with a time and space varying</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.C43B0498M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.C43B0498M"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> monitoring using Continuous Timeseries-Forced Diffusion (CT-FD): Development, Validation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McArthur, G. S.; Risk, D. A.; Nickerson, N. R.; Creelman, C. A.; Beltrami, H.</p> <p>2009-12-01</p> <p>Land-based <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements are a key indicator of the biological, chemical and physical processes occurring in the soil. While highly dense temporal <span class="hlt">flux</span> measurements can be acquired using Eddy Covariance towers, or <span class="hlt">flux</span> chambers, the challenge of gathering data that is rich both temporally and spatially persists. Over the past two years we have developed a new technique for measuring soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, called continuous timeseries-forced diffusion (CT-FD) attempts to satisfy the need for spatially and temporally rich data. The CT-FD probe consists of a Vaisala <span class="hlt">CO</span><span class="hlt">2</span> sensor, embodied in a PVC casing, with tear/UV resistant Tyvek membranes at both the inlet and outlet. The probe delivers continuous <span class="hlt">flux</span> data and can be inexpensively replicated across the landscape.The CT-FD technique works by forcing a known diffusive regime between the soil and the atmosphere, allowing the calculation of <span class="hlt">fluxes</span> across the soil/atmosphere boundary to be made from; the internal concentration of a CT-FD probe placed at the soil surface; and a common reference probe designed to capture the atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. For every concentration measurement, the difference between the probe and the reference concentration is indicative of a unique <span class="hlt">flux</span> value. Here we examine properties of the instrument and method, as documented by a long series of developmental studies involving numerical gas transport modeling, laboratory and field experiments. A suite of 1D and 3D modeling experiments were needed to optimize embodiment and geometries of the probe. These show that the probe should have a relatively long collar, with relatively high diffusivity made possible by having large, highly diffusive membranes, both of which help to induce 1D movement of gases into the probe and reduce the lateral diffusion around the probe. Modeling also shows that correction for lateral diffusion is feasible. As for error, sensor error transfers linearly to errors in the <span class="hlt">flux</span>, and that the sensor can be used in non free</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C21B1120W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C21B1120W"><span>Autonomous <span class="hlt">Ice</span> Mass Balance Buoys for Seasonal Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whitlock, J. D.; Planck, C.; Perovich, D. K.; Parno, J. T.; Elder, B. C.; Richter-Menge, J.; Polashenski, C. M.</p> <p>2017-12-01</p> <p>The <span class="hlt">ice</span> mass-balance represents the integration of all surface and ocean heat <span class="hlt">fluxes</span> and attributing the impact of these forcing <span class="hlt">fluxes</span> on the <span class="hlt">ice</span> cover can be accomplished by increasing temporal and spatial measurements. Mass balance information can be used to understand the ongoing changes in the Arctic sea <span class="hlt">ice</span> cover and to improve predictions of future <span class="hlt">ice</span> conditions. Thinner seasonal <span class="hlt">ice</span> in the Arctic necessitates the deployment of Autonomous <span class="hlt">Ice</span> Mass Balance buoys (IMB's) capable of long-term, in situ data collection in both <span class="hlt">ice</span> and open ocean. Seasonal IMB's (SIMB's) are free floating IMB's that allow data collection in thick <span class="hlt">ice</span>, thin <span class="hlt">ice</span>, during times of transition, and even open water. The newest generation of SIMB aims to increase the number of reliable IMB's in the Arctic by leveraging inexpensive commercial-grade instrumentation when combined with specially developed monitoring hardware. Monitoring tasks are handled by a custom, expandable data logger that provides low-cost flexibility for integrating a large range of instrumentation. The SIMB features ultrasonic sensors for direct measurement of both snow depth and <span class="hlt">ice</span> thickness and a digital temperature chain (DTC) for temperature measurements every <span class="hlt">2</span>cm through both snow and <span class="hlt">ice</span>. <span class="hlt">Air</span> temperature and pressure, along with GPS data complete the Arctic picture. Additionally, the new SIMB is more compact to maximize deployment opportunities from multiple types of platforms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22066218','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22066218"><span>Forest soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> as a function of understory removal and N-fixing species addition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Haifang; Fu, Shenglei; Zhao, Hongting; Xia, Hanping</p> <p>2011-01-01</p> <p>We report on the effects of forest management practices of understory removal and N-fixing species (Cassia alata) addition on soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in an Eucalyptus urophylla plantation (EUp), Acacia crassicarpa plantation (ACp), 10-species-mixed plantation (Tp), and 30-species-mixed plantation (THp) using the static chamber method in southern China. Four forest management treatments, including (1) understory removal (UR); (<span class="hlt">2</span>) C. alata addition (CA); (3) understory removal and replacement with C. alata (UR+CA); and (4) control without any disturbances (CK), were applied in the above four forest plantations with three replications for each treatment. The results showed that soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> rates remained at a high level during the rainy season (from April to September), followed by a rapid decrease after October reaching a minimum in February. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were significantly higher (P < 0.01) in EUp (132.6 mg/(m<span class="hlt">2</span> x hr)) and ACp (139.8 mg/(m<span class="hlt">2</span> x hr)) than in Tp (94.0 mg/(m<span class="hlt">2</span> x hr)) and THp (102.9 mg/(m<span class="hlt">2</span> x hr)). Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in UR and CA were significantly higher (P < 0.01) among the four treatments, with values of 105.7, 120.4, 133.6 and 112.<span class="hlt">2</span> mg/(m<span class="hlt">2</span> x hr) for UR+CA, UR, CA and CK, respectively. Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were positively correlated with soil temperature (P < 0.01), soil moisture (P < 0.01), NO3(-)-N (P < 0.05), and litterfall (P < 0.01), indicating that all these factors might be important controlling variables for soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. This study sheds some light on our understanding of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> dynamics in forest plantations under various management practices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22661254-abundance-atmospheric-co-sub-ocean-exoplanets-novel-co-sub-deposition-mechanism','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22661254-abundance-atmospheric-co-sub-ocean-exoplanets-novel-co-sub-deposition-mechanism"><span>The Abundance of Atmospheric <span class="hlt">CO</span>{sub <span class="hlt">2</span>} in Ocean Exoplanets: a Novel <span class="hlt">CO</span>{sub <span class="hlt">2</span>} Deposition Mechanism</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Levi, A.; Sasselov, D.; Podolak, M., E-mail: amitlevi.planetphys@gmail.com</p> <p></p> <p>We consider super-Earth sized planets which have a water mass fraction large enough to form an external mantle composed of high-pressure water-<span class="hlt">ice</span> polymorphs and also lack a substantial H/He atmosphere. We consider such planets in their habitable zone, so that their outermost condensed mantle is a global, deep, liquid ocean. For these ocean planets, we investigate potential internal reservoirs of <span class="hlt">CO</span>{sub <span class="hlt">2</span>}, the amount of <span class="hlt">CO</span>{sub <span class="hlt">2</span>} dissolved in the ocean for the various saturation conditions encountered, and the ocean-atmosphere exchange <span class="hlt">flux</span> of <span class="hlt">CO</span>{sub <span class="hlt">2</span>}. We find that, in a steady state, the abundance of <span class="hlt">CO</span>{sub <span class="hlt">2</span>} in the atmospheremore » has two possible states. When wind-driven circulation is the dominant <span class="hlt">CO</span>{sub <span class="hlt">2</span>} exchange mechanism, an atmosphere of tens of bars of <span class="hlt">CO</span>{sub <span class="hlt">2</span>} results, where the exact value depends on the subtropical ocean surface temperature and the deep ocean temperature. When sea-<span class="hlt">ice</span> formation, acting on these planets as a <span class="hlt">CO</span>{sub <span class="hlt">2</span>} deposition mechanism, is the dominant exchange mechanism, an atmosphere of a few bars of <span class="hlt">CO</span>{sub <span class="hlt">2</span>} is established. The exact value depends on the subpolar surface temperature. Our results suggest the possibility of a negative feedback mechanism, unique to water planets, where a reduction in the subpolar temperature drives more <span class="hlt">CO</span>{sub <span class="hlt">2</span>} into the atmosphere to increase the greenhouse effect.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V21C3048H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V21C3048H"><span>Controls on the fore-arc <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> along the Central America margin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hilton, D. R.; Barry, P. H.; Ramirez, C. J.; Kulongoski, J. T.; Patel, B. S.; Virrueta, C.; Blackmon, K.</p> <p>2015-12-01</p> <p>The subduction of carbon to the deep mantle via subduction zones is interrupted by outputs via the fore-arc, volcanic front, and back-arc regions. Whereas output <span class="hlt">fluxes</span> for arc and back-arc locales are well constrained for the Central America Volcanic Arc (CAVA) [1-<span class="hlt">2</span>], the fore-arc <span class="hlt">flux</span> via cold seeps and ground waters is poorly known. We present new He and <span class="hlt">CO</span><span class="hlt">2</span> data (isotopes and relative abundances) for the volcanic front and inner fore-arc of western Panama to complement on-going studies of fore-arc C-<span class="hlt">fluxes</span> in Costa Rica [3-4] and to determine tectonic controls on the fore-arc C-outgassing <span class="hlt">fluxes</span>. Helium isotope (3He/4He) values at Baru, La Yeguada, and El Valle volcanoes are high (5-8RA), consistent with results for other Central America volcanoes. However, <span class="hlt">CO</span><span class="hlt">2</span>/3He values are variable (from > 1012 to < 108). Baru has an arc-like δ13C of - 4‰, whereas the other volcanoes have δ13C < -10 ‰. Cold seeps collected in the coastal fore-arc of Panama show a trend of decreasing He-isotopes from west (~6RA) to east (~1RA). This trend is mirrored by δ13C (-5‰ to <-20‰) values. <span class="hlt">CO</span><span class="hlt">2</span>/3He values of the seeps are also variable and fall between 106 and 1012. Using <span class="hlt">CO</span><span class="hlt">2</span>/3He-δ13C mixing plots with conventional endmember values for Limestone, Organic Sediment and Mantle <span class="hlt">CO</span><span class="hlt">2</span>, we show that several Panama samples have been extensively modified by crustal processes. Nevertheless, there are clear west-to east trends (both volcanoes and coastal seeps), whereby L dominates the <span class="hlt">CO</span><span class="hlt">2</span> inventory in the west, similar to Costa Rica, and S-derived <span class="hlt">CO</span><span class="hlt">2</span> increases eastward towards central Panama. Previously [4], we limited the Costa Rica subaerial fore-arc <span class="hlt">flux</span> to ~ 6 × 107 gCkm-1yr-1, or ~ 4% of the total incoming sedimentary C-load. This <span class="hlt">flux</span> diminishes to zero within ~400 km to the east of Baru volcano. The transition from orthogonal subduction of the Cocos Plate to oblique subduction of the Nazca Plate, relative to the common over-riding Caribbean Plate, is the major impediment to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....11433I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....11433I"><span>Short-term effects of rainfall on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> above rangelands dominated by Artemisia, Bromus tectorum, and Agropyron</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivans, S.; Saliendra, N. Z.; Johnson, D. A.</p> <p>2003-04-01</p> <p>The short-term effects of rainfall on carbon dioxide (<span class="hlt">CO</span>_<span class="hlt">2</span>) <span class="hlt">fluxes</span> have not been well documented in rangelands of the Intermountain Region of the western USA. We used the Bowen ratio-energy balance technique to continuously measure <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> above three rangeland sites in Idaho and Utah dominated by: 1) Artemisia (sagebrush) near Malta, Idaho; <span class="hlt">2</span>) Bromus tectorum (cheatgrass) near Malta, Idaho; and 3) Agropyron (crested wheatgrass) in Rush Valley, Utah. We examined <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> immediately before and after rainfall during periods of 10--19 July 2001 (Summer), 8--17 October 2001 (Autumn), and 16--30 May 2002 (Spring). On sunny days before rainfall during Spring, all three sites were sinks for <span class="hlt">CO</span>_<span class="hlt">2</span>. After rainfall in Spring, all three sites became sources of <span class="hlt">CO</span>_<span class="hlt">2</span> for about two days and after that became <span class="hlt">CO</span>_<span class="hlt">2</span> sinks again. During Summer and Autumn when water was limiting, sites were small sources of <span class="hlt">CO</span>_<span class="hlt">2</span> and became larger sources for one day after rainfall. In all three seasons, daytime <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> decreased and nighttime <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> increased after rainfall, suggesting that rainfall stimulated belowground respiration at all three sites. Results from this study indicated that <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> above rangeland sites in the Intermountain West changed markedly after rainfall, especially during Spring when <span class="hlt">fluxes</span> were highest. KEY WORDS: Bowen ratio-energy balance, Intermountain West, rangelands, sagebrush, cheatgrass, crested wheatgrass</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004DPS....36.1104G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004DPS....36.1104G"><span>Geographic Distribution of N<span class="hlt">2</span>, CH4, <span class="hlt">CO</span><span class="hlt">2</span>, and H<span class="hlt">2</span>O <span class="hlt">Ices</span> on Triton from Near-IR Spectroscopic Monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grundy, W. M.; Young, L. A.; Young, E. F.; Buie, M. W.; Spencer, J. R.</p> <p>2004-11-01</p> <p>We present new 0.8 to <span class="hlt">2</span>.4 μ m spectral observations of Neptune's satellite Triton, obtained at IRTF\\slash SpeX between 2001 and 2004 as part of an ongoing search for time-variable phenomena associated with Triton's seasonal volatile transport processes, and also perhaps with reported shorter-term "reddening" events. The ability to detect spectral changes on these time scales depends critically on accurate characterization of any cyclic variations resulting from Triton's 5.877 day rotation period. We will report on our observations of periodic variations of Triton's near-IR absorption bands of N<span class="hlt">2</span>, CH4, and H<span class="hlt">2</span>O <span class="hlt">ices</span>, but not of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>, in this initial stage of our Triton monitoring program. The observed variations (or lack thereof) give an indication of how these four <span class="hlt">ice</span> species are distributed in longitude. The most heterogeneously distributed <span class="hlt">ice</span> is N<span class="hlt">2</span>, which shows nearly twice as much absorption on Triton's Neptune-facing hemisphere as on the anti-Neptune hemisphere. Comparison with Voyager-era, visual wavelength imaging of Triton's surface suggest that the observed N<span class="hlt">2</span> <span class="hlt">ice</span> is concentrated on low-latitude regions of Triton's polar cap, which are predominantly located on the Neptune-facing hemisphere. Non-volatile H<span class="hlt">2</span>O <span class="hlt">ice</span> seems to be slightly concentrated on Triton's leading hemisphere. Despite being highly diluted in N<span class="hlt">2</span> <span class="hlt">ice</span>, the longitudinal distribution of Triton's CH4 <span class="hlt">ice</span> differs from that of Triton's N<span class="hlt">2</span> <span class="hlt">ice</span>, being slightly concentrated on Triton's trailing hemisphere. Triton's <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> shows the least longitudinal variation, suggesting that it is either very uniformly distributed or that it is confined to high latitudes. This work was supported by NASA's Planetary Astronomy and Planetary Geology &\\ Geophysics programs, and by NSF's Planetary Astronomy program. \\hangindent=0.3truein Grundy, W.M., and L.A. Young (2004) Near infrared spectral monitoring of Triton with IRTF\\slash SpeX I: Establishing a baseline. Icarus (in press).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020039165','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020039165"><span>The 2140 cm(exp -1) (4.673 Microns) Solid <span class="hlt">CO</span> Band: The Case for Interstellar O<span class="hlt">2</span> and N<span class="hlt">2</span> and the Photochemistry of Non-Polar Interstellar <span class="hlt">Ice</span> Analogs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elsila, Jamie; Allamandola, Louis J.; Sandford, Scott A.; Witteborn, Fred C. (Technical Monitor)</p> <p>1996-01-01</p> <p>The infrared spectra of <span class="hlt">CO</span> frozen in non-polar <span class="hlt">ices</span> containing N<span class="hlt">2</span>, <span class="hlt">CO</span><span class="hlt">2</span>, O<span class="hlt">2</span>, and H<span class="hlt">2</span>O, and the ultraviolet photochemistry of these interstellar/precometary <span class="hlt">ice</span> analogs are reported. The spectra are used to test the hypothesis that the narrow 2140/cm (4.673 micrometer) interstellar absorption feature attributed to solid <span class="hlt">CO</span> might be produced by <span class="hlt">CO</span> frozen in <span class="hlt">ices</span> containing non-polar species such as N<span class="hlt">2</span> and O<span class="hlt">2</span>. It is shown that mixed molecular <span class="hlt">ices</span> containing <span class="hlt">CO</span>, N<span class="hlt">2</span>, O<span class="hlt">2</span>, and <span class="hlt">CO</span><span class="hlt">2</span> provide a very good match to the interstellar band at all temperatures between 12 and 30 K both before and after photolysis. The optical constants (real and imaginary parts of the index of refraction) in the region of the solid <span class="hlt">CO</span> feature are reported for several of these <span class="hlt">ices</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.P34A..01P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.P34A..01P"><span>SHARAD Finds Voluminous <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Sequestered in the Martian South Polar Layered Deposits</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phillips, R. J.; Davis, B. J.; Byrne, S.; Campbell, B. A.; Carter, L. M.; Haberle, R. M.; Holt, J. W.; Kahre, M. A.; Nunes, D. C.; Plaut, J. J.; Putzig, N. E.; Smith, I. B.; Smrekar, S. E.; Tanaka, K. L.; Titus, T. N.</p> <p>2010-12-01</p> <p>The SHARAD instrument on the Mars Reconnaissance Orbiter (MRO) mission has carried out systematic radar soundings of the layered deposits at both martian polar regions. While well-organized sets of radar reflectors are ubiquitous in the North Polar Layered Deposits, those in the South Polar Layered Deposits (SPLD) are limited to specific regions, and it is difficult to map SPLD-wide radar stratigraphy. What is evident in the radar observations are four regional reflection-free zones (RFZ) distinguished qualitatively by their radar characteristics. They are up to a kilometer in thickness and extend downward from near the surface. One such zone (RFZ3) occurs beneath the South Polar Residual Cap (SPRC), which is composed of ~5 m of solid <span class="hlt">CO</span><span class="hlt">2</span> underlain by an apparently thin layer of water <span class="hlt">ice</span>. Using a correlation technique, we inverted for the real permittivity, ɛ', on each of 41 usable SHARAD orbits over RFZ3. The results were mean values of ɛ' = <span class="hlt">2</span>.0 or <span class="hlt">2</span>.1, with a σ of 0.<span class="hlt">2</span>. A secondary technique based on the “smoothest” solution gave similar results. These values are exceptionally close to the laboratory-measured permittivity value of bulk <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> [Pettinelli et al., 2003] and distant from the bulk water <span class="hlt">ice</span> value (ɛ' = 3.15); water <span class="hlt">ice</span> is the dominant volatile in the SPLD. An alternative hypothesis for ɛ' = <span class="hlt">2.0-2</span>.1 is that the RFZ3 material is porous water <span class="hlt">ice</span>, but this can be strongly discounted based on theoretical and empirical models of ɛ' of porous water <span class="hlt">ice</span> vs. thickness. By the same arguments, the proposed <span class="hlt">CO</span><span class="hlt">2</span> material also cannot be very porous, and ɛ' should be close to the bulk value. With the permittivity estimates, radar time delays were converted to depth, and for RFZ3 a mean thickness of 210-220 m and a volume of 4,200-4,400 km3 result. This is unlikely to be the entire volume because MRO’s orbital inclination precludes SHARAD sounding poleward of ~87°S, where RFZ3 appears to extend. We do find a very good spatial correlation of RFZ3 with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1080410','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1080410"><span>Growth Kinetics, Carbohydrate, and Leaf Phosphate Content of Clover (Trifolium subterraneum L.) after Transfer to a High <span class="hlt">CO</span><span class="hlt">2</span> Atmosphere or to High Light and Ambient <span class="hlt">Air</span> 1</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Morin, Francoise; André, Marcel; Betsche, Thomas</p> <p>1992-01-01</p> <p>Intact <span class="hlt">air</span>-grown (photosynthetic photon <span class="hlt">flux</span> density, 400 microeinsteins per square meter per second) clover plants (Trifolium subterraneum L.) were transfered to high <span class="hlt">CO</span><span class="hlt">2</span> (4000 microliters <span class="hlt">CO</span><span class="hlt">2</span> per liter; photosynthetic photon <span class="hlt">flux</span> density, 400 microeinsteins per square meter per second) or to high light (340 microliters <span class="hlt">CO</span><span class="hlt">2</span> per liter; photosynthetic photon <span class="hlt">flux</span> density, 800 microeinsteins per square meter per second) to similarly stimulate photosynthetic net <span class="hlt">CO</span><span class="hlt">2</span> uptake. The daily increment of net <span class="hlt">CO</span><span class="hlt">2</span> uptake declined transiently in high <span class="hlt">CO</span><span class="hlt">2</span>, but not in high light, below the values in <span class="hlt">air</span>/standard light. After about 3 days in high <span class="hlt">CO</span><span class="hlt">2</span>, the daily increment of net <span class="hlt">CO</span><span class="hlt">2</span> uptake increased but did not reach the high light values. Nightly <span class="hlt">CO</span><span class="hlt">2</span> release increased immediately in high light, whereas there was a 3-day lag phase in high <span class="hlt">CO</span><span class="hlt">2</span>. During this time, starch accumulated to a high level, and leaf deterioration was observed only in high <span class="hlt">CO</span><span class="hlt">2</span>. After 12 days, starch was two- to threefold higher in high <span class="hlt">CO</span><span class="hlt">2</span> than in high light, whereas sucrose was similar. Leaf carbohydrates were determined during the first and fourth day in high <span class="hlt">CO</span><span class="hlt">2</span>. Starch increased rapidly throughout the day. Early in the day, sucrose was low and similar in high <span class="hlt">CO</span><span class="hlt">2</span> and ambient <span class="hlt">air</span> (same light). Later, sucrose increased considerably in high <span class="hlt">CO</span><span class="hlt">2</span>. The findings that (a) much more photosynthetic carbon was partitioned into the leaf starch pool in high <span class="hlt">CO</span><span class="hlt">2</span> than in high light, although net <span class="hlt">CO</span><span class="hlt">2</span> uptake was similar, and that (b) rapid starch formation occurred in high <span class="hlt">CO</span><span class="hlt">2</span> even when leaf sucrose was only slightly elevated suggest that low sink capacity was not the main constraint in high <span class="hlt">CO</span><span class="hlt">2</span>. It is proposed that carbon partitioning between starch (chloroplast) and sucrose (cytosol) was perturbed by high <span class="hlt">CO</span><span class="hlt">2</span> because of the lack of photorespiration. Total phosphate pools were determined in leaves. Concentrations based on fresh weight of orthophosphate, soluble esterified phosphate, and total phosphate markedly declined</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9924L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9924L"><span>Soil methane and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in rainforest and rubber plantations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lang, Rong; Blagodatsky, Sergey; Goldberg, Stefanie; Xu, Jianchu</p> <p>2017-04-01</p> <p>Expansion of rubber plantations in South-East Asia has been a land use transformation trend leading to losses of natural forest cover in the region. Besides impact on ecosystem carbon stocks, this conversion influences the dynamics of greenhouse gas <span class="hlt">fluxes</span> from soil driven by microbial activity, which has been insufficiently studied. Aimed to understand how land use change affects the soil <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span>, we measured surface gas <span class="hlt">fluxes</span>, gas concentration gradient, and 13C signature in CH4 and soil organic matter in profiles in a transect in Xishuangbanna, including a rainforest site and three rubber plantation sites with age gradient. Gas <span class="hlt">fluxes</span> were measured by static chamber method and open chamber respiration system. Soil gases were sampled from installed gas samplers at 5, 10, 30, and 75cm depth at representative time in dry and rainy season. The soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was comparable in rainforest and old rubber plantations, while young rubber plantation had the lowest rate. Total carbon content in the surface soil well explained the difference of soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> between sites. All sites were CH4 sinks in dry season and uptake decreased in the order of rainforest, old rubber plantations and young rubber plantation. From dry season to rainy season, CH4 consumption decreased with increasing CH4 concentration in the soil profile at all depths. The enrichment of methane by 13CH4 shifted towards to lowerδ13C, being the evidence of enhanced CH4 production process while net surface methane <span class="hlt">flux</span> reflected the consumption in wet condition. Increment of CH4 concentration in the profile from dry to rainy season was higher in old rubber plantation compared to rainforest, while the shifting of δ13CH4 was larger in rainforest than rubber sites. Turnover rates of soil <span class="hlt">CO</span><span class="hlt">2</span> and CH4 suggested that the 0-5 cm surface soil was the most active layer for gaseous carbon exchange. δ13C in soil organic matter and soil moisture increased from rainforest, young rubber plantation to old</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33G2447M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33G2447M"><span>High-resolution <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> inverse modeling combining GOSAT, OCO-<span class="hlt">2</span> and ground-based observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maksyutov, S. S.; Oda, T.; Saito, M.; Ito, A.; Janardanan Achari, R.; Sasakawa, M.; Machida, T.; Kaiser, J. W.; Belikov, D.; Valsala, V.; O'Dell, C.; Yoshida, Y.; Matsunaga, T.</p> <p>2017-12-01</p> <p>We develop a high-resolution <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">flux</span> inversion system that is based on the Lagrangian-Eulerian coupled tracer transport model, and is designed to estimate surface <span class="hlt">fluxes</span> from atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and CH4 data observed by the GOSAT and OCO-<span class="hlt">2</span> satellites and by global in-situ networks, including observation in Siberia. We use the Lagrangian particle dispersion model (LPDM) FLEXPART to estimate the surface <span class="hlt">flux</span> footprints for each observation at 0.1-degree spatial resolution for three days of transport. The LPDM is coupled to a global atmospheric tracer transport model (NIES-TM). The adjoint of the coupled transport model is used in an iterative optimization procedure based on either quasi-Newtonian algorithm or singular value decomposition. Combining surface and satellite data for use in inversion requires correcting for biases present in satellite observation data, that is done in a two-step procedure. As a first step, bi-weekly corrections to prior <span class="hlt">flux</span> fields are estimated for the period of 2009 to 2015 from in-situ <span class="hlt">CO</span><span class="hlt">2</span> and CH4 data from global observation network, included in Obspack-GVP (for <span class="hlt">CO</span><span class="hlt">2</span>), WDCGG (CH4) and JR-STATION datasets. High-resolution prior <span class="hlt">fluxes</span> were prepared for anthropogenic emissions (ODIAC and EDGAR), biomass burning (GFAS), and the terrestrial biosphere. The terrestrial biosphere <span class="hlt">flux</span> was constructed using a vegetation mosaic map and separate simulations of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by the VISIT model for each vegetation type present in a grid. The prior <span class="hlt">flux</span> uncertainty for land is scaled proportionally to monthly mean GPP by the MODIS product for <span class="hlt">CO</span><span class="hlt">2</span> and EDGAR emissions for CH4. Use of the high-resolution transport leads to improved representation of the anthropogenic plumes, often observed at continental continuous observation sites. OCO-<span class="hlt">2</span> observations are aggregated to 1 second averages, to match the 0.1 degree resolution of the transport model. Before including satellite observations in the inversion, the monthly varying latitude-dependent bias is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/39384','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/39384"><span>Do plant species influence soil <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> in a diverse tropical forest?</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>J.L.M. van Haren; R.C. de Oliveira; N. Restrepo-Coupe; L. Hutyra; P. B. de Camargo; Michael Keller; S.R. Saleska</p> <p>2010-01-01</p> <p>[1] To test whether plant species influence greenhouse gas production in diverse ecosystems, we measured wet season soil <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> close to 300 large (>35 cm in diameter at breast height (DBH)) trees of 15 species at three clay‐rich forest sites in central Amazonia. We found that soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> were 38% higher near large trees than at control sites >10...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B51D0457D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B51D0457D"><span>Comparing Amazon Basin <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from an atmospheric inversion with TRENDY biosphere models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diffenbaugh, N. S.; Alden, C. B.; Harper, A. B.; Ahlström, A.; Touma, D. E.; Miller, J. B.; Gatti, L. V.; Gloor, M.</p> <p>2015-12-01</p> <p>Net exchange of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) between the atmosphere and the terrestrial biosphere is sensitive to environmental conditions, including extreme heat and drought. Of particular importance for local and global carbon balance and climate are the expansive tracts of tropical rainforest located in the Amazon Basin. Because of the Basin's size and ecological heterogeneity, net biosphere <span class="hlt">CO</span><span class="hlt">2</span> exchange with the atmosphere remains largely un-constrained. In particular, the response of net <span class="hlt">CO</span><span class="hlt">2</span> exchange to changes in environmental conditions such as temperature and precipitation are not yet well known. However, proper representation of these relationships in biosphere models is a necessary constraint for accurately modeling future climate and climate-carbon cycle feedbacks. In an effort to compare biosphere response to climate across different biosphere models, the TRENDY model intercomparison project coordinated the simulation of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> between the biosphere and atmosphere, in response to historical climate forcing, by 9 different Dynamic Global Vegetation Models. We examine the TRENDY model results in the Amazon Basin, and compare this "bottom-up" method with <span class="hlt">fluxes</span> derived from a "top-down" approach to estimating net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, obtained through atmospheric inverse modeling using <span class="hlt">CO</span><span class="hlt">2</span> measurements sampled by aircraft above the basin. We compare the "bottom-up" and "top-down" <span class="hlt">fluxes</span> in 5 sub-regions of the Amazon basin on a monthly basis for 2010-2012. Our results show important periods of agreement between some models in the TRENDY suite and atmospheric inverse model results, notably the simulation of increased biosphere <span class="hlt">CO</span><span class="hlt">2</span> loss during wet season heat in the Central Amazon. During the dry season, however, model ability to simulate observed response of net <span class="hlt">CO</span><span class="hlt">2</span> exchange to drought was varied, with few models able to reproduce the "top-down" inversion <span class="hlt">flux</span> signals. Our results highlight the value of atmospheric trace gas observations for helping to narrow the</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23873747','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23873747"><span>Environmental controls of temporal and spatial variability in <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> in a neotropical peatland.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wright, Emma L; Black, Colin R; Turner, Benjamin L; Sjögersten, Sofie</p> <p>2013-12-01</p> <p>Tropical peatlands play an important role in the global storage and cycling of carbon (C) but information on carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) and methane (CH4) <span class="hlt">fluxes</span> from these systems is sparse, particularly in the Neotropics. We quantified short and long-term temporal and small scale spatial variation in <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> from three contrasting vegetation communities in a domed ombrotrophic peatland in Panama. There was significant variation in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> among vegetation communities in the order Campnosperma panamensis > Raphia taedigera > Cyperus. There was no consistent variation among sites and no discernible seasonal pattern of CH4 <span class="hlt">flux</span> despite the considerable range of values recorded (e.g. -1.0 to 12.6 mg m(-<span class="hlt">2</span>) h(-1) in 2007). <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> varied seasonally in 2007, being greatest in drier periods (300-400 mg m(-<span class="hlt">2</span>) h(-1)) and lowest during the wet period (60-132 mg m(-<span class="hlt">2</span>) h(-1)) while very high emissions were found during the 2009 wet period, suggesting that peak <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> may occur following both low and high rainfall. In contrast, only weak relationships between CH4 <span class="hlt">flux</span> and rainfall (positive at the C. panamensis site) and solar radiation (negative at the C. panamensis and Cyperus sites) was found. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> showed a diurnal pattern across sites and at the Cyperus sp. site <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> were positively correlated. The amount of dissolved carbon and nutrients were strong predictors of small scale within-site variability in gas release but the effect was site-specific. We conclude that (i) temporal variability in <span class="hlt">CO</span><span class="hlt">2</span> was greater than variation among vegetation communities; (ii) rainfall may be a good predictor of <span class="hlt">CO</span><span class="hlt">2</span> emissions from tropical peatlands but temporal variation in CH4 does not follow seasonal rainfall patterns; and (iii) diurnal variation in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> across different vegetation communities can be described by a Fourier model. © 2013 John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.B51A0302O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.B51A0302O"><span>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Following Wetting Events: Field Observations and Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Donnell, F. C.; Caylor, K. K.</p> <p>2009-12-01</p> <p>Carbon exchange data from eddy <span class="hlt">flux</span> towers in drylands suggest that the Birch Effect, a pulse of soil <span class="hlt">CO</span><span class="hlt">2</span> efflux triggered by the first rain following a dry period, may contribute significantly to the annual carbon budget of these ecosystems. Laboratory experiments on dryland soils have shown that microbes adapted to live in arid ecosystems may be able to remain dormant in dry soil for much longer than expected and an osmotic shock response to sudden increases in soil water potential may play a role in the Birch Effect. However, little has been done to understand how a dry soil profile responds to a rainfall event. We measured soil <span class="hlt">CO</span><span class="hlt">2</span> production during experimental wetting events in treatment plots at a site on the Botswana portion of the Kalahari Transect (KT). We buried small, solid-state sensors that continuously measure <span class="hlt">CO</span><span class="hlt">2</span> concentration in the soil <span class="hlt">air</span> space at four depths and the soil surface and applied wetting treatments intended to simulate typical rainfall for the region to the plots, including single 10 mm wettings (the mean storm depth for the KT), single 20 mm wettings, and repeated 10 mm wettings. We solved a finite difference approximation of the governing equation for <span class="hlt">CO</span><span class="hlt">2</span> in the soil airspace to determine the source rate of <span class="hlt">CO</span><span class="hlt">2</span> during and after the wetting treatments, using Richard’s equation to approximate the change in <span class="hlt">air</span>-filled porosity due to infiltrating water. The wetting treatments induced a rapid spike in the source rate of <span class="hlt">CO</span><span class="hlt">2</span> in the soil, the timing and magnitude of which were consistent with laboratory experiments that observed a microbial osmotic shock response. The source rate averaged over the first three hours after wetting showed that a 20 mm wetting produced a larger response than the 10 mm wettings. It also showed that a second wetting event produced a smaller response than the first and though it was not significant, an upward trend in response was apparent through the two month period. These results suggest that there may be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUSM...B41A03D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUSM...B41A03D"><span>Multiple <span class="hlt">Flux</span> Footprints, <span class="hlt">Flux</span> Divergences and Boundary Layer Mixing Ratios: Studies of Ecosystem-Atmosphere <span class="hlt">CO</span><span class="hlt">2</span> Exchange Using the WLEF Tall Tower.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, K. J.; Bakwin, P. S.; Yi, C.; Cook, B. D.; Wang, W.; Denning, A. S.; Teclaw, R.; Isebrands, J. G.</p> <p>2001-05-01</p> <p>Long-term, tower-based measurements using the eddy-covariance method have revealed a wealth of detail about the temporal dynamics of netecosystem-atmosphere exchange (NEE) of <span class="hlt">CO</span><span class="hlt">2</span>. The data also provide a measure of the annual net <span class="hlt">CO</span><span class="hlt">2</span> exchange. The area represented by these <span class="hlt">flux</span> measurements, however, is limited, and doubts remain about possible systematic errors that may bias the annual net exchange measurements. <span class="hlt">Flux</span> and mixing ratio measurements conducted at the WLEF tall tower as part of the Chequamegon Ecosystem-Atmosphere Study (ChEAS) allow for unique assessment of the uncertainties in NEE of <span class="hlt">CO</span><span class="hlt">2</span>. The synergy between <span class="hlt">flux</span> and mixing ratio observations shows the potential for comparing inverse and eddy-covariance methods of estimating NEE of <span class="hlt">CO</span><span class="hlt">2</span>. Such comparisons may strengthen confidence in both results and begin to bridge the huge gap in spatial scales (at least 3 orders of magnitude) between continental or hemispheric scale inverse studies and kilometer-scale eddy covariance <span class="hlt">flux</span> measurements. Data from WLEF and Willow Creek, another ChEAS tower, are used to estimate random and systematic errors in NEE of <span class="hlt">CO</span><span class="hlt">2</span>. Random uncertainty in seasonal exchange rates and the annual integrated NEE, including both turbulent sampling errors and variability in enviromental conditions, is small. Systematic errors are identified by examining changes in <span class="hlt">flux</span> as a function of atmospheric stability and wind direction, and by comparing the multiple level <span class="hlt">flux</span> measurements on the WLEF tower. Nighttime drainage is modest but evident. Systematic horizontal advection occurs during the morning turbulence transition. The potential total systematic error appears to be larger than random uncertainty, but still modest. The total systematic error, however, is difficult to assess. It appears that the WLEF region ecosystems were a small net sink of <span class="hlt">CO</span><span class="hlt">2</span> in 1997. It is clear that the summer uptake rate at WLEF is much smaller than that at most deciduous forest sites, including the nearby</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ClDy...50..101R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ClDy...50..101R"><span>Evaluation of energy <span class="hlt">fluxes</span> in the NCEP climate forecast system version <span class="hlt">2</span>.0 (CFSv<span class="hlt">2</span>)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rai, Archana; Saha, Subodh Kumar</p> <p>2018-01-01</p> <p>The energy <span class="hlt">fluxes</span> at the surface and top of the atmosphere (TOA) from a long free run by the NCEP climate forecast system version <span class="hlt">2</span>.0 (CFSv<span class="hlt">2</span>) are validated against several observation and reanalysis datasets. This study focuses on the annual mean energy <span class="hlt">fluxes</span> and tries to link it with the systematic cold biases in the <span class="hlt">2</span> m <span class="hlt">air</span> temperature, particularly over the land regions. The imbalance in the long term mean global averaged energy <span class="hlt">fluxes</span> are also evaluated. The global averaged imbalance at the surface and at the TOA is found to be 0.37 and 6.43 Wm-<span class="hlt">2</span>, respectively. It is shown that CFSv<span class="hlt">2</span> overestimates the land surface albedo, particularly over the snow region, which in turn contributes to the cold biases in <span class="hlt">2</span> m <span class="hlt">air</span> temperature. On the other hand, surface albedo is highly underestimated over the coastal region around Antarctica and that may have contributed to the warm bias over that oceanic region. This study highlights the need for improvements in the parameterization of snow/sea-<span class="hlt">ice</span> albedo scheme for a realistic simulation of surface temperature and that may have implications on the global energy imbalance in the model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993Icar..106..478S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993Icar..106..478S"><span>The condensation and vaporization behavior of <span class="hlt">ices</span> containing SO<span class="hlt">2</span>, H<span class="hlt">2</span>S, and <span class="hlt">CO</span><span class="hlt">2</span> - Implications for Io</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sandford, Scott A.; Allamandola, Louis J.</p> <p>1993-12-01</p> <p>The present compilation of measurements of the physical and IR spectral properties of <span class="hlt">ices</span> whose molecular compositions are relevant to the case of Io encompasses <span class="hlt">ice</span> systems containing SO<span class="hlt">2</span>, H<span class="hlt">2</span>S, and <span class="hlt">CO</span><span class="hlt">2</span>. Surface-binding energies used to calculate the residence times of molecules on a surface as a function of temperature furnish crucially important parameters for models attending to the transport of such molecules to the surface of Io. The values thus derived show that SO<span class="hlt">2</span> frosts anneal rapidly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43C2464G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43C2464G"><span>The use of fair-weather cases from the ACT-America Summer 2016 field campaign to better constrain regional biogenic <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaudet, B. J.; Davis, K. J.; DiGangi, J. P.; Feng, S.; Hoffman, K.; Jacobson, A. R.; Lauvaux, T.; McGill, M. J.; Miles, N.; Pal, S.; Pauly, R.; Richardson, S.</p> <p>2017-12-01</p> <p>The Atmospheric Carbon and Transport - America (ACT-America) study is a multi-year NASA-funded project designed to increase our understanding of regional-scale greenhouse gas (GHG) <span class="hlt">fluxes</span> over North America through aircraft, satellite, and tower-based observations. This is being accomplished through a series of field campaigns that cover three focus regions (Mid-Atlantic, Gulf Coast, and Midwest), and all four seasons (summer, winter, fall, and spring), as well as a variety of meteorological conditions. While constraints on GHG <span class="hlt">fluxes</span> can be derived on the global scale (through remote-site concentration measurements and global <span class="hlt">flux</span> inversion models) and the local scale (through eddy-covariance <span class="hlt">flux</span> tower measurements), observational constraints on the intermediate scales are not as readily available. Biogenic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are particularly challenging because of their strong seasonal and diurnal cycles and large spatial variability. During the summer 2016 ACT field campaign, fair weather days were targeted for special flight patterns designed to estimate surface <span class="hlt">fluxes</span> at scales on the order of 105 km<span class="hlt">2</span> using a modified mass-balance approach. For some onshore flow cases in the Gulf Coast, atmospheric boundary layer (ABL) flight transects were performed both inland and offshore when it could be reasonably inferred that the homogeneous Gulf <span class="hlt">air</span> provided the background GHG field for the inland transect. On other days, two-day flight sequences were performed, where the second-day location of the flight patterns was designed to encompass the <span class="hlt">air</span> mass that was sampled on the first day. With these flight patterns, the average regional <span class="hlt">flux</span> can be estimated from the ABL <span class="hlt">CO</span><span class="hlt">2</span> concentration change. Direct measurements of ABL depth from both aircraft profiles and high-resolution airborne lidar will be used, while winds and free-tropospheric <span class="hlt">CO</span><span class="hlt">2</span> can be determined from model output and in situ aircraft observations. Here we will present examples of this <span class="hlt">flux</span> estimation for both Gulf</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18044541','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18044541"><span>Energy and material balance of <span class="hlt">CO</span><span class="hlt">2</span> capture from ambient <span class="hlt">air</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zeman, Frank</p> <p>2007-11-01</p> <p>Current Carbon Capture and Storage (CCS) technologies focus on large, stationary sources that produce approximately 50% of global <span class="hlt">CO</span><span class="hlt">2</span> emissions. We propose an industrial technology that captures <span class="hlt">CO</span><span class="hlt">2</span> directly from ambient <span class="hlt">air</span> to target the remaining emissions. First, a wet scrubbing technique absorbs <span class="hlt">CO</span><span class="hlt">2</span> into a sodium hydroxide solution. The resultant carbonate is transferred from sodium ions to calcium ions via causticization. The captured <span class="hlt">CO</span><span class="hlt">2</span> is released from the calcium carbonate through thermal calcination in a modified kiln. The energy consumption is calculated as 350 kJ/mol of <span class="hlt">CO</span><span class="hlt">2</span> captured. It is dominated by the thermal energy demand of the kiln and the mechanical power required for <span class="hlt">air</span> movement. The low concentration of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> requires a throughput of 3 million cubic meters of <span class="hlt">air</span> per ton of <span class="hlt">CO</span><span class="hlt">2</span> removed, which could result in significant water losses. Electricity consumption in the process results in <span class="hlt">CO</span><span class="hlt">2</span> emissions and the use of coal power would significantly reduce to net amount captured. The thermodynamic efficiency of this process is low but comparable to other "end of pipe" capture technologies. As another carbon mitigation technology, <span class="hlt">air</span> capture could allow for the continued use of liquid hydrocarbon fuels in the transportation sector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19215133','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19215133"><span>Kinetics of <span class="hlt">CO</span>(<span class="hlt">2</span>) <span class="hlt">fluxes</span> outgassing from champagne glasses in tasting conditions: the role of temperature.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liger-Belair, Gérard; Villaume, Sandra; Cilindre, Clara; Jeandet, Philippe</p> <p>2009-03-11</p> <p>Measurements of <span class="hlt">CO</span>(<span class="hlt">2</span>) <span class="hlt">fluxes</span> outgassing from a flute poured with a standard Champagne wine initially holding about 11 g L(-1) of dissolved <span class="hlt">CO</span>(<span class="hlt">2</span>) were presented, in tasting conditions, all along the first 10 min following the pouring process. Experiments were performed at three sets of temperature, namely, 4 degrees C, 12 degrees C, and 20 degrees C, respectively. It was demonstrated that the lower the champagne temperature, the lower <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">fluxes</span> outgassing from the flute. Therefore, the lower the champagne temperature, the lower its progressive loss of dissolved <span class="hlt">CO</span>(<span class="hlt">2</span>) concentration with time, which constitutes the first analytical proof that low champagne temperatures prolong the drink's chill and helps retains its effervescence. A correlation was also proposed between <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">fluxes</span> outgassing from the flute poured with champagne and its continuously decreasing dissolved <span class="hlt">CO</span>(<span class="hlt">2</span>) concentration. Finally, the contribution of effervescence to the global kinetics of <span class="hlt">CO</span>(<span class="hlt">2</span>) release was discussed and modeled by the use of results developed over recent years. The temperature dependence of the champagne viscosity was found to play a major role in the kinetics of <span class="hlt">CO</span>(<span class="hlt">2</span>) outgassing from a flute. On the basis of this bubbling model, the theoretical influence of champagne temperature on <span class="hlt">CO</span>(<span class="hlt">2</span>) volume <span class="hlt">fluxes</span> outgassing from a flute was discussed and found to be in quite good accordance with our experimental results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMGC51G..04D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMGC51G..04D"><span>Retrieval of Paris <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> emissions using a boundary layer budget method in the framework of the <span class="hlt">CO</span><span class="hlt">2</span>-MEGAPARIS project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dieudonné, E.; Gibert, F.; Xueref-remy, I. C.; Lopez, M.; Schmidt, M.; Ravetta, F.</p> <p>2012-12-01</p> <p>. These anthropogenic <span class="hlt">fluxes</span> are compared to the CITEPA and IER emission inventories using the <span class="hlt">air</span> mass footprint from a Lagrangian Particle Dispersion Model in backward mode. Results from a case study in March 2012 are presented to assess the propagation of Paris <span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">CO</span> plume, the precision of the method and its ability to provide an independent verification of urban emission inventories. References: [a] Xueref-Remy et al., Abstract n°A13F-0277, AGU Fall Meeting 2010, San Francisco, USA [b] http://<span class="hlt">co</span><span class="hlt">2</span>-megaparis.lsce.ipsl.fr/ [c] Gibert et al., J. Geophys. Research, 112, D10301 (2007) [d] http://www.icos-infrastructure.eu/</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JMS...154..192W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JMS...154..192W"><span>Seasonality of vertical <span class="hlt">flux</span> and sinking particle characteristics in an <span class="hlt">ice</span>-free high arctic fjord-Different from subarctic fjords?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wiedmann, Ingrid; Reigstad, Marit; Marquardt, Miriam; Vader, Anna; Gabrielsen, Tove M.</p> <p>2016-02-01</p> <p>The arctic Adventfjorden (78°N, 15°E, Svalbard) used to be seasonally <span class="hlt">ice</span>-covered but has mostly been <span class="hlt">ice</span>-free since 2007. We used this <span class="hlt">ice</span>-free arctic fjord as a model area to investigate (1) how the vertical <span class="hlt">flux</span> of biomass (chlorophyll a and particulate organic carbon, POC) follows the seasonality of suspended material, (<span class="hlt">2</span>) how sinking particle characteristics change seasonally and affect the vertical <span class="hlt">flux</span>, and (3) if the vertical <span class="hlt">flux</span> in the <span class="hlt">ice</span>-free arctic fjord with glacial runoff resembles the <span class="hlt">flux</span> in subarctic <span class="hlt">ice</span>-free fjords. During seven field investigations (December 2011-September 2012), suspended biomass was determined (5, 15, 25, and 60 m), and short-term sediment traps were deployed (20, 30, 40, and 60 m), partly modified with gel-filled jars to study the size and frequency distribution of sinking particles. During winter, resuspension from the seafloor resulted in large, detrital sinking particles. Intense sedimentation of fresh biomass occurred during the spring bloom. The highest POC <span class="hlt">flux</span> was found during autumn (770-1530 mg POC m- <span class="hlt">2</span> d- 1), associated with sediment-loaded glacial runoff and high pteropod abundances. The vertical biomass <span class="hlt">flux</span> in the <span class="hlt">ice</span>-free arctic Adventfjorden thus resembled that in subarctic fjords during winter and spring, but a higher POC sedimentation was observed during autumn.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26ES...40a2027X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26ES...40a2027X"><span>Experimental investigation of static <span class="hlt">ice</span> refrigeration <span class="hlt">air</span> conditioning system driven by distributed photovoltaic energy system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Y. F.; Li, M.; Luo, X.; Wang, Y. F.; Yu, Q. F.; Hassanien, R. H. E.</p> <p>2016-08-01</p> <p>The static <span class="hlt">ice</span> refrigeration <span class="hlt">air</span> conditioning system (SIRACS) driven by distributed photovoltaic energy system (DPES) was proposed and the test experiment have been investigated in this paper. Results revealed that system energy utilization efficiency is low because energy losses were high in <span class="hlt">ice</span> making process of <span class="hlt">ice</span> slide maker. So the immersed evaporator and <span class="hlt">co</span>-integrated exchanger were suggested in system structure optimization analysis and the system COP was improved nearly 40%. At the same time, we have researched that <span class="hlt">ice</span> thickness and <span class="hlt">ice</span> super-cooled temperature changed along with time and the relationship between system COP and <span class="hlt">ice</span> thickness was obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRC..121.8419K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRC..121.8419K"><span>Reconciling estimates of the ratio of heat and salt <span class="hlt">fluxes</span> at the <span class="hlt">ice</span>-ocean interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keitzl, T.; Mellado, J. P.; Notz, D.</p> <p>2016-12-01</p> <p>The heat exchange between floating <span class="hlt">ice</span> and the underlying ocean is determined by the interplay of diffusive <span class="hlt">fluxes</span> directly at the <span class="hlt">ice</span>-ocean interface and turbulent <span class="hlt">fluxes</span> away from it. In this study, we examine this interplay through direct numerical simulations of free convection. Our results show that an estimation of the interface <span class="hlt">flux</span> ratio based on direct measurements of the turbulent <span class="hlt">fluxes</span> can be difficult because the <span class="hlt">flux</span> ratio varies with depth. As an alternative, we present a consistent evaluation of the <span class="hlt">flux</span> ratio based on the total heat and salt <span class="hlt">fluxes</span> across the boundary layer. This approach allows us to reconcile previous estimates of the <span class="hlt">ice</span>-ocean interface conditions. We find that the ratio of heat and salt <span class="hlt">fluxes</span> directly at the interface is 83-100 rather than 33 as determined by previous turbulence measurements in the outer layer. This can cause errors in the estimated <span class="hlt">ice</span>-ablation rate from field measurements of up to 40% if they are based on the three-equation formulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018APJAS..54....1K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018APJAS..54....1K"><span>Effect of Data Assimilation Parameters on The Optimized Surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> in Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Hyunjung; Kim, Hyun Mee; Kim, Jinwoong; Cho, Chun-Ho</p> <p>2018-02-01</p> <p>In this study, CarbonTracker, an inverse modeling system based on the ensemble Kalman filter, was used to evaluate the effects of data assimilation parameters (assimilation window length and ensemble size) on the estimation of surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Asia. Several experiments with different parameters were conducted, and the results were verified using <span class="hlt">CO</span><span class="hlt">2</span> concentration observations. The assimilation window lengths tested were 3, 5, 7, and 10 weeks, and the ensemble sizes were 100, 150, and 300. Therefore, a total of 12 experiments using combinations of these parameters were conducted. The experimental period was from January 2006 to December 2009. Differences between the optimized surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of the experiments were largest in the Eurasian Boreal (EB) area, followed by Eurasian Temperate (ET) and Tropical Asia (TA), and were larger in boreal summer than in boreal winter. The effect of ensemble size on the optimized biosphere <span class="hlt">flux</span> is larger than the effect of the assimilation window length in Asia, but the importance of them varies in specific regions in Asia. The optimized biosphere <span class="hlt">flux</span> was more sensitive to the assimilation window length in EB, whereas it was sensitive to the ensemble size as well as the assimilation window length in ET. The larger the ensemble size and the shorter the assimilation window length, the larger the uncertainty (i.e., spread of ensemble) of optimized surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The 10-week assimilation window and 300 ensemble size were the optimal configuration for CarbonTracker in the Asian region based on several verifications using <span class="hlt">CO</span><span class="hlt">2</span> concentration measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040062530&hterms=hydrate&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dhydrate','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040062530&hterms=hydrate&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dhydrate"><span>Remote-Raman and Micro-Raman Studies of Solid <span class="hlt">CO</span><span class="hlt">2</span>, CH4, Gas Hydrates and <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sharma, S. K.; Misra, A. K.; Lucey, P. G.; Exarhos, G. J.; Windisch, C. F., Jr.</p> <p>2004-01-01</p> <p>It is well known that on Mars <span class="hlt">CO</span><span class="hlt">2</span> is the principal constituent of the thin atmosphere and on a seasonal basis <span class="hlt">CO</span><span class="hlt">2</span> snow and frost coats the polar caps. Also over 25% of the Martian atmosphere freezes out and sublimes again each year. The Mars Odyssey Emission Imaging system (THEMIS) has discovered water <span class="hlt">ice</span> exposed near the edge of Mars southern perennials cap. In recent years, it has been suggested that in Martian subsurface <span class="hlt">CO</span><span class="hlt">2</span> may exist as gas hydrate (8<span class="hlt">CO</span><span class="hlt">2</span> + 44 H<span class="hlt">2</span>O) with melting temperature of 10C. Since the crust of Mars has been stable for enough time there is also a possibility that methane formed by magmatic processes and/or as a byproduct of anaerobic deep biosphere activity to have raised toward the planet s surface. This methane would have been captured and stored as methane hydrate, which concentrates methane and water. Determination of abundance and distribution of these <span class="hlt">ices</span> on the surface and in the near surface are of fundamental importance for understanding Martian atmosphere, and for future exploration of Mars. In this work, we have evaluated feasibility of using remote Raman and micro-Raman spectroscopy as potential nondestructive and non-contact techniques for detecting solid <span class="hlt">CO</span><span class="hlt">2</span>, CH4 gas, and gas hydrates as well as water-<span class="hlt">ice</span> on planetary surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1394156','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1394156"><span>Historical <span class="hlt">CO</span><span class="hlt">2</span> Records from the Law Dome DE08, DE08-<span class="hlt">2</span>, and DSS <span class="hlt">Ice</span> Cores (1006 A.D.-1978 A.D)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Etheridge, D. M. [Commonwealth Scientific and Industrial Research Organization (CSIRO), Aspendale, Australia; Barnola, J. M. [Laboratoire de Glaciologie et Géophysique de l'Environnement, Saint Martin d'Hères-Cedex, France; Morgan, V. I. [Antarctic CRC and Australian Antarctic Division, Hobart, Tasmania, Australia; Steele, L. P. [Commonwealth Scientific and Industrial Research Organization (CSIRO), Aspendale, Australia; Langenfelds, R. L. [Commonwealth Scientific and Industrial Research Organization (CSIRO), Aspendale, Australia; Francey, R. J. [Commonwealth Scientific and Industrial Research Organization (CSIRO), Aspendale, Australia; Martinez, Monica [Oak Ridge National Laboratory, Oak Ridge, TN (USA)</p> <p>1998-01-01</p> <p>The <span class="hlt">CO</span><span class="hlt">2</span> records presented here are derived from three <span class="hlt">ice</span> cores obtained at Law Dome, East Antarctica from 1987 to 1993. The Law Dome site satisfies many of the desirable characteristics of an ideal <span class="hlt">ice</span> core site for atmospheric <span class="hlt">CO</span><span class="hlt">2</span> reconstructions including negligible melting of the <span class="hlt">ice</span> sheet surface, low concentrations of impurities, regular stratigraphic layering undisturbed at the surface by wind or at depth by <span class="hlt">ice</span> flow, and high snow accumulation rate. Further details on the site, drilling, and cores are provided in Etheridge et al. (1996), Etheridge and Wookey (1989), and Morgan et al (1997).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010TCD.....4..153D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010TCD.....4..153D"><span>Brief communication: ikaite (Ca<span class="hlt">CO</span>3*6H<span class="hlt">2</span>O) discovered in Arctic sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dieckmann, G. S.; Nehrke, G.; Uhlig, C.; Göttlicher, J.; Gerland, S.; Granskog, M. A.; Thomas, D. N.</p> <p>2010-02-01</p> <p>We report for the first time on the discovery of calcium carbonate crystals as ikaite (Ca<span class="hlt">CO</span>3*6H<span class="hlt">2</span>O) in sea <span class="hlt">ice</span> from the Arctic (Kongsfjorden, Svalbard). This finding demonstrates that the precipitation of calcium carbonate during the freezing of sea <span class="hlt">ice</span> is not restricted to the Antarctic, where it was observed for the first time in 2008. This finding is an important step in the quest to quantify its impact on the sea <span class="hlt">ice</span> driven carbon cycle and should in the future enable improvement parametrization sea <span class="hlt">ice</span> carbon models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P21B2106K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P21B2106K"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Formation and <span class="hlt">CO</span><span class="hlt">2</span> Gas Depletion in the Polar Winter Atmosphere of Mars from Mars Climate Sounder Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kleinboehl, A.; Patel, P. K.; Schofield, J. T.; Kass, D. M.; Hayne, P. O.; McCleese, D. J.</p> <p>2016-12-01</p> <p>Temperatures in the martian lower atmosphere commonly reach the frost point of <span class="hlt">CO</span><span class="hlt">2</span> in the polar winter vortices over an extended vertical range. New retrievals from the Mars Climate Sounder (MCS) instrument on Mars Reconnaissance Orbiter allow the characterization of the winter polar regions with improved accuracy. MCS is a passive infrared sounder with 5 mid-infrared, 3 far infrared, and one broadband visible/near-infrared channels. Each spectral channel uses a linear detector array consisting of 21 elements, which provides -10 to 90 km altitude coverage when pointed at the Mars limb. From the infrared measurements, vertical profiles of temperature and aerosols are retrieved with an altitude resolution of about 5 km. Due to their long optical path through the atmosphere, limb measurements are susceptible to horizontal gradients in temperature or absorber amount in their line-of-sight, an effect that is particularly important in polar winter regions due to strong latitudinal temperature gradients in the atmosphere. The new retrievals take horizontal gradients in temperature and aerosols into account by means of a two-dimensional radiative transfer scheme. The resulting temperature profiles reveal that temperatures in the south winter polar region repeatedly drop several degrees below the frost point of <span class="hlt">CO</span><span class="hlt">2</span>. This behavior is consistent with the removal of <span class="hlt">CO</span><span class="hlt">2</span> from the atmosphere through condensation, resulting in an atmosphere that is depleted in gaseous <span class="hlt">CO</span><span class="hlt">2</span> and enhanced in non-condensable gases like N<span class="hlt">2</span> and Ar. In these regions emission features at 22 μm are often found in MCS limb measurements, consistent with the presence of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> in the polar vortex. We will map these depletions of <span class="hlt">CO</span><span class="hlt">2</span> gas and show correlations with the occurrence of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span>. We will provide comparisons of these effects between the southern and the northern polar winter vortices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995TellB..47..447I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995TellB..47..447I"><span><span class="hlt">Air</span>-sea exchange of <span class="hlt">CO</span><span class="hlt">2</span> in the central and western equatorial Pacific in 1990</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishii, Masao; Yoshikawa Inoue, Hisayuki</p> <p>1995-09-01</p> <p>Measurements of <span class="hlt">CO</span><span class="hlt">2</span> in marine boundary <span class="hlt">air</span> and in surface seawater of the central and western Pacific west of 150°W were made during the period from September to December 1990. The meridional section along 150°W showed p<span class="hlt">CO</span><span class="hlt">2</span>(sea) maximum over 410 µatm between the equator and 3°S due to strong equatorial upwelling. In the equatorial Pacific between 150°W and 179°E, p<span class="hlt">CO</span><span class="hlt">2</span>(sea) decreased gradually toward the west as a result of biological <span class="hlt">CO</span><span class="hlt">2</span> uptake and surface sea temperature increase. Between 179°E and 170°E, the p<span class="hlt">CO</span><span class="hlt">2</span>(sea) decreased steeply from 400 µatm to 350 µatm along with a decrease of salinity. West of 170°E, where the salinity is low owing to the heavy rainfall, p<span class="hlt">CO</span><span class="hlt">2</span>(sea) was nearly equal to p<span class="hlt">CO</span><span class="hlt">2</span>(<span class="hlt">air</span>). The distribution of the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration showed a considerable variability (±3ppm) in the area north of the Intertropical Convergence Zone due to the regional net source-sink strength of the terrestrial biosphere. The net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from the sea to the atmosphere in the equatorial region of the central and western Pacific (15°S-10°N, 140°E-150°W) was evaluated from the Δp<span class="hlt">CO</span><span class="hlt">2</span> distribution and the several gas transfer coefficients reported so far. It ranged from 0.13 GtC year<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1-0.29 GtC year<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1. This <span class="hlt">CO</span><span class="hlt">2</span> outflux is thought to almost disappear during the period of an El Niño event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.3916I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.3916I"><span>Regional variability of grassland <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in Tyrol/Austria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Irschick, Christoph; Hammerle, Albin; Haslwanter, Alois; Wohlfahrt, Georg</p> <p>2010-05-01</p> <p>The FLUXNET project [1] aims at quantifying the magnitude and controls on the <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O and energy exchange of terrestrial ecosystems. Ideally, the various biomes of the Earth would be sampled in proportion to their spatial extent - in reality, however, study site selection is usually based on other (more practical) criteria so that a bias exists towards certain biomes and ecosystem types. This may be problematic because FLUXNET data are used to calibrate/parameterize models at various scales - if certain ecosystems are poorly replicated this may bias model predictions. Here we present data from a project in Tyrol/Austria where we have been investigating the <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O and energy exchange of five grassland sites during 2005-2007. The five permanent grassland sites were exposed to similar climate, but differed slightly in management. In a FLUXNET style approach, any of these sites might have been selected for making long-term <span class="hlt">flux</span> measurements - the aim of this project was to examine the representativeness of these sites and, if evident, elucidate the causes for and controls on differences between sites. To this end we conducted continuous eddy covariance <span class="hlt">flux</span> measurements at one (anchor) site [<span class="hlt">2</span>, 3], and episodic, month long <span class="hlt">flux</span> measurements at the four additional sites using a roving eddy covariance tower. These data were complemented by measurements of environmental drivers, the amount of above ground phytomass and basic data on vegetation and soil type, as well as management. Data are subject to a rigorous statistical analysis in order to quantify significant differences in the <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O and energy exchange between the sites and to identify the factors which are responsible for these differences. In the present contribution we report results on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Our major findings are that (i) site-identity of the surveyed grassland ecosystems was a significant factor for the net ecosystem <span class="hlt">CO</span><span class="hlt">2</span> exchange (NEE), somewhat less for gross primary production (GPP) and not for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29358631','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29358631"><span>High geothermal heat <span class="hlt">flux</span> in close proximity to the Northeast Greenland <span class="hlt">Ice</span> Stream.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rysgaard, Søren; Bendtsen, Jørgen; Mortensen, John; Sejr, Mikael K</p> <p>2018-01-22</p> <p>The Greenland <span class="hlt">ice</span> sheet (GIS) is losing mass at an increasing rate due to surface melt and flow acceleration in outlet glaciers. Currently, there is a large disagreement between observed and simulated <span class="hlt">ice</span> flow, which may arise from inaccurate parameterization of basal motion, subglacial hydrology or geothermal heat sources. Recently it was suggested that there may be a hidden heat source beneath GIS caused by a higher than expected geothermal heat <span class="hlt">flux</span> (GHF) from the Earth's interior. Here we present the first direct measurements of GHF from beneath a deep fjord basin in Northeast Greenland. Temperature and salinity time series (2005-2015) in the deep stagnant basin water are used to quantify a GHF of 93 ± 21 mW m -<span class="hlt">2</span> which confirm previous indirect estimated values below GIS. A compilation of heat <span class="hlt">flux</span> recordings from Greenland show the existence of geothermal heat sources beneath GIS and could explain high glacial <span class="hlt">ice</span> speed areas such as the Northeast Greenland <span class="hlt">ice</span> stream.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1511498F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1511498F"><span>Aircraft observations of the urban <span class="hlt">CO</span><span class="hlt">2</span> dome in London and calculated daytime <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at the urban-regional scale</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Font, Anna; Morgui, Josep Anton; Grimmond, Sue; Barratt, Benjamin</p> <p>2013-04-01</p> <p> dispersed downwind, with peak concentrations displaced from the urban centre along the main wind direction. The urban-regional surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was calculated for four days in October 2011 by either the Integrative Mass Boundary Layer (IMBL) or the Column Integration method (CIM), dependent on meteorological conditions. The diurnal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in London obtained from the aircraft observations ranged from 36 to 71 μmol <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> s-1 during the day time. This compared well with continuous measurements of <span class="hlt">CO</span><span class="hlt">2</span> exchange by an eddy-covariance system located in central London. The day-to-day variability observed in the calculated <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> responded to the spatial variability of the influence area and emissions that observations were sensitive to. This study provides an example how aircraft surveys in urban areas can be used to estimate <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> at the urban-regional scale. It also presents an important cross-validation of two independent measurement-based methods to infer the contribution of urban areas to climate change in terms of <span class="hlt">CO</span><span class="hlt">2</span> emissions that complement bottom-up emissions inventories. References Committee on Methods for Estimating Greenhouse Gas Emissions (2010), The National Academia Press. DECC (2012), http://www.decc.gov.uk/en/content/cms/statistics/indicators/ni186/ni186.aspx</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApJ...811..120R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApJ...811..120R"><span>Ion Irradiation of H<span class="hlt">2</span>-Laden Porous Water-<span class="hlt">ice</span> Films: Implications for Interstellar <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raut, U.; Mitchell, E. H.; Baragiola, R. A.</p> <p>2015-10-01</p> <p>To understand the effects of cosmic-ray (CR) impacts on interstellar icy grains immersed in H<span class="hlt">2</span> gas, we have irradiated porous water-<span class="hlt">ice</span> films loaded with H<span class="hlt">2</span> with 100 keV H+. The <span class="hlt">ice</span> films were exposed to H<span class="hlt">2</span> gas at different pressures following deposition and during irradiation. A net H<span class="hlt">2</span> loss is observed during irradiation due to competition between ion-induced sputtering and gas adsorption. The initial H<span class="hlt">2</span> loss cross-section, 4(1) × 10-14 cm<span class="hlt">2</span>, was independent of film thickness, H<span class="hlt">2</span>, and proton <span class="hlt">fluxes</span>. In addition to sputtering, irradiation also closes nanopores, trapping H<span class="hlt">2</span> in the film with binding that exceeds physical absorption energies. As a result, <span class="hlt">2</span>%-7% H<span class="hlt">2</span> is retained in the <span class="hlt">ice</span> following irradiation to high fluences. We find that the trapped H<span class="hlt">2</span> concentration increases with decreasing Φ, the ratio of ion to H<span class="hlt">2</span> <span class="hlt">fluxes</span>, suggesting that as high as 8% solid H<span class="hlt">2</span> can be trapped in interstellar <span class="hlt">ice</span> by CR or stellar wind impacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19904911','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19904911"><span>"Self-preservation" of <span class="hlt">CO</span>(<span class="hlt">2</span>) gas hydrates--surface microstructure and <span class="hlt">ice</span> perfection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Falenty, Andrzej; Kuhs, Werner F</p> <p>2009-12-10</p> <p>Gas hydrates can exhibit an anomalously slow decomposition outside their thermodynamic stability field; the phenomenon is called "self-preservation" and is mostly studied at ambient pressure and at temperatures between approximately 240 K and the melting point of <span class="hlt">ice</span>. Here, we present a combination of in situ neutron diffraction studies, pVT work, and ex situ scanning electron microscopy (SEM) on <span class="hlt">CO</span>(<span class="hlt">2</span>) clathrates covering a much broader p-T field, stretching from 200 to 270 K and pressures between the hydrate stability limit and 0.6 kPa (6 mbar), a pressure far outside stability. The self-preservation regime above 240 K is confirmed over a broad pressure range and appears to be caused by the annealing of an <span class="hlt">ice</span> cover formed in the initial hydrate decomposition. Another, previously unknown regime of the self-preservation exists below this temperature, extending however only over a rather narrow pressure range. In this case, the initial <span class="hlt">ice</span> microstructure is dominated by a fast two-dimensional growth covering rapidly the clathrate surface. All observations lend strong support to the idea that the phenomenon of self-preservation is linked to the permeability of the <span class="hlt">ice</span> cover governed by (1) the initial microstructure of <span class="hlt">ice</span> and/or (<span class="hlt">2</span>) the subsequent annealing of this <span class="hlt">ice</span> coating. The interplay of the microstructure of newly formed <span class="hlt">ice</span> and its annealing with the ongoing decomposition reaction leads to various decomposition paths and under certain conditions to a very pronounced preservation anomaly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006TellB..58...73W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006TellB..58...73W"><span>The role of Southern Ocean mixing and upwelling in glacial-interglacial atmospheric <span class="hlt">CO</span><span class="hlt">2</span> change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Watson, Andrew J.; Naveira Garabato, Alberto C.</p> <p>2006-02-01</p> <p>Decreased ventilation of the Southern Ocean in glacial time is implicated in most explanations of lower glacial atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. Today, the deep (>2000 m) ocean south of the Polar Front is rapidly ventilated from below, with the interaction of deep currents with topography driving high mixing rates well up into the water column. We show from a buoyancy budget that mixing rates are high in all the deep waters of the Southern Ocean. Between the surface and ~2000 m depth, water is upwelled by a residual meridional overturning that is directly linked to buoyancy <span class="hlt">fluxes</span> through the ocean surface. Combined with the rapid deep mixing, this upwelling serves to return deep water to the surface on a short time scale. We propose two new mechanisms by which, in glacial time, the deep Southern Ocean may have been more isolated from the surface. Firstly, the deep ocean appears to have been more stratified because of denser bottom water resulting from intense sea <span class="hlt">ice</span> formation near Antarctica. The greater stratification would have slowed the deep mixing. Secondly, subzero atmospheric temperatures may have meant that the present-day buoyancy <span class="hlt">flux</span> from the atmosphere to the ocean surface was reduced or reversed. This in turn would have reduced or eliminated the upwelling (contrary to a common assumption, upwelling is not solely a function of the wind stress but is coupled to the <span class="hlt">air</span>-sea buoyancy <span class="hlt">flux</span> too). The observed very close link between Antarctic temperatures and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> could then be explained as a natural consequence of the connection between the <span class="hlt">air</span>-sea buoyancy <span class="hlt">flux</span> and upwelling in the Southern Ocean, if slower ventilation of the Southern Ocean led to lower atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. Here we use a box model, similar to those of previous authors, to show that weaker mixing and reduced upwelling in the Southern Ocean can explain the low glacial atmospheric <span class="hlt">CO</span><span class="hlt">2</span> in such a formulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930009382','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930009382"><span>Sea <span class="hlt">ice</span> - atmosphere interaction: Application of multispectral satellite data in polar surface energy <span class="hlt">flux</span> estimates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steffen, Konrad; Schweiger, A.; Maslanik, J.; Key, J.; Haefliger, M.; Weaver, R.</p> <p>1991-01-01</p> <p>In the past six months, work has continued on energy <span class="hlt">flux</span> sensitivity studies, <span class="hlt">ice</span> surface temperature retrievals, corrections to Advanced Very High Resolution Radiometer (AVHRR) thermal infrared data, modelling of cloud fraction retrievals, and radiation climatologies. We tentatively conclude that the SSM/I may not provide accurate enough estimates of <span class="hlt">ice</span> concentration and type to improve our shorter term energy <span class="hlt">flux</span> estimates. SSM/I derived parameters may still be applicable in longer term climatological <span class="hlt">flux</span> characterizations. We hold promise for a system coupling observation to a <span class="hlt">ice</span> deformation model. Such a model may provide information on <span class="hlt">ice</span> distribution which can be used in energy <span class="hlt">flux</span> calculations. Considerable variation was found in modelled energy <span class="hlt">flux</span> estimates when bulk transfer coefficients are modulated by lead fetch. It is still unclear what the optimum formulation is and this will be the subject of further work. Data sets for <span class="hlt">ice</span> surface temperature retrievals were assembled and preliminary data analysis was started. Finally, construction of a conceptual framework for further modelling of the Arctic radiation <span class="hlt">flux</span> climatology was started.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApJ...817L..18K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApJ...817L..18K"><span>Revisiting the Scattering Greenhouse Effect of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kitzmann, D.</p> <p>2016-02-01</p> <p>Carbon dioxide <span class="hlt">ice</span> clouds are thought to play an important role for cold terrestrial planets with thick <span class="hlt">CO</span><span class="hlt">2</span> dominated atmospheres. Various previous studies showed that a scattering greenhouse effect by carbon dioxide <span class="hlt">ice</span> clouds could result in a massive warming of the planetary surface. However, all of these studies only employed simplified two-stream radiative transfer schemes to describe the anisotropic scattering. Using accurate radiative transfer models with a general discrete ordinate method, this study revisits this important effect and shows that the positive climatic impact of carbon dioxide clouds was strongly overestimated in the past. The revised scattering greenhouse effect can have important implications for the early Mars, but also for planets like the early Earth or the position of the outer boundary of the habitable zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....11892I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....11892I"><span><span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> response to precipitation events in Juniperus osteosperma and Artemisia tridentata ecosystems using eddy covariance measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivans, S.; Hipps, L. E.</p> <p>2003-04-01</p> <p>Eddy covariance measurements were used to determine the seasonal changes of net <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">flux</span>, and the response to intermittent precipitation events in juniper (Juniperus osteosperma) and sagebrush (Artemisia tridentata) plant communities in a semi-arid region in the Great Basin of the United States over the entire growing seasons of 2001 and 2002. The net <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> were negative or downward in each community during the spring when soil water availability was largest. During this time, rain events resulted in large increases of net <span class="hlt">CO</span>_<span class="hlt">2</span> uptake in juniper within 24 hours after the rain. The relative increases were larger in the dry spring of 2001 compared to the wetter conditions of 2002. Response of sage to rain events in the spring was smaller in magnitude. During the dry periods of summer and early fall net <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">flux</span> was upward at each site in both years. In these periods the respiration of soil and vegetation apparently exceeded any assimilation by the plants. During these dry periods increases in <span class="hlt">CO</span>_<span class="hlt">2</span> efflux were observed at both sites following rain events, presumably as a result of increases in soil respiration. The response of <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> to these events lasted generally <span class="hlt">2</span> to 3 days. During late fall and early winter, no significant changes in <span class="hlt">CO</span>_<span class="hlt">2</span> <span class="hlt">fluxes</span> were observed at either site in response to rainfall because of significantly lower temperatures and plant dormancy in the year 2001. However in 2002, because of warmer weather, rainfall events triggered a temporary change in the <span class="hlt">flux</span> direction at both sites from <span class="hlt">CO</span>_<span class="hlt">2</span> efflux to <span class="hlt">CO</span>_<span class="hlt">2</span> uptake, suggesting that the plants were actively photosynthesizing. Energy balance closure values for both sites ranged from 0.75--0.80 in the moist conditions of spring, and increased to 0.80--0.85 in the dry conditions of summer and fall. It is not yet clear why energy balance closure is dependent upon the relative sizes of sensible and latent heat <span class="hlt">fluxes</span>. The issue of whether or not to force closure by adding to the <span class="hlt">fluxes</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28645049','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28645049"><span>Gaseous elemental mercury in the marine boundary layer and <span class="hlt">air</span>-sea <span class="hlt">flux</span> in the Southern Ocean in austral summer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Jiancheng; Xie, Zhouqing; Wang, Feiyue; Kang, Hui</p> <p>2017-12-15</p> <p>Gaseous elemental mercury (GEM) in the marine boundary layer (MBL), and dissolved gaseous mercury (DGM) in surface seawater of the Southern Ocean were measured in the austral summer from December 13, 2014 to February 1, 2015. GEM concentrations in the MBL ranged from 0.4 to 1.9ngm -3 (mean±standard deviation: 0.9±0.<span class="hlt">2</span>ngm -3 ), whereas DGM concentrations in surface seawater ranged from 7.0 to 75.9pgL -1 (mean±standard deviation: 23.7±13.<span class="hlt">2</span>pgL -1 ). The occasionally observed low GEM in the MBL suggested either the occurrence of atmospheric mercury depletion in summer, or the transport of GEM-depleted <span class="hlt">air</span> from the Antarctic Plateau. Elevated GEM concentrations in the MBL and DGM concentrations in surface seawater were consistently observed in the <span class="hlt">ice</span>-covered region of the Ross Sea implying the influence of the sea <span class="hlt">ice</span> environment. Diminishing sea <span class="hlt">ice</span> could cause more mercury evasion from the ocean to the <span class="hlt">air</span>. Using the thin film gas exchange model, the <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> of gaseous mercury in non-<span class="hlt">ice</span>-covered area during the study period were estimated to range from 0.0 to 6.5ngm -<span class="hlt">2</span> h -1 with a mean value of 1.5±1.8ngm -<span class="hlt">2</span> h -1 , revealing GEM (re-)emission from the East Southern Ocean in summer. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRE..121..753N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRE..121..753N"><span>Laboratory measurements of heterogeneous <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> nucleation on nanoparticles under conditions relevant to the Martian mesosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nachbar, Mario; Duft, Denis; Mangan, Thomas Peter; Martin, Juan Carlos Gomez; Plane, John M. C.; Leisner, Thomas</p> <p>2016-05-01</p> <p>Clouds of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles have been observed in the Martian mesosphere. These clouds are believed to be formed through heterogeneous nucleation of <span class="hlt">CO</span><span class="hlt">2</span> on nanometer-sized meteoric smoke particles (MSPs) or upward propagated Martian dust particles (MDPs). Large uncertainties still exist in parameterizing the microphysical formation process of these clouds as key physicochemical parameters are not well known. We present measurements on the nucleation and growth of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> on sub-4 nm radius iron oxide and silica particles representing MSPs at conditions close to the mesosphere of Mars. For both particle materials we determine the desorption energy of <span class="hlt">CO</span><span class="hlt">2</span> to be ΔFdes = (18.5 ± 0.<span class="hlt">2</span>) kJ mol-1 corresponding to ΔFdes = (0.192 ± 0.002) eV and obtain m = 0.78 ± 0.02 for the contact parameter that governs heterogeneous nucleation by analyzing the measurements using classical heterogeneous nucleation theory. We did not find any temperature dependence for the contact parameter in the temperature range examined (64 K to 73 K). By applying these values for MSPs in the Martian mesosphere, we derive characteristic temperatures for the onset of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> nucleation, which are 8-18 K below the <span class="hlt">CO</span><span class="hlt">2</span> frost point temperature, depending on particle size. This is in line with the occurrence of highly supersaturated conditions extending to 20 K below frost point temperature without the observation of clouds. Moreover, the sticking coefficient of <span class="hlt">CO</span><span class="hlt">2</span> on solid <span class="hlt">CO</span><span class="hlt">2</span> was determined to be near unity. We further argue that the same parameters can be applied to <span class="hlt">CO</span><span class="hlt">2</span> nucleation on upward propagated MDPs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A43A..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A43A..08M"><span>Long-Term Observations of Atmospheric <span class="hlt">CO</span><span class="hlt">2</span>, O3 and BrO over the Transitioning Arctic Ocean Pack-<span class="hlt">ice</span>: The O-Buoy Chemical Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matrai, P.</p> <p>2016-02-01</p> <p>Autonomous, sea <span class="hlt">ice</span>-tethered O-Buoys have been deployed (2009-2016) across the Arctic sea <span class="hlt">ice</span> for long-term atmospheric measurements (http://www.o-buoy.org). O-Buoys (15) provide in-situ concentrations of three sentinel atmospheric chemicals, ozone, <span class="hlt">CO</span><span class="hlt">2</span> and BrO, as well as meteorological parameters and imagery, over the frozen ocean. O-Buoys were designed to transmit daily data over a period of <span class="hlt">2</span> years while deployed in sea <span class="hlt">ice</span>, as part of automated <span class="hlt">ice</span>-drifting stations that include snow/<span class="hlt">ice</span> measurement systems (e.g. <span class="hlt">Ice</span> Mass Balance buoys) and oceanographic measurements (e.g. <span class="hlt">Ice</span> Tethered Profilers). Seasonal changes in Arctic atmospheric chemistry are influenced by changes in the characteristics and presence of the sea <span class="hlt">ice</span> vs. open water as well as <span class="hlt">air</span> mass trajectories, especially during the winter-spring and summer-fall transitions when sea <span class="hlt">ice</span> is melting and freezing, respectively. The O-Buoy Chemical Network provides the unique opportunity to observe these transition periods in real-time with high temporal resolution, and to compare them with those collected on land-based monitoring stations located. Due to the logistical challenges of measurements over the Arctic Ocean region, most long term, in-situ observations of atmospheric chemistry have been made at coastal or island sites around the periphery of the Arctic Ocean, leaving large spatial and temporal gaps that O-Buoys overcome. Advances in floatation, communications, power management, and sensor hardware have been made to overcome the challenges of diminished Arctic sea <span class="hlt">ice</span>. O-Buoy data provide insights into enhanced seasonal, interannual and spatial variability in atmospheric composition, atmospheric boundary layer control on the amount of halogen activation, enhancement of the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> signal over the more variable and porous pack <span class="hlt">ice</span>, and to develop an integrated picture of the coupled ocean/<span class="hlt">ice</span>/atmosphere system. As part of the Arctic Observing Network, we provide data to the community (www.aoncadis.org).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/871875','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/871875"><span><span class="hlt">Air</span> conditioning system with supplemental <span class="hlt">ice</span> storing and cooling capacity</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Weng, Kuo-Lianq; Weng, Kuo-Liang</p> <p>1998-01-01</p> <p>The present <span class="hlt">air</span> conditioning system with <span class="hlt">ice</span> storing and cooling capacity can generate and store <span class="hlt">ice</span> in its pipe assembly or in an <span class="hlt">ice</span> storage tank particularly equipped for the system, depending on the type of the <span class="hlt">air</span> conditioning system. The system is characterized in particular in that <span class="hlt">ice</span> can be produced and stored in the <span class="hlt">air</span> conditioning system whereby the time of supplying cooled <span class="hlt">air</span> can be effectively extended with the merit that the operation cycle of the on and off of the compressor can be prolonged, extending the operation lifespan of the compressor in one aspect. In another aspect, <span class="hlt">ice</span> production and storage in great amount can be performed in an off-peak period of the electrical power consumption and the stored <span class="hlt">ice</span> can be utilized in the peak period of the power consumption so as to provide supplemental cooling capacity for the compressor of the <span class="hlt">air</span> conditioning system whereby the shift of peak and off-peak power consumption can be effected with ease. The present <span class="hlt">air</span> conditioning system can lower the installation expense for an <span class="hlt">ice</span>-storing <span class="hlt">air</span> conditioning system and can also be applied to an old conventional <span class="hlt">air</span> conditioning system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005TellB..57....1M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005TellB..57....1M"><span>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from three ecosystems in tropical peatland of Sarawak, Malaysia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melling, Lulie; Hatano, Ryusuke; Goh, Kah Joo</p> <p>2005-02-01</p> <p>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was measured monthly over a year from tropical peatland of Sarawak, Malaysia using a closed-chamber technique. The soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> ranged from 100 to 533 mg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> h<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1 for the forest ecosystem, 63 to 245 mg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> h<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1 for the sago and 46 to 335 mg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> h<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1 for the oil palm. Based on principal component analysis (PCA), the environmental variables over all sites could be classified into three components, namely, climate, soil moisture and soil bulk density, which accounted for 86% of the seasonal variability. A regression tree approach showed that <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in each ecosystem was related to different underlying environmental factors. They were relative humidity for forest, soil temperature at 5 cm for sago and water-filled pore space for oil palm. On an annual basis, the soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was highest in the forest ecosystem with an estimated production of <span class="hlt">2</span>.1 kg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> yr<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1 followed by oil palm at 1.5 kg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> yr<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img>1 and sago at 1.1 kg C m<img src="/entityImage/script/2212.gif" alt="-" border="0" style="font-weight: bold"></img><span class="hlt">2</span> yr<img src="/entityImage/script/2212.gif" alt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070023316&hterms=casa&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dcasa','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070023316&hterms=casa&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dcasa"><span>Progress in Modeling Global Atmospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> and Transport: Results from Simulations with Diurnal <span class="hlt">Fluxes</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Collatz, G. James; Kawa, R.</p> <p>2007-01-01</p> <p>Progress in better determining <span class="hlt">CO</span><span class="hlt">2</span> sources and sinks will almost certainly rely on utilization of more extensive and intensive <span class="hlt">CO</span><span class="hlt">2</span> and related observations including those from satellite remote sensing. Use of advanced data requires improved modeling and analysis capability. Under NASA Carbon Cycle Science support we seek to develop and integrate improved formulations for 1) atmospheric transport, <span class="hlt">2</span>) terrestrial uptake and release, 3) biomass and 4) fossil fuel burning, and 5) observational data analysis including inverse calculations. The transport modeling is based on meteorological data assimilation analysis from the Goddard Modeling and Assimilation Office. Use of assimilated met data enables model comparison to <span class="hlt">CO</span><span class="hlt">2</span> and other observations across a wide range of scales of variability. In this presentation we focus on the short end of the temporal variability spectrum: hourly to synoptic to seasonal. Using <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at varying temporal resolution from the SIB <span class="hlt">2</span> and CASA biosphere models, we examine the model's ability to simulate <span class="hlt">CO</span><span class="hlt">2</span> variability in comparison to observations at different times, locations, and altitudes. We find that the model can resolve much of the variability in the observations, although there are limits imposed by vertical resolution of boundary layer processes. The influence of key process representations is inferred. The high degree of fidelity in these simulations leads us to anticipate incorporation of realtime, highly resolved observations into a multiscale carbon cycle analysis system that will begin to bridge the gap between top-down and bottom-up <span class="hlt">flux</span> estimation, which is a primary focus of NACP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B41C0458G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B41C0458G"><span>Effects of experimental warming and elevated <span class="hlt">CO</span><span class="hlt">2</span> on surface methane and CO­<span class="hlt">2</span> <span class="hlt">fluxes</span> from a boreal black spruce peatland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gill, A. L.; Finzi, A.; Giasson, M. A.</p> <p>2015-12-01</p> <p>High latitude peatlands represent a major terrestrial carbon store sensitive to climate change, as well as a globally significant methane source. While elevated atmospheric carbon dioxide concentrations and warming temperatures may increase peat respiration and C losses to the atmosphere, reductions in peatland water tables associated with increased growing season evapotranspiration may alter the nature of trace gas emission and increase peat C losses as <span class="hlt">CO</span><span class="hlt">2</span> relative to methane (CH4). As CH4 is a greenhouse gas with twenty times the warming potential of <span class="hlt">CO</span><span class="hlt">2</span>, it is critical to understand how surface <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 will be influenced by factors associated with global climate change. We used automated soil respiration chambers to assess the influence of elevated atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and whole ecosystem warming on peatland CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at the SPRUCE (Spruce and Peatland Responses Under Climatic and Environmental Change) Experiment in northern Minnesota. Belowground warming treatments were initiated in July 2014 and whole ecosystem warming and elevated <span class="hlt">CO</span><span class="hlt">2</span> treatments began in August 2015. Here we report soil i<span class="hlt">CO</span><span class="hlt">2</span> and iCH4 <span class="hlt">flux</span> responses to the first year of belowground warming and the first two months of whole ecosystem manipulation. We also leverage the spatial and temporal density of measurements across the twenty autochambers to assess how physical (i.e., plant species composition, microtopography) and environmental (i.e., peat temperature, water table position, oxygen availability) factors influence observed rates of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> loss. We find that methane <span class="hlt">fluxes</span> increased significantly across warming treatments following the first year of belowground warming, while belowground warming alone had little influence on soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Peat microtopography strongly influenced trace gas emission rates, with higher CH4 <span class="hlt">fluxes</span> in hollow locations and higher <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in hummock locations. While there was no difference in the isotopic composition of the methane</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.C23E..06W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.C23E..06W"><span>Organic carbon export from the Greenland <span class="hlt">Ice</span> Sheet: sources, sinks and downstream <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wadham, J. L.; Lawson, E.; Tranter, M.; Stibal, M.; Telling, J.; Lis, G. P.; Nienow, P. W.; Anesio, A. M.; Butler, C. E.</p> <p>2012-12-01</p> <p>Runoff from small glacier systems has been shown to contain dissolved organic carbon (DOC) rich in low molecular weight (LMW), and hence more labile forms, designating glaciers as an important source of carbon for downstream heterotrophic activity. Here we assess glacier surfaces as potential sources of labile DOC to downstream ecosystems, presenting data from a wide range of glacier systems to determine sources and sinks of DOC in glacial and proglacial systems. We subsequently focus upon the Greenland <span class="hlt">Ice</span> Sheet (GrIS) which is the largest source of glacial runoff at present (400 km3 yr-1), with predicted increases in future decades. We report high <span class="hlt">fluxes</span> of particulate organic carbon (POC), DOC and LMW labile fractions from a large GrIS catchment during two contrasting melt seasons. POC dominates OC export, is sourced from the <span class="hlt">ice</span> sheet bed and contains a significant bioreactive component (~10% carbohydrates). The LMW-DOC "labile" fraction derives almost entirely from microbial activity on the <span class="hlt">ice</span> sheet surface, which is supported by data from glacier systems also presented here. Annual <span class="hlt">fluxes</span> of DOC, POC and labile components were lower in 2010 than 2009, despite a ~<span class="hlt">2</span> fold increase in runoff <span class="hlt">fluxes</span> in 2010, suggesting production-limited DOC/POC sources. Scaled to the entire <span class="hlt">ice</span> sheet, combined DOC and POC <span class="hlt">fluxes</span> are of a similar order of magnitude to other large Arctic river systems and may represent an important source of organic carbon to the North Atlantic, Greenland and Labrador Seas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12898382','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12898382"><span>Elevated <span class="hlt">CO</span><span class="hlt">2</span> reduces sap <span class="hlt">flux</span> in mature deciduous forest trees.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cech, Patrick G; Pepin, Steeve; Körner, Christian</p> <p>2003-10-01</p> <p>We enriched in <span class="hlt">CO</span><span class="hlt">2</span> the canopy of 14 broad-leaved trees in a species-rich, ca. 30-m-tall forest in NW Switzerland to test whether elevated <span class="hlt">CO</span><span class="hlt">2</span> reduces water use in mature forest trees. Measurements of sap <span class="hlt">flux</span> density (JS) were made prior to <span class="hlt">CO</span><span class="hlt">2</span> enrichment (summer 2000) and throughout the first whole growing season of <span class="hlt">CO</span><span class="hlt">2</span> exposure (2001) using the constant heat-flow technique. The short-term responses of sap <span class="hlt">flux</span> to brief (1.5-3 h) interruptions of <span class="hlt">CO</span><span class="hlt">2</span> enrichment were also examined. There were no significant a priori differences in morphological and physiological traits between trees which were later exposed to elevated <span class="hlt">CO</span><span class="hlt">2</span> (n=14) and trees later used as controls (n=19). Over the entire growing season, <span class="hlt">CO</span><span class="hlt">2</span> enrichment resulted in an average 10.7% reduction in mean daily JS across all species compared to control trees. Responses were most pronounced in Carpinus, Acer, Prunus and Tilia, smaller in Quercus and close to zero in Fagus trees. The JS of treated trees significantly increased by 7% upon transient exposure to ambient <span class="hlt">CO</span><span class="hlt">2</span> concentrations at noon. Hence, responses of the different species were, in the short term, similar in magnitude to those observed over the whole season (though opposite because of the reversed treatment). The reductions in mean JS of <span class="hlt">CO</span><span class="hlt">2</span>-enriched trees were high (22%) under conditions of low evaporative demand (vapour pressure deficit, VPD <5 hPa) and small (<span class="hlt">2</span>%) when mean daily VPD was greater than 10 hPa. During a relatively dry period, the effect of elevated <span class="hlt">CO</span><span class="hlt">2</span> on JS even appeared to be reversed. These results suggest that daily water savings by <span class="hlt">CO</span><span class="hlt">2</span>-enriched trees may have accumulated to a significantly improved water status by the time when control trees were short of soil moisture. Our data indicate that the magnitude of <span class="hlt">CO</span><span class="hlt">2</span> effects on stand transpiration will depend on rainfall regimes and the relative abundance of the different species, being more pronounced under humid conditions and in stands dominated by species such as Carpinus and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43F2533S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43F2533S"><span>Measurement of NOx and <span class="hlt">CO</span> <span class="hlt">Fluxes</span> from a Tall Tower in Beijing.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Squires, F. A.; Drysdale, W. S.; Hamilton, J.; Lee, J. D.; Vaughan, A. R.; Wild, O.; Mullinger, N.; Nemitz, E.; Metzger, S.; Zhang, Q.</p> <p>2017-12-01</p> <p>China's <span class="hlt">air</span> quality problems are well publicised; in 2010, 1.<span class="hlt">2</span> million premature deaths were attributed to outdoor <span class="hlt">air</span> pollution in China. One of the major <span class="hlt">air</span> quality issues is high concentrations of nitrogen oxides (NOx). China is the largest NOx emitter, contributing an estimated 18 % to global NOx emissions. Beijing itself is reported to have NO<span class="hlt">2</span> concentrations 42 % higher than the annual national standard. Given the high levels of pollution, increased focus has been placed on improving emissions estimates which are typically developed using a `bottom-up' approach where emissions are predicted from their sources. Emission inventories in China have large uncertainties and are rapidly changing with time in response to economic development, environmental regulation and new technologies. In fact, China is the largest contributor to the uncertainty in the source and the magnitude of <span class="hlt">air</span> pollutants in <span class="hlt">air</span> quality models. Recent studies have shown a discrepancy between NOx inventories and measured NOx emissions for UK cities, highlighting the limitations of bottom-up emissions inventories and the importance of accurate measurement data to improve the estimates. 5 Hz measurements of NOx and <span class="hlt">CO</span> concentration were made as part of the <span class="hlt">Air</span> Pollutants in Beijing (AIRPOLL-Beijing) project during two field campaigns in Nov-Dec 2016 and May-June 2017. Sampling took place from an inlet <span class="hlt">co</span>-located with a sonic anemometer at 102 m on a meteorological tower in central Beijing. Analysis of the covariance between vertical wind speed and concentration enabled the calculation of emission <span class="hlt">flux</span>, with an estimated footprint of between <span class="hlt">2</span> - 5 km from the tower (which typically included some major ring roads and expressways). <span class="hlt">Fluxes</span> were quantified using the continuous wavelet transformation (CWT) method, which enabled one minute resolved <span class="hlt">fluxes</span> to be calculated. These data were compared to existing emissions estimates from the Multi-resolution Emission Inventory for China (MEIC). It is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4632A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4632A"><span>Diffuse <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from Santiago and Congro volcanic lakes (São Miguel, Azores archipelago)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrade, César; Cruz, José; Viveiros, Fátima; Branco, Rafael</p> <p>2017-04-01</p> <p>Diffuse <span class="hlt">CO</span><span class="hlt">2</span> degassing occurring in Santiago and Congro lakes, both located in depressions associated to maars from São Miguel Island (Azores, Portugal), was studied through detailed <span class="hlt">flux</span> measurements. Four sampling campaigns were developed between 2013 and 2016 in each water body, split by the cold and wet seasons. São Miguel has an area of 744.6 km<span class="hlt">2</span>, being the largest island of the archipelago. The geology of the island is dominated by three quiescent central volcanoes (Sete Cidades, Fogo and Furnas), linked by volcanic fissural zones (Picos and Congro Fissural Volcanic systems). The oldest volcanic systems of the island are located in its eastern part (Povoação-Nordeste). Santiago lake, with a surface area of 0.26 km<span class="hlt">2</span> and a depth of 30.5 m, is located inside a maar crater in the Sete Cidades volcano at an altitude of 355 m. The watershed of the lake has an area of 0.97 km<span class="hlt">2</span> and a surface flow estimated as 1.54x10 m3/a. A total of 1612 <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements using the accumulation chamber method were made at Santiago lake, 253 in the first campaign (November 2013), and 462, 475 and 422 in the three other campaigns, respectively, in April 2014, September 2016 and December 2016. The total <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimated for this lake varies between 0.4 t d-1 and 0.59 t d-1, for the surveys performed, respectively, in November 2013 and September 2016; higher <span class="hlt">CO</span><span class="hlt">2</span> outputs of 1.57 and 5.87 t d-1 were calculated for the surveys carried out in April 2014 and December 2016. These higher <span class="hlt">CO</span><span class="hlt">2</span> emissions were associated with a period without water column stratification. Similarly to Santiago lake, Congro lake is located inside a maar, in the Congro Fissural Volcanic system, and has a surface area of 0.04 km<span class="hlt">2</span> with 18.5 m depth and a storage of about <span class="hlt">2</span>.4x105 m3/a. The lake, located at an altitude of 420 m, is fed by a watershed with an area of 0.33 km<span class="hlt">2</span> and a runoff estimated as about 8x104 m3/a. In Congro lake a total of 713 <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements were performed during four surveys from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApJ...758...37K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApJ...758...37K"><span>Electron Irradiation of Kuiper Belt Surface <span class="hlt">Ices</span>: Ternary N<span class="hlt">2</span>-CH4-<span class="hlt">CO</span> Mixtures as a Case Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Y. S.; Kaiser, R. I.</p> <p>2012-10-01</p> <p>The space weathering of icy Kuiper Belt Objects was investigated in this case study by exposing methane (CH4) and carbon monoxide (<span class="hlt">CO</span>) doped nitrogen (N<span class="hlt">2</span>) <span class="hlt">ices</span> at 10 K to ionizing radiation in the form of energetic electrons. Online and in situ Fourier transform infrared spectroscopy was utilized to monitor the radiation-induced chemical processing of these <span class="hlt">ices</span>. Along with isocyanic acid (HNCO), the products could be mainly derived from those formed in irradiated binary <span class="hlt">ices</span> of the N<span class="hlt">2</span>-CH4 and <span class="hlt">CO</span>-CH4 systems: nitrogen-bearing products were found in the form of hydrogen cyanide (HCN), hydrogen isocyanide (HNC), diazomethane (CH<span class="hlt">2</span>N<span class="hlt">2</span>), and its radical fragment (HCN<span class="hlt">2</span>); oxygen-bearing products were of acetaldehyde (CH3CHO), formyl radical (HCO), and formaldehyde (H<span class="hlt">2</span><span class="hlt">CO</span>). As in the pure <span class="hlt">ices</span>, the methyl radical (CH3) and ethane (C<span class="hlt">2</span>H6) were also detected, as were carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) and the azide radical (N3). Based on the temporal evolution of the newly formed products, kinetic reaction schemes were then developed to fit the temporal profiles of the newly formed species, resulting in numerical sets of rate constants. The current study highlights important constraints on the preferential formation of isocyanic acid (HNCO) over hydrogen cyanide (HCN) and hydrogen isocyanide (HNC), thus guiding the astrobiological and chemical evolution of those distant bodies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1340454-co2-capture-from-ambient-air-crystallization-guanidine-sorbent','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1340454-co2-capture-from-ambient-air-crystallization-guanidine-sorbent"><span><span class="hlt">CO</span> <span class="hlt">2</span> Capture from Ambient <span class="hlt">Air</span> by Crystallization with a Guanidine Sorbent</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Seipp, Charles A.; Univ. of Texas, Austin, TX; Williams, Neil J.; ...</p> <p>2016-12-21</p> <p>Carbon capture and storage is an important strategy for stabilizing the increasing concentration of atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> and the global temperature. A possible approach toward reversing this trend and decreasing the atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> concentration is to remove the <span class="hlt">CO</span> <span class="hlt">2</span> directly from <span class="hlt">air</span> (direct <span class="hlt">air</span> capture). In this paper, we report a simple aqueous guanidine sorbent that captures <span class="hlt">CO</span> <span class="hlt">2</span> from ambient <span class="hlt">air</span> and binds it as a crystalline carbonate salt by guanidinium hydrogen bonding. The resulting solid has very low aqueous solubility (K sp=1.0(4)×10 -8), which facilitates its separation from solution by filtration. The bound <span class="hlt">CO</span> <span class="hlt">2</span> canmore » be released by relatively mild heating of the crystals at 80–120 °C, which regenerates the guanidine sorbent quantitatively. Finally and thus, this crystallization-based approach to <span class="hlt">CO</span> <span class="hlt">2</span> separation from <span class="hlt">air</span> requires minimal energy and chemical input, and offers the prospect for low-cost direct <span class="hlt">air</span> capture technologies.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JChPh.148p4702E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148p4702E"><span>Glycine formation in <span class="hlt">CO</span><span class="hlt">2</span>:CH4:NH3 <span class="hlt">ices</span> induced by 0-70 eV electrons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Esmaili, Sasan; Bass, Andrew D.; Cloutier, Pierre; Sanche, Léon; Huels, Michael A.</p> <p>2018-04-01</p> <p>Glycine (Gly), the simplest amino-acid building-block of proteins, has been identified on icy dust grains in the interstellar medium, icy comets, and <span class="hlt">ice</span> covered meteorites. These astrophysical <span class="hlt">ices</span> contain simple molecules (e.g., <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O, CH4, HCN, and NH3) and are exposed to complex radiation fields, e.g., UV, γ, or X-rays, stellar/solar wind particles, or cosmic rays. While much current effort is focused on understanding the radiochemistry induced in these <span class="hlt">ices</span> by high energy radiation, the effects of the abundant secondary low energy electrons (LEEs) it produces have been mostly assumed rather than studied. Here we present the results for the exposure of multilayer <span class="hlt">CO</span><span class="hlt">2</span>:CH4:NH3 <span class="hlt">ice</span> mixtures to 0-70 eV electrons under simulated astrophysical conditions. Mass selected temperature programmed desorption (TPD) of our electron irradiated films reveals multiple products, most notably intact glycine, which is supported by control measurements of both irradiated or un-irradiated binary mixture films, and un-irradiated <span class="hlt">CO</span><span class="hlt">2</span>:CH4:NH3 <span class="hlt">ices</span> spiked with Gly. The threshold of Gly formation by LEEs is near 9 eV, while the TPD analysis of Gly film growth allows us to determine the "quantum" yield for 70 eV electrons to be about 0.004 Gly per incident electron. Our results show that simple amino acids can be formed directly from simple molecular ingredients, none of which possess preformed C—C or C—N bonds, by the copious secondary LEEs that are generated by ionizing radiation in astrophysical <span class="hlt">ices</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29716196','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29716196"><span>Glycine formation in <span class="hlt">CO</span><span class="hlt">2</span>:CH4:NH3 <span class="hlt">ices</span> induced by 0-70 eV electrons.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Esmaili, Sasan; Bass, Andrew D; Cloutier, Pierre; Sanche, Léon; Huels, Michael A</p> <p>2018-04-28</p> <p>Glycine (Gly), the simplest amino-acid building-block of proteins, has been identified on icy dust grains in the interstellar medium, icy comets, and <span class="hlt">ice</span> covered meteorites. These astrophysical <span class="hlt">ices</span> contain simple molecules (e.g., <span class="hlt">CO</span> <span class="hlt">2</span> , H <span class="hlt">2</span> O, CH 4 , HCN, and NH 3 ) and are exposed to complex radiation fields, e.g., UV, γ, or X-rays, stellar/solar wind particles, or cosmic rays. While much current effort is focused on understanding the radiochemistry induced in these <span class="hlt">ices</span> by high energy radiation, the effects of the abundant secondary low energy electrons (LEEs) it produces have been mostly assumed rather than studied. Here we present the results for the exposure of multilayer <span class="hlt">CO</span> <span class="hlt">2</span> :CH 4 :NH 3 <span class="hlt">ice</span> mixtures to 0-70 eV electrons under simulated astrophysical conditions. Mass selected temperature programmed desorption (TPD) of our electron irradiated films reveals multiple products, most notably intact glycine, which is supported by control measurements of both irradiated or un-irradiated binary mixture films, and un-irradiated <span class="hlt">CO</span> <span class="hlt">2</span> :CH 4 :NH 3 <span class="hlt">ices</span> spiked with Gly. The threshold of Gly formation by LEEs is near 9 eV, while the TPD analysis of Gly film growth allows us to determine the "quantum" yield for 70 eV electrons to be about 0.004 Gly per incident electron. Our results show that simple amino acids can be formed directly from simple molecular ingredients, none of which possess preformed C-C or C-N bonds, by the copious secondary LEEs that are generated by ionizing radiation in astrophysical <span class="hlt">ices</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B44D..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B44D..06G"><span>Effects of experimental warming and elevated <span class="hlt">CO</span><span class="hlt">2</span> on surface methane and CO­<span class="hlt">2</span> <span class="hlt">fluxes</span> from a boreal black spruce peatland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gill, A. L.; Finzi, A.; Hsieh, I. F.; Giasson, M. A.</p> <p>2016-12-01</p> <p>High latitude peatlands represent a major terrestrial carbon store sensitive to climate change, as well as a globally significant methane source. While elevated atmospheric carbon dioxide concentrations and warming temperatures may increase peat respiration and C losses to the atmosphere, reductions in peatland water tables associated with increased growing season evapotranspiration may alter the nature of trace gas emission and increase peat C losses as <span class="hlt">CO</span><span class="hlt">2</span> relative to methane (CH4). As CH4 is a greenhouse gas with twenty times the warming potential of <span class="hlt">CO</span><span class="hlt">2</span>, it is critical to understand how surface <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 will be influenced by factors associated with global climate change. We used automated soil respiration chambers to assess the influence of elevated atmospheric <span class="hlt">CO</span><span class="hlt">2</span> and whole ecosystem warming on peatland CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at the SPRUCE (Spruce and Peatland Responses Under Climatic and Environmental Change) Experiment in northern Minnesota. Here we report soil i<span class="hlt">CO</span><span class="hlt">2</span> and iCH4 <span class="hlt">flux</span> responses to the first year of belowground warming and the first season of whole ecosystem warming and elevated <span class="hlt">CO</span><span class="hlt">2</span> treatments. We find that peat methane <span class="hlt">fluxes</span> are more sensitive to warming treatments than peat <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, particularly in hollow peat microforms. Surface <span class="hlt">CO</span><span class="hlt">2</span>:CH4 <span class="hlt">flux</span> ratios decreased across warming treatments, suggesting that the temperature sensitivity of methane production overshadows the effect of peat drying and surface aeration in the short term. δ13C of the emitted methane was more depleted in the early and late growing season, indicating a transition from hydrogenotrophic to acetoclastic methanogenesis during periods of high photosynthetic input. The measurement record demonstrates that belowground warming has measureable impacts on the nature of peat greenhouse gas emission within one year of treatment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1224019-amineoxide-hybrid-materials-co-capture-from-ambient-air','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1224019-amineoxide-hybrid-materials-co-capture-from-ambient-air"><span>Amine–Oxide Hybrid Materials for <span class="hlt">CO</span> <span class="hlt">2</span> Capture from Ambient <span class="hlt">Air</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Didas, Stephanie A.; Choi, Sunho; Chaikittisilp, Watcharop; ...</p> <p>2015-09-10</p> <p>CONSPECTUS: Oxide supports functionalized with amine moieties have been used for decades as catalysts and chromatographic media. Owing to the recognized impact of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> on global climate change, the study of the use of amine-oxide hybrid materials as <span class="hlt">CO</span><span class="hlt">2</span> sorbents has exploded in the past decade. While the majority of the work has concerned separation of <span class="hlt">CO</span><span class="hlt">2</span> from dilute mixtures such as flue gas from coal-fired power plants, it has been recognized by us and others that such supported amine materials are also perhaps uniquely suited to extract <span class="hlt">CO</span><span class="hlt">2</span> from ultradilute gas mixtures, such as ambient <span class="hlt">air</span>. As unique,more » low temperature chemisorbents, they can operate under ambient conditions, spontaneously extracting <span class="hlt">CO</span><span class="hlt">2</span> from ambient <span class="hlt">air</span>, while being regenerated under mild conditions using heat or the combination of heat and vacuum. This Account describes the evolution of our activities on the design of amine-functionalized silica materials for catalysis to the design, characterization, and utilization of these materials in <span class="hlt">CO</span><span class="hlt">2</span> separations. New materials developed in our laboratory, such as hyperbranched aminosilica materials, and previously known amine-oxide hybrid compositions, have been extensively studied for <span class="hlt">CO</span><span class="hlt">2</span> extraction from simulated ambient <span class="hlt">air</span> (400 ppm of <span class="hlt">CO</span><span class="hlt">2</span>). The role of amine type and structure (molecular, polymeric), support type and structure, the stability of the various compositions under simulated operating conditions, and the nature of the adsorbed <span class="hlt">CO</span><span class="hlt">2</span> have been investigated in detail. The requirements for an effective, practical <span class="hlt">air</span> capture process have been outlined and the ability of amine−oxide hybrid materials to meet these needs has been discussed. Ultimately, the practicality of such a “direct <span class="hlt">air</span> capture” process is predicated not only on the physicochemical properties of the sorbent, but also how the sorbent operates in a practical process that offers a scalable gas−solid contacting strategy. In this regard, the utility of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1224019-amineoxide-hybrid-materials-co2-capture-from-ambient-air','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1224019-amineoxide-hybrid-materials-co2-capture-from-ambient-air"><span>Amine–Oxide Hybrid Materials for <span class="hlt">CO</span> <span class="hlt">2</span> Capture from Ambient <span class="hlt">Air</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Didas, Stephanie A.; Choi, Sunho; Chaikittisilp, Watcharop; ...</p> <p>2015-09-10</p> <p>Oxide supports functionalized with amine moieties have been used for decades as catalysts and chromatographic media. Owing to the recognized impact of atmospheric <span class="hlt">CO</span> <span class="hlt">2</span> on global climate change, the study of the use of amine-oxide hybrid materials as <span class="hlt">CO</span> <span class="hlt">2</span> sorbents has exploded in the past decade. While the majority of the work has concerned separation of <span class="hlt">CO</span> <span class="hlt">2</span> from dilute mixtures such as flue gas from coal-fired power plants, it has been recognized by us and others that such supported amine materials are also perhaps uniquely suited to extract <span class="hlt">CO</span> <span class="hlt">2</span> from ultradilute gas mixtures, such as ambientmore » <span class="hlt">air</span>. As unique, low temperature chemisorbents, they can operate under ambient conditions, spontaneously extracting <span class="hlt">CO</span> <span class="hlt">2</span> from ambient <span class="hlt">air</span>, while being regenerated under mild conditions using heat or the combination of heat and vacuum. This Account describes the evolution of our activities on the design of amine-functionalized silica materials for catalysis to the design, characterization, and utilization of these materials in <span class="hlt">CO</span> <span class="hlt">2</span> separations. New materials developed in our laboratory, such as hyperbranched aminosilica materials, and previously known amine-oxide hybrid compositions, have been extensively studied for <span class="hlt">CO</span> <span class="hlt">2</span> extraction from simulated ambient <span class="hlt">air</span> (400 ppm of <span class="hlt">CO</span> <span class="hlt">2</span>). The role of amine type and structure (molecular, polymeric), support type and structure, the stability of the various compositions under simulated operating conditions, and the nature of the adsorbed <span class="hlt">CO</span> <span class="hlt">2</span> have been investigated in detail. The requirements for an effective, practical <span class="hlt">air</span> capture process have been outlined and the ability of amine-oxide hybrid materials to meet these needs has been discussed. Ultimately, the practicality of such a “direct <span class="hlt">air</span> capture” process is predicated not only on the physicochemical properties of the sorbent, but also how the sorbent operates in a practical process that offers a scalable gas-solid contacting strategy. In conclusion, the utility of low</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/43512','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/43512"><span>Consequences of incomplete surface energy balance closure for <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from open-path <span class="hlt">CO</span><span class="hlt">2</span>/H<span class="hlt">2</span>O infrared gas analyzers</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Heping Liu; James T. Randerson; Jamie Lindfors; William J. Massman; Thomas Foken</p> <p>2006-01-01</p> <p>We present an approach for assessing the impact of systematic biases in measured energy <span class="hlt">fluxes</span> on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> estimates obtained from open-path eddy-covariance systems. In our analysis, we present equations to analyse the propagation of errors through the Webb, Pearman, and Leuning (WPL) algorithm [Quart. J. Roy. Meteorol. Soc. 106, 85­100, 1980] that is widely used to...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.B51B0309S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.B51B0309S"><span>An analytical model for the distribution of <span class="hlt">CO</span><span class="hlt">2</span> sources and sinks, <span class="hlt">fluxes</span>, and mean concentration within the roughness sub-layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Siqueira, M. B.; Katul, G. G.</p> <p>2009-12-01</p> <p>A one-dimensional analytical model that predicts foliage <span class="hlt">CO</span><span class="hlt">2</span> uptake rates, turbulent <span class="hlt">fluxes</span>, and mean concentration throughout the roughness sub-layer (RSL), a layer that extends from the ground surface up to 5 times the canopy height (h), is proposed. The model combines the mean continuity equation for <span class="hlt">CO</span><span class="hlt">2</span> with first-order closure principles for turbulent <span class="hlt">fluxes</span> and simplified physiological and radiative transfer schemes for foliage uptake. This combination results in a second-order ordinary differential equation in which it is imposed soil respiration (RE) as lower and <span class="hlt">CO</span><span class="hlt">2</span> concentration well above the RSL as upper boundary conditions. An inverse version of the model was tested against data sets from two contrasting ecosystems: a tropical forest (TF, h=40 m) and a managed irrigated rice canopy (RC, h=0.7 m) - with good agreement noted between modeled and measured mean <span class="hlt">CO</span><span class="hlt">2</span> concentration profiles within the entire RSL (see figure). Sensitivity analysis on the model parameters revealed a plausible scaling regime between them and a dimensionless parameter defined by the ratio between external (RE) and internal (stomatal conductance) characteristics controlling the <span class="hlt">CO</span><span class="hlt">2</span> exchange process. The model can be used to infer the thickness of the RSL for <span class="hlt">CO</span><span class="hlt">2</span> exchange, the inequality in zero-plane displacement between <span class="hlt">CO</span><span class="hlt">2</span> and momentum, and its consequences on modeled <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. A simplified version of the solution is well suited for being incorporated into large-scale climate models. Furthermore, the model framework here can be used to a priori estimate relative contributions from the soil surface and the atmosphere to canopy-<span class="hlt">air</span> <span class="hlt">CO</span><span class="hlt">2</span> concentration thereby making it synergetic to stable isotopes studies. Panels a) and c): Profiles of normalized measured leaf area density distribution (a) for TF and RC, respectively. Continuous lines are the constant a used in the model and dashed lines represent data-derived profiles. Panels b) and d) are modeled and ensemble-averaged measured</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APh....78....1A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APh....78....1A"><span>Characterization of the atmospheric muon <span class="hlt">flux</span> in <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aartsen, M. G.; Abraham, K.; Ackermann, M.; Adams, J.; Aguilar, J. A.; Ahlers, M.; Ahrens, M.; Altmann, D.; Anderson, T.; Archinger, M.; Argüelles, C.; Arlen, T. C.; Auffenberg, J.; Bai, X.; Barwick, S. W.; Baum, V.; Bay, R.; Beatty, J. J.; Becker Tjus, J.; Becker, K.-H.; Beiser, E.; BenZvi, S.; Berghaus, P.; Berley, D.; Bernardini, E.; Bernhard, A.; Besson, D. Z.; Binder, G.; Bindig, D.; Bissok, M.; Blaufuss, E.; Blumenthal, J.; Boersma, D. J.; Bohm, C.; Börner, M.; Bos, F.; Bose, D.; Böser, S.; Botner, O.; Braun, J.; Brayeur, L.; Bretz, H.-P.; Brown, A. M.; Buzinsky, N.; Casey, J.; Casier, M.; Cheung, E.; Chirkin, D.; Christov, A.; Christy, B.; Clark, K.; Classen, L.; Coenders, S.; Cowen, D. F.; Cruz Silva, A. H.; Daughhetee, J.; Davis, J. C.; Day, M.; de André, J. P. A. M.; De Clercq, C.; Dembinski, H.; De Ridder, S.; Desiati, P.; de Vries, K. D.; de Wasseige, G.; de With, M.; DeYoung, T.; Díaz-Vélez, J. C.; Dumm, J. P.; Dunkman, M.; Eagan, R.; Eberhardt, B.; Ehrhardt, T.; Eichmann, B.; Euler, S.; Evenson, P. A.; Fadiran, O.; Fahey, S.; Fazely, A. R.; Fedynitch, A.; Feintzeig, J.; Felde, J.; Filimonov, K.; Finley, C.; Fischer-Wasels, T.; Flis, S.; Fuchs, T.; Glagla, M.; Gaisser, T. K.; Gaior, R.; Gallagher, J.; Gerhardt, L.; Ghorbani, K.; Gier, D.; Gladstone, L.; Glüsenkamp, T.; Goldschmidt, A.; Golup, G.; Gonzalez, J. G.; Góra, D.; Grant, D.; Gretskov, P.; Groh, J. C.; Groß, A.; Ha, C.; Haack, C.; Haj Ismail, A.; Hallgren, A.; Halzen, F.; Hansmann, B.; Hanson, K.; Hebecker, D.; Heereman, D.; Helbing, K.; Hellauer, R.; Hellwig, D.; Hickford, S.; Hignight, J.; Hill, G. C.; Hoffman, K. D.; Hoffmann, R.; Holzapfel, K.; Homeier, A.; Hoshina, K.; Huang, F.; Huber, M.; Huelsnitz, W.; Hulth, P. O.; Hultqvist, K.; In, S.; Ishihara, A.; Jacobi, E.; Japaridze, G. S.; Jero, K.; Jurkovic, M.; Kaminsky, B.; Kappes, A.; Karg, T.; Karle, A.; Kauer, M.; Keivani, A.; Kelley, J. L.; Kemp, J.; Kheirandish, A.; Kiryluk, J.; Kläs, J.; Klein, S. R.; Kohnen, G.; Koirala, R.; Kolanoski, H.; Konietz, R.; Koob, A.; Köpke, L.; Kopper, C.; Kopper, S.; Koskinen, D. J.; Kowalski, M.; Krings, K.; Kroll, G.; Kroll, M.; Kunnen, J.; Kurahashi, N.; Kuwabara, T.; Labare, M.; Lanfranchi, J. L.; Larson, M. J.; Lesiak-Bzdak, M.; Leuermann, M.; Leuner, J.; Lünemann, J.; Madsen, J.; Maggi, G.; Mahn, K. B. M.; Maruyama, R.; Mase, K.; Matis, H. S.; Maunu, R.; McNally, F.; Meagher, K.; Medici, M.; Meli, A.; Menne, T.; Merino, G.; Meures, T.; Miarecki, S.; Middell, E.; Middlemas, E.; Miller, J.; Mohrmann, L.; Montaruli, T.; Morse, R.; Nahnhauer, R.; Naumann, U.; Niederhausen, H.; Nowicki, S. C.; Nygren, D. R.; Obertacke, A.; Olivas, A.; Omairat, A.; O'Murchadha, A.; Palczewski, T.; Pandya, H.; Paul, L.; Pepper, J. A.; Pérez de los Heros, C.; Pfendner, C.; Pieloth, D.; Pinat, E.; Posselt, J.; Price, P. B.; Przybylski, G. T.; Pütz, J.; Quinnan, M.; Rädel, L.; Rameez, M.; Rawlins, K.; Redl, P.; Reimann, R.; Relich, M.; Resconi, E.; Rhode, W.; Richman, M.; Richter, S.; Riedel, B.; Robertson, S.; Rongen, M.; Rott, C.; Ruhe, T.; Ryckbosch, D.; Saba, S. M.; Sabbatini, L.; Sander, H.-G.; Sandrock, A.; Sandroos, J.; Sarkar, S.; Schatto, K.; Scheriau, F.; Schimp, M.; Schmidt, T.; Schmitz, M.; Schoenen, S.; Schöneberg, S.; Schönwald, A.; Schukraft, A.; Schulte, L.; Seckel, D.; Seunarine, S.; Shanidze, R.; Smith, M. W. E.; Soldin, D.; Spiczak, G. M.; Spiering, C.; Stahlberg, M.; Stamatikos, M.; Stanev, T.; Stanisha, N. A.; Stasik, A.; Stezelberger, T.; Stokstad, R. G.; Stößl, A.; Strahler, E. A.; Ström, R.; Strotjohann, N. L.; Sullivan, G. W.; Sutherland, M.; Taavola, H.; Taboada, I.; Ter-Antonyan, S.; Terliuk, A.; Tešić, G.; Tilav, S.; Toale, P. A.; Tobin, M. N.; Tosi, D.; Tselengidou, M.; Turcati, A.; Unger, E.; Usner, M.; Vallecorsa, S.; van Eijndhoven, N.; Vandenbroucke, J.; van Santen, J.; Vanheule, S.; Veenkamp, J.; Vehring, M.; Voge, M.; Vraeghe, M.; Walck, C.; Wallraff, M.; Wandkowsky, N.; Weaver, Ch.; Wendt, C.; Westerhoff, S.; Whelan, B. J.; Whitehorn, N.; Wichary, C.; Wiebe, K.; Wiebusch, C. H.; Wille, L.; Williams, D. R.; Wissing, H.; Wolf, M.; Wood, T. R.; Woschnagg, K.; Xu, D. L.; Xu, X. W.; Xu, Y.; Yáñez, J. P.; Yodh, G.; Yoshida, S.; Zarzhitsky, P.; Zoll, M.</p> <p>2016-05-01</p> <p>Muons produced in atmospheric cosmic ray showers account for the by far dominant part of the event yield in large-volume underground particle detectors. The <span class="hlt">Ice</span>Cube detector, with an instrumented volume of about a cubic kilometer, has the potential to conduct unique investigations on atmospheric muons by exploiting the large collection area and the possibility to track particles over a long distance. Through detailed reconstruction of energy deposition along the tracks, the characteristics of muon bundles can be quantified, and individual particles of exceptionally high energy identified. The data can then be used to constrain the cosmic ray primary <span class="hlt">flux</span> and the contribution to atmospheric lepton <span class="hlt">fluxes</span> from prompt decays of short-lived hadrons. In this paper, techniques for the extraction of physical measurements from atmospheric muon events are described and first results are presented. The multiplicity spectrum of TeV muons in cosmic ray <span class="hlt">air</span> showers for primaries in the energy range from the knee to the ankle is derived and found to be consistent with recent results from surface detectors. The single muon energy spectrum is determined up to PeV energies and shows a clear indication for the emergence of a distinct spectral component from prompt decays of short-lived hadrons. The magnitude of the prompt <span class="hlt">flux</span>, which should include a substantial contribution from light vector meson di-muon decays, is consistent with current theoretical predictions. The variety of measurements and high event statistics can also be exploited for the evaluation of systematic effects. In the course of this study, internal inconsistencies in the zenith angle distribution of events were found which indicate the presence of an unexplained effect outside the currently applied range of detector systematics. The underlying cause could be related to the hadronic interaction models used to describe muon production in <span class="hlt">air</span> showers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMED41A0839B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMED41A0839B"><span>Effect of Wildfire on Sequoiadendron giganteum Growth and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barwegen, S.</p> <p>2016-12-01</p> <p>Due to global warming, parts of the United States are becoming drier than ever before. In 2015, we surpassed 9 million acres burned by wildfires nationally (Rice 2015). Wildfires are most common in the Western United States due to drought, and the fact that the summer months are drier than other areas such as the East Coast, so there is a higher risk for wildland fires (Donegan 2016). These high-growth forests that are more frequently burned by wildfires each year are located near mountain ranges on the west side of the United States. They are important to tourism, contain many endangered species, and need to maintain the natural cycle of fire and regrowth for the continued success of the native plant life. This project investigated the effect of burnt soil on Sequoiadendron giganteum trees. Three were grown in burnt potting soil that had been roasted over a grill for 45 minutes (which is the average destructive fire time), and the other three were the control group in unburned potting soil. We assessed growth by measuring height, color, photosynthetically active radiation (PAR), and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> to evaluate the health of the trees in the two soil conditions. We noted that after two weeks the trunks of the trees growing in burnt soil began to brown in color, and they lost leaves. Over the course of the experiment, the trees growing in burnt soil had reduced levels of photosynthesis as compared to the unburned soil (as measured by the net change in <span class="hlt">CO</span><span class="hlt">2</span> concentration in a sealed chamber over the course of fifteen minutes intervals). On average, the trees growing in burnt soil had <span class="hlt">flux</span> rates that were 19.59 ppm <span class="hlt">CO</span><span class="hlt">2</span> /min. more than those growing in unburned soil. In the dark reactions, the burnt soil <span class="hlt">flux</span> was 54.5 ppm <span class="hlt">CO</span><span class="hlt">2</span>/min., while the unburned soil averaged 40.5 ppm <span class="hlt">CO</span><span class="hlt">2</span>/min. Our results help quantify the impact of fire on delicate ecosystems that are experiencing an increase in fire activity caused by global warming.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A41E2327D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A41E2327D"><span>Controlling factors of evaporation and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> over an open water lake in southeastern margin of Tibetan Plateau</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Du, Q.; Liu, H.; Liu, Y.; Wang, L.; Xu, L.</p> <p>2017-12-01</p> <p>Erhai lake is located in the southeastern margin of Tibetan Plateau. Based on the 4 years measurement over Erhai lake with eddy covariance technique (EC) from 2012 to 2015, the diurnal and seasonal variations of latent and sensible heat and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, and their controlling factors over different time scales were analyzed. The diurnal average LE ranged from 31 to 171 Wm-<span class="hlt">2</span>, while Hs ranged from -31 to 21 Wm-<span class="hlt">2</span>. Bowen ratio was larger during January and May and smaller during June and October. The lake continued storing heat during January and June, and releasing heat since July. The diurnal average <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> during nighttime were higher than the daytime, and carbon uptake was almost observed during the midday time of the day for the whole study period. The annual carbon budget fluctuated from 117.5 to 161.7 g C m-<span class="hlt">2</span> a-1, while annual total evaporation (ET) from 1120.8 to 1228.5 mm for the four-years period. The Erhai Lake behaved as a net carbon source over the whole period but carbon uptake was observed during the middle time of each year. The difference between water surface and <span class="hlt">air</span> temperature (DeltaT) and the product of DeltaT and wind speed were the main controlling factors for Hs from halfhourly to monthly scale. There was significant relationship between wind speed, the product of wind speed and vapor pressure deficit (VPD) and LE on halfhourly and daily scales. The total cloud amount and net radiation (Rn) had a large effect on monthly variation of LE. Photosynthetic active radiation (PAR) and wind speed was mainly responsible for the variation of halfhourly and daily <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, respectively. The total cloud amount was the most important factors controlling for annual total ET. The annual rainfall, water surface temperature was observed to be negatively related with annual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/35420','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/35420"><span>LBA-ECO TG-07 Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> by Automated Chamber, Para, Brazil: 2001-2003</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>R.K. Varner; M.M. Keller</p> <p>2009-01-01</p> <p>Measurements of the soil-atmosphere <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> were made at the km 67 <span class="hlt">flux</span> tower site in the Tapajos National Forest, Santarem, Para, Brazil. Eight chambers were set up to measure trace gas exchange between the soil and atmosphere about 5 times a day (during daylight and night) at this undisturbed forest site from April 2001 to April 2003. <span class="hlt">CO</span><span class="hlt">2</span> soil efflux data are...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.B11F0421L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.B11F0421L"><span>Carbon dioxide(<span class="hlt">CO</span><span class="hlt">2</span>) and nitrous oxide (N<span class="hlt">2</span>O) <span class="hlt">fluxes</span> in an agro-ecosystems under changing physical and biological conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, L.; Eberwein, J.; Oikawa, P.; Jenerette, D.; Grantz, D. A.</p> <p>2013-12-01</p> <p>Liyin Liang1, Jennifer Eberwein1, Patty Oikawa1, Darrel Jenerette1, David Grantz1 1Department of Botany and Plant Sciences, University of California, Riverside, CA 92521, USA Carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) and nitrous oxide (N<span class="hlt">2</span>O) are the major greenhouse gases and together produce a strong positive radiative forcing in the atmosphere. The <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O from soil to atmosphere vary with physical and biological factors, e.g., temperature, soil moisture, pH value, soil organic carbon contents, microorganism communities and so on. Understanding the interactions among these factors is critical to estimation of <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O emissions. We investigate these <span class="hlt">fluxes</span> in an extreme production environment with very high maximum temperatures, at the agricultural experiment station of University of California-Desert Research Center in the Imperial Valley of southern California. In this research, we measured the <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> from soil incubation under controlled laboratory conditions, in surface chambers under field conditions and by eddy covariance. We explore the variation of <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> and relationship between them in this extreme biofuel production environment. The discrete chamber measurements showed that the N<span class="hlt">2</span>O <span class="hlt">flux</span> in our field sites is <span class="hlt">2</span>.39×0.70 μg N m-<span class="hlt">2</span> hr-1, with a 95% confidence interval (CI) from 0.86 to 3.92 μg N m-<span class="hlt">2</span> hr-1. Compared to the previous reported value (0.45~26.26 μg N m-<span class="hlt">2</span> hr-1) of N<span class="hlt">2</span>O <span class="hlt">flux</span> in California, the N<span class="hlt">2</span>O <span class="hlt">flux</span> from biofuel crop land is in the lower level, although more observations should be took to confirm it. The N<span class="hlt">2</span>O <span class="hlt">flux</span> also shows very high variability within a field of biomass Sorghum, ranging from 0.40 to 8.19 μg N m-<span class="hlt">2</span> hr-1 across 11 sites owning to the high variability of physical and biological factors. Soil incubation measurements will be conducted to identify the sources of this variability. The eddy covariance measurements will allow calculation of the <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O emissions at the ecosystem level as a step in quantifying</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PalOc..25.3201J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PalOc..25.3201J"><span>Response of <span class="hlt">air</span>-sea carbon <span class="hlt">fluxes</span> and climate to orbital forcing changes in the Community Climate System Model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jochum, M.; Peacock, S.; Moore, K.; Lindsay, K.</p> <p>2010-07-01</p> <p>A global general circulation model coupled to an ocean ecosystem model is used to quantify the response of carbon <span class="hlt">fluxes</span> and climate to changes in orbital forcing. Compared to the present-day simulation, the simulation with the Earth's orbital parameters from 115,000 years ago features significantly cooler northern high latitudes but only moderately cooler southern high latitudes. This asymmetry is explained by a 30% reduction of the strength of the Atlantic Meridional Overturning Circulation that is caused by an increased Arctic sea <span class="hlt">ice</span> export and a resulting freshening of the North Atlantic. The strong northern high-latitude cooling and the direct insolation induced tropical warming lead to global shifts in precipitation and winds to the order of 10%-20%. These climate shifts lead to regional differences in <span class="hlt">air</span>-sea carbon <span class="hlt">fluxes</span> of the same order. However, the differences in global net <span class="hlt">air</span>-sea carbon <span class="hlt">fluxes</span> are small, which is due to several effects, two of which stand out: first, colder sea surface temperature leads to a more effective solubility pump but also to increased sea <span class="hlt">ice</span> concentration which blocks <span class="hlt">air</span>-sea exchange, and second, the weakening of Southern Ocean winds that is predicted by some idealized studies occurs only in part of the basin, and is compensated by stronger winds in other parts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JGR...10427693K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JGR...10427693K"><span>Carbon trace gases in lake and beaver pond <span class="hlt">ice</span> near Thompson, Manitoba, Canada</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuhlbusch, Thomas A. J.; Zepp, Richard G.</p> <p>1999-11-01</p> <p>Concentrations of <span class="hlt">CO</span><span class="hlt">2</span>, <span class="hlt">CO</span>, and CH4 were measured in beaver pond and lake <span class="hlt">ice</span> in April 1996 near Thompson, Manitoba to derive information on possible impacts of <span class="hlt">ice</span> melting on corresponding atmospheric trace gas concentrations. CH4 concentrations in beaver pond and lake <span class="hlt">ice</span> ranged between 0.3-150 mmol m-3 and 3.1-56.<span class="hlt">2</span> μmol m-3, respectively. The corresponding <span class="hlt">CO</span> concentrations showed no significant differences between the two lakes. They varied between 50 and 250 μmol m-3. These <span class="hlt">CO</span> concentrations are some of the highest determined in any aquatic system. The differences in CH4 concentrations between lake and pond can be explained by the differences in production and microbial oxidation rates between the two systems. No explanation can be given for the similar <span class="hlt">CO</span> concentrations. Supersaturation factors for <span class="hlt">CO</span> were 660±130 and 630±330, and 65-35000 and 0.6-13 for CH4 in the <span class="hlt">ice</span> of the beaver pond and Troy Lake, respectively. When digging into the beaver pond <span class="hlt">ice</span>, a continuous flow of bubbles with 0.32±0.06 vol% CH4, <span class="hlt">2.2</span>±0.3 vol% <span class="hlt">CO</span><span class="hlt">2</span>, and 482±98 ppb <span class="hlt">CO</span> coming out of the slash <span class="hlt">ice</span> for about 20-30 minutes was noticed. Wintertime <span class="hlt">flux</span> estimates of CH4 and <span class="hlt">CO</span> showed that they represent at minimum 6.4% and <span class="hlt">2.2</span>% of that of the summer. It has to be noted that these wintertime <span class="hlt">fluxes</span> will mostly be released to the atmosphere during the time of snowmelt, thus a limited time period of weeks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090026508','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090026508"><span>An Investigation of the <span class="hlt">Icing</span> and Heated-<span class="hlt">air</span> De-<span class="hlt">icing</span> Characteristics of the R-2600-13 Induction System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chapman, Gilbert E.</p> <p>1946-01-01</p> <p>A laboratory investigation was made on a Holley 1685-HB carburetor mounted on an R-2600-13 supercharger assembly to determine the <span class="hlt">icing</span> characteristics and the heated-<span class="hlt">air</span> de-<span class="hlt">icing</span> requirements of this portion of the B-25D airplane induction system. <span class="hlt">Icing</span> has been found to be most prevalent at relatively small throttle openings and, consequently, all runs were made at simulated 60-percent normal rated power condition. <span class="hlt">Icing</span> characteristics were determined during a series of 15-minute runs over a range of inlet-<span class="hlt">air</span> conditions. For the de-<span class="hlt">icing</span> investigation severe impact <span class="hlt">ice</span> was allowed to form in the induction system and the time required for the recovery of 95 percent of the maximum possible <span class="hlt">air</span> flow at the original throttle setting was then determined for a range of wet-bulb temperatures. Results of these runs showed that <span class="hlt">ice</span> on the walls of the carburetor adapter and on the rim of the impeller-shroud portion of the supercharger diffuser plate did not affect engine operation at 60-percent normal rated power. <span class="hlt">Ice</span> that adversely affected the <span class="hlt">air</span> flow and the fuel-<span class="hlt">air</span> ratio was formed only on the central web of the carburetor and then only when the inlet <span class="hlt">air</span> was saturated or contained free moisture in excess of saturation. No serious <span class="hlt">ice</span> formations were observed at inlet-<span class="hlt">air</span> temperatures above 66 0 F or with an inlet-<span class="hlt">air</span> enthalpy greater than 34 Btu per pound. The maximum temperature at. which any trace of <span class="hlt">icing</span> could be detected was 1110 F with a relative humidity of approximately 28 percent, The <span class="hlt">air</span>-flow recovery time for emergency de-<span class="hlt">icing</span> was 0.3 minute for.an enthalpy of 35 Btu per pound or wet-bulb temperature of 68 0 F. Further increase in enthalpy and wet-bulb temperature above these values resulted in very slight improvement in recovery time. The fuel-<span class="hlt">air</span> ratio restored by a 5-Minute application of heated <span class="hlt">air</span> was approximately 7 percent less than the initial value for cold-<span class="hlt">air</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25207956','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25207956"><span>Reducing the cost of Ca-based direct <span class="hlt">air</span> capture of <span class="hlt">CO</span><span class="hlt">2</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zeman, Frank</p> <p>2014-10-07</p> <p>Direct <span class="hlt">air</span> capture, the chemical removal of <span class="hlt">CO</span><span class="hlt">2</span> directly from the atmosphere, may play a role in mitigating future climate risk or form the basis of a sustainable transportation infrastructure. The current discussion is centered on the estimated cost of the technology and its link to "overshoot" trajectories, where atmospheric <span class="hlt">CO</span><span class="hlt">2</span> levels are actively reduced later in the century. The American Physical Society (APS) published a report, later updated, estimating the cost of a one million tonne <span class="hlt">CO</span><span class="hlt">2</span> per year <span class="hlt">air</span> capture facility constructed today that highlights several fundamental concepts of chemical <span class="hlt">air</span> capture. These fundamentals are viewed through the lens of a chemical process that cycles between removing <span class="hlt">CO</span><span class="hlt">2</span> from the <span class="hlt">air</span> and releasing the absorbed <span class="hlt">CO</span><span class="hlt">2</span> in concentrated form. This work builds on the APS report to investigate the effect of modifications to the <span class="hlt">air</span> capture system based on suggestions in the report and subsequent publications. The work shows that reduced carbon electricity and plastic packing materials (for the contactor) may have significant effects on the overall price, reducing the APS estimate from $610 to $309/t<span class="hlt">CO</span><span class="hlt">2</span> avoided. Such a reduction does not challenge postcombustion capture from point sources, estimated at $80/t<span class="hlt">CO</span><span class="hlt">2</span>, but does make <span class="hlt">air</span> capture a feasible alternative for the transportation sector and a potential negative emissions technology. Furthermore, <span class="hlt">air</span> capture represents atmospheric reductions rather than simply avoided emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B41D0082M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B41D0082M"><span>Annual Greenhouse Gas (<span class="hlt">CO</span><span class="hlt">2</span>, CH4, and N<span class="hlt">2</span>O) <span class="hlt">Fluxes</span> Via Ebullition from a Temperate Emergent Wetland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mcnicol, G.; Sturtevant, C. S.; Knox, S. H.; Baldocchi, D. D.; Silver, W. L.</p> <p>2014-12-01</p> <p>Quantifying wetland greenhouse gas exchange is necessary to evaluate their potential for mitigating climate change via carbon sequestration. However measuring greenhouse gas <span class="hlt">fluxes</span> of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), methane (CH4), and nitrous oxide (N<span class="hlt">2</span>O) in wetlands is difficult due to high spatial and temporal variability, and multiple transport pathways of emission. Transport of biogenic soil gas via highly sporadic ebullition (bubbling) events is often ignored or quantified poorly in wetland greenhouse gas budgets, but can rapidly release large volumes of gas to the atmosphere. To quantify a robust annual ebullition <span class="hlt">flux</span> we measured rates continuously for a year (2013-2014) using custom-built chambers deployed in a restored emergent wetland located in the Sacramento-San Joaquin Delta, CA. We combined ebullition <span class="hlt">flux</span> rates with observations of gas concentrations to estimate annual ebullition emissions of <span class="hlt">CO</span><span class="hlt">2</span>, CH4, and N<span class="hlt">2</span>O and compare <span class="hlt">flux</span> rates to whole-ecosystem exchange of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 measured simultaneously by eddy covariance.Mean ebullition <span class="hlt">flux</span> rates were 18.3 ± 5.6 L m-<span class="hlt">2</span> yr-1. Ebullition CH4 concentrations were very high and ranged from 23-76 % with a mean of 47 ± <span class="hlt">2</span>.9 %; <span class="hlt">CO</span><span class="hlt">2</span> concentrations were lower and ranged from 0.7-6.6 % with a mean of <span class="hlt">2</span>.8 ± 0.3 %; N<span class="hlt">2</span>O concentrations were below atmospheric concentrations and ranged from 130-389 ppb(v) with a mean of 257 ± 13 ppb(v). We calculated well-constrained annual ebullition <span class="hlt">fluxes</span> of: 6.<span class="hlt">2</span> ± 1.9 g CH4 m-<span class="hlt">2</span> yr-1, 1.0 ± 0.3 g <span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> yr-1 and 9.3 ± <span class="hlt">2</span>.8 mg N<span class="hlt">2</span>O m-<span class="hlt">2</span> yr-1. Methane emissions via ebullition were very large, representing 15-25 % of total wetland CH4 emissions measured at this site, whereas ebullition released only relatively small quantities of <span class="hlt">CO</span><span class="hlt">2</span> and N<span class="hlt">2</span>O. Our results demonstrate that large releases of CH4 via ebullition from open water surfaces can be a significant component of restored wetland greenhouse gas budgets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...13.2243C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...13.2243C"><span>Improved simulation of group averaged <span class="hlt">CO</span><span class="hlt">2</span> surface concentrations using GEOS-Chem and <span class="hlt">fluxes</span> from VEGAS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Z. H.; Zhu, J.; Zeng, N.</p> <p>2013-01-01</p> <p><span class="hlt">CO</span><span class="hlt">2</span> measurements have been combined with simulated <span class="hlt">CO</span><span class="hlt">2</span> distributions from a transport model in order to produce the optimal estimates of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">fluxes</span> in inverse modeling. However one persistent problem in using model-observation comparisons for this goal relates to the issue of compatibility. Observations at a single site reflect all underlying processes of various scales that usually cannot be fully resolved by model simulations at the grid points nearest the site due to lack of spatial or temporal resolution or missing processes in models. In this article we group site observations of multiple stations according to atmospheric mixing regimes and surface characteristics. The group averaged values of <span class="hlt">CO</span><span class="hlt">2</span> concentration from model simulations and observations are used to evaluate the regional model results. Using the group averaged measurements of <span class="hlt">CO</span><span class="hlt">2</span> reduces the noise of individual stations. The difference of group averaged values between observation and modeled results reflects the uncertainties of the large scale <span class="hlt">flux</span> in the region where the grouped stations are. We compared the group averaged values between model results with two biospheric <span class="hlt">fluxes</span> from the model Carnegie-Ames-Stanford-Approach (CASA) and VEgetation-Global-Atmosphere-Soil (VEGAS) and observations to evaluate the regional model results. Results show that the modeling group averaged values of <span class="hlt">CO</span><span class="hlt">2</span> concentrations in all regions with <span class="hlt">fluxes</span> from VEGAS have significant improvements for most regions. There is still large difference between two model results and observations for grouped average values in North Atlantic, Indian Ocean, and South Pacific Tropics. This implies possible large uncertainties in the <span class="hlt">fluxes</span> there.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B42C..03H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B42C..03H"><span>Response of surface CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> to whole ecosystem warming and elevated <span class="hlt">CO</span><span class="hlt">2</span> in a boreal black spruce peatland, northern Minnesota</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hsieh, I. F.; Gill, A. L.; Finzi, A.</p> <p>2017-12-01</p> <p>Potential increase in peatland C losses by environmental change has been presented by impacting the balance of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 sequestration and release. While temperature warming may accelerate the temperature-sensitive processes and release <span class="hlt">CO</span><span class="hlt">2</span> and CH4 from peat C stores, factors associated with warming and that associated with elevated <span class="hlt">CO</span><span class="hlt">2</span> concentration may alter the intrinsic characteristics of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 emission from peatland. By leveraging Spruce and Peatland Responses Under Changing Environments (SPRUCE) experiment, we measured peat surface <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> and their i13C signatures across a gradient of warming temperatures in a boreal black spruce peat bog in 2015 and 2016 growing seasons. Elevated <span class="hlt">CO</span><span class="hlt">2</span> (e<span class="hlt">CO</span><span class="hlt">2</span>) treatment was added to the warming experiment in June, 2016. Our results show both CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> increased with warming temperature in the two-year measurement period. Total emission for both gases were higher in 2016 with whole ecosystem warming than that in 2015 with deep peat heat warming. The 2016 increase in <span class="hlt">CO</span><span class="hlt">2</span> emission was significantly larger in the hummock microtopographic position compared to hollows. The opposite was true for CH4 <span class="hlt">fluxes</span>, where the increase was strongest in the hollows. In fact, CH4 <span class="hlt">flux</span> from hummocks declined in 2016 compared to 2015, suggesting lower overall rates of CH4 production and/or greater rates of methanotrophy. The increase (less depleted) in i13C -CH4 signatures suggest acetoclastic methanogensis increased its contribution to total CH4 production across the growing season and in response to experimental warming, while hydrogenotrophic methanogenesis dominated total CH4 production. On the contrary, results of i13C-<span class="hlt">CO</span><span class="hlt">2</span> show no significant change in the contribution of different sources to total <span class="hlt">CO</span><span class="hlt">2</span> emission through time or across warming temperature. On the other hand, i13C-<span class="hlt">CO</span><span class="hlt">2</span> signatures under <span class="hlt">CO</span><span class="hlt">2</span> fumigation in 2016 was significantly depleted since the e<span class="hlt">CO</span><span class="hlt">2</span> initiation, indicating a rapid increase in plant</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010022518','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010022518"><span>BOREAS TGB-5 <span class="hlt">CO</span><span class="hlt">2</span>, CH4 and <span class="hlt">CO</span> Chamber <span class="hlt">Flux</span> Data Over the NSA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Burke, Roger; Hall, Forrest G. (Editor); Conrad, Sara K. (Editor); Zepp, Richard</p> <p>2000-01-01</p> <p>The BOReal Ecosystem-Atmosphere Study Trace Gas Biogeochemistry (BOREAS TGB-5) team collected a variety of trace gas concentration and <span class="hlt">flux</span> measurements at several NSA sites. This data set contains carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), methane (CH4), and carbon monoxide (<span class="hlt">CO</span>) chamber <span class="hlt">flux</span> measurements conducted in 1994 at upland forest sites that experienced stand-replacement fires. These measurements were acquired to understand the impact of fires on soil biogeochemistry and related changes in trace gas exchange in boreal forest soils. Relevant ancillary data, including data concerning the soil temperature, solar irradiance, and information from nearby un-burned control sites, are included to provide a basis for modeling the regional impacts of fire and climate changes on trace gas biogeochemistry. The data are provided in tabular ASCII files.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014594','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014594"><span>Ocean Winds and Turbulent <span class="hlt">Air</span>-Sea <span class="hlt">Fluxes</span> Inferred From Remote Sensing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bourassa, Mark A.; Gille, Sarah T.; Jackson, Daren L.; Roberts, J. Brent; Wick, Gary A.</p> <p>2010-01-01</p> <p><span class="hlt">Air</span>-sea turbulent <span class="hlt">fluxes</span> determine the exchange of momentum, heat, freshwater, and gas between the atmosphere and ocean. These exchange processes are critical to a broad range of research questions spanning length scales from meters to thousands of kilometers and time scales from hours to decades. Examples are discussed (section <span class="hlt">2</span>). The estimation of surface turbulent <span class="hlt">fluxes</span> from satellite is challenging and fraught with considerable errors (section 3); however, recent developments in retrievals (section 3) will greatly reduce these errors. Goals for the future observing system are summarized in section 4. Surface <span class="hlt">fluxes</span> are defined as the rate per unit area at which something (e.g., momentum, energy, moisture, or <span class="hlt">CO</span> Z ) is transferred across the <span class="hlt">air</span>/sea interface. Wind- and buoyancy-driven surface <span class="hlt">fluxes</span> are called surface turbulent <span class="hlt">fluxes</span> because the mixing and transport are due to turbulence. Examples of nonturbulent processes are radiative <span class="hlt">fluxes</span> (e.g., solar radiation) and precipitation (Schmitt et al., 2010). Turbulent <span class="hlt">fluxes</span> are strongly dependent on wind speed; therefore, observations of wind speed are critical for the calculation of all turbulent surface <span class="hlt">fluxes</span>. Wind stress, the vertical transport of horizontal momentum, also depends on wind direction. Stress is very important for many ocean processes, including upper ocean currents (Dohan and Maximenko, 2010) and deep ocean currents (Lee et al., 2010). On short time scales, this horizontal transport is usually small compared to surface <span class="hlt">fluxes</span>. For long-term processes, transport can be very important but again is usually small compared to surface <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMOS22B..07M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMOS22B..07M"><span>Wintertime <span class="hlt">Air</span>-Sea Gas Transfer Rates and <span class="hlt">Air</span> Injection <span class="hlt">Fluxes</span> at Station Papa in the NE Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McNeil, C.; Steiner, N.; Vagle, S.</p> <p>2008-12-01</p> <p>In recent studies of <span class="hlt">air</span>-sea <span class="hlt">fluxes</span> of N<span class="hlt">2</span> and O<span class="hlt">2</span> in hurricanes, McNeil and D'Asaro (2007) used a simplified model formulation of <span class="hlt">air</span>-sea gas <span class="hlt">flux</span> to estimate simultaneous values of gas transfer rate, KT, and <span class="hlt">air</span> injection <span class="hlt">flux</span>, VT. The model assumes <span class="hlt">air</span>-sea gas <span class="hlt">fluxes</span> at high to extreme wind speeds can be explained by a combination of two processes: 1) <span class="hlt">air</span> injection, by complete dissolution of small bubbles drawn down into the ocean boundary layer by turbulent currents, and <span class="hlt">2</span>) near-surface equilibration processes, such as occurs within whitecaps. This analysis technique relies on <span class="hlt">air</span>-sea gas <span class="hlt">flux</span> estimates for two gases, N<span class="hlt">2</span> and O<span class="hlt">2</span>, to solve for the two model parameters, KT and VT. We present preliminary results of similar analysis of time series data collected during winter storms at Station Papa in the NE Pacific during 2003/2004. The data show a clear increase in KT and VT with increasing NCEP derived wind speeds and acoustically measured bubble penetration depth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B43E2180T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B43E2180T"><span><span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> in a Spartina salt marsh and brackish Phragmites marsh in Massachusetts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, J.; Wang, F.; Kroeger, K. D.; Gonneea, M. E.</p> <p>2017-12-01</p> <p>Coastal salt marshes play an important role in global and regional carbon cycling. Tidally restricted marshes reduce salinity and provide a habitat suitable for Phragmites invasion. We measured greenhouse gas (GHG) emissions (<span class="hlt">CO</span><span class="hlt">2</span> and CH4) continuously with the eddy covariance method and biweekly with the static chamber method in a Spartina salt marsh and a Phragmites marsh on Cape Cod, Massachusetts, USA. We did not find significant difference in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> between the two sites, but the CH4 <span class="hlt">fluxes</span> were much higher in the Phragmites site than the Spartina marsh. Temporally, tidal cycles influence the <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> in both sites. We found that the salt marsh was a significant carbon sink when <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> were combined. Restoring tidally restricted marshes will significantly reduce CH4 emissions and provide a strong ecosystem carbon service.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860038376&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dmarginal','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860038376&hterms=marginal&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dmarginal"><span>Coupled <span class="hlt">ice</span>-ocean dynamics in the marginal <span class="hlt">ice</span> zones Upwelling/downwelling and eddy generation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hakkinen, S.</p> <p>1986-01-01</p> <p>This study is aimed at modeling mesoscale processes such as upwelling/downwelling and <span class="hlt">ice</span> edge eddies in the marginal <span class="hlt">ice</span> zones. A two-dimensional coupled <span class="hlt">ice</span>-ocean model is used for the study. The <span class="hlt">ice</span> model is coupled to the reduced gravity ocean model through interfacial stresses. The parameters of the ocean model were chosen so that the dynamics would be nonlinear. The model was tested by studying the dynamics of upwelling. Wings parallel to the <span class="hlt">ice</span> edge with the <span class="hlt">ice</span> on the right produce upwelling because the <span class="hlt">air-ice</span> momentum <span class="hlt">flux</span> is much greater than <span class="hlt">air</span>-ocean momentum <span class="hlt">flux</span>; thus the Ekman transport is greater than the <span class="hlt">ice</span> than in the open water. The stability of the upwelling and downwelling jets is discussed. The downwelling jet is found to be far more unstable than the upwelling jet because the upwelling jet is stabilized by the divergence. The constant wind field exerted on a varying <span class="hlt">ice</span> cover will generate vorticity leading to enhanced upwelling/downwelling regions, i.e., wind-forced vortices. Steepening and strengthening of vortices are provided by the nonlinear terms. When forcing is time-varying, the advection terms will also redistribute the vorticity. The wind reversals will separate the vortices from the <span class="hlt">ice</span> edge, so that the upwelling enhancements are pushed to the open ocean and the downwelling enhancements are pushed underneath the <span class="hlt">ice</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JCrGr.289..605W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JCrGr.289..605W"><span><span class="hlt">Flux</span> growth of high-quality <span class="hlt">Co</span>Fe <span class="hlt">2</span>O 4 single crystals and their characterization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, W. H.; Ren, X.</p> <p>2006-04-01</p> <p>We report the growth of high-quality <span class="hlt">Co</span>Fe <span class="hlt">2</span>O 4 single crystals using a borax <span class="hlt">flux</span> method. The crystals were characterized by powder X-ray diffraction, electron probe microanalysis and Raman spectroscopy. We found the crystals are <span class="hlt">flux</span>-free and highly homogeneous in composition. X-ray rocking curves of the <span class="hlt">Co</span>Fe <span class="hlt">2</span>O 4 single crystals showed a full-width at half-maximum of 0.15°. The saturation magnetization of the <span class="hlt">Co</span>Fe <span class="hlt">2</span>O 4 single crystals was measured to be 90 emu/g or equivalently 3.65 μ B/f.u. at 5 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=309452','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=309452"><span>Changes in <span class="hlt">fluxes</span> of heat, H<span class="hlt">2</span>O, <span class="hlt">CO</span><span class="hlt">2</span> caused by a large wind farm</span></a></p> <p><a target="_blank" href="https://www.ars.usda.gov/research/publications/find-a-publication/">USDA-ARS?s Scientific Manuscript database</a></p> <p></p> <p></p> <p>The Crop Wind Energy Experiment (CWEX) provides a platform to investigate the effect of wind turbines and large wind farms on surface <span class="hlt">fluxes</span> of momentum, heat, moisture and carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>). In 2010 and 2011, eddy covariance <span class="hlt">flux</span> stations were installed between two lines of turbines at the south...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN13B0074H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN13B0074H"><span>Comparisons of a Quantum Annealing and Classical Computer Neural Net Approach for Inferring Global Annual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> over Land</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halem, M.; Radov, A.; Singh, D.</p> <p>2017-12-01</p> <p>Investigations of mid to high latitude atmospheric <span class="hlt">CO</span><span class="hlt">2</span> show growing amplitudes in seasonal variations over the past several decades. Recent high-resolution satellite measurements of <span class="hlt">CO</span><span class="hlt">2</span> concentration are now available for three years from the Orbiting Carbon Observatory-<span class="hlt">2</span>. The Atmospheric Radiation Measurement (ARM) program of DOE has been making long-term <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">flux</span> measurements (in addition to <span class="hlt">CO</span><span class="hlt">2</span> concentration and an array of other meteorological quantities) at several towers and mobile sites located around the globe at half-hour frequencies. Recent papers have shown <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> inferred by assimilating <span class="hlt">CO</span><span class="hlt">2</span> observations into ecosystem models are largely inconsistent with station observations. An investigation of how the biosphere has reacted to changes in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> is essential to our understanding of potential climate-vegetation feedbacks. Thus, new approaches for calculating <span class="hlt">CO</span><span class="hlt">2</span>-<span class="hlt">flux</span> for assimilation into land surface models are necessary for improving the prediction of annual carbon uptake. In this study, we calculate and compare the predicted <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> results employing a Feed Forward Backward Propagation Neural Network model on two architectures, (i) an IBM Minsky Computer node and (ii) a hybrid version of the ARC D-Wave quantum annealing computer. We compare the neural net results of predictions of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from ARM station data for three different DOE ecosystem sites; an arid plains near Oklahoma City, a northern arctic site at Barrows AL, and a tropical rainforest site in the Amazon. Training times and predictive results for the calculating annual <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the two architectures for each of the three sites are presented. Comparative results of predictions as measured by RMSE and MAE are discussed. Plots and correlations of observed vs predicted <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> are also presented for all three sites. We show the estimated training times for quantum and classical calculations when extended to calculating global annual Carbon Uptake over land. We also</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15825257','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15825257"><span>Effects of <span class="hlt">air</span> velocity on photosynthesis of plant canopies under elevated <span class="hlt">CO</span><span class="hlt">2</span> levels in a plant culture system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kitaya, Y; Shibuya, T; Yoshida, M; Kiyota, M</p> <p>2004-01-01</p> <p>To obtain basic data for adequate <span class="hlt">air</span> circulation for promoting plant growth in closed plant production modules in bioregenerative life support systems in space, effects of <span class="hlt">air</span> velocities ranging from 0.1 to 0.8 m s-1 on photosynthesis in tomato seedlings canopies were investigated under atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations of 0.4 and 0.8 mmol mol-1. The canopy of tomato seedlings on a plug tray (0.4 x 0.4 m<span class="hlt">2</span>) was set in a wind-tunnel-type chamber (0.6 x 0.4 x 0.3 m3) installed in a semi-closed-type assimilation chamber (0.9 x 0.5 x 0.4 m3). The net photosynthetic rate in the plant canopy was determined with the differences in <span class="hlt">CO</span><span class="hlt">2</span> concentrations between the inlet and outlet of the assimilation chamber multiplied by the volumetric <span class="hlt">air</span> exchange rate of the chamber. Photosynthetic photon <span class="hlt">flux</span> (PPF) on the plant canopy was kept at 0.25 mmol m-<span class="hlt">2</span> s-1, <span class="hlt">air</span> temperature at 23 degrees C and relative humidity at 55%. The leaf area indices (LAIs) of the plant canopies were 0.6-<span class="hlt">2</span>.5 and plant heights were 0.05-0.<span class="hlt">2</span> m. The net photosynthetic rate of the plant canopy increased with increasing <span class="hlt">air</span> velocities inside plant canopies and saturated at 0.<span class="hlt">2</span> m s-1. The net photosynthetic rate at the <span class="hlt">air</span> velocity of 0.4 m s-1 was 1.3 times that at 0.1 m s-1 under <span class="hlt">CO</span><span class="hlt">2</span> concentrations of 0.4 and 0.8 mmol mol-1. The net photosynthetic rate under <span class="hlt">CO</span><span class="hlt">2</span> concentrations of 0.8 mmol mol-1 was 1.<span class="hlt">2</span> times that under 0.4 mmol mol-1 at the <span class="hlt">air</span> velocity ranging from 0.1 to 0.8 m s-1. The results confirmed the importance of controlling <span class="hlt">air</span> movement for enhancing the canopy photosynthesis under an elevated <span class="hlt">CO</span><span class="hlt">2</span> level as well as under a normal <span class="hlt">CO</span><span class="hlt">2</span> level in the closed plant production modules. c2004 COSPAR. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.B33E1085H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.B33E1085H"><span>Simultaneous Micrometeorological <span class="hlt">Flux</span> Observations of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 at a Sub-Arctic Black-Spruce Forest in Alaska</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harazono, Y.; Ueyama, M.; Miyata, A.</p> <p>2005-12-01</p> <p>Carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) and methane (CH4) <span class="hlt">fluxes</span> were measured at a black spruce forest over discontinuous permafrost in central Alaska since November 2002. <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was measured by open-path eddy correlation system and CH4 <span class="hlt">flux</span> was measured by gradient method continuously. <span class="hlt">CO</span><span class="hlt">2</span> uptake was observed during daytime after DOY 60 when the forest floor was snow-covered with low temperature (<-10 °C). At the moment, CH4 <span class="hlt">flux</span> was negative (uptake) during daytime and nearing to zero at night, which varied with surface temperature. During snow melt and following permafrost thawing periods (around DOY 110-140, 2003), nocturnal <span class="hlt">CO</span><span class="hlt">2</span> efflux was larger than daytime uptake resulted in a daily <span class="hlt">CO</span><span class="hlt">2</span> source, and CH4 <span class="hlt">flux</span> became small positive in daytime and nearing zero at night resulted in a weak daily CH4 source. After DOY 140 in 2003, <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was strong uptake and the maximum level was 1.0 g m-<span class="hlt">2</span> h-1 in late July around 10:30h when 3 hr earlier than solar noon. During mid summer (DOY 180-230, 2003), daytime CH4 uptake was weak and was near zero at night resulted in a weak daily CH4 sink. 2004 was low snow fall and draught summer, the seasonal patterns of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> shifted more than 3-weeks earlier than that in 2003, resulted in high <span class="hlt">CO</span><span class="hlt">2</span> and CH4 emissions in early summer. Daily amount of CH4 <span class="hlt">flux</span> in mid summer 2003 and 2004 were 1.<span class="hlt">2</span> and 0.5 mg CH4 m-<span class="hlt">2</span> d-1, respectively. Sum of observed NEE and <span class="hlt">CO</span><span class="hlt">2</span> storage term within the canopy, NEP were -482 and -366.6 g<span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> y-1 in 2003 and 2004. However, application of u* filtering correction made NEP reduce to the ranges between -434.8 and -315.9 g<span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> y-1 (under u<0.05 ms-1 and u<0.<span class="hlt">2</span> ms-1) in 2003 and to -282.5 and -215.9 g<span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> y-1 in 2004. The low NEP in 2004 was caused by high temperature and low precipitation during growing season. CH4 emission was also higher in 2004. <span class="hlt">CO</span><span class="hlt">2</span> and CH4 exchanges at sub-arctic forest were quite sensitive to draught and summer temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PPCF...59f4004A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PPCF...59f4004A"><span>High <span class="hlt">flux</span>, beamed neutron sources employing deuteron-rich ion beams from D<span class="hlt">2</span>O-<span class="hlt">ice</span> layered targets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alejo, A.; Krygier, A. G.; Ahmed, H.; Morrison, J. T.; Clarke, R. J.; Fuchs, J.; Green, A.; Green, J. S.; Jung, D.; Kleinschmidt, A.; Najmudin, Z.; Nakamura, H.; Norreys, P.; Notley, M.; Oliver, M.; Roth, M.; Vassura, L.; Zepf, M.; Borghesi, M.; Freeman, R. R.; Kar, S.</p> <p>2017-06-01</p> <p>A forwardly-peaked bright neutron source was produced using a laser-driven, deuteron-rich ion beam in a pitcher-catcher scenario. A proton-free ion source was produced via target normal sheath acceleration from Au foils having a thin layer of D<span class="hlt">2</span>O <span class="hlt">ice</span> at the rear side, irradiated by sub-petawatt laser pulses (˜200 J, ˜750 fs) at peak intensity ˜ <span class="hlt">2</span>× {10}20 {{W}} {{cm}}-<span class="hlt">2</span>. The neutrons were preferentially produced in a beam of ˜70° FWHM cone along the ion beam forward direction, with maximum energy up to ˜40 MeV and a peak <span class="hlt">flux</span> along the axis ˜ <span class="hlt">2</span>× {10}9 {{n}} {{sr}}-1 for neutron energy above <span class="hlt">2</span>.5 MeV. The experimental data is in good agreement with the simulations carried out for the d(d,n)3He reaction using the deuteron beam produced by the <span class="hlt">ice</span>-layered target.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28841262','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28841262"><span>Measuring 13 C-enriched <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> with a cavity ring-down spectroscopy gas analyser: Evaluation and calibration.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dickinson, Dane; Bodé, Samuel; Boeckx, Pascal</p> <p>2017-11-30</p> <p>Cavity ring-down spectroscopy (CRDS) is becoming increasingly popular for δ 13 C-<span class="hlt">CO</span> <span class="hlt">2</span> analysis of <span class="hlt">air</span>. However, little is known about the effect of high 13 C abundances on the performance of CRDS. Overlap between 12 <span class="hlt">CO</span> <span class="hlt">2</span> and 13 <span class="hlt">CO</span> <span class="hlt">2</span> spectral lines may adversely affect isotopic-<span class="hlt">CO</span> <span class="hlt">2</span> CRDS measurements of 13 C-enriched samples. Resolving this issue is important so that CRDS analysers can be used in <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> studies involving 13 C-labelled tracers. We tested a Picarro G2131-i CRDS isotopic-<span class="hlt">CO</span> <span class="hlt">2</span> gas analyser with specialty gravimetric standards of widely varying 13 C abundance (from natural to 20.1 atom%) and <span class="hlt">CO</span> <span class="hlt">2</span> mole fraction (x<span class="hlt">CO</span> <span class="hlt">2</span> : <0.1 to 2116 ppm) in synthetic <span class="hlt">air</span>. The presence of spectroscopic interference between 12 <span class="hlt">CO</span> <span class="hlt">2</span> and 13 <span class="hlt">CO</span> <span class="hlt">2</span> bands was assessed by analysing errors in measurements of the standards. A multi-component calibration strategy was adopted, incorporating isotope ratio and mole fraction data to ensure accuracy and consistency in corrected values of δ 13 C-<span class="hlt">CO</span> <span class="hlt">2</span> , x 12 <span class="hlt">CO</span> <span class="hlt">2</span> , and x 13 <span class="hlt">CO</span> <span class="hlt">2</span> . CRDS measurements of x 13 <span class="hlt">CO</span> <span class="hlt">2</span> were found to be accurate throughout the tested range (<0.005 to 100 ppm). On the other hand, spectral cross-talk in x 12 <span class="hlt">CO</span> <span class="hlt">2</span> measurements of standards containing elevated levels of 13 <span class="hlt">CO</span> <span class="hlt">2</span> led to inaccuracy in x 12 <span class="hlt">CO</span> <span class="hlt">2</span> , total-x<span class="hlt">CO</span> <span class="hlt">2</span> (x 12 <span class="hlt">CO</span> <span class="hlt">2</span>  + x 13 <span class="hlt">CO</span> <span class="hlt">2</span> ), and δ 13 C-<span class="hlt">CO</span> <span class="hlt">2</span> data. An empirical relationship for x 12 <span class="hlt">CO</span> <span class="hlt">2</span> measurements that incorporated the 13 C/ 12 C isotope ratio (i.e. 13 <span class="hlt">CO</span> <span class="hlt">2</span> / 12 <span class="hlt">CO</span> <span class="hlt">2</span> , RCO<span class="hlt">2</span>) as a secondary (non-linear) variable was found to compensate for the perturbations, and enabled accurate instrument calibration for all <span class="hlt">CO</span> <span class="hlt">2</span> compositions covered by our standard gases. 13 C-enrichement in <span class="hlt">CO</span> <span class="hlt">2</span> leads to minor errors in CRDS measurements of x 12 <span class="hlt">CO</span> <span class="hlt">2</span> . We propose an empirical correction for measurements of 13 C-enriched <span class="hlt">CO</span> <span class="hlt">2</span> in <span class="hlt">air</span> by CRDS instruments such as the Picarro G2131-i. Copyright © 2017 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013A%26A...557A...6K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013A%26A...557A...6K"><span>Clouds in the atmospheres of extrasolar planets. IV. On the scattering greenhouse effect of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles: Numerical radiative transfer studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kitzmann, D.; Patzer, A. B. C.; Rauer, H.</p> <p>2013-09-01</p> <p>Context. Owing to their wavelength-dependent absorption and scattering properties, clouds have a strong impact on the climate of planetary atmospheres. The potential greenhouse effect of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds in the atmospheres of terrestrial extrasolar planets is of particular interest because it might influence the position and thus the extension of the outer boundary of the classic habitable zone around main sequence stars. Such a greenhouse effect, however, is a complicated function of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles' optical properties. Aims: We study the radiative effects of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles obtained by different numerical treatments to solve the radiative transfer equation. To determine the effectiveness of the scattering greenhouse effect caused by <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds, the radiative transfer calculations are performed over the relevant wide range of particle sizes and optical depths, employing different numerical methods. Methods: We used Mie theory to calculate the optical properties of particle polydispersion. The radiative transfer calculations were done with a high-order discrete ordinate method (DISORT). Two-stream radiative transfer methods were used for comparison with previous studies. Results: The comparison between the results of a high-order discrete ordinate method and simpler two-stream approaches reveals large deviations in terms of a potential scattering efficiency of the greenhouse effect. The two-stream methods overestimate the transmitted and reflected radiation, thereby yielding a higher scattering greenhouse effect. For the particular case of a cool M-type dwarf, the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> particles show no strong effective scattering greenhouse effect by using the high-order discrete ordinate method, whereas a positive net greenhouse effect was found for the two-stream radiative transfer schemes. As a result, previous studies of the effects of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> clouds using two-stream approximations overrated the atmospheric warming caused by the scattering greenhouse effect</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...852...59C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...852...59C"><span>Origin of the High-energy Neutrino <span class="hlt">Flux</span> at <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carceller, J. M.; Illana, J. I.; Masip, M.; Meloni, D.</p> <p>2018-01-01</p> <p>We discuss the spectrum of the different components in the astrophysical neutrino <span class="hlt">flux</span> reaching the Earth, and the possible contribution of each component to the high-energy <span class="hlt">Ice</span>Cube data. We show that the diffuse <span class="hlt">flux</span> from cosmic ray (CR) interactions with gas in our galaxy implies just two events among the 54-event sample. We argue that the neutrino <span class="hlt">flux</span> from CR interactions in the intergalactic (intracluster) space depends critically on the transport parameter δ describing the energy dependence in the diffusion coefficient of galactic CRs. Our analysis motivates a {E}-<span class="hlt">2</span>.1 neutrino spectrum with a drop at PeV energies that fits the data well, including the non-observation of the Glashow resonance at 6.3 PeV. We also show that a CR <span class="hlt">flux</span> described by an unbroken power law may produce a neutrino <span class="hlt">flux</span> with interesting spectral features (bumps and breaks) related to changes in the CR composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AtmEn.143..164W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AtmEn.143..164W"><span>Temporal variability in the sources and <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> in a residential area in an evergreen subtropical city</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weissert, L. F.; Salmond, J. A.; Turnbull, J. C.; Schwendenmann, L.</p> <p>2016-10-01</p> <p>Measurements of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in temperate climates have shown that urban areas are a net source of <span class="hlt">CO</span><span class="hlt">2</span> and that photosynthetic <span class="hlt">CO</span><span class="hlt">2</span> uptake is generally not sufficient to offset local <span class="hlt">CO</span><span class="hlt">2</span> emissions. However, little is known about the role of vegetation in cities where biogenic <span class="hlt">CO</span><span class="hlt">2</span> uptake is not limited to a <span class="hlt">2</span>-8 months growing season. This study used the eddy covariance technique to quantify the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> over a period of 12 months in a residential area in subtropical Auckland, New Zealand, where the vegetation cover (surface cover fraction: 47%) is dominated by evergreen vegetation. Radiocarbon isotope measurements of <span class="hlt">CO</span><span class="hlt">2</span> were conducted at three different times of the day (06:00-09:00, 12:00-15:00, 01:00-04:00) for four consecutive weekdays in summer and winter to differentiate anthropogenic sources of <span class="hlt">CO</span><span class="hlt">2</span> (fossil fuel combustion) from biogenic sources (ecosystem respiration, combustion of biofuel/biomass). The results reveal previously unreported patterns for <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, with no seasonal variability and negative (net uptake) <span class="hlt">CO</span><span class="hlt">2</span> midday <span class="hlt">fluxes</span> throughout the year, demonstrating photosynthetic uptake by the evergreen vegetation all year-round. The winter radiocarbon measurements showed that 85% of the <span class="hlt">CO</span><span class="hlt">2</span> during the morning rush hour was attributed to fossil fuel emissions, when wind was from residential areas. However, for all other time periods radiocarbon measurements showed that fossil fuel combustion was not a large source of <span class="hlt">CO</span><span class="hlt">2</span>, suggesting that biogenic processes likely dominate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> at this residential site. Overall, our findings highlight the importance of vegetation in residential areas to mitigate local <span class="hlt">CO</span><span class="hlt">2</span> emissions, particularly in cities with a climate that allows evergreen vegetation to maintain high photosynthetic rates over winter. As urban areas grow, urban planners need to consider the role of urban greenspace to mitigate urban <span class="hlt">CO</span><span class="hlt">2</span> emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007BoLMe.124..161Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007BoLMe.124..161Y"><span>Influence of leaf water potential on diurnal changes in <span class="hlt">CO</span><span class="hlt">2</span> and water vapour <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Qiang; Xu, Shouhua; Wang, Jing; Lee, Xuhui</p> <p>2007-08-01</p> <p>Mass and energy <span class="hlt">fluxes</span> between the atmosphere and vegetation are driven by meteorological variables, and controlled by plant water status, which may change more markedly diurnally than soil water. We tested the hypothesis that integration of dynamic changes in leaf water potential may improve the simulation of <span class="hlt">CO</span><span class="hlt">2</span> and water <span class="hlt">fluxes</span> over a wheat canopy. Simulation of leaf water potential was integrated into a comprehensive model (the ChinaAgrosys) of heat, water and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and crop growth. Photosynthesis from individual leaves was integrated to the canopy by taking into consideration the attenuation of radiation when penetrating the canopy. Transpiration was calculated with the Shuttleworth-Wallace model in which canopy resistance was taken as a link between energy balance and physiological regulation. A revised version of the Ball-Woodrow-Berry stomatal model was applied to produce a new canopy resistance model, which was validated against measured <span class="hlt">CO</span><span class="hlt">2</span> and water vapour <span class="hlt">fluxes</span> over winter wheat fields in Yucheng (36°57' N, 116°36' E, 28 m above sea level) in the North China Plain during 1997, 2001 and 2004. Leaf water potential played an important role in causing stomatal conductance to fall at midday, which caused diurnal changes in photosynthesis and transpiration. Changes in soil water potential were less important. Inclusion of the dynamics of leaf water potential can improve the precision of the simulation of <span class="hlt">CO</span><span class="hlt">2</span> and water vapour <span class="hlt">fluxes</span>, especially in the afternoon under water stress conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/23725','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/23725"><span>Seasonal patterns in soil surface <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> under snow cover in 50 and 300 year old subalpine forests</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Robert M. Hubbard; Michael G. Ryan; Kelly Elder; Charles C. Rhoades</p> <p>2005-01-01</p> <p>Soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> can contribute as much as 60-80% of total ecosystem respiration in forests. Although considerable research has focused on quantifying this <span class="hlt">flux</span> during the growing season, comparatively little effort has focused on non-growing season <span class="hlt">fluxes</span>. We measured soil <span class="hlt">CO</span><span class="hlt">2</span> efflux through snow in 50 and 300 year old subalpine forest stands near Fraser <span class="hlt">CO</span>. Our...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GBioC..31.1192G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GBioC..31.1192G"><span>Global evaluation of particulate organic carbon <span class="hlt">flux</span> parameterizations and implications for atmospheric p<span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gloege, Lucas; McKinley, Galen A.; Mouw, Colleen B.; Ciochetto, Audrey B.</p> <p>2017-07-01</p> <p>The shunt of photosynthetically derived particulate organic carbon (POC) from the euphotic zone and deep remineralization comprises the basic mechanism of the "biological carbon pump." POC raining through the "twilight zone" (euphotic depth to 1 km) and "midnight zone" (1 km to 4 km) is remineralized back to inorganic form through respiration. Accurately modeling POC <span class="hlt">flux</span> is critical for understanding the "biological pump" and its impacts on <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange and, ultimately, long-term ocean carbon sequestration. Yet commonly used parameterizations have not been tested quantitatively against global data sets using identical modeling frameworks. Here we use a single one-dimensional physical-biogeochemical modeling framework to assess three common POC <span class="hlt">flux</span> parameterizations in capturing POC <span class="hlt">flux</span> observations from moored sediment traps and thorium-234 depletion. The exponential decay, Martin curve, and ballast model are compared to data from 11 biogeochemical provinces distributed across the globe. In each province, the model captures satellite-based estimates of surface primary production within uncertainties. Goodness of fit is measured by how well the simulation captures the observations, quantified by bias and the root-mean-square error and displayed using "target diagrams." Comparisons are presented separately for the twilight zone and midnight zone. We find that the ballast hypothesis shows no improvement over a globally or regionally parameterized Martin curve. For all provinces taken together, Martin's b that best fits the data is [0.70, 0.98]; this finding reduces by at least a factor of 3 previous estimates of potential impacts on atmospheric p<span class="hlt">CO</span><span class="hlt">2</span> of uncertainty in POC export to a more modest range [-16 ppm, +12 ppm].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.3717S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.3717S"><span>The Coca-campaign: An Attempt To Derive The Carbon Exchange of A Forested Region Using Airborne <span class="hlt">Co</span><span class="hlt">2</span> and <span class="hlt">Co</span> Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmitgen, S.; Ciais, P.; Geiß, H.; Kley, D.; Neininger, B.; Baeumle, M.; Fuchs, W.; Brunet, Y.</p> <p></p> <p>As part of the project COCA an attempt was made to measure the daytime biogenic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> over a forest area (about 15 by 30 km). This campaign took place around the CARBOEUROFLUX site "Le Bray" (Pinus pinaster) close to Bordeaux in France end of June 2001. Based on continuous airborne <span class="hlt">CO</span><span class="hlt">2</span>, H<span class="hlt">2</span>O and <span class="hlt">CO</span> <span class="hlt">flux</span> and concen- tration measurements a Lagrangian budgeting approach was chosen for the determi- nation of the regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The objective is to determine the <span class="hlt">CO</span><span class="hlt">2</span> uptake of the extended forest area from the <span class="hlt">CO</span><span class="hlt">2</span>/<span class="hlt">CO</span> gradients up- and downwind of the ecosystem, using <span class="hlt">CO</span> as <span class="hlt">air</span> mass tracer and such eliminating the influence of anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> advected into the area. First results will be shown of a flight on June 23rd, where fair wind speeds (about 5 m/s) and a low CBL height led to the observation of a clear decrease in <span class="hlt">CO</span><span class="hlt">2</span> at the downwind flight stacks with basically constant <span class="hlt">CO</span> concentrations. For other flights with very low wind speeds, local effects dominate the observa- tions leading to a larger variability in the observations. Both, correlations and anti- correlations of <span class="hlt">CO</span><span class="hlt">2</span> with the anthropogenic tracer <span class="hlt">CO</span> have been observed. Positive correlations indicate fresh plumes of anthropogenic <span class="hlt">CO</span><span class="hlt">2</span>. Negative correlations are indicative of entrainment of free tropospheric <span class="hlt">air</span>, that was marked by relatively higher <span class="hlt">CO</span><span class="hlt">2</span> and lower <span class="hlt">CO</span> concentrations than the average CBL concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.4781F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.4781F"><span>Consistent regional <span class="hlt">fluxes</span> of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> inferred from GOSAT proxy XCH4 : XCO<span class="hlt">2</span> retrievals, 2010-2014</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feng, Liang; Palmer, Paul I.; Bösch, Hartmut; Parker, Robert J.; Webb, Alex J.; Correia, Caio S. C.; Deutscher, Nicholas M.; Domingues, Lucas G.; Feist, Dietrich G.; Gatti, Luciana V.; Gloor, Emanuel; Hase, Frank; Kivi, Rigel; Liu, Yi; Miller, John B.; Morino, Isamu; Sussmann, Ralf; Strong, Kimberly; Uchino, Osamu; Wang, Jing; Zahn, Andreas</p> <p>2017-04-01</p> <p>We use the GEOS-Chem global 3-D model of atmospheric chemistry and transport and an ensemble Kalman filter to simultaneously infer regional <span class="hlt">fluxes</span> of methane (CH4) and carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) directly from GOSAT retrievals of XCH4 : XCO<span class="hlt">2</span>, using sparse ground-based CH4 and <span class="hlt">CO</span><span class="hlt">2</span> mole fraction data to anchor the ratio. This work builds on the previously reported theory that takes into account that (1) these ratios are less prone to systematic error than either the full-physics data products or the proxy CH4 data products; and (<span class="hlt">2</span>) the resulting CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are self-consistent. We show that a posteriori <span class="hlt">fluxes</span> inferred from the GOSAT data generally outperform the <span class="hlt">fluxes</span> inferred only from in situ data, as expected. GOSAT CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are consistent with global growth rates for <span class="hlt">CO</span><span class="hlt">2</span> and CH4 reported by NOAA and have a range of independent data including new profile measurements (0-7 km) over the Amazon Basin that were collected specifically to help validate GOSAT over this geographical region. We find that large-scale multi-year annual a posteriori <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> inferred from GOSAT data are similar to those inferred from the in situ surface data but with smaller uncertainties, particularly over the tropics. GOSAT data are consistent with smaller peak-to-peak seasonal amplitudes of <span class="hlt">CO</span><span class="hlt">2</span> than either the a priori or in situ inversion, particularly over the tropics and the southern extratropics. Over the northern extratropics, GOSAT data show larger uptake than the a priori but less than the in situ inversion, resulting in small net emissions over the year. We also find evidence that the carbon balance of tropical South America was perturbed following the droughts of 2010 and 2012 with net annual <span class="hlt">fluxes</span> not returning to an approximate annual balance until 2013. In contrast, GOSAT data significantly changed the a priori spatial distribution of CH4 emission with a 40 % increase over tropical South America and tropical Asia and a smaller decrease over Eurasia and temperate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27400026','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27400026"><span>Contrasting ecosystem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> of inland and coastal wetlands: a meta-analysis of eddy covariance data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lu, Weizhi; Xiao, Jingfeng; Liu, Fang; Zhang, Yue; Liu, Chang'an; Lin, Guanghui</p> <p>2017-03-01</p> <p>Wetlands play an important role in regulating the atmospheric carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span> ) concentrations and thus affecting the climate. However, there is still lack of quantitative evaluation of such a role across different wetland types, especially at the global scale. Here, we conducted a meta-analysis to compare ecosystem <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> among various types of wetlands using a global database compiled from the literature. This database consists of 143 site-years of eddy covariance data from 22 inland wetland and 21 coastal wetland sites across the globe. Coastal wetlands had higher annual gross primary productivity (GPP), ecosystem respiration (R e ), and net ecosystem productivity (NEP) than inland wetlands. On a per unit area basis, coastal wetlands provided large <span class="hlt">CO</span> <span class="hlt">2</span> sinks, while inland wetlands provided small <span class="hlt">CO</span> <span class="hlt">2</span> sinks or were nearly <span class="hlt">CO</span> <span class="hlt">2</span> neutral. The annual <span class="hlt">CO</span> <span class="hlt">2</span> sink strength was 93.15 and 208.37 g C m -<span class="hlt">2</span> for inland and coastal wetlands, respectively. Annual <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> were mainly regulated by mean annual temperature (MAT) and mean annual precipitation (MAP). For coastal and inland wetlands combined, MAT and MAP explained 71%, 54%, and 57% of the variations in GPP, R e , and NEP, respectively. The <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> of wetlands were also related to leaf area index (LAI). The <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> also varied with water table depth (WTD), although the effects of WTD were not statistically significant. NEP was jointly determined by GPP and R e for both inland and coastal wetlands. However, the NEP/R e and NEP/GPP ratios exhibited little variability for inland wetlands and decreased for coastal wetlands with increasing latitude. The contrasting of <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> between inland and coastal wetlands globally can improve our understanding of the roles of wetlands in the global C cycle. Our results also have implications for informing wetland management and climate change policymaking, for example, the efforts being made by international organizations and enterprises to restore coastal</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=321468','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=321468"><span>Comparing <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> data from eddy covariance methods with bowen ratio energy balance methods from contrasting soil management</span></a></p> <p><a target="_blank" href="https://www.ars.usda.gov/research/publications/find-a-publication/">USDA-ARS?s Scientific Manuscript database</a></p> <p></p> <p></p> <p>Measuring <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from contrasting soil management practices is important for understanding the role of agriculture in source-sink relationship with <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. There are several micrometeorological methods for measuring <span class="hlt">CO</span><span class="hlt">2</span> emissions, however all are expensive and thus do not easily lend themselve...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24066532','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24066532"><span>[Temperature sensitivity of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from rhizosphere soil mineralization and root decomposition in Pinus massoniana and Castanopsis sclerophylla forests].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Yu; Hu, Xiao-Fei; Chen, Fu-Sheng; Yuan, Ping-Cheng</p> <p>2013-06-01</p> <p>Rhizospheric and non-rhizospheric soils and the absorption, transition, and storage roots were sampled from the mid-subtropical Pinus massoniana and Castanopsis sclerophylla forests to study the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from soil mineralization and root decomposition in the forests. The samples were incubated in closed jars at 15 degrees C, 25 degrees C, 35 degrees C, and 45 degrees C, respectively, and alkali absorption method was applied to measure the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> during 53 days incubation. For the two forests, the rhizospheric effect (ratio of rhizospheric to non-rhizospheric soil) on the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from soil mineralization across all incubation temperature ranged from 1.12 to 3.09, with a decreasing trend along incubation days. There was no significant difference in the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from soil mineralization between the two forests at 15 degrees C, but the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was significantly higher in P. massoniana forest than in C. sclerophylla forest at 25 degrees C and 35 degrees C, and in an opposite pattern at 45 degrees C. At all incubation temperature, the <span class="hlt">CO</span><span class="hlt">2</span> release from the absorption root decomposition was higher than that from the transition and storage roots decomposition, and was smaller in P. massoniana than in C. sclerophylla forest for all the root functional types. The Q10 values of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from the two forests were higher for soils (1.21-1.83) than for roots (0.96-1.36). No significant differences were observed in the Q10 values of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from soil mineralization between the two forests, but the Q10 value of the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from root decomposition was significantly higher in P. massoniana than in C. sclerophylla forest. It was suggested that the increment of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from soil mineralization under global warming was far higher than that from root decomposition, and for P. massoniana than for C. sclerophylla forest. In subtropics of China, the adaptability of zonal climax community to global warming would be stronger than that of pioneer community.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeCoA.177...62P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeCoA.177...62P"><span>Measurements of 14C in ancient <span class="hlt">ice</span> from Taylor Glacier, Antarctica constrain in situ cosmogenic 14CH4 and 14<span class="hlt">CO</span> production rates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Petrenko, Vasilii V.; Severinghaus, Jeffrey P.; Schaefer, Hinrich; Smith, Andrew M.; Kuhl, Tanner; Baggenstos, Daniel; Hua, Quan; Brook, Edward J.; Rose, Paul; Kulin, Robb; Bauska, Thomas; Harth, Christina; Buizert, Christo; Orsi, Anais; Emanuele, Guy; Lee, James E.; Brailsford, Gordon; Keeling, Ralph; Weiss, Ray F.</p> <p>2016-03-01</p> <p>Carbon-14 (14C) is incorporated into glacial <span class="hlt">ice</span> by trapping of atmospheric gases as well as direct near-surface in situ cosmogenic production. 14C of trapped methane (14CH4) is a powerful tracer for past CH4 emissions from ;old; carbon sources such as permafrost and marine CH4 clathrates. 14C in trapped carbon dioxide (14<span class="hlt">CO</span><span class="hlt">2</span>) can be used for absolute dating of <span class="hlt">ice</span> cores. In situ produced cosmogenic 14C in carbon monoxide (14<span class="hlt">CO</span>) can potentially be used to reconstruct the past cosmic ray <span class="hlt">flux</span> and past solar activity. Unfortunately, the trapped atmospheric and in situ cosmogenic components of 14C in glacial <span class="hlt">ice</span> are difficult to disentangle and a thorough understanding of the in situ cosmogenic component is needed in order to extract useful information from <span class="hlt">ice</span> core 14C. We analyzed very large (≈1000 kg) <span class="hlt">ice</span> samples in the <span class="hlt">2</span>.26-19.53 m depth range from the ablation zone of Taylor Glacier, Antarctica, to study in situ cosmogenic production of 14CH4 and 14<span class="hlt">CO</span>. All sampled <span class="hlt">ice</span> is >50 ka in age, allowing for the assumption that most of the measured 14C originates from recent in situ cosmogenic production as ancient <span class="hlt">ice</span> is brought to the surface via ablation. Our results place the first constraints on cosmogenic 14CH4 production rates and improve on prior estimates of 14<span class="hlt">CO</span> production rates in <span class="hlt">ice</span>. We find a constant 14CH4/14<span class="hlt">CO</span> production ratio (0.0076 ± 0.0003) for samples deeper than 3 m, which allows the use of 14<span class="hlt">CO</span> for correcting the 14CH4 signals for the in situ cosmogenic component. Our results also provide the first unambiguous confirmation of 14C production by fast muons in a natural setting (<span class="hlt">ice</span> or rock) and suggest that the 14C production rates in <span class="hlt">ice</span> commonly used in the literature may be too high.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918076S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918076S"><span>True eddy accumulation and eddy covariance methods and instruments intercomparison for <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span>, CH4 and H<span class="hlt">2</span>O above the Hainich Forest</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Siebicke, Lukas</p> <p>2017-04-01</p> <p>The eddy covariance (EC) method is state-of-the-art in directly measuring vegetation-atmosphere exchange of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O at ecosystem scale. However, the EC method is currently limited to a small number of atmospheric tracers by the lack of suitable fast-response analyzers or poor signal-to-noise ratios. High resource and power demands may further restrict the number of spatial sampling points. True eddy accumulation (TEA) is an alternative method for direct and continuous <span class="hlt">flux</span> observations. Key advantages are the applicability to a wider range of <span class="hlt">air</span> constituents such as greenhouse gases, isotopes, volatile organic compounds and aerosols using slow-response analyzers. In contrast to relaxed eddy accumulation (REA), true eddy accumulation (Desjardins, 1977) has the advantage of being a direct method which does not require proxies. True Eddy Accumulation has the potential to overcome above mentioned limitations of eddy covariance but has hardly ever been successfully demonstrated in practice in the past. This study presents <span class="hlt">flux</span> measurements using an innovative approach to true eddy accumulation by directly, continuously and automatically measuring trace gas <span class="hlt">fluxes</span> using a flow-through system. We merge high-frequency <span class="hlt">flux</span> contributions from TEA with low-frequency covariances from the same sensors. We show <span class="hlt">flux</span> measurements of <span class="hlt">CO</span><span class="hlt">2</span>, CH4 and H<span class="hlt">2</span>O by TEA and EC above an old-growth forest at the ICOS <span class="hlt">flux</span> tower site "Hainich" (DE-Hai). We compare and evaluate the performance of the two direct turbulent <span class="hlt">flux</span> measurement methods eddy covariance and true eddy accumulation using side-by-side trace gas <span class="hlt">flux</span> observations. We further compare performance of seven instrument complexes, i.e. combinations of sonic anemometers and trace gas analyzers. We compare gas analyzers types of open-path, enclosed-path and closed-path design. We further differentiate data from two gas analysis technologies: infrared gas analysis (IRGA) and laser spectrometry (open path and CRDS closed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApJ...812..150M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApJ...812..150M"><span><span class="hlt">Ice</span> Chemistry on Outer Solar System Bodies: Electron Radiolysis of N<span class="hlt">2</span>-, CH4-, and <span class="hlt">CO</span>-Containing <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Materese, Christopher K.; Cruikshank, Dale P.; Sandford, Scott A.; Imanaka, Hiroshi; Nuevo, Michel</p> <p>2015-10-01</p> <p>Radiation processing of the surface <span class="hlt">ices</span> of outer Solar System bodies may be an important process for the production of complex chemical species. The refractory materials resulting from radiation processing of known <span class="hlt">ices</span> are thought to impart to them a red or brown color, as perceived in the visible spectral region. In this work, we analyzed the refractory materials produced from the 1.<span class="hlt">2</span>-keV electron bombardment of low-temperature N<span class="hlt">2</span>-, CH4-, and <span class="hlt">CO</span>-containing <span class="hlt">ices</span> (100:1:1), which simulates the radiation from the secondary electrons produced by cosmic ray bombardment of the surface <span class="hlt">ices</span> of Pluto. Despite starting with extremely simple <span class="hlt">ices</span> dominated by N<span class="hlt">2</span>, electron irradiation processing results in the production of refractory material with complex oxygen- and nitrogen-bearing organic molecules. These refractory materials were studied at room temperature using multiple analytical techniques including Fourier-transform infrared spectroscopy, X-ray absorption near-edge structure (XANES) spectroscopy, and gas chromatography coupled with mass spectrometry (GC-MS). Infrared spectra of the refractory material suggest the presence of alcohols, carboxylic acids, ketones, aldehydes, amines, and nitriles. XANES spectra of the material indicate the presence of carboxyl groups, amides, urea, and nitriles, and are thus consistent with the IR data. Atomic abundance ratios for the bulk composition of these residues from XANES analysis show that the organic residues are extremely N-rich, having ratios of N/C ∼ 0.9 and O/C ∼ 0.<span class="hlt">2</span>. Finally, GC-MS data reveal that the residues contain urea as well as numerous carboxylic acids, some of which are of interest for prebiotic and biological chemistries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V21A2484W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V21A2484W"><span>Gas composition and soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at Changbaishan intra-plate volcano, NE China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>wen, H.; Yang, T. F.; Guo, Z.; Fu, C.; Zhang, M.</p> <p>2011-12-01</p> <p>Changbaishan, located on the border of China and North Korea, is one of the most active volcanoes in China. This volcano violently erupted 1000 years ago and produced massive magma and widespread volcanic ash, resulting in one of the largest explosive eruptions during the last 2000 years. Recent gas emissions and seismic events in the Tianchi area suggested potential increasing volcanic activities. If that is so, then 1 million residents living on the crater flank shall be endangered by enormous volcanic hazards, including the threat of <span class="hlt">2</span> billion tons of water in the crater lake . In order to better understand current status of Changbaishan, we investigated gas geochemistry in samples from the Tianchi crater lake and surrounding areas. Bubbling gas from hot springs were collected and analyzed. The results show that <span class="hlt">CO</span><span class="hlt">2</span> is the major component gas for most samples. The maximum value of helium isotopic ratio 5.8 RA (where RA = 3He/4He in <span class="hlt">air</span>) implies more than 60% of helium is contributed by mantle component, while carbon isotope values fall in the range of -5.8 to -<span class="hlt">2</span>.0% (vs. PDB), indicating magmatic source signatures as well. Nitrogen dominated samples, 18Dawgo, have helium isotopic ratio 0.7 RA and carbon isotope value -11.4% implying the gas source might be associated with regional crustal components in 18Dawgo. The first-time systematic soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements indicate the <span class="hlt">flux</span> is 22.8 g m-<span class="hlt">2</span> day-1 at the western flank of Changbaishan, which is at the same level as the background value in the Tatun Volcano Group (24.6 g m-<span class="hlt">2</span> day-1), implying that it may not be as active as TVG.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.488...36L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.488...36L"><span>Precession and atmospheric <span class="hlt">CO</span><span class="hlt">2</span> modulated variability of sea <span class="hlt">ice</span> in the central Okhotsk Sea since 130,000 years ago</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lo, Li; Belt, Simon T.; Lattaud, Julie; Friedrich, Tobias; Zeeden, Christian; Schouten, Stefan; Smik, Lukas; Timmermann, Axel; Cabedo-Sanz, Patricia; Huang, Jyh-Jaan; Zhou, Liping; Ou, Tsong-Hua; Chang, Yuan-Pin; Wang, Liang-Chi; Chou, Yu-Min; Shen, Chuan-Chou; Chen, Min-Te; Wei, Kuo-Yen; Song, Sheng-Rong; Fang, Tien-Hsi; Gorbarenko, Sergey A.; Wang, Wei-Lung; Lee, Teh-Quei; Elderfield, Henry; Hodell, David A.</p> <p>2018-04-01</p> <p>Recent reduction in high-latitude sea <span class="hlt">ice</span> extent demonstrates that sea <span class="hlt">ice</span> is highly sensitive to external and internal radiative forcings. In order to better understand sea <span class="hlt">ice</span> system responses to external orbital forcing and internal oscillations on orbital timescales, here we reconstruct changes in sea <span class="hlt">ice</span> extent and summer sea surface temperature (SSST) over the past 130,000 yrs in the central Okhotsk Sea. We applied novel organic geochemical proxies of sea <span class="hlt">ice</span> (IP25), SSST (TEX86L) and open water marine productivity (a tri-unsaturated highly branched isoprenoid and biogenic opal) to marine sediment core MD01-2414 (53°11.77‧N, 149°34.80‧E, water depth 1123 m). To complement the proxy data, we also carried out transient Earth system model simulations and sensitivity tests to identify contributions of different climatic forcing factors. Our results show that the central Okhotsk Sea was <span class="hlt">ice</span>-free during Marine Isotope Stage (MIS) 5e and the early-mid Holocene, but experienced variable sea <span class="hlt">ice</span> cover during MIS <span class="hlt">2</span>-4, consistent with intervals of relatively high and low SSST, respectively. Our data also show that the sea <span class="hlt">ice</span> extent was governed by precession-dominated insolation changes during intervals of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations ranging from 190 to 260 ppm. However, the proxy record and the model simulation data show that the central Okhotsk Sea was near <span class="hlt">ice</span>-free regardless of insolation forcing throughout the penultimate interglacial, and during the Holocene, when atmospheric <span class="hlt">CO</span><span class="hlt">2</span> was above ∼260 ppm. Past sea <span class="hlt">ice</span> conditions in the central Okhotsk Sea were therefore strongly modulated by both orbital-driven insolation and <span class="hlt">CO</span><span class="hlt">2</span>-induced radiative forcing during the past glacial/interglacial cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.4297L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.4297L"><span>Using eddy covariance to measure the dependence of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> exchange rate on friction velocity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Landwehr, Sebastian; Miller, Scott D.; Smith, Murray J.; Bell, Thomas G.; Saltzman, Eric S.; Ward, Brian</p> <p>2018-03-01</p> <p>Parameterisation of the <span class="hlt">air</span>-sea gas transfer velocity of <span class="hlt">CO</span><span class="hlt">2</span> and other trace gases under open-ocean conditions has been a focus of <span class="hlt">air</span>-sea interaction research and is required for accurately determining ocean carbon uptake. Ships are the most widely used platform for <span class="hlt">air</span>-sea <span class="hlt">flux</span> measurements but the quality of the data can be compromised by airflow distortion and sensor cross-sensitivity effects. Recent improvements in the understanding of these effects have led to enhanced corrections to the shipboard eddy covariance (EC) measurements.Here, we present a revised analysis of eddy covariance measurements of <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> and momentum <span class="hlt">fluxes</span> from the Southern Ocean Surface Ocean Aerosol Production (SOAP) study. We show that it is possible to significantly reduce the scatter in the EC data and achieve consistency between measurements taken on station and with the ship underway. The gas transfer velocities from the EC measurements correlate better with the EC friction velocity (u*) than with mean wind speeds derived from shipboard measurements corrected with an airflow distortion model. For the observed range of wind speeds (u10 N = 3-23 m s-1), the transfer velocities can be parameterised with a linear fit to u*. The SOAP data are compared to previous gas transfer parameterisations using u10 N computed from the EC friction velocity with the drag coefficient from the Coupled Ocean-Atmosphere Response Experiment (COARE) model version 3.5. The SOAP results are consistent with previous gas transfer studies, but at high wind speeds they do not support the sharp increase in gas transfer associated with bubble-mediated transfer predicted by physically based models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150005617&hterms=infrared+temperature+sensor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dinfrared%2Btemperature%2Bsensor','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150005617&hterms=infrared+temperature+sensor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dinfrared%2Btemperature%2Bsensor"><span>Sensitivity Analysis for Atmospheric Infrared Sounder (<span class="hlt">AIRS</span>) <span class="hlt">CO</span><span class="hlt">2</span> Retrieval</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gat, Ilana</p> <p>2012-01-01</p> <p>The Atmospheric Infrared Sounder (<span class="hlt">AIRS</span>) is a thermal infrared sensor able to retrieve the daily atmospheric state globally for clear as well as partially cloudy field-of-views. The <span class="hlt">AIRS</span> spectrometer has 2378 channels sensing from 15.4 micrometers to 3.7 micrometers, of which a small subset in the 15 micrometers region has been selected, to date, for <span class="hlt">CO</span><span class="hlt">2</span> retrieval. To improve upon the current retrieval method, we extended the retrieval calculations to include a prior estimate component and developed a channel ranking system to optimize the channels and number of channels used. The channel ranking system uses a mathematical formalism to rapidly process and assess the retrieval potential of large numbers of channels. Implementing this system, we identifed a larger optimized subset of <span class="hlt">AIRS</span> channels that can decrease retrieval errors and minimize the overall sensitivity to other iridescent contributors, such as water vapor, ozone, and atmospheric temperature. This methodology selects channels globally by accounting for the latitudinal, longitudinal, and seasonal dependencies of the subset. The new methodology increases accuracy in <span class="hlt">AIRS</span> <span class="hlt">CO</span><span class="hlt">2</span> as well as other retrievals and enables the extension of retrieved <span class="hlt">CO</span><span class="hlt">2</span> vertical profiles to altitudes ranging from the lower troposphere to upper stratosphere. The extended retrieval method for <span class="hlt">CO</span><span class="hlt">2</span> vertical profile estimation using a maximum-likelihood estimation method. We use model data to demonstrate the beneficial impact of the extended retrieval method using the new channel ranking system on <span class="hlt">CO</span><span class="hlt">2</span> retrieval.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhDT........67W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhDT........67W"><span><span class="hlt">Ice</span>-atmosphere interactions in the Canadian High Arctic: Implications for the thermo-mechanical evolution of terrestrial <span class="hlt">ice</span> masses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wohlleben, Trudy M. H.</p> <p></p> <p>Canadian High Arctic terrestrial <span class="hlt">ice</span> masses and the polar atmosphere evolve codependently, and interactions between the two systems can lead to feedbacks, positive and negative. The two primary positive cryosphere-atmosphere feedbacks are: (1) The snow/<span class="hlt">ice</span>-albedo feedback (where area changes in snow and/or <span class="hlt">ice</span> cause changes in surface albedo and surface <span class="hlt">air</span> temperatures, leading to further area changes in snow/<span class="hlt">ice</span>); and (<span class="hlt">2</span>) The elevation - mass balance feedback (where thickness changes in terrestrial <span class="hlt">ice</span> masses cause changes to atmospheric circulation and precipitation patterns, leading to further <span class="hlt">ice</span> thickness changes). In this thesis, numerical experiments are performed to: (1) quantify the magnitudes of the two feedbacks for chosen Canadian High Arctic terrestrial <span class="hlt">ice</span> masses; and (<span class="hlt">2</span>) to examine the direct and indirect consequences of surface <span class="hlt">air</span> temperature changes upon englacial temperatures with implications for <span class="hlt">ice</span> flow, mass <span class="hlt">flux</span> divergence, and topographic evolution. Model results show that: (a) for John Evans Glacier, Ellesmere Island, the magnitude of the terrestrial snow/<span class="hlt">ice</span>-albedo feedback can locally exceed that of sea <span class="hlt">ice</span> on less than decadal timescales, with implications for glacier response times to climate perturbations; (b) although historical <span class="hlt">air</span> temperature changes might be the direct cause of measured englacial temperature anomalies in various glacier and <span class="hlt">ice</span> cap accumulation zones, they can also be the indirect cause of their enhanced diffusive loss; (c) while the direct result of past <span class="hlt">air</span> temperature changes has been to cool the interior of John Evans Glacier, and its bed, the indirect result has been to create and maintain warm (pressure melting point) basal temperatures in the ablation zone; and (d) for Devon <span class="hlt">Ice</span> Cap, observed mass gains in the northwest sector of the <span class="hlt">ice</span> cap would be smaller without orographic precipitation and the mass balance---elevation feedback, supporting the hypothesis that this feedback is playing a role in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A51F..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A51F..06C"><span>Comparing inversion techniques for constraining <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the Brazilian Amazon Basin with aircraft observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chow, V. Y.; Gerbig, C.; Longo, M.; Koch, F.; Nehrkorn, T.; Eluszkiewicz, J.; Ceballos, J. C.; Longo, K.; Wofsy, S. C.</p> <p>2012-12-01</p> <p>The Balanço Atmosférico Regional de Carbono na Amazônia (BARCA) aircraft program spanned the dry to wet and wet to dry transition seasons in November 2008 & May 2009 respectively. It resulted in ~150 vertical profiles covering the Brazilian Amazon Basin (BAB). With the data we attempt to estimate a carbon budget for the BAB, to determine if regional aircraft experiments can provide strong constraints for a budget, and to compare inversion frameworks when optimizing <span class="hlt">flux</span> estimates. We use a LPDM to integrate satellite-, aircraft-, & surface-data with mesoscale meteorological fields to link bottom-up and top-down models to provide constraints and error bounds for regional <span class="hlt">fluxes</span>. The Stochastic Time-Inverted Lagrangian Transport (STILT) model driven by meteorological fields from BRAMS, ECMWF, and WRF are coupled to a biosphere model, the Vegetation Photosynthesis Respiration Model (VPRM), to determine regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> for the BAB. The VPRM is a prognostic biosphere model driven by MODIS 8-day EVI and LSWI indices along with shortwave radiation and temperature from tower measurements and mesoscale meteorological data. VPRM parameters are tuned using eddy <span class="hlt">flux</span> tower data from the Large-Scale Biosphere Atmosphere experiment. VPRM computes hourly <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> by calculating Gross Ecosystem Exchange (GEE) and Respiration (R) for 8 different vegetation types. The VPRM <span class="hlt">fluxes</span> are scaled up to the BAB by using time-averaged drivers (shortwave radiation & temperature) from high-temporal resolution runs of BRAMS, ECMWF, and WRF and vegetation maps from SYNMAP and IGBP2007. Shortwave radiation from each mesoscale model is validated using surface data and output from GL 1.<span class="hlt">2</span>, a global radiation model based on GOES 8 visible imagery. The vegetation maps are updated to 2008 and 2009 using landuse scenarios modeled by Sim Amazonia <span class="hlt">2</span> and Sim Brazil. A priori <span class="hlt">fluxes</span> modeled by STILT-VPRM are optimized using data from BARCA, eddy covariance sites, and flask measurements. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020054331&hterms=Organic+fertilizers&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DOrganic%2Bfertilizers','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020054331&hterms=Organic+fertilizers&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DOrganic%2Bfertilizers"><span>Interannual Variability in Soil Trace Gas (<span class="hlt">CO</span><span class="hlt">2</span>, N<span class="hlt">2</span>O, NO) <span class="hlt">Fluxes</span> and Analysis of Controllers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Potter, C.; Klooster, S.; Peterson, David L. (Technical Monitor)</p> <p>1997-01-01</p> <p>Interannual variability in <span class="hlt">flux</span> rates of biogenic trace gases must be quantified in order to understand the differences between short-term trends and actual long-term change in biosphere-atmosphere interactions. We simulated interannual patterns (1983-1988) of global trace gas <span class="hlt">fluxes</span> from soils using the NASA Ames model version of CASA (Carnegie-Ames-Stanford Approach) in a transient simulation mode. This ecosystem model has been recalibrated for simulations driven by satellite vegetation index data from the NOAA Advanced Very High Resolution Radiometer (AVHRR) over the mid-1980s. The predicted interannual pattern of soil heterotropic <span class="hlt">CO</span><span class="hlt">2</span> emissions indicates that relatively large increases in global carbon <span class="hlt">flux</span> from soils occurred about three years following the strong El Nino Southern Oscillation (ENSO) event of 1983. Results for the years 1986 and 1987 showed an annual increment of +1 Pg (1015 g) C-<span class="hlt">CO</span><span class="hlt">2</span> emitted from soils, which tended to dampen the estimated global increase in net ecosystem production with about a two year lag period relative to plant carbon fixation. Zonal discrimination of model results implies that 80-90 percent of the yearly positive increments in soil <span class="hlt">CO</span><span class="hlt">2</span> emission during 1986-87 were attributable to soil organic matter decomposition in the low-latitudes (between 30 N and 30 S). Soils of the northern middle-latitude zone (between 30 N and 60 N) accounted for the residual of these annual increments. Total annual emissions of nitrogen trace gases (N<span class="hlt">2</span>O and NO) from soils were estimated to vary from <span class="hlt">2</span>-4 percent over the time period modeled, a level of variability which is consistent with predicted interannual fluctuations in global soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Interannual variability of precipitation in tropical and subtropical zones (30 N to 20 S appeared to drive the dynamic inverse relationship between higher annual emissions of NO versus emissions of N<span class="hlt">2</span>O. Global mean emission rates from natural (heterotrophic) soil sources over the period modeled (1983</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B41C0071S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B41C0071S"><span>Sampling Soil <span class="hlt">CO</span><span class="hlt">2</span> for Isotopic <span class="hlt">Flux</span> Partitioning: Non Steady State Effects and Methodological Biases</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Snell, H. S. K.; Robinson, D.; Midwood, A. J.</p> <p>2014-12-01</p> <p>Measurements of δ13C of soil <span class="hlt">CO</span><span class="hlt">2</span> are used to partition the surface <span class="hlt">flux</span> into autotrophic and heterotrophic components. Models predict that the δ13<span class="hlt">CO</span><span class="hlt">2</span> of the soil efflux is perturbed by non-steady state (NSS) diffusive conditions. These could be large enough to render δ13<span class="hlt">CO</span><span class="hlt">2</span> unsuitable for accurate <span class="hlt">flux</span> partitioning. Field studies sometimes find correlations between efflux δ13<span class="hlt">CO</span><span class="hlt">2</span> and <span class="hlt">flux</span> or temperature, or that efflux δ13<span class="hlt">CO</span><span class="hlt">2</span> is not correlated as expected with biological drivers. We tested whether NSS effects in semi-natural soil were comparable with those predicted. We compared chamber designs and their sensitivity to changes in efflux δ13<span class="hlt">CO</span><span class="hlt">2</span>. In a natural soil mesocosm, we controlled temperature to generate NSS conditions of <span class="hlt">CO</span><span class="hlt">2</span> production. We measured the δ13C of soil <span class="hlt">CO</span><span class="hlt">2</span> using in situ probes to sample the subsurface, and dynamic and forced-diffusion chambers to sample the surface efflux. Over eight hours we raised soil temperature by 4.5 OC to increase microbial respiration. Subsurface <span class="hlt">CO</span><span class="hlt">2</span> concentration doubled, surface efflux became 13C-depleted by 1 ‰ and subsurface <span class="hlt">CO</span><span class="hlt">2</span> became 13C-enriched by around <span class="hlt">2</span> ‰. Opposite changes occurred when temperature was lowered and <span class="hlt">CO</span><span class="hlt">2</span> production was decreasing. Different chamber designs had inherent biases but all detected similar changes in efflux δ13<span class="hlt">CO</span><span class="hlt">2</span>, which were comparable to those predicted. Measurements using dynamic chambers were more 13C-enriched than expected, probably due to advection of <span class="hlt">CO</span><span class="hlt">2</span> into the chamber. In the mesocosm soil, δ13<span class="hlt">CO</span><span class="hlt">2</span> of both efflux and subsurface was determined by physical processes of <span class="hlt">CO</span><span class="hlt">2</span> production and diffusion. Steady state conditions are unlikely to prevail in the field, so spot measurements of δ13<span class="hlt">CO</span><span class="hlt">2</span> and assumptions based on the theoretical 4.4 ‰ diffusive fractionation will not be accurate for estimating source δ13<span class="hlt">CO</span><span class="hlt">2</span>. Continuous measurements could be integrated over a period suitable to reduce the influence of transient NSS conditions. It will be difficult to disentangle</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.B51B0544R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.B51B0544R"><span>Year-round record of Dry Valley soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> provides insights into Antarctic soil dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Risk, D. A.; Lee, C.; Macintyre, C. M.; Cary, C.</p> <p>2012-12-01</p> <p>The McMurdo Dry Valleys of Antarctica host extreme soil microbial communities that have been extensively studied within the past decade. Activity of microbial communities is routinely measured via soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, and some useful Antarctic measurements have been made during short Austral summers. These studies are mostly spatial in nature, but temporal patterns are also valuable and may provide insights into critical thresholds and the interplay between various mechanisms that drive <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and its variation. New membrane-based Forced Diffusion (FD) soil efflux techniques offer promise for this application. The purpose of this study was to use a specially designed FD instrument in Hidden Valley of the Antarctic Dry Valleys to evaluate hardware performance in year-round deployments, and to identify features of interest with respect to soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> variation. Overall, the deployment was successful. Small but sustained positive <span class="hlt">fluxes</span> were present only twice during the year. The first such event was small but consistent and of long duration, occurring in the Austral winter. The second was more volatile and likely of microbial origin, and appeared for roughly a month at the end of the calendar year within the Austral summer. The observed patterns suggest that Hidden Valley soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> are not solely biological in nature, but likely modulated by a combination of biological, geological, and physical processes, which will be discussed in this presentation. In future studies, additional measurement locations, and simultaneous subsurface and lower atmospheric gradient concentration measurements (power-permitting) would be extremely valuable for interpreting measured <span class="hlt">fluxes</span>, to help identify advective depletion events, the depth source of <span class="hlt">fluxes</span>, and changes in soil and atmospheric diffusivities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A33F0242W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A33F0242W"><span>An Inversion Analysis of Recent Variability in Natural <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Using GOSAT and In Situ Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, J. S.; Kawa, S. R.; Baker, D. F.; Collatz, G. J.; Ott, L. E.</p> <p>2015-12-01</p> <p>About one-half of the global <span class="hlt">CO</span><span class="hlt">2</span> emissions from fossil fuel combustion and deforestation accumulates in the atmosphere, where it contributes to global warming. The rest is taken up by vegetation and the ocean. The precise contribution of the two sinks, and their location and year-to-year variability are, however, not well understood. We use two different approaches, batch Bayesian synthesis inversion and variational data assimilation, to deduce the global spatiotemporal distributions of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> during 2009-2010. One of our objectives is to assess different sources of uncertainties in inferred <span class="hlt">fluxes</span>, including uncertainties in prior <span class="hlt">flux</span> estimates and observations, and differences in inversion techniques. For prior constraints, we utilize <span class="hlt">fluxes</span> and uncertainties from the CASA-GFED model of the terrestrial biosphere and biomass burning driven by satellite observations and interannually varying meteorology. We also use measurement-based ocean <span class="hlt">flux</span> estimates and two sets of fixed fossil <span class="hlt">CO</span><span class="hlt">2</span> emissions. Here, our inversions incorporate column <span class="hlt">CO</span><span class="hlt">2</span> measurements from the GOSAT satellite (ACOS retrieval, filtered and bias-corrected) and in situ observations (individual flask and afternoon-average continuous observations) to estimate <span class="hlt">fluxes</span> in 108 regions over 8-day intervals for the batch inversion and at 3° x 3.75° weekly for the variational system. Relationships between <span class="hlt">fluxes</span> and atmospheric concentrations are derived consistently for the two inversion systems using the PCTM atmospheric transport model driven by meteorology from the MERRA reanalysis. We compare the posterior <span class="hlt">fluxes</span> and uncertainties derived using different data sets and the two inversion approaches, and evaluate the posterior atmospheric concentrations against independent data including aircraft measurements. The optimized <span class="hlt">fluxes</span> generally resemble those from other studies. For example, the results indicate that the terrestrial biosphere is a net <span class="hlt">CO</span><span class="hlt">2</span> sink, and a GOSAT-only inversion suggests a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160000370','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160000370"><span>An Inversion Analysis of Recent Variability in Natural <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Using GOSAT and In Situ Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wang, James S.; Kawa, S. Randolph; Collatz, G. James; Baker, David F.; Ott, Lesley</p> <p>2015-01-01</p> <p>About one-half of the global <span class="hlt">CO</span><span class="hlt">2</span> emissions from fossil fuel combustion and deforestation accumulates in the atmosphere, where it contributes to global warming. The rest is taken up by vegetation and the ocean. The precise contribution of the two sinks, and their location and year-to-year variability are, however, not well understood. We use two different approaches, batch Bayesian synthesis inversion and variational data assimilation, to deduce the global spatiotemporal distributions of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> during 2009-2010. One of our objectives is to assess different sources of uncertainties in inferred <span class="hlt">fluxes</span>, including uncertainties in prior <span class="hlt">flux</span> estimates and observations, and differences in inversion techniques. For prior constraints, we utilize <span class="hlt">fluxes</span> and uncertainties from the CASA-GFED model of the terrestrial biosphere and biomass burning driven by satellite observations and interannually varying meteorology. We also use measurement-based ocean <span class="hlt">flux</span> estimates and two sets of fixed fossil <span class="hlt">CO</span><span class="hlt">2</span> emissions. Here, our inversions incorporate column <span class="hlt">CO</span><span class="hlt">2</span> measurements from the GOSAT satellite (ACOS retrieval, filtered and bias-corrected) and in situ observations (individual flask and afternoon-average continuous observations) to estimate <span class="hlt">fluxes</span> in 108 regions over 8-day intervals for the batch inversion and at 3 x 3.75 weekly for the variational system. Relationships between <span class="hlt">fluxes</span> and atmospheric concentrations are derived consistently for the two inversion systems using the PCTM atmospheric transport model driven by meteorology from the MERRA reanalysis. We compare the posterior <span class="hlt">fluxes</span> and uncertainties derived using different data sets and the two inversion approaches, and evaluate the posterior atmospheric concentrations against independent data including aircraft measurements. The optimized <span class="hlt">fluxes</span> generally resemble those from other studies. For example, the results indicate that the terrestrial biosphere is a net <span class="hlt">CO</span><span class="hlt">2</span> sink, and a GOSAT-only inversion suggests a shift in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28434669','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28434669"><span>Diurnal variation of <span class="hlt">CO</span><span class="hlt">2</span>, CH4, and N<span class="hlt">2</span>O emission <span class="hlt">fluxes</span> continuously monitored in-situ in three environmental habitats in a subtropical estuarine wetland.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Wen-Bin; Yuan, Chung-Shin; Tong, Chuan; Yang, Pin; Yang, Lei; Huang, Bang-Qin</p> <p>2017-06-15</p> <p>Wetlands play a crucial role in modulating atmospheric concentrations of greenhouse gases (GHGs) such as carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span> ), methane (CH 4 ), and nitrous oxide (N <span class="hlt">2</span> O). The key factors controlling GHG emission from subtropical estuarine wetlands were investigated in this study, which continuously monitored the uptake/emission of GHGs (<span class="hlt">CO</span> <span class="hlt">2</span> , CH 4 , and N <span class="hlt">2</span> O) by/from a subtropical estuarine wetland located in the Minjiang estuary in the coastal region of southeastern China. A self-designed floating chamber was used to collect <span class="hlt">air</span> samples on-site at three environmental habitats (Phragmites australis marsh, mudflats, and river water). The <span class="hlt">CO</span> <span class="hlt">2</span> , CH 4 , and N <span class="hlt">2</span> O concentrations were then measured using an automated nondispersive infrared analyzer. The magnitudes of the <span class="hlt">CO</span> <span class="hlt">2</span> and N <span class="hlt">2</span> O emission <span class="hlt">fluxes</span> at the three habitats were ordered as river water>P. australis>mudflats. P. australis emitted GHGs through photosynthesis and respiration processes. Emissions of CH 4 from P. australis and the mudflats were revealed to be slightly higher than those from the river water. The total GHG emission <span class="hlt">fluxes</span> at the three environmental habitats were quite similar (4.68-4.78gm -<span class="hlt">2</span> h -1 ). However, when the total carbon dioxide equivalent <span class="hlt">fluxes</span> (<span class="hlt">CO</span> <span class="hlt">2</span> -e) were considered, the river water was discovered to emit the most <span class="hlt">CO</span> <span class="hlt">2</span> -e compared with P. australis and the mudflats. Based on its potential to increase global warming, N <span class="hlt">2</span> O was the main contributor to the total GHG emission, with that emitted from the river water being the most considerable. Tidal water carried onto the marsh had its own GHG content and thus has acted as a source or sink of GHGs. However, water quality had a large effect on GHG emissions from the river water whereas the tidal water height did not. Both high salinity and large amounts of sulfates in the wetlands explicitly inhibited the activity of CH 4 -producing bacteria, particularly at nighttime. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080030789&hterms=erickson&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Derickson','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080030789&hterms=erickson&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Derickson"><span>Evaluating the Capacity of Global <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> and Atmospheric Transport Models to Incorporate New Satellite Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kawa, S. R.; Collatz, G. J.; Erickson, D. J.; Denning, A. S.; Wofsy, S. C.; Andrews, A. E.</p> <p>2007-01-01</p> <p>As we enter the new era of satellite remote sensing for <span class="hlt">CO</span><span class="hlt">2</span> and other carbon cyclerelated quantities, advanced modeling and analysis capabilities are required to fully capitalize on the new observations. Model estimates of <span class="hlt">CO</span><span class="hlt">2</span> surface <span class="hlt">flux</span> and atmospheric transport are required for initial constraints on inverse analyses, to connect atmospheric observations to the location of surface sources and sinks, and ultimately for future projections of carbon-climate interactions. For application to current, planned, and future remotely sensed <span class="hlt">CO</span><span class="hlt">2</span> data, it is desirable that these models are accurate and unbiased at time scales from less than daily to multi-annual and at spatial scales from several kilometers or finer to global. Here we focus on simulated <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from terrestrial vegetation and atmospheric transport mutually constrained by analyzed meteorological fields from the Goddard Modeling and Assimilation Office for the period 1998 through 2006. Use of assimilated meteorological data enables direct model comparison to observations across a wide range of scales of variability. The biospheric <span class="hlt">fluxes</span> are produced by the CASA model at lxi degrees on a monthly mean basis, modulated hourly with analyzed temperature and sunlight. Both physiological and biomass burning <span class="hlt">fluxes</span> are derived using satellite observations of vegetation, burned area (as in GFED-<span class="hlt">2</span>), and analyzed meteorology. For the purposes of comparison to <span class="hlt">CO</span><span class="hlt">2</span> data, fossil fuel and ocean <span class="hlt">fluxes</span> are also included in the transport simulations. In this presentation we evaluate the model's ability to simulate <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and mixing ratio variability in comparison to in situ observations at sites in Northern mid latitudes and the continental tropics. The influence of key process representations is inferred. We find that the model can resolve much of the hourly to synoptic variability in the observations, although there are limits imposed by vertical resolution of boundary layer processes. The seasonal cycle and its</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.6008T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.6008T"><span>Influences of Ocean Thermohaline Stratification on Arctic Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Toole, J. M.; Timmermans, M.-L.; Perovich, D. K.; Krishfield, R. A.; Proshutinsky, A.; Richter-Menge, J. A.</p> <p>2009-04-01</p> <p>The Arctic Ocean's surface mixed layer constitutes the dynamical and thermodynamical link between the sea <span class="hlt">ice</span> and the underlying waters. Wind stress, acting directly on the surface mixed layer or via wind-forced <span class="hlt">ice</span> motion, produce surface currents that can in turn drive deep ocean flow. Mixed layer temperature is intimately related to basal sea <span class="hlt">ice</span> growth and melting. Heat <span class="hlt">fluxes</span> into or out of the surface mixed layer can occur at both its upper and lower interfaces: the former via <span class="hlt">air</span>-sea exchange at leads and conduction through the <span class="hlt">ice</span>, the latter via turbulent mixing and entrainment at the layer base. Variations in Arctic Ocean mixed layer properties are documented based on more than 16,000 temperature and salinity profiles acquired by <span class="hlt">Ice</span>-Tethered Profilers since summer 2004 and analyzed in conjunction with sea <span class="hlt">ice</span> observations from <span class="hlt">Ice</span> Mass Balance Buoys and atmospheric heat <span class="hlt">flux</span> estimates. Guidance interpreting the observations is provided by a one-dimensional ocean mixed layer model. The study focuses attention on the very strong density stratification about the mixed layer base in the Arctic that, in regions of sea <span class="hlt">ice</span> melting, is increasing with time. The intense stratification greatly impedes mixed layer deepening by vertical convection and shear mixing, and thus limits the <span class="hlt">flux</span> of deep ocean heat to the surface that could influence sea <span class="hlt">ice</span> growth/decay. Consistent with previous work, this study demonstrates that the Arctic sea <span class="hlt">ice</span> is most sensitive to changes in ocean mixed layer heat resulting from <span class="hlt">fluxes</span> across its upper (<span class="hlt">air</span>-sea and/or <span class="hlt">ice</span>-water) interface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004DSRI...51..307P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004DSRI...51..307P"><span>Geochemical particle <span class="hlt">fluxes</span> in the Southern Indian Ocean seasonal <span class="hlt">ice</span> zone: Prydz Bay region, East Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pilskaln, C. H.; Manganini, S. J.; Trull, T. W.; Armand, L.; Howard, W.; Asper, V. L.; Massom, R.</p> <p>2004-02-01</p> <p>Time-series sediment traps were deployed between December 1998 and January 2000 and from March 2000 to February 2001 at two offshore Prydz Bay sites within the seasonal <span class="hlt">ice</span> zone (SIZ) of the Southern Indian Ocean located between 62-63°S and 73-76°E to quantify seasonal biogeochemical particle <span class="hlt">fluxes</span>. Samples were obtained from traps placed at 1400, 2400, and 3400 m during the first deployment year (PZB-1) and from 3300 m in the second deployment year (PZB-<span class="hlt">2</span>). All geochemical export <span class="hlt">fluxes</span> were highly seasonal with primary peaks occurring during the austral summer and relatively low <span class="hlt">fluxes</span> prevailing through the winter months. Secondary <span class="hlt">flux</span> peaks in mid-winter and in early spring were suggestive of small-scale, sea-<span class="hlt">ice</span> break-up events and the spring retreat of seasonal <span class="hlt">ice</span>, respectively. Biogenic silica represented over 70% (by weight) of the collected trap material and provided an annual opal export of 18 g m -<span class="hlt">2</span> to 1 km and 3-10 g m -<span class="hlt">2</span> to 3 km. POC <span class="hlt">fluxes</span> supplied an annual export of approximately 1 g m -<span class="hlt">2</span>, equal to the estimated ocean-wide average. Elevated particulate C org/C inorg and Si bio/C inorg molar ratios indicate a productive, diatom-dominated system, although consistently small <span class="hlt">fluxes</span> of planktonic foraminifera and pteropod shells document a heterotrophic source of carbonate to deeper waters in the SIZ. The observation of high Si bio/C org ratios and the δ15N time-series data suggest enhanced rates of diatom-POC remineralization in the upper 1000 m relative to bioSiO <span class="hlt">2</span>. The occurrence in this region of a pronounced temperature minimum, associated with a strong pycnocline and subsurface particle maximum at 50-100 m, may represent a zone where sinking, diatom-rich particulates temporarily accumulate and POC is remineralized.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRF..117.2029B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRF..117.2029B"><span>In situ cosmogenic radiocarbon production and <span class="hlt">2</span>-D <span class="hlt">ice</span> flow line modeling for an Antarctic blue <span class="hlt">ice</span> area</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buizert, Christo; Petrenko, Vasilii V.; Kavanaugh, Jeffrey L.; Cuffey, Kurt M.; Lifton, Nathaniel A.; Brook, Edward J.; Severinghaus, Jeffrey P.</p> <p>2012-06-01</p> <p>Radiocarbon measurements at <span class="hlt">ice</span> margin sites and blue <span class="hlt">ice</span> areas can potentially be used for <span class="hlt">ice</span> dating, ablation rate estimates and paleoclimatic reconstructions. Part of the measured signal comes from in situ cosmogenic 14C production in <span class="hlt">ice</span>, and this component must be well understood before useful information can be extracted from 14C data. We combine cosmic ray scaling and production estimates with a two-dimensional <span class="hlt">ice</span> flow line model to study cosmogenic 14C production at Taylor Glacier, Antarctica. We find (1) that 14C production through thermal neutron capture by nitrogen in <span class="hlt">air</span> bubbles is negligible; (<span class="hlt">2</span>) that including <span class="hlt">ice</span> flow patterns caused by basal topography can lead to a surface 14C activity that differs by up to 25% from the activity calculated using an ablation-only approximation, which is used in all prior work; and (3) that at high ablation margin sites, solar modulation of the cosmic ray <span class="hlt">flux</span> may change the strength of the dominant spallogenic production by up to 10%. As part of this effort we model two-dimensional <span class="hlt">ice</span> flow along the central flow line of Taylor Glacier. We present two methods for parameterizing vertical strain rates, and assess which method is more reliable for Taylor Glacier. Finally, we present a sensitivity study from which we conclude that uncertainties in published cosmogenic production rates are the largest source of potential error. The results presented here can inform ongoing and future 14C and <span class="hlt">ice</span> flow studies at <span class="hlt">ice</span> margin sites, including important paleoclimatic applications such as the reconstruction of paleoatmospheric 14C content of methane.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B21F2017D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B21F2017D"><span>Characterization And Partitioning Of CH4 And <span class="hlt">CO</span><span class="hlt">2</span> Eddy <span class="hlt">Flux</span> Data Measured at NGEE-Arctic Sites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dengel, S.; Chafe, O.; Curtis, J. B.; Biraud, S.; Torn, M. S.; Wullschleger, S. D.</p> <p>2017-12-01</p> <p>The high latitudes are experiencing rapid warming with permafrost ecosystems being highly vulnerable to this change. Since the advancement in Eddy Covariance (EC) measurements, the number of high latitude sites measuring greenhouse gases and energy (<span class="hlt">CO</span><span class="hlt">2</span>, CH4 and H<span class="hlt">2</span>O) <span class="hlt">fluxes</span> is steadily increasing, with new sites being established each year. Data from these sites are not only valuable for annual carbon budget calculations, but also vital to the modeling community for improving their predictions of emission rates and trends. CH4 <span class="hlt">flux</span> measurements are not as straightforward as <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. They tend to be less predictable or as easily interpretable as <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Understanding CH4 emission patterns are often challenging. Moreover, gas <span class="hlt">flux</span> fluctuations are spatially and temporally diverse, and in many cases event-based. An improvement in understanding would also contribute to improvements in the fidelity of model predictions. These rely on having high quality data, and thus will entail developing new QA/QC and gap-filling methods for Arctic systems, in particularly for CH4. Contributing to these challenges is the limited number of ancillary measurements carried out at many sites and the lack of standardized data processing, QA/QC, and gap-filling procedures, in particular for CH4. <span class="hlt">CO</span><span class="hlt">2</span>, CH4, and energy <span class="hlt">flux</span> measurements are ongoing at, both NGEE-Arctic/Ameri<span class="hlt">Flux</span>, US-NGB (Arctic coastal plain), and US-NGC (subarctic tussock tundra) sites. The sites, with underlying continuous permafrost, show a high degree of inter-annual and seasonal variability in CH4 <span class="hlt">fluxes</span>. In order to interpret this variability, we apply a variety of models, such as footprint characterization, generalized additive models, as well as artificial neural networks, in an attempt to decipher these diverse <span class="hlt">fluxes</span>, patterns and events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5544137','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5544137"><span>Simultaneously reducing <span class="hlt">CO</span><span class="hlt">2</span> and particulate exposures via fractional recirculation of vehicle cabin <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Jung, Heejung S.; Grady, Michael L.; Victoroff, Tristan; Miller, Arthur L.</p> <p>2017-01-01</p> <p>Prior studies demonstrate that <span class="hlt">air</span> recirculation can reduce exposure to nanoparticles in vehicle cabins. However when people occupy confined spaces, <span class="hlt">air</span> recirculation can lead to carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) accumulation which can potentially lead to deleterious effects on cognitive function. This study proposes a fractional <span class="hlt">air</span> recirculation system for reducing nanoparticle concentration while simultaneously suppressing <span class="hlt">CO</span><span class="hlt">2</span> levels in the cabin. Several recirculation scenarios were tested using a custom-programmed HVAC (heat, ventilation, <span class="hlt">air</span> conditioning) unit that varied the recirculation door angle in the test vehicle. Operating the recirculation system with a standard cabin filter reduced particle concentrations to 1000 particles/cm3, although <span class="hlt">CO</span><span class="hlt">2</span> levels rose to 3000 ppm. When as little as 25% fresh <span class="hlt">air</span> was introduced (75% recirculation), <span class="hlt">CO</span><span class="hlt">2</span> levels dropped to 1000 ppm, while particle concentrations remained below 5000 particles/cm3. We found that nanoparticles were removed selectively during recirculation and demonstrated the trade-off between cabin <span class="hlt">CO</span><span class="hlt">2</span> concentration and cabin particle concentration using fractional <span class="hlt">air</span> recirculation. Data showed significant increases in <span class="hlt">CO</span><span class="hlt">2</span> levels during 100% recirculation. For various fan speeds, recirculation fractions of 50–75% maintained lower <span class="hlt">CO</span><span class="hlt">2</span> levels in the cabin, while still reducing particulate levels. We recommend fractional recirculation as a simple method to reduce occupants’ exposures to particulate matter and <span class="hlt">CO</span><span class="hlt">2</span> in vehicles. A design with several fractional recirculation settings could allow <span class="hlt">air</span> exchange adequate for reducing both particulate and <span class="hlt">CO</span><span class="hlt">2</span> exposures. Developing this technology could lead to reductions in airborne nanoparticle exposure, while also mitigating safety risks from <span class="hlt">CO</span><span class="hlt">2</span> accumulation. PMID:28781568</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28781568','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28781568"><span>Simultaneously reducing <span class="hlt">CO</span><span class="hlt">2</span> and particulate exposures via fractional recirculation of vehicle cabin <span class="hlt">air</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jung, Heejung S; Grady, Michael L; Victoroff, Tristan; Miller, Arthur L</p> <p>2017-07-01</p> <p>Prior studies demonstrate that <span class="hlt">air</span> recirculation can reduce exposure to nanoparticles in vehicle cabins. However when people occupy confined spaces, <span class="hlt">air</span> recirculation can lead to carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span> ) accumulation which can potentially lead to deleterious effects on cognitive function. This study proposes a fractional <span class="hlt">air</span> recirculation system for reducing nanoparticle concentration while simultaneously suppressing <span class="hlt">CO</span> <span class="hlt">2</span> levels in the cabin. Several recirculation scenarios were tested using a custom-programmed HVAC (heat, ventilation, <span class="hlt">air</span> conditioning) unit that varied the recirculation door angle in the test vehicle. Operating the recirculation system with a standard cabin filter reduced particle concentrations to 1000 particles/cm 3 , although <span class="hlt">CO</span> <span class="hlt">2</span> levels rose to 3000 ppm. When as little as 25% fresh <span class="hlt">air</span> was introduced (75% recirculation), <span class="hlt">CO</span> <span class="hlt">2</span> levels dropped to 1000 ppm, while particle concentrations remained below 5000 particles/cm 3 . We found that nanoparticles were removed selectively during recirculation and demonstrated the trade-off between cabin <span class="hlt">CO</span> <span class="hlt">2</span> concentration and cabin particle concentration using fractional <span class="hlt">air</span> recirculation. Data showed significant increases in <span class="hlt">CO</span> <span class="hlt">2</span> levels during 100% recirculation. For various fan speeds, recirculation fractions of 50-75% maintained lower <span class="hlt">CO</span> <span class="hlt">2</span> levels in the cabin, while still reducing particulate levels. We recommend fractional recirculation as a simple method to reduce occupants' exposures to particulate matter and <span class="hlt">CO</span> <span class="hlt">2</span> in vehicles. A design with several fractional recirculation settings could allow <span class="hlt">air</span> exchange adequate for reducing both particulate and <span class="hlt">CO</span> <span class="hlt">2</span> exposures. Developing this technology could lead to reductions in airborne nanoparticle exposure, while also mitigating safety risks from <span class="hlt">CO</span> <span class="hlt">2</span> accumulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmEn.160...77J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmEn.160...77J"><span>Simultaneously reducing <span class="hlt">CO</span><span class="hlt">2</span> and particulate exposures via fractional recirculation of vehicle cabin <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jung, Heejung S.; Grady, Michael L.; Victoroff, Tristan; Miller, Arthur L.</p> <p>2017-07-01</p> <p>Prior studies demonstrate that <span class="hlt">air</span> recirculation can reduce exposure to nanoparticles in vehicle cabins. However when people occupy confined spaces, <span class="hlt">air</span> recirculation can lead to carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) accumulation which can potentially lead to deleterious effects on cognitive function. This study proposes a fractional <span class="hlt">air</span> recirculation system for reducing nanoparticle concentration while simultaneously suppressing <span class="hlt">CO</span><span class="hlt">2</span> levels in the cabin. Several recirculation scenarios were tested using a custom-programmed HVAC (heat, ventilation, <span class="hlt">air</span> conditioning) unit that varied the recirculation door angle in the test vehicle. Operating the recirculation system with a standard cabin filter reduced particle concentrations to 1000 particles/cm3, although <span class="hlt">CO</span><span class="hlt">2</span> levels rose to 3000 ppm. When as little as 25% fresh <span class="hlt">air</span> was introduced (75% recirculation), <span class="hlt">CO</span><span class="hlt">2</span> levels dropped to 1000 ppm, while particle concentrations remained below 5000 particles/cm3. We found that nanoparticles were removed selectively during recirculation and demonstrated the trade-off between cabin <span class="hlt">CO</span><span class="hlt">2</span> concentration and cabin particle concentration using fractional <span class="hlt">air</span> recirculation. Data showed significant increases in <span class="hlt">CO</span><span class="hlt">2</span> levels during 100% recirculation. For various fan speeds, recirculation fractions of 50-75% maintained lower <span class="hlt">CO</span><span class="hlt">2</span> levels in the cabin, while still reducing particulate levels. We recommend fractional recirculation as a simple method to reduce occupants' exposures to particulate matter and <span class="hlt">CO</span><span class="hlt">2</span> in vehicles. A design with several fractional recirculation settings could allow <span class="hlt">air</span> exchange adequate for reducing both particulate and <span class="hlt">CO</span><span class="hlt">2</span> exposures. Developing this technology could lead to reductions in airborne nanoparticle exposure, while also mitigating safety risks from <span class="hlt">CO</span><span class="hlt">2</span> accumulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B22A..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B22A..03W"><span>Annual dynamics of N<span class="hlt">2</span>O, CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from the agricultural irrigation watersheds in southeast China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, S.; Zou, J.; Liu, S.; Chen, J.; Kong, D.; Geng, Y.</p> <p>2017-12-01</p> <p>Agricultural irrigation watershed covers a large area in southeast of China and is a potentially important source of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>), methane (CH4) and nitrous oxide (N<span class="hlt">2</span>O). However, the <span class="hlt">flux</span> magnitudes contribution to the overall catchment greenhouse gas (GHGs) <span class="hlt">fluxes</span> and their drivers of seasonal variability are limited in agricultural irrigation watersheds. An in-situ observation was performed to measure annual <span class="hlt">CO</span><span class="hlt">2</span>, CH4 and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> from an agricultural irrigation watershed in southeast of China from September 2014 to September 2016. GHGs <span class="hlt">fluxes</span> were measured using floating chambers and a gas exchange model was also used to predict CH4 and N<span class="hlt">2</span>O <span class="hlt">fluxes</span>. All GHGs showed varied seasonally with highest <span class="hlt">fluxes</span> in early summer (July) and lowest in winter. Estimated seasonal CH4-C <span class="hlt">fluxes</span> (11.5-97.6 mg m-<span class="hlt">2</span> hr-1) and N<span class="hlt">2</span>O-N <span class="hlt">fluxes</span> (<span class="hlt">2</span>.8-80.8μg m-<span class="hlt">2</span> hr-1) were in relative agreement with measured CH4-C <span class="hlt">fluxes</span> (0.05-74.9mg m-<span class="hlt">2</span> hr-1) and N<span class="hlt">2</span>O-N <span class="hlt">fluxes</span> (3.9-68.7μg m-<span class="hlt">2</span> hr-1) <span class="hlt">fluxes</span> using floating chambers. Both CH4 and N<span class="hlt">2</span>O <span class="hlt">fluxes</span> were positively related to water temperature. The CH4 <span class="hlt">fluxes</span> were negatively related to water dissolved oxygen (DO) concentration but positively related to sediment dissolved organic carbon (DOC). The N<span class="hlt">2</span>O <span class="hlt">fluxes</span> were positively related to water NH4+ and NO3-. The calculated EF5-r value in this study (mean = 0.0016; range = 0.0013-0.0018) was below the current IPCC (2006) default value of 0.0025. This implied that IPCC methodology may over estimates of N<span class="hlt">2</span>O emissions associated with nitrogen leaching and runoff from agriculture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016BGeo...13.6107V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016BGeo...13.6107V"><span>The role of Phragmites in the CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in a minerotrophic peatland in southwest Germany</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van den Berg, Merit; Ingwersen, Joachim; Lamers, Marc; Streck, Thilo</p> <p>2016-11-01</p> <p>Peatlands are interesting as a carbon storage option, but are also natural emitters of the greenhouse gas methane (CH4). Phragmites peatlands are particularly interesting due to the global abundance of this wetland plant (Phragmites australis) and the highly efficient internal gas transport mechanism, which is called humidity-induced convection (HIC). The research aims were to (1) clarify how this plant-mediated gas transport influences the CH4 <span class="hlt">fluxes</span>, (<span class="hlt">2</span>) which other environmental variables influence the <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span>, and (3) whether Phragmites peatlands are a net source or sink of greenhouse gases. <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> were measured with the eddy covariance technique within a <span style="" class="text">Phragmites-dominated fen in southwest Germany. One year of <span class="hlt">flux</span> data (March 2013-February 2014) shows very clear diurnal and seasonal patterns for both <span class="hlt">CO</span><span class="hlt">2</span> and CH4. The diurnal pattern of CH4 <span class="hlt">fluxes</span> was only visible when living, green reed was present. In August the diurnal cycle of CH4 was the most distinct, with 11 times higher midday <span class="hlt">fluxes</span> (15.7 mg CH4 m-<span class="hlt">2</span> h-1) than night <span class="hlt">fluxes</span> (1.41 mg CH4 m-<span class="hlt">2</span> h-1). This diurnal cycle has the highest correlation with global radiation, which suggests a high influence of the plants on the CH4 <span class="hlt">flux</span>. But if the cause were the HIC, it would be expected that relative humidity would correlate stronger with CH4 <span class="hlt">flux</span>. Therefore, we conclude that in addition to HIC, at least one additional mechanism must be involved in the creation of the convective flow within the Phragmites plants. Overall, the fen was a sink for carbon and greenhouse gases in the measured year, with a total carbon uptake of 221 g C m-<span class="hlt">2</span> yr-1 (26 % of the total assimilated carbon). The net uptake of greenhouse gases was 52 g <span class="hlt">CO</span><span class="hlt">2</span> eq. m-<span class="hlt">2</span> yr-1, which is obtained from an uptake of <span class="hlt">CO</span><span class="hlt">2</span> of 894 g <span class="hlt">CO</span><span class="hlt">2</span> eq. m-<span class="hlt">2</span> yr-1 and a release of CH4 of 842 g <span class="hlt">CO</span><span class="hlt">2</span> eq. m-<span class="hlt">2</span> yr-1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014OcSci..10..485H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014OcSci..10..485H"><span>The land-<span class="hlt">ice</span> contribution to 21st-century dynamic sea level rise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Howard, T.; Ridley, J.; Pardaens, A. K.; Hurkmans, R. T. W. L.; Payne, A. J.; Giesen, R. H.; Lowe, J. A.; Bamber, J. L.; Edwards, T. L.; Oerlemans, J.</p> <p>2014-06-01</p> <p>Climate change has the potential to influence global mean sea level through a number of processes including (but not limited to) thermal expansion of the oceans and enhanced land <span class="hlt">ice</span> melt. In addition to their contribution to global mean sea level change, these two processes (among others) lead to local departures from the global mean sea level change, through a number of mechanisms including the effect on spatial variations in the change of water density and transport, usually termed dynamic sea level changes. In this study, we focus on the component of dynamic sea level change that might be given by additional freshwater inflow to the ocean under scenarios of 21st-century land-based <span class="hlt">ice</span> melt. We present regional patterns of dynamic sea level change given by a global-coupled atmosphere-ocean climate model forced by spatially and temporally varying projected <span class="hlt">ice</span>-melt <span class="hlt">fluxes</span> from three sources: the Antarctic <span class="hlt">ice</span> sheet, the Greenland <span class="hlt">Ice</span> Sheet and small glaciers and <span class="hlt">ice</span> caps. The largest <span class="hlt">ice</span> melt <span class="hlt">flux</span> we consider is equivalent to almost 0.7 m of global mean sea level rise over the 21st century. The temporal evolution of the dynamic sea level changes, in the presence of considerable variations in the <span class="hlt">ice</span> melt <span class="hlt">flux</span>, is also analysed. We find that the dynamic sea level change associated with the <span class="hlt">ice</span> melt is small, with the largest changes occurring in the North Atlantic amounting to 3 cm above the global mean rise. Furthermore, the dynamic sea level change associated with the <span class="hlt">ice</span> melt is similar regardless of whether the simulated <span class="hlt">ice</span> <span class="hlt">fluxes</span> are applied to a simulation with fixed <span class="hlt">CO</span><span class="hlt">2</span> or under a business-as-usual greenhouse gas warming scenario of increasing <span class="hlt">CO</span><span class="hlt">2</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B51H0526M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B51H0526M"><span>Estimating <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Pre and Post Drought Using Remote Sensing Data in the Sierra Nevada Range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazzi, J. R.; Grigsby, S.; Goulden, M.; Ustin, S.</p> <p>2015-12-01</p> <p>The recent California drought presents an opportunity to study <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> changes over time due to insufficient water uptake by plant life using remote sensing data. Three <span class="hlt">flux</span> towers were used to create linear regressions between AVIRIS derived Net Ecosystem Exchange (NEE = PRI * NDVI * PAR) and tower measured <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the San Joaquin Experimental Range. To estimate <span class="hlt">CO</span><span class="hlt">2</span> from NEE, two linear regressions were used based on time of day and season, with R<span class="hlt">2</span> values of 0.85 and 0.87 respectively. Per-pixel <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was estimated for AVIRIS flights flown in June 2013, 2014, and 2015, as well as September 2011 and October 2014. There was a significant decrease in post drought photosynthetic <span class="hlt">CO</span><span class="hlt">2</span> uptake over the 6,700 km<span class="hlt">2</span> studied, totaling <span class="hlt">2</span>,977 grams per minute less (15.9% decrease) from June 2013 to June 2014. Data from the 2015 HyspIRI flights suggest a continuation of this trend for June 2015. Pre-drought conditions over a 33 km<span class="hlt">2</span> area show that the photosynthetic <span class="hlt">CO</span><span class="hlt">2</span> uptake dropped from 74 mg per minute on September 24, 2011, to 35 mg per minute on October 6, 2014 (a 53% decrease). HyspIRI flight lines also include 434 km<span class="hlt">2</span> of the Rim Fire, an area that saw a decrease in <span class="hlt">CO</span><span class="hlt">2</span> uptake of 413 grams per minute (71.7% decrease from June 2013 to June 2014) from the burn alone. It is estimated that the entire Rim Fire (1,041 km<span class="hlt">2</span>) has caused a total decrease in photosynthetic <span class="hlt">CO</span><span class="hlt">2</span> uptake totaling 988 grams less per minute from 2013 to 2014, with some recovery evident in 2015.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AtmEn..99..546A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AtmEn..99..546A"><span>Quantifying the <span class="hlt">air</span> quality-<span class="hlt">CO</span><span class="hlt">2</span> tradeoff potential for airports</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ashok, Akshay; Dedoussi, Irene C.; Yim, Steve H. L.; Balakrishnan, Hamsa; Barrett, Steven R. H.</p> <p>2014-12-01</p> <p>Aircraft movements on the airport surface are responsible for <span class="hlt">CO</span><span class="hlt">2</span> emissions that contribute to climate change and other emissions that affect <span class="hlt">air</span> quality and human health. While the potential for optimizing aircraft surface movements to minimize <span class="hlt">CO</span><span class="hlt">2</span> emissions has been assessed, the implications of <span class="hlt">CO</span><span class="hlt">2</span> emissions minimization for <span class="hlt">air</span> quality have not been quantified. In this paper, we identify conditions in which there is a tradeoff between <span class="hlt">CO</span><span class="hlt">2</span> emissions and population exposure to O3 and secondary PM<span class="hlt">2</span>.5 - i.e. where decreasing fuel burn (which is directly proportional to <span class="hlt">CO</span><span class="hlt">2</span> emissions) results in increased exposure. Fuel burn and emissions are estimated as a function of thrust setting for five common gas turbine engines at 34 US airports. Regional <span class="hlt">air</span> quality impacts, which are dominated by ozone and secondary PM<span class="hlt">2</span>.5, are computed as a function of airport location and time using the adjoint of the GEOS-Chem chemistry-transport model. Tradeoffs between <span class="hlt">CO</span><span class="hlt">2</span> emissions and population exposure to PM<span class="hlt">2</span>.5 and O3 occur between <span class="hlt">2</span>-18% and 5-60% of the year, respectively, depending on airport location, engine type, and thrust setting. The total duration of tradeoff conditions is 5-12 times longer at maximum thrust operations (typical for takeoff) relative to 4% thrust operations (typical for taxiing). Per kilogram of additional fuel burn at constant thrust setting during tradeoff conditions, reductions in population exposure to PM<span class="hlt">2</span>.5 and O3 are 6-13% and 32-1060% of the annual average (positive) population exposure per kilogram fuel burn, where the ranges encompass the medians over the 34 airports. For fuel burn increases due to thrust increases (i.e. for constant operating time), reductions in both PM<span class="hlt">2</span>.5 and O3 exposure are 1.5-6.4 times larger in magnitude than those due to increasing fuel burn at constant thrust (i.e. increasing operating time). Airports with relatively high population exposure reduction potentials - which occur due to a combination of high duration and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017P%26SS..135...17E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017P%26SS..135...17E"><span>Atomistic and infrared study of <span class="hlt">CO</span>-water amorphous <span class="hlt">ice</span> onto olivine dust grain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Escamilla-Roa, Elizabeth; Moreno, Fernando; López-Moreno, J. Juan; Sainz-Díaz, C. Ignacio</p> <p>2017-01-01</p> <p>This work is a study of <span class="hlt">CO</span> and H<span class="hlt">2</span>O molecules as adsorbates that interact on the surface of olivine dust grains. Olivine (forsterite) is present on the Earth, planetary dust, in the interstellar medium (ISM) and in particular in comets. The composition of amorphous <span class="hlt">ice</span> is very important for the interpretation of processes that occur in the solar system and the ISM. Dust particles in ISM are composed of a heterogeneous mixture of amorphous or crystalline silicates (e.g. olivine) organic material, carbon, and other minor constituents. These dust grains are embedded in a matrix of <span class="hlt">ices</span>, such as H<span class="hlt">2</span>O, <span class="hlt">CO</span>, <span class="hlt">CO</span><span class="hlt">2</span>, NH3, and CH4. We consider that any amorphous <span class="hlt">ice</span> will interact and grow faster on dust grain surfaces. In this work we explore the adsorption of <span class="hlt">CO</span>-H<span class="hlt">2</span>O amorphous <span class="hlt">ice</span> onto several (100) forsterite surfaces (dipolar and non-dipolar), by using first principle calculations based on density functional theory (DFT). These models are applied to two possible situations: i) adsorption of <span class="hlt">CO</span> molecules mixed into an amorphous <span class="hlt">ice</span> matrix (gas mixture) and adsorbed directly onto the forsterite surface. This interaction has lower adsorption energy than polar molecules (H<span class="hlt">2</span>O and NH3) adsorbed on this surface; ii) adsorption of <span class="hlt">CO</span> when the surface has previously been covered by amorphous water <span class="hlt">ice</span> (onion model). In this case the calculations show that adsorption energy is low, indicating that this interaction is weak and therefore the <span class="hlt">CO</span> can be desorbed with a small increase of temperature. Vibration spectroscopy for the most stable complex was also studied and the frequencies were in good agreement with experimental frequency values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1613217Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1613217Q"><span>Temporal changes in soil water repellency linked to the soil respiration and CH4 and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qassem, Khalid; Urbanek, Emilia; van Keulen, Geertje</p> <p>2014-05-01</p> <p>Soil water repellency (SWR) is known to be a spatially and temporally variable phenomenon. The seasonal changes in soil moisture lead to development of soil water repellency, which in consequence may affect the microbial activity and in consequence alter the <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> from soils. Soil microbial activity is strongly linked to the temperature and moisture status of the soil. In terms of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> intermediate moisture contents are most favourable for the optimal microbial activity and highest <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. Methanogenesis occurs primarily in anaerobic water-logged habitats while methanotrophy is a strictly aerobic process. In the study we hypothesise that the changes in <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span> are closely linked to critical moisture thresholds for soil water repellency. This research project aims to adopt a multi-disciplinary approach to comprehensively determine the effect of SWR on <span class="hlt">CO</span><span class="hlt">2</span> and CH4 <span class="hlt">fluxes</span>. Research is conducted in situ at four sites exhibiting SWR in the southern UK. <span class="hlt">Flux</span> measurements are carried out concomitant with meteorological and SWR observations Field observations are supported by laboratory measurements carried out on intact soil samples collected at the above identified field sites. The laboratory analyses are conducted under constant temperatures with controlled changes of soil moisture content. Methanogenic and Methanotrophic microbial populations are being analysed at different SWR and moisture contents using the latest metagenomic and metatranscriptomic approaches. Currently available data show that greenhouse gas <span class="hlt">flux</span> are closely linked with soil moisture thresholds for SWR development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4237463','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4237463"><span>Net uptake of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> by coastal submerged aquatic vegetation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tokoro, Tatsuki; Hosokawa, Shinya; Miyoshi, Eiichi; Tada, Kazufumi; Watanabe, Kenta; Montani, Shigeru; Kayanne, Hajime; Kuwae, Tomohiro</p> <p>2014-01-01</p> <p>‘Blue Carbon’, which is carbon captured by marine living organisms, has recently been highlighted as a new option for climate change mitigation initiatives. In particular, coastal ecosystems have been recognized as significant carbon stocks because of their high burial rates and long-term sequestration of carbon. However, the direct contribution of Blue Carbon to the uptake of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> through <span class="hlt">air</span>-sea gas exchange remains unclear. We performed in situ measurements of carbon flows, including <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>, dissolved inorganic carbon changes, net ecosystem production, and carbon burial rates in the boreal (Furen), temperate (Kurihama), and subtropical (Fukido) seagrass meadows of Japan from 2010 to 2013. In particular, the <span class="hlt">air</span>-sea <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> was measured using three methods: the bulk formula method, the floating chamber method, and the eddy covariance method. Our empirical results show that submerged autotrophic vegetation in shallow coastal waters can be functionally a sink for atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. This finding is contrary to the conventional perception that most near-shore ecosystems are sources of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. The key factor determining whether or not coastal ecosystems directly decrease the concentration of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> may be net ecosystem production. This study thus identifies a new ecosystem function of coastal vegetated systems; they are direct sinks of atmospheric <span class="hlt">CO</span><span class="hlt">2</span>. PMID:24623530</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.sciencemag.org/content/332/6031/838.short','USGSPUBS'); return false;" href="http://www.sciencemag.org/content/332/6031/838.short"><span>Massive <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Ice</span> Deposits Sequestered in the South Polar Layered Deposits of Mars</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Phillips, Roger J.; Davis, Brian J.; Tanaka, Kenneth L.; Byrne, Shane; Mellon, Michael T.; Putzig, Nathaniel E.; Haberle, Robert M.; Kahre, Melinda A.; Campbell, Bruce A.; Carter, Lynn M.; Smith, Isaac B.; Holt, John W.; Smrekar, Suzanne E.; Nunes, Daniel C.; Plaut, Jeffrey J.; Egan, Anthony F.; Titus, Timothy N.; Seu, Roberto</p> <p>2011-01-01</p> <p>Shallow Radar soundings from the Mars Reconnaissance Orbiter reveal a buried deposit of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) <span class="hlt">ice</span> within the south polar layered deposits of Mars with a volume of 9500 to 12,500 cubic kilometers, about 30 times that previously estimated for the south pole residual cap. The deposit occurs within a stratigraphic unit that is uniquely marked by collapse features and other evidence of interior <span class="hlt">CO</span><span class="hlt">2</span> volatile release. If released into the atmosphere at times of high obliquity, the <span class="hlt">CO</span><span class="hlt">2</span> reservoir would increase the atmospheric mass by up to 80%, leading to more frequent and intense dust storms and to more regions where liquid water could persist without boiling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950031260&hterms=biodegradation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dbiodegradation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950031260&hterms=biodegradation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dbiodegradation"><span><span class="hlt">Flux</span> to the atmosphere of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> from wetland ponds on the Hudson Bay lowlands (HBLs)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hamilton, J. David; Kelly, Carol A.; Rudd, John W. M.; Hesslein, Raymond H.; Roulet, Nigel T.</p> <p>1994-01-01</p> <p>Ponds on peatlands of the Hudson Bay lowlands (HBLs) are complex ecosystems in which the <span class="hlt">fluxes</span> to the atmosphere of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> were controlled by interacting physical and biological factors. This resulted in strong diel variations of both dissolved gas concentrations and gas <span class="hlt">fluxes</span> to the atmosphere, necessitating frequent sampling on a 24-hour schedule to enable accurate estimates of daily <span class="hlt">fluxes</span>. Ponds at three sites on the HBL were constant net sources of CH4 and <span class="hlt">CO</span><span class="hlt">2</span> to the atmosphere at mean rates of 110-180 mg CH4 m(exp -<span class="hlt">2</span>)/d and 3700-11,000 mg <span class="hlt">CO</span><span class="hlt">2</span> m(exp -<span class="hlt">2</span>)/d. Rates peaked in August and September. For CH4 the pond <span class="hlt">fluxes</span> were 3-30 times higher than adjacent vegetated surfaces. For <span class="hlt">CO</span><span class="hlt">2</span> the net pond <span class="hlt">fluxes</span> were similar in magnitude to the vegetated <span class="hlt">fluxes</span> but the direction of the <span class="hlt">flux</span> was opposite, toward atmosphere. Even though ponds cover only 8-12% of the HBL area, they accounted for 30% of its total CH4 <span class="hlt">flux</span> to the atmosphere. There is some circumstantial evidence that the ponds are being formed by decomposition of the underlying peat and that this decomposition is being stimulated by the activity of N<span class="hlt">2</span> fixing cyanobacteria that grow in mats at the peat-water interface. The fact that the gas <span class="hlt">fluxes</span> from the ponds were so different from the surrounding vegetated surfaces means that any change in the ratio of pond to vegetated area, as may occur in response to climate change, would affect the total HBL <span class="hlt">fluxes</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B24D..03H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B24D..03H"><span>High-resolution mapping of biogenic carbon <span class="hlt">fluxes</span> to improve urban <span class="hlt">CO</span><span class="hlt">2</span> monitoring, reporting, and verification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hardiman, B. S.; Hutyra, L.; Gately, C.; Raciti, S. M.</p> <p>2014-12-01</p> <p>Urban areas are home to 80% of the US population and 70% of energy related fossil fuel emissions originate from urban areas. Efforts to accurately monitor, report, and verify anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> missions using atmospheric measurements require reliable partitioning of anthropogenic and biogenic sources. Anthropogenic emissions peak during the daytime, coincident with biogenic drawdown of <span class="hlt">CO</span><span class="hlt">2</span>. In contrast, biogenic respiration emissions peak at night when anthropogenic emissions are lower. This temporal aliasing of <span class="hlt">fluxes</span> requires careful modeling of both biogenic and anthropogenic <span class="hlt">fluxes</span> for accurate source attribution through inverse modeling. Biogenic <span class="hlt">fluxes</span> in urban regions can be a significant component of the urban carbon cycle. However, vegetation in urban areas is subject to longer growing seasons, reduced competition, higher rates of nitrogen deposition, and altered patterns of biomass inputs, all interacting to elevate C turnover rates relative to analogous non-urban ecosystems. These conditions suggest that models that ignore urban vegetation or base biogenic <span class="hlt">flux</span> estimates on non-urban forests are likely to produce inaccurate estimates of anthropogenic <span class="hlt">CO</span><span class="hlt">2</span> emissions. Biosphere models often omit biogenic <span class="hlt">fluxes</span> in urban areas despite potentially extensive vegetation coverage. For example, in Massachusetts, models mask out as much as 40% of land area, effectively assuming they have no biological <span class="hlt">flux</span>. This results in a ~32% underestimate of aboveground biomass (AGB) across the state as compared to higher resolution vegetation maps. Our analysis suggests that some common biomass maps may underestimate forest biomass by ~520 Tg C within the state of Massachusetts. Moreover, omitted portions of the state have the highest population density, indicating that we know least about regions where most people live. We combine remote sensing imagery of urban vegetation cover with ground surveys of tree growth and mortality to improve estimates of aboveground biomass and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AMT.....6..817W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AMT.....6..817W"><span>Jena Reference <span class="hlt">Air</span> Set (JRAS): a multi-point scale anchor for isotope measurements of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wendeberg, M.; Richter, J. M.; Rothe, M.; Brand, W. A.</p> <p>2013-03-01</p> <p>The need for a unifying scale anchor for isotopes of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> was brought to light at the 11th WMO/IAEA Meeting of Experts on Carbon Dioxide in Tokyo 2001. During discussions about persistent discrepancies in isotope measurements between the worlds leading laboratories, it was concluded that a unifying scale anchor for Vienna Pee Dee Belemnite (VPDB) of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> was desperately needed. Ten years later, at the 2011 Meeting of Experts on Carbon Dioxide in Wellington, it was recommended that the Jena Reference <span class="hlt">Air</span> Set (JRAS) become the official scale anchor for isotope measurements of <span class="hlt">CO</span><span class="hlt">2</span> in <span class="hlt">air</span> (Brailsford, 2012). The source of <span class="hlt">CO</span><span class="hlt">2</span> used for JRAS is two calcites. After releasing <span class="hlt">CO</span><span class="hlt">2</span> by reaction with phosphoric acid, the gases are mixed into <span class="hlt">CO</span><span class="hlt">2</span>-free <span class="hlt">air</span>. This procedure ensures both isotopic stability and longevity of the <span class="hlt">CO</span><span class="hlt">2</span>. That the reference <span class="hlt">CO</span><span class="hlt">2</span> is generated from calcites and supplied as an <span class="hlt">air</span> mixture is unique to JRAS. This is made to ensure that any measurement bias arising from the extraction procedure is eliminated. As every laboratory has its own procedure for extracting the <span class="hlt">CO</span><span class="hlt">2</span>, this is of paramount importance if the local scales are to be unified with a common anchor. For a period of four years, JRAS has been evaluated through the IMECC1 program, which made it possible to distribute sets of JRAS gases to 13 laboratories worldwide. A summary of data from the six laboratories that have reported the full set of results is given here along with a description of the production and maintenance of the JRAS scale anchors. 1 IMECC refers to the EU project "Infrastructure for Measurements of the European Carbon Cycle" (<a href="http://imecc.ipsl.jussieu.fr/"target="_blank">http://imecc.ipsl.jussieu.fr/</a>).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1170088-distance-dependent-radiation-chemistry-oxidation-versus-hydrogenation-co-electron-irradiated-h2o-co-h2o-ices','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1170088-distance-dependent-radiation-chemistry-oxidation-versus-hydrogenation-co-electron-irradiated-h2o-co-h2o-ices"><span>Distance-dependent radiation chemistry: Oxidation versus hydrogenation of <span class="hlt">CO</span> in electron-irradiated H<span class="hlt">2</span>O/<span class="hlt">CO</span>/H<span class="hlt">2</span>O <span class="hlt">ices</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Petrik, Nikolay G.; Monckton, Rhiannon J.; Koehler, Sven</p> <p></p> <p>Electron-stimulated oxidation of <span class="hlt">CO</span> in layered H<span class="hlt">2</span>O/<span class="hlt">CO</span>/H<span class="hlt">2</span>O <span class="hlt">ices</span> was investigated with infrared reflection-absorption spectroscopy (IRAS) as function of the distance of the <span class="hlt">CO</span> layer from the water/vacuum interface. The results show that while both oxidation and reduction reactions occur within the irradiated water films, there are distinct regions where either oxidation or reduction reactions are dominant. At depths less than ~ 15 ML, <span class="hlt">CO</span> oxidation dominates over the sequential hydrogenation of <span class="hlt">CO</span> to methanol (CH3OH), and <span class="hlt">CO</span><span class="hlt">2</span> is the major product of <span class="hlt">CO</span> oxidation, consistent with previous observations. At its highest yield, <span class="hlt">CO</span><span class="hlt">2</span> accounts for ~45% of all the reactedmore » <span class="hlt">CO</span>. Another oxidation product is identified as the formate anion (HCO<span class="hlt">2</span>-). In contrast, for <span class="hlt">CO</span> buried more than ~ 35 ML below the water/vacuum interface, the <span class="hlt">CO</span>-to-methanol conversion efficiency is close to 100%. Production of <span class="hlt">CO</span><span class="hlt">2</span> and formate are not observed for the more deeply buried <span class="hlt">CO</span> layers, where hydrogenation dominates. Experiments with <span class="hlt">CO</span> dosed on pre-irradiated ASW samples suggest that OH radicals are primarily responsible for the oxidation reactions. Possible mechanisms of <span class="hlt">CO</span> oxidation, involving primary and secondary processes of water radiolysis at low temperature, are discussed. The observed distance-dependent radiation chemistry results from the higher mobility of hydrogen atoms that are created by the interaction of the 100 eV electrons with the water films. These hydrogen atoms, which are primarily created at or near the water/vacuum interface, can desorb from or diffuse into the water films, while the less-mobile OH radicals remain in the near-surface zone resulting in preferential oxidation reactions there. The diffusing hydrogen atoms are responsible for the hydrogenation reactions that are dominant for the more deeply buried <span class="hlt">CO</span> layers.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMPP41F..08W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMPP41F..08W"><span>Polar <span class="hlt">Ice</span> Sheets Drive Paleohydroclimate Affecting Terrestrial Plant Distribution and <span class="hlt">CO</span><span class="hlt">2</span> Exchange Potential during the Upper Carboniferous</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>White, J. D.; Poulsen, C. J.; Montanez, I. P.; McElwain, J.; Wilson, J. P.; Hren, M. T.</p> <p>2016-12-01</p> <p>Variation in atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration and presence or absence of polar <span class="hlt">ice</span> sheets simulated for 310 mya using the GENESIS model show changes in terrestrial temperature, precipitation, and potential evapotranspiration at mid and lower latitudes. Classifying the data into Holdridge life zones for simulations with 280, 560, and 1120 ppm <span class="hlt">CO</span><span class="hlt">2</span>, in the presence of a southern Gondwanan <span class="hlt">ice</span> sheet resulted in progressive increase of cool temperate, humid-to-subhumid and tropical subhumid zones. Without the <span class="hlt">ice</span> sheet, subtropical subhumid to semiarid zones expanded. Simulation results show that approximately 50% of the land area was classified as polar or tundra followed by 35 to 42%, depending on the scenario, classified as sub-tropical semiarid-to-subhumid. Only 5-8% were classified as temperate humid-to-subhumid or tropical humid-to-perhumid. Also, the absence of <span class="hlt">ice</span> sheets reduced the moister sub-climates, such as within the tropical climate zone. Because different plant assemblages dominated each climate zone, for example cordaitaleans in the subtropical and medullosans and lycophytes in the tropics, physiological differences in these plants may have resulted in unequal <span class="hlt">CO</span><span class="hlt">2</span> exchange feedbacks to the atmosphere during climate shifts. Previous physiological modeling based on plant foliar traits indicates that late Paleozoic plant species differed in <span class="hlt">CO</span><span class="hlt">2</span> uptake capacity with highest sensitivity to water availability during periods with low atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration. This implies that vegetation climate feedbacks during this period may have been non-uniform during climate change events. Inference of plant contribution to climate forcing must rely on understanding geographic distribution of affected vegetation, inherent vegetation physiological properties, and antecedent atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentrations. Our results indicate that seasonally dry climates prevailed in the low-latitude land area, and that slightly cooler temperatures than today must be considered. This</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B21H0573M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B21H0573M"><span>Beyond the Methanogenic Black-Box: Greenhouse Gas <span class="hlt">Fluxes</span> (<span class="hlt">CO</span><span class="hlt">2</span>, CH4, N<span class="hlt">2</span>O) as Evidence for Wetlands as Dynamic Redox Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mcnicol, G.; Knox, S. H.; Sturtevant, C. S.; Baldocchi, D. D.; Silver, W. L.</p> <p>2015-12-01</p> <p>Seminal wetland research in the 1990s demonstrated that annual methane (CH4) <span class="hlt">fluxes</span> scaled positively with ecosystem production across distinctive wetlands globally. This relationship implies a model of flooded wetland ecosystems as 'methanogenic black-boxes'; poised at a low redox state, and tending to release a fixed fraction of incoming annual productivity as CH4. In contrast, recent studies have reported high ratios of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) to CH4 emissions, and are adding to a body of evidence suggesting wetlands can vary more widely in their redox state. To explore this apparent incongruence we used principles of redox thermodynamics and laboratory experiments to develop predictions of wetland greenhouse gas (GHG) <span class="hlt">fluxes</span> under different redox regimes. We then used a field study to test the hypothesis that ecosystem seasonality in gross primary productivity (GPP) and temperature would drive changes in GHG emissions, mediated by a dynamic - as opposed to static - redox regime. We estimated wetland GHG emissions from an emergent marsh in the Sacramento Delta, CA from March 2014-2015. We measured <span class="hlt">CO</span><span class="hlt">2</span>, CH4 and N<span class="hlt">2</span>O emissions via diffusion and ebullition with manual sampling, and whole-ecosystem <span class="hlt">fluxes</span> of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 using eddy-covariance. Ebullition and diffusive CH4 <span class="hlt">fluxes</span> were strongly seasonal, with minimum rates (0.86 and 0.35 mg C-CH­­4 m-<span class="hlt">2</span> yr-1, respectively) during winter, and maximum rates (1.3 and 1.8 g C-CH­­4 m-<span class="hlt">2</span> yr-1, respectively) during the summer growing season. In contrast, winter diffusive <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> (494 g C-<span class="hlt">CO</span><span class="hlt">2</span> m-<span class="hlt">2</span> yr-1) and fall bubble <span class="hlt">CO</span><span class="hlt">2</span> concentrations (1.49%) were highest, despite being seasons of lower GPP, temperature, and CH4 <span class="hlt">flux</span>. Further, diffusive and ebullition <span class="hlt">fluxes</span> of N<span class="hlt">2</span>O showed zero net <span class="hlt">flux</span> only during spring and summer months, whereas the wetland was a significant source of N<span class="hlt">2</span>O during winter (81.<span class="hlt">2</span> ± 24.4 mg N-N<span class="hlt">2</span>O m-<span class="hlt">2</span> yr-1). These seasonal <span class="hlt">flux</span> dynamics contradict a 'methanogenic black box' model of wetland redox, which</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21096927','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21096927"><span>Tactile communication using a <span class="hlt">CO</span>(<span class="hlt">2</span>) <span class="hlt">flux</span> stimulation for blind or deafblind people.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>da Cunha, Jose Carlos; Bordignon, Luiz Alberto; Nohama, Percy</p> <p>2010-01-01</p> <p>This paper describes a tactile stimulation system for producing nonvisual image patterns to blind or deafblind people. The stimulator yields a <span class="hlt">CO</span>(<span class="hlt">2</span>) pulsatile <span class="hlt">flux</span> directed to the user's skin throughout a needle that is coupled to a <span class="hlt">2</span>-D tactile plotter. The fluxtactile plotter operates with two step motor mounted on a wood structure, controlled by a program developed to produce alphanumerical characters and geometric figures of different size and speed, which will be used to investigate the psychophysical properties of this kind of tactile communication. <span class="hlt">CO</span>(<span class="hlt">2</span>) is provided by a cylinder that delivers a stable <span class="hlt">flux</span>, which is converted to a pulsatile mode through a high frequency solenoid valve that can chop it up to 1 kHz. Also, system temperature is controlled by a Peltier based device. Tests on the prototype indicate that the system is a valuable tool to investigate the psychophysical properties of the skin in response to stimulation by <span class="hlt">CO</span>(<span class="hlt">2</span>) jet, allowing a quantitative and qualitative analysis as a function of stimulation parameters. With the system developed, it was possible to plot the geometric figures proposed: triangles, rectangles and octagons, in different sizes and speeds, and verify the control of the frequency of <span class="hlt">CO</span>(<span class="hlt">2</span>) jet stimuli.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33A2334Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33A2334Z"><span>Constraining biosphere <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at regional scale with WRF-<span class="hlt">CO</span><span class="hlt">2</span> 4DVar assimilation system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, T.</p> <p>2017-12-01</p> <p>The WRF-<span class="hlt">CO</span><span class="hlt">2</span> 4DVar assimilation system is updated to include (1) operators for tower based observations (<span class="hlt">2</span>) chemistry initial and boundary condition in the state vector (3) mechanism for aggregation from simulation model grid to state vector space. The update system is first tested with synthetic data to ensure its accuracy. The system is then used to test regional scale <span class="hlt">CO</span><span class="hlt">2</span> inversion at MCI (Midcontinental intensive) sites where <span class="hlt">CO</span><span class="hlt">2</span> mole fraction data were collected at multiple high towers during 2007-2008. The model domain is set to center on Iowa and include 8 towers within its boundary, and it is of 12x12km horizontal grid spacing. First, the relative impacts of the initial and boundary condition are assessed by the system's adjoint model. This is done with 24, 48, 72 hour time span. Second, we assessed the impacts of the transport error, including the misrepresentation of the boundary layer and cumulus activities. Third, we evaluated the different aggregation approach from the native model grid to the control variables (including scaling factors for <span class="hlt">flux</span>, initial and boundary conditions). Four, we assessed the inversion performance using <span class="hlt">CO</span><span class="hlt">2</span> observation with different time-interval, and from different tower levels. We also examined the appropriate treatment of the background and observation error covariance in relation with these varying observation data sets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010TCry....4..227D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010TCry....4..227D"><span>Brief Communication: Ikaite (Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) discovered in Arctic sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dieckmann, G. S.; Nehrke, G.; Uhlig, C.; Göttlicher, J.; Gerland, S.; Granskog, M. A.; Thomas, D. N.</p> <p>2010-05-01</p> <p>We report for the first time on the discovery of calcium carbonate crystals as ikaite (Ca<span class="hlt">CO</span>3·6H<span class="hlt">2</span>O) in sea <span class="hlt">ice</span> from the Arctic (Kongsfjorden, Svalbard) as confirmed by morphology and indirectly by X-ray diffraction as well as XANES spectroscopy of its amorophous decomposition product. This finding demonstrates that the precipitation of calcium carbonate during the freezing of sea <span class="hlt">ice</span> is not restricted to the Antarctic, where it was observed for the first time in 2008. This observation is an important step in the quest to quantify its impact on the sea <span class="hlt">ice</span> driven carbon cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GBioC..31..709G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GBioC..31..709G"><span>Calculating the balance between atmospheric <span class="hlt">CO</span><span class="hlt">2</span> drawdown and organic carbon oxidation in subglacial hydrochemical systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Graly, Joseph A.; Drever, James I.; Humphrey, Neil F.</p> <p>2017-04-01</p> <p>In order to constrain <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> from biogeochemical processes in subglacial environments, we model the evolution of pH and alkalinity over a range of subglacial weathering conditions. We show that subglacial waters reach or exceed atmospheric p<span class="hlt">CO</span><span class="hlt">2</span> levels when atmospheric gases are able to partially access the subglacial environment. Subsequently, closed system oxidation of sulfides is capable of producing p<span class="hlt">CO</span><span class="hlt">2</span> levels well in excess of atmosphere levels without any input from the decay of organic matter. We compared this model to published pH and alkalinity measurements from 21 glaciers and <span class="hlt">ice</span> sheets. Most subglacial waters are near atmospheric p<span class="hlt">CO</span><span class="hlt">2</span> values. The assumption of an initial period of open system weathering requires substantial organic carbon oxidation in only 4 of the 21 analyzed <span class="hlt">ice</span> bodies. If the subglacial environment is assumed to be closed from any input of atmospheric gas, large organic carbon inputs are required in nearly all cases. These closed system assumptions imply that order of 10 g m-<span class="hlt">2</span> y-1 of organic carbon are removed from a typical subglacial environment—a rate too high to represent soil carbon built up over previous interglacial periods and far in excess of <span class="hlt">fluxes</span> of surface deposited organic carbon. Partial open system input of atmospheric gases is therefore likely in most subglacial environments. The decay of organic carbon is still important to subglacial inorganic chemistry where substantial reserves of ancient organic carbon are found in bedrock. In glaciers and <span class="hlt">ice</span> sheets on silicate bedrock, substantial long-term drawdown of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> occurs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.C12A..01A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.C12A..01A"><span>Turbulent Surface <span class="hlt">Flux</span> Measurements over Snow-Covered Sea <span class="hlt">Ice</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andreas, E. L.; Fairall, C. W.; Grachev, A. A.; Guest, P. S.; Jordan, R. E.; Persson, P. G.</p> <p>2006-12-01</p> <p>Our group has used eddy correlation to make over 10,000 hours of measurements of the turbulent momentum and heat <span class="hlt">fluxes</span> over snow-covered sea <span class="hlt">ice</span> in both the Arctic and the Antarctic. Polar sea <span class="hlt">ice</span> is an ideal site for studying fundamental processes for turbulent exchange over snow. Both our Arctic and Antarctic sites---in the Beaufort Gyre and deep into the Weddell Sea, respectively---were expansive, flat areas with continuous snow cover; and both were at least 300 km from any topography that might have complicated the atmospheric flow. In this presentation, we will review our measurements of the turbulent <span class="hlt">fluxes</span> of momentum and sensible and latent heat. In particular, we will describe our experiences making turbulence instruments work in the fairly harsh polar, marine boundary layer. For instance, several of our Arctic sites were remote from our main camp and ran unattended for a week at a time. Besides simply making <span class="hlt">flux</span> measurements, we have been using the data to develop a bulk <span class="hlt">flux</span> algorithm and to study fundamental turbulence processes in the atmospheric surface layer. The bulk <span class="hlt">flux</span> algorithm predicts the turbulent surface <span class="hlt">fluxes</span> from mean meteorological quantities and, thus, will find use in data analyses and models. For example, components of the algorithm are already embedded in our one- dimensional mass and energy budget model SNTHERM. Our fundamental turbulence studies have included deducing new scaling regimes in the stable boundary layer; examining the Monin-Obukhov similarity functions, especially in stable stratification; and evaluating the von Kármán constant with the largest atmospheric data set ever applied to such a study. During this presentation, we will highlight some of this work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010096159','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010096159"><span>Balance Mass <span class="hlt">Flux</span> and Velocity Across the Equilibrium Line in <span class="hlt">Ice</span> Drainage Systems of Greenland</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zwally, H. Jay; Giovinetto, Mario B.; Koblinsky, Chester J. (Technical Monitor)</p> <p>2001-01-01</p> <p>Estimates of balance mass <span class="hlt">flux</span> and the depth-averaged <span class="hlt">ice</span> velocity through the cross-section aligned with the equilibrium line are produced for each of six drainage systems in Greenland. (The equilibrium line, which lies at approximately 1200 m elevation on the <span class="hlt">ice</span> sheet, is the boundary between the area of net snow accumulation at higher elevations and the areas of net melting at lower elevations around the <span class="hlt">ice</span> sheet.) <span class="hlt">Ice</span> drainage divides and six major drainage systems are delineated using surface topography from ERS (European Remote Sensing) radar altimeter data. The net accumulation rate in the accumulation zone bounded by the equilibrium line is 399 Gt/yr and net ablation rate in the remaining area is 231 Gt/yr. (1 GigaTon of <span class="hlt">ice</span> is 1090 kM(exp 3). The mean balance mass <span class="hlt">flux</span> and depth-averaged <span class="hlt">ice</span> velocity at the cross-section aligned with the modeled equilibrium line are 0.1011 Gt kM(exp -<span class="hlt">2</span>)/yr and 0.111 km/yr, respectively, with little variation in these values from system to system. The ratio of the <span class="hlt">ice</span> mass above the equilibrium line to the rate of mass output implies an effective exchange time of approximately 6000 years for total mass exchange. The range of exchange times, from a low of 3 ka in the SE drainage system to 14 ka in the NE, suggests a rank as to which regions of the <span class="hlt">ice</span> sheet may respond more rapidly to climate fluctuations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CliPa...9.2789S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CliPa...9.2789S"><span>High-resolution mineral dust and sea <span class="hlt">ice</span> proxy records from the Talos Dome <span class="hlt">ice</span> core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schüpbach, S.; Federer, U.; Kaufmann, P. R.; Albani, S.; Barbante, C.; Stocker, T. F.; Fischer, H.</p> <p>2013-12-01</p> <p>In this study we report on new non-sea salt calcium (nssCa<span class="hlt">2</span>+, mineral dust proxy) and sea salt sodium (ssNa+, sea <span class="hlt">ice</span> proxy) records along the East Antarctic Talos Dome deep <span class="hlt">ice</span> core in centennial resolution reaching back 150 thousand years (ka) before present. During glacial conditions nssCa<span class="hlt">2</span>+ <span class="hlt">fluxes</span> in Talos Dome are strongly related to temperature as has been observed before in other deep Antarctic <span class="hlt">ice</span> core records, and has been associated with synchronous changes in the main source region (southern South America) during climate variations in the last glacial. However, during warmer climate conditions Talos Dome mineral dust input is clearly elevated compared to other records mainly due to the contribution of additional local dust sources in the Ross Sea area. Based on a simple transport model, we compare nssCa<span class="hlt">2</span>+ <span class="hlt">fluxes</span> of different East Antarctic <span class="hlt">ice</span> cores. From this multi-site comparison we conclude that changes in transport efficiency or atmospheric lifetime of dust particles do have a minor effect compared to source strength changes on the large-scale concentration changes observed in Antarctic <span class="hlt">ice</span> cores during climate variations of the past 150 ka. Our transport model applied on <span class="hlt">ice</span> core data is further validated by climate model data. The availability of multiple East Antarctic nssCa<span class="hlt">2</span>+ records also allows for a revision of a former estimate on the atmospheric <span class="hlt">CO</span><span class="hlt">2</span> sensitivity to reduced dust induced iron fertilisation in the Southern Ocean during the transition from the Last Glacial Maximum to the Holocene (T1). While a former estimate based on the EPICA Dome C (EDC) record only suggested 20 ppm, we find that reduced dust induced iron fertilisation in the Southern Ocean may be responsible for up to 40 ppm of the total atmospheric <span class="hlt">CO</span><span class="hlt">2</span> increase during T1. During the last interglacial, ssNa+ levels of EDC and EPICA Dronning Maud Land (EDML) are only half of the Holocene levels, in line with higher temperatures during that period, indicating much reduced sea</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E2709R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E2709R"><span>Radiation Effects in Hydrogen-Laden Porous Water <span class="hlt">Ice</span> Films: Implications for Interstellar <span class="hlt">Ices</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raut, Ujjwal; Baragiola, Raul; Mitchell, Emma; Shi, Jianming</p> <p></p> <p>H _{<span class="hlt">2</span>} is the dominant gas in the dense clouds of the interstellar medium (ISM). At densities of 10 (5) cm (-3) , an H _{<span class="hlt">2</span>} molecule arrives at the surface of a 0.1 mum-sized, <span class="hlt">ice</span>-covered dust grain once every few seconds [1]. At 10 K, H _{<span class="hlt">2</span>} can diffuse into the pores of the <span class="hlt">ice</span> mantle and adsorb at high-energy binding sites, loading the <span class="hlt">ice</span> with hydrogen over the lifetime of the cloud. These icy grains are also impacted by galactic cosmic rays and stellar winds (in clouds with embedded protostar). Based on the available cosmic proton <span class="hlt">flux</span> spectrum [<span class="hlt">2</span>], we estimate a small impact rate of nearly 1 hit per year on a 0.1 μm sized grain, or 10 (-7) times the impact frequency of the neutral H _{<span class="hlt">2</span>}. The energy deposited by such impacts can release the adsorbed H _{<span class="hlt">2</span>} into the gas phase (impact desorption or sputtering). Recently, we have reported on a new process of ion-induced enhanced adsorption, where molecules from the gas phase are incorporated into the film when irradiation is performed in the presence of ambient gas [3]. The interplay between ion-induced ejection and adsorption can be important in determining the gas-solid balance in the ISM. To understand the effects of cosmic rays/stellar winds impacts on interstellar <span class="hlt">ice</span> immersed in H _{<span class="hlt">2</span>} gas, we have performed irradiation of porous amorphous <span class="hlt">ice</span> films loaded with H _{<span class="hlt">2</span>} through <span class="hlt">co</span>-deposition or adsorption following growth. The irradiations were performed with 100 keV H (+) using <span class="hlt">fluxes</span> of 10 (10) -10 (12) H (+) cm (-<span class="hlt">2</span>) s (-1) at 7 K, in presence of ambient H _{<span class="hlt">2</span>} at pressures ranging from 10 (-5) to 10 (-8) Torr. Our initial results show a net loss in adsorbed H _{<span class="hlt">2</span>} during irradiation, from competing ion-induced ejection and adsorption. The H _{<span class="hlt">2</span>} loss per ion decreases exponentially with fluence, with a cross-section of 10 (-13) cm (<span class="hlt">2</span>) . In addition to hydrogen removal, irradiation also leads to trapping of H _{<span class="hlt">2</span>} in the <span class="hlt">ice</span> film, from closing of the pores during irradiation [4]. As a result, <span class="hlt">2</span>.6 percent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFM.B41A..07P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFM.B41A..07P"><span>Land-use change effects on <span class="hlt">fluxes</span> and isotopic composition of <span class="hlt">CO</span><span class="hlt">2</span> and CH4 in Panama, and possible insights into the atmospheric H<span class="hlt">2</span> cycle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pendall, E.; Schwendenmann, L.; Potvin, C.</p> <p>2003-12-01</p> <p>Land-use changes in tropical regions are believed to release a quantity of C to the atmosphere which is similar in magnitude to the entire "missing" sink for anthropogenic <span class="hlt">CO</span><span class="hlt">2</span>. Our research attempts to evaluate carbon cycling in three land-cover systems in central Panama: cow pasture, native tree plantation, and undisturbed moist forest. In this ongoing project, we are collecting samples of <span class="hlt">air</span> from profiles in the stable, nocturnal boundary layer, which is dominated by ecosystem respiration. Samples are analyzed for <span class="hlt">CO</span><span class="hlt">2</span> and its isotopes, CH4 and its C isotopic composition, N<span class="hlt">2</span>O, H<span class="hlt">2</span>, <span class="hlt">CO</span>, and SF6. We use a <span class="hlt">flux</span>-gradient method to estimate ecosystem-scale <span class="hlt">fluxes</span> of trace gases from soil to the atmosphere. Keeling plot intercepts reflect the respiratory contribution of C3 and C4 biomass under contrasting land cover systems, and how this varies with pronounced wet-dry seasonal cycles. C isotopes of methane and gradients of molecular hydrogen provide insight into the source of methane production from pasture and plantation soils. Rainforest soils, in contrast, are sinks for both atmospheric methane and hydrogen. The process oriented nature of this field experiment will contribute to parameterization of carbon cycle models at a variety of spatial scales.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JVGR..327..208R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JVGR..327..208R"><span>Diffuse degassing at Longonot volcano, Kenya: Implications for <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in continental rifts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Robertson, Elspeth; Biggs, Juliet; Edmonds, Marie; Clor, Laura; Fischer, Tobias P.; Vye-Brown, Charlotte; Kianji, Gladys; Koros, Wesley; Kandie, Risper</p> <p>2016-11-01</p> <p>Magma movement, fault structures and hydrothermal systems influence volatile emissions at rift volcanoes. Longonot is a Quaternary caldera volcano located in the southern Kenyan Rift, where regional extension controls recent shallow magma ascent. Here we report the results of a soil carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>) survey in the vicinity of Longonot volcano, as well as fumarolic gas compositions and carbon isotope data. The total non-biogenic <span class="hlt">CO</span><span class="hlt">2</span> degassing is estimated at < 300 kg d- 1, and is largely controlled by crater faults and fractures close to the summit. Thus, recent volcanic structures, rather than regional tectonics, control fluid pathways and degassing. Fumarolic gases are characterised by a narrow range in carbon isotope ratios (δ13C), from - 4.7‰ to - 6.4‰ (vs. PDB) suggesting a magmatic origin with minor contributions from biogenic <span class="hlt">CO</span><span class="hlt">2</span>. Comparison with other degassing measurements in the East African Rift shows that records of historical eruptions or unrest do not correspond directly to the magnitude of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from volcanic centres, which may instead reflect the current size and characteristics of the subsurface magma reservoir. Interestingly, the integrated <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from faulted rift basins is reported to be an order of magnitude higher than that from any of the volcanic centres for which <span class="hlt">CO</span><span class="hlt">2</span> surveys have so far been reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1412635','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1412635"><span>Two-component <span class="hlt">flux</span> explanation for the high energy neutrino events at <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Chen, Chien-Yi; Dev, P. S. Bhupal; Soni, Amarjit</p> <p></p> <p>In understanding the spectral and flavor composition of the astrophysical neutrino <span class="hlt">flux</span> responsible for the recently observed ultrahigh-energy events at <span class="hlt">Ice</span>Cube we see how important both astrophysics and particle physics are. Here, we perform a statistical likelihood analysis to the three-year <span class="hlt">Ice</span>Cube data and derive the allowed range of the spectral index and <span class="hlt">flux</span> normalization for various well-motivated physical flavor compositions at the source. While most of the existing analyses so far assume the flavor composition of the neutrinos at an astrophysical source to be (1:<span class="hlt">2</span>:0), it seems rather unnatural to assume only one type of source, once we recognizemore » the possibility of at least two physical sources. Bearing this in mind, we entertain the possibility of a two-component source for the analysis of <span class="hlt">Ice</span>Cube data. It appears that our two-component hypothesis explains some key features of the data better than a single-component scenario; i.e. it addresses the apparent energy gap between 400 TeV and about 1 PeV and easily accommodates the observed track-to-shower ratio. Given the extreme importance of the flavor composition for the correct interpretation of the underlying astrophysical processes as well as for the ramification for particle physics, this two-component <span class="hlt">flux</span> should be tested as more data is accumulated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1412635-two-component-flux-explanation-high-energy-neutrino-events-icecube','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1412635-two-component-flux-explanation-high-energy-neutrino-events-icecube"><span>Two-component <span class="hlt">flux</span> explanation for the high energy neutrino events at <span class="hlt">Ice</span>Cube</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Chen, Chien-Yi; Dev, P. S. Bhupal; Soni, Amarjit</p> <p>2015-10-01</p> <p>In understanding the spectral and flavor composition of the astrophysical neutrino <span class="hlt">flux</span> responsible for the recently observed ultrahigh-energy events at <span class="hlt">Ice</span>Cube we see how important both astrophysics and particle physics are. Here, we perform a statistical likelihood analysis to the three-year <span class="hlt">Ice</span>Cube data and derive the allowed range of the spectral index and <span class="hlt">flux</span> normalization for various well-motivated physical flavor compositions at the source. While most of the existing analyses so far assume the flavor composition of the neutrinos at an astrophysical source to be (1:<span class="hlt">2</span>:0), it seems rather unnatural to assume only one type of source, once we recognizemore » the possibility of at least two physical sources. Bearing this in mind, we entertain the possibility of a two-component source for the analysis of <span class="hlt">Ice</span>Cube data. It appears that our two-component hypothesis explains some key features of the data better than a single-component scenario; i.e. it addresses the apparent energy gap between 400 TeV and about 1 PeV and easily accommodates the observed track-to-shower ratio. Given the extreme importance of the flavor composition for the correct interpretation of the underlying astrophysical processes as well as for the ramification for particle physics, this two-component <span class="hlt">flux</span> should be tested as more data is accumulated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A41F0091W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A41F0091W"><span>An Inversion Analysis of Recent Variability in <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Using GOSAT and In Situ Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, J. S.; Kawa, S. R.; Baker, D. F.; Collatz, G. J.</p> <p>2016-12-01</p> <p>About one-half of the global <span class="hlt">CO</span><span class="hlt">2</span> emissions from fossil fuel combustion and deforestation accumulates in the atmosphere, where it contributes to global warming. The rest is taken up by vegetation and the ocean. The precise contribution of the two sinks and their location and year-to-year variability are not well understood. We use two different approaches, batch Bayesian synthesis inversion and variational data assimilation, to deduce the global spatiotemporal distributions of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> during 2009-2010. One of our objectives is to assess different sources of uncertainties in inferred <span class="hlt">fluxes</span>, including uncertainties in prior <span class="hlt">flux</span> estimates and observations, and differences in inversion techniques. For prior constraints, we utilize <span class="hlt">fluxes</span> and uncertainties from the CASA-GFED model of the terrestrial biosphere and biomass burning driven by satellite observations. We also use measurement-based ocean <span class="hlt">flux</span> estimates and fixed fossil <span class="hlt">CO</span><span class="hlt">2</span> emissions. Our inversions incorporate column <span class="hlt">CO</span><span class="hlt">2</span> measurements from the GOSAT satellite (ACOS retrieval, bias-corrected) and in situ observations (individual flask and afternoon-average continuous observations) to estimate <span class="hlt">fluxes</span> in 108 regions over 8-day intervals for the batch inversion and at 3° x 3.75° weekly for the variational system. Relationships between <span class="hlt">fluxes</span> and atmospheric concentrations are derived consistently for the two inversion systems using the PCTM transport model with MERRA meteorology. We compare the posterior <span class="hlt">fluxes</span> and uncertainties derived using different data sets and the two inversion approaches, and evaluate the posterior atmospheric concentrations against independent data including aircraft measurements. The optimized <span class="hlt">fluxes</span> generally resemble each other and those from other studies. For example, a GOSAT-only inversion suggests a shift in the global sink from the tropics/south to the north relative to the prior and to an in-situ-only inversion. The posterior <span class="hlt">fluxes</span> of the GOSAT inversion are better</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C33C1202F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C33C1202F"><span>Determination of a Critical Sea <span class="hlt">Ice</span> Thickness Threshold for the Central Arctic Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ford, V.; Frauenfeld, O. W.; Nowotarski, C. J.</p> <p>2017-12-01</p> <p>While sea <span class="hlt">ice</span> extent is readily measurable from satellite observations and can be used to assess the overall survivability of the Arctic sea <span class="hlt">ice</span> pack, determining the spatial variability of sea <span class="hlt">ice</span> thickness remains a challenge. Turbulent and conductive heat <span class="hlt">fluxes</span> are extremely sensitive to <span class="hlt">ice</span> thickness but are dominated by the sensible heat <span class="hlt">flux</span>, with energy exchange expected to increase with thinner <span class="hlt">ice</span> cover. <span class="hlt">Fluxes</span> over open water are strongest and have the greatest influence on the atmosphere, while <span class="hlt">fluxes</span> over thick sea <span class="hlt">ice</span> are minimal as heat conduction from the ocean through thick <span class="hlt">ice</span> cannot reach the atmosphere. We know that turbulent energy <span class="hlt">fluxes</span> are strongest over open ocean, but is there a "critical thickness of <span class="hlt">ice</span>" where <span class="hlt">fluxes</span> are considered non-negligible? Through polar-optimized Weather Research and Forecasting model simulations, this study assesses how the wintertime Arctic surface boundary layer, via sensible heat <span class="hlt">flux</span> exchange and surface <span class="hlt">air</span> temperature, responds to sea <span class="hlt">ice</span> thinning. The region immediately north of Franz Josef Land is characterized by a thickness gradient where sea <span class="hlt">ice</span> transitions from the thickest multi-year <span class="hlt">ice</span> to the very thin marginal <span class="hlt">ice</span> seas. This provides an ideal location to simulate how the diminishing Arctic sea <span class="hlt">ice</span> interacts with a warming atmosphere. Scenarios include both fixed sea surface temperature domains for idealized thickness variability, and fixed <span class="hlt">ice</span> fields to detect changes in the ocean-<span class="hlt">ice</span>-atmosphere energy exchange. Results indicate that a critical thickness threshold exists below 1 meter. The threshold is between 0.4-1 meters thinner than the critical thickness for melt season survival - the difference between first year and multi-year <span class="hlt">ice</span>. Turbulent heat <span class="hlt">fluxes</span> and surface <span class="hlt">air</span> temperature increase as sea <span class="hlt">ice</span> thickness transitions from perennial <span class="hlt">ice</span> to seasonal <span class="hlt">ice</span>. While models predict a sea <span class="hlt">ice</span> free Arctic at the end of the warm season in future decades, sea <span class="hlt">ice</span> will continue to transform</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhRvD..84h2001A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhRvD..84h2001A"><span>Search for a diffuse <span class="hlt">flux</span> of astrophysical muon neutrinos with the <span class="hlt">Ice</span>Cube 40-string detector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abbasi, R.; Abdou, Y.; Abu-Zayyad, T.; Adams, J.; Aguilar, J. A.; Ahlers, M.; Altmann, D.; Andeen, K.; Auffenberg, J.; Bai, X.; Baker, M.; Barwick, S. W.; Bay, R.; Bazo Alba, J. L.; Beattie, K.; Beatty, J. J.; Bechet, S.; Becker, J. K.; Becker, K.-H.; Benabderrahmane, M. L.; Benzvi, S.; Berdermann, J.; Berghaus, P.; Berley, D.; Bernardini, E.; Bertrand, D.; Besson, D. Z.; Bindig, D.; Bissok, M.; Blaufuss, E.; Blumenthal, J.; Boersma, D. J.; Bohm, C.; Bose, D.; Böser, S.; Botner, O.; Brown, A. M.; Buitink, S.; Caballero-Mora, K. S.; Carson, M.; Chirkin, D.; Christy, B.; Clem, J.; Clevermann, F.; Cohen, S.; Colnard, C.; Cowen, D. F.; D'Agostino, M. V.; Danninger, M.; Daughhetee, J.; Davis, J. C.; de Clercq, C.; Demirörs, L.; Denger, T.; Depaepe, O.; Descamps, F.; Desiati, P.; de Vries-Uiterweerd, G.; Deyoung, T.; Díaz-Vélez, J. C.; Dierckxsens, M.; Dreyer, J.; Dumm, J. P.; Ehrlich, R.; Eisch, J.; Ellsworth, R. W.; Engdegård, O.; Euler, S.; Evenson, P. A.; Fadiran, O.; Fazely, A. R.; Fedynitch, A.; Feintzeig, J.; Feusels, T.; Filimonov, K.; Finley, C.; Fischer-Wasels, T.; Foerster, M. M.; Fox, B. D.; Franckowiak, A.; Franke, R.; Gaisser, T. K.; Gallagher, J.; Gerhardt, L.; Gladstone, L.; Glüsenkamp, T.; Goldschmidt, A.; Goodman, J. A.; Gora, D.; Grant, D.; Griesel, T.; Groß, A.; Grullon, S.; Gurtner, M.; Ha, C.; Hajismail, A.; Hallgren, A.; Halzen, F.; Han, K.; Hanson, K.; Heinen, D.; Helbing, K.; Herquet, P.; Hickford, S.; Hill, G. C.; Hoffman, K. D.; Homeier, A.; Hoshina, K.; Hubert, D.; Huelsnitz, W.; Hülß, J.-P.; Hulth, P. O.; Hultqvist, K.; Hussain, S.; Ishihara, A.; Jacobsen, J.; Japaridze, G. S.; Johansson, H.; Joseph, J. M.; Kampert, K.-H.; Kappes, A.; Karg, T.; Karle, A.; Kenny, P.; Kiryluk, J.; Kislat, F.; Klein, S. R.; Köhne, J.-H.; Kohnen, G.; Kolanoski, H.; Köpke, L.; Kopper, S.; Koskinen, D. J.; Kowalski, M.; Kowarik, T.; Krasberg, M.; Krings, T.; Kroll, G.; Kurahashi, N.; Kuwabara, T.; Labare, M.; Lafebre, S.; Laihem, K.; Landsman, H.; Larson, M. J.; Lauer, R.; Lünemann, J.; Madsen, J.; Majumdar, P.; Marotta, A.; Maruyama, R.; Mase, K.; Matis, H. S.; Meagher, K.; Merck, M.; Mészáros, P.; Meures, T.; Middell, E.; Milke, N.; Miller, J.; Montaruli, T.; Morse, R.; Movit, S. M.; Nahnhauer, R.; Nam, J. W.; Naumann, U.; Nießen, P.; Nygren, D. R.; Odrowski, S.; Olivas, A.; Olivo, M.; O'Murchadha, A.; Ono, M.; Panknin, S.; Paul, L.; Pérez de Los Heros, C.; Petrovic, J.; Piegsa, A.; Pieloth, D.; Porrata, R.; Posselt, J.; Price, P. B.; Przybylski, G. T.; Rawlins, K.; Redl, P.; Resconi, E.; Rhode, W.; Ribordy, M.; Rizzo, A.; Rodrigues, J. P.; Roth, P.; Rothmaier, F.; Rott, C.; Ruhe, T.; Rutledge, D.; Ruzybayev, B.; Ryckbosch, D.; Sander, H.-G.; Santander, M.; Sarkar, S.; Schatto, K.; Schmidt, T.; Schönwald, A.; Schukraft, A.; Schultes, A.; Schulz, O.; Schunck, M.; Seckel, D.; Semburg, B.; Seo, S. H.; Sestayo, Y.; Seunarine, S.; Silvestri, A.; Slipak, A.; Spiczak, G. M.; Spiering, C.; Stamatikos, M.; Stanev, T.; Stephens, G.; Stezelberger, T.; Stokstad, R. G.; Stössl, A.; Stoyanov, S.; Strahler, E. A.; Straszheim, T.; Stür, M.; Sullivan, G. W.; Swillens, Q.; Taavola, H.; Taboada, I.; Tamburro, A.; Tepe, A.; Ter-Antonyan, S.; Tilav, S.; Toale, P. A.; Toscano, S.; Tosi, D.; Turčan, D.; van Eijndhoven, N.; Vandenbroucke, J.; van Overloop, A.; van Santen, J.; Vehring, M.; Voge, M.; Walck, C.; Waldenmaier, T.; Wallraff, M.; Walter, M.; Weaver, Ch.; Wendt, C.; Westerhoff, S.; Whitehorn, N.; Wiebe, K.; Wiebusch, C. H.; Williams, D. R.; Wischnewski, R.; Wissing, H.; Wolf, M.; Wood, T. R.; Woschnagg, K.; Xu, C.; Xu, X. W.; Yodh, G.; Yoshida, S.; Zarzhitsky, P.; Zoll, M.</p> <p>2011-10-01</p> <p>The <span class="hlt">Ice</span>Cube Neutrino Observatory is a 1km3 detector currently taking data at the South Pole. One of the main strategies used to look for astrophysical neutrinos with <span class="hlt">Ice</span>Cube is the search for a diffuse <span class="hlt">flux</span> of high-energy neutrinos from unresolved sources. A hard energy spectrum of neutrinos from isotropically distributed astrophysical sources could manifest itself as a detectable signal that may be differentiated from the atmospheric neutrino background by spectral measurement. This analysis uses data from the <span class="hlt">Ice</span>Cube detector collected in its half completed configuration which operated between April 2008 and May 2009 to search for a diffuse <span class="hlt">flux</span> of astrophysical muon neutrinos. A total of 12 877 upward-going candidate neutrino events have been selected for this analysis. No evidence for a diffuse <span class="hlt">flux</span> of astrophysical muon neutrinos was found in the data set leading to a 90% C.L. upper limit on the normalization of an E-<span class="hlt">2</span> astrophysical νμ <span class="hlt">flux</span> of 8.9×10-9GeVcm-<span class="hlt">2</span>s-1sr-1. The analysis is sensitive in the energy range between 35 TeV and 7 PeV. The 12 877 candidate neutrino events are consistent with atmospheric muon neutrinos measured from 332 GeV to 84 TeV and no evidence for a prompt component to the atmospheric neutrino spectrum is found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996PCE....21..409I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996PCE....21..409I"><span>Eddy-correlation measurements of <span class="hlt">fluxes</span> of <span class="hlt">CO</span> <span class="hlt">2</span> and H <span class="hlt">2</span>O above a spruce stand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ibrom, A.; Schütz, C.; Tworek, T.; Morgenstern, K.; Oltchev, A.; Falk, M.; Constantin, J.; Gravenhorst, G.</p> <p>1996-12-01</p> <p>Atmospheric <span class="hlt">fluxes</span> of <span class="hlt">CO</span> <span class="hlt">2</span> and H <span class="hlt">2</span>O above a mature spruce stand ( Picea abies (L.) Karst.) have been investigated using the eddy- correlation technique. A closed path sensor adapted to the special requirements of long-term studies has been developed and tested. Field measurements have been performed since April 1995. Estimates of fetch showed a very narrow source area dimension under instable stratification (≤ 200 m). Fetch requirements at night are not met in some directions. Energy balance closure was influenced systematically by the wind direction indicating a substantial attenuation of the vertical wind motion by the tower (up to 40 %). Even for optimal flow directions, energy balance closure was about 88%. Intercomparison of the used ultra sonic anemometer (USAT-3) with a GILL - anemometer showed systematically lower values of vertical wind speed fluctuations (13 %). Average <span class="hlt">CO</span> <span class="hlt">2</span>-<span class="hlt">fluxes</span> ranged between -13 at noon to 3 μ mol m-<span class="hlt">2</span>, s-1 at night in summer. In November and December the stand released <span class="hlt">CO</span> <span class="hlt">2</span> on a daily basis. A preliminary estimate of the cumulative net carbon balance over the observed period of 9 months is 4-5 t, Cha-1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3870746','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3870746"><span>Sensitivity to ocean acidification parallels natural p<span class="hlt">CO</span><span class="hlt">2</span> gradients experienced by Arctic copepods under winter sea <span class="hlt">ice</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lewis, Ceri N.; Brown, Kristina A.; Edwards, Laura A.; Cooper, Glenn; Findlay, Helen S.</p> <p>2013-01-01</p> <p>The Arctic Ocean already experiences areas of low pH and high <span class="hlt">CO</span><span class="hlt">2</span>, and it is expected to be most rapidly affected by future ocean acidification (OA). Copepods comprise the dominant Arctic zooplankton; hence, their responses to OA have important implications for Arctic ecosystems, yet there is little data on their current under-<span class="hlt">ice</span> winter ecology on which to base future monitoring or make predictions about climate-induced change. Here, we report results from Arctic under-<span class="hlt">ice</span> investigations of copepod natural distributions associated with late-winter carbonate chemistry environmental data and their response to manipulated p<span class="hlt">CO</span><span class="hlt">2</span> conditions (OA exposures). Our data reveal that species and life stage sensitivities to manipulated OA conditions were correlated with their vertical migration behavior and with their natural exposures to different p<span class="hlt">CO</span><span class="hlt">2</span> ranges. Vertically migrating adult Calanus spp. crossed a p<span class="hlt">CO</span><span class="hlt">2</span> range of >140 μatm daily and showed only minor responses to manipulated high <span class="hlt">CO</span><span class="hlt">2</span>. Oithona similis, which remained in the surface waters and experienced a p<span class="hlt">CO</span><span class="hlt">2</span> range of <75 μatm, showed significantly reduced adult and nauplii survival in high <span class="hlt">CO</span><span class="hlt">2</span> experiments. These results support the relatively untested hypothesis that the natural range of p<span class="hlt">CO</span><span class="hlt">2</span> experienced by an organism determines its sensitivity to future OA and highlight that the globally important copepod species, Oithona spp., may be more sensitive to future high p<span class="hlt">CO</span><span class="hlt">2</span> conditions compared with the more widely studied larger copepods. PMID:24297880</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1611798J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1611798J"><span>Chambers versus Relaxed Eddy Accumulation: an intercomparison study of two methods for short-term measurements of biogenic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jasek, Alina; Zimnoch, Miroslaw; Gorczyca, Zbigniew; Chmura, Lukasz; Necki, Jaroslaw</p> <p>2014-05-01</p> <p>The presented work is a part of comprehensive study aimed at thorough characterization of carbon cycle in the urban environment of Krakow, southern Poland. In the framework of this study two independent methods were employed to quantify biogenic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> in the city: (i) closed chambers, and (ii) Relaxed Eddy Accumulation (REA). The results of a three-day intensive intercomparison campaign performed in July 2013 and utilizing both measurement methods are reported here. The chamber method is a widely used approach for measurements of gas exchange between the soil and the atmosphere. The system implemented in this study consisted of a single chamber operating in a closed-dynamic mode, combined with Vaisala CarboCAP infrared <span class="hlt">CO</span><span class="hlt">2</span> sensor in a mobile setup. An alternative <span class="hlt">flux</span> measurement method, covering larger area is represented by REA, which is a modification of the eddy covariance method. It consists of a 3D anemometer (Gill Windmaster Pro) and the system collecting updraft and downdraft samples to 5-litre Tedlar bags. The <span class="hlt">CO</span><span class="hlt">2</span> mixing ratios in the collected samples are measured by Picarro G2101i analyzer. The setup consists of two sets of bags so that the sampling can be performed continuously with 15-min temporal resolution. A 48-hectares open meadow located close the city center was chosen as a test site for comparison of the two methods of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> measurements outlined above. In the middle of the meadow a 3-metre high tripod was installed with the anemometer and REA inlet system. For a period of 46 hours the system was measuring net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from the surrounding area. A meteorological conditions and intensity of photosynthetically active radiation (PAR) were also recorded. In the same time, <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> from several points around the REA inlet was measured with the chamber system, resulting in 93 values for both respiration and net <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. Chamber results show rather homogenous distribution of the soil <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> (the mean value equal to 40.9 ± <span class="hlt">2.2</span> mmol/m<span class="hlt">2</span>h), with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.U32A..03R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.U32A..03R"><span>The Milankovitch Signature of the <span class="hlt">air</span> Content Along the EPICA DC <span class="hlt">Ice</span> Record: a Tool Towards an Absolute Dating and Implication for <span class="hlt">ice</span> Flow Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raynaud, D.; Duval, P.; Lemieux-Dudon, B.; Lipenkov, V.; Parrenin, F.</p> <p>2006-12-01</p> <p><span class="hlt">Air</span> content of polar <span class="hlt">ice</span>, V, depends primarily on <span class="hlt">air</span> pressure, temperature and pore volume at close-off prevailing at the site of <span class="hlt">ice</span> formation. Here we present the recently measured V record of the EPICA DC (EDC) Antarctic <span class="hlt">ice</span> core covering the last 650,000 years. The first 440,000 years remarkably displays the fundamental Milankovitch orbital frequencies. The 100 kyr period, corresponding to the eccentricity of the Earth's orbit and found in the V record, likely reflects essentially the pressure/elevation signature of V. But most of the variations observed in the V record cannot be explained neither by <span class="hlt">air</span> pressure nor by temperature changes, and then should reflect properties influencing the porosity at close-off other than temperature. A wavelet analysis indicates a dominant period around 41 kyr, the period characteristic of the obliquity variations of the Earth's axis. We propose that the local insolation, via the solar radiation absorbed by the snow, leaves its imprint on the snow structure, then affects the snow-firn transition, and therefore is one of the controlling factors for the porosity at close-off. Such mechanism could account for the observed anti-correlation between local insolation and V. We estimate the variations of the absorbed solar <span class="hlt">flux</span> in the near-surface snow layers on the basis of a simple albedo model (Lemieux-Dudon et al., this session). We compare the dating of the <span class="hlt">ice</span> obtained using the local insolation signal deduced from the V record with a chronology based on <span class="hlt">ice</span> flow modelling. We discuss the glaciological implications of the comparison between the two chronologies, as well as the potential of local insolation markers for approaching an absolute dating of <span class="hlt">ice</span> core. The latest results covering the period 440-650 kyr BP will also be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.B33A0392D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.B33A0392D"><span>Global Monthly <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> Inversion Based on Results of Terrestrial Ecosystem Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deng, F.; Chen, J.; Peters, W.; Krol, M.</p> <p>2008-12-01</p> <p>Most of our understanding of the sources and sinks of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> has come from inverse studies of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration measurements. However, the number of currently available observation stations and our ability to simulate the diurnal planetary boundary layer evolution over continental regions essentially limit the number of regions that can be reliably inverted globally, especially over continental areas. In order to overcome these restrictions, a nested inverse modeling system was developed based on the Bayesian principle for estimating carbon <span class="hlt">fluxes</span> of 30 regions in North America and 20 regions for the rest of the globe. Inverse modeling was conducted in monthly steps using <span class="hlt">CO</span><span class="hlt">2</span> concentration measurements of 5 years (2000 - 2005) with the following two models: (a) An atmospheric transport model (TM5) is used to generate the transport matrix where the diurnal variation n of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> concentration is considered to enhance the use of the afternoon-hour average <span class="hlt">CO</span><span class="hlt">2</span> concentration measurements over the continental sites. (b) A process-based terrestrial ecosystem model (BEPS) is used to produce hourly step carbon <span class="hlt">fluxes</span>, which could minimize the limitation due to our inability to solve the inverse problem in a high resolution, as the background of our inversion. We will present our recent results achieved through a combination of the bottom-up modeling with BEPS and the top-down modeling based on TM5 driven by offline meteorological fields generated by the European Centre for Medium Range Weather Forecast (ECMFW).</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A52C..03K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A52C..03K"><span>Evaluation of Diagnostic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">Flux</span> and Transport Modeling in NU-WRF and GEOS-5</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kawa, S. R.; Collatz, G. J.; Tao, Z.; Wang, J. S.; Ott, L. E.; Liu, Y.; Andrews, A. E.; Sweeney, C.</p> <p>2015-12-01</p> <p>We report on recent diagnostic (constrained by observations) model simulations of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> and transport using a newly developed facility in the NASA Unified-Weather Research and Forecast (NU-WRF) model. The results are compared to <span class="hlt">CO</span><span class="hlt">2</span> data (ground-based, airborne, and GOSAT) and to corresponding simulations from a global model that uses meteorology from the NASA GEOS-5 Modern Era Retrospective analysis for Research and Applications (MERRA). The objective of these intercomparisons is to assess the relative strengths and weaknesses of the respective models in pursuit of an overall carbon process improvement at both regional and global scales. Our guiding hypothesis is that the finer resolution and improved land surface representation in NU-WRF will lead to better comparisons with <span class="hlt">CO</span><span class="hlt">2</span> data than those using global MERRA, which will, in turn, inform process model development in global prognostic models. Initial intercomparison results, however, have generally been mixed: NU-WRF is better at some sites and times but not uniformly. We are examining the model transport processes in detail to diagnose differences in the <span class="hlt">CO</span><span class="hlt">2</span> behavior. These comparisons are done in the context of a long history of simulations from the Parameterized Chemistry and Transport Model, based on GEOS-5 meteorology and Carnegie Ames-Stanford Approach-Global Fire Emissions Database (CASA-GFED) <span class="hlt">fluxes</span>, that capture much of the <span class="hlt">CO</span><span class="hlt">2</span> variation from synoptic to seasonal to global scales. We have run the NU-WRF model using unconstrained, internally generated meteorology within the North American domain, and with meteorological 'nudging' from Global Forecast System and North American Regional Reanalysis (NARR) in an effort to optimize the <span class="hlt">CO</span><span class="hlt">2</span> simulations. Output results constrained by NARR show the best comparisons to data. Discrepancies, of course, may arise either from <span class="hlt">flux</span> or transport errors and compensating errors are possible. Resolving their interplay is also important to using the data in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16668401','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16668401"><span>Relationships between the Efficiencies of Photosystems I and II and Stromal Redox State in <span class="hlt">CO</span>(<span class="hlt">2</span>)-Free <span class="hlt">Air</span> : Evidence for Cyclic Electron Flow in Vivo.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Harbinson, J; Foyer, C H</p> <p>1991-09-01</p> <p>The responses of the efficiencies of photosystems I and II, stromal redox state (as indicated by NADP-malate dehydrogenase activation state), and activation of the Benson-Calvin cycle enzymes ribulose 1,5-bisphosphate carboxylase and fructose 1,6-bisphosphatase to varying irradiance were measured in pea (Pisum sativum L.) leaves operating close to the <span class="hlt">CO</span>(<span class="hlt">2</span>) compensation point. A comparison of the relationships among these parameters obtained from leaves in <span class="hlt">air</span> was made with those obtained when the leaves were maintained in <span class="hlt">air</span> from which the <span class="hlt">CO</span>(<span class="hlt">2</span>) had been removed. P700 was more oxidized at any measured irradiance in <span class="hlt">CO</span>(<span class="hlt">2</span>)-free <span class="hlt">air</span> than in <span class="hlt">air</span>. The relationship between the quantum efficiencies of the photosystems in <span class="hlt">CO</span>(<span class="hlt">2</span>)-free <span class="hlt">air</span> was distinctly curvilinear in contrast to the predominantly linear relationship obtained with leaves in <span class="hlt">air</span>. This nonlinearity may be consistent with the operation of cyclic electron flow around photosystem I because the quantum efficiency of photosystem II was much more restricted than the quantum efficiency of photosystem I. In <span class="hlt">CO</span>(<span class="hlt">2</span>)-free <span class="hlt">air</span>, measured NADP-malate dehydrogenase activities varied considerably at low irradiances. However, at high irradiance the activity of the enzyme was low, implying that the stroma was oxidized. In contrast, fructose-1,6-bisphosphatase activities tended to increase with increasing electron <span class="hlt">flux</span> through the photosystems. Ribulose-1,5-bisphosphate carboxylase activity remained relatively constant with respect to irradiance in <span class="hlt">CO</span>(<span class="hlt">2</span>)-free <span class="hlt">air</span>, with an activation state 50% of maximum. We conclude that, at the <span class="hlt">CO</span>(<span class="hlt">2</span>) compensation point and high irradiance, low redox states are favored and that cyclic electron flow may be substantial. These two features may be the requirements necessary to trigger and maintain the dissipative processes in the thylakoid membrane.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C33B1192G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C33B1192G"><span>Direct observations of atmosphere - sea <span class="hlt">ice</span> - ocean interactions during Arctic winter and spring storms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Graham, R. M.; Itkin, P.; Granskog, M. A.; Assmy, P.; Cohen, L.; Duarte, P.; Doble, M. J.; Fransson, A.; Fer, I.; Fernandez Mendez, M.; Frey, M. M.; Gerland, S.; Haapala, J. J.; Hudson, S. R.; Liston, G. E.; Merkouriadi, I.; Meyer, A.; Muilwijk, M.; Peterson, A.; Provost, C.; Randelhoff, A.; Rösel, A.; Spreen, G.; Steen, H.; Smedsrud, L. H.; Sundfjord, A.</p> <p>2017-12-01</p> <p>To study the thinner and younger sea <span class="hlt">ice</span> that now dominates the Arctic the Norwegian Young Sea <span class="hlt">ICE</span> expedition (N-<span class="hlt">ICE</span>2015) was launched in the <span class="hlt">ice</span>-covered region north of Svalbard, from January to June 2015. During this time, eight local and remote storms affected the region and rare direct observations of the atmosphere, snow, <span class="hlt">ice</span> and ocean were conducted. Six of these winter storms passed directly over the expedition and resulted in <span class="hlt">air</span> temperatures rising from below -30oC to near 0oC, followed by abrupt cooling. Substantial snowfall prior to the campaign had already formed a snow pack of approximately 50 cm, to which the February storms contributed an additional 6 cm. The deep snow layer effectively isolated the <span class="hlt">ice</span> cover and prevented bottom <span class="hlt">ice</span> growth resulting in low brine <span class="hlt">fluxes</span>. Peak wind speeds during winter storms exceeded 20 m/s, causing strong snow re-distribution, release of sea salt aerosol and sea <span class="hlt">ice</span> deformation. The heavy snow load caused widespread negative freeboard; during sea <span class="hlt">ice</span> deformation events, level <span class="hlt">ice</span> floes were flooded by sea water, and at least 6-10 cm snow-<span class="hlt">ice</span> layer was formed. Elevated deformation rates during the most powerful winter storms damaged the <span class="hlt">ice</span> cover permanently such that the response to wind forcing increased by 60 %. As a result of a remote storm in April deformation processes opened about 4 % of the total area into leads with open water, while a similar amount of <span class="hlt">ice</span> was deformed into pressure ridges. The strong winds also enhanced ocean mixing and increased ocean heat <span class="hlt">fluxes</span> three-fold in the pycnocline from 4 to 12 W/m<span class="hlt">2</span>. Ocean heat <span class="hlt">fluxes</span> were extremely large (over 300 W/m<span class="hlt">2</span>) during storms in regions where the warm Atlantic inflow is located close to surface over shallow topography. This resulted in very large (5-25 cm/day) bottom <span class="hlt">ice</span> melt and in cases flooding due to heavy snow load. Storm events increased the carbon dioxide exchange between the atmosphere and ocean but also affected the p<span class="hlt">CO</span><span class="hlt">2</span> in surface waters</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=314066','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=314066"><span>Seasonal variation in measured H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> of irrigated rice in the Mid-South</span></a></p> <p><a target="_blank" href="https://www.ars.usda.gov/research/publications/find-a-publication/">USDA-ARS?s Scientific Manuscript database</a></p> <p></p> <p></p> <p>Rice production in the Lower Mississippi River Basin constitutes over half of US rice production, but little research has been done on water and carbon <span class="hlt">flux</span> in this region at the field scale. Eddy covariance measurements of water and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> allow for an integrated field measurement of the interac...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B41B0409L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B41B0409L"><span>A gap-filling model for eddy covariance <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>: Estimating carbon assimilated by a subtropical evergreen broad-leaved forest at the Lien-Hua-Chih <span class="hlt">flux</span> observation site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lan, C. Y.; Li, M. H.; Chen, Y. Y.</p> <p>2016-12-01</p> <p>Appropriate estimations of gaps appeared in eddy covariance (EC) <span class="hlt">flux</span> observations are critical to the reliability of long-term EC applications. In this study we present a semi-parametric multivariate gap-filling model for tower-based measurement of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. The raw EC data passing QC/QA was separated into two groups, clear sky, having net radiation greater than 50 W/m<span class="hlt">2</span>, and nighttime/cloudy. For the clear sky conditions, the principle component analysis (PCA) was used to resolve the multicollinearity relationships among various environmental variables, including net radiation, wind speed, vapor pressure deficit, soil moisture deficit, leaf area index, and soil temperature, in association with <span class="hlt">CO</span><span class="hlt">2</span> assimilated by forest. After the principal domains were determined by the PCA, the relationships between <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and selected PCs (key factors) were built up by nonlinear interpolations to estimate the gap-filled <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>. In view of limited photosynthesis at nighttime/cloudy conditions, respiration rate of the forest ecosystem was estimated by the Lloyd-Tylor equation. Artificial gaps were randomly selected to exam the applicability of our PCA approach. Based on tower-based measurement of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> at the Lien-Hua-Chih site, a total of 5.8 ton-C/ha/yr was assimilated in 2012.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008Icar..197..152H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008Icar..197..152H"><span>Release of N <span class="hlt">2</span>, CH 4, <span class="hlt">CO</span> <span class="hlt">2</span>, and H <span class="hlt">2</span>O from surface <span class="hlt">ices</span> on Enceladus</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hodyss, Robert; Goguen, Jay D.; Johnson, Paul V.; Campbell, Colin; Kanik, Isik</p> <p>2008-09-01</p> <p>We vapor deposit at 20 K a mixture of gases with the specific Enceladus plume composition measured in situ by the Cassini INMS [Waite, J.H., Combi, M.R., Ip, W.H., Cravens, T.E., McNutt, R.L., Kasprzak, W., Yelle, R., Luhmann, J., Niemann, H., Gell, D., Magee, B., Fletcher, G., Lunine, J., Tseng, W.L., 2006. Science 311, 1419-1422] to form a mixed molecular <span class="hlt">ice</span>. As the sample is slowly warmed, we monitor the escaping gas quantity and composition with a mass spectrometer. Pioneering studies [Schmitt, B., Klinger, J., 1987. Different trapping mechanisms of gases by water <span class="hlt">ice</span> and their relevance for comet nuclei. In: Rolfe, E.J., Battrick, B. (Eds.), Diversity and Similarity of Comets. SP-278. ESA, Noordwijk, The Netherlands, pp. 613-619; Bar-Nun, A., Kleinfeld, I., Kochavi, E., 1988. Phys. Rev. B 38, 7749-7754; Bar-Nun, A., Kleinfeld, I., 1989. Icarus 80, 243-253] have shown that significant quantities of volatile gases can be trapped in a water <span class="hlt">ice</span> matrix well above the temperature at which the pure volatile <span class="hlt">ice</span> would sublime. For our Enceladus <span class="hlt">ice</span> mixture, a composition of escaping gases similar to that detected by Cassini in the Enceladus plume can be generated by the sublimation of the H <span class="hlt">2</span>O:<span class="hlt">CO</span> <span class="hlt">2</span>:CH 4:N <span class="hlt">2</span> mixture at temperatures between 135 and 155 K, comparable to the high temperatures inferred from the CIRS measurements [Spencer, J.R., Pearl, J.C., Segura, M., Flasar, F.M., Mamoutkine, A., Romani, P., Buratti, B.J., Hendrix, A.R., Spilker, L.J., Lopes, R.M.C., 2006. Science 311, 1401-1405] of the Enceladus "tiger stripes." This suggests that the gas escape phenomena that we measure in our experiments are an important process contributing to the gases emitted from Enceladus. A similar experiment for <span class="hlt">ice</span> deposited at 70 K shows that both the processes of volatile trapping and release are temperature dependent over the temperature range relevant to Enceladus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.6028L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.6028L"><span>Using New Remotely-sensed Biomass To Estimate <span class="hlt">Co</span><span class="hlt">2</span> <span class="hlt">Fluxes</span> Over Siberia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lafont, S.; Kergoat, L.; Dedieu, G.; Le Toan, T.</p> <p></p> <p>Two european programs recently focused on Siberia. The first one, Eurosiberian Car- bonflux was a faisability study for an observation system of the regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span>. The second one, SIBERIA was a big effort to develop and validate a biomass map on Siberia using radar data from satelltes (J-ERS, ERS). Here, we extend the simula- tion of NPP performed for the first program by using the biomass data of the second program. The TURC model, used here, is a global NPP model, based on light use efficiency, where photosynthetic assimilation is driven by satellite vegetation index, and au- totrophic respiration is driven by biomass. In this study, we will present a n´ zoom z on siberian region. The TURC model was run with a fine resolution (few kilometers) and a daily time step. We will discuss the impact of a new biomass dataset description on Net Primary Pro- ductivity (NPP) and <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> estimation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6207452-monitoring-seasonal-state-mapping-species-alaskan-taiga-using-imaging-radar-input-co-sub-flux-models','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6207452-monitoring-seasonal-state-mapping-species-alaskan-taiga-using-imaging-radar-input-co-sub-flux-models"><span>Monitoring seasonal state and mapping species in Alaskan taiga using imaging radar as input to <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> models</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Way, J.B.; Rignot, E.; McDonald, K.</p> <p>1993-06-01</p> <p>Changes in the seasonal <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> of the boreal forests may result from increased atmospheric <span class="hlt">CO</span>[sub <span class="hlt">2</span>] concentrations and associated atmospheric warming. To monitor this potential change, a combination of remote sensing information and ecophysiological models are required. In this paper we address the use of synthetic aperture radar (SAR) data to provide some of the input to the ecophysiological models: forest type, freeze/thaw state which limits the growing season for conifers, and leaf on/off state which limits the growing season for deciduous species. AIRSAR data collected in March 1988 during an early thaw event and May 1991 duringmore » spring breakup are used to generate species maps and to determine the sensitivity of SAR to canopy freeze/thaw transitions. These data are also used to validate a microwave scattering model which is then used to determine the sensitivity of SAR to leaf on/off and soil freeze/thaw transitions. Finally, a <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> algorithm which utilizes SAR data and an ecophysiological model to estimate <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> is presented. <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> maps are generated from which areal estimates of <span class="hlt">CO</span>[sub <span class="hlt">2</span>] <span class="hlt">flux</span> are derived. This work was carried out at the Jet Propulsion Laboratory under contract to the NASA.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.489..123S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.489..123S"><span>Infiltration-driven metamorphism, New England, USA: Regional <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and implications for Devonian climate and extinctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stewart, E. M.; Ague, Jay J.</p> <p>2018-05-01</p> <p>We undertake thermodynamic pseudosection modeling of metacarbonate rocks in the Wepawaug Schist, Connecticut, USA, and examine the implications for <span class="hlt">CO</span><span class="hlt">2</span> outgassing from collisional orogenic belts. Two broad types of pseudosections are calculated: (1) a fully closed-system model with no fluid infiltration and (<span class="hlt">2</span>) a fluid-buffered model including an H<span class="hlt">2</span>O-<span class="hlt">CO</span><span class="hlt">2</span> fluid of a fixed composition. This fluid-buffered model is used to approximate a system open to infiltration by a water-bearing fluid. In all cases the fully closed-system model fails to reproduce the observed major mineral zones, mineral compositions, reaction temperatures, and fluid compositions. The fluid-infiltrated models, on the other hand, successfully reproduce these observations when the XCO<span class="hlt">2</span> of the fluid is in the range ∼0.05 to ∼0.15. Fluid-infiltrated models predict significant progressive <span class="hlt">CO</span><span class="hlt">2</span> loss, peaking at ∼50% decarbonation at amphibolite facies. The closed-system models dramatically underestimate the degree of decarbonation, predicting only ∼15% <span class="hlt">CO</span><span class="hlt">2</span> loss at peak conditions, and, remarkably, <1% <span class="hlt">CO</span><span class="hlt">2</span> loss below ∼600 °C. We propagate the results of fluid-infiltrated pseudosections to determine an areal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span> for the Wepawaug Schist. This yields ∼1012 mol <span class="hlt">CO</span><span class="hlt">2</span> km-<span class="hlt">2</span> Myr-1, consistent with multiple independent estimates of the metamorphic <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">flux</span>, and comparable in magnitude to <span class="hlt">fluxes</span> from mid-ocean ridges and volcanic arcs. Extrapolating to the area of the Acadian orogenic belt, we suggest that metamorphic <span class="hlt">CO</span><span class="hlt">2</span> degassing is a plausible driver of global warming, sea level rise, and, perhaps, extinction in the mid- to late-Devonian.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100032897&hterms=nz&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnz','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100032897&hterms=nz&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnz"><span>Validation of <span class="hlt">AIRS</span> Retrievals of <span class="hlt">CO</span><span class="hlt">2</span> via Comparison to In Situ Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, Edward T.; Chahine, Moustafa T.; Chen, Luke L.; Jiang, Xun; Pagano, Thomas S.; Yung, Yuk L.</p> <p>2008-01-01</p> <p>Topics include <span class="hlt">AIRS</span> on Aqua, 2002-present with discussion about continued operation to 2011 and beyond and background, including spectrum, weighting functions, and initialization; comparison with aircraft and FTIR measurements in Masueda (CONTRAIL) JAL flask measurements, Park Falls, WI FTIR, Bremen, GDF, and Spitsbergen, Norway; <span class="hlt">AIRS</span> retrievals over addition FTIR sites in Darwin, AU and Lauder, NZ; and mid-tropospheric carbon dioxide weather and contribution from major surface sources. Slide titles include typical <span class="hlt">AIRS</span> infrared spectrum, <span class="hlt">AIRS</span> sensitivity for retrieving <span class="hlt">CO</span><span class="hlt">2</span> profiles, independence of <span class="hlt">CO</span><span class="hlt">2</span> solution with respect to the initial guess, available in situ measurements for validation and comparison, comparison of collocated V1.5x <span class="hlt">AIRS</span> <span class="hlt">CO</span><span class="hlt">2</span> (N_coll greater than or equal to 9) with INTEX-NA and SPURT;</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015BGD....12.4405O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015BGD....12.4405O"><span>Response of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">fluxes</span> of a mountainous tropical rain forest in equatorial Indonesia to El Niño events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olchev, A.; Ibrom, A.; Panferov, O.; Gushchina, D.; Propastin, P.; Kreilein, H.; June, T.; Rauf, A.; Gravenhorst, G.; Knohl, A.</p> <p>2015-03-01</p> <p>The possible impact of El Niño-Southern Oscillation (ENSO) events on the main components of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O <span class="hlt">fluxes</span> in a pristine mountainous tropical rainforest growing in Central Sulawesi in Indonesia is described. The <span class="hlt">fluxes</span> were continuously measured using the eddy covariance method for the period from January 2004 to June 2008. During this period, two episodes of El Niño and one episode of La Niña were observed. All these ENSO episodes had moderate intensity and were of Central Pacific type. The temporal variability analysis of the main meteorological parameters and components of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O exchange showed a very high sensitivity of Evapotranspiration (ET) and Gross Primary Production (GPP) of the tropical rain forest to meteorological variations caused by both El Niño and La Niña episodes. Incoming solar radiation is the main governing factor that is responsible for ET and GPP variability. Ecosystem Respiration (RE) dynamics depend mainly on the <span class="hlt">air</span> temperature changes and are almost insensitive to ENSO. Changes of precipitation due to moderate ENSO events did not cause any notable effect on ET and GPP, mainly because of sufficient soil moisture conditions even in periods of anomalous reduction of precipitation in the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.5740E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.5740E"><span>δ13Catm and [<span class="hlt">CO</span><span class="hlt">2</span>] measurements in Antarctic <span class="hlt">ice</span> cores, 160 kyrBP - present</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eggleston, Sarah; Schmitt, Jochen; Schneider, Robert; Joos, Fortunat; Fischer, Hubertus</p> <p>2014-05-01</p> <p>Measurements from Antarctic <span class="hlt">ice</span> cores allow us to reconstruct atmospheric concentrations of climatically important gases including <span class="hlt">CO</span><span class="hlt">2</span> over the past 800 kyr. Such measurements show that [<span class="hlt">CO</span><span class="hlt">2</span>] has varied in parallel with Antarctic temperatures on glacial-interglacial timescales. Knowledge of the variations of the stable carbon isotope of <span class="hlt">CO</span><span class="hlt">2</span>, δ13Catm, can help us better understand the processes involved in these fluctuations. Here, we present a first complete δ13Catmrecord extending from 160 kyrBP to the present accompanied by δ15N<span class="hlt">2</span> measurements during Marine Isotope Stage 3 (MIS 3, 57 - 29 kyrBP). The present record, measured primarily on <span class="hlt">ice</span> from the EPICA Dome C and Talos Dome <span class="hlt">ice</span> cores, has an average resolution of 500 yr, focused mainly on the Last Glacial Maximum and termination (180 yr; Schmitt et al., 2012), MIS 3 (660 yr), and Termination II through MIS 5.4 (590 yr; Schneider et al., 2013). Throughout the record, δ13Catm varies between approximately -6.8 and -6.4‰Following a period of relatively constant δ13Catm at the end of MIS 6 (around -6.8), the boundaries of MIS 5 correspond roughly with the beginning and end of a gradual enrichment in this isotope. In comparison, the more recent record depicts three more abrupt excursions to lighter values around 63 - 59, 46, and 17 kyrBP, in each case followed by a slower return (0.4o over the course of 5 - 15 kyr) to more enriched isotopic values. These coincide with Heinrich events 6, 5, and 1, respectively. No direct correlation is observed between the concentration and carbon isotope of <span class="hlt">CO</span><span class="hlt">2</span> over the last 160 kyr. The data indicate rather that numerous processes, such as uptake and release of atmospheric <span class="hlt">CO</span><span class="hlt">2</span> by the ocean and land biosphere, perhaps influenced by regions of growing permafrost during MIS 3 and 4, acting on a variety of timescales must be considered in explaining the evolution of δ13Catm on glacial-interglacial timescales. References: Schmitt, J. et al. Science 336, 711-714 (2012) Schneider</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/24496','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/24496"><span>Interaction of <span class="hlt">ice</span> storms and management practices on current carbon sequestration in forests with potential mitigation under future <span class="hlt">CO</span><span class="hlt">2</span> atmosphere</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Heather R. McCarthy; Ram Oren; Hyun-Seok Kim; Kurt H. Johnsen; Chris Maier; Seth G. Pritchard; Michael A. Davis</p> <p>2006-01-01</p> <p><span class="hlt">Ice</span> storms are disturbance events with potential impacts on carbon sequestration. Common forest management practices, such as fertilization and thinning, can change wood and stand properties and thus may change vulnerability to <span class="hlt">ice</span> storm damage. At the same time, increasing atmospheric <span class="hlt">CO</span><span class="hlt">2</span> levels may also influence <span class="hlt">ice</span> storm vulnerability. Here...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ClDy...41.2267M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ClDy...41.2267M"><span>Relative impacts of insolation changes, meltwater <span class="hlt">fluxes</span> and <span class="hlt">ice</span> sheets on African and Asian monsoons during the Holocene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marzin, Charline; Braconnot, Pascale; Kageyama, Masa</p> <p>2013-11-01</p> <p>In order to better understand the evolution of the Afro-Asian monsoon in the early Holocene, we investigate the impact on boreal summer monsoon characteristics of (1) a freshwater <span class="hlt">flux</span> in the North Atlantic from the surrounding melting <span class="hlt">ice</span> sheets and (<span class="hlt">2</span>) a remnant <span class="hlt">ice</span> sheet over North America and Europe. Sensitivity experiments run with the IPSL_CM4 model show that both the meltwater <span class="hlt">flux</span> and the remnant <span class="hlt">ice</span> sheets induce a cooling of similar amplitude of the North Atlantic leading to a southward shift of the Inter-Tropical Convergence Zone over the tropical Atlantic and to a reduction of the African monsoon. The two perturbations have different impacts in the Asian sector. The meltwater <span class="hlt">flux</span> results in a weakening of the Indian monsoon and no change in the East Asian monsoon, whereas the remnant <span class="hlt">ice</span> sheets induce a strengthening of the Indian monsoon and a strong weakening of the East Asian monsoon. Despite the similar coolings in the Atlantic Ocean, the ocean heat transport is reduced only in the meltwater <span class="hlt">flux</span> experiment, which induces slight differences between the two experiments in the role of the surface latent heat <span class="hlt">flux</span> in the tropical energetics. In the meltwater experiment, the southward shift of the subtropical jet acts to cool the upper atmosphere over the Tibetan Plateau and hence to weaken the Indian monsoon. In the <span class="hlt">ice</span> sheet experiment this effect is overwhelmed by the changes in extratropical stationary waves induced by the <span class="hlt">ice</span> sheets, which are associated with a larger cooling over the Eurasian continent than in the meltwater experiment. However these sensitivity experiments suggest that insolation is the dominant factor explaining the relative changes of the African, Indian and East Asian monsoons from the early to the mid-Holocene.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27126229','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27126229"><span>Temporal and spatial patterns of internal and external stem <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in a sub-Mediterranean oak.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Salomón, Roberto L; Valbuena-Carabaña, María; Gil, Luis; McGuire, Mary Anne; Teskey, Robert O; Aubrey, Doug P; González-Doncel, Inés; Rodríguez-Calcerrada, Jesús</p> <p>2016-11-01</p> <p>To accurately estimate stem respiration (R S ), measurements of both carbon dioxide (<span class="hlt">CO</span> <span class="hlt">2</span> ) efflux to the atmosphere (E A ) and internal <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">flux</span> through xylem (F T ) are needed because xylem sap transports respired <span class="hlt">CO</span> <span class="hlt">2</span> upward. However, reports of seasonal dynamics of F T and E A are scarce and no studies exist in Mediterranean species under drought stress conditions. Internal and external <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> at three stem heights, together with radial stem growth, temperature, sap flow and shoot water potential, were measured in Quercus pyrenaica Willd. in four measurement campaigns during one growing season. Substantial daytime depressions in temperature-normalized E A were observed throughout the experiment, including prior to budburst, indicating that diel hysteresis between stem temperature and E A cannot be uniquely ascribed to diversion of <span class="hlt">CO</span> <span class="hlt">2</span> in the transpiration stream. Low internal [<span class="hlt">CO</span> <span class="hlt">2</span> ] (<0.5%) resulted in low contributions of F T to R S throughout the growing season, and R S was mainly explained by E A (>90%). Internal [<span class="hlt">CO</span> <span class="hlt">2</span> ] was found to vary vertically along the stems. Seasonality in resistance to radial <span class="hlt">CO</span> <span class="hlt">2</span> diffusion was related to shoot water potential. The low internal [<span class="hlt">CO</span> <span class="hlt">2</span> ] and F T observed in our study may result from the downregulation of xylem respiration in response to a legacy of coppicing as well as high radial diffusion of <span class="hlt">CO</span> <span class="hlt">2</span> through cambium, phloem and bark tissues, which was related to low water content of stems. Long-term studies analyzing temporal and spatial variation in internal and external <span class="hlt">CO</span> <span class="hlt">2</span> <span class="hlt">fluxes</span> and their interactions are needed to mechanistically understand and model respiration of woody tissues. © The Author 2016. Published by Oxford University Press. All rights reserved. For Permissions, please email: journals.permissions@oup.com.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A..80B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A..80B"><span>Efficiency of radial transport of <span class="hlt">ices</span> in protoplanetary disks probed with infrared observations: the case of <span class="hlt">CO</span><span class="hlt">2</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bosman, Arthur D.; Tielens, Alexander G. G. M.; van Dishoeck, Ewine F.</p> <p>2018-04-01</p> <p>Context. Radial transport of icy solid material from the cold outer disk to the warm inner disk is thought to be important for planet formation. However, the efficiency at which this happens is currently unconstrained. Efficient radial transport of icy dust grains could significantly alter the composition of the gas in the inner disk, enhancing the gas-phase abundances of the major <span class="hlt">ice</span> constituents such as H<span class="hlt">2</span>O and <span class="hlt">CO</span><span class="hlt">2</span>. Aim. Our aim is to model the gaseous <span class="hlt">CO</span><span class="hlt">2</span> abundance in the inner disk and use this to probe the efficiency of icy dust transport in a viscous disk. From the model predictions, infrared <span class="hlt">CO</span><span class="hlt">2</span> spectra are simulated and features that could be tracers of icy <span class="hlt">CO</span><span class="hlt">2</span>, and thus dust, radial transport efficiency are investigated. Methods: We have developed a 1D viscous disk model that includes gas accretion and gas diffusion as well as a description for grain growth and grain transport. Sublimation and freeze-out of <span class="hlt">CO</span><span class="hlt">2</span> and H<span class="hlt">2</span>O has been included as well as a parametrisation of the <span class="hlt">CO</span><span class="hlt">2</span> chemistry. The thermo-chemical code DALI was used to model the mid-infrared spectrum of <span class="hlt">CO</span><span class="hlt">2</span>, as can be observed with JWST-MIRI. Results: <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> sublimating at the iceline increases the gaseous <span class="hlt">CO</span><span class="hlt">2</span> abundance to levels equal to the <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">ice</span> abundance of 10-5, which is three orders of magnitude more than the gaseous <span class="hlt">CO</span><span class="hlt">2</span> abundances of 10-8 observed by Spitzer. Grain growth and radial drift increase the rate at which <span class="hlt">CO</span><span class="hlt">2</span> is transported over the iceline and thus the gaseous <span class="hlt">CO</span><span class="hlt">2</span> abundance, further exacerbating the problem. In the case without radial drift, a <span class="hlt">CO</span><span class="hlt">2</span> destruction rate of at least 10-11 s-1 or a destruction timescale of at most 1000 yr is needed to reconcile model prediction with observations. This rate is at least two orders of magnitude higher than the fastest destruction rate included in chemical databases. A range of potential physical mechanisms to explain the low observed <span class="hlt">CO</span><span class="hlt">2</span> abundances are discussed. Conclusions: We conclude that transport processes in disks can have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.B34A0337O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.B34A0337O"><span>Are changes in the phytoplankton community structure altering the <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span> in regions of the North Atlantic?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ostle, C.; Landschutzer, P.; Johnson, M.; Schuster, U.; Watson, A. J.; Edwards, M.; Robinson, C.</p> <p>2016-02-01</p> <p>The North Atlantic Ocean is a globally important sink of carbon dioxide (<span class="hlt">CO</span><span class="hlt">2</span>). However, the strength of the sink varies temporally and regionally. This study uses a neural network method to map the surface ocean p<span class="hlt">CO</span><span class="hlt">2</span> (partial pressure of <span class="hlt">CO</span><span class="hlt">2</span>) and <span class="hlt">flux</span> of <span class="hlt">CO</span><span class="hlt">2</span>from the atmosphere to the ocean alongside measurements of plankton abundance collected from the Continuous Plankton Recorder (CPR) survey to determine the relationship between regional changes in phytoplankton community structure and regional differences in carbon <span class="hlt">flux</span>. Despite increasing sea surface temperatures, the Grand Banks of Newfoundland show a decrease in sea surface p<span class="hlt">CO</span><span class="hlt">2</span> of -<span class="hlt">2</span> µatm yr-1 from 1993 to 2011. The carbon <span class="hlt">flux</span> in the North Sea is variable over the same period. This is in contrast to most of the open ocean within the North Atlantic, where increases in sea surface p<span class="hlt">CO</span><span class="hlt">2</span> follow the trend of increasing <span class="hlt">CO</span><span class="hlt">2</span> in the atmosphere, i.e. the <span class="hlt">flux</span> or sink remains constant. The increasing <span class="hlt">CO</span><span class="hlt">2</span> sink in the Grand Banks of Newfoundland and the variable sink in the North Sea correlate with changes in phytoplankton community composition. This study investigates the biogeochemical and oceanographic mechanisms potentially linking increasing sea surface temperature, changes in phytoplankton community structure and the changing carbon sink in these two important regions of the Atlantic Ocean. The use of volunteer ships to concurrently collect these datasets demonstrates the potential to investigate relationships between plankton community structure and carbon <span class="hlt">flux</span> in a cost-effective way. These results not only have implications for plankton-dynamic biogeochemical models, but also likely influence carbon export, as different phytoplankton communities have different carbon export efficiencies. Extending and maintaining such datasets is critical to improving our understanding of and monitoring carbon cycling in the surface ocean and improving climate model accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29714795','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29714795"><span>Humidity-swing mechanism for <span class="hlt">CO</span><span class="hlt">2</span> capture from ambient <span class="hlt">air</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Hao; Singh, Manmilan; Schaefer, Jacob</p> <p>2018-05-10</p> <p>A humidity-swing polymeric sorbent captures <span class="hlt">CO</span><span class="hlt">2</span> from ambient <span class="hlt">air</span> at room temperature simply by changing the humidity level. To date there has been no direct experimental evidence to characterize the chemical mechanism for this process. In this report we describe the use of solid-state NMR to study the humidity-swing <span class="hlt">CO</span><span class="hlt">2</span> absorption/desorption cycle directly. We find that at low humidity levels <span class="hlt">CO</span><span class="hlt">2</span> is absorbed as HCO3-. At high humidity levels, HCO3- is replaced by hydrated OH- and the absorbed <span class="hlt">CO</span><span class="hlt">2</span> is released.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EL....11343002T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EL....11343002T"><span>Effects of van der Waals forces and salt ions on the growth of water films on <span class="hlt">ice</span> and the detachment of <span class="hlt">CO</span><span class="hlt">2</span> bubbles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thiyam, P.; Lima, E. R. A.; Malyi, O. I.; Parsons, D. F.; Buhmann, S. Y.; Persson, C.; Boström, M.</p> <p>2016-02-01</p> <p>We study the effect of salts on the thickness of wetting films on melting <span class="hlt">ice</span> and interactions acting on <span class="hlt">CO</span><span class="hlt">2</span> bubble near <span class="hlt">ice</span>-water and vapor-water interfaces. Governing mechanisms are the Lifshitz and the double-layer interactions in the respective three-layer geometries. We demonstrate that the latter depend on the Casimir-Polder interaction of the salt ions dissolved in water with the respective <span class="hlt">ice</span>, vapor and <span class="hlt">CO</span><span class="hlt">2</span> interfaces, as calculated using different models for their effective polarizability in water. Significant variation in the predicted thickness of the equilibrium water film is observed for different salt ions and when using different models for the ions' polarizabilities. We find that <span class="hlt">CO</span><span class="hlt">2</span> bubbles are attracted towards the <span class="hlt">ice</span>-water interface and repelled from the vapor-water interface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1715084M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1715084M"><span>Agricultural crops and soil treatment impacts on the daily and seasonal dynamics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> in the field agroecosystems at the Central region of Russia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazirov, Ilya; Vasenev, Ivan; Meshalkina, Joulia; Yaroslavtsev, Alexis; Berezovskiy, Egor; Djancharov, Turmusbek</p> <p>2015-04-01</p> <p>The problem of greenhouse gases' concentrations increasing becomes more and more important due to global changes issues. The main component of greenhouse gases is carbon dioxide. The researches focused on its <span class="hlt">fluxes</span> in natural and anthropogenic modified landscapes can help in this problem solution. Our research has been done with support of the RF Government grants # 11.G34.31.0079 and # 14.120.14.4266 and of FP7 Grant # 603542 LUC4C in the representative for Central Region of Russia field agroecosystems at the Precision Farming Experimental Field of Russian Timiryazev State Agrarian University with cultivated sod podzoluvisols, barley and oats - vetch grass mix (Moscow station of the Rus<span class="hlt">Flux</span>Net). The daily and seasonal dynamics of the carbon dioxide have been studied at the ecosystem level by the Eddy covariance method (<span class="hlt">2</span> stations) and at the soil level by the exposition chamber method (40 chambers) with mobile infra red gas analyzer (Li-Cor 820). The primary Eddy covariance monitoring data on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> and water vapor have been processed by EddyPro software developed by LI-COR Biosciences. According to the two-year monitoring data the daily <span class="hlt">CO</span><span class="hlt">2</span> sink during the vegetation season is usually approximately two times higher than its emission at night. Seasonal <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> comparative stabilization has been fixed in case the plants height around 10-12 cm and it usually persist until the wax ripeness phase. There is strong dependence between the soil <span class="hlt">CO</span><span class="hlt">2</span> emission and the <span class="hlt">air</span> temperature with the correlation coefficient 0.86 in average (due to strong input of the soil thin top functional subhorizon), but it drops essentially at the end of the season - till 0.38. The soil moisture impact on <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> dynamics was less, with negative correlation at the end of the season. High daily dynamics of <span class="hlt">CO</span><span class="hlt">2</span> <span class="hlt">fluxes</span> determines the protocol requirements for seasonal soil monitoring investigation with less limitation at the end of the season. The accumulated monitoring data will be</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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