Sample records for air-surface exchange model

  1. New directions: Time for a new approach to modeling surface-atmosphere exchanges in air quality models?

    NASA Astrophysics Data System (ADS)

    Saylor, Rick D.; Hicks, Bruce B.

    2016-03-01

    Just as the exchange of heat, moisture and momentum between the Earth's surface and the atmosphere are critical components of meteorological and climate models, the surface-atmosphere exchange of many trace gases and aerosol particles is a vitally important process in air quality (AQ) models. Current state-of-the-art AQ models treat the emission and deposition of most gases and particles as separate model parameterizations, even though evidence has accumulated over time that the emission and deposition processes of many constituents are often two sides of the same coin, with the upward (emission) or downward (deposition) flux over a landscape depending on a range of environmental, seasonal and biological variables. In this note we argue that the time has come to integrate the treatment of these processes in AQ models to provide biological, physical and chemical consistency and improved predictions of trace gases and particles.

  2. Processes of Ammonia Air-Surface Exchange in a Fertilized Zea Mays Canopy

    EPA Science Inventory

    Recent incorporation of coupled soil biogeochemical and bi-directional NH3 air-surface exchange algorithms into regional air quality models holds promise for further reducing uncertainty in estimates of NH3 emissions from fertilized soils. While this advancement represents a sig...

  3. Investigation of ammonia air-surface exchange processes in a ...

    EPA Pesticide Factsheets

    Recent assessments of atmospheric deposition in North America note the increasing importance of reduced (NHx = NH3 + NH4+) forms of nitrogen (N) relative to oxidized forms. This shift in in the composition of inorganic nitrogen deposition has both ecological and policy implications. Deposition budgets developed from inferential models applied at the landscape scale, as well as regional and global chemical transport models, indicate that NH3 dry deposition contributes a significant portion of inorganic N deposition in many areas. However, the bidirectional NH3 flux algorithms employed in these models have not been extensively evaluated for North American conditions (e.g, atmospheric chemistry, meteorology, biogeochemistry). Further understanding of the processes controlling NH3 air-surface exchange in natural systems is critically needed. Based on preliminary results from the Southern Appalachian Nitrogen Deposition Study (SANDS), this presentation examines processes of NH3 air-surface exchange in a deciduous montane forest at the Coweeta Hydrologic Laboratory in western North Carolina. A combination of measurements and modeling are used to investigate net fluxes of NH3 above the forest and sources and sinks of NH3 within the canopy and forest floor. Measurements of biogeochemical NH4+ pools are used to characterize emission potential and NH3 compensation points of canopy foliage (i.e., green vegetation), leaf litter, and soil and their relation to NH3 fluxes

  4. A review of air exchange rate models for air pollution exposure assessments.

    PubMed

    Breen, Michael S; Schultz, Bradley D; Sohn, Michael D; Long, Thomas; Langstaff, John; Williams, Ronald; Isaacs, Kristin; Meng, Qing Yu; Stallings, Casson; Smith, Luther

    2014-11-01

    A critical aspect of air pollution exposure assessments is estimation of the air exchange rate (AER) for various buildings where people spend their time. The AER, which is the rate of exchange of indoor air with outdoor air, is an important determinant for entry of outdoor air pollutants and for removal of indoor-emitted air pollutants. This paper presents an overview and critical analysis of the scientific literature on empirical and physically based AER models for residential and commercial buildings; the models highlighted here are feasible for exposure assessments as extensive inputs are not required. Models are included for the three types of airflows that can occur across building envelopes: leakage, natural ventilation, and mechanical ventilation. Guidance is provided to select the preferable AER model based on available data, desired temporal resolution, types of airflows, and types of buildings included in the exposure assessment. For exposure assessments with some limited building leakage or AER measurements, strategies are described to reduce AER model uncertainty. This review will facilitate the selection of AER models in support of air pollution exposure assessments.

  5. Global observations and modeling of atmosphere-surface exchange of elemental mercury: a critical review

    NASA Astrophysics Data System (ADS)

    Zhu, Wei; Lin, Che-Jen; Wang, Xun; Sommar, Jonas; Fu, Xuewu; Feng, Xinbin

    2016-04-01

    Reliable quantification of air-surface fluxes of elemental Hg vapor (Hg0) is crucial for understanding mercury (Hg) global biogeochemical cycles. There have been extensive measurements and modeling efforts devoted to estimating the exchange fluxes between the atmosphere and various surfaces (e.g., soil, canopies, water, snow, etc.) in the past three decades. However, large uncertainties remain due to the complexity of Hg0 bidirectional exchange, limitations of flux quantification techniques and challenges in model parameterization. In this study, we provide a critical review on the state of science in the atmosphere-surface exchange of Hg0. Specifically, the advancement of flux quantification techniques, mechanisms in driving the air-surface Hg exchange and modeling efforts are presented. Due to the semi-volatile nature of Hg0 and redox transformation of Hg in environmental media, Hg deposition and evasion are influenced by multiple environmental variables including seasonality, vegetative coverage and its life cycle, temperature, light, moisture, atmospheric turbulence and the presence of reactants (e.g., O3, radicals, etc.). However, the effects of these processes on flux have not been fundamentally and quantitatively determined, which limits the accuracy of flux modeling. We compile an up-to-date global observational flux database and discuss the implication of flux data on the global Hg budget. Mean Hg0 fluxes obtained by micrometeorological measurements do not appear to be significantly greater than the fluxes measured by dynamic flux chamber methods over unpolluted surfaces (p = 0.16, one-tailed, Mann-Whitney U test). The spatiotemporal coverage of existing Hg0 flux measurements is highly heterogeneous with large data gaps existing in multiple continents (Africa, South Asia, Middle East, South America and Australia). The magnitude of the evasion flux is strongly enhanced by human activities, particularly at contaminated sites. Hg0 flux observations in East

  6. A model of air-sea gas exchange incorporating the physics of the turbulent boundary layer and the properties of the sea surface

    NASA Astrophysics Data System (ADS)

    Soloviev, Alexander; Schluessel, Peter

    The model presented contains interfacial, bubble-mediated, ocean mixed layer, and remote sensing components. The interfacial (direct) gas transfer dominates under conditions of low and—for quite soluble gases like CO2—moderate wind speeds. Due to the similarity between the gas and heat transfer, the temperature difference, ΔT, across the thermal molecular boundary layer (cool skin of the ocean) and the interfacial gas transfer coefficient, Kint are presumably interrelated. A coupled parameterization for ΔT and Kint has been derived in the context of a surface renewal model [Soloviev and Schluessel, 1994]. In addition to the Schmidt, Sc, and Prandtl, Pr, numbers, the important parameters are the surface Richardson number, Rƒ0, and the Keulegan number, Ke. The more readily available cool skin data are used to determine the coefficients that enter into both parameterizations. At high wind speeds, the Ke-number dependence is further verified with the formula for transformation of the surface wind stress to form drag and white capping, which follows from the renewal model. A further extension of the renewal model includes effects of solar radiation and rainfall. The bubble-mediated component incorporates the Merlivat et al. [1993] parameterization with the empirical coefficients estimated by Asher and Wanninkhof [1998]. The oceanic mixed layer component accounts for stratification effects on the air-sea gas exchange. Based on the example of GasEx-98, we demonstrate how the results of parameterization and modeling of the air-sea gas exchange can be extended to the global scale, using remote sensing techniques.

  7. Exchange of Groundwater and Surface-Water Mediated by Permafrost Response to Seasonal and Long Term Air Temperature Variation

    USGS Publications Warehouse

    Ge, Shemin; McKenzie, Jeffrey; Voss, Clifford; Wu, Qingbai

    2011-01-01

    Permafrost dynamics impact hydrologic cycle processes by promoting or impeding groundwater and surface water exchange. Under seasonal and decadal air temperature variations, permafrost temperature changes control the exchanges between groundwater and surface water. A coupled heat transport and groundwater flow model, SUTRA, was modified to simulate groundwater flow and heat transport in the subsurface containing permafrost. The northern central Tibet Plateau was used as an example of model application. Modeling results show that in a yearly cycle, groundwater flow occurs in the active layer from May to October. Maximum groundwater discharge to the surface lags the maximum subsurface temperature by two months. Under an increasing air temperature scenario of 3?C per 100 years, over the initial 40-year period, the active layer thickness can increase by three-fold. Annual groundwater discharge to the surface can experience a similar three-fold increase in the same period. An implication of these modeling results is that with increased warming there will be more groundwater flow in the active layer and therefore increased groundwater discharge to rivers. However, this finding only holds if sufficient upgradient water is available to replenish the increased discharge. Otherwise, there will be an overall lowering of the water table in the recharge portion of the catchment.

  8. Exchange of groundwater and surface-water mediated by permafrost response to seasonal and long term air temperature variation

    USGS Publications Warehouse

    Ge, S.; McKenzie, J.; Voss, C.; Wu, Q.

    2011-01-01

    Permafrost dynamics impact hydrologic cycle processes by promoting or impeding groundwater and surface water exchange. Under seasonal and decadal air temperature variations, permafrost temperature changes control the exchanges between groundwater and surface water. A coupled heat transport and groundwater flow model, SUTRA, was modified to simulate groundwater flow and heat transport in the subsurface containing permafrost. The northern central Tibet Plateau was used as an example of model application. Modeling results show that in a yearly cycle, groundwater flow occurs in the active layer from May to October. Maximum groundwater discharge to the surface lags the maximum subsurface temperature by two months. Under an increasing air temperature scenario of 3C per 100 years, over the initial 40-year period, the active layer thickness can increase by three-fold. Annual groundwater discharge to the surface can experience a similar three-fold increase in the same period. An implication of these modeling results is that with increased warming there will be more groundwater flow in the active layer and therefore increased groundwater discharge to rivers. However, this finding only holds if sufficient upgradient water is available to replenish the increased discharge. Otherwise, there will be an overall lowering of the water table in the recharge portion of the catchment. Copyright 2011 by the American Geophysical Union.

  9. Review of Air Exchange Rate Models for Air Pollution Exposure Assessments

    EPA Science Inventory

    A critical aspect of air pollution exposure assessments is estimation of the air exchange rate (AER) for various buildings, where people spend their time. The AER, which is rate the exchange of indoor air with outdoor air, is an important determinant for entry of outdoor air pol...

  10. Thermal modelling and control of 130kw direct contact (salt/air) heat exchanger

    NASA Astrophysics Data System (ADS)

    Qureshi, Omer A.; Calvet, Nicolas; Armstrong, Peter R.

    2017-06-01

    This work investigates the transient response of a certain type of direct contact heat exchanger (DCHX) that consists of packing (Raschig Rings) to increase the surface area for effective heat transfer between molten salt and air. Molten salt from the hot tank enters the heat exchanger (HX) and exit after heating the air still in the molten form. Thermal capacitance of the HX, mainly due to packing and resident salt inside the HX, results in strong transient response. Pure delay from salt residence time may also impact transient response. Both phenomena have been modelled in this paper. A Proportional-Integral controller (PI control) performance has been evaluated to maintain the minimum salt temperature above avoid crystallization temperature of the salt.

  11. Low GWP Refrigerants Modelling Study for a Room Air Conditioner Having Microchannel Heat Exchangers

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Shen, Bo; Bhandari, Mahabir S

    Microchannel heat exchangers (MHX) have found great successes in residential and commercial air conditioning applications, being compact heat exchangers, to reduce refrigerant charge and material cost. This investigation aims to extend the application of MHXs in split, room air conditioners (RAC), per fundamental heat exchanger and system modelling. For this paper, microchannel condenser and evaporator models were developed, using a segment-to-segment modelling approach. The microchannel heat exchanger models were integrated to a system design model. The system model is able to predict the performance indices, such as cooling capacity, efficiency, sensible heat ratio, etc. Using the calibrated system and heatmore » exchanger models, we evaluated numerous low GWP (global warming potential) refrigerants. The predicted system performance indices, e.g. cooling efficiency, compressor discharge temperature, and required compressor displacement volume etc., are compared. Suitable replacements for R22 and R-410A for the room air conditioner application are recommended.« less

  12. Spume Drops: Their Potential Role in Air-Sea Gas Exchange

    NASA Astrophysics Data System (ADS)

    Monahan, Edward C.; Staniec, Allison; Vlahos, Penny

    2017-12-01

    After summarizing the time scales defining the change of the physical properties of spume and other droplets cast up from the sea surface, the time scales governing drop-atmosphere gas exchange are compared. Following a broad review of the spume drop production functions described in the literature, a subset of these functions is selected via objective criteria, to represent typical, upper bound, and lower bound production functions. Three complementary mechanisms driving spume-atmosphere gas exchange are described, and one is then used to estimate the relative importance, over a broad range of wind speeds, of this spume drop mechanism compared to the conventional, diffusional, sea surface mechanism in air-sea gas exchange. While remaining uncertainties in the wind dependence of the spume drop production flux, and in the immediate sea surface gas flux, preclude a definitive conclusion, the findings of this study strongly suggest that, at high wind speeds (>20 m s-1 for dimethyl sulfide and >30 m s-1 for gases such a carbon dioxide), spume drops do make a significant contribution to air-sea gas exchange.Plain Language SummaryThis paper evaluates the existing spume drop generation functions available to date and selects a reasonable upper, lower and mid range function that are reasonable for use in <span class="hlt">air</span> sea <span class="hlt">exchange</span> <span class="hlt">models</span>. Based on these the contribution of spume drops to overall <span class="hlt">air</span> sea gas <span class="hlt">exchange</span> at different wind speeds is then evaluated to determine the % contribution of spume. Generally below 20ms-1 spume drops contribute <1% of gas <span class="hlt">exchange</span> but may account for a significant amount of gas <span class="hlt">exchange</span> at higher wind speeds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14667723','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14667723"><span>Current issues and uncertainties in the measurement and <span class="hlt">modelling</span> of <span class="hlt">air</span>-vegetation <span class="hlt">exchange</span> and within-plant processing of POPs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barber, Jonathan L; Thomas, Gareth O; Kerstiens, Gerhard; Jones, Kevin C</p> <p>2004-01-01</p> <p><span class="hlt">Air</span>-vegetation <span class="hlt">exchange</span> of POPs is an important process controlling the entry of POPs into terrestrial food chains, and may also have a significant effect on the global movement of these compounds. Many factors affect the <span class="hlt">air</span>-vegetation transfer including: the physicochemical properties of the compounds of interest; environmental factors such as temperature, wind speed, humidity and light conditions; and plant characteristics such as functional type, leaf <span class="hlt">surface</span> area, cuticular structure, and leaf longevity. The purpose of this review is to quantify the effects these differences might have on <span class="hlt">air</span>/plant <span class="hlt">exchange</span> of POPs, and to point out the major gaps in the knowledge of this subject that require further research. Uptake mechanisms are complicated, with the role of each factor in controlling partitioning, fate and behaviour process still not fully understood. Consequently, current <span class="hlt">models</span> of <span class="hlt">air</span>-vegetation <span class="hlt">exchange</span> do not incorporate variability in these factors, with the exception of temperature. These <span class="hlt">models</span> instead rely on using average values for a number of environmental factors (e.g. plant lipid content, <span class="hlt">surface</span> area), ignoring the large variations in these values. The available <span class="hlt">models</span> suggest that boundary layer conductance is of key importance in the uptake of POPs, although large uncertainties in the cuticular pathway prevents confirmation of this with any degree of certainty, and experimental data seems to show plant-side resistance to be important. <span class="hlt">Models</span> are usually based on the assumption that POP uptake occurs through the lipophilic cuticle which covers aerial <span class="hlt">surfaces</span> of plants. However, some authors have recently attached greater importance to the stomatal route of entry into the leaf for gas phase compounds. There is a need for greater mechanistic understanding of <span class="hlt">air</span>-plant <span class="hlt">exchange</span> and the 'scaling' of factors affecting it. The review also suggests a number of key variables that researchers should measure in their experiments to allow comparisons</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28447675','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28447675"><span>Back-<span class="hlt">exchange</span>: a novel approach to quantifying oxygen diffusion and <span class="hlt">surface</span> <span class="hlt">exchange</span> in ambient atmospheres.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cooper, Samuel J; Niania, Mathew; Hoffmann, Franca; Kilner, John A</p> <p>2017-05-17</p> <p>A novel two-step Isotopic <span class="hlt">Exchange</span> (IE) technique has been developed to investigate the influence of oxygen containing components of ambient <span class="hlt">air</span> (such as H 2 O and CO 2 ) on the effective <span class="hlt">surface</span> <span class="hlt">exchange</span> coefficient (k*) of a common mixed ionic electronic conductor material. The two step 'back-<span class="hlt">exchange</span>' technique was used to introduce a tracer diffusion profile, which was subsequently measured using Time-of-Flight Secondary Ion Mass Spectrometry (ToF-SIMS). The isotopic fraction of oxygen in a dense sample as a function of distance from the <span class="hlt">surface</span>, before and after the second <span class="hlt">exchange</span> step, could then be used to determine the <span class="hlt">surface</span> <span class="hlt">exchange</span> coefficient in each atmosphere. A new analytical solution was found to the diffusion equation in a semi-infinite domain with a variable <span class="hlt">surface</span> <span class="hlt">exchange</span> boundary, for the special case where D* and k* are constant for all <span class="hlt">exchange</span> steps. This solution validated the results of a numerical, Crank-Nicolson type finite-difference simulation, which was used to extract the parameters from the experimental data. When <span class="hlt">modelling</span> electrodes, D* and k* are important input parameters, which significantly impact performance. In this study La 0.6 Sr 0.4 Co 0.2 Fe 0.8 O 3-δ (LSCF6428) was investigated and it was found that the rate of <span class="hlt">exchange</span> was increased by around 250% in ambient <span class="hlt">air</span> compared to high purity oxygen at the same pO 2 . The three experiments performed in this study were used to validate the back-<span class="hlt">exchange</span> approach and show its utility.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=335530&Lab=NERL&keyword=smith&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=335530&Lab=NERL&keyword=smith&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>Probabilistic estimation of residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates for population-based human exposure <span class="hlt">modeling</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>Residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) are a key determinant in the infiltration of ambient <span class="hlt">air</span> pollution indoors. Population-based human exposure <span class="hlt">models</span> using probabilistic approaches to estimate personal exposure to <span class="hlt">air</span> pollutants have relied on input distributions from AER meas...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....1611125W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....1611125W"><span>Emission-dominated gas <span class="hlt">exchange</span> of elemental mercury vapor over natural <span class="hlt">surfaces</span> in China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Xun; Lin, Che-Jen; Yuan, Wei; Sommar, Jonas; Zhu, Wei; Feng, Xinbin</p> <p>2016-09-01</p> <p>Mercury (Hg) emission from natural <span class="hlt">surfaces</span> plays an important role in global Hg cycling. The present estimate of global natural emission has large uncertainty and remains unverified against field data, particularly for terrestrial <span class="hlt">surfaces</span>. In this study, a mechanistic <span class="hlt">model</span> is developed for estimating the emission of elemental mercury vapor (Hg0) from natural <span class="hlt">surfaces</span> in China. The development implements recent advancements in the understanding of <span class="hlt">air</span>-soil and <span class="hlt">air</span>-foliage <span class="hlt">exchange</span> of Hg0 and redox chemistry in soil and on <span class="hlt">surfaces</span>, incorporates the effects of soil characteristics and land use changes by agricultural activities, and is examined through a systematic set of sensitivity simulations. Using the <span class="hlt">model</span>, the net <span class="hlt">exchange</span> of Hg0 between the atmosphere and natural <span class="hlt">surfaces</span> of mainland China is estimated to be 465.1 Mg yr-1, including 565.5 Mg yr-1 from soil <span class="hlt">surfaces</span>, 9.0 Mg yr-1 from water bodies, and -100.4 Mg yr-1 from vegetation. The <span class="hlt">air-surface</span> <span class="hlt">exchange</span> is strongly dependent on the land use and meteorology, with 9 % of net emission from forest ecosystems; 50 % from shrubland, savanna, and grassland; 33 % from cropland; and 8 % from other land uses. Given the large agricultural land area in China, farming activities play an important role on the <span class="hlt">air-surface</span> <span class="hlt">exchange</span> over farmland. Particularly, rice field shift from a net sink (3.3 Mg uptake) during April-October (rice planting) to a net source when the farmland is not flooded (November-March). Summing up the emission from each land use, more than half of the total emission occurs in summer (51 %), followed by spring (28 %), autumn (13 %), and winter (8 %). <span class="hlt">Model</span> verification is accomplished using observational data of <span class="hlt">air-soil/air</span>-water fluxes and Hg deposition through litterfall for forest ecosystems in China and Monte Carlo simulations. In contrast to the earlier estimate by Shetty et al. (2008) that reported large emission from vegetative <span class="hlt">surfaces</span> using an evapotranspiration approach, the estimate in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA115928','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA115928"><span>Generic <span class="hlt">Surface-to-Air</span> Missile <span class="hlt">Model</span>.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1979-10-01</p> <p>describes the Generic <span class="hlt">Surface-to-Air</span> Missile <span class="hlt">Model</span> (GENSAM) which evaluates the outcome of an engagement between a <span class="hlt">surface-to-air</span> missile system and an...DETAILS OF THE GENERIC SAM <span class="hlt">MODEL</span> 3-1 3.1 Coordinate Transformations 3-1 3.1.1 Coordinate Systems 3-1 3.1.2 Coordinate Transformations 3-4 3.1.3 Functions...Tracking Radars 3-54 3.3.11 Deception Jamming and Tracking Radars 3-55 3.3.12 Jaming and Track Radar Downlinks 3-56 3.3.13 Infrared Surveillance Systems 3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=332786','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=332786"><span>Impact of aerodynamic resistance formulations used in two-source <span class="hlt">modeling</span> of energy <span class="hlt">exchange</span> from the soil and vegetation using land <span class="hlt">surface</span> temperature</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>Application of the Two-Source Energy Balance (TSEB) <span class="hlt">Model</span> using land <span class="hlt">surface</span> temperature (LST) requires aerodynamic resistance parameterizations for the flux <span class="hlt">exchange</span> above the canopy layer, within the canopy <span class="hlt">air</span> space and at the soil/substrate <span class="hlt">surface</span>. There are a number of aerodynamic resistance f...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.891a2135C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.891a2135C"><span>Research on Heat <span class="hlt">Exchange</span> Process in Aircraft <span class="hlt">Air</span> Conditioning System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chichindaev, A. V.</p> <p>2017-11-01</p> <p>Using of heat-<span class="hlt">exchanger</span>-condenser in the <span class="hlt">air</span> conditioning system of the airplane Tu-204 (Boeing, Airbus, Superjet 100, MS-21, etc.) for cooling the compressed <span class="hlt">air</span> by the cold <span class="hlt">air</span> with negative temperature exiting the turbine results in a number of operational problems. Mainly it’s frosting of the heat <span class="hlt">exchange</span> <span class="hlt">surface</span>, which is the cause of live-section channels frosting, resistance increasing and airflow in the system decreasing. The purpose of this work is to analyse the known freeze-up-fighting methods for heat-<span class="hlt">exchanger</span>-condenser, description of the features of anti-icing protection and offering solutions to this problem. For the problem of optimizing the design of heat <span class="hlt">exchangers</span> in this work used generalized criterion that describes the ratio of thermal resistances of cold and hot sections, which include: the ratio of the initial values of heat transfer agents flow state; heat <span class="hlt">exchange</span> <span class="hlt">surface</span> finning coefficients; factors which describes the ratio of operating parameters and finning area. By controlling the ratio of the thermal resistances can be obtained the desired temperature of the heat <span class="hlt">exchange</span> <span class="hlt">surface</span>, which would prevent freezing. The work presents the results of a numerical study of the effect of different combinations of regime and geometrical factors changes on reduction of the heat-<span class="hlt">exchanger</span>-condenser freezing <span class="hlt">surface</span> area, including using of variable ratio of thermal resistances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A23A..04C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A23A..04C"><span><span class="hlt">Air</span>-Sea Momentum and Enthalpy <span class="hlt">Exchange</span> in Coupled Atmosphere-Wave-Ocean <span class="hlt">Modeling</span> of Tropical Cyclones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Curcic, M.; Chen, S. S.</p> <p>2016-02-01</p> <p>The atmosphere and ocean are coupled through momentum, enthalpy, and mass fluxes. Accurate representation of these fluxes in a wide range of weather and climate conditions is one of major challenges in prediction <span class="hlt">models</span>. Their current parameterizations are based on sparse observations in low-to-moderate winds and are not suited for high wind conditions such as tropical cyclones (TCs) and winter storms. In this study, we use the Unified Wave INterface - Coupled <span class="hlt">Model</span> (UWIN-CM), a high resolution, fully-coupled atmosphere-wave-ocean <span class="hlt">model</span>, to better understand the role of ocean <span class="hlt">surface</span> waves in mediating <span class="hlt">air</span>-sea momentum and enthalpy <span class="hlt">exchange</span> in TCs. In particular, we focus on the explicit treatment of wave growth and dissipation for calculating atmospheric and oceanic stress, and its role in upper ocean mixing and <span class="hlt">surface</span> cooling in the wake of the storm. Wind-wave misalignment and local wave disequilibrium result in difference between atmospheric and oceanic stress being largest on the left side of the storm. We find that explicit wave calculation in the coupled <span class="hlt">model</span> reduces momentum transfer into the ocean by more than 10% on average, resulting in reduced cooling in TC's wake and subsequent weakening of the storm. We also investigate the impacts of sea <span class="hlt">surface</span> temperature and upper ocean parameterization on <span class="hlt">air</span>-sea enthalpy fluxes in the fully coupled <span class="hlt">model</span>. High-resolution UWIN-CM simulations of TCs with various intensities and structure are conducted in this study to better understand the complex TC-ocean interaction and improve the representation of <span class="hlt">air</span>-sea coupling processes in coupled prediction <span class="hlt">models</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li class="active"><span>1</span></li> <li><a href="#" onclick='return showDiv("page_2");'>2</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><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_1 --> <div id="page_2" 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 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> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="21"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......178W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......178W"><span>Aqueous turbulence structure immediately adjacent to the <span class="hlt">air</span> - water interface and interfacial gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Binbin</p> <p></p> <p><span class="hlt">Air</span>-sea interaction and the interfacial <span class="hlt">exchange</span> of gas across the <span class="hlt">air</span>-water interface are of great importance in coupled atmospheric-oceanic environmental systems. Aqueous turbulence structure immediately adjacent to the <span class="hlt">air</span>-water interface is the combined result of wind, <span class="hlt">surface</span> waves, currents and other environmental forces and plays a key role in energy budgets, gas fluxes and hence the global climate system. However, the quantification of turbulence structure sufficiently close to the <span class="hlt">air</span>-water interface is extremely difficult. The physical relationship between interfacial gas <span class="hlt">exchange</span> and near <span class="hlt">surface</span> turbulence remains insufficiently investigated. This dissertation aims to measure turbulence in situ in a complex environmental forcing system on Lake Michigan and to reveal the relationship between turbulent statistics and the CO2 flux across the <span class="hlt">air</span>-water interface. The major objective of this dissertation is to investigate the physical control of the interfacial gas <span class="hlt">exchange</span> and to provide a universal parameterization of gas transfer velocity from environmental factors, as well as to propose a mechanistic <span class="hlt">model</span> for the global CO2 flux that can be applied in three dimensional climate-ocean <span class="hlt">models</span>. Firstly, this dissertation presents an advanced measurement instrument, an in situ free floating Particle Image Velocimetry (FPIV) system, designed and developed to investigate the small scale turbulence structure immediately below the <span class="hlt">air</span>-water interface. Description of hardware components, design of the system, measurement theory, data analysis procedure and estimation of measurement error were provided. Secondly, with the FPIV system, statistics of small scale turbulence immediately below the <span class="hlt">air</span>-water interface were investigated under a variety of environmental conditions. One dimensional wave-number spectrum and structure function sufficiently close to the water <span class="hlt">surface</span> were examined. The vertical profiles of turbulent dissipation rate were intensively studied</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10369593','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10369593"><span>Effect of humidity on posterior lens opacification during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Harlan, J B; Lee, E T; Jensen, P S; de Juan, E</p> <p>1999-06-01</p> <p>To study the relationship of humidity and the rate of lens opacity formation during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> using an animal <span class="hlt">model</span>. Vitrectomy and fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> was carried out using 16 eyes of 8 pigmented rabbits. One eye of each rabbit was exposed to dry <span class="hlt">air</span> and the fellow eye received humidified <span class="hlt">air</span> using an intraocular <span class="hlt">air</span> humidifier. In each case, the percent humidity of the intraocular <span class="hlt">air</span> was measured using an in-line hygrometer. Elapsed time from initial <span class="hlt">air</span> entry to lens feathering was recorded for each eye, with the surgeon-observer unaware of the percent humidity of the <span class="hlt">air</span> infusion. In each rabbit, use of humidified <span class="hlt">air</span> resulted in a delay in lens feathering (P<.02), with an overall increase in time to feathering of 80% for humidified <span class="hlt">air</span> vs room <span class="hlt">air</span>. Use of a humidifier during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> prolongs intraoperative lens clarity in the rabbit <span class="hlt">model</span>, suggesting that humidified <span class="hlt">air</span> should prolong lens clarity during phakic fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> in patients. Use of humidified <span class="hlt">air</span> during vitrectomy and fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> may retard the intraoperative loss of lens clarity, promoting better visualization of the posterior segment and enhancing surgical performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27..874S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27..874S"><span>Observational Studies of Parameters Influencing <span class="hlt">Air</span>-sea Gas <span class="hlt">Exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schimpf, U.; Frew, N. M.; Bock, E. J.; Hara, T.; Garbe, C. S.; Jaehne, B.</p> <p></p> <p>A physically-based <span class="hlt">modeling</span> of the <span class="hlt">air</span>-sea gas transfer that can be used to predict the gas transfer rates with sufficient accuracy as a function of micrometeorological parameters is still lacking. State of the art are still simple gas transfer rate/wind speed relationships. Previous measurements from Coastal Ocean Experiment in the Atlantic revealed positive correlations between mean square slope, near <span class="hlt">surface</span> turbulent dis- sipation, and wind stress. It also demonstrated a strong negative correlation between mean square slope and the fluorescence of <span class="hlt">surface</span>-enriched colored dissolved organic matter. Using heat as a proxy tracer for gases the <span class="hlt">exchange</span> process at the <span class="hlt">air</span>/water interface and the micro turbulence at the water <span class="hlt">surface</span> can be investigated. The anal- ysis of infrared image sequences allow the determination of the net heat flux at the ocean <span class="hlt">surface</span>, the temperature gradient across the <span class="hlt">air</span>/sea interface and thus the heat transfer velocity and gas transfer velocity respectively. Laboratory studies were carried out in the new Heidelberg wind-wave facility AELOTRON. Direct measurements of the Schmidt number exponent were done in conjunction with classical mass balance methods to estimate the transfer velocity. The laboratory results allowed to validate the basic assumptions of the so called controlled flux technique by applying differ- ent tracers for the gas <span class="hlt">exchange</span> in a large Schmidt number regime. Thus a <span class="hlt">modeling</span> of the Schmidt number exponent is able to fill the gap between laboratory and field measurements field. Both, the results from the laboratory and the field measurements should be able to give a further understanding of the mechanisms controlling the trans- port processes across the aqueous boundary layer and to relate the forcing functions to parameters measured by remote sensing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=213610&Lab=NERL&keyword=NASA&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=213610&Lab=NERL&keyword=NASA&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>Impact of High Resolution Land-Use Data in Meteorology and <span class="hlt">Air</span> Quality <span class="hlt">Modeling</span> Systems</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>Accurate land use information is important in meteorology for land <span class="hlt">surface</span> <span class="hlt">exchanges</span>, in emission <span class="hlt">modeling</span> for emission spatial allocation, and in <span class="hlt">air</span> quality <span class="hlt">modeling</span> for chemical <span class="hlt">surface</span> fluxes. Currently, meteorology, emission, and <span class="hlt">air</span> quality <span class="hlt">models</span> often use outdated USGS Gl...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..4412324M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..4412324M"><span>Enrichment of Extracellular Carbonic Anhydrase in the Sea <span class="hlt">Surface</span> Microlayer and Its Effect on <span class="hlt">Air</span>-Sea CO2 <span class="hlt">Exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mustaffa, N. I. H.; Striebel, M.; Wurl, O.</p> <p>2017-12-01</p> <p>This paper describes the quantification of extracellular carbonic anhydrase (eCA) concentrations in the sea <span class="hlt">surface</span> microlayer (SML), the boundary layer between the ocean and the atmosphere of the Indo-West Pacific. We demonstrated that the SML is enriched with eCA by 1.5 ± 0.7 compared to the mixed underlying water. Enrichment remains up to a wind speed of 7 m s-1 (i.e., under typical oceanic conditions). As eCA catalyzes the interconversion of HCO3- and CO2, it has been hypothesized that its enrichment in the SML enhances the <span class="hlt">air</span>-sea CO2 <span class="hlt">exchange</span>. We detected concentrations in the range of 0.12 to 0.76 n<fi>M</fi>, which can enhance the <span class="hlt">exchange</span> by up to 15% based on the <span class="hlt">model</span> approach described in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPhCS.655a2035D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPhCS.655a2035D"><span><span class="hlt">Modelling</span> heat and mass transfer in a membrane-based <span class="hlt">air-to-air</span> enthalpy <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dugaria, S.; Moro, L.; Del, D., Col</p> <p>2015-11-01</p> <p>The diffusion of total energy recovery systems could lead to a significant reduction in the energy demand for building <span class="hlt">air</span>-conditioning. With these devices, sensible heat and humidity can be recovered in winter from the exhaust airstream, while, in summer, the incoming <span class="hlt">air</span> stream can be cooled and dehumidified by transferring the excess heat and moisture to the exhaust <span class="hlt">air</span> stream. Membrane based enthalpy <span class="hlt">exchangers</span> are composed by different channels separated by semi-permeable membranes. The membrane allows moisture transfer under vapour pressure difference, or water concentration difference, between the two sides and, at the same time, it is ideally impermeable to <span class="hlt">air</span> and other contaminants present in exhaust <span class="hlt">air</span>. Heat transfer between the airstreams occurs through the membrane due to the temperature gradient. The aim of this work is to develop a detailed <span class="hlt">model</span> of the coupled heat and mass transfer mechanisms through the membrane between the two airstreams. After a review of the most relevant <span class="hlt">models</span> published in the scientific literature, the governing equations are presented and some simplifying assumptions are analysed and discussed. As a result, a steady-state, two-dimensional finite difference numerical <span class="hlt">model</span> is setup. The developed <span class="hlt">model</span> is able to predict temperature and humidity evolution inside the channels. Sensible and latent heat transfer rate, as well as moisture transfer rate, are determined. A sensitive analysis is conducted in order to determine the more influential parameters on the thermal and vapour transfer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AtmEn.174..148P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AtmEn.174..148P"><span>Impact of chemical lateral boundary conditions in a regional <span class="hlt">air</span> quality forecast <span class="hlt">model</span> on <span class="hlt">surface</span> ozone predictions during stratospheric intrusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pendlebury, Diane; Gravel, Sylvie; Moran, Michael D.; Lupu, Alexandru</p> <p>2018-02-01</p> <p>A regional <span class="hlt">air</span> quality forecast <span class="hlt">model</span>, GEM-MACH, is used to examine the conditions under which a limited-area <span class="hlt">air</span> quality <span class="hlt">model</span> can accurately forecast near-<span class="hlt">surface</span> ozone concentrations during stratospheric intrusions. Periods in 2010 and 2014 with known stratospheric intrusions over North America were <span class="hlt">modelled</span> using four different ozone lateral boundary conditions obtained from a seasonal climatology, a dynamically-interpolated monthly climatology, global <span class="hlt">air</span> quality forecasts, and global <span class="hlt">air</span> quality reanalyses. It is shown that the mean bias and correlation in <span class="hlt">surface</span> ozone over the course of a season can be improved by using time-varying ozone lateral boundary conditions, particularly through the correct assignment of stratospheric vs. tropospheric ozone along the western lateral boundary (for North America). Part of the improvement in <span class="hlt">surface</span> ozone forecasts results from improvements in the characterization of near-<span class="hlt">surface</span> ozone along the lateral boundaries that then directly impact <span class="hlt">surface</span> locations near the boundaries. However, there is an additional benefit from the correct characterization of the location of the tropopause along the western lateral boundary such that the <span class="hlt">model</span> can correctly simulate stratospheric intrusions and their associated <span class="hlt">exchange</span> of ozone from stratosphere to troposphere. Over a three-month period in spring 2010, the mean bias was seen to improve by as much as 5 ppbv and the correlation by 0.1 depending on location, and on the form of the chemical lateral boundary condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850005886&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dheat%2Bexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850005886&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dheat%2Bexchange"><span><span class="hlt">Air</span>-sea heat <span class="hlt">exchange</span>, an element of the water cycle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chahine, M. T.</p> <p>1984-01-01</p> <p>The distribution and variation of water vapor, clouds and precipitation are examined. Principal driving forces for these distributions are energy <span class="hlt">exchange</span> and evaporation at the <span class="hlt">air</span>-sea interface, which are also important elements of <span class="hlt">air</span>-sea interaction studies. The overall aim of <span class="hlt">air</span>-sea interaction studies is to quantitatively determine mass, momentum and energy fluxes, with the goal of understanding the mechanisms controlling them. The results of general circulation simulations indicate that the atmosphere in mid-latitudes responds to changes in the oceanic <span class="hlt">surface</span> conditions in the tropics. This correlation reflects the strong interaction between tropical and mid-latitude conditions caused by the transport of heat and momentum from the tropics. Studies of <span class="hlt">air</span>-sea <span class="hlt">exchanges</span> involve a large number of physica, chemical and dynamical processes including heat flux, radiation, sea-<span class="hlt">surface</span> temperature, precipitation, winds and ocean currents. The fluxes of latent heat are studied and the potential use of satellite data in determining them evaluated. Alternative ways of inferring heat fluxes will be considered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1611343P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1611343P"><span>Surfactant control of <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> across contrasting biogeochemical regimes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pereira, Ryan; Schneider-Zapp, Klaus; Upstill-Goddard, Robert</p> <p>2014-05-01</p> <p><span class="hlt">Air</span>-sea gas <span class="hlt">exchange</span> is important to the global partitioning of CO2.<span class="hlt">Exchange</span> fluxes are products of an <span class="hlt">air</span>-sea gas concentration difference, ΔC, and a gas transfer velocity, kw. The latter is controlled by the rate of turbulent diffusion at the <span class="hlt">air</span>-sea interface but it cannot be directly measured and has a high uncertainty that is now considered one of the greatest challenges to quantifying net global <span class="hlt">air</span>-sea CO2 <span class="hlt">exchange</span> ...(Takahashi et al., 2009). One important control on kw is exerted by sea <span class="hlt">surface</span> surfactants that arise both naturally from biological processes and through anthropogenic activity. They influence gas <span class="hlt">exchange</span> in two fundamental ways: as a monolayer physical barrier and through modifying sea <span class="hlt">surface</span> hydrodynamics and hence turbulent energy transfer. These effects have been demonstrated in the laboratory with artificial surfactants ...(Bock et al., 1999; Goldman et al., 1988) and through purposeful surfactant releases in coastal waters .(.).........().(Brockmann et al., 1982) and in the open ocean (Salter et al., 2011). Suppression of kwin these field experiments was ~5-55%. While changes in both total surfactant concentration and the composition of the natural surfactant pool might be expected to impact kw, the required in-situ studies are lacking. New data collected from the coastal North Sea in 2012-2013 shows significant spatio-temporal variability in the surfactant activity of organic matter within the sea <span class="hlt">surface</span> microlayer that ranges from 0.07-0.94 mg/L T-X-100 (AC voltammetry). The surfactant activities show a strong winter/summer seasonal bias and general decrease in concentration with increasing distance from the coastline possibly associated with changing terrestrial vs. phytoplankton sources. Gas <span class="hlt">exchange</span> experiments of this seawater using a novel laboratory tank and gas tracers (CH4 and SF6) demonstrate a 12-45% reduction in kw compared to surfactant-free water. Seasonally there is higher gas <span class="hlt">exchange</span> suppression in the summer</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PrOce.144...15W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PrOce.144...15W"><span>Biofilm-like properties of the sea <span class="hlt">surface</span> and predicted effects on <span class="hlt">air</span>-sea CO2 <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wurl, Oliver; Stolle, Christian; Van Thuoc, Chu; The Thu, Pham; Mari, Xavier</p> <p>2016-05-01</p> <p>Because the sea <span class="hlt">surface</span> controls various interactions between the ocean and the atmosphere, it has a profound function for marine biogeochemistry and climate regulation. The sea <span class="hlt">surface</span> is the gateway for the <span class="hlt">exchange</span> of climate-relevant gases, heat and particles. Thus, in order to determine how the ocean and the atmosphere interact and respond to environmental changes on a global scale, the characterization and understanding of the sea <span class="hlt">surface</span> are essential. The uppermost part of the water column is defined as the sea-<span class="hlt">surface</span> microlayer and experiences strong spatial and temporal dynamics, mainly due to meteorological forcing. Wave-damped areas at the sea <span class="hlt">surface</span> are caused by the accumulation of <span class="hlt">surface</span>-active organic material and are defined as slicks. Natural slicks are observed frequently but their biogeochemical properties are poorly understood. In the present study, we found up to 40 times more transparent exopolymer particles (TEP), the foundation of any biofilm, in slicks compared to the underlying bulk water at multiple stations in the North Pacific, South China Sea, and Baltic Sea. We found a significant lower enrichment of TEP (up to 6) in non-slick sea <span class="hlt">surfaces</span> compared to its underlying bulk water. Moreover, slicks were characterized by a large microbial biomass, another shared feature with conventional biofilms on solid <span class="hlt">surfaces</span>. Compared to non-slick samples (avg. pairwise similarity of 70%), the community composition of bacteria in slicks was increasingly (avg. pairwise similarity of 45%) different from bulk water communities, indicating that the TEP-matrix creates specific environments for its inhabitants. We, therefore, conclude that slicks can feature biofilm-like properties with the excessive accumulation of particles and microbes. We also assessed the potential distribution and frequency of slick-formation in coastal and oceanic regions, and their effect on <span class="hlt">air</span>-sea CO2 <span class="hlt">exchange</span> based on literature data. We estimate that slicks can reduce CO2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED259926.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED259926.pdf"><span>Heat Recovery Ventilation for Housing: <span class="hlt">Air-to-Air</span> Heat <span class="hlt">Exchangers</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Corbett, Robert J.; Miller, Barbara</p> <p></p> <p>The <span class="hlt">air-to-air</span> heat <span class="hlt">exchanger</span> (a fan powered ventilation device that recovers heat from stale outgoing <span class="hlt">air</span>) is explained in this six-part publication. Topic areas addressed are: (1) the nature of <span class="hlt">air-to-air</span> heat <span class="hlt">exchangers</span> and how they work; (2) choosing and sizing the system; (3) installation, control, and maintenance of the system; (4) heat…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ACPD...1227927E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ACPD...1227927E"><span><span class="hlt">Air-surface</span> <span class="hlt">exchange</span> measurements of gaseous elemental mercury over naturally enriched and background terrestrial landscapes in Australia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Edwards, G. C.; Howard, D. A.</p> <p>2012-10-01</p> <p>This paper presents the first gaseous elemental mercury (GEM) <span class="hlt">air-surface</span> <span class="hlt">exchange</span> measurements obtained over naturally enriched and background (< 0.1 μg g-1 Hg) terrestrial landscapes in Australia. Two pilot field studies were carried out during the Australian autumn and winter periods at a copper-gold-cobalt-arsenic-mercury mineral field near Pulganbar, NSW. GEM fluxes using a dynamic flux chamber approach were measured, along with controlling environmental parameters over three naturally enriched and three background substrates. The enriched sites results showed net emission to the atmosphere and a strong correlation between flux and substrate Hg concentration, with average fluxes ranging from 14 ± 1 ng m-2 h-1 to 113 ± 6 ng m-2 h-1. Measurements at background sites showed both emission and deposition. The average Hg flux from all background sites showed an overall net emission of 0.36 ± 0.06 ng m-2 h-1. Fluxes show strong relationships with temperature, radiation, and substrate parameters. A compensation point of 2.48, representative of bare soils was determined. Comparison of the Australian data to North American data confirmed the need for Australian specific mercury <span class="hlt">air-surface</span> <span class="hlt">exchange</span> data representative of Australia's unique climatic conditions, vegetation types, land use patterns, and soils.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA282842','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA282842"><span>Oceanic Whitecaps and Associated, Bubble-Mediated, <span class="hlt">Air</span>-Sea <span class="hlt">Exchange</span> Processes</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1992-10-01</p> <p>experiments performed in laboratory conditions using <span class="hlt">Air</span>-Sea <span class="hlt">Exchange</span> Monitoring System (A-SEMS). EXPERIMENTAL SET-UP In a first look, the <span class="hlt">Air</span>-Sea <span class="hlt">Exchange...Model</span> 225, equipped with a <span class="hlt">Model</span> 519 plug-in module. Other complementary information on A-SEMS along with results from first tests and calibration...between 9.50C and 22.40C within the first 24 hours after transferring the water sample into laboratory conditions. The results show an enhancement of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGeo...10.5793S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGeo...10.5793S"><span>Biology and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> controls on the distribution of carbon isotope ratios (δ13C) in the ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmittner, A.; Gruber, N.; Mix, A. C.; Key, R. M.; Tagliabue, A.; Westberry, T. K.</p> <p>2013-09-01</p> <p>Analysis of observations and sensitivity experiments with a new three-dimensional global <span class="hlt">model</span> of stable carbon isotope cycling elucidate processes that control the distribution of δ13C of dissolved inorganic carbon (DIC) in the contemporary and preindustrial ocean. Biological fractionation and the sinking of isotopically light δ13C organic matter from the <span class="hlt">surface</span> into the interior ocean leads to low δ13CDIC values at depths and in high latitude <span class="hlt">surface</span> waters and high values in the upper ocean at low latitudes with maxima in the subtropics. <span class="hlt">Air</span>-sea gas <span class="hlt">exchange</span> has two effects. First, it acts to reduce the spatial gradients created by biology. Second, the associated temperature-dependent fractionation tends to increase (decrease) δ13CDIC values of colder (warmer) water, which generates gradients that oppose those arising from biology. Our <span class="hlt">model</span> results suggest that both effects are similarly important in influencing <span class="hlt">surface</span> and interior δ13CDIC distributions. However, since <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> is slow in the modern ocean, the biological effect dominates spatial δ13CDIC gradients both in the interior and at the <span class="hlt">surface</span>, in contrast to conclusions from some previous studies. Calcium carbonate cycling, pH dependency of fractionation during <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>, and kinetic fractionation have minor effects on δ13CDIC. Accumulation of isotopically light carbon from anthropogenic fossil fuel burning has decreased the spatial variability of <span class="hlt">surface</span> and deep δ13CDIC since the industrial revolution in our <span class="hlt">model</span> simulations. Analysis of a new synthesis of δ13CDIC measurements from years 1990 to 2005 is used to quantify preformed and remineralized contributions as well as the effects of biology and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>. The <span class="hlt">model</span> reproduces major features of the observed large-scale distribution of δ13CDIC as well as the individual contributions and effects. Residual misfits are documented and analyzed. Simulated <span class="hlt">surface</span> and subsurface δ13CDIC are influenced by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/1208301','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/1208301"><span>[Comparative study of respiratory <span class="hlt">exchanging</span> <span class="hlt">surfaces</span> in birds and mammals].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jammes, Y</p> <p>1975-01-01</p> <p>Anatomical studies of the respiratory apparatus of birds show evidences for a gas <span class="hlt">exchanging</span> tubular system (parabronchi and <span class="hlt">air</span> capillaries); these <span class="hlt">exchanging</span> structures are entirely dissociated from the ventilatory drive acting on the <span class="hlt">air</span> sacs. A "cross-current" gas <span class="hlt">exchanging</span> system (perpendicular disposition of <span class="hlt">air</span> and blood capillaries) allow a good wash-out of carbon dioxide (PaCO2 lower than PECO2). The great efficiency of this lung is allowed by its very large diffusive <span class="hlt">surface</span> (ASa) and by the high values of lung specific oxygen diffusing capacity (DO2/ASa) and of O2 extraction coefficient in inspired <span class="hlt">air</span>. The ventilatory pattern of birds is characterized by a greater tidal volume and a smaller respiratory frequency than in mammals of same weight. Respiratory centers of birds receive afferences from lung stretch receptors, CO2-sensitive lung receptors and arterial chemoreceptors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009GeCoA..73..543S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009GeCoA..73..543S"><span>A <span class="hlt">surface</span> complexation and ion <span class="hlt">exchange</span> <span class="hlt">model</span> of Pb and Cd competitive sorption on natural soils</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Serrano, Susana; O'Day, Peggy A.; Vlassopoulos, Dimitri; García-González, Maria Teresa; Garrido, Fernando</p> <p>2009-02-01</p> <p>The bioavailability and fate of heavy metals in the environment are often controlled by sorption reactions on the reactive <span class="hlt">surfaces</span> of soil minerals. We have developed a non-electrostatic equilibrium <span class="hlt">model</span> (NEM) with both <span class="hlt">surface</span> complexation and ion <span class="hlt">exchange</span> reactions to describe the sorption of Pb and Cd in single- and binary-metal systems over a range of pH and metal concentration. Mineralogical and <span class="hlt">exchange</span> properties of three different acidic soils were used to constrain <span class="hlt">surface</span> reactions in the <span class="hlt">model</span> and to estimate <span class="hlt">surface</span> densities for sorption sites, rather than treating them as adjustable parameters. Soil heterogeneity was <span class="hlt">modeled</span> with >FeOH and >SOH functional groups, representing Fe- and Al-oxyhydroxide minerals and phyllosilicate clay mineral edge sites, and two ion <span class="hlt">exchange</span> sites (X - and Y -), representing clay mineral <span class="hlt">exchange</span>. An optimization process was carried out using the entire experimental sorption data set to determine the binding constants for Pb and Cd <span class="hlt">surface</span> complexation and ion <span class="hlt">exchange</span> reactions. <span class="hlt">Modeling</span> results showed that the adsorption of Pb and Cd was distributed between ion <span class="hlt">exchange</span> sites at low pH values and specific adsorption sites at higher pH values, mainly associated with >FeOH sites. <span class="hlt">Modeling</span> results confirmed the greater tendency of Cd to be retained on <span class="hlt">exchange</span> sites compared to Pb, which had a higher affinity than Cd for specific adsorption on >FeOH sites. Lead retention on >FeOH occurred at lower pH than for Cd, suggesting that Pb sorbs to <span class="hlt">surface</span> hydroxyl groups at pH values at which Cd interacts only with <span class="hlt">exchange</span> sites. The results from the binary system (both Pb and Cd present) showed that Cd retained in >FeOH sites decreased significantly in the presence of Pb, while the occupancy of Pb in these sites did not change in the presence of Cd. As a consequence of this competition, Cd was shifted to ion <span class="hlt">exchange</span> sites, where it competes with Pb and possibly Ca (from the background electrolyte). Sorption on >SOH</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019914','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019914"><span>Coupled land <span class="hlt">surface</span>/hydrologic/atmospheric <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pielke, Roger; Steyaert, Lou; Arritt, Ray; Lahtakia, Mercedes; Smith, Chris; Ziegler, Conrad; Soong, Su Tzai; Avissar, Roni; Wetzel, Peter; Sellers, Piers</p> <p>1993-01-01</p> <p>The topics covered include the following: prototype land cover characteristics data base for the conterminous United States; <span class="hlt">surface</span> evapotranspiration effects on cumulus convection and implications for mesoscale <span class="hlt">models</span>; the use of complex treatment of <span class="hlt">surface</span> hydrology and thermodynamics within a mesoscale <span class="hlt">model</span> and some related issues; initialization of soil-water content for regional-scale atmospheric prediction <span class="hlt">models</span>; impact of <span class="hlt">surface</span> properties on dryline and MCS evolution; a numerical simulation of heavy precipitation over the complex topography of California; representing mesoscale fluxes induced by landscape discontinuities in global climate <span class="hlt">models</span>; emphasizing the role of subgrid-scale heterogeneity in <span class="hlt">surface-air</span> interaction; and problems with <span class="hlt">modeling</span> and measuring biosphere-atmosphere <span class="hlt">exchanges</span> of energy, water, and carbon on large scales.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B24A..04M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B24A..04M"><span>Relationships between Hg <span class="hlt">Air-surface</span> <span class="hlt">exchange</span>, Soil Moisture and Precipitation at a Background Vegetated Site in South-Eastern Australia.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macsween, K.; Edwards, G. C.</p> <p>2017-12-01</p> <p>Despite many decades of research, the controlling mechanisms of mercury (Hg) <span class="hlt">air-surface</span> exhange are still poorly understood. Particularly in Australian ecosystems where there are few anthropogenic inputs. A clear understanding of these mechanisms is vital for accurate representation in the global Hg <span class="hlt">models</span>, particularly regarding re-emission. Water is known to have a considerable influence on Hg <span class="hlt">exchange</span> within a terrestrial ecosystem. Precipitation has been found to cause spikes is Hg emissions during the initial stages of rain event. While, Soil moisture content is known to enhance fluxes between 15 and 30% Volumetric soil water (VSW), above which fluxes become suppressed. Few field experiments exist to verify these dominantly laboratory or controlled experiments. Here we present work looking at Hg fluxes over an 8-month period at a vegetated background site. The aim of this study is to identify how changes to precipitation intensity and duration, coupled with variable soil moisture content may influence Hg flux across seasons. As well as the influence of other meteorological variables. Experimentation was undertaken using aerodynamic gradient micrometeorological flux method, avoiding disruption to the <span class="hlt">surface</span>, soil moisture probes and rain gauge measurements to monitor alterations to substrate conditions. Meteorological and <span class="hlt">air</span> chemistry variables were also measured concurrently throughout the duration of the study. During the study period, South-Eastern Australia experienced several intense east coast low storm systems during the Autumn and Spring months and an unusually dry winter. VSW rarely reached above 30% even following the intense rainfall experienced during the east coast lows. The generally dry conditions throughout winter resulted in an initial spike in Hg emissions when rainfall occurred. Fluxes decreased shortly after the rain began but remained slightly elevated. Given the reduced net radiation and cooler temperatures experienced during the winter</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5228218','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5228218"><span>Impacts of Changes of Indoor <span class="hlt">Air</span> Pressure and <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate in Vapor Intrusion Scenarios</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shen, Rui; Suuberg, Eric M.</p> <p>2016-01-01</p> <p>There has, in recent years, been increasing interest in understanding the transport processes of relevance in vapor intrusion of volatile organic compounds (VOCs) into buildings on contaminated sites. These studies have included fate and transport <span class="hlt">modeling</span>. Most such <span class="hlt">models</span> have simplified the prediction of indoor <span class="hlt">air</span> contaminant vapor concentrations by employing a steady state assumption, which often results in difficulties in reconciling these results with field measurements. This paper focuses on two major factors that may be subject to significant transients in vapor intrusion situations, including the indoor <span class="hlt">air</span> pressure and the <span class="hlt">air</span> <span class="hlt">exchange</span> rate in the subject building. A three-dimensional finite element <span class="hlt">model</span> was employed with consideration of daily and seasonal variations in these factors. From the results, the variations of indoor <span class="hlt">air</span> pressure and <span class="hlt">air</span> <span class="hlt">exchange</span> rate are seen to contribute to significant variations in indoor <span class="hlt">air</span> contaminant vapor concentrations. Depending upon the assumptions regarding the variations in these parameters, the results are only sometimes consistent with the reports of several orders of magnitude in indoor <span class="hlt">air</span> concentration variations from field studies. The results point to the need to examine more carefully the interplay of these factors in order to quantitatively understand the variations in potential indoor <span class="hlt">air</span> exposures. PMID:28090133</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28090133','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28090133"><span>Impacts of Changes of Indoor <span class="hlt">Air</span> Pressure and <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate in Vapor Intrusion Scenarios.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shen, Rui; Suuberg, Eric M</p> <p>2016-02-01</p> <p>There has, in recent years, been increasing interest in understanding the transport processes of relevance in vapor intrusion of volatile organic compounds (VOCs) into buildings on contaminated sites. These studies have included fate and transport <span class="hlt">modeling</span>. Most such <span class="hlt">models</span> have simplified the prediction of indoor <span class="hlt">air</span> contaminant vapor concentrations by employing a steady state assumption, which often results in difficulties in reconciling these results with field measurements. This paper focuses on two major factors that may be subject to significant transients in vapor intrusion situations, including the indoor <span class="hlt">air</span> pressure and the <span class="hlt">air</span> <span class="hlt">exchange</span> rate in the subject building. A three-dimensional finite element <span class="hlt">model</span> was employed with consideration of daily and seasonal variations in these factors. From the results, the variations of indoor <span class="hlt">air</span> pressure and <span class="hlt">air</span> <span class="hlt">exchange</span> rate are seen to contribute to significant variations in indoor <span class="hlt">air</span> contaminant vapor concentrations. Depending upon the assumptions regarding the variations in these parameters, the results are only sometimes consistent with the reports of several orders of magnitude in indoor <span class="hlt">air</span> concentration variations from field studies. The results point to the need to examine more carefully the interplay of these factors in order to quantitatively understand the variations in potential indoor <span class="hlt">air</span> exposures.</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('http://adsabs.harvard.edu/abs/2013ACP....13.5325E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACP....13.5325E"><span><span class="hlt">Air-surface</span> <span class="hlt">exchange</span> measurements of gaseous elemental mercury over naturally enriched and background terrestrial landscapes in Australia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Edwards, G. C.; Howard, D. A.</p> <p>2013-05-01</p> <p>This paper presents the first gaseous elemental mercury (GEM) <span class="hlt">air-surface</span> <span class="hlt">exchange</span> measurements obtained over naturally enriched and background (<0.1 μg g-1 Hg) terrestrial landscapes in Australia. Two pilot field studies were carried out during the Australian autumn and winter periods at a copper-gold-cobalt-arsenic-mercury mineral field near Pulganbar, NSW. GEM fluxes using a dynamic flux chamber approach were measured, along with controlling environmental parameters over three naturally enriched and three background substrates. The enriched sites results showed net emission to the atmosphere and a strong correlation between flux and substrate Hg concentration, with average fluxes ranging from 14 ± 1 ng m-2 h-1 to 113 ± 6 ng m-2 h-1. Measurements at background sites showed both emission and deposition. The average Hg flux from all background sites showed an overall net emission of 0.36 ± 0.06 ng m-2 h-1. Fluxes show strong relationships with temperature, radiation, and substrate parameters. A compensation point of 2.48, representative of bare soils was determined. For periods of deposition, dry deposition velocities ranged from 0.00025 cm s-1 to 0.0083 cm s-1 with an average of 0.0041 ± 0.00018 cm s-1, representing bare soil, nighttime conditions. Comparison of the Australian data to North American data suggests the need for Australian-specific mercury <span class="hlt">air-surface</span> <span class="hlt">exchange</span> data representative of Australia's unique climatic conditions, vegetation types, land use patterns and soils.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JCoPh.271..172N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JCoPh.271..172N"><span>Reprint of: A numerical <span class="hlt">modelling</span> of gas <span class="hlt">exchange</span> mechanisms between <span class="hlt">air</span> and turbulent water with an aquarium chemical reaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagaosa, Ryuichi S.</p> <p>2014-08-01</p> <p>This paper proposes a new numerical <span class="hlt">modelling</span> to examine environmental chemodynamics of a gaseous material <span class="hlt">exchanged</span> between the <span class="hlt">air</span> and turbulent water phases across a gas-liquid interface, followed by an aquarium chemical reaction. This study uses an extended concept of a two-compartment <span class="hlt">model</span>, and assumes two physicochemical substeps to approximate the gas <span class="hlt">exchange</span> processes. The first substep is the gas-liquid equilibrium between the <span class="hlt">air</span> and water phases, A(g)⇌A(aq), with Henry's law constant H. The second is a first-order irreversible chemical reaction in turbulent water, A(aq)+H2O→B(aq)+H+ with a chemical reaction rate κA. A direct numerical simulation (DNS) technique has been employed to obtain details of the gas <span class="hlt">exchange</span> mechanisms and the chemical reaction in the water compartment, while zero velocity and uniform concentration of A is considered in the <span class="hlt">air</span> compartment. The study uses the different Schmidt numbers between 1 and 8, and six nondimensional chemical reaction rates between 10(≈0) to 101 at a fixed Reynolds number. It focuses on the effects of the Schmidt number and the chemical reaction rate on fundamental mechanisms of the gas <span class="hlt">exchange</span> processes across the interface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B34A..02L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B34A..02L"><span><span class="hlt">Air</span>-Water <span class="hlt">Exchange</span> of Legacy and Emerging Organic Pollutants across the Great Lakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lohmann, R.; Ruge, Z.; Khairy, M.; Muir, D.; Helm, P.</p> <p>2014-12-01</p> <p>Organochlorine pesticides (OCPs) and polychlorinated biphenyls (PCBs) are transported to great water bodies via long-range atmospheric transport and released from the <span class="hlt">surface</span> water as <span class="hlt">air</span> concentrations continue to diminish. As the largest fresh water bodies in North America, the Great Lakes have both the potential to accumulate and serve as a secondary source of persistent bioaccumulative toxins. OCP and PCB concentrations were sampled at 30+ sites across Lake Superior, Ontario and Erie in the summer of 2011. Polyethylene passive samplers (PEs) were simultaneously deployed in <span class="hlt">surface</span> water and near <span class="hlt">surface</span> atmosphere to determine <span class="hlt">air</span>-water gaseous <span class="hlt">exchange</span> of OCPs and PCBs. In Lake Superior, <span class="hlt">surface</span> water and atmospheric concentrations were dominated by α-HCH (average 250 pg/L and 4.2 pg/m3, respectively), followed by HCB (average 17 pg/L and 89 pg/m3, respectively). <span class="hlt">Air</span>-water <span class="hlt">exchange</span> varied greatly between sites and individual OCPs, however α-endosulfan was consistently deposited into the <span class="hlt">surface</span> water (average 19 pg/m2/day). PCBs in the <span class="hlt">air</span> and water were characterized by penta- and hexachlorobiphenyls with distribution along the coast correlated with proximity to developed areas. <span class="hlt">Air</span>-water <span class="hlt">exchange</span> gradients generally yielded net volatilization of PCBs out of Lake Superior. Gaseous concentrations of hexachlorobenzene, dieldrin and chlordanes were significantly higher (p < 0.05) at Lake Erie than Lake Ontario. A multiple linear regression that incorporated meteorological, landuse and population data was used to explain variability in the atmospheric concentrations. Results indicated that landuse (urban and/or cropland) greatly explained the variability in the data. Freely dissolved concentrations of OCPs (<LOD-114 pg/L) were lower than previously detected concentrations. Nonetheless, concentrations of p,p'-DDE and chlordanes were higher than water quality guidelines for the protection of human health from the consumption of fish. Spatial distributions of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25386953','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25386953"><span><span class="hlt">Modeling</span> spatial and temporal variability of residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates for the Near-Road Exposures and Effects of Urban <span class="hlt">Air</span> Pollutants Study (NEXUS).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Breen, Michael S; Burke, Janet M; Batterman, Stuart A; Vette, Alan F; Godwin, Christopher; Croghan, Carry W; Schultz, Bradley D; Long, Thomas C</p> <p>2014-11-07</p> <p><span class="hlt">Air</span> pollution health studies often use outdoor concentrations as exposure surrogates. Failure to account for variability of residential infiltration of outdoor pollutants can induce exposure errors and lead to bias and incorrect confidence intervals in health effect estimates. The residential <span class="hlt">air</span> <span class="hlt">exchange</span> rate (AER), which is the rate of <span class="hlt">exchange</span> of indoor <span class="hlt">air</span> with outdoor <span class="hlt">air</span>, is an important determinant for house-to-house (spatial) and temporal variations of <span class="hlt">air</span> pollution infiltration. Our goal was to evaluate and apply mechanistic <span class="hlt">models</span> to predict AERs for 213 homes in the Near-Road Exposures and Effects of Urban <span class="hlt">Air</span> Pollutants Study (NEXUS), a cohort study of traffic-related <span class="hlt">air</span> pollution exposures and respiratory effects in asthmatic children living near major roads in Detroit, Michigan. We used a previously developed <span class="hlt">model</span> (LBL), which predicts AER from meteorology and questionnaire data on building characteristics related to <span class="hlt">air</span> leakage, and an extended version of this <span class="hlt">model</span> (LBLX) that includes natural ventilation from open windows. As a critical and novel aspect of our AER <span class="hlt">modeling</span> approach, we performed a cross validation, which included both parameter estimation (i.e., <span class="hlt">model</span> calibration) and <span class="hlt">model</span> evaluation, based on daily AER measurements from a subset of 24 study homes on five consecutive days during two seasons. The measured AER varied between 0.09 and 3.48 h(-1) with a median of 0.64 h(-1). For the individual <span class="hlt">model</span>-predicted and measured AER, the median absolute difference was 29% (0.19 h‑1) for both the LBL and LBLX <span class="hlt">models</span>. The LBL and LBLX <span class="hlt">models</span> predicted 59% and 61% of the variance in the AER, respectively. Daily AER predictions for all 213 homes during the three year study (2010-2012) showed considerable house-to-house variations from building leakage differences, and temporal variations from outdoor temperature and wind speed fluctuations. Using this novel approach, NEXUS will be one of the first epidemiology studies to apply calibrated and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BGeo...14.5595B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BGeo...14.5595B"><span>Continuous measurement of <span class="hlt">air</span>-water gas <span class="hlt">exchange</span> by underwater 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>Berg, Peter; Pace, Michael L.</p> <p>2017-12-01</p> <p><span class="hlt">Exchange</span> of gases, such as O2, CO2, and CH4, over the <span class="hlt">air</span>-water interface is an important component in aquatic ecosystem studies, but <span class="hlt">exchange</span> rates are typically measured or estimated with substantial uncertainties. This diminishes the precision of common ecosystem assessments associated with gas <span class="hlt">exchanges</span> such as primary production, respiration, and greenhouse gas emission. Here, we used the aquatic eddy covariance technique - originally developed for benthic O2 flux measurements - right below the <span class="hlt">air</span>-water interface (˜ 4 cm) to determine gas <span class="hlt">exchange</span> rates and coefficients. Using an acoustic Doppler velocimeter and a fast-responding dual O2-temperature sensor mounted on a floating platform the 3-D water velocity, O2 concentration, and temperature were measured at high-speed (64 Hz). By combining these data, concurrent vertical fluxes of O2 and heat across the <span class="hlt">air</span>-water interface were derived, and gas <span class="hlt">exchange</span> coefficients were calculated from the former. Proof-of-concept deployments at different river sites gave standard gas <span class="hlt">exchange</span> coefficients (k600) in the range of published values. A 40 h long deployment revealed a distinct diurnal pattern in <span class="hlt">air</span>-water <span class="hlt">exchange</span> of O2 that was controlled largely by physical processes (e.g., diurnal variations in <span class="hlt">air</span> temperature and associated <span class="hlt">air</span>-water heat fluxes) and not by biological activity (primary production and respiration). This physical control of gas <span class="hlt">exchange</span> can be prevalent in lotic systems and adds uncertainty to assessments of biological activity that are based on measured water column O2 concentration changes. For example, in the 40 h deployment, there was near-constant river flow and insignificant winds - two main drivers of lotic gas <span class="hlt">exchange</span> - but we found gas <span class="hlt">exchange</span> coefficients that varied by several fold. This was presumably caused by the formation and erosion of vertical temperature-density gradients in the <span class="hlt">surface</span> water driven by the heat flux into or out of the river that affected the turbulent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=62405&keyword=FAN&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=62405&keyword=FAN&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>FACTORS AFFECTING <span class="hlt">AIR</span> <span class="hlt">EXCHANGE</span> IN TWO HOUSES</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><span class="hlt">Air</span> <span class="hlt">exchange</span> rate is critical to determining the relationship between indoor and outdoor concentrations of hazardous pollutants. Approximately 150 <span class="hlt">air</span> <span class="hlt">exchange</span> experiments were completed in two residences: a two-story detached house located in Redwood City, CA and a three-story...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=59799&keyword=Exchange+AND+gaseous&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=59799&keyword=Exchange+AND+gaseous&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>THE EFFECT OF SALINITY ON RATES OF ELEMENTAL MERCURY <span class="hlt">AIR</span>/WATER <span class="hlt">EXCHANGE</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>The U.S. EPA laboratory in Athens, Georgia i spursuing the goal of developing a <span class="hlt">model</span> for describing toxicant vapor phase <span class="hlt">air</span>/water <span class="hlt">exchange</span> under all relevant environmental conditions. To date, the two-layer <span class="hlt">exchange</span> <span class="hlt">model</span> (suitable for low wind speed conditions) has been modif...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20000740-coupling-phytoplankton-uptake-air-water-exchange-persistent-organic-pollutants','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20000740-coupling-phytoplankton-uptake-air-water-exchange-persistent-organic-pollutants"><span>Coupling of phytoplankton uptake and <span class="hlt">air</span>-water <span class="hlt">exchange</span> of persistent organic pollutants</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>Dachs, J.; Eisenreich, S.J.; Baker, J.E.</p> <p>1999-10-15</p> <p>A dynamic <span class="hlt">model</span> that couples <span class="hlt">air</span>-water <span class="hlt">exchange</span> and phytoplankton uptake of persistent organic pollutants has been developed and then applied to PCB data from a small experimental lake. A sensitivity analysis of the <span class="hlt">model</span>, taking into account the influence of physical environmental conditions such as temperature, wind speed, and mixing depth as well as plankton-related parameters such as biomass and growth rate was carried out for a number of PCBs with different physical-chemical properties. The results indicate that <span class="hlt">air</span>-water <span class="hlt">exchange</span> dynamics are influenced not only by physical parameters but also by phytoplankton biomass and growth rate. New phytoplankton production resultsmore » in substantially longer times to reach equilibrium. Phytoplankton uptake-induced depletion of the dissolved phase concentration maintains <span class="hlt">air</span> and water phases out of equilibrium. Furthermore, PCBs in phytoplankton also take longer times to reach equilibrium with the dissolved water phase when the latter is supported by diffusive <span class="hlt">air</span>-water <span class="hlt">exchange</span>. However, both <span class="hlt">model</span> analysis and <span class="hlt">model</span> application to the Experimental Lakes Area of northwestern Ontario (Canada) suggest that the gas phase supports the concentrations of persistent organic pollutants, such as PCBs, in atmospherically driven aquatic environments.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA615405','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA615405"><span>Forecasting Foreign Currency <span class="hlt">Exchange</span> Rates for <span class="hlt">Air</span> Force Budgeting</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-03-26</p> <p>FORECASTING FOREIGN CURRENCY <span class="hlt">EXCHANGE</span> RATES FOR <span class="hlt">AIR</span> FORCE BUDGETING THESIS MARCH 2015...States. AFIT-ENV-MS-15-M-178 FORECASTING FOREIGN CURRENCY <span class="hlt">EXCHANGE</span> RATES FOR <span class="hlt">AIR</span> FORCE BUDGETING THESIS Presented to the Faculty...FORECASTING FOREIGN CURRENCY <span class="hlt">EXCHANGE</span> RATES FOR <span class="hlt">AIR</span> FORCE BUDGETING Nicholas R. Gardner, BS Captain, USAF Committee Membership: Lt Col Jonathan</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21700320','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21700320"><span>Assessing the ability of mechanistic volatilization <span class="hlt">models</span> to simulate soil <span class="hlt">surface</span> conditions: a study with the Volt'<span class="hlt">Air</span> <span class="hlt">model</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Garcia, L; Bedos, C; Génermont, S; Braud, I; Cellier, P</p> <p>2011-09-01</p> <p>Ammonia and pesticide volatilization in the field is a <span class="hlt">surface</span> phenomenon involving physical and chemical processes that depend on the soil <span class="hlt">surface</span> temperature and water content. The water transfer, heat transfer and energy budget sub <span class="hlt">models</span> of volatilization <span class="hlt">models</span> are adapted from the most commonly accepted formalisms and parameterizations. They are less detailed than the dedicated <span class="hlt">models</span> describing water and heat transfers and <span class="hlt">surface</span> status. The aim of this work was to assess the ability of one of the available mechanistic volatilization <span class="hlt">models</span>, Volt'<span class="hlt">Air</span>, to accurately describe the pedo-climatic conditions of a soil <span class="hlt">surface</span> at the required time and space resolution. The assessment involves: (i) a sensitivity analysis, (ii) an evaluation of Volt'<span class="hlt">Air</span> outputs in the light of outputs from a reference Soil-Vegetation-Atmosphere Transfer <span class="hlt">model</span> (SiSPAT) and three experimental datasets, and (iii) the study of three tests based on modifications of SiSPAT to establish the potential impact of the simplifying assumptions used in Volt'<span class="hlt">Air</span>. The analysis confirmed that a 5 mm <span class="hlt">surface</span> layer was well suited, and that Volt'<span class="hlt">Air</span> <span class="hlt">surface</span> temperature correlated well with the experimental measurements as well as with SiSPAT outputs. In terms of liquid water transfers, Volt'<span class="hlt">Air</span> was overall consistent with SiSPAT, with discrepancies only during major rainfall events and dry weather conditions. The tests enabled us to identify the main source of the discrepancies between Volt'<span class="hlt">Air</span> and SiSPAT: the lack of gaseous water transfer description in Volt'<span class="hlt">Air</span>. They also helped to explain why neither Volt'<span class="hlt">Air</span> nor SiSPAT was able to represent lower values of <span class="hlt">surface</span> water content: current classical water retention and hydraulic conductivity <span class="hlt">models</span> are not yet adapted to cases of very dry conditions. Given the outcomes of this study, we discuss to what extent the volatilization <span class="hlt">models</span> can be improved and the questions they pose for current research in water transfer <span class="hlt">modeling</span> and parameterization</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21069949','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21069949"><span>Predicting residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates from questionnaires and meteorology: <span class="hlt">model</span> evaluation in central North Carolina.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Breen, Michael S; Breen, Miyuki; Williams, Ronald W; Schultz, Bradley D</p> <p>2010-12-15</p> <p>A critical aspect of <span class="hlt">air</span> pollution exposure <span class="hlt">models</span> is the estimation of the <span class="hlt">air</span> <span class="hlt">exchange</span> rate (AER) of individual homes, where people spend most of their time. The AER, which is the airflow into and out of a building, is a primary mechanism for entry of outdoor <span class="hlt">air</span> pollutants and removal of indoor source emissions. The mechanistic Lawrence Berkeley Laboratory (LBL) AER <span class="hlt">model</span> was linked to a leakage area <span class="hlt">model</span> to predict AER from questionnaires and meteorology. The LBL <span class="hlt">model</span> was also extended to include natural ventilation (LBLX). Using literature-reported parameter values, AER predictions from LBL and LBLX <span class="hlt">models</span> were compared to data from 642 daily AER measurements across 31 detached homes in central North Carolina, with corresponding questionnaires and meteorological observations. Data was collected on seven consecutive days during each of four consecutive seasons. For the individual <span class="hlt">model</span>-predicted and measured AER, the median absolute difference was 43% (0.17 h(-1)) and 40% (0.17 h(-1)) for the LBL and LBLX <span class="hlt">models</span>, respectively. Additionally, a literature-reported empirical scale factor (SF) AER <span class="hlt">model</span> was evaluated, which showed a median absolute difference of 50% (0.25 h(-1)). The capability of the LBL, LBLX, and SF <span class="hlt">models</span> could help reduce the AER uncertainty in <span class="hlt">air</span> pollution exposure <span class="hlt">models</span> used to develop exposure metrics for health studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150018068','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150018068"><span>National <span class="hlt">Air</span> Space (NAS) Data <span class="hlt">Exchange</span> Environment Through 2060</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roy, Aloke</p> <p>2015-01-01</p> <p>NASA's NextGen Concepts and Technology Development (CTD) Project focuses on capabilities to improve safety, capacity and efficiency of the National <span class="hlt">Air</span> Space (NAS). In order to achieve those objectives, NASA sought industry-Government partnerships to research and identify solutions for traffic flow management, dynamic airspace configuration, separation assurance, super density operations, airport <span class="hlt">surface</span> operations and similar forward-looking <span class="hlt">air</span>-traffic modernization (ATM) concepts. Data <span class="hlt">exchanges</span> over NAS being the key enabler for most of these ATM concepts, the Sub-Topic area 3 of the CTD project sought to identify technology candidates that can satisfy <span class="hlt">air-to-air</span> and <span class="hlt">air</span>/ground communications needs of the NAS in the year 2060 timeframe. Honeywell, under a two-year contract with NASA, is working on this communications technology research initiative. This report summarizes Honeywell's research conducted during the second year of the study task.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12806145','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12806145"><span>Mercury <span class="hlt">exchange</span> at the <span class="hlt">air</span>-water-soil interface: an overview of methods.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fang, Fengman; Wang, Qichao; Liu, Ruhai</p> <p>2002-06-12</p> <p>An attempt is made to assess the present knowledge about the methods of determining mercury (Hg) <span class="hlt">exchange</span> at the <span class="hlt">air</span>-water-soil interface during the past 20 years. Methods determining processes of wet and dry removal/deposition of atmospheric Hg to aquatic and terrestrial ecosystems, as well as methods determining Hg emission fluxes to the atmosphere from natural <span class="hlt">surfaces</span> (soil and water) are discussed. On the basis of the impressive advances that have been made in the areas relating to Hg <span class="hlt">exchange</span> among <span class="hlt">air</span>-soil-water interfaces, we analyzed existing problems and shortcomings in our current knowledge. In addition, some important fields worth further research are discussed and proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930036604&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DCO2%2BH2O','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930036604&hterms=CO2+H2O&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DCO2%2BH2O"><span><span class="hlt">Air-surface</span> <span class="hlt">exchange</span> of H2O, CO2, and O3 at a tallgrass prairie in relation to remotely sensed vegetation indices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gao, W.; Wesely, M. L.; Cook, D. R.; Hart, R. L.</p> <p>1992-01-01</p> <p>Parameters derived from eddy correlation measurements of the <span class="hlt">air-surface</span> <span class="hlt">exchange</span> rates of H2O, CO2, and O3 over a tallgrass prairie are examined in terms of their relationships with spectral reflectance data remotely sensed from aircraft and satellites during the four 1987 intensive field campaigns of the First ISLSCP Field Experiment (FIFE). The <span class="hlt">surface</span> conductances were strongly modulated by photosynthetically active radiation received at the <span class="hlt">surface</span> when the grass was green and well watered; mesophyll resistances were large for CO2 but negligible for H2O and O3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308472&Lab=NERL&keyword=simulation+AND+processes&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=308472&Lab=NERL&keyword=simulation+AND+processes&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>Development and Evaluation of a New <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate Algorithm for the Stochastic Human Exposure and Dose Simulation <span class="hlt">Model</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>between-home and between-city variability in residential pollutant infiltration. This is likely a result of differences in home ventilation, or <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AER). The Stochastic Human Exposure and Dose Simulation (SHEDS) <span class="hlt">model</span> is a population exposure <span class="hlt">model</span> that uses a pro...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12095811','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12095811"><span>Effects of humidified and dry <span class="hlt">air</span> on corneal endothelial cells during vitreal fluid-<span class="hlt">air</span> <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cekiç, Osman; Ohji, Masahito; Hayashi, Atsushi; Fang, Xiao Y; Kusaka, Shunji; Tano, Yasuo</p> <p>2002-07-01</p> <p>To report the immediate anatomic and functional alterations in corneal endothelial cells following use of humidified <span class="hlt">air</span> and dry <span class="hlt">air</span> during vitreal fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> in rabbits. Experimental study. Rabbits undergoing pars plana vitrectomy and lensectomy were perfused with either dry or humidified <span class="hlt">air</span> during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> for designated durations. Three different experiments were performed. First, control and experimental corneas were examined by scanning electron microscopy (SEM). Second, corneas were stained with Phalloidin-FITC and examined by fluorescein microscopy. Finally, third, transendothelial permeability for carboxyfluorescein was determined using a diffusion chamber. While different from the corneal endothelial cells, those cells exposed to humidified <span class="hlt">air</span> were less stressed than cells exposed to dry <span class="hlt">air</span> by SEM. Actin cytoskeleton was found highly disorganized with dry <span class="hlt">air</span> exposure. Humidified <span class="hlt">air</span> maintained the normal actin cytoskeleton throughout the 20 minutes of fluid-<span class="hlt">air</span> <span class="hlt">exchange</span>. Paracellular carboxyfluorescein leakage was significantly higher in dry <span class="hlt">air</span> insufflated eyes compared with that of the humidified <span class="hlt">air</span> after 5, 10, and 20 minutes of fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> (P =.002, P =.004, and P =.002, respectively). Dry <span class="hlt">air</span> stress during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> causes significant immediate alterations in monolayer appearance, actin cytoskeleton, and barrier function of corneal endothelium in aphakic rabbit eyes. Use of humidified <span class="hlt">air</span> largely prevents the alterations in monolayer appearance, actin cytoskeleton, and barrier function of corneal endothelial cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMOS31B1280P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMOS31B1280P"><span>Micrometeorological Measurement of Fetch- and Atmospheric Stability-Dependent <span class="hlt">Air</span>- Water <span class="hlt">Exchange</span> of Legacy Semivolatile Organic Contaminants in Lake Superior</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Perlinger, J. A.; Tobias, D. E.; Rowe, M. D.</p> <p>2008-12-01</p> <p>Coastal waters including the Laurentian Great Lakes are particularly susceptible to local, regional, and long- range transport and deposition of semivolatile organic contaminants (SOCs) as gases and/or associated with particles. Recently-marketed SOCs can be expected to undergo net deposition in <span class="hlt">surface</span> waters, whereas legacy SOCs such as polychlorinated biphenyls (PCBs) are likely to be at equilibrium with respect to <span class="hlt">air</span>-water <span class="hlt">exchange</span>, or, if atmospheric concentrations decrease through, e.g., policy implementation, to undergo net gas emission. SOC <span class="hlt">air</span>-water <span class="hlt">exchange</span> flux is usually estimated using the two-film <span class="hlt">model</span>. This <span class="hlt">model</span> describes molecular diffusion through the <span class="hlt">air</span> and water films adjacent to the <span class="hlt">air</span>-water interface. <span class="hlt">Air</span>-water <span class="hlt">exchange</span> flux is estimated as the product of SOC fugacity, typically based on on-shore gaseous concentration measurements, and a transfer coefficient, the latter which is estimated from SOC properties and environmental conditions. The transfer coefficient formulation commonly applied neglects resistance to <span class="hlt">exchange</span> in the internal boundary layer under atmospherically stable conditions, and the use of on-shore gaseous concentration neglects fetch-dependent equilibration, both of which will tend to cause overestimation of flux magnitude. Thus, for legacy chemicals or in any highly contaminated <span class="hlt">surface</span> water, the rate at which the water is cleansed through gas emission tends to be over-predicted using this approach. Micrometeorological measurement of <span class="hlt">air</span>-water <span class="hlt">exchange</span> rates of legacy SOCs was carried out on ships during four transect experiments during off-shore flow in Lake Superior using novel multicapillary collection devices and thermal extraction technology to measure parts-per-quadrillion SOC levels. Employing sensible heat in the modified Bowen ratio, fluxes at three over-water stations along the transects were measured, along with up-wind, onshore gaseous concentration and aqueous concentration. The atmosphere was unstable for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.ars.usda.gov/research/publications/publication/?seqNo115=328803','TEKTRAN'); return false;" href="http://www.ars.usda.gov/research/publications/publication/?seqNo115=328803"><span>Impacts of differing aerodynamic resistance formulae on <span class="hlt">modeled</span> energy <span class="hlt">exchange</span> at the above-canopy/within-canopy/soil interface</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>Application of the Two-Source Energy Balance (TSEB) <span class="hlt">Model</span> using land <span class="hlt">surface</span> temperature (LST) requires aerodynamic resistance parameterizations for the flux <span class="hlt">exchange</span> above the canopy layer, within the canopy <span class="hlt">air</span> space and at the soil/substrate <span class="hlt">surface</span>. There are a number of aerodynamic resistance f...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A11A1877F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A11A1877F"><span>Global Validation of MODIS Atmospheric Profile-Derived Near-<span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature and Dew Point Estimates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Famiglietti, C.; Fisher, J.; Halverson, G. H.</p> <p>2017-12-01</p> <p>This study validates a method of remote sensing near-<span class="hlt">surface</span> meteorology that vertically interpolates MODIS atmospheric profiles to <span class="hlt">surface</span> pressure level. The extraction of <span class="hlt">air</span> temperature and dew point observations at a two-meter reference height from 2001 to 2014 yields global moderate- to fine-resolution near-<span class="hlt">surface</span> temperature distributions that are compared to geographically and temporally corresponding measurements from 114 ground meteorological stations distributed worldwide. This analysis is the first robust, large-scale validation of the MODIS-derived near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature and dew point estimates, both of which serve as key inputs in <span class="hlt">models</span> of energy, water, and carbon <span class="hlt">exchange</span> between the land <span class="hlt">surface</span> and the atmosphere. Results show strong linear correlations between remotely sensed and in-situ near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements (R2 = 0.89), as well as between dew point observations (R2 = 0.77). Performance is relatively uniform across climate zones. The extension of mean climate-wise percent errors to the entire remote sensing dataset allows for the determination of MODIS <span class="hlt">air</span> temperature and dew point uncertainties on a global scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998PhDT........22V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998PhDT........22V"><span>Photochemical influences on the <span class="hlt">air</span>-water <span class="hlt">exchange</span> of mercury</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vette, Alan Frederic</p> <p></p> <p>The formation of dissolved gaseous mercury (DGM) in natural waters is an important component in the biogeochemical cycle of mercury (Hg). The predominate form of DGM in natural waters, gaseous elemental Hg (Hg0), may be transferred from the water to the atmosphere. Gas <span class="hlt">exchange</span> may reduce the amount of Hg available for methyl-Hg formation, the most toxic form of Hg that bioaccumulates in the food chain. Determining the mechanisms and rates of DGM formation is essential in understanding the fate and cycling of Hg in aquatic ecosystems. Field and laboratory experiments were conducted to evaluate the effect of light on DGM formation in <span class="hlt">surface</span> waters containing different levels of dissolved organic carbon (DOC). Water samples collected from the Tahqwamenon River and Whitefish Bay on Lake Superior were amended with divalent Hg (Hg2+) and irradiated under a variety of reaction conditions to determine rates of DGM formation. The water samples were also analyzed for various Hg species (total, filtered, easily reducible and dissolved gaseous Hg), DOC and light attenuation. Additional field studies were conducted on Lake Michigan to measure gaseous Hg in <span class="hlt">air</span> and water. These data were used to develop a mechanistic <span class="hlt">model</span> to estimate <span class="hlt">air</span>-water <span class="hlt">exchange</span> of gaseous Hg. This research found that photochemical formation of DGM was affected by penetration of UV A radiation (320-400 nm). Formation of DGM was enhanced at higher DOC concentrations, indicating DOC photosensitized the reduction of Hg2+ to Hg0. Wavelength studies determined that formation of DGM was significantly reduced in the absence of UV A. Field studies showed DGM concentrations were highest near the water <span class="hlt">surface</span> and peaked at mid-day, indicating a photo-induced source of DGM. The conversion of reducible Hg2+ to Hg0 was suppressed in high DOC waters where UV A penetration was limited. The mechanistic <span class="hlt">model</span> predicted similar DGM concentrations to the observed values and demonstrated that deposition and emission</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('https://www.ncbi.nlm.nih.gov/pubmed/24047550','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24047550"><span>Polycyclic aromatic hydrocarbons in <span class="hlt">surface</span> soil across the Tibetan Plateau: spatial distribution, source and <span class="hlt">air</span>-soil <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Chuanfei; Wang, Xiaoping; Gong, Ping; Yao, Tandong</p> <p>2014-01-01</p> <p>There are limited data on polycyclic aromatic hydrocarbons (PAHs) in both the atmosphere and soil of the Tibetan Plateau (TP). Concentrations of PAHs were therefore measured in 13 XAD resin-based passive <span class="hlt">air</span> samplers and 41 <span class="hlt">surface</span> (0-5 cm) soil samples across the TP. The average concentration of atmospheric PAHs was 5.55 ng/m(3), which was lower than that reported for other background areas, but higher than the Arctic. Concentrations in the soils fell in a wide range from 5.54 to 389 ng/g, with an average of 59.9 ng/g. Elevation was found to play an important role in determining the spatial distribution of soil PAHs. The <span class="hlt">air</span>-soil <span class="hlt">exchange</span> state showed that the soils of the TP will likely remain as a sink for high molecular weight PAHs, but may become a potential "secondary source" for low molecular weight PAHs. Copyright © 2013 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18754367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18754367"><span><span class="hlt">Modeling</span> dynamic <span class="hlt">exchange</span> of gaseous elemental mercury at polar sunrise.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dastoor, Ashu P; Davignon, Didier; Theys, Nicolas; Van Roozendael, Michel; Steffen, Alexandra; Ariya, Parisa A</p> <p>2008-07-15</p> <p>At polar sunrise, gaseous elemental mercury (GEM) undergoes an exceptional dynamic <span class="hlt">exchange</span> in the <span class="hlt">air</span> and at the snow <span class="hlt">surface</span> during which GEM can be rapidly removed from the atmosphere (the so-called atmospheric mercury depletion events (AMDEs)) as well as re-emitted from the snow within a few hours to days in the Polar Regions. Although high concentrations of total mercury in snow following AMDEs is well documented, there is very little data available on the redox transformation processes of mercury in the snow and the fluxes of mercury at the <span class="hlt">air</span>/snow interface. Therefore, the net gain of mercury in the Polar Regions as a result of AMDEs is still an open question. We developed a new version of the global mercury <span class="hlt">model</span>, GRAHM, which includes for the first time bidirectional <span class="hlt">surface</span> <span class="hlt">exchange</span> of GEM in Polar Regions in spring and summer by developing schemes for mercury halogen oxidation, deposition, and re-emission. Also for the first time, GOME satellite data-derived boundary layer concentrations of BrO have been used in a global mercury <span class="hlt">model</span> for representation of halogen mercury chemistry. Comparison of <span class="hlt">model</span> simulated and measured atmospheric concentrations of GEM at Alert, Canada, for 3 years (2002-2004) shows the <span class="hlt">model</span>'s capability in simulating the rapid cycling of mercury during and after AMDEs. Brooks et al. (1) measured mercury deposition, reemission, and net <span class="hlt">surface</span> gain fluxes of mercury at Barrow, AK, during an intensive measurement campaign for a 2 week period in spring (March 25 to April 7, 2003). They reported 1.7, 1.0 +/- 0.2, and 0.7 +/- 0.2 microg m(-2) deposition, re-emission, and net <span class="hlt">surface</span> gain, respectively. Using the optimal configuration of the <span class="hlt">model</span>, we estimated 1.8 microg m(-2) deposition, 1.0 microg m(-2) re-emission, and 0.8 microg m(-2) net <span class="hlt">surface</span> gain of mercury for the same time period at Barrow. The estimated net annual accumulation of mercury within the Arctic Circle north of 66.5 degrees is approximately 174 t with +/-7 t of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38.3367R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38.3367R"><span><span class="hlt">Air</span> Circulation and Heat <span class="hlt">Exchange</span> under Reduced Pressures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rygalov, Vadim; Wheeler, Raymond; Dixon, Mike; Hillhouse, Len; Fowler, Philip</p> <p></p> <p>Low pressure atmospheres were suggested for Space Greenhouses (SG) design to minimize sys-tem construction and re-supply materials, as well as system manufacturing and deployment costs. But rarified atmospheres modify heat <span class="hlt">exchange</span> mechanisms what finally leads to alter-ations in thermal control for low pressure closed environments. Under low atmospheric pressures (e.g., lower than 25 kPa compare to 101.3 kPa for normal Earth atmosphere), convection is becoming replaced by diffusion and rate of heat <span class="hlt">exchange</span> reduces significantly. During a period from 2001 to 2009, a series of hypobaric experiments were conducted at Space Life Sciences Lab (SLSLab) NASA's Kennedy Space Center and the Department of Space Studies, University of North Dakota. Findings from these experiments showed: -<span class="hlt">air</span> circulation rate decreases non-linearly with lowering of total atmospheric pressure; -heat <span class="hlt">exchange</span> slows down with pressure decrease creating risk of thermal stress (elevated leaf tem-peratures) for plants in closed environments; -low pressure-induced thermal stress could be reduced by either lowering system temperature set point or increasing forced convection rates (circulation fan power) within certain limits; <span class="hlt">Air</span> circulation is an important constituent of controlled environments and plays crucial role in material and heat <span class="hlt">exchange</span>. Theoretical schematics and mathematical <span class="hlt">models</span> are developed from a series of observations. These <span class="hlt">models</span> can be used to establish optimal control algorithms for low pressure environments, such as a space greenhouse, as well as assist in fundamental design concept developments for these or similar habitable structures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28675863','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28675863"><span>Polychlorinated biphenyls in Nepalese <span class="hlt">surface</span> soils: Spatial distribution, <span class="hlt">air</span>-soil <span class="hlt">exchange</span>, and soil-<span class="hlt">air</span> partitioning.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yadav, Ishwar Chandra; Devi, Ningombam Linthoingambi; Li, Jun; Zhang, Gan</p> <p>2017-10-01</p> <p>Regardless of the ban on the polychlorinated biphenyls (PCBs) decade ago, significant measures of PCBs are still transmitted from essential sources in cities and are all inclusive ecological contaminants around the world. In this study, the concentrations of PCBs in soil, the <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of PCBs, and the soil-<span class="hlt">air</span> partitioning coefficient (K SA ) of PCBs were investigated in four noteworthy urban areas in Nepal. Overall, the concentrations of ∑ 30 PCBs ranged from 10 to 59.4ng/g dry weight; dw (mean 12.2ng/g ±11.2ng/g dw). The hexa-CBs (22-31%) was most dominant among several PCB-homologues, followed by tetra-CBs (20-29%), hepta-CBs (12-21%), penta-CBs (15-17%) and tri-CBs (9-19%). The sources of elevated level of PCBs discharge in Nepalese soil was identified as emission from transformer oil, lubricants, breaker oil, cutting oil and paints, and cable insulation. Slightly strong correlation of PCBs with TOC than BC demonstrated that amorphous organic matter (AOM) assumes a more critical part in holding of PCBs than BC in Nepalese soil. The fugacity fraction (ff) results indicated the soil being the source of PCB in <span class="hlt">air</span> through volatilization and net transport from soil to <span class="hlt">air</span>. The soil-<span class="hlt">air</span> partitioning coefficient study suggests the absorption by soil organic matter control soil-<span class="hlt">air</span> partitioning of PCBs. Slightly weak but positive correlation of measured Log K SA with Log K OA (R 2 = 0.483) and Log K BC-A (R 2 = 0.438) suggests that both Log K OA and Log K BC-A can predict soil-<span class="hlt">air</span> partitioning to lesser extent for PCBs. Copyright © 2017 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2013-08-14/pdf/2013-19756.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2013-08-14/pdf/2013-19756.pdf"><span>78 FR 49484 - <span class="hlt">Exchange</span> of <span class="hlt">Air</span> Force Real Property for Non-<span class="hlt">Air</span> Force Real Property</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2013-08-14</p> <p>... DEPARTMENT OF DEFENSE Department of <span class="hlt">Air</span> Force <span class="hlt">Exchange</span> of <span class="hlt">Air</span> Force Real Property for Non-<span class="hlt">Air</span> Force Real Property SUMMARY: Notice identifies excess Federal real property under administrative jurisdiction of the United States <span class="hlt">Air</span> Force it intends to <span class="hlt">exchange</span> for real property not currently owned by the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGD....10.8415S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGD....10.8415S"><span>Biology and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> controls on the distribution of carbon isotope ratios (δ13C) in the ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmittner, A.; Gruber, N.; Mix, A. C.; Key, R. M.; Tagliabue, A.; Westberry, T. K.</p> <p>2013-05-01</p> <p>Analysis of observations and sensitivity experiments with a new three-dimensional global <span class="hlt">model</span> of stable carbon isotope cycling elucidate the processes that control the distribution of δ13C in the contemporary and preindustrial ocean. Biological fractionation dominates the distribution of δ13CDIC of dissolved inorganic carbon (DIC) due to the sinking of isotopically light δ13C organic matter from the <span class="hlt">surface</span> into the interior ocean. This process leads to low δ13CDIC values at dephs and in high latitude <span class="hlt">surface</span> waters and high values in the upper ocean at low latitudes with maxima in the subtropics. <span class="hlt">Air</span>-sea gas <span class="hlt">exchange</span> provides an important secondary influence due to two effects. First, it acts to reduce the spatial gradients created by biology. Second, the associated temperature dependent fractionation tends to increase (decrease) δ13CDIC values of colder (warmer) water, which generates gradients that oppose those arising from biology. Our <span class="hlt">model</span> results suggest that both effects are similarly important in influencing <span class="hlt">surface</span> and interior δ13CDIC distributions. However, <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> is slow, so biological effect dominate spatial δ13CDIC gradients both in the interior and at the <span class="hlt">surface</span>, in constrast to conclusions from some previous studies. Analysis of a new synthesis of δ13CDIC measurements from years 1990 to 2005 is used to quantify preformed (δ13Cpre) and remineralized (δ13Crem) contributions as well as the effects of biology (Δδ13Cbio) and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> (δ13C*). The <span class="hlt">model</span> reproduces major features of the observed large-scale distribution of δ13CDIC, δ13Cpre, δ13Crem, δ13C*, and Δδ13Cbio. Residual misfits are documented and analyzed. Simulated <span class="hlt">surface</span> and subsurface δ13CDIC are influenced by details of the ecosystem <span class="hlt">model</span> formulation. For example, inclusion of a simple parameterization of iron limitation of phytoplankton growth rates and temperature-dependent zooplankton grazing rates improves the agreement with δ13CDIC</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28303599','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28303599"><span>Impact of <span class="hlt">surface</span> ozone interactions on indoor <span class="hlt">air</span> chemistry: A <span class="hlt">modeling</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kruza, M; Lewis, A C; Morrison, G C; Carslaw, N</p> <p>2017-09-01</p> <p>An INdoor <span class="hlt">air</span> Detailed Chemical <span class="hlt">Model</span> was developed to investigate the impact of ozone reactions with indoor <span class="hlt">surfaces</span> (including occupants), on indoor <span class="hlt">air</span> chemistry in simulated apartments subject to ambient <span class="hlt">air</span> pollution. The results are consistent with experimental studies showing that approximately 80% of ozone indoors is lost through deposition to <span class="hlt">surfaces</span>. The human body removes ozone most effectively from indoor <span class="hlt">air</span> per square meter of <span class="hlt">surface</span>, but the most significant <span class="hlt">surfaces</span> for C 6 -C 10 aldehyde formation are soft furniture and painted walls owing to their large internal <span class="hlt">surfaces</span>. Mixing ratios of between 8 and 11 ppb of C 6 -C 10 aldehydes are predicted to form in apartments in various locations in summer, the highest values are when ozone concentrations are enhanced outdoors. The most important aldehyde formed indoors is predicted to be nonanal (5-7 ppb), driven by oxidation-derived emissions from painted walls. In addition, ozone-derived emissions from human skin were estimated for a small bedroom at nighttime with concentrations of nonanal, decanal, and 4-oxopentanal predicted to be 0.5, 0.7, and 0.7 ppb, respectively. A detailed chemical analysis shows that ozone-derived <span class="hlt">surface</span> aldehyde emissions from materials and people change chemical processing indoors, through enhanced formation of nitrated organic compounds and decreased levels of oxidants. © 2017 The Authors. Indoor <span class="hlt">Air</span> Published by John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980Tell...32..470H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980Tell...32..470H"><span>Gas <span class="hlt">exchange</span> across the <span class="hlt">air</span>-sea interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hasse, L.; Liss, P. S.</p> <p>1980-10-01</p> <p>The physics of gas <span class="hlt">exchange</span> at the <span class="hlt">air</span>-sea interface are reviewed. In order to describe the transfer of gases in the liquid near the boundary, a molecular plus eddy diffusivity concept is used, which has been found useful for smooth flow over solid <span class="hlt">surfaces</span>. From consideration of the boundary conditions, a similar dependence of eddy diffusivity on distance from the interface can be derived for the flow beneath a gas/liquid interface, at least in the absence of waves. The influence of waves is then discussed. It is evident from scale considerations that the effect of gravity waves is small. It is known from wind tunnel work that capillary waves enhance gas transfer considerably. The existing hypotheses are apparently not sufficient to explain the observations. Examination of field data is even more frustrating since the data do not show the expected increase of gas <span class="hlt">exchange</span> with wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010APS..MART14015Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010APS..MART14015Y"><span>Designing Energy-Efficient Heat <span class="hlt">Exchangers</span>--- Creating Micro-Channels on the Aluminum Fin <span class="hlt">Surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ying, Jia; Sommers, Andrew; Eid, Khalid</p> <p>2010-03-01</p> <p>In this research, a method for patterning micro-channels on aluminum <span class="hlt">surfaces</span> is described for the purpose of exploiting those features to affect the <span class="hlt">surface</span> wettability. Minimizing water retention on aluminum is important in the design of energy-efficient heat <span class="hlt">exchangers</span> because water retention can deteriorate the performance of such devices. It increases the <span class="hlt">air</span>-side pressure drop and can decrease the sensible heat transfer coefficient thereby increasing energy consumption and contributing to higher pollution levels in the environment. Photolithography is used to create the micro-scale channels and a hydrophobic polymer is used to reduce the <span class="hlt">surface</span> energy of the aluminum plates. Droplets are both injected on the <span class="hlt">surface</span> using a micro-syringe and condensed on the <span class="hlt">surface</span> using an environmentally-controlled chamber. A ram'e-hart goniometer is used to determine the advancing and receding contact angles of water droplets on these modified <span class="hlt">surfaces</span>, and a tilt-table assembly is used to measure the critical inclination angle for sliding. Our results show that droplets placed on these patterned <span class="hlt">surfaces</span> not only have significantly lower critical inclination angles for sliding but are easier to remove from the <span class="hlt">surface</span> at low <span class="hlt">air</span> flow rates. Efforts to <span class="hlt">model</span> the onset of droplet movement on these <span class="hlt">surfaces</span> using a simple force balance relationship are currently underway.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A43C0283L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A43C0283L"><span><span class="hlt">Air</span>-sea <span class="hlt">Exchange</span> of Polycyclic Aromatic Hydrocarbons (PAHs), Polychlorinated Biphenyls (PCBs), Organochlorine Pesticides (OCPs) and Polybrominated Diphenyl Ethers (PBDEs) in the Mediterranean Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lammel, G. P.; Heil, A.; Kukucka, P.; Meixner, F. X.; Mulder, M. D.; Prybilova, P.; Prokes, R.; Rusina, T. S.; Song, G. Z.; Vrana, B.</p> <p>2015-12-01</p> <p>The marine atmospheric environment is a receptor for persistent organic pollutants (POPs) which are advected from sources on land, primary, such as biomass burning by-products (PAHs, dioxins), and secondary, such as volatilization from contaminated soils (PCBs, pesticides). Primary sources do not exist in the marine environment, except for PAHs (ship engines) but following previous atmospheric deposition, the sea <span class="hlt">surface</span> may turn to a secondary source by reversal of diffusive <span class="hlt">air</span>-sea mass <span class="hlt">exchange</span>. No monitoring is in place. We studied the vertical fluxes of a wide range of primary and secondary emitted POPs based on measurements in <span class="hlt">air</span> and <span class="hlt">surface</span> seawater at a remote coastal site in the eastern Mediterranean (2012). To this end, silicon rubbers were used as passive water samplers, vertical concentration gradients were determined in <span class="hlt">air</span> and fluxes were quantified based on Eddy covariance. Diffusive <span class="hlt">air</span>-sea <span class="hlt">exchange</span> fluxes of hexachlorocyclohexanes (HCHs) and semivolatile PAHs were found close to phase equilibrium, except one PAH, retene, a wood burning tracer, was found seasonally net-volatilisational. Some PCBs, p,p'-DDE, penta- and hexachlorobenzene (PeCB, HCB) were mostly net-depositional, while PBDEs were net-volatilizational. Fluxes determined at a a remote coastal site ranged -33 - +2.4 µg m-2 d-1 for PAHs and -4.0 - +0.3 µg m-2 d-1for halogenated compounds (< 0 means net-deposition, > 0 means net-volatilization). It is concluded that nowadays in open seas more pollutants are undergoing reversal of the direction of <span class="hlt">air</span>-sea <span class="hlt">exchange</span>. Recgional fire activity records in combination with box <span class="hlt">model</span> simulations suggest that deposition of retene during summer is followed by a reversal of <span class="hlt">air</span>-sea <span class="hlt">exchange</span>. The seawater <span class="hlt">surface</span> as secondary source of pollution should be assessed based on flux measurements across seasons and over longer time periods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51B2059Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51B2059Z"><span>Responses of <span class="hlt">Surface</span> Ozone <span class="hlt">Air</span> Quality to Anthropogenic Nitrogen Deposition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, L.; Zhao, Y.; Tai, A. P. K.; Chen, Y.; Pan, Y.</p> <p>2017-12-01</p> <p>Human activities have substantially increased atmospheric deposition of reactive nitrogen to the Earth's <span class="hlt">surface</span>, inducing unintentional effects on ecosystems with complex environmental and climate consequences. One consequence remaining unexplored is how <span class="hlt">surface</span> <span class="hlt">air</span> quality might respond to the enhanced nitrogen deposition through <span class="hlt">surface</span>-atmosphere <span class="hlt">exchange</span>. We combine a chemical transport <span class="hlt">model</span> (GEOS-Chem) and a global land <span class="hlt">model</span> (Community Land <span class="hlt">Model</span>) to address this issue with a focus on ozone pollution in the Northern Hemisphere. We consider three processes that are important for <span class="hlt">surface</span> ozone and can be perturbed by addition of atmospheric deposited nitrogen: emissions of biogenic volatile organic compounds (VOCs), ozone dry deposition, and soil nitrogen oxide (NOx) emissions. We find that present-day anthropogenic nitrogen deposition (65 Tg N a-1 to the land), through enhancing plant growth (represented as increases in vegetation leaf area index (LAI) in the <span class="hlt">model</span>), could increase <span class="hlt">surface</span> ozone from increased biogenic VOC emissions, but could also decrease ozone due to higher ozone dry deposition velocities. Meanwhile, deposited anthropogenic nitrogen to soil enhances soil NOx emissions. The overall effect on summer mean <span class="hlt">surface</span> ozone concentrations show general increases over the globe (up to 1.5-2.3 ppbv over the western US and South Asia), except for some regions with high anthropogenic NOx emissions (0.5-1.0 ppbv decreases over the eastern US, Western Europe, and North China). We compare the <span class="hlt">surface</span> ozone changes with those driven by the past 20-year climate and historical land use changes. We find that the impacts from anthropogenic nitrogen deposition can be comparable to the climate and land use driven <span class="hlt">surface</span> ozone changes at regional scales, and partly offset the <span class="hlt">surface</span> ozone reductions due to land use changes reported in previous studies. Our study emphasizes the complexity of biosphere-atmosphere interactions, which can have important</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvF...1c3905N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvF...1c3905N"><span><span class="hlt">Air</span> entrainment in hairy <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nasto, Alice; Regli, Marianne; Brun, P.-T.; Alvarado, José; Clanet, Christophe; Hosoi, A. E.</p> <p>2016-07-01</p> <p>Motivated by diving semiaquatic mammals, we investigate the mechanism of dynamic <span class="hlt">air</span> entrainment in hairy <span class="hlt">surfaces</span> submerged in liquid. Hairy <span class="hlt">surfaces</span> are cast out of polydimethylsiloxane elastomer and plunged into a fluid bath at different velocities. Experimentally, we find that the amount of <span class="hlt">air</span> entrained is greater than what is expected for smooth <span class="hlt">surfaces</span>. Theoretically, we show that the hairy <span class="hlt">surface</span> can be considered as a porous medium and we describe the <span class="hlt">air</span> entrainment via a competition between the hydrostatic forcing and the viscous resistance in the pores. A phase diagram that includes data from our experiments and biological data from diving semiaquatic mammals is included to place the <span class="hlt">model</span> system in a biological context and predict the regime for which the animal is protected by a plastron of <span class="hlt">air</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A41C0107O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A41C0107O"><span>Comparing and evaluating <span class="hlt">model</span> estimates of background ozone in <span class="hlt">surface</span> <span class="hlt">air</span> over North America</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oberman, J.; Fiore, A. M.; Lin, M.; Zhang, L.; Jacob, D. J.; Naik, V.; Horowitz, L. W.</p> <p>2011-12-01</p> <p>Tropospheric ozone adversely affects human health and vegetation, and is thus a criteria pollutant regulated by the U.S. Environmental Protection Agency (EPA) under the National Ambient <span class="hlt">Air</span> Quality Standard (NAAQS). Ozone is produced in the atmosphere via photo-oxidation of volatile organic compounds (VOCs) and carbon monoxide (CO) in the presence of nitrogen oxides (NOx). The present EPA approach considers health risks associated with exposure to ozone enhancement above the policy-relevant background (PRB), which is currently defined as the <span class="hlt">surface</span> concentration of ozone that would exist without North American anthropogenic emissions. PRB thus includes production by natural precursors, production by precursors emitted on foreign continents, and transport of stratospheric ozone into <span class="hlt">surface</span> <span class="hlt">air</span>. As PRB is not an observable quantity, it must be estimated using numerical <span class="hlt">models</span>. We compare PRB estimates for the year 2006 from the GFDL Atmospheric <span class="hlt">Model</span> 3 (AM3) chemistry-climate <span class="hlt">model</span> (CCM) and the GEOS-Chem (GC) chemical transport <span class="hlt">model</span> (CTM). We evaluate the skill of the <span class="hlt">models</span> in reproducing total <span class="hlt">surface</span> ozone observed at the U.S. Clean <span class="hlt">Air</span> Status and Trends Network (CASTNet), dividing the stations into low-elevation (< 1.5 km in altitude, primarily eastern) and high-elevation (> 1.5 km in altitude, all western) subgroups. At the low-elevation sites AM3 estimates of PRB (38±9 ppbv in spring, 27±9 ppbv in summer) are higher than GC (27±7 ppbv in spring, 21±8 ppbv in summer) in both seasons. Analysis at these sites is complicated by a positive bias in AM3 total ozone with respect to the observed total ozone, the source of which is yet unclear. At high-elevation sites, AM3 PRB is higher in the spring (47±8 ppbv) than in the summer (33±8 ppbv). In contrast, GC simulates little seasonal variation at high elevation sites (39±5 ppbv in spring vs. 38±7 ppbv in summer). Seasonal average total ozone at these sites was within 4 ppbv of the observations for both</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=335530&keyword=air&subject=air%20research&showcriteria=2&fed_org_id=111&datebeginpublishedpresented=02/22/2012&dateendpublishedpresented=02/22/2017&sortby=pubdateyear','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=335530&keyword=air&subject=air%20research&showcriteria=2&fed_org_id=111&datebeginpublishedpresented=02/22/2012&dateendpublishedpresented=02/22/2017&sortby=pubdateyear"><span>Probabilistic estimation of residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates for ...</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>Residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) are a key determinant in the infiltration of ambient <span class="hlt">air</span> pollution indoors. Population-based human exposure <span class="hlt">models</span> using probabilistic approaches to estimate personal exposure to <span class="hlt">air</span> pollutants have relied on input distributions from AER measurements. An algorithm for probabilistically estimating AER was developed based on the Lawrence Berkley National Laboratory Infiltration <span class="hlt">model</span> utilizing housing characteristics and meteorological data with adjustment for window opening behavior. The algorithm was evaluated by comparing <span class="hlt">modeled</span> and measured AERs in four US cities (Los Angeles, CA; Detroit, MI; Elizabeth, NJ; and Houston, TX) inputting study-specific data. The impact on the <span class="hlt">modeled</span> AER of using publically available housing data representative of the region for each city was also assessed. Finally, <span class="hlt">modeled</span> AER based on region-specific inputs was compared with those estimated using literature-based distributions. While <span class="hlt">modeled</span> AERs were similar in magnitude to the measured AER they were consistently lower for all cities except Houston. AERs estimated using region-specific inputs were lower than those using study-specific inputs due to differences in window opening probabilities. The algorithm produced more spatially and temporally variable AERs compared with literature-based distributions reflecting within- and between-city differences, helping reduce error in estimates of <span class="hlt">air</span> pollutant exposure. Published in the Journal of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=104827&keyword=applications+AND+thermodynamic&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=104827&keyword=applications+AND+thermodynamic&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>A CRITICAL ASSESSMENT OF ELEMENTAL MERCURY <span class="hlt">AIR</span>/WATER <span class="hlt">EXCHANGE</span> PARTNERS</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>Although evasion of elemental mercury from aquatic systems can significantly deplete net mercury accumulation resulting from atmospheric deposition, the current ability to <span class="hlt">model</span> elemental mercury <span class="hlt">air</span>/water <span class="hlt">exchange</span> is limited by uncertainties in our understanding of all gaseous a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26196214','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26196214"><span>20 Years of <span class="hlt">Air</span>-Water Gas <span class="hlt">Exchange</span> Observations for Pesticides in the Western Arctic Ocean.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jantunen, Liisa M; Wong, Fiona; Gawor, Anya; Kylin, Henrik; Helm, Paul A; Stern, Gary A; Strachan, William M J; Burniston, Deborah A; Bidleman, Terry F</p> <p>2015-12-01</p> <p>The Arctic has been contaminated by legacy organochlorine pesticides (OCPs) and currently used pesticides (CUPs) through atmospheric transport and oceanic currents. Here we report the time trends and <span class="hlt">air</span>-water <span class="hlt">exchange</span> of OCPs and CUPs from research expeditions conducted between 1993 and 2013. Compounds determined in both <span class="hlt">air</span> and water were trans- and cis-chlordanes (TC, CC), trans- and cis-nonachlors (TN, CN), heptachlor exo-epoxide (HEPX), dieldrin (DIEL), chlorobornanes (ΣCHBs and toxaphene), dacthal (DAC), endosulfans and metabolite endosulfan sulfate (ENDO-I, ENDO-II, and ENDO SUL), chlorothalonil (CHT), chlorpyrifos (CPF), and trifluralin (TFN). Pentachloronitrobenzene (PCNB and quintozene) and its soil metabolite pentachlorothianisole (PCTA) were also found in <span class="hlt">air</span>. Concentrations of most OCPs declined in <span class="hlt">surface</span> water, whereas some CUPs increased (ENDO-I, CHT, and TFN) or showed no significant change (CPF and DAC), and most compounds declined in <span class="hlt">air</span>. Chlordane compound fractions TC/(TC + CC) and TC/(TC + CC + TN) decreased in water and <span class="hlt">air</span>, while CC/(TC + CC + TN) increased. TN/(TC + CC + TN) also increased in <span class="hlt">air</span> and slightly, but not significantly, in water. These changes suggest selective removal of more labile TC and/or a shift in chlordane sources. Water-<span class="hlt">air</span> fugacity ratios indicated net volatilization (FR > 1.0) or near equilibrium (FR not significantly different from 1.0) for most OCPs but net deposition (FR < 1.0) for ΣCHBs. Net deposition was shown for ENDO-I on all expeditions, while the net <span class="hlt">exchange</span> direction of other CUPs varied. Understanding the processes and current state of <span class="hlt">air-surface</span> <span class="hlt">exchange</span> helps to interpret environmental exposure and evaluate the effectiveness of international protocols and provides insights for the environmental fate of new and emerging chemicals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21216057','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21216057"><span>A passive <span class="hlt">air</span> sampler for characterizing the vertical concentration profile of gaseous phase polycyclic aromatic hydrocarbons in near soil <span class="hlt">surface</span> <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>Zhang, Yuzhong; Deng, Shuxing; Liu, Yanan; Shen, Guofeng; Li, Xiqing; Cao, Jun; Wang, Xilong; Reid, Brian; Tao, Shu</p> <p>2011-03-01</p> <p><span class="hlt">Air</span>-soil <span class="hlt">exchange</span> is an important process governing the fate of polycyclic aromatic hydrocarbons (PAHs). A novel passive <span class="hlt">air</span> sampler was designed and tested for measuring the vertical concentration profile of 4 low molecular weight PAHs in gaseous phase (PAH(LMW4)) in near soil <span class="hlt">surface</span> <span class="hlt">air</span>. <span class="hlt">Air</span> at various heights from 5 to 520 mm above the ground was sampled by polyurethane foam disks held in down-faced cartridges. The samplers were tested at three sites: A: an extremely contaminated site, B: a site near A, and C: a background site on a university campus. Vertical concentration gradients were revealed for PAH(LMW4) within a thin layer close to soil <span class="hlt">surface</span> at the three sites. PAH concentrations either decreased (Site A) or increased (Sites B and C) with height, suggesting either deposition to or evaporation from soils. The sampler is a useful tool for investigating <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of gaseous phase semi-volatile organic chemicals. Copyright © 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AtmEn.122..628S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AtmEn.122..628S"><span>Measuring and <span class="hlt">modeling</span> <span class="hlt">air</span> <span class="hlt">exchange</span> rates inside taxi cabs in Los Angeles, California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shu, Shi; Yu, Nu; Wang, Yueyan; Zhu, Yifang</p> <p>2015-12-01</p> <p><span class="hlt">Air</span> <span class="hlt">exchange</span> rates (AERs) have a direct impact on traffic-related <span class="hlt">air</span> pollutant (TRAP) levels inside vehicles. Taxi drivers are occupationally exposed to TRAP on a daily basis, yet there is limited measurement of AERs in taxi cabs. To fill this gap, AERs were quantified in 22 representative Los Angeles taxi cabs including 10 Prius, 5 Crown Victoria, 3 Camry, 3 Caravan, and 1 Uplander under realistic driving (RD) conditions. To further study the impacts of window position and ventilation settings on taxi AERs, additional tests were conducted on 14 taxis with windows closed (WC) and on the other 8 taxis with not only windows closed but also medium fan speed (WC-MFS) under outdoor <span class="hlt">air</span> mode. Under RD conditions, the AERs in all 22 cabs had a mean of 63 h-1 with a median of 38 h-1. Similar AERs were observed under WC condition when compared to those measured under RD condition. Under WC-MFS condition, AERs were significantly increased in all taxi cabs, when compared with those measured under RD condition. A General Estimating Equation (GEE) <span class="hlt">model</span> was developed and the <span class="hlt">modeling</span> results showed that vehicle <span class="hlt">model</span> was a significant factor in determining the AERs in taxi cabs under RD condition. Driving speed and car age were positively associated with AERs but not statistically significant. Overall, AERs measured in taxi cabs were much higher than typical AERs people usually encounter in indoor environments such as homes, offices, and even regular passenger vehicles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGD....10.5385F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGD....10.5385F"><span>Advances in understanding, <span class="hlt">models</span> and parameterisations of biosphere-atmosphere ammonia <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flechard, C. R.; Massad, R.-S.; Loubet, B.; Personne, E.; Simpson, D.; Bash, J. O.; Cooter, E. J.; Nemitz, E.; Sutton, M. A.</p> <p>2013-03-01</p> <p>Atmospheric ammonia (NH3) dominates global emissions of total reactive nitrogen (Nr), while emissions from agricultural production systems contribute about two thirds of global NH3 emissions; the remaining third emanates from oceans, natural vegetation, humans, wild animals and biomass burning. On land, NH3 emitted from the various sources eventually returns to the biosphere by dry deposition to sink areas, predominantly semi-natural vegetation, and by wet and dry deposition as ammonium (NH4+) to all <span class="hlt">surfaces</span>. However, the land/atmosphere <span class="hlt">exchange</span> of gaseous NH3 is in fact bi-directional over unfertilized as well as fertilized ecosystems, with periods and areas of emission and deposition alternating in time (diurnal, seasonal) and space (patchwork landscapes). The <span class="hlt">exchange</span> is controlled by a range of environmental factors, including meteorology, <span class="hlt">surface</span> layer turbulence, thermodynamics, <span class="hlt">air</span> and <span class="hlt">surface</span> heterogeneous-phase chemistry, canopy geometry, plant development stage, leaf age, organic matter decomposition, soil microbial turnover, and, in agricultural systems, by fertilizer application rate, fertilizer type, soil type, crop type, and agricultural management practices. We review the range of processes controlling NH3 emission and uptake in the different parts of the soil-canopy-atmosphere continuum, with NH3 emission potentials defined at the substrate and leaf levels by different [NH4+] / [H+] ratios (Γ). <span class="hlt">Surface</span>/atmosphere <span class="hlt">exchange</span> <span class="hlt">models</span> for NH3 are necessary to compute the temporal and spatial patterns of emissions and deposition at the soil, plant, field, landscape, regional and global scales, in order to assess the multiple environmental impacts of <span class="hlt">air</span>-borne and deposited NH3 and NH4+. <span class="hlt">Models</span> of soil/vegetation/atmosphereem NH3 <span class="hlt">exchange</span> are reviewed from the substrate and leaf scales to the global scale. They range from simple steady-state, "big leaf" canopy resistance <span class="hlt">models</span>, to dynamic, multi-layer, multi-process, multi</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=223609&keyword=water+AND+gas+AND+exchange&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=223609&keyword=water+AND+gas+AND+exchange&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><span class="hlt">Air</span>-water Gas <span class="hlt">Exchange</span> Rates on a Large Impounded River Measured Using Floating Domes (Poster)</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>Mass balance <span class="hlt">models</span> of dissolved gases in rivers typically serve as the basis for whole-system estimates of greenhouse gas emission rates. An important component of these <span class="hlt">models</span> is the <span class="hlt">exchange</span> of dissolved gases between <span class="hlt">air</span> and water. Controls on gas <span class="hlt">exchange</span> rates (K) have 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_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('http://adsabs.harvard.edu/abs/2013EGUGA..1511944T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1511944T"><span>A theoretical <span class="hlt">model</span> of the influence of spray on the <span class="hlt">exchange</span> of momentum, with storm and hurricane winds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Troitskaya, Yuliya; Ezhova, Ekaterina; Soustova, Irina</p> <p>2013-04-01</p> <p>A stochastic <span class="hlt">model</span> of the "life cycle" of a droplet, the torn off the crest of a steep <span class="hlt">surface</span> wave and then falling down to the water is constructed. The <span class="hlt">model</span> includes the following constituents: i) a <span class="hlt">model</span> of motion of a heavy particle in the forcing <span class="hlt">air</span> flow (equation of motion), ii) a <span class="hlt">model</span> of the wind flow (wind velocity, wave-induced disturbances, turbulent fluctuations), iii) a <span class="hlt">model</span> of spray injection, iiii) the droplet statistics (size distribution, wind-speed dependence) The interaction of water droplets in the atmospheric boundary layer with turbulent fluctuations is described in terms of the Markovian chain. The mean wind field in the marine atmospheric boundary layer is determined by the momentum <span class="hlt">exchange</span> associated with the turbulent and wave momentum transfer and by sprays. The wave and turbulent momentum <span class="hlt">exchange</span> is parameterized by the Charnok expression for the roughness parameter. Wave disturbances induced in the <span class="hlt">air</span> flow by waves at the <span class="hlt">surface</span>, were calculated within the <span class="hlt">model</span> of the marine atmospheric boundary suggested in [1]. The greatest uncertainty in this <span class="hlt">model</span> is the mechanism of droplets injection. We consider two <span class="hlt">models</span> for the injection of droplets in the <span class="hlt">air</span> flow. In the first <span class="hlt">model</span> the droplets formed by the development of the Kelvin-Helmholtz instability, are entered in the flow with the orbital velocity of the wave (Koga's <span class="hlt">model</span> [2]), The second mechanism, investigated in many papers, considers droplets from the breakdown of a jet which rises at high speeds from the bottom of the collapsing <span class="hlt">air</span> bubble cavity [3]. To determine the number of drops injected to the atmospheric boundary layer from the sea <span class="hlt">surface</span>, the Spray generation function proposed in [4] was in use. Within the <span class="hlt">model</span> the momentum acquired by every droplet in the interaction with the <span class="hlt">air</span> flow was calculated. Depending on the particular field of <span class="hlt">air</span> velocity, wave parameters and the radius of the droplet, it can both get and deliver momentum give impetus to the <span class="hlt">air</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=310737&Lab=NERL&keyword=health+AND+physics&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=310737&Lab=NERL&keyword=health+AND+physics&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>Global evaluation of ammonia bidirectional <span class="hlt">exchange</span> and livestock diurnal variation schemes</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>Bidirectional air–<span class="hlt">surface</span> <span class="hlt">exchange</span> of ammonia (NH3) has been neglected in many <span class="hlt">air</span> quality <span class="hlt">models</span>. In this study, we implement the bidirectional <span class="hlt">exchange</span> of NH3 in the GEOS-Chem global chemical transport <span class="hlt">model</span>. We also introduce an updated diurnal variability scheme for NH3...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18522097','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18522097"><span>Measurement and <span class="hlt">modeling</span> of diel variability of polybrominated diphenyl ethers and chlordanes in <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>Moeckel, Claudia; Macleod, Matthew; Hungerbühler, Konrad; Jones, Kevin C</p> <p>2008-05-01</p> <p>Short-term variability of concentrations of polybrominated diphenyl ethers (PBDEs) and chlordanes in <span class="hlt">air</span> at a semirural site in England over a 5 day period is reported. Four-hour <span class="hlt">air</span> samples were collected during a period dominated by a high pressure system that produced stable diel (24-h) patterns of meteorological conditions such as temperature and atmospheric boundary layer height. PBDE and chlordane concentrations showed clear diel variability with concentrations in the afternoon and evening being 1.9 - 2.7 times higher than in the early morning. The measurements are interpreted using a multimedia mass balance <span class="hlt">model</span> parametrized with forcing functions representing local temperature, atmospheric boundary layer height, wind speed and hydroxyl radical concentrations. <span class="hlt">Model</span> results indicate that reversible, temperature-controlled <span class="hlt">air-surface</span> <span class="hlt">exchange</span> is the primary driver of the diel concentration pattern observed for chlordanes and PBDE 28. For higher brominated PBDE congeners (47, 99 and 100), the effect of variable atmospheric mixing height in combination with irreversible deposition on aerosol particles is dominant and explains the diel patterns almost entirely. Higher concentrations of chlordanes and PBDEs in <span class="hlt">air</span> observed at the end of the study period could be related to likely source areas using back trajectory analysis. This is the first study to clearly document diel variability in concentrations of PBDEs in <span class="hlt">air</span> over a period of several days. Our <span class="hlt">model</span> analysis indicates that high daytime and low nighttime concentrations of semivolatile organic chemicals can arise from different underlying driving processes, and are not necessarily evidence of reversible <span class="hlt">air-surface</span> <span class="hlt">exchange</span> on a 24-h time scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007GeCoA..71.1098T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007GeCoA..71.1098T"><span>Two cation <span class="hlt">exchange</span> <span class="hlt">models</span> for direct and inverse <span class="hlt">modelling</span> of solution major cation composition in equilibrium with illite <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tournassat, Christophe; Gailhanou, Hélène; Crouzet, Catherine; Braibant, Gilles; Gautier, Anne; Lassin, Arnault; Blanc, Philippe; Gaucher, Eric C.</p> <p>2007-03-01</p> <p>Na/K, Na/Ca and Na/Mg <span class="hlt">exchange</span> isotherms were performed on the fine fraction (<2 μm) of Imt-2 illite samples at a total normality of about 0.005 mol/L in anionic chloride medium. The derived selectivity coefficients for Na/K, Na/Ca and Na/Mg were found to vary as a function of the <span class="hlt">exchanger</span> composition and compared well with the data collected in the literature for similar experimental conditions. Two <span class="hlt">models</span> were built to reproduce the data: the first was a multi(2)-site <span class="hlt">model</span> with constant Gaines and Thomas selectivity coefficients; the second was a one-site <span class="hlt">model</span> taking into account <span class="hlt">surface</span> species activity coefficients. The results of the <span class="hlt">models</span> were in rather good agreement with both our data and literature data. The multi-site <span class="hlt">model</span> proved to be efficient in predicting the <span class="hlt">exchanger</span> composition as a function of the Na/Ca/Mg/K concentrations in solution, whereas the one-site <span class="hlt">model</span> proved to be a better approach to derive the Na/Ca/Mg/K concentrations in solution based on the knowledge of the <span class="hlt">exchanger</span> composition and the total normality of the solution. The interest of this approach is illustrated by the need for major cation solute concentration predictions in compacted clay for the characterization of nuclear deep disposal host rock repositories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21917934','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21917934"><span><span class="hlt">Air</span>-gas <span class="hlt">exchange</span> reevaluated: clinically important results of a computer simulation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shunmugam, Manoharan; Shunmugam, Sudhakaran; Williamson, Tom H; Laidlaw, D Alistair</p> <p>2011-10-21</p> <p>The primary aim of this study was to evaluate the efficiency of <span class="hlt">air</span>-gas <span class="hlt">exchange</span> techniques and the factors that influence the final concentration of an intraocular gas tamponade. Parameters were varied to find the optimum method of performing an <span class="hlt">air</span>-gas <span class="hlt">exchange</span> in ideal circumstances. A computer <span class="hlt">model</span> of the eye was designed using 3D software with fluid flow analysis capabilities. Factors such as angular distance between ports, gas infusion gauge, exhaust vent gauge and depth were varied in the <span class="hlt">model</span>. Flow rate and axial length were also modulated to simulate faster injections and more myopic eyes, respectively. The flush volume of gas required to achieve a 97% intraocular gas fraction concentration were compared. Modulating individual factors did not reveal any clinically significant difference in the angular distance between ports, exhaust vent size, and depth or rate of gas injection. In combination, however, there was a 28% increase in <span class="hlt">air</span>-gas <span class="hlt">exchange</span> efficiency comparing the most efficient with the least efficient studied parameters in this <span class="hlt">model</span>. The gas flush volume required to achieve a 97% gas fill also increased proportionately at a ratio of 5.5 to 6.2 times the volume of the eye. A 35-mL flush is adequate for eyes up to 25 mm in axial length; however, eyes longer than this would require a much greater flush volume, and surgeons should consider using two separate 50-mL gas syringes to ensure optimal gas concentration for eyes greater than 25 mm in axial length.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5381A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5381A"><span><span class="hlt">Air</span>SWOT observations versus hydrodynamic <span class="hlt">model</span> outputs of water <span class="hlt">surface</span> elevation and slope in a multichannel river</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Altenau, Elizabeth H.; Pavelsky, Tamlin M.; Moller, Delwyn; Lion, Christine; Pitcher, Lincoln H.; Allen, George H.; Bates, Paul D.; Calmant, Stéphane; Durand, Michael; Neal, Jeffrey C.; Smith, Laurence C.</p> <p>2017-04-01</p> <p>Anabranching rivers make up a large proportion of the world's major rivers, but quantifying their flow dynamics is challenging due to their complex morphologies. Traditional in situ measurements of water levels collected at gauge stations cannot capture out of bank flows and are limited to defined cross sections, which presents an incomplete picture of water fluctuations in multichannel systems. Similarly, current remotely sensed measurements of water <span class="hlt">surface</span> elevations (WSEs) and slopes are constrained by resolutions and accuracies that limit the visibility of <span class="hlt">surface</span> waters at global scales. Here, we present new measurements of river WSE and slope along the Tanana River, AK, acquired from <span class="hlt">Air</span>SWOT, an airborne analogue to the <span class="hlt">Surface</span> Water and Ocean Topography (SWOT) mission. Additionally, we compare the <span class="hlt">Air</span>SWOT observations to hydrodynamic <span class="hlt">model</span> outputs of WSE and slope simulated across the same study area. Results indicate <span class="hlt">Air</span>SWOT errors are significantly lower than <span class="hlt">model</span> outputs. When compared to field measurements, RMSE for <span class="hlt">Air</span>SWOT measurements of WSEs is 9.0 cm when averaged over 1 km squared areas and 1.0 cm/km for slopes along 10 km reaches. Also, <span class="hlt">Air</span>SWOT can accurately reproduce the spatial variations in slope critical for characterizing reach-scale hydraulics, while <span class="hlt">model</span> outputs of spatial variations in slope are very poor. Combining <span class="hlt">Air</span>SWOT and future SWOT measurements with hydrodynamic <span class="hlt">models</span> can result in major improvements in <span class="hlt">model</span> simulations at local to global scales. Scientists can use <span class="hlt">Air</span>SWOT measurements to constrain <span class="hlt">model</span> parameters over long reach distances, improve understanding of the physical processes controlling the spatial distribution of <span class="hlt">model</span> parameters, and validate <span class="hlt">models</span>' abilities to reproduce spatial variations in slope. Additionally, <span class="hlt">Air</span>SWOT and SWOT measurements can be assimilated into lower-complexity <span class="hlt">models</span> to try and approach the accuracies achieved by higher-complexity <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27974151','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27974151"><span>Using a passive <span class="hlt">air</span> sampler to monitor <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of organochlorine pesticides in the pasture of the central Tibetan Plateau.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Chuanfei; Wang, Xiaoping; Ren, Jiao; Gong, Ping; Yao, Tandong</p> <p>2017-02-15</p> <p><span class="hlt">Air</span>-soil <span class="hlt">exchange</span> is a key process controlling the fate of persistent organic pollutants (POPs). However, the "sink effect" of soil for POPs in Tibetan pasture has not been clear. In NamCo, in the central Tibetan Plateau (TP) where the land is covered by grass, a modified passive <span class="hlt">air</span> sampler (PAS) (thickness: 2cm) was tested. Using the PAS, the atmospheric gaseous phase organochlorine pesticides (OCPs) at 11 heights from close-to-<span class="hlt">surface</span> (2cm) to 200cm above ground, in summer and in winter, were measured. Concentrations of OCPs in summer were higher than those in winter. Both in summer and winter, atmospheric concentrations of OCPs decreased with decreasing height from 200 to 2cm, indicating that OCPs were being deposited from <span class="hlt">air</span> to soil. <span class="hlt">Air</span> deposition of OCPs was possibly driven by wind speed. Furthermore, based on <span class="hlt">air</span> OCPs at 0-3cm near the <span class="hlt">surface</span>, the interface <span class="hlt">exchange</span> of OCPs between <span class="hlt">air</span> and soil was studied by the fugacity method. The results showed that pastural soil in the TP was a "sink" of OCPs even in summer. The mean deposition fluxes of α-HCH, γ-HCH and o,p'-DDT were 0.72, 0.24 and 0.54pg/h/m 2 , respectively, and it was estimated that the level of these pollutants in the soil will double every 24, 66 and 206years, respectively. This study will contribute to the further understanding of global cycling of POPs in different land covers. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JASTP.164..259P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JASTP.164..259P"><span>Impacts of spectral nudging on the simulated <span class="hlt">surface</span> <span class="hlt">air</span> temperature in summer compared with the selection of shortwave radiation and land <span class="hlt">surface</span> <span class="hlt">model</span> physics parameterization in a high-resolution regional atmospheric <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, Jun; Hwang, Seung-On</p> <p>2017-11-01</p> <p>The impact of a spectral nudging technique for the dynamical downscaling of the summer <span class="hlt">surface</span> <span class="hlt">air</span> temperature in a high-resolution regional atmospheric <span class="hlt">model</span> is assessed. The performance of this technique is measured by comparing 16 analysis-driven simulation sets of physical parameterization combinations of two shortwave radiation and four land <span class="hlt">surface</span> <span class="hlt">model</span> schemes of the <span class="hlt">model</span>, which are known to be crucial for the simulation of the <span class="hlt">surface</span> <span class="hlt">air</span> temperature. It is found that the application of spectral nudging to the outermost domain has a greater impact on the regional climate than any combination of shortwave radiation and land <span class="hlt">surface</span> <span class="hlt">model</span> physics schemes. The optimal choice of two <span class="hlt">model</span> physics parameterizations is helpful for obtaining more realistic spatiotemporal distributions of land <span class="hlt">surface</span> variables such as the <span class="hlt">surface</span> <span class="hlt">air</span> temperature, precipitation, and <span class="hlt">surface</span> fluxes. However, employing spectral nudging adds more value to the results; the improvement is greater than using sophisticated shortwave radiation and land <span class="hlt">surface</span> <span class="hlt">model</span> physical parameterizations. This result indicates that spectral nudging applied to the outermost domain provides a more accurate lateral boundary condition to the innermost domain when forced by analysis data by securing the consistency with large-scale forcing over a regional domain. This consequently indirectly helps two physical parameterizations to produce small-scale features closer to the observed values, leading to a better representation of the <span class="hlt">surface</span> <span class="hlt">air</span> temperature in a high-resolution downscaled climate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRC..117.5035A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRC..117.5035A"><span>Statistics of <span class="hlt">surface</span> divergence and their relation to <span class="hlt">air</span>-water gas transfer velocity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asher, William E.; Liang, Hanzhuang; Zappa, Christopher J.; Loewen, Mark R.; Mukto, Moniz A.; Litchendorf, Trina M.; Jessup, Andrew T.</p> <p>2012-05-01</p> <p><span class="hlt">Air</span>-sea gas fluxes are generally defined in terms of the <span class="hlt">air</span>/water concentration difference of the gas and the gas transfer velocity,kL. Because it is difficult to measure kLin the ocean, it is often parameterized using more easily measured physical properties. <span class="hlt">Surface</span> divergence theory suggests that infrared (IR) images of the water <span class="hlt">surface</span>, which contain information concerning the movement of water very near the <span class="hlt">air</span>-water interface, might be used to estimatekL. Therefore, a series of experiments testing whether IR imagery could provide a convenient means for estimating the <span class="hlt">surface</span> divergence applicable to <span class="hlt">air</span>-sea <span class="hlt">exchange</span> were conducted in a synthetic jet array tank embedded in a wind tunnel. Gas transfer velocities were measured as a function of wind stress and mechanically generated turbulence; laser-induced fluorescence was used to measure the concentration of carbon dioxide in the top 300 μm of the water <span class="hlt">surface</span>; IR imagery was used to measure the spatial and temporal distribution of the aqueous skin temperature; and particle image velocimetry was used to measure turbulence at a depth of 1 cm below the <span class="hlt">air</span>-water interface. It is shown that an estimate of the <span class="hlt">surface</span> divergence for both wind-shear driven turbulence and mechanically generated turbulence can be derived from the <span class="hlt">surface</span> skin temperature. The estimates derived from the IR images are compared to velocity field divergences measured by the PIV and to independent estimates of the divergence made using the laser-induced fluorescence data. Divergence is shown to scale withkLvalues measured using gaseous tracers as predicted by conceptual <span class="hlt">models</span> for both wind-driven and mechanically generated turbulence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.A41A0025M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.A41A0025M"><span>Eddy covariance measurement of the spatial heterogeneity of <span class="hlt">surface</span> energy <span class="hlt">exchanges</span> over Heron Reef, Great Barrier Reef, Australia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>MacKellar, M.; McGowan, H. A.; Phinn, S. R.</p> <p>2011-12-01</p> <p>Coral reefs cover 2.8 to 6.0 x 105 km2 of the Earth's <span class="hlt">surface</span> and are warm, shallow regions that are believed to contribute enhanced sensible and latent heat to the atmosphere, relative to the surrounding ocean. To predict the impact of climate variability on coral reefs and their weather and climate including cloud, winds, rainfall patterns and cyclone genesis, accurate parameterisation of <span class="hlt">air</span>-sea energy <span class="hlt">exchanges</span> over coral reefs is essential. This is also important for the parameterisation and validation of regional to global scale forecast <span class="hlt">models</span> to improve prediction of tropical and sub-tropical marine and coastal weather. Eddy covariance measurements of <span class="hlt">air</span>-sea fluxes over coral reefs are rare due to the complexities of installing instrumentation over shallow, tidal water. Consequently, measurements of radiation and turbulent flux data for coral reefs have been captured remotely (satellite data) or via single measurement sites downwind of coral reefs (e.g. terrestrial or shipboard instrumentation). The resolution of such measurements and those that have been made at single locations on reefs may not capture the spatial heterogeneity of <span class="hlt">surface</span>-atmosphere energy <span class="hlt">exchanges</span> due to the different geomorphic and biological zones on coral reefs. Accordingly, the heterogeneity of coral reefs with regard to substrate, benthic communities and hydrodynamic processes are not considered in the characterization of the <span class="hlt">surface</span> radiation energy flux transfers across the water-atmosphere interface. In this paper we present a unique dataset of concurrent in situ eddy covariance measurements made on instrumented pontoons of the <span class="hlt">surface</span> energy balance over different geomorphic zones of a coral reef (shallow reef flat, shallow and deep lagoons). Significant differences in radiation transfers and <span class="hlt">air</span>-sea turbulent flux <span class="hlt">exchanges</span> over the reef were highlighted, with higher Bowen ratios over the shallow reef flat. Increasing wind speed was shown to increase flux divergence between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28526196','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28526196"><span>Use of a numerical simulation approach to improve the estimation of <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes of polycyclic aromatic hydrocarbons in a coastal zone.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lai, I-Chien; Lee, Chon-Lin; Ko, Fung-Chi; Lin, Ju-Chieh; Huang, Hu-Ching; Shiu, Ruei-Feng</p> <p>2017-07-15</p> <p>The <span class="hlt">air</span>-water <span class="hlt">exchange</span> is important for determining the transport, fate, and chemical loading of polycyclic aromatic hydrocarbons (PAHs) in the atmosphere and in aquatic systems. Investigations of PAH <span class="hlt">air</span>-water <span class="hlt">exchange</span> are mostly based on observational data obtained using complicated field sampling processes. This study proposes a new approach to improve the estimation of long-term PAH <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes by using a multivariate regression <span class="hlt">model</span> to simulate hourly gaseous PAH concentrations. <span class="hlt">Model</span> performance analysis and the benefits from this approach indicate its effectiveness at improving the flux estimations and at decreasing the field sampling difficulty. The proposed GIS mapping approach is useful for box <span class="hlt">model</span> establishment and is tested for visualization of the spatiotemporal variations of <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes in a coastal zone. The <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes illustrated by contour maps suggest that the atmospheric PAHs might have greater impacts on offshore sites than on the coastal area in this study. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70195393','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70195393"><span>On factors influencing <span class="hlt">air</span>-water gas <span class="hlt">exchange</span> in emergent wetlands</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Ho, David T.; Engel, Victor C.; Ferron, Sara; Hickman, Benjamin; Choi, Jay; Harvey, Judson W.</p> <p>2018-01-01</p> <p>Knowledge of gas <span class="hlt">exchange</span> in wetlands is important in order to determine fluxes of climatically and biogeochemically important trace gases and to conduct mass balances for metabolism studies. Very few studies have been conducted to quantify gas transfer velocities in wetlands, and many wind speed/gas <span class="hlt">exchange</span> parameterizations used in oceanographic or limnological settings are inappropriate under conditions found in wetlands. Here six measurements of gas transfer velocities are made with SF6 tracer release experiments in three different years in the Everglades, a subtropical peatland with <span class="hlt">surface</span> water flowing through emergent vegetation. The experiments were conducted under different flow conditions and with different amounts of emergent vegetation to determine the influence of wind, rain, water flow, waterside thermal convection, and vegetation on <span class="hlt">air</span>-water gas <span class="hlt">exchange</span> in wetlands. Measured gas transfer velocities under the different conditions ranged from 1.1 cm h−1 during baseline conditions to 3.2 cm h−1 when rain and water flow rates were high. Commonly used wind speed/gas <span class="hlt">exchange</span> relationships would overestimate the gas transfer velocity by a factor of 1.2 to 6.8. Gas <span class="hlt">exchange</span> due to thermal convection was relatively constant and accounted for 14 to 51% of the total measured gas <span class="hlt">exchange</span>. Differences in rain and water flow among the different years were responsible for the variability in gas <span class="hlt">exchange</span>, with flow accounting for 37 to 77% of the gas <span class="hlt">exchange</span>, and rain responsible for up to 40%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20026678-short-term-temperature-dependent-air-surface-exchange-atmospheric-concentrations-polychlorinated-naphthalenes-organochlorine-pesticides','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20026678-short-term-temperature-dependent-air-surface-exchange-atmospheric-concentrations-polychlorinated-naphthalenes-organochlorine-pesticides"><span>Short-term temperature-dependent <span class="hlt">air-surface</span> <span class="hlt">exchange</span> and atmospheric concentrations of polychlorinated naphthalenes and organochlorine pesticides</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, R.G.M.; Burnett, V.; Harner, T.</p> <p>2000-02-01</p> <p>Atmospheric concentrations of five organochlorine (OC) pesticides, some of which have been banned for a number of years, and polychlorinated naphthalenes (PCNs) were measured at a U.K. site over periods of 6 h for 7 days resulting in 28 samples. Mean concentrations of the pesticides were {alpha}-HCH 90 pg m{sup {minus}3}, {gamma}-HCH 500, {rho},{rho}{prime}-DDE 8, dieldrin 63, endrin 22, and HCB 39. PCN mean homologue concentrations were {sub 3}CNs 67 pg m{sup {minus}3}, {sub 4}CNs 78, {sub 5}CNs 5, {sub 6}CNs 0.6, {sub 7}CNs 0.6, and {Sigma}PCNs 152. TEQ concentrations for those PCNs ascribed TEF values ranged between 0.36 andmore » 3.6 fg m{sup {minus}3} which corresponds to {approximately}3.0--30% of the TEQ concentrations of PCDD/Fs at the same site. All the compounds measured, except HCB, exhibited a strong temperature-dependent diurnal cycling. Results from Clausius-Clapeyron plots show that pesticide concentrations were controlled by temperature-driven <span class="hlt">air-surface</span> recycling throughout the first 5 days when stable atmospheric conditions were dominant, while during the last 2 days advection became more influential as more unstable and cooler weather started to influence the site. PCN concentrations were controlled primarily by a mixture of recycling and advection throughout the first 5 days and then by advection in the final 2 days, suggesting that there are ongoing emissions from diffuse point sources of PCNs into the U.K. atmosphere. This study provides further evidence of the rapid <span class="hlt">air-surface</span> <span class="hlt">exchange</span> of semivolatile organic compounds (SOCs) and shows how different factors alone or in combination can produce rapid changes in the atmospheric concentrations of past and present SOCs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20850199','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20850199"><span>Molecular-level removal of proteinaceous contamination from <span class="hlt">model</span> <span class="hlt">surfaces</span> and biomedical device materials by <span class="hlt">air</span> plasma treatment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Banerjee, K K; Kumar, S; Bremmell, K E; Griesser, H J</p> <p>2010-11-01</p> <p>Established methods for cleaning and sterilising biomedical devices may achieve removal of bioburden only at the macroscopic level while leaving behind molecular levels of contamination (mainly proteinaceous). This is of particular concern if the residue might contain prions. We investigated at the molecular level the removal of <span class="hlt">model</span> and real-life proteinaceous contamination from <span class="hlt">model</span> and practical <span class="hlt">surfaces</span> by <span class="hlt">air</span> plasma (ionised <span class="hlt">air</span>) treatment. The <span class="hlt">surface</span>-sensitive technique of X-ray photoelectron spectroscopy (XPS) was used to assess the removal of proteinaceous contamination, with the nitrogen (N1s) photoelectron signal as its marker. <span class="hlt">Model</span> proteinaceous contamination (bovine serum albumin) adsorbed on to a <span class="hlt">model</span> <span class="hlt">surface</span> (silicon wafer) and the residual proteinaceous contamination resulting from incubating surgical stainless steel (a practical biomaterial) in whole human blood exhibited strong N1s signals [16.8 and 18.5 atomic percent (at.%), respectively] after thorough washing. After 5min <span class="hlt">air</span> plasma treatment, XPS detected no nitrogen on the sample <span class="hlt">surfaces</span>, indicating complete removal of proteinaceous contamination, down to the estimated XPS detection limit 10ng/cm(2). Applying the same plasma treatment, the 7.7at.% nitrogen observed on a clinically cleaned dental bur was reduced to a level reflective of new, as-received burs. Contact angle measurements and atomic force microscopy also indicated complete molecular-level removal of the proteinaceous contamination upon <span class="hlt">air</span> plasma treatment. This study demonstrates the effectiveness of <span class="hlt">air</span> plasma treatment for removing proteinaceous contamination from both <span class="hlt">model</span> and practical <span class="hlt">surfaces</span> and offers a method for ensuring that no molecular residual contamination such as prions is transferred upon re-use of surgical and dental instruments. Crown Copyright © 2010. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27209375','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27209375"><span>Gas <span class="hlt">Exchange</span> <span class="hlt">Models</span> for a Flexible Insect Tracheal System.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Simelane, S M; Abelman, S; Duncan, F D</p> <p>2016-06-01</p> <p>In this paper two <span class="hlt">models</span> for movement of respiratory gases in the insect trachea are presented. One <span class="hlt">model</span> considers the tracheal system as a single flexible compartment while the other <span class="hlt">model</span> considers the trachea as a single flexible compartment with gas <span class="hlt">exchange</span>. This work represents an extension of Ben-Tal's work on compartmental gas <span class="hlt">exchange</span> in human lungs and is applied to the insect tracheal system. The purpose of the work is to study nonlinear phenomena seen in the insect respiratory system. It is assumed that the flow inside the trachea is laminar, and that the <span class="hlt">air</span> inside the chamber behaves as an ideal gas. Further, with the isothermal assumption, the expressions for the tracheal partial pressures of oxygen and carbon dioxide, rate of volume change, and the rates of change of oxygen concentration and carbon dioxide concentration are derived. The effects of some flow parameters such as diffusion capacities, reaction rates and <span class="hlt">air</span> concentrations on net flow are studied. Numerical simulations of the tracheal flow characteristics are performed. The <span class="hlt">models</span> developed provide a mathematical framework to further investigate gas <span class="hlt">exchange</span> in insects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A12F..05I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A12F..05I"><span>Measurements and <span class="hlt">Modeling</span> of Turbulent Fluxes during Persistent Cold <span class="hlt">Air</span> Pool Events in Salt Lake Valley, Utah</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivey, C. E.; Sun, X.; Holmes, H.</p> <p>2017-12-01</p> <p>Land <span class="hlt">surface</span> processes are important in meteorology and climate research since they control the partitioning of <span class="hlt">surface</span> energy and water <span class="hlt">exchange</span> at the earth's <span class="hlt">surface</span>. The <span class="hlt">surface</span> layer is coupled to the planetary boundary layer (PBL) by <span class="hlt">surface</span> fluxes, which serve as sinks or sources of energy, moisture, momentum, and atmospheric pollutants. Quantifying the <span class="hlt">surface</span> heat and momentum fluxes at the land-atmosphere interface, especially for different <span class="hlt">surface</span> land cover types, is important because they can further influence the atmospheric dynamics, vertical mixing, and transport processes that impact local, regional, and global climate. A cold <span class="hlt">air</span> pool (CAP) forms when a topographic depression (i.e., valley) fills with cold <span class="hlt">air</span>, where the <span class="hlt">air</span> in the stagnant layer is colder than the <span class="hlt">air</span> aloft. Insufficient <span class="hlt">surface</span> heating, which is not able to sufficiently erode the temperature inversion that forms during the nighttime stable boundary layer, can lead to the formation of persistent CAPs during wintertime. These persistent CAPs can last for days, or even weeks, and are associated with increased <span class="hlt">air</span> pollution concentrations. Thus, realistic simulations of the land-atmosphere <span class="hlt">exchange</span> are meaningful to achieve improved predictions of the accumulation, transport, and dispersion of <span class="hlt">air</span> pollution concentrations. The focus of this presentation is on observations and <span class="hlt">modeling</span> results using turbulence data collected in Salt Lake Valley, Utah during the 2010-2011 wintertime Persistent Cold <span class="hlt">Air</span> Pool Study (PCAPS). Turbulent fluxes and the <span class="hlt">surface</span> energy balance over seven land use types are quantified. The urban site has an energy balance ratio (EBR) larger than one (1.276). Negative Bowen ratio (-0.070) is found at the cropland site. In addition to turbulence observations, half-hourly WRF simulated net radiation, latent heat, sensible heat, ground heat fluxes during one persistent CAP event are evaluated using the PCAPS observations. The results show that sensible and latent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16527753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16527753"><span>Scraped <span class="hlt">surface</span> heat <span class="hlt">exchangers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rao, Chetan S; Hartel, Richard W</p> <p>2006-01-01</p> <p>Scraped <span class="hlt">surface</span> heat <span class="hlt">exchangers</span> (SSHEs) are commonly used in the food, chemical, and pharmaceutical industries for heat transfer, crystallization, and other continuous processes. They are ideally suited for products that are viscous, sticky, that contain particulate matter, or that need some degree of crystallization. Since these characteristics describe a vast majority of processed foods, SSHEs are especially suited for pumpable food products. During operation, the product is brought in contact with a heat transfer <span class="hlt">surface</span> that is rapidly and continuously scraped, thereby exposing the <span class="hlt">surface</span> to the passage of untreated product. In addition to maintaining high and uniform heat <span class="hlt">exchange</span>, the scraper blades also provide simultaneous mixing and agitation. Heat <span class="hlt">exchange</span> for sticky and viscous foods such as heavy salad dressings, margarine, chocolate, peanut butter, fondant, ice cream, and shortenings is possible only by using SSHEs. High heat transfer coefficients are achieved because the boundary layer is continuously replaced by fresh material. Moreover, the product is in contact with the heating <span class="hlt">surface</span> for only a few seconds and high temperature gradients can be used without the danger of causing undesirable reactions. SSHEs are versatile in the use of heat transfer medium and the various unit operations that can be carried out simultaneously. This article critically reviews the current understanding of the operations and applications of SSHEs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.3291C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.3291C"><span>Progress in remote sensing of global land <span class="hlt">surface</span> heat fluxes and evaporations with a turbulent heat <span class="hlt">exchange</span> parameterization method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Xuelong; Su, Bob</p> <p>2017-04-01</p> <p>Remote sensing has provided us an opportunity to observe Earth land <span class="hlt">surface</span> with a much higher resolution than any of GCM simulation. Due to scarcity of information for land <span class="hlt">surface</span> physical parameters, up-to-date GCMs still have large uncertainties in the coupled land <span class="hlt">surface</span> process <span class="hlt">modeling</span>. One critical issue is a large amount of parameters used in their land <span class="hlt">surface</span> <span class="hlt">models</span>. Thus remote sensing of land <span class="hlt">surface</span> spectral information can be used to provide information on these parameters or assimilated to decrease the <span class="hlt">model</span> uncertainties. Satellite imager could observe the Earth land <span class="hlt">surface</span> with optical, thermal and microwave bands. Some basic Earth land <span class="hlt">surface</span> status (land <span class="hlt">surface</span> temperature, canopy height, canopy leaf area index, soil moisture etc.) has been produced with remote sensing technique, which already help scientists understanding Earth land and atmosphere interaction more precisely. However, there are some challenges when applying remote sensing variables to calculate global land-<span class="hlt">air</span> heat and water <span class="hlt">exchange</span> fluxes. Firstly, a global turbulent <span class="hlt">exchange</span> parameterization scheme needs to be developed and verified, especially for global momentum and heat roughness length calculation with remote sensing information. Secondly, a compromise needs to be innovated to overcome the spatial-temporal gaps in remote sensing variables to make the remote sensing based land <span class="hlt">surface</span> fluxes applicable for GCM <span class="hlt">model</span> verification or comparison. A flux network data library (more 200 flux towers) was collected to verify the designed method. Important progress in remote sensing of global land flux and evaporation will be presented and its benefits for GCM <span class="hlt">models</span> will also be discussed. Some in-situ studies on the Tibetan Plateau and problems of land <span class="hlt">surface</span> process simulation will also be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7300088-operating-experiences-rotary-air-air-heat-exchangers-hospitals-schools-nursing-homes-swimming-pools','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7300088-operating-experiences-rotary-air-air-heat-exchangers-hospitals-schools-nursing-homes-swimming-pools"><span>Operating experiences with rotary <span class="hlt">air-to-air</span> heat <span class="hlt">exchangers</span>: hospitals, schools, nursing homes, swimming pools</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>Pearson, R.J.</p> <p>1976-01-01</p> <p>Systems utilizing rotary <span class="hlt">air-to-air</span> heat <span class="hlt">exchangers</span> are discussed. Basic considerations of use (fresh <span class="hlt">air</span> requirements, system configurations, cost considerations), typical system layout/design considerations, and operating observations by engineers, staff and maintenance personnel are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A54D..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A54D..05K"><span>Effects of wintertime atmospheric river landfalls on <span class="hlt">surface</span> <span class="hlt">air</span> temperatures in the Western US: Analyses and <span class="hlt">model</span> evaluation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, J.; Guan, B.; Waliser, D. E.; Ferraro, R.</p> <p>2016-12-01</p> <p>Landfalling atmospheric rivers (ARs) affect the wintertime <span class="hlt">surface</span> <span class="hlt">air</span> temperatures as shown in earlier studies. The AR-related <span class="hlt">surface</span> <span class="hlt">air</span> temperatures can exert significant influence on the hydrology in the US Pacific coast region especially through rainfall-snowfall partitioning and the snowpack in high elevation watersheds as they are directly related with the freezing-level altitudes. These effects of temperature perturbations can in turn affect hydrologic events of various time scales such as flash flooding by the combined effects of rainfall and snowmelt, and the warm season runoff from melting snowpack, especially in conjunction with the AR effects on winter precipitation and rain-on-snow events in WUS. Thus, understanding the effects of AR landfalls on the <span class="hlt">surface</span> temperatures and examining the capability of climate <span class="hlt">models</span> in simulating these effects are an important practical concern for WUS. This study aims to understand the effects of AR landfalls on the characteristics of <span class="hlt">surface</span> <span class="hlt">air</span> temperatures in WUS, especially seasonal means and PDFs and to evaluate the fidelity of <span class="hlt">model</span> data produced in the NASA downscaling experiment for the 10 winters from Nov. 1999 to Mar. 2010 using an AR-landfall chronology based on the vertically-integrated water vapor flux calculated from the MERRA2 reanalysis. <span class="hlt">Model</span> skill is measured using metrics including regional means, a skill score based on correlations and mean-square errors, the similarity between two PDF shapes, and Taylor diagrams. Results show that the AR landfalls are related with higher <span class="hlt">surface</span> <span class="hlt">air</span> temperatures in WUS, especially in inland regions. The AR landfalls also reduce the range of <span class="hlt">surface</span> <span class="hlt">air</span> temperature PDF, largely by reducing the events in the lower temperature range. The shift in the <span class="hlt">surface</span> <span class="hlt">air</span> temperature PDF is consistent with the positive anomalies in the winter-mean temperature. <span class="hlt">Model</span> data from the NASA downscaling experiment reproduce the AR effects on the temperature PDF, at least</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('https://www.ncbi.nlm.nih.gov/pubmed/26672387','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26672387"><span><span class="hlt">Modeling</span> packed bed sorbent systems with the Pore <span class="hlt">Surface</span> Diffusion <span class="hlt">Model</span>: Evidence of facilitated <span class="hlt">surface</span> diffusion of arsenate in nano-metal (hydr)oxide hybrid ion <span class="hlt">exchange</span> media.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dale, Sachie; Markovski, Jasmina; Hristovski, Kiril D</p> <p>2016-09-01</p> <p>This study explores the possibility of employing the Pore <span class="hlt">Surface</span> Diffusion <span class="hlt">Model</span> (PSDM) to predict the arsenic breakthrough curve of a packed bed system operated under continuous flow conditions with realistic groundwater, and consequently minimize the need to conduct pilot scale tests. To provide the nano-metal (hydr)oxide hybrid ion <span class="hlt">exchange</span> media's performance in realistic water matrices without engaging in taxing pilot scale testing, the multi-point equilibrium batch sorption tests under pseudo-equilibrium conditions were performed; arsenate breakthrough curve of short bed column (SBC) was predicted by the PSDM in the continuous flow experiments; SBC tests were conducted under the same conditions to validate the <span class="hlt">model</span>. The overlapping Freundlich isotherms suggested that the water matrix and competing ions did not have any denoting effect on sorption capacity of the media when the matrix was changed from arsenic-only <span class="hlt">model</span> water to real groundwater. As expected, the PSDM provided a relatively good prediction of the breakthrough profile for arsenic-only <span class="hlt">model</span> water limited by intraparticle mass transports. In contrast, the groundwater breakthrough curve demonstrated significantly faster intraparticle mass transport suggesting to a <span class="hlt">surface</span> diffusion process, which occurs in parallel to the pore diffusion. A simple selection of DS=1/2 DP appears to be sufficient when describing the facilitated <span class="hlt">surface</span> diffusion of arsenate inside metal (hydr)oxide nano-enabled hybrid ion-<span class="hlt">exchange</span> media in presence of sulfate, however, quantification of the factors determining the <span class="hlt">surface</span> diffusion coefficient's magnitude under different treatment scenarios remained unexplored. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15914236','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15914236"><span>Passive <span class="hlt">air</span> sampling theory for semivolatile organic compounds.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bartkow, Michael E; Booij, Kees; Kennedy, Karen E; Müller, Jochen F; Hawker, Darryl W</p> <p>2005-07-01</p> <p>The mathematical <span class="hlt">modelling</span> underlying passive <span class="hlt">air</span> sampling theory can be based on mass transfer coefficients or rate constants. Generally, these <span class="hlt">models</span> have not been inter-related. Starting with basic <span class="hlt">models</span>, the <span class="hlt">exchange</span> of chemicals between the gaseous phase and the sampler is developed using mass transfer coefficients and rate constants. Importantly, the inter-relationships between the approaches are demonstrated by relating uptake rate constants and loss rate constants to mass transfer coefficients when either sampler-side or <span class="hlt">air</span>-side resistance is dominating chemical <span class="hlt">exchange</span>. The influence of sampler area and sampler volume on chemical <span class="hlt">exchange</span> is discussed in general terms and as they relate to frequently used parameters such as sampling rates and time to equilibrium. Where <span class="hlt">air</span>-side or sampler-side resistance dominates, an increase in the <span class="hlt">surface</span> area of the sampler will increase sampling rates. Sampling rates are not related to the sampler/<span class="hlt">air</span> partition coefficient (K(SV)) when <span class="hlt">air</span>-side resistance dominates and increase with K(SV) when sampler-side resistance dominates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24997510','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24997510"><span>Unfolding of a <span class="hlt">model</span> protein on ion <span class="hlt">exchange</span> and mixed mode chromatography <span class="hlt">surfaces</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gospodarek, Adrian M; Hiser, Diana E; O'Connell, John P; Fernandez, Erik J</p> <p>2014-08-15</p> <p>Recent studies with proteins indicate that conformational changes and aggregation can occur during ion <span class="hlt">exchange</span> chromatography (IEC). Such behavior is not usually expected, but could lead to decreased yield and product degradation from both IEC and multi mode chromatography (MMC) that has ligands of both hydrophobic and charged functionalities. In this study, we used hydrogen <span class="hlt">exchange</span> mass spectrometry to investigate unfolding of the <span class="hlt">model</span> protein BSA on IEC and MMC <span class="hlt">surfaces</span> under different solution conditions at 25°C. Increased solvent exposure, indicating greater unfolding relative to that in solution, was found for protein adsorbed on cationic IEC and MMC <span class="hlt">surfaces</span> in the pH range of 3.0 to 4.5, where BSA has decreased stability in solution. There was no effect of anionic <span class="hlt">surfaces</span> at pH values in the range from 6.0 to 9.0. Differences of solvent exposure of whole molecules when adsorbed and in solution suggest that adsorbed BSA unfolds at lower pH values and may show aggregation, depending upon pH and the <span class="hlt">surface</span> type. Measurements on digested peptides showed that classifications of stability can be made for various regions; these are generally retained as pH is changed. When salt was added to MMC systems, where electrostatic interactions would be minimized, less solvent exposure was seen, implying that it is the cationic moieties, rather than the hydrophobic ligands, which cause greater <span class="hlt">surface</span> unfolding at low salt concentrations. These results suggest that proteins of lower stability may exhibit unfolding and aggregation during IEC and MMC separations, as they can with hydrophobic interaction chromatography. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28486355','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28486355"><span><span class="hlt">Air</span>-Abrasive Disinfection of Implant <span class="hlt">Surfaces</span> in a Simulated <span class="hlt">Model</span> of Periimplantitis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Quintero, David George; Taylor, Robert Bonnie; Miller, Matthew Braden; Merchant, Keith Roshanali; Pasieta, Scott Anthony</p> <p>2017-06-01</p> <p>This in vitro study aimed to evaluate the ability of <span class="hlt">air</span>-powder abrasion to decontaminate dental implants. Twenty-six implants were inoculated with a Streptococcus sanguinis biofilm media in a novel periimplantitis defect <span class="hlt">model</span>. Six implants served as controls, and 20 implants were disinfected with either the Cavitron JET Plus or the <span class="hlt">AIR</span>-FLOW PERIO <span class="hlt">air</span>-powder abrasion units. Residual bacteria were cultured, and colony forming units (CFUs) were totaled at 24 hours. As expected, negative control implant cultures showed no evidence of viable bacteria. Bacterial growth was observed on all positive control cultures, whereas only 15% of the experimental cultures displayed evidence of viable bacteria. The average CFU per streak for the positive control was 104 compared with a maximum of 10 and 4 CFUs for the Cavitron JET Plus and <span class="hlt">AIR</span>-FLOW PERIO, respectively. There was a 99.9% reduction in bacteria for both <span class="hlt">air</span>-powder abrasion instruments. <span class="hlt">Air</span>-powder abrasion is an effective technique for the decontamination of dental implants, and the Cavitron JET Plus and <span class="hlt">AIR</span>-FLOW PERIO are equally successful at eliminating viable bacteria from implant <span class="hlt">surfaces</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16271812','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16271812"><span>Atmospheric concentrations and <span class="hlt">air</span>-sea <span class="hlt">exchanges</span> of nonylphenol, tertiary octylphenol and nonylphenol monoethoxylate in the North Sea.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xie, Zhiyong; Lakaschus, Soenke; Ebinghaus, Ralf; Caba, Armando; Ruck, Wolfgang</p> <p>2006-07-01</p> <p>Concentrations of nonylphenol isomers (NP), tertiary octylphenol (t-OP) and nonylphenol monoethoxylate isomers (NP1EO) have been simultaneously determined in the sea water and atmosphere of the North Sea. A decreasing concentration profile appeared following the distance increasing from the coast to the central part of the North Sea. <span class="hlt">Air</span>-sea <span class="hlt">exchanges</span> of t-OP and NP were estimated using the two-film resistance <span class="hlt">model</span> based upon relative <span class="hlt">air</span>-water concentrations and experimentally derived Henry's law constant. The average of <span class="hlt">air</span>-sea <span class="hlt">exchange</span> fluxes was -12+/-6 ng m(-2)day(-1) for t-OP and -39+/-19 ng m(-2)day(-1) for NP, which indicates a net deposition is occurring. These results suggest that the <span class="hlt">air</span>-sea vapour <span class="hlt">exchange</span> is an important process that intervenes in the mass balance of alkylphenols in the North Sea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070032692','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070032692"><span>Land <span class="hlt">Surface</span> Process and <span class="hlt">Air</span> Quality Research and Applications at MSFC</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Quattrochi, Dale; Khan, Maudood</p> <p>2007-01-01</p> <p>This viewgraph presentation provides an overview of land <span class="hlt">surface</span> process and <span class="hlt">air</span> quality research at MSFC including atmospheric <span class="hlt">modeling</span> and ongoing research whose objective is to undertake a comprehensive spatiotemporal analysis of the effects of accurate land <span class="hlt">surface</span> characterization on atmospheric <span class="hlt">modeling</span> results, and public health applications. Land use maps as well as 10 meter <span class="hlt">air</span> temperature, <span class="hlt">surface</span> wind, PBL mean difference heights, NOx, ozone, and O3+NO2 plots as well as spatial growth <span class="hlt">model</span> outputs are included. Emissions and general <span class="hlt">air</span> quality <span class="hlt">modeling</span> are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=337693&Lab=NERL&keyword=forensics&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=337693&Lab=NERL&keyword=forensics&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><span class="hlt">Modeling</span> and Measurements to Improve Bidirectional <span class="hlt">Exchange</span> in CMAQ</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>Ammonia, NH3, is an emerging atmospheric pollutant of interest. It is an aerosol precursor and growing constituent of nitrogen deposition. In this presentation, the bidirectional <span class="hlt">exchange</span> <span class="hlt">model</span> for NH¬3 in the Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span> will be reviewed and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=335741&Lab=NERL&keyword=forensics&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=335741&Lab=NERL&keyword=forensics&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>Recent Enhancements to the Community Multiscale <span class="hlt">Air</span> Quality <span class="hlt">Model</span> (CMAQ)</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>This presentation overviews recent updates to the CMAQ <span class="hlt">modeling</span> system. The presentation will be given as part of the information <span class="hlt">exchange</span> session on Regional <span class="hlt">Air</span> Pollution <span class="hlt">Modeling</span> at the UK-US Collaboration Meeting on <span class="hlt">Air</span> Pollution Exposure Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.220..291T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.220..291T"><span><span class="hlt">Modeling</span> uranium(VI) adsorption onto montmorillonite under varying carbonate concentrations: A <span class="hlt">surface</span> complexation <span class="hlt">model</span> accounting for the spillover effect on <span class="hlt">surface</span> potential</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tournassat, C.; Tinnacher, R. M.; Grangeon, S.; Davis, J. A.</p> <p>2018-01-01</p> <p>The prediction of U(VI) adsorption onto montmorillonite clay is confounded by the complexities of: (1) the montmorillonite structure in terms of adsorption sites on basal and edge <span class="hlt">surfaces</span>, and the complex interactions between the electrical double layers at these <span class="hlt">surfaces</span>, and (2) U(VI) solution speciation, which can include cationic, anionic and neutral species. Previous U(VI)-montmorillonite adsorption and <span class="hlt">modeling</span> studies have typically expanded classical <span class="hlt">surface</span> complexation <span class="hlt">modeling</span> approaches, initially developed for simple oxides, to include both cation <span class="hlt">exchange</span> and <span class="hlt">surface</span> complexation reactions. However, previous <span class="hlt">models</span> have not taken into account the unique characteristics of electrostatic <span class="hlt">surface</span> potentials that occur at montmorillonite edge sites, where the electrostatic <span class="hlt">surface</span> potential of basal plane cation <span class="hlt">exchange</span> sites influences the <span class="hlt">surface</span> potential of neighboring edge sites ('spillover' effect). A series of U(VI) - Na-montmorillonite batch adsorption experiments was conducted as a function of pH, with variable U(VI), Ca, and dissolved carbonate concentrations. Based on the experimental data, a new type of <span class="hlt">surface</span> complexation <span class="hlt">model</span> (SCM) was developed for montmorillonite, that specifically accounts for the spillover effect using the edge <span class="hlt">surface</span> speciation <span class="hlt">model</span> by Tournassat et al. (2016a). The SCM allows for a prediction of U(VI) adsorption under varying chemical conditions with a minimum number of fitting parameters, not only for our own experimental results, but also for a number of published data sets. The <span class="hlt">model</span> agreed well with many of these datasets without introducing a second site type or including the formation of ternary U(VI)-carbonato <span class="hlt">surface</span> complexes. The <span class="hlt">model</span> predictions were greatly impacted by utilizing analytical measurements of dissolved inorganic carbon (DIC) concentrations in individual sample solutions rather than assuming solution equilibration with a specific partial pressure of CO2, even when the gas phase was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/864049','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864049"><span>Fluidized bed heat <span class="hlt">exchanger</span> with water cooled <span class="hlt">air</span> distributor and dust hopper</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Jukkola, Walfred W.; Leon, Albert M.; Van Dyk, Jr., Garritt C.; McCoy, Daniel E.; Fisher, Barry L.; Saiers, Timothy L.; Karstetter, Marlin E.</p> <p>1981-11-24</p> <p>A fluidized bed heat <span class="hlt">exchanger</span> is provided in which <span class="hlt">air</span> is passed through a bed of particulate material containing fuel. A steam-water natural circulation system is provided for heat <span class="hlt">exchange</span> and the housing of the heat <span class="hlt">exchanger</span> has a water-wall type construction. Vertical in-bed heat <span class="hlt">exchange</span> tubes are provided and the <span class="hlt">air</span> distributor is water-cooled. A water-cooled dust hopper is provided in the housing to collect particulates from the combustion gases and separate the combustion zone from a volume within said housing in which convection heat <span class="hlt">exchange</span> tubes are provided to extract heat from the exiting combustion gases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1212391','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1212391"><span>Metal-<span class="hlt">air</span> cell with ion <span class="hlt">exchange</span> material</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Friesen, Cody A.; Wolfe, Derek; Johnson, Paul Bryan</p> <p>2015-08-25</p> <p>Embodiments of the invention are related to anion <span class="hlt">exchange</span> membranes used in electrochemical metal-<span class="hlt">air</span> cells in which the membranes function as the electrolyte material, or are used in conjunction with electrolytes such as ionic liquid electrolytes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150020902','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150020902"><span>Technology Candidates for <span class="hlt">Air-to-Air</span> and <span class="hlt">Air</span>-to-Ground Data <span class="hlt">Exchange</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Haynes, Brian D.</p> <p>2015-01-01</p> <p>Technology Candidates for <span class="hlt">Air-to-Air</span> and <span class="hlt">Air</span>-to-Ground Data <span class="hlt">Exchange</span> is a two-year research effort to visualize the U. S. aviation industry at a point 50 years in the future, and to define potential communication solutions to meet those future data <span class="hlt">exchange</span> needs. The research team, led by XCELAR, was tasked with identifying future National Airspace System (NAS) scenarios, determining requirements and functions (including gaps), investigating technical and business issues for <span class="hlt">air</span>, ground, & <span class="hlt">air</span>-to-ground interactions, and reporting on the results. The project was conducted under technical direction from NASA and in collaboration with XCELAR's partner, National Institute of Aerospace, and NASA technical representatives. Parallel efforts were initiated to define the information <span class="hlt">exchange</span> functional needs of the future NAS, and specific communication link technologies to potentially serve those needs. Those efforts converged with the mapping of each identified future NAS function to potential enabling communication solutions; those solutions were then compared with, and ranked relative to, each other on a technical basis in a structured analysis process. The technical solutions emerging from that process were then assessed from a business case perspective to determine their viability from a real-world adoption and deployment standpoint. The results of that analysis produced a proposed set of future solutions and most promising candidate technologies. Gap analyses were conducted at two points in the process, the first examining technical factors, and the second as part of the business case analysis. In each case, no gaps or unmet needs were identified in applying the solutions evaluated to the requirements identified. The future communication solutions identified in the research comprise both specific link technologies and two enabling technologies that apply to most or all specific links. As a result, the research resulted in a new analysis approach, viewing the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.B11I..08O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.B11I..08O"><span>CentNet—A deployable 100-station network for <span class="hlt">surface</span> <span class="hlt">exchange</span> research</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oncley, S.; Horst, T. W.; Semmer, S.; Militzer, J.; Maclean, G.; Knudson, K.</p> <p>2014-12-01</p> <p>Climate, <span class="hlt">air</span> quality, atmospheric composition, <span class="hlt">surface</span> hydrology, and ecological processes are directly affected by the Earth's <span class="hlt">surface</span>. Complexity of this <span class="hlt">surface</span> exists at multiple spatial scales, which complicates the understanding of these processes. NCAR/EOL currently provides a facility to the research community to make direct eddy-covariance flux observations to quantify <span class="hlt">surface</span>-atmosphere interactions. However, just as <span class="hlt">model</span> resolution has continued to increase, there is a need to increase the spatial density of flux measurements to capture the wide variety of scales that contribute to <span class="hlt">exchange</span> processes close to the <span class="hlt">surface</span>. NCAR/EOL now has developed the CentNet facility, that is envisioned to have on the order of 100 <span class="hlt">surface</span> flux stations deployable for periods of months to years. Each station would measure standard meteorological variables, all components of the <span class="hlt">surface</span> energy balance (including turbulence fluxes and radiation), atmospheric composition, and other quantities to characterize the <span class="hlt">surface</span>. Thus, CentNet can support observational research in the biogeosciences, hydrology, urban meteorology, basic meteorology, and turbulence. CentNet has been designed to be adaptable to a wide variety of research problems while keeping operations manageable. Tower infrastructure has been designed to be lightweight, easily deployed, and with a minimal set-up footprint. CentNet uses sensor networks to increase spatial sampling at each station. The data system saves every sample on site to retain flexibility in data analysis. We welcome guidance on development and funding priorities as we build CentNet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24184550','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24184550"><span>Organochlorine pesticides in <span class="hlt">surface</span> soils from obsolete pesticide dumping ground in Hyderabad City, Pakistan: contamination levels and their potential for <span class="hlt">air</span>-soil <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alamdar, Ambreen; Syed, Jabir Hussain; Malik, Riffat Naseem; Katsoyiannis, Athanasios; Liu, Junwen; Li, Jun; Zhang, Gan; Jones, Kevin C</p> <p>2014-02-01</p> <p>This study was conducted to examine organochlorine pesticides (OCPs) contamination levels in the <span class="hlt">surface</span> soil and <span class="hlt">air</span> samples together with <span class="hlt">air</span>-soil <span class="hlt">exchange</span> fluxes at an obsolete pesticide dumping ground and the associated areas from Hyderabad City, Pakistan. Among all the sampling sites, concentrations of OCPs in the soil and <span class="hlt">air</span> samples were found highest in obsolete pesticide dumping ground, whereas dominant contaminants were dichlorodiphenyltrichloroethane (DDTs) (soil: 77-212,200 ng g(-1); <span class="hlt">air</span>: 90,700 pg m(-3)) and hexachlorocyclohexane (HCHs) (soil: 43-4,090 ng g(-1); <span class="hlt">air</span>: 97,400 pg m(-3)) followed by chlordane, heptachlor and hexachlorobenzene (HCB). OCPs diagnostic indicative ratios reflect historical use as well as fresh input in the study area. Moreover, the <span class="hlt">air</span> and soil fugacity ratios (0.9-1.0) at the dumping ground reflecting a tendency towards net volatilization of OCPs, while at the other sampling sites, the fugacity ratios indicate in some cases deposition and in other cases volatilization. Elevated concentrations of DDTs and HCHs at pesticide dumping ground and its surroundings pose potential exposure risk to biological organisms, to the safety of agricultural products and to the human health. Our study thus emphasizes the need of spatio-temporal monitoring of OCPs at local and regional scale to assess and remediate the future adverse implications. © 2013.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308482&keyword=temperature+AND+variability&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=308482&keyword=temperature+AND+variability&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>Exposure <span class="hlt">Modeling</span> of Residential <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rates for NEXUS Participants</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>Due to cost and participant burden of personal measurements, <span class="hlt">air</span> pollution health studies often estimate exposures using local ambient <span class="hlt">air</span> monitors. Since outdoor levels do not necessarily reflect personal exposures, we developed the Exposure <span class="hlt">Model</span> for Individuals (EMI) to improv...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=311909&Lab=NERL&keyword=wind&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=311909&Lab=NERL&keyword=wind&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>Exposure <span class="hlt">Modeling</span> of Residential <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rates for NEXUS Participants.</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>Due to cost and participant burden of personal measurements, <span class="hlt">air</span> pollution health studies often estimate exposures using local ambient <span class="hlt">air</span> monitors. Since outdoor levels do not necessarily reflect personal exposures, we developed the Exposure <span class="hlt">Model</span> for Individuals (EMI) to improv...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12719071','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12719071"><span>Experimental study of viscoelastic in the prevention of corneal endothelial desiccation injury from vitreal fluid-<span class="hlt">air</span> <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cekiç, Osman; Ohji, Masahito; Zheng, Yuping; Hayashi, Atsushi; Kusaka, Shunji; Tano, Yasuo</p> <p>2003-05-01</p> <p>To evaluate the usefulness of viscoelastic in protecting the corneal endothelium from desiccation injury associated with fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> in a rabbit <span class="hlt">model</span>. Experimental study. Rabbit eyes undergoing pars plana lensectomy and vitrectomy were insufflated with either dry or humidified <span class="hlt">air</span> for 20 minutes following introduction of either Opegan (sodium hyaluronate 1.0%; Santen, Osaka, Japan) or Viscoat (sodium hyaluronate 3%-chondroitin sulfate 4%; Alcon, Tokyo, Japan) into the anterior chamber. In two other groups of rabbit eyes, the same procedure was performed without using any viscoelastic agent. Corneas obtained from rabbits undergoing surgery were compared with corneas obtained from rabbits not undergoing surgery. Potential alterations in the corneal endothelium were investigated by scanning electron microscopy, by Phalloidin-FITC staining of actin and by in vitro measurements of corneal permeability for carboxyfluorescein using a diffusion chamber. Scanning electron microscopy displayed less distortion of corneal endothelium with Opegan and Viscoat compared with the dry <span class="hlt">air</span>-only exposed corneas. Using humidified <span class="hlt">air</span> in Opegan and Viscoat coated corneas maintained the normal actin cytoskeleton during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span>. Paracellular leakage was much less with Opegan and Viscoat use following infusion of dry <span class="hlt">air</span> comparing to that of dry <span class="hlt">air</span>-only group (P =.026 and P =.041). The difference was much more striking following humidified <span class="hlt">air</span> infusion in Opegan or Viscoat coated corneas comparing to dry <span class="hlt">air</span>-only infused corneas (P <.002 and P <.002). Coating of rabbit corneal endothelium with Opegan or Viscoat before fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> largely prevents dry <span class="hlt">air</span> damage to the endothelium. Infusion of humidified <span class="hlt">air</span> further protects corneal endothelium during fluid-<span class="hlt">air</span> <span class="hlt">exchange</span> in aphakic rabbit eyes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EPJWC..6702023D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EPJWC..6702023D"><span>Heat <span class="hlt">exchanger</span> design for hot <span class="hlt">air</span> ericsson-brayton piston engine</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ďurčanský, P.; Lenhard, R.; Jandačka, J.</p> <p>2014-03-01</p> <p>One of the solutions without negative consequences for the increasing energy consumption in the world may be use of alternative energy sources in micro-cogeneration. Currently it is looking for different solutions and there are many possible ways. Cogeneration is known for long time and is widely used. But the installations are often large and the installed output is more suitable for cities or industry companies. When we will speak about decentralization, the small machines have to be used. The article deals with the principle of hot-<span class="hlt">air</span> engines, their use in combined heat and electricity production from biomass and with heat <span class="hlt">exchangers</span> as primary energy transforming element. In the article is hot <span class="hlt">air</span> engine presented as a heat engine that allows the conversion of heat into mechanical energy while heat supply can be external. In the contribution are compared cycles of hot-<span class="hlt">air</span> engine. Then are compared suitable heat <span class="hlt">exchangers</span> for use with hot <span class="hlt">air</span> Ericsson-Brayton engine. In the final part is proposal of heat <span class="hlt">exchanger</span> for use in closed Ericsson-Brayton cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGeo...10.5183F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGeo...10.5183F"><span>Advances in understanding, <span class="hlt">models</span> and parameterizations of biosphere-atmosphere ammonia <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flechard, C. R.; Massad, R.-S.; Loubet, B.; Personne, E.; Simpson, D.; Bash, J. O.; Cooter, E. J.; Nemitz, E.; Sutton, M. A.</p> <p>2013-07-01</p> <p>Atmospheric ammonia (NH3) dominates global emissions of total reactive nitrogen (Nr), while emissions from agricultural production systems contribute about two-thirds of global NH3 emissions; the remaining third emanates from oceans, natural vegetation, humans, wild animals and biomass burning. On land, NH3 emitted from the various sources eventually returns to the biosphere by dry deposition to sink areas, predominantly semi-natural vegetation, and by wet and dry deposition as ammonium (NH4+) to all <span class="hlt">surfaces</span>. However, the land/atmosphere <span class="hlt">exchange</span> of gaseous NH3 is in fact bi-directional over unfertilized as well as fertilized ecosystems, with periods and areas of emission and deposition alternating in time (diurnal, seasonal) and space (patchwork landscapes). The <span class="hlt">exchange</span> is controlled by a range of environmental factors, including meteorology, <span class="hlt">surface</span> layer turbulence, thermodynamics, <span class="hlt">air</span> and <span class="hlt">surface</span> heterogeneous-phase chemistry, canopy geometry, plant development stage, leaf age, organic matter decomposition, soil microbial turnover, and, in agricultural systems, by fertilizer application rate, fertilizer type, soil type, crop type, and agricultural management practices. We review the range of processes controlling NH3 emission and uptake in the different parts of the soil-canopy-atmosphere continuum, with NH3 emission potentials defined at the substrate and leaf levels by different [NH4+] / [H+] ratios (Γ). <span class="hlt">Surface</span>/atmosphere <span class="hlt">exchange</span> <span class="hlt">models</span> for NH3 are necessary to compute the temporal and spatial patterns of emissions and deposition at the soil, plant, field, landscape, regional and global scales, in order to assess the multiple environmental impacts of airborne and deposited NH3 and NH4+. <span class="hlt">Models</span> of soil/vegetation/atmosphere NH3 <span class="hlt">exchange</span> are reviewed from the substrate and leaf scales to the global scale. They range from simple steady-state, "big leaf" canopy resistance <span class="hlt">models</span>, to dynamic, multi-layer, multi-process, multi-chemical species schemes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002539','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002539"><span>Assessing <span class="hlt">Air</span>-Sea Interaction in the Evolving NASA GEOS <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clayson, Carol Anne; Roberts, J. Brent</p> <p>2015-01-01</p> <p>In order to understand how the climate responds to variations in forcing, one necessary component is to understand the full distribution of variability of <span class="hlt">exchanges</span> of heat and moisture between the atmosphere and ocean. <span class="hlt">Surface</span> heat and moisture fluxes are critical to the generation and decay of many coupled <span class="hlt">air</span>-sea phenomena. These mechanisms operate across a number of scales and contain contributions from interactions between the anomalous (i.e. non-mean), often extreme-valued, flux components. Satellite-derived estimates of the <span class="hlt">surface</span> turbulent and radiative heat fluxes provide an opportunity to assess results from <span class="hlt">modeling</span> systems. Evaluation of only time mean and variability statistics, however only provides limited traceability to processes controlling what are often regime-dependent errors. This work will present an approach to evaluate the representation of the turbulent fluxes at the <span class="hlt">air</span>-sea interface in the current and evolving Goddard Earth Observing System (GEOS) <span class="hlt">model</span>. A temperature and moisture vertical profile-based clustering technique is used to identify robust weather regimes, and subsequently intercompare the turbulent fluxes and near-<span class="hlt">surface</span> parameters within these regimes in both satellite estimates and GEOS-driven data sets. Both <span class="hlt">model</span> reanalysis (MERRA) and seasonal-to-interannual coupled GEOS <span class="hlt">model</span> simulations will be evaluated. Particular emphasis is placed on understanding the distribution of the fluxes including extremes, and the representation of near-<span class="hlt">surface</span> forcing variables directly related to their estimation. Results from these analyses will help identify the existence and source of regime-dependent biases in the GEOS <span class="hlt">model</span> ocean <span class="hlt">surface</span> turbulent fluxes. The use of the temperature and moisture profiles for weather-state clustering will be highlighted for its potential broad application to 3-D output typical of <span class="hlt">model</span> simulations.</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/2014AGUFM.A41P..05C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A41P..05C"><span>Assessing <span class="hlt">air</span>-sea interaction in the evolving NASA GEOS <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clayson, C. A.; Roberts, J. B.</p> <p>2014-12-01</p> <p>In order to understand how the climate responds to variations in forcing, one necessary component is to understand the full distribution of variability of <span class="hlt">exchanges</span> of heat and moisture between the atmosphere and ocean. <span class="hlt">Surface</span> heat and moisture fluxes are critical to the generation and decay of many coupled <span class="hlt">air</span>-sea phenomena. These mechanisms operate across a number of scales and contain contributions from interactions between the anomalous (i.e. non-mean), often extreme-valued, flux components. Satellite-derived estimates of the <span class="hlt">surface</span> turbulent and radiative heat fluxes provide an opportunity to assess results from <span class="hlt">modeling</span> systems. Evaluation of only time mean and variability statistics, however only provides limited traceability to processes controlling what are often regime-dependent errors. This work will present an approach to evaluate the representation of the turbulent fluxes at the <span class="hlt">air</span>-sea interface in the current and evolving Goddard Earth Observing System (GEOS) <span class="hlt">model</span>. A temperature and moisture vertical profile-based clustering technique is used to identify robust weather regimes, and subsequently intercompare the turbulent fluxes and near-<span class="hlt">surface</span> parameters within these regimes in both satellite estimates and GEOS-driven data sets. Both <span class="hlt">model</span> reanalysis (MERRA) and seasonal-to-interannual coupled GEOS <span class="hlt">model</span> simulations will be evaluated. Particular emphasis is placed on understanding the distribution of the fluxes including extremes, and the representation of near-<span class="hlt">surface</span> forcing variables directly related to their estimation. Results from these analyses will help identify the existence and source of regime-dependent biases in the GEOS <span class="hlt">model</span> ocean <span class="hlt">surface</span> turbulent fluxes. The use of the temperature and moisture profiles for weather-state clustering will be highlighted for its potential broad application to 3-D output typical of <span class="hlt">model</span> simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21141036','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21141036"><span>Advances in quantifying <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> and environmental forcing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wanninkhof, Rik; Asher, William E; Ho, David T; Sweeney, Colm; McGillis, Wade R</p> <p>2009-01-01</p> <p>The past decade has seen a substantial amount of research on <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> and its environmental controls. These studies have significantly advanced the understanding of processes that control gas transfer, led to higher quality field measurements, and improved estimates of the flux of climate-relevant gases between the ocean and atmosphere. This review discusses the fundamental principles of <span class="hlt">air</span>-sea gas transfer and recent developments in gas transfer theory, parameterizations, and measurement techniques in the context of the <span class="hlt">exchange</span> of carbon dioxide. However, much of this discussion is applicable to any sparingly soluble, non-reactive gas. We show how the use of global variables of environmental forcing that have recently become available and gas <span class="hlt">exchange</span> relationships that incorporate the main forcing factors will lead to improved estimates of global and regional <span class="hlt">air</span>-sea gas fluxes based on better fundamental physical, chemical, and biological foundations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007890','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007890"><span>Estimation of <span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature from MODIS 1km Resolution Land <span class="hlt">Surface</span> Temperature Over Northern China</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shen, Suhung; Leptoukh, Gregory G.; Gerasimov, Irina</p> <p>2010-01-01</p> <p><span class="hlt">Surface</span> <span class="hlt">air</span> temperature is a critical variable to describe the energy and water cycle of the Earth-atmosphere system and is a key input element for hydrology and land <span class="hlt">surface</span> <span class="hlt">models</span>. It is a very important variable in agricultural applications and climate change studies. This is a preliminary study to examine statistical relationships between ground meteorological station measured <span class="hlt">surface</span> daily maximum/minimum <span class="hlt">air</span> temperature and satellite remotely sensed land <span class="hlt">surface</span> temperature from MODIS over the dry and semiarid regions of northern China. Studies were conducted for both MODIS-Terra and MODIS-Aqua by using year 2009 data. Results indicate that the relationships between <span class="hlt">surface</span> <span class="hlt">air</span> temperature and remotely sensed land <span class="hlt">surface</span> temperature are statistically significant. The relationships between the maximum <span class="hlt">air</span> temperature and daytime land <span class="hlt">surface</span> temperature depends significantly on land <span class="hlt">surface</span> types and vegetation index, but the minimum <span class="hlt">air</span> temperature and nighttime land <span class="hlt">surface</span> temperature has little dependence on the <span class="hlt">surface</span> conditions. Based on linear regression relationship between <span class="hlt">surface</span> <span class="hlt">air</span> temperature and MODIS land <span class="hlt">surface</span> temperature, <span class="hlt">surface</span> maximum and minimum <span class="hlt">air</span> temperatures are estimated from 1km MODIS land <span class="hlt">surface</span> temperature under clear sky conditions. The statistical errors (sigma) of the estimated daily maximum (minimum) <span class="hlt">air</span> temperature is about 3.8 C(3.7 C).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790060856&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790060856&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries"><span>A <span class="hlt">model</span> of the planetary boundary layer over a snow <span class="hlt">surface</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Halberstam, I.; Melendez, R.</p> <p>1979-01-01</p> <p>A <span class="hlt">model</span> of the planetary boundary layer over a snow <span class="hlt">surface</span> has been developed. It contains the vertical heat <span class="hlt">exchange</span> processes due to radiation, conduction, and atmospheric turbulence. Parametrization of the boundary layer is based on similarity functions developed by Hoffert and Sud (1976), which involve a dimensionless variable, dependent on boundary-layer height and a localized Monin-Obukhov length. The <span class="hlt">model</span> also contains the atmospheric <span class="hlt">surface</span> layer and the snowpack itself, where snowmelt and snow evaporation are calculated. The results indicate a strong dependence of <span class="hlt">surface</span> temperatures, especially at night, on the bursts of turbulence which result from the frictional damping of <span class="hlt">surface</span>-layer winds during periods of high stability, as described by Businger (1973). The <span class="hlt">model</span> also shows the cooling and drying effect of the snow on the atmosphere, which may be the mechanism for <span class="hlt">air</span> mass transformation in sub-Arctic regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830046452&hterms=water+gas+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwater%2Bgas%2Bexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830046452&hterms=water+gas+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwater%2Bgas%2Bexchange"><span>Methane flux across the <span class="hlt">air</span>-water interface - <span class="hlt">Air</span> velocity effects</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sebacher, D. I.; Harriss, R. C.; Bartlett, K. B.</p> <p>1983-01-01</p> <p>Methane loss to the atmosphere from flooded wetlands is influenced by the degree of supersaturation and wind stress at the water <span class="hlt">surface</span>. Measurements in freshwater ponds in the St. Marks Wildlife Refuge, Florida, demonstrated that for the combined variability of CH4 concentrations in <span class="hlt">surface</span> water and <span class="hlt">air</span> velocity over the water <span class="hlt">surface</span>, CH4 flux varied from 0.01 to 1.22 g/sq m/day. The liquid <span class="hlt">exchange</span> coefficient for a two-layer <span class="hlt">model</span> of the gas-liquid interface was calculated as 1.7 cm/h for CH4 at <span class="hlt">air</span> velocity of zero and as 1.1 + 1.2 v to the 1.96th power cm/h for <span class="hlt">air</span> velocities from 1.4 to 3.5 m/s and water temperatures of 20 C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27460608','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27460608"><span>Oxygen <span class="hlt">exchange</span> at gas/oxide interfaces: how the apparent activation energy of the <span class="hlt">surface</span> <span class="hlt">exchange</span> coefficient depends on the kinetic regime.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fielitz, Peter; Borchardt, Günter</p> <p>2016-08-10</p> <p>In the dedicated literature the oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> coefficient KO and the equilibrium oxygen <span class="hlt">exchange</span> rate [Fraktur R] are considered to be directly proportional to each other regardless of the experimental circumstances. Recent experimental observations, however, contradict the consequences of this assumption. Most surprising is the finding that the apparent activation energy of KO depends dramatically on the kinetic regime in which it has been determined, i.e. <span class="hlt">surface</span> <span class="hlt">exchange</span> controlled vs. mixed or diffusion controlled. This work demonstrates how the diffusion boundary condition at the gas/solid interface inevitably entails a correlation between the oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> coefficient KO and the oxygen self-diffusion coefficient DO in the bulk ("on top" of the correlation between KO and [Fraktur R] for the pure <span class="hlt">surface</span> <span class="hlt">exchange</span> regime). The <span class="hlt">model</span> can thus quantitatively explain the range of apparent activation energies measured in the different regimes: in the <span class="hlt">surface</span> <span class="hlt">exchange</span> regime the apparent activation energy only contains the contribution of the equilibrium <span class="hlt">exchange</span> rate, whereas in the mixed or in the diffusion controlled regime the contribution of the oxygen self-diffusivity has also to be taken into account, which may yield significantly higher apparent activation energies and simultaneously quantifies the correlation KO ∝ DO(1/2) observed for a large number of oxides in the mixed or diffusion controlled regime, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001PhDT.......266B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001PhDT.......266B"><span>On the physical <span class="hlt">air</span>-sea fluxes for climate <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bonekamp, J. G.</p> <p>2001-02-01</p> <p>At the sea <span class="hlt">surface</span>, the atmosphere and the ocean <span class="hlt">exchange</span> momentum, heat and freshwater. Mechanisms for the <span class="hlt">exchange</span> are wind stress, turbulent mixing, radiation, evaporation and precipitation. These <span class="hlt">surface</span> fluxes are characterized by a large spatial and temporal variability and play an important role in not only the mean atmospheric and oceanic circulation, but also in the generation and sustainment of coupled climate fluctuations such as the El Niño/La Niña phenomenon. Therefore, a good knowledge of <span class="hlt">air</span>-sea fluxes is required for the understanding and prediction of climate changes. As part of long-term comprehensive atmospheric reanalyses with `Numerical Weather Prediction/Data assimilation' systems, data sets of global <span class="hlt">air</span>-sea fluxes are generated. A good example is the 15-year atmospheric reanalysis of the European Centre for Medium--Range Weather Forecasts (ECMWF). <span class="hlt">Air</span>-sea flux data sets from these reanalyses are very beneficial for climate research, because they combine a good spatial and temporal coverage with a homogeneous and consistent method of calculation. However, atmospheric reanalyses are still imperfect sources of flux information due to shortcomings in <span class="hlt">model</span> variables, <span class="hlt">model</span> parameterizations, assimilation methods, sampling of observations, and quality of observations. Therefore, assessments of the errors and the usefulness of <span class="hlt">air</span>-sea flux data sets from atmospheric (re-)analyses are relevant contributions to the quantitative study of climate variability. Currently, much research is aimed at assessing the quality and usefulness of the reanalysed <span class="hlt">air</span>-sea fluxes. Work in this thesis intends to contribute to this assessment. In particular, it attempts to answer three relevant questions. The first question is: What is the best parameterization of the momentum flux? A comparison is made of the wind stress parameterization of the ERA15 reanalysis, the currently generated ERA40 reanalysis and the wind stress measurements over the open ocean. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.7664L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.7664L"><span>Atmospheric deposition and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> fluxes of DDT and HCH in the Yangtze River Estuary, East China Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Zhongxia; Lin, Tian; Li, Yuanyuan; Jiang, Yuqing; Guo, Zhigang</p> <p>2017-07-01</p> <p>The Yangtze River Estuary (YRE) is strongly influenced by the Yangtze River and lies on the pathway of the East Asian Monsoon. This study examined atmospheric deposition and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> fluxes of dichlorodiphenyltrichloroethane (DDT) and hexachlorocyclohexane (HCH) to determine whether the YRE is a sink or source of selected pesticides at the <span class="hlt">air</span>-water interface under the influences of river input and atmospheric transport. The <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> of DDT was characterized by net volatilization with a marked difference in its fluxes between summer (140 ng/m2/d) and the other three seasons (12 ng/m2/d), possibly due to the high <span class="hlt">surface</span> seawater temperatures and larger riverine input in summer. However, there was no obvious seasonal variation in the atmospheric HCH deposition, and the <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> reached equilibrium because of low HCH levels in the <span class="hlt">air</span> and seawater after the long-term banning of HCH and the degradation. The gas <span class="hlt">exchange</span> flux of HCH was comparable to the dry and wet deposition fluxes at the <span class="hlt">air</span>-water interface. This suggests that the influences from the Yangtze River input and East Asian continental outflow on the fate of HCH in the YRE were limited. The gas <span class="hlt">exchange</span> flux of DDT was about fivefold higher than the total dry and wet deposition fluxes. DDT residues in agricultural soil transported by enhanced riverine runoff were responsible for sustaining such a high net volatilization in summer. Moreover, our results indicated that there were fresh sources of DDT from the local environment to sustain net volatilization throughout the year.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018HMT...tmp...45B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018HMT...tmp...45B"><span>Numerical investigation on aluminum foam application in a tubular heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buonomo, Bernardo; di Pasqua, Anna; Ercole, Davide; Manca, Oronzio; Nardini, Sergio</p> <p>2018-02-01</p> <p>A numerical study has been conducted to examine the thermal and fluiddynamic behaviors of a tubular heat <span class="hlt">exchanger</span> in aluminum foam. A plate in metal foam with a single array of five circular tubes is the geometrical domain under examination. Darcy-Forchheimer flow <span class="hlt">model</span> and the thermal non-equilibrium energy <span class="hlt">model</span> are used to execute two-dimensional simulations on metal foam heat <span class="hlt">exchanger</span>. The foam is characterized by porosity and (number) pores per inch respectively equal to 0.935 and 20. Different <span class="hlt">air</span> flow rates are imposed to the entrance of the heat <span class="hlt">exchanger</span> with an assigned <span class="hlt">surface</span> tube temperature. The results are provided in terms of local heat transfer coefficient and Nusselt number evaluated on the external <span class="hlt">surface</span> of the tubes. Furthermore, local <span class="hlt">air</span> temperature and velocity profiles in the smaller cross section, between two consecutive tubes are given. Finally, the Energy Performance Ratio (EPR) is evaluated in order to demonstrate the effectiveness of the metal foam.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B21B0445Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B21B0445Y"><span>Study on a Dynamic Vegetation <span class="hlt">Model</span> for Simulating Land <span class="hlt">Surface</span> Flux <span class="hlt">Exchanges</span> at Lien-Hua-Chih Flux Observation Site in Taiwan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yeh, T. Y.; Li, M. H.; Chen, Y. Y.; Ryder, J.; McGrath, M.; Otto, J.; Naudts, K.; Luyssaert, S.; MacBean, N.; Bastrikov, V.</p> <p>2016-12-01</p> <p>Dynamic vegetation <span class="hlt">model</span> ORCHIDEE (Organizing Carbon and Hydrology In Dynamic EcosystEms) is a state of art land <span class="hlt">surface</span> component of the IPSL (Institute Pierre Simon Laplace) Earth System <span class="hlt">Model</span>. It has been used world-wide to investigate variations of water, carbon, and energy <span class="hlt">exchanges</span> between the land <span class="hlt">surface</span> and the atmosphere. In this study we assessed the applicability of using ORCHIDEE-CAN, a new feature with 3-D CANopy structure (Naudts et al., 2015; Ryder et al., 2016), to simulate <span class="hlt">surface</span> fluxes measured at tower-based eddy covariance fluxes at the Lien-Hua-Chih experimental watershed in Taiwan. The atmospheric forcing including radiation, <span class="hlt">air</span> temperature, wind speed, and the dynamics of vertical canopy structure for driving the <span class="hlt">model</span> were obtained from the observations site. Suitable combinations of default plant function types were examined to meet in-situ observations of soil moisture and leaf area index from 2009 to 2013. The simulated top layer soil moisture was ranging from 0.1 to 0.4 and total leaf area was ranging from 2.2 to 4.4, respectively. A sensitivity analysis was performed to investigate the sensitive of <span class="hlt">model</span> parameters and <span class="hlt">model</span> skills of ORCHIDEE-CAN on capturing seasonal variations of <span class="hlt">surface</span> fluxes. The most sensitive parameters were suggested and calibrated by an automatic data assimilation tool ORCHDAS (ORCHIDEE Data Assimilation Systems; http://orchidas.lsce.ipsl.fr/). Latent heat, sensible heat, and carbon fluxes simulated by the <span class="hlt">model</span> were compared with long-term observations at the site. ORCHIDEE-CAN by making use of calibrated <span class="hlt">surface</span> parameters was used to study variations of land-atmosphere interactions on a variety of temporal scale in associations with changes in both land and atmospheric conditions. Ref: Naudts, K., et al.,: A vertically discretised canopy description for ORCHIDEE (SVN r2290) and the modifications to the energy, water and carbon fluxes, Geoscientific <span class="hlt">Model</span> Development, 8, 2035-2065, doi:10.5194/gmd-8</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E3SWC..2200002A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E3SWC..2200002A"><span>Experimental investigation and CFD simulation of multi-pipe earth-to-<span class="hlt">air</span> heat <span class="hlt">exchangers</span> (EAHEs) flow performance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amanowicz, Łukasz; Wojtkowiak, Janusz</p> <p>2017-11-01</p> <p>In this paper the experimentally obtained flow characteristics of multi-pipe earth-to-<span class="hlt">air</span> heat <span class="hlt">exchangers</span> (EAHEs) were used to validate the EAHE flow performance numerical <span class="hlt">model</span> prepared by means of CFD software Ansys Fluent. The cut-cell meshing and the k-ɛ realizable turbulence <span class="hlt">model</span> with default coefficients values and enhanced wall treatment was used. The total pressure losses and airflow in each pipe of multi-pipe <span class="hlt">exchangers</span> was investigated both experimentally and numerically. The results show that airflow in each pipe of multi-pipe EAHE structures is not equal. The validated numerical <span class="hlt">model</span> can be used for a proper designing of multi-pipe EAHEs from the flow characteristics point of view. The influence of EAHEs geometrical parameters on the total pressure losses and airflow division between the <span class="hlt">exchanger</span> pipes can be also analysed. Usage of CFD for designing the EAHEs can be helpful for HVAC engineers (Heating Ventilation and <span class="hlt">Air</span> Conditioning) for optimizing the geometrical structure of multi-pipe EAHEs in order to save the energy and decrease operational costs of low-energy buildings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860008821','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860008821"><span>Aeorodynamic characteristics of an <span class="hlt">air-exchanger</span> system for the 40- by 80-foot wind tunnel at Ames Research Center</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rossow, V. J.; Schmidt, G. I.; Meyn, L. A.; Ortner, K. R.; Holmes, R. E.</p> <p>1986-01-01</p> <p>A 1/50-scale <span class="hlt">model</span> of the 40- by 80-Foot Wind Tunnel at Ames Research Center was used to study various <span class="hlt">air-exchange</span> configurations. System components were tested throughout a range of parameters, and approximate analytical relationships were derived to explain the observed characteristics. It is found that the efficiency of the <span class="hlt">air</span> <span class="hlt">exchanger</span> could be increased (1) by adding a shaped wall to smoothly turn the incoming <span class="hlt">air</span> downstream, (2) by changing to a contoured door at the inlet to control the flow rate, and (3) by increasing the size of the exhaust opening. The static pressures inside the circuit then remain within the design limits at the higher tunnel speeds if the <span class="hlt">air-exchange</span> rate is about 5% or more. Since the <span class="hlt">model</span> is much smaller than the full-scale facility, it is not possible to completely duplicate the tunnel, and it will be necessary to measure such characteristics as flow rate and tunnel pressures during implementation of the remodeled facility. The aerodynamic loads estimated for the inlet door and for nearby walls are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27617333','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27617333"><span>Persistent organochlorine pesticides and polychlorinated biphenyls in <span class="hlt">air</span> of the North Sea region and <span class="hlt">air</span>-sea <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mai, Carolin; Theobald, Norbert; Hühnerfuss, Heinrich; Lammel, Gerhard</p> <p>2016-12-01</p> <p>Organochlorine pesticides (OCPs) and polychlorinated biphenyls (PCBs) were studied to determine occurrence, levels and spatial distribution in the marine atmosphere and <span class="hlt">surface</span> seawater during cruises in the German Bight and the wider North Sea in spring and summer 2009-2010. In general, the concentrations found in <span class="hlt">air</span> are similar to, or below, the levels at coastal or near-coastal sites in Europe. Hexachlorobenzene and α-hexachlorocyclohexane (α-HCH) were close to phase equilibrium, whereas net atmospheric deposition was observed for γ-HCH. The results suggest that declining trends of HCH in seawater have been continuing for γ-HCH but have somewhat levelled off for α-HCH. Dieldrin displayed a close to phase equilibrium in nearly all the sampling sites, except in the central southwestern part of the North Sea. Here atmospheric deposition dominates the <span class="hlt">air</span>-sea <span class="hlt">exchange</span>. This region, close to the English coast, showed remarkably increased <span class="hlt">surface</span> seawater concentrations. This observation depended neither on riverine input nor on the elevated abundances of dieldrin in the <span class="hlt">air</span> masses of central England. A net depositional flux of p,p'-DDE into the North Sea was indicated by both its abundance in the marine atmosphere and the changes in metabolite pattern observed in the <span class="hlt">surface</span> water from the coast towards the open sea. The long-term trends show that the atmospheric concentrations of DDT and its metabolites are not declining. Riverine input is a major source of PCBs in the German Bight and the wider North Sea. Atmospheric deposition of the lower molecular weight PCBs (PCB28 and PCB52) was indicated as a major source for <span class="hlt">surface</span> seawater pollution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......189H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......189H"><span>Heat Transfer in Metal Foam Heat <span class="hlt">Exchangers</span> at High Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hafeez, Pakeeza</p> <p></p> <p>Heat transfer though open-cell metal foam is experimentally studied for heat <span class="hlt">exchanger</span> and heat shield applications at high temperatures (˜750°C). Nickel foam sheets with pore densities of 10 and 40 pores per linear inch (PPI), have been used to make the heat <span class="hlt">exchangers</span> and heat shields by using thermal spray coating to deposit an Inconel skin on a foam core. Heat transfer measurements were performed on a test rig capable of generating hot gas up to 1000°C. The heat <span class="hlt">exchangers</span> were tested by exposing their outer <span class="hlt">surface</span> to combustion gases at a temperature of 550°C and 750°C while being cooled by <span class="hlt">air</span> flowing through them at room temperature at velocities up to 5 m/s. The temperature rise of the <span class="hlt">air</span>, the <span class="hlt">surface</span> temperature of the heat <span class="hlt">exchangers</span> and the <span class="hlt">air</span> temperature inside the heat <span class="hlt">exchanger</span> were measured. The volumetric heat transfer coefficient and Nusselt number were calculated for different velocities. The heat transfer performance of the 40PPI sample brazed with the foil is found to be the most efficient. Pressure drop measurements were also performed for 10 and 40PPI metal foam. Thermographic measurements were done on 40PPI foam heat <span class="hlt">exchangers</span> using a high temperature infrared camera. A high power electric heater was used to produce hot <span class="hlt">air</span> at 300°C that passed over the foam heat <span class="hlt">exchanger</span> while the cooling <span class="hlt">air</span> was blown through it. Heat shields were made by depositing porous skins on metal foam and it was observed that a small amount of coolant leaking through the pores notably reduces the heat transfer from the hot gases. An analytical <span class="hlt">model</span> was developed based assuming local thermal non-equilibrium that accounts for the temperature difference between solid and fluid phase. The experimental results are found to be in good agreement with the predicted values of the <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JGRD..118.3794P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JGRD..118.3794P"><span>Development and evaluation of an ammonia bidirectional flux parameterization for <span class="hlt">air</span> quality <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pleim, Jonathan E.; Bash, Jesse O.; Walker, John T.; Cooter, Ellen J.</p> <p>2013-05-01</p> <p>is an important contributor to particulate matter in the atmosphere and can significantly impact terrestrial and aquatic ecosystems. <span class="hlt">Surface</span> <span class="hlt">exchange</span> between the atmosphere and biosphere is a key part of the ammonia cycle. New <span class="hlt">modeling</span> techniques are being developed for use in <span class="hlt">air</span> quality <span class="hlt">models</span> that replace current ammonia emissions from fertilized crops and ammonia dry deposition with a bidirectional <span class="hlt">surface</span> flux <span class="hlt">model</span> including linkage to a detailed biogeochemical and farm management <span class="hlt">model</span>. Recent field studies involving <span class="hlt">surface</span> flux measurements over crops that predominate in North America have been crucial for extending earlier bidirectional flux <span class="hlt">models</span> toward more realistic treatment of NH3 fluxes for croplands. Comparisons of the ammonia bidirection flux algorithm to both lightly fertilized soybeans and heavily fertilized corn demonstrate that the <span class="hlt">model</span> can capture the magnitude and dynamics of observed ammonia fluxes, both net deposition and evasion, over a range of conditions with overall biases on the order of the uncertainty of the measurements. However, successful application to the field experiment in heavily fertilized corn required substantial modification of the <span class="hlt">model</span> to include new parameterizations for in-soil diffusion resistance, ground quasi-laminar boundary layer resistance, and revised cuticular resistance that is dependent on in-canopy NH3 concentration and RH at the leaf <span class="hlt">surface</span>. This new bidirectional flux algorithm has been incorporated in an <span class="hlt">air</span> quality <span class="hlt">modeling</span> system, which also includes an implementation of a soil nitrification <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16508435','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16508435"><span>Retinal damage caused by <span class="hlt">air</span>-fluid <span class="hlt">exchange</span> during pars plana vitrectomy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Sam S; McDonald, H Richard; Everett, A I; Johnson, Robert N; Jumper, J Michael; Fu, Arthur D</p> <p>2006-03-01</p> <p>To report two cases of retinal damage associated with <span class="hlt">air</span> infusion during pars plana vitrectomy. Observational case report. The authors reviewed the course of two patients who had retinal damage during par plana vitrectomy and <span class="hlt">air</span>-fluid <span class="hlt">exchange</span> for the treatment of macular hole and optic pit-related macular detachment, respectively. The intraoperative observations, postoperative course, and outcomes were reported. As a result of high <span class="hlt">air</span> infusion flow during <span class="hlt">air</span>-fluid <span class="hlt">exchange</span>, retinal damage was created in the area contralateral to the infusion port. In Case 1, an oval area of whitening was noted on the first postoperative day. This area subsequently developed into a large retinal break associated with retinal detachment. In the second case, retinal whitening was noted intraoperatively. This region of pallor resolved quickly during the early postoperative period but resulted in a corresponding inferotemporal visual field defect. High infusion flow during <span class="hlt">air</span>-fluid <span class="hlt">exchange</span> in eyes undergoing vitrectomy surgery may result in significant retinal damage. This pressure-induced trauma initially causes retinal whitening that may be seen intraoperatively or during the early postoperative period. The region of damaged retina may develop a retinal break and detachment or a corresponding visual field defect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10970675','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10970675"><span>Turbulence and wave breaking effects on <span class="hlt">air</span>-water gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boettcher; Fineberg; Lathrop</p> <p>2000-08-28</p> <p>We present an experimental characterization of the effects of turbulence and breaking gravity waves on <span class="hlt">air</span>-water gas <span class="hlt">exchange</span> in standing waves. We identify two regimes that govern aeration rates: turbulent transport when no wave breaking occurs and bubble dominated transport when wave breaking occurs. In both regimes, we correlate the qualitative changes in the aeration rate with corresponding changes in the wave dynamics. In the latter regime, the strongly enhanced aeration rate is correlated with measured acoustic emissions, indicating that bubble creation and dynamics dominate <span class="hlt">air</span>-water <span class="hlt">exchange</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.9781Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.9781Z"><span>Responses of <span class="hlt">surface</span> ozone <span class="hlt">air</span> quality to anthropogenic nitrogen deposition in the Northern Hemisphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Yuanhong; Zhang, Lin; Tai, Amos P. K.; Chen, Youfan; Pan, Yuepeng</p> <p>2017-08-01</p> <p>Human activities have substantially increased atmospheric deposition of reactive nitrogen to the Earth's <span class="hlt">surface</span>, inducing unintentional effects on ecosystems with complex environmental and climate consequences. One consequence remaining unexplored is how <span class="hlt">surface</span> <span class="hlt">air</span> quality might respond to the enhanced nitrogen deposition through <span class="hlt">surface</span>-atmosphere <span class="hlt">exchange</span>. Here we combine a chemical transport <span class="hlt">model</span> (GEOS-Chem) and a global land <span class="hlt">model</span> (Community Land <span class="hlt">Model</span>, CLM) to address this issue with a focus on ozone pollution in the Northern Hemisphere. We consider three processes that are important for <span class="hlt">surface</span> ozone and can be perturbed by the addition of atmospheric deposited nitrogen - namely, emissions of biogenic volatile organic compounds (VOCs), ozone dry deposition, and soil nitrogen oxide (NOx) emissions. We find that present-day anthropogenic nitrogen deposition (65 Tg N a-1 to the land), through enhancing plant growth (represented as increases in vegetation leaf area index, LAI, in the <span class="hlt">model</span>), could increase <span class="hlt">surface</span> ozone from increased biogenic VOC emissions (e.g., a 6.6 Tg increase in isoprene emission), but it could also decrease ozone due to higher ozone dry deposition velocities (up to 0.02-0.04 cm s-1 increases). Meanwhile, deposited anthropogenic nitrogen to soil enhances soil NOx emissions. The overall effect on summer mean <span class="hlt">surface</span> ozone concentrations shows general increases over the globe (up to 1.5-2.3 ppbv over the western US and South Asia), except for some regions with high anthropogenic NOx emissions (0.5-1.0 ppbv decreases over the eastern US, western Europe, and North China). We compare the <span class="hlt">surface</span> ozone changes with those driven by the past 20-year climate and historical land use changes. We find that the impacts from anthropogenic nitrogen deposition can be comparable to the climate- and land-use-driven <span class="hlt">surface</span> ozone changes at regional scales and partly offset the <span class="hlt">surface</span> ozone reductions due to land use changes reported in previous studies</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25597683','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25597683"><span><span class="hlt">Air</span>-soil <span class="hlt">exchange</span> of organochlorine pesticides in a sealed chamber.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Bing; Han, Baolu; Xue, Nandong; Zhou, Lingli; Li, Fasheng</p> <p>2015-01-01</p> <p>So far little is known about <span class="hlt">air</span>-soil <span class="hlt">exchange</span> under any sealed circumstances (e.g., in plastic and glass sheds), which however has huge implications for the soil-<span class="hlt">air</span>-plant pathways of persistent organic pollutants including organochlorine pesticides (OCPs). A newly designed passive <span class="hlt">air</span> sampler was tested in a sealed chamber for measuring the vertical concentration profiles of gaseous phase OCPs (hexachlorocyclohexanes (HCHs) and dichlorodiphenyltrichloroethanes (DDTs)). <span class="hlt">Air</span> was sampled at 5, 15, and 30 cm above ground level every 10th day during a 60-day period by deploying polyurethane foam cylinders housed in acrylonitrile butadiene styrene-covered cartridges. Concentrations and compositions of OCPs along the vertical sections indicated a clear relationship with proximity to the mixture of HCHs and DDTs which escapes from the soils. In addition, significant positive correlations were found between <span class="hlt">air</span> temperatures and concentrations of HCHs and DDTs. These results indicated revolatilization and re-deposition being at or close to dynamic pseudo-equilibrium with the overlying <span class="hlt">air</span>. The sampler used for addressing <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of persistent organic pollutants in any sealed conditions is discussed. Copyright © 2014. Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.agu.org/journals/jc/v096/iC04/90JC02642/','USGSPUBS'); return false;" href="http://www.agu.org/journals/jc/v096/iC04/90JC02642/"><span>Atmospheric organochlorine pollutants and <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of hexachlorocyclohexane in the Bering and Chukchi Seas</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hinckley, D.A.; Bidleman, T.F.; Rice, C.P.</p> <p>1991-01-01</p> <p>Organochlorine pesticides have been found in Arctic fish, marine mammals, birds, and plankton for some time. The lack of local sources and remoteness of the region imply long-range transport and deposition of contaminants into the Arctic from sources to the south. While on the third Soviet-American Joint Ecological Expedition to the Bering and Chukchi Seas (August 1988), high-volume <span class="hlt">air</span> samples were taken and analyzed for organochlorine pesticides. Hexachlorocyclohexane (HCH), hexachlorobenzene, polychlorinated camphenes, and chlordane (listed in order of abundance, highest to lowest) were quantified. The <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> of HCH was estimated at 18 stations during the cruise. Average alpha-HCH concentrations in concurrent atmosphere and <span class="hlt">surface</span> water samples were 250 pg m-3 and 2.4 ng L-1, respectively, and average gamma-HCH concentrations were 68 pg m-3 in the atmosphere and 0.6 ng L-1 in <span class="hlt">surface</span> water. Calculations based on experimentally derived Henry's law constants showed that the <span class="hlt">surface</span> water was undersaturated with respect to the atmosphere at most stations (alpha-HCH, average 79% saturation; gamma-HCH, average 28% saturation). The flux for alpha-HCH ranged from -47 ng m-2 day-1 (sea to <span class="hlt">air</span>) to 122 ng m-2 d-1 (<span class="hlt">air</span> to sea) and averaged 25 ng m-2 d-1 <span class="hlt">air</span> to sea. All fluxes of gamma-HCH were from <span class="hlt">air</span> to sea, ranged from 17 to 54 ng m-2 d-1, and averaged 31 ng m-2 d-1.</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/2018ACP....18.1507C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.1507C"><span><span class="hlt">Modelling</span> the physical multiphase interactions of HNO3 between snow and <span class="hlt">air</span> on the Antarctic Plateau (Dome C) and coast (Halley)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chan, Hoi Ga; Frey, Markus M.; King, Martin D.</p> <p>2018-02-01</p> <p>Emissions of nitrogen oxide (NOx = NO + NO2) from the photolysis of nitrate (NO3-) in snow affect the oxidising capacity of the lower troposphere especially in remote regions of high latitudes with little pollution. Current <span class="hlt">air</span>-snow <span class="hlt">exchange</span> <span class="hlt">models</span> are limited by poor understanding of processes and often require unphysical tuning parameters. Here, two multiphase <span class="hlt">models</span> were developed from physically based parameterisations to describe the interaction of nitrate between the <span class="hlt">surface</span> layer of the snowpack and the overlying atmosphere. The first <span class="hlt">model</span> is similar to previous approaches and assumes that below a threshold temperature, To, the <span class="hlt">air</span>-snow grain interface is pure ice and above To a disordered interface (DI) emerges covering the entire grain <span class="hlt">surface</span>. The second <span class="hlt">model</span> assumes that <span class="hlt">air</span>-ice interactions dominate over all temperatures below melting of ice and that any liquid present above the eutectic temperature is concentrated in micropockets. The <span class="hlt">models</span> are used to predict the nitrate in <span class="hlt">surface</span> snow constrained by year-round observations of mixing ratios of nitric acid in <span class="hlt">air</span> at a cold site on the Antarctic Plateau (Dome C; 75°06' S, 123°33' E; 3233 m a.s.l.) and at a relatively warm site on the Antarctic coast (Halley; 75°35' S, 26°39' E; 35 m a.s.l). The first <span class="hlt">model</span> agrees reasonably well with observations at Dome C (Cv(RMSE) = 1.34) but performs poorly at Halley (Cv(RMSE) = 89.28) while the second <span class="hlt">model</span> reproduces with good agreement observations at both sites (Cv(RMSE) = 0.84 at both sites). It is therefore suggested that in winter <span class="hlt">air</span>-snow interactions of nitrate are determined by non-equilibrium <span class="hlt">surface</span> adsorption and co-condensation on ice coupled with solid-state diffusion inside the grain, similar to Bock et al. (2016). In summer, however, the <span class="hlt">air</span>-snow <span class="hlt">exchange</span> of nitrate is mainly driven by solvation into liquid micropockets following Henry's law with contributions to total <span class="hlt">surface</span> snow NO3- concentrations of 75 and 80 % at Dome C and Halley</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950032432&hterms=regional+impacts+climate+change&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dregional%2Bimpacts%2Bclimate%2Bchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950032432&hterms=regional+impacts+climate+change&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dregional%2Bimpacts%2Bclimate%2Bchange"><span>Regional climates in the GISS general circulation <span class="hlt">model</span>: <span class="hlt">Surface</span> <span class="hlt">air</span> temperature</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hewitson, Bruce</p> <p>1994-01-01</p> <p>One of the more viable research techniques into global climate change for the purpose of understanding the consequent environmental impacts is based on the use of general circulation <span class="hlt">models</span> (GCMs). However, GCMs are currently unable to reliably predict the regional climate change resulting from global warming, and it is at the regional scale that predictions are required for understanding human and environmental responses. Regional climates in the extratropics are in large part governed by the synoptic-scale circulation and the feasibility of using this interscale relationship is explored to provide a way of moving to grid cell and sub-grid cell scales in the <span class="hlt">model</span>. The relationships between the daily circulation systems and <span class="hlt">surface</span> <span class="hlt">air</span> temperature for points across the continental United States are first developed in a quantitative form using a multivariate index based on principal components analysis (PCA) of the <span class="hlt">surface</span> circulation. These relationships are then validated by predicting daily temperature using observed circulation and comparing the predicted values with the observed temperatures. The relationships predict <span class="hlt">surface</span> temperature accurately over the major portion of the country in winter, and for half the country in summer. These relationships are then applied to the <span class="hlt">surface</span> synoptic circulation of the Goddard Institute for Space Studies (GISS) GCM control run, and a set of <span class="hlt">surface</span> grid cell temperatures are generated. These temperatures, based on the larger-scale validated circulation, may now be used with greater confidence at the regional scale. The generated temperatures are compared to those of the <span class="hlt">model</span> and show that the <span class="hlt">model</span> has regional errors of up to 10 C in individual grid cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ThEng..64..680B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ThEng..64..680B"><span>Investigation and optimization of the depth of flue gas heat recovery in <span class="hlt">surface</span> heat <span class="hlt">exchangers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bespalov, V. V.; Bespalov, V. I.; Melnikov, D. V.</p> <p>2017-09-01</p> <p>Economic issues associated with designing deep flue gas heat recovery units for natural gas-fired boilers are examined. The governing parameter affecting the performance and cost of <span class="hlt">surface</span>-type condensing heat recovery heat <span class="hlt">exchangers</span> is the heat transfer <span class="hlt">surface</span> area. When firing natural gas, the heat recovery depth depends on the flue gas temperature at the condenser outlet and determines the amount of condensed water vapor. The effect of the outlet flue gas temperature in a heat recovery heat <span class="hlt">exchanger</span> on the additionally recovered heat power is studied. A correlation has been derived enabling one to determine the best heat recovery depth (or the final cooling temperature) maximizing the anticipated reduced annual profit of a power enterprise from implementation of energy-saving measures. Results of optimization are presented for a <span class="hlt">surface</span>-type condensing gas-<span class="hlt">air</span> plate heat recovery heat <span class="hlt">exchanger</span> for the climatic conditions and the economic situation in Tomsk. The predictions demonstrate that it is economically feasible to design similar heat recovery heat <span class="hlt">exchangers</span> for a flue gas outlet temperature of 10°C. In this case, the payback period for the investment in the heat recovery heat <span class="hlt">exchanger</span> will be 1.5 years. The effect of various factors on the optimal outlet flue gas temperature was analyzed. Most climatic, economical, or technological factors have a minor effect on the best outlet temperature, which remains between 5 and 20°C when varying the affecting factors. The derived correlation enables us to preliminary estimate the outlet (final) flue gas temperature that should be used in designing the heat transfer <span class="hlt">surface</span> of a heat recovery heat <span class="hlt">exchanger</span> for a gas-fired boiler as applied to the specific climatic conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.6719V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.6719V"><span><span class="hlt">Air</span>-sea <span class="hlt">exchange</span> over Black Sea estimated from high resolution regional climate simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Velea, Liliana; Bojariu, Roxana; Cica, Roxana</p> <p>2013-04-01</p> <p>Black Sea is an important influencing factor for the climate of bordering countries, showing cyclogenetic activity (Trigo et al, 1999) and influencing Mediterranean cyclones passing over. As for other seas, standard observations of the atmosphere are limited in time and space and available observation-based estimations of <span class="hlt">air</span>-sea <span class="hlt">exchange</span> terms present quite large ranges of uncertainty. The reanalysis datasets (e.g. ERA produced by ECMWF) provide promising validation estimates of climatic characteristics against the ones in available climatic data (Schrum et al, 2001), while cannot reproduce some local features due to relatively coarse horizontal resolution. Detailed and realistic information on smaller-scale processes are foreseen to be provided by regional climate <span class="hlt">models</span>, due to continuous improvements of physical parameterizations and numerical solutions and thus affording simulations at high spatial resolution. The aim of the study is to assess the potential of three regional climate <span class="hlt">models</span> in reproducing known climatological characteristics of <span class="hlt">air</span>-sea <span class="hlt">exchange</span> over Black Sea, as well as to explore the added value of the <span class="hlt">model</span> compared to the input (reanalysis) data. We employ results of long-term (1961-2000) simulations performed within ENSEMBLE project (http://ensemblesrt3.dmi.dk/) using <span class="hlt">models</span> ETHZ-CLM, CNRM-ALADIN, METO-HadCM, for which the integration domain covers the whole area of interest. The analysis is performed for the entire basin for several variables entering the heat and water budget terms and available as direct output from the <span class="hlt">models</span>, at seasonal and annual scale. A comparison with independent data (ERA-INTERIM) and findings from other studies (e.g. Schrum et al, 2001) is also presented. References: Schrum, C., Staneva, J., Stanev, E. and Ozsoy, E., 2001: <span class="hlt">Air</span>-sea <span class="hlt">exchange</span> in the Black Sea estimated from atmospheric analysis for the period 1979-1993, J. Marine Systems, 31, 3-19 Trigo, I. F., T. D. Davies, and G. R. Bigg (1999): Objective</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..117a2012I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..117a2012I"><span>The effects of green areas on <span class="hlt">air</span> <span class="hlt">surface</span> temperature of the Kuala Lumpur city using WRF-ARW <span class="hlt">modelling</span> and 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>Isa, N. A.; Mohd, W. M. N. Wan; Salleh, S. A.; Ooi, M. C. G.</p> <p>2018-02-01</p> <p>Matured trees contain high concentration of chlorophyll that encourages the process of photosynthesis. This process produces oxygen as a by-product and releases it into the atmosphere and helps in lowering the ambient temperature. This study attempts to analyse the effect of green area on <span class="hlt">air</span> <span class="hlt">surface</span> temperature of the Kuala Lumpur city. The <span class="hlt">air</span> <span class="hlt">surface</span> temperatures of two different dates which are, in March 2006 and March 2016 were simulated using the Weather Research and Forecasting (WRF) <span class="hlt">model</span>. The green area in the city was extracted using the Normalized Difference Vegetation Index (NDVI) from two Landsat satellite images. The relationship between the <span class="hlt">air</span> <span class="hlt">surface</span> temperature and the green area were analysed using linear regression <span class="hlt">models</span>. From the study, it was found that, the green area was significantly affecting the distribution of <span class="hlt">air</span> temperature within the city. A strong negative correlation was identified through this study which indicated that higher NDVI values tend to have lower <span class="hlt">air</span> <span class="hlt">surface</span> temperature distribution within the focus study area. It was also found that, different urban setting in mixed built-up and vegetated areas resulted in different distributions of <span class="hlt">air</span> <span class="hlt">surface</span> temperature. Future studies should focus on analysing the <span class="hlt">air</span> <span class="hlt">surface</span> temperature within the area of mixed built-up and vegetated area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........17O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........17O"><span>Observations and <span class="hlt">Modeling</span> of Turbulent <span class="hlt">Air</span>-Sea Coupling in Coastal and Strongly Forced Condition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ortiz-Suslow, David G.</p> <p></p> <p>The turbulent fluxes of momentum, mass, and energy across the ocean-atmosphere boundary are fundamental to our understanding of a myriad of geophysical processes, such as wind-wave generation, oceanic circulation, and <span class="hlt">air</span>-sea gas transfer. In order to better understand these fluxes, empirical relationships were developed to quantify the interfacial <span class="hlt">exchange</span> rates in terms of easily observed parameters (e.g., wind speed). However, mounting evidence suggests that these empirical formulae are only valid over the relatively narrow parametric space, i.e. open ocean conditions in light to moderate winds. Several near-<span class="hlt">surface</span> processes have been observed to cause significant variance in the <span class="hlt">air</span>-sea fluxes not predicted by the conventional functions, such as a heterogeneous <span class="hlt">surfaces</span>, swell waves, and wave breaking. Further study is needed to fully characterize how these types of processes can modulate the interfacial <span class="hlt">exchange</span>; in order to achieve this, a broad investigation into <span class="hlt">air</span>-sea coupling was undertaken. The primary focus of this work was to use a combination of field and laboratory observations and numerical <span class="hlt">modeling</span>, in regimes where conventional theories would be expected to breakdown, namely: the nearshore and in very high winds. These seemingly disparate environments represent the marine atmospheric boundary layer at its physical limit. In the nearshore, the convergence of land, <span class="hlt">air</span>, and sea in a depth-limited domain marks the transition from a marine to a terrestrial boundary layer. Under extreme winds, the physical nature of the boundary layer remains unknown as an intermediate substrate layer, sea spray, develops between the atmosphere and ocean <span class="hlt">surface</span>. At these ends of the MABL physical spectrum, direct measurements of the near-<span class="hlt">surface</span> processes were made and directly related to local sources of variance. Our results suggest that the conventional treatment of <span class="hlt">air</span>-sea fluxes in terms of empirical relationships developed from a relatively narrow set of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JSSCh.262..199T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JSSCh.262..199T"><span><span class="hlt">Surface</span> defect chemistry and oxygen <span class="hlt">exchange</span> kinetics in La2-xCaxNiO4+δ</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tropin, E. S.; Ananyev, M. V.; Farlenkov, A. S.; Khodimchuk, A. V.; Berenov, A. V.; Fetisov, A. V.; Eremin, V. A.; Kolchugin, A. A.</p> <p>2018-06-01</p> <p><span class="hlt">Surface</span> oxygen <span class="hlt">exchange</span> kinetics and diffusion in La2-xCaxNiO4+δ (x = 0; 0.1; 0.3) have been studied by the isotope <span class="hlt">exchange</span> method with gas phase equilibration in the temperature range of 600-800 °C and oxygen pressure range 0.13-2.5 kPa. Despite an enhanced electrical conductivity of La2-xCaxNiO4+δ theirs oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> (k*) and oxygen tracer diffusion (D*) coefficients were significantly lower in comparison with La2NiO4+δ. The rates of the elementary stages of oxygen <span class="hlt">exchange</span> have been calculated. Upon Ca doping the change of the rate-determining stage was observed. The <span class="hlt">surface</span> of the oxides was found to be inhomogeneous towards oxygen <span class="hlt">exchange</span> process according to the recently developed <span class="hlt">model</span>. The reasons of such inhomogeneity are discussed as well as Ca influence on the <span class="hlt">surface</span> defect chemistry and oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> and diffusivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015HydJ...23..305S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015HydJ...23..305S"><span>Insights on <span class="hlt">surface</span>-water/groundwater <span class="hlt">exchange</span> in the upper Floridan aquifer, north-central Florida (USA), from streamflow data and numerical <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sutton, James E.; Screaton, Elizabeth J.; Martin, Jonathan B.</p> <p>2015-03-01</p> <p><span class="hlt">Surface</span>-water/groundwater <span class="hlt">exchange</span> impacts water quality and budgets. In karst aquifers, these <span class="hlt">exchanges</span> also play an important role in dissolution. Five years of river discharge data were analyzed and a transient groundwater flow <span class="hlt">model</span> was developed to evaluate large-scale temporal and spatial variations of <span class="hlt">exchange</span> between an 80-km stretch of the Suwannee River in north-central Florida (USA) and the karstic upper Floridan aquifer. The one-layer transient groundwater flow <span class="hlt">model</span> was calibrated using groundwater levels from 59 monitoring wells, and fluxes were compared to the <span class="hlt">exchange</span> calculated from discharge data. Both the numerical <span class="hlt">modeling</span> and the discharge analysis suggest that the Suwannee River loses water under both low- and high-stage conditions. River losses appear greatest at the inside of a large meander, and the former river water may continue across the meander within the aquifer rather than return to the river. In addition, the numerical <span class="hlt">model</span> calibration reveals that aquifer transmissivity is elevated within this large meander, which is consistent with enhanced dissolution due to river losses. The results show the importance of temporal and spatial variations in head gradients to <span class="hlt">exchange</span> between streams and karst aquifers and dissolution of the aquifers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19778365','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19778365"><span>Why and how terrestrial plants <span class="hlt">exchange</span> gases with <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>Cieslik, S; Omasa, K; Paoletti, E</p> <p>2009-11-01</p> <p>This work is intended as a review of gas <span class="hlt">exchange</span> processes between the atmosphere and the terrestrial vegetation, which have been known for more than two centuries since the discovery of photosynthesis. The physical and biological mechanisms of <span class="hlt">exchange</span> of carbon dioxide, water vapour, volatile organic compounds emitted by plants and <span class="hlt">air</span> pollutants taken up by them, is critically reviewed. The role of stomatal physiology is emphasised, as it controls most of these processes. The techniques used for measurement of gas <span class="hlt">exchange</span> fluxes between the atmosphere and vegetation are outlined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JEPT...89.1369G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JEPT...89.1369G"><span>Heat <span class="hlt">Exchange</span> with <span class="hlt">Air</span> and Temperature Profile of a Moving Oversize Tire</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grinchuk, P. S.; Fisenko, S. P.</p> <p>2016-11-01</p> <p>A one-dimensional mathematical <span class="hlt">model</span> of heat transfer in a tire with account for the deformation energy dissipation and heat <span class="hlt">exchange</span> of a moving tire with <span class="hlt">air</span> has been developed. The mean temperature profiles are calculated and transition to a stationary thermal regime is considered. The influence of the rate of energy dissipation and of effective thermal conductivity of rubber on the temperature field is investigated quantitatively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEMat..46.3062L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEMat..46.3062L"><span>Optimization of Heat <span class="hlt">Exchangers</span> with Dimpled <span class="hlt">Surfaces</span> to Improve the Performance in Thermoelectric Generators Using a Kriging <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Shuai; Wang, Yiping; Wang, Tao; Yang, Xue; Deng, Yadong; Su, Chuqi</p> <p>2017-05-01</p> <p>Thermoelectric generators (TEGs) have become a topic of interest for vehicle exhaust energy recovery. Electrical power generation is deeply influenced by temperature differences, temperature uniformity and topological structures of TEGs. When the dimpled <span class="hlt">surfaces</span> are adopted in heat <span class="hlt">exchangers</span>, the heat transfer rates can be augmented with a minimal pressure drop. However, the temperature distribution shows a large gradient along the flow direction which has adverse effects on the power generation. In the current study, the heat <span class="hlt">exchanger</span> performance was studied in a computational fluid dynamics (CFD) <span class="hlt">model</span>. The dimple depth, dimple print diameter, and channel height were chosen as design variables. The objective function was defined as a combination of average temperature, temperature uniformity and pressure loss. The optimal Latin hypercube method was used to determine the experiment points as a method of design of the experiment in order to analyze the sensitivity of the design variables. A Kriging surrogate <span class="hlt">model</span> was built and verified according to the database resulting from the CFD simulation. A multi-island genetic algorithm was used to optimize the structure in the heat <span class="hlt">exchanger</span> based on the surrogate <span class="hlt">model</span>. The results showed that the average temperature of the heat <span class="hlt">exchanger</span> was most sensitive to the dimple depth. The pressure loss and temperature uniformity were most sensitive to the parameter of channel rear height, h 2. With an optimal design of channel structure, the temperature uniformity can be greatly improved compared with the initial <span class="hlt">exchanger</span>, and the additional pressure loss also increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26910987','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26910987"><span>[Summer Greenhouse Gases <span class="hlt">Exchange</span> Flux Across Water-<span class="hlt">air</span> Interface in Three Water Reservoirs Located in Different Geologic Setting in Guangxi, China].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Jian-hong; Pu, Jun-bing; Sun, Ping-an; Yuan, Dao-xian; Liu, Wen; Zhang, Tao; Mo, Xue</p> <p>2015-11-01</p> <p>Due to special hydrogeochemical characteristics of calcium-rich, alkaline and DIC-rich ( dissolved inorganic carbon) environment controlled by the weathering products from carbonate rock, the <span class="hlt">exchange</span> characteristics, processes and controlling factors of greenhouse gas (CO2 and CH4) across water-<span class="hlt">air</span> interface in karst water reservoir show obvious differences from those of non-karst water reservoir. Three water reservoirs (Dalongdong reservoir-karst reservoir, Wulixia reservoir--semi karst reservoir, Si'anjiang reservoir-non-karst reservoir) located in different geologic setting in Guangxi Zhuang Autonomous Region, China were chosen to reveal characteristics and controlling factors of greenhouse gas <span class="hlt">exchange</span> flux across water-<span class="hlt">air</span> interface. Two common approaches, floating chamber (FC) and thin boundary layer <span class="hlt">models</span> (TBL), were employed to research and contrast greenhouse gas <span class="hlt">exchange</span> flux across water-<span class="hlt">air</span> interface from three reservoirs. The results showed that: (1) <span class="hlt">surface</span>-layer water in reservoir area and discharging water under dam in Dalongdong water reservoir were the source of atmospheric CO2 and CH4. <span class="hlt">Surface</span>-layer water in reservoir area in Wulixia water reservoir was the sink of atmospheric CO2 and the source of atmospheric CH4, while discharging water under dam was the source of atmospheric CO2 and CH4. <span class="hlt">Surface</span>-layer water in Si'anjiang water reservoir was the sink of atmospheric CO2 and source of atmospheric CH4. (2) CO2 and CH4 effluxes in discharging water under dam were much more than those in <span class="hlt">surface</span>-layer water in reservoir area regardless of karst reservoir or non karst reservoir. Accordingly, more attention should be paid to the CO2 and CH4 emission from discharging water under dam. (3) In the absence of submerged soil organic matters and plants, the difference of CH4 effluxes between karst groundwater-fed reservoir ( Dalongdong water reservoir) and non-karst area ( Wulixia water reservoir and Si'anjiang water reservoir) was less. However, CO2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19..307S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19..307S"><span><span class="hlt">Surface</span> atmosphere <span class="hlt">exchange</span> in dry and a wet regime over the Ganges valley: a comprehensive investigation with direct observations and numerical simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sathyanadh, Anusha; Prabhakaran, Thara; Karipot, Anandakumar</p> <p>2017-04-01</p> <p> microwave radiometer, radiosonde sounding and SODAR measurements compared well with the <span class="hlt">model</span> vertical profiles. All the schemes are able to capture the development of a drying phase, its persistence and revival after the drying, similar to observation. The characteristic features of the drying such as decrease in mixing ratio, PBL warming, enhanced PBL growth, variations in wind speed, etc were reproduced by the <span class="hlt">model</span> simulations. Results indicate that <span class="hlt">model</span> is simulating a drier and deeper <span class="hlt">surface</span> and mixed layer, compared to the observations, which is assisted by enhanced mixing through deep updrafts rooted from the <span class="hlt">surface</span> layer and downdrafts associated with the subsiding <span class="hlt">air</span> reaching down to the <span class="hlt">surface</span>. Two issues are identified with <span class="hlt">model</span> as a) relating to enhanced mixing also assisted by the subsiding <span class="hlt">air</span> at top of the boundary layer and b) the energy partitioning at the <span class="hlt">surface</span> with significantly excess energy partitioned in to sensible heat flux, thus warming the <span class="hlt">model</span> <span class="hlt">surface</span> layer. A few aircraft observations are used to investigate entrainment issue and results from these analysis and inferences will be presented. The <span class="hlt">surface</span> layer eddy covariance measurements of sensible and latent heat fluxes and <span class="hlt">surface</span> layer relationships are used to tune the <span class="hlt">surface</span> layer <span class="hlt">exchanges</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70120200','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70120200"><span><span class="hlt">Air</span>-sea interactions during strong winter extratropical storms</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Nelson, Jill; He, Ruoying; Warner, John C.; Bane, John</p> <p>2014-01-01</p> <p>A high-resolution, regional coupled atmosphere–ocean <span class="hlt">model</span> is used to investigate strong air–sea interactions during a rapidly developing extratropical cyclone (ETC) off the east coast of the USA. In this two-way coupled system, <span class="hlt">surface</span> momentum and heat fluxes derived from the Weather Research and Forecasting <span class="hlt">model</span> and sea <span class="hlt">surface</span> temperature (SST) from the Regional Ocean <span class="hlt">Modeling</span> System are <span class="hlt">exchanged</span> via the <span class="hlt">Model</span> Coupling Toolkit. Comparisons are made between the <span class="hlt">modeled</span> and observed wind velocity, sea level pressure, 10 m <span class="hlt">air</span> temperature, and sea <span class="hlt">surface</span> temperature time series, as well as a comparison between the <span class="hlt">model</span> and one glider transect. Vertical profiles of <span class="hlt">modeled</span> <span class="hlt">air</span> temperature and winds in the marine atmospheric boundary layer and temperature variations in the upper ocean during a 3-day storm period are examined at various cross-shelf transects along the eastern seaboard. It is found that the air–sea interactions near the Gulf Stream are important for generating and sustaining the ETC. In particular, locally enhanced winds over a warm sea (relative to the land temperature) induce large <span class="hlt">surface</span> heat fluxes which cool the upper ocean by up to 2 °C, mainly during the cold <span class="hlt">air</span> outbreak period after the storm passage. Detailed heat budget analyses show the ocean-to-atmosphere heat flux dominates the upper ocean heat content variations. Results clearly show that dynamic air–sea interactions affecting momentum and buoyancy flux <span class="hlt">exchanges</span> in ETCs need to be resolved accurately in a coupled atmosphere–ocean <span class="hlt">modeling</span> framework.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....1611283Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....1611283Z"><span><span class="hlt">Surface</span>-atmosphere <span class="hlt">exchange</span> of ammonia over peatland using QCL-based eddy-covariance measurements and inferential <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zöll, Undine; Brümmer, Christian; Schrader, Frederik; Ammann, Christof; Ibrom, Andreas; Flechard, Christophe R.; Nelson, David D.; Zahniser, Mark; Kutsch, Werner L.</p> <p>2016-09-01</p> <p>Recent advances in laser spectrometry offer new opportunities to investigate ecosystem-atmosphere <span class="hlt">exchange</span> of environmentally relevant trace gases. In this study, we demonstrate the applicability of a quantum cascade laser (QCL) absorption spectrometer to continuously measure ammonia concentrations at high time resolution and thus to quantify the net <span class="hlt">exchange</span> between a seminatural peatland ecosystem and the atmosphere based on the eddy-covariance approach. Changing diurnal patterns of both ammonia concentration and fluxes were found during different periods of the campaign. We observed a clear tipping point in early spring with decreasing ammonia deposition velocities and increasingly bidirectional fluxes that occurred after the switch from dormant vegetation to CO2 uptake but was triggered by a significant weather change. While several biophysical parameters such as temperature, radiation, and <span class="hlt">surface</span> wetness were identified to partially regulate ammonia <span class="hlt">exchange</span> at the site, the seasonal concentration pattern was clearly dominated by agricultural practices in the surrounding area. Comparing the results of a compensation point <span class="hlt">model</span> with our measurement-based flux estimates showed considerable differences in some periods of the campaign due to overestimation of non-stomatal resistances caused by low acid ratios. The total cumulative campaign <span class="hlt">exchange</span> of ammonia after 9 weeks, however, differed only in a 6 % deviation with 911 and 857 g NH3-N ha-1 deposition being found by measurements and <span class="hlt">modeling</span>, respectively. Extrapolating our findings to an entire year, ammonia deposition was lower than reported by Hurkuck et al. (2014) for the same site in previous years using denuder systems. This was likely due to a better representation of the emission component in the net signal of eddy-covariance fluxes as well as better adapted site-specific parameters in the <span class="hlt">model</span>. Our study not only stresses the importance of high-quality measurements for studying and assessing land</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988asme.conf....2B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988asme.conf....2B"><span>Heat transfer and pressure drop measurements in an <span class="hlt">air</span>/molten salt direct-contact heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bohn, Mark S.</p> <p>1988-11-01</p> <p>This paper presents a comparison of experimental data with a recently published <span class="hlt">model</span> of heat <span class="hlt">exchange</span> in irrigated packed beds. Heat transfer and pressure drop were measured in a 150 mm (ID) column with a 610 mm bed of metal Pall rings. Molten nitrate salt and preheated <span class="hlt">air</span> were the working fluids with a salt inlet temperature of approximately 440 C and <span class="hlt">air</span> inlet temperatures of approximately 230 C. A comparison between the experimental data and the heat transfer <span class="hlt">model</span> is made on the basis of heat transfer from the salt. For the range of <span class="hlt">air</span> and salt flow rates tested, 0.3 to 1.2 kg/sq m/s <span class="hlt">air</span> flow and 6 to 18 kg/sq m/s salt flow, the data agree with the <span class="hlt">model</span> within 22 percent standard deviation. In addition, a <span class="hlt">model</span> for the column pressure drop was validated, agreeing with the experimental data within 18 percent standard deviation over the range of column pressure drop from 40 to 1250 Pa/m.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDH36008C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDH36008C"><span><span class="hlt">Surface</span> nanobubble nucleation dynamics during water-ethanol <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chan, Chon U.; Ohl, Claus-Dieter</p> <p>2015-11-01</p> <p>Water-ethanol <span class="hlt">exchange</span> has been a promising nucleation method for <span class="hlt">surface</span> attached nanobubbles since their discovery. In this process, water and ethanol displace each other sequentially on a substrate. As the gas solubility is 36 times higher in ethanol than water, it was suggested that the <span class="hlt">exchange</span> process leads to transient supersaturation and is responsible for the nanobubble nucleation. In this work, we visualize the nucleation dynamics by controllably mixing water and ethanol. It depicts the temporal evolution of the conventional <span class="hlt">exchange</span> in a single field of view, detailing the conditions for <span class="hlt">surface</span> nanobubble nucleation and the flow field that influences their spatial organization. This technique can also pattern <span class="hlt">surface</span> nanobubbles with variable size distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AdSpR..50.1231K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AdSpR..50.1231K"><span>A <span class="hlt">model</span> for calculating the vertical distribution of the atmospheric electric potential in the <span class="hlt">exchange</span> layer in a maritime clean atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kulkarni, M. N.; Kamra, A. K.</p> <p>2012-11-01</p> <p>A theoretical <span class="hlt">model</span> is developed for calculating the vertical distribution of atmospheric electric potential in <span class="hlt">exchange</span> layer of maritime clean atmosphere. The transport of space charge in electrode layer acts as a convective generator in this <span class="hlt">model</span> and plays a major role in determining potential distribution in vertical. Eddy diffusion is the main mechanism responsible for the distribution of space charge in vertical. Our results show that potential at a particular level increases with increase in the strength of eddy diffusion under similar conditions. A method is suggested to estimate columnar resistance, the ionospheric potential and the vertical atmospheric electric potential distribution in <span class="hlt">exchange</span> layer from measurements of total <span class="hlt">air</span>-earth current density and <span class="hlt">surface</span> electric field made over oceans. The results are validated and found to be in very good agreement with the previous aircraft measurements. Different parameters involved in the proposed methodology can be determined either theoretically, as in the present work, or experimentally using the near <span class="hlt">surface</span> atmospheric electrical measurements or using some other <span class="hlt">surface</span>-based measurement technique such as LIDAR. A graphical relationship between the atmospheric eddy diffusion coefficient and height of <span class="hlt">exchange</span> layer obtained from atmospheric electrical approach, is reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/10114385','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/10114385"><span>Parameterizing atmosphere-land <span class="hlt">surface</span> <span class="hlt">exchange</span> for climate <span class="hlt">models</span> with satellite data: A case study for the Southern Great Plains CART site</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>Gao, W.</p> <p></p> <p>High-resolution satellite data provide detailed, quantitative descriptions of land <span class="hlt">surface</span> characteristics over large areas so that objective scale linkage becomes feasible. With the aid of satellite data, Sellers et al. and Wood and Lakshmi examined the linearity of processes scaled up from 30 m to 15 km. If the phenomenon is scale invariant, then the aggregated value of a function or flux is equivalent to the function computed from aggregated values of controlling variables. The linear relation may be realistic for limited land areas having no large <span class="hlt">surface</span> contrasts to cause significant horizontal <span class="hlt">exchange</span>. However, for areas with sharp surfacemore » contrasts, horizontal <span class="hlt">exchange</span> and different dynamics in the atmospheric boundary may induce nonlinear interactions, such as at interfaces of land-water, forest-farm land, and irrigated crops-desert steppe. The linear approach, however, represents the simplest scenario, and is useful for developing an effective scheme for incorporating subgrid land <span class="hlt">surface</span> processes into large-scale <span class="hlt">models</span>. Our studies focus on coupling satellite data and ground measurements with a satellite-data-driven land <span class="hlt">surface</span> <span class="hlt">model</span> to parameterize <span class="hlt">surface</span> fluxes for large-scale climate <span class="hlt">models</span>. In this case study, we used <span class="hlt">surface</span> spectral reflectance data from satellite remote sensing to characterize spatial and temporal changes in vegetation and associated <span class="hlt">surface</span> parameters in an area of about 350 {times} 400 km covering the southern Great Plains (SGP) Cloud and Radiation Testbed (CART) site of the US Department of Energy`s Atmospheric Radiation Measurement (ARM) Program.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26ES...35a2003A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26ES...35a2003A"><span>The potential role of sea spray droplets in facilitating <span class="hlt">air</span>-sea gas transfer</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.; Vlahos, P.; Monahan, E. C.</p> <p>2016-05-01</p> <p>For over 30 years, <span class="hlt">air</span>-sea interaction specialists have been evaluating and parameterizing the role of whitecap bubbles in <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>. To our knowledge, no one, however, has studied the mirror image process of whether sea spray droplets can facilitate <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>. We are therefore using theory, data analysis, and numerical <span class="hlt">modeling</span> to quantify the role of spray on <span class="hlt">air</span>-sea gas transfer. In this, our first formal work on this subject, we seek the rate-limiting step in spray-mediated gas transfer by evaluating the three time scales that govern the <span class="hlt">exchange</span>: τ <span class="hlt">air</span> , which quantifies the rate of transfer between the atmospheric gas reservoir and the <span class="hlt">surface</span> of the droplet; τ int , which quantifies the <span class="hlt">exchange</span> rate across the <span class="hlt">air</span>-droplet interface; and τ aq , which quantifies gas mixing within the aqueous solution droplet.</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('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=56137&Lab=NERL&keyword=database+AND+academic&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=56137&Lab=NERL&keyword=database+AND+academic&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>EMISSION AND <span class="hlt">SURFACE</span> <span class="hlt">EXCHANGE</span> PROCESS</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>This task supports the development, evaluation, and application of emission and dry deposition algorithms in <span class="hlt">air</span> quality simulation <span class="hlt">models</span>, such as the <span class="hlt">Models</span>-3/Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">modeling</span> system. Emission estimates influence greatly the accuracy of <span class="hlt">air</span> qual...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880003414','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880003414"><span>Measured performance of the heat <span class="hlt">exchanger</span> in the NASA icing research tunnel under severe icing and dry-<span class="hlt">air</span> conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, W.; Vanfossen, J.; Nussle, R.</p> <p>1987-01-01</p> <p>Measurements were made of the pressure drop and thermal perfomance of the unique refrigeration heat <span class="hlt">exchanger</span> in the NASA Lewis Icing Research Tunnel (IRT) under severe icing and frosting conditions and also with dry <span class="hlt">air</span>. This data will be useful to those planning to use or extend the capability of the IRT and other icing facilities (e.g., the Altitude Wind Tunnel-AWT). The IRT heat <span class="hlt">exchanger</span> and refrigeration system is able to cool <span class="hlt">air</span> passing through the test section down to at least a total temperature of -30 C (well below icing requirements), and usually up to -2 C. The system maintains a uniform temperature across the test section at all airspeeds, which is more difficult and time consuming at low airspeeds, at high temperatures, and on hot, humid days when the cooling towers are less efficient. The very small <span class="hlt">surfaces</span> of the heat <span class="hlt">exchanger</span> prevent any icing cloud droplets from passing through it and going through the tests section again. The IRT heat <span class="hlt">exchanger</span> was originally designed not to be adversely affected by severe icing. During a worst-case icing test the heat <span class="hlt">exchanger</span> iced up enough so that the temperature uniformaity was no worse than about +/- 1 deg C. The conclusion is that the heat <span class="hlt">exchanger</span> design performs well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..217a2021D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..217a2021D"><span>Working parameters affecting earth-<span class="hlt">air</span> heat <span class="hlt">exchanger</span> (EAHE) system performance for passive cooling: A review</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Darius, D.; Misaran, M. S.; Rahman, Md. M.; Ismail, M. A.; Amaludin, A.</p> <p>2017-07-01</p> <p>The study on the effect of the working parameters such as pipe material, pipe length, pipe diameter, depth of burial of the pipe, <span class="hlt">air</span> flow rate and different types of soils on the thermal performance of earth-<span class="hlt">air</span> heat <span class="hlt">exchanger</span> (EAHE) systems is very crucial to ensure that thermal comfort can be achieved. In the past decade, researchers have performed studies to develop numerical <span class="hlt">models</span> for analysis of EAHE systems. Until recently, two-dimensional <span class="hlt">models</span> replaced the numerical <span class="hlt">models</span> in the 1990s and in recent times, more advanced analysis using three-dimensional <span class="hlt">models</span>, specifically the Computational Fluid Dynamics (CFD) simulation in the analysis of EAHE system. This paper reviews previous <span class="hlt">models</span> used to analyse the EAHE system and working parameters that affects the earth-<span class="hlt">air</span> heat <span class="hlt">exchanger</span> (EAHE) thermal performance as of February 2017. Recent findings on the parameters affecting EAHE performance are also presented and discussed. As a conclusion, with the advent of CFD methods, investigational work have geared up to <span class="hlt">modelling</span> and simulation work as it saves time and cost. Comprehension of the EAHE working parameters and its effect on system performance is largely established. However, the study on type of soil and its characteristics on the performance of EAHEs systems are surprisingly barren. Therefore, future studies should focus on the effect of soil characteristics such as moisture content, density of soil, and type of soil on the thermal performance of EAHEs system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3497365','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3497365"><span>Seasonal Variations of Indoor Microbial Exposures and Their Relation to Temperature, Relative Humidity, and <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bekö, Gabriel; Timm, Michael; Gustavsen, Sine; Hansen, Erik Wind</p> <p>2012-01-01</p> <p>Indoor microbial exposure has been related to adverse pulmonary health effects. Exposure assessment is not standardized, and various factors may affect the measured exposure. The aim of this study was to investigate the seasonal variation of selected microbial exposures and their associations with temperature, relative humidity, and <span class="hlt">air</span> <span class="hlt">exchange</span> rates in Danish homes. Airborne inhalable dust was sampled in five Danish homes throughout the four seasons of 1 year (indoors, n = 127; outdoors, n = 37). Measurements included culturable fungi and bacteria, endotoxin, N-acetyl-beta-d-glucosaminidase, total inflammatory potential, particles (0.75 to 15 μm), temperature, relative humidity, and <span class="hlt">air</span> <span class="hlt">exchange</span> rates. Significant seasonal variation was found for all indoor microbial exposures, excluding endotoxin. Indoor fungi peaked in summer (median, 235 CFU/m3) and were lowest in winter (median, 26 CFU/m3). Indoor bacteria peaked in spring (median, 2,165 CFU/m3) and were lowest in summer (median, 240 CFU/m3). Concentrations of fungi were predominately higher outdoors than indoors, whereas bacteria, endotoxin, and inhalable dust concentrations were highest indoors. Bacteria and endotoxin correlated with the mass of inhalable dust and number of particles. Temperature and <span class="hlt">air</span> <span class="hlt">exchange</span> rates were positively associated with fungi and N-acetyl-beta-d-glucosaminidase and negatively with bacteria and the total inflammatory potential. Although temperature, relative humidity, and <span class="hlt">air</span> <span class="hlt">exchange</span> rates were significantly associated with several indoor microbial exposures, they could not fully explain the observed seasonal variations when tested in a mixed statistical <span class="hlt">model</span>. In conclusion, the season significantly affects indoor microbial exposures, which are influenced by temperature, relative humidity, and <span class="hlt">air</span> <span class="hlt">exchange</span> rates. PMID:23001651</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17346778','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17346778"><span><span class="hlt">Modelling</span> of the long-term fate of pesticide residues in agricultural soils and their <span class="hlt">surface</span> <span class="hlt">exchange</span> with the atmosphere: Part II. Projected long-term fate of pesticide residues.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Scholtz, M T; Bidleman, T F</p> <p>2007-05-01</p> <p>In the first part of this paper, a simple coupled dynamic soil-atmosphere <span class="hlt">model</span> for studying the gaseous <span class="hlt">exchange</span> of pesticide soil residues with the atmosphere is described and evaluated by comparing <span class="hlt">model</span> results with published measurements of pesticide concentrations in <span class="hlt">air</span> and soil. In Part II, the <span class="hlt">model</span> is used to study the concentration profiles of pesticide residues in both undisturbed and annually tilled agricultural soils. Future trends are estimated for the measured <span class="hlt">air</span> and soil concentrations of lindane and six highly persistent pesticides (toxaphene, p,p'-DDE, dieldrin, cis- and trans-chlordane and trans-nonachlor) over a twenty-year period due to volatilization and leaching into the deeper soil. Wet deposition and particle associated pesticide deposition (that increase soil residue concentrations) and soil erosion, degradation in the soil (other than for lindane) and run-off in precipitation are not considered in this study. Estimates of the rain deposition fluxes are reported that show that, other than for lindane, net volatilization fluxes greatly exceed rain deposition fluxes. The <span class="hlt">model</span> shows that the persistent pesticides studied are highly immobile in soil and that loss of these highly persistent residues from the soil is by volatilization rather than leaching into the deeper soil. The soil residue levels of these six pesticides are currently sources of net volatilization to the atmosphere and will remain so for many years. The maximum rate of volatilization from the soil was simulated by setting the atmospheric background concentration to zero; these simulations show that the rates of volatilization will not be significantly increased since soil resistance rather than the atmospheric concentration controls the volatilization rates. Annual tilling of the soils increases the volatilization loss to the atmosphere. Nonetheless, the <span class="hlt">model</span> predicts that, if only <span class="hlt">air</span>-soil <span class="hlt">exchange</span> is considered, more than 76% of current persistent pesticide residues</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JGRD..11310105L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JGRD..11310105L"><span>Assessment of <span class="hlt">surface</span> <span class="hlt">air</span> temperature over the Arctic Ocean in reanalysis and IPCC AR4 <span class="hlt">model</span> simulations with IABP/POLES observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Jiping; Zhang, Zhanhai; Hu, Yongyun; Chen, Liqi; Dai, Yongjiu; Ren, Xiaobo</p> <p>2008-05-01</p> <p>The <span class="hlt">surface</span> <span class="hlt">air</span> temperature (SAT) over the Arctic Ocean in reanalyses and global climate <span class="hlt">model</span> simulations was assessed using the International Arctic Buoy Programme/Polar <span class="hlt">Exchange</span> at the Sea <span class="hlt">Surface</span> (IABP/POLES) observations for the period 1979-1999. The reanalyses, including the National Centers for Environmental Prediction Reanalysis II (NCEP2) and European Centre for Medium-Range Weather Forecast 40-year Reanalysis (ERA40), show encouraging agreement with the IABP/POLES observations, although some spatiotemporal discrepancies are noteworthy. The reanalyses have warm annual mean biases and underestimate the observed interannual SAT variability in summer. Additionally, NCEP2 shows an excessive warming trend. Most <span class="hlt">model</span> simulations (coordinated by the International Panel on Climate Change for its Fourth Assessment Report) reproduce the annual mean, seasonal cycle, and trend of the observed SAT reasonably well, particularly the multi-<span class="hlt">model</span> ensemble mean. However, large discrepancies are found. Some <span class="hlt">models</span> have the annual mean SAT biases far exceeding the standard deviation of the observed interannul SAT variability and the across-<span class="hlt">model</span> standard deviation. Spatially, the largest inter-<span class="hlt">model</span> variance of the annual mean SAT is found over the North Pole, Greenland Sea, Barents Sea and Baffin Bay. Seasonally, a large spread of the simulated SAT among the <span class="hlt">models</span> is found in winter. The <span class="hlt">models</span> show interannual variability and decadal trend of various amplitudes, and can not capture the observed dominant SAT mode variability and cooling trend in winter. Further discussions of the possible attributions to the identified SAT errors for some <span class="hlt">models</span> suggest that the <span class="hlt">model</span>'s performance in the sea ice simulation is an important factor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhFl...29d5107S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhFl...29d5107S"><span><span class="hlt">Surface</span> velocity divergence <span class="hlt">model</span> of <span class="hlt">air</span>/water interfacial gas transfer in open-channel flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sanjou, M.; Nezu, I.; Okamoto, T.</p> <p>2017-04-01</p> <p><span class="hlt">Air</span>/water interfacial gas transfer through a free <span class="hlt">surface</span> plays a significant role in preserving and restoring water quality in creeks and rivers. However, direct measurements of the gas transfer velocity and reaeration coefficient are still difficult, and therefore a reliable prediction <span class="hlt">model</span> needs to be developed. Varying systematically the bulk-mean velocity and water depth, laboratory flume experiments were conducted and we measured <span class="hlt">surface</span> velocities and dissolved oxygen (DO) concentrations in open-channel flows to reveal the relationship between DO transfer velocity and <span class="hlt">surface</span> divergence (SD). Horizontal particle image velocimetry measurements provide the time-variations of <span class="hlt">surface</span> velocity divergence. Positive and negative regions of <span class="hlt">surface</span> velocity divergence are transferred downstream in time, as occurs in boil phenomenon on natural river free-<span class="hlt">surfaces</span>. The result implies that interfacial gas transfer is related to bottom-situated turbulence motion and vertical mass transfer. The original SD <span class="hlt">model</span> focuses mainly on small-scale viscous motion, and this <span class="hlt">model</span> strongly depends on the water depth. Therefore, we modify the SD <span class="hlt">model</span> theoretically to accommodate the effects of the water depth on gas transfer, introducing a non-dimensional parameter that includes contributions of depth-scale large-vortex motion, such as secondary currents, to <span class="hlt">surface</span> renewal events related to DO transport. The modified SD <span class="hlt">model</span> proved effective and reasonable without any dependence on the bulk mean velocity and water depth, and has a larger coefficient of determination than the original SD <span class="hlt">model</span>. Furthermore, <span class="hlt">modeling</span> of friction velocity with the Reynolds number improves the practicality of a new formula that is expected to be used in studies of natural rivers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/203613-gaseous-exchange-polycyclic-aromatic-hydrocarbons-across-air-water-interface-lower-chesapeake-bay','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/203613-gaseous-exchange-polycyclic-aromatic-hydrocarbons-across-air-water-interface-lower-chesapeake-bay"><span>Gaseous <span class="hlt">exchange</span> of polycyclic aromatic hydrocarbons across the <span class="hlt">air</span>-water interface of lower Chesapeake Bay</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>Gustafson, K.E.; Dickhut, R.M.</p> <p>1995-12-31</p> <p>The gaseous <span class="hlt">exchange</span> fluxes of polycyclic aromatic hydrocarbons (PAHs) across the <span class="hlt">air</span>-water interface of lower Chesapeake Bay were determined using a modified two-film <span class="hlt">exchange</span> <span class="hlt">model</span>. Sampling covered the period January 1994 to June 1995 for five sites on lower Chesapeake Bay ranging from rural to urban and highly industrialized. Simultaneous <span class="hlt">air</span> and water samples were collected and the atmospheric gas phase and water column dissolved phase analyzed via GC/MS for 17 PAHs. The direction and magnitude of flux for each PAH was calculated using Henry`s law constants, hydrological and meteorological parameters, Temperature was observed to be an important environmental factormore » in determining both the direction and magnitude of PAH gas <span class="hlt">exchange</span>. Nonetheless, wind speed significantly impacts mass transfer coefficients, and therefore was found to control the magnitude of flux. Spatial and temporal variation of PAH gaseous <span class="hlt">exchange</span> fluxes were examined. Fluxes were determined to be both into and out of Chesapeake Bay. The range of gas <span class="hlt">exchange</span> fluxes ({minus}560 to 600{micro}g/M{sup 2}*Mo) is of the same order to 10X greater than atmospheric wet and dry depositional fluxes to lower Chesapeake Bay. The results of this study support the hypothesis that gas <span class="hlt">exchange</span> is a major transport process affecting the net loadings of PAHs in lower Chesapeake Bay.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDL20011S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDL20011S"><span>Boundary layers at a dynamic interface: <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of heat and mass</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Szeri, Andrew</p> <p>2017-11-01</p> <p><span class="hlt">Exchange</span> of mass or heat across a turbulent liquid-gas interface is a problem of critical interest, especially in <span class="hlt">air</span>-sea transfer of natural and man-made gases involved in climate change. The goal in this research area is to determine the gas flux from <span class="hlt">air</span> to sea or vice versa. For sparingly soluble non-reactive gases, this is controlled by liquid phase turbulent velocity fluctuations that act on the thin species concentration boundary layer on the liquid side of the interface. If the fluctuations in <span class="hlt">surface</span>-normal velocity and gas concentration differences are known, then it is possible to determine the turbulent contribution to the gas flux. However, there is no suitable fundamental direct approach in the general case where neither of these quantities can be easily measured. A new approach is presented to deduce key aspects about the near-<span class="hlt">surface</span> turbulent motions from remote measurements, which allows one to determine the gas transfer velocity, or gas flux per unit area if overall concentration differences are known. The approach is illustrated with conceptual examples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=261773&keyword=Human+AND+interaction&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=261773&keyword=Human+AND+interaction&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>Spatiotemporally‐Resolved <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate as a Modifier of Acute <span class="hlt">Air</span> Pollution‐Related Morbidity in AtlantaMorbidity in Atlanta</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>Epidemiological studies frequently use central site concentrations as surrogates of exposure to <span class="hlt">air</span> pollutants. Variability in <span class="hlt">air</span> pollutant infiltration due to differential <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) is potentially a major factor affecting the relationship between central site c...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMEP43D0770P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMEP43D0770P"><span>Wind driven vertical transport in a vegetated, wetland water column with <span class="hlt">air</span>-water gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poindexter, C.; Variano, E. A.</p> <p>2010-12-01</p> <p> gas transfer coefficient, k, for both a vegetated condition and a control condition (no cylinders). The presence of cylinders in the tank substantially increased the rate of the gas transfer. For the highest wind speed, the gas transfer coefficient was several times higher when cylinders were present compared to when they were not. The gas transfer coefficient for the vegetated condition also proved sensitive to wind speed, increasing markedly with increasing mean wind speeds. Profiles of dissolved oxygen revealed well-mixed conditions in the bulk water column following prolonged <span class="hlt">air</span>-flow above the water <span class="hlt">surface</span>, suggesting application of the thin-film <span class="hlt">model</span> is appropriate. The enhanced gas <span class="hlt">exchange</span> observed might be explained by increased turbulent kinetic energy within the water column and the anisotropy of the cylinder array, which constrains horizontal motions more than vertical motions. Improved understanding of gas <span class="hlt">exchange</span> in vegetated water columns may be of particularly use to investigations of carbon fluxes and soil accretion in wetlands. Reference: Nepf, H. (1999), Drag, turbulence, and diffusion in flow through emergent vegetation, Water Resour. Res., 35(2), 479-489.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.2781S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.2781S"><span>Boundary layers at a dynamic interface: <span class="hlt">Air</span>-sea <span class="hlt">exchange</span> of heat and mass</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Szeri, Andrew J.</p> <p>2017-04-01</p> <p><span class="hlt">Exchange</span> of mass or heat across a turbulent liquid-gas interface is a problem of critical interest, especially in <span class="hlt">air</span>-sea transfer of natural and anthropogenic gases involved in the study of climate. The goal in this research area is to determine the gas flux from <span class="hlt">air</span> to sea or vice versa. For sparingly soluble nonreactive gases, this is controlled by liquid phase turbulent velocity fluctuations that act on the thin species concentration boundary layer on the liquid side of the interface. If the fluctuations in <span class="hlt">surface</span>-normal velocity w' and gas concentration c' are known, then it is possible to determine the turbulent contribution to the gas flux. However, there is no suitable fundamental direct approach in the general case where neither w' nor c' can be easily measured. A new approach is presented to deduce key aspects about the near-<span class="hlt">surface</span> turbulent motions from measurements that can be taken by an infrared (IR) camera. An equation is derived with inputs being the <span class="hlt">surface</span> temperature and heat flux, and a solution method developed for the <span class="hlt">surface</span>-normal strain experienced over time by boundary layers at the interface. Because the thermal and concentration boundary layers experience the same near-<span class="hlt">surface</span> fluid motions, the solution for the <span class="hlt">surface</span>-normal strain determines the gas flux or gas transfer velocity. Examples illustrate the approach in the cases of complete <span class="hlt">surface</span> renewal, partial <span class="hlt">surface</span> renewal, and insolation. The prospects for use of the approach in flows characterized by sheared interfaces or rapid boundary layer straining are explored.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880025281&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dheat%2Bexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880025281&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dheat%2Bexchange"><span>Heat transfer to and from vegetated <span class="hlt">surfaces</span> - An analytical method for the bulk <span class="hlt">exchange</span> coefficients</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Massman, William J.</p> <p>1987-01-01</p> <p>The semianalytical <span class="hlt">model</span> outlined in a previous study (Massman, 1987) to describe momentum <span class="hlt">exchange</span> between the atmosphere and vegetated <span class="hlt">surfaces</span> is extended to include the <span class="hlt">exchange</span> of heat. The methods employed are based on one-dimensional turbulent diffusivities, and use analytical solutions to the steady-state diffusion equation. The <span class="hlt">model</span> is used to assess the influence that the canopy foliage structure and density, the wind profile structure within the canopy, and the shelter factor can have upon the inverse <span class="hlt">surface</span> Stanton number (kB exp -1), as well as to explore the consequences of introducing a scalar displacement height which can be different from the momentum displacement height. In general, the triangular foliage area density function gives results which agree more closely with observations than that for constant foliage area density. The intended application of this work is for parameterizing the bulk aerodynamic resistances for heat and momentum <span class="hlt">exchange</span> for use within large-scale <span class="hlt">models</span> of plant-atmosphere <span class="hlt">exchanges</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018BoLMe.167..445L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018BoLMe.167..445L"><span>Signatures of <span class="hlt">Air</span>-Wave Interactions Over a Large Lake</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Qi; Bou-Zeid, Elie; Vercauteren, Nikki; Parlange, Marc</p> <p>2018-06-01</p> <p>The <span class="hlt">air</span>-water <span class="hlt">exchange</span> of momentum and scalars (temperature and water vapour) is investigated using the Lake-Atmosphere Turbulent <span class="hlt">EXchange</span> (LATEX) dataset. The wind waves and swell are found to affect the coupling between the water <span class="hlt">surface</span> and the <span class="hlt">air</span> differently. The <span class="hlt">surface</span>-stress vector aligns with the wind velocity in the presence of wind waves, but a wide range of stress-wind misalignment angles is observed during swell. The momentum transport efficiency decreases when significant stress-wind misalignment is present, suggesting a strong influence of <span class="hlt">surface</span> wave properties on <span class="hlt">surface</span> drag. Based on this improved understanding of the role of wave-wind misalignment, a new relative wind speed for <span class="hlt">surface</span>-layer similarity formulations is proposed and tested using the data. The new expression yields a value of the von Kármán constant (κ ) of 0.38, compared to 0.36 when using the absolute wind speed, as well as reduced data fitting errors. Finally, the ratios of aerodynamic to scalar roughness lengths are computed and various existing <span class="hlt">models</span> in the literature are tested using least-square fitting to the observed ratios. The tests are able to discriminate between the performance of various <span class="hlt">models</span>; however, they also indicate that more investigations are required to understand the physics of scalar <span class="hlt">exchanges</span> over waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25985421','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25985421"><span>Impact of <span class="hlt">air</span> and water vapor environments on the hydrophobicity of <span class="hlt">surfaces</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weisensee, Patricia B; Neelakantan, Nitin K; Suslick, Kenneth S; Jacobi, Anthony M; King, William P</p> <p>2015-09-01</p> <p>Droplet wettability and mobility play an important role in dropwise condensation heat transfer. Heat <span class="hlt">exchangers</span> and heat pipes operate at liquid-vapor saturation. We hypothesize that the wetting behavior of liquid water on microstructures surrounded by pure water vapor differs from that for water droplets in <span class="hlt">air</span>. The static and dynamic contact angles and contact angle hysteresis of water droplets were measured in <span class="hlt">air</span> and pure water vapor environments inside a pressure vessel. Pressures ranged from 60 to 1000 mbar, with corresponding saturation temperatures between 36 and 100°C. The wetting behavior was studied on four hydrophobic <span class="hlt">surfaces</span>: flat Teflon-coated, micropillars, micro-scale meshes, and nanoparticle-coated with hierarchical micro- and nanoscale roughness. Static advancing contact angles are 9° lower in the water vapor environment than in <span class="hlt">air</span> on a flat <span class="hlt">surface</span>. One explanation for this reduction in contact angles is water vapor adsorption to the Teflon. On microstructured <span class="hlt">surfaces</span>, the vapor environment has little effect on the static contact angles. In all cases, variations in pressure and temperature do not influence the wettability and mobility of the water droplets. In most cases, advancing contact angles increase and contact angle hysteresis decreases when the droplets are sliding or rolling down an inclined <span class="hlt">surface</span>. Copyright © 2015 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009GeoRL..3621605V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009GeoRL..3621605V"><span>A generalized <span class="hlt">model</span> for the <span class="hlt">air</span>-sea transfer of dimethyl sulfide at high wind speeds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vlahos, Penny; Monahan, Edward C.</p> <p>2009-11-01</p> <p>The <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of dimethyl sulfide (DMS) is an important component of ocean biogeochemistry and global climate <span class="hlt">models</span>. Both laboratory experiments and field measurements of DMS transfer rates have shown that the <span class="hlt">air</span>-sea flux of DMS is analogous to that of other significant greenhouse gases such as CO2 at low wind speeds (<10 m/s) but that these DMS transfer rates may diverge from other gases as wind speeds increase. Herein we provide a mechanism that predicts the attenuation of DMS transfer rates at high wind speeds. The <span class="hlt">model</span> is based on the amphiphilic nature of DMS that leads to transfer delay at the water-bubble interface and becomes significant at wind speeds above >10 m/s. The result is an attenuation of the dimensionless Henry's Law constant (H) where (Heff = H/(1 + (Cmix/Cw) ΦB) by a solubility enhancement Cmix/Cw, and the fraction of bubble <span class="hlt">surface</span> area per m2 <span class="hlt">surface</span> ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.H31A1400O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.H31A1400O"><span>Investigation of the influence of atmospheric stability and turbulence on land-atmosphere <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Osibanjo, O.; Holmes, H.</p> <p>2015-12-01</p> <p><span class="hlt">Surface</span> energy fluxes are <span class="hlt">exchanged</span> between the <span class="hlt">surface</span> of the earth and the atmosphere and impact weather, climate, and <span class="hlt">air</span> quality. The radiation from the sun triggers the <span class="hlt">surface</span>-atmosphere interaction during the day as heat is transmitted to the <span class="hlt">surface</span> and the <span class="hlt">surface</span> heats the <span class="hlt">air</span> directly above generating wind (i.e., thermal turbulence) that transports heat, moisture, and momentum in the atmospheric boundary layer (ABL). This process is impacted by greenhouse gasses (i.e., water vapor, carbon dioxide and other trace gases) that absorb heat emitted by the earth's <span class="hlt">surface</span>. The concentrations of atmospheric greenhouse gasses are increasing leading to changes in ABL dynamics as a result of the changing <span class="hlt">surface</span> energy balance. The ABL processes are important to characterize because they are difficult to parameterize in global and regional scale atmospheric <span class="hlt">models</span>. Empirical data can be collected using eddy covariance micrometeorological methods to measure turbulent fluxes (e.g., sensible heat, moisture, and CO2) and quantify the <span class="hlt">exchange</span> between the <span class="hlt">surface</span> and the atmosphere. The objective of this work is to calculate <span class="hlt">surface</span> fluxes using observational data collected during one week in September 2014 from a monitoring site in Echo, Oregon. The site is located in the Columbia Basin with rolling terrain, irrigated farmland, and over 100 wind turbines. The 10m tower was placed in a small valley depression to isolate nighttime cold <span class="hlt">air</span> pools. This work will present observations of momentum, sensible heat, moisture, and carbon dioxide fluxes from data collected at a sampling frequency of 10Hz at four heights. Atmospheric stability is determined using Monin-Obukov length and flux Richardson number, and the impact of stability on <span class="hlt">surface</span>-atmosphere <span class="hlt">exchange</span> is investigated. This work will provide a better understanding of <span class="hlt">surface</span> fluxes and mixing, particularly during stable ABL periods, and the results can be used to compare with numerical <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880053801&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dheat%2Bexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880053801&hterms=heat+exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dheat%2Bexchange"><span>A four-layer <span class="hlt">model</span> for the heat budget of homogeneous land <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Choudhury, B. J.; Monteith, J. L.</p> <p>1988-01-01</p> <p>The present <span class="hlt">model</span> envisions the heat balance of a homogeneous land <span class="hlt">surface</span> in terms of available energy, a set of driving potentials, and parameters for the physical state of the soil and vegetation. Two unique features of the <span class="hlt">model</span> are: (1) the expression of the interaction of evaporation from the soil and from foliage by changes in the value of the saturation vapor pressure deficit of <span class="hlt">air</span> in the canopy (the conclusions of this interaction being consistent with field observations); and (2) the treatment of sensible and latent heat <span class="hlt">exchange</span> between the atmosphere and a soil consisting of two discrete layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22145748','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22145748"><span>Selective permeation of moisture and VOCs through polymer membranes used in total heat <span class="hlt">exchangers</span> for indoor <span class="hlt">air</span> ventilation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, L-Z; Zhang, X-R; Miao, Q-Z; Pei, L-X</p> <p>2012-08-01</p> <p>Fresh <span class="hlt">air</span> ventilation is central to indoor environmental control. Total heat <span class="hlt">exchangers</span> can be key equipment for energy conservation in ventilation. Membranes have been used for total heat <span class="hlt">exchangers</span> for more than a decade. Much effort has been spent to achieve water vapor permeability of various membranes; however, relatively little attention has been paid to the selectivity of moisture compared with volatile organic compounds (VOCs) through such membranes. In this investigation, the most commonly used membranes, both hydrophilic and hydrophobic ones, are tested for their permeability for moisture and five VOCs (acetic acid, formaldehyde, acetaldehyde, toluene, and ethane). The selectivity of moisture vs. VOCs in these membranes is then evaluated. With a solution-diffusion <span class="hlt">model</span>, the solubility and diffusivity of moisture and VOCs in these membranes are calculated. The resulting data could provide some reference for future material selection. Total heat <span class="hlt">exchangers</span> are important equipment for fresh <span class="hlt">air</span> ventilation with energy conservation. However, their implications for indoor <span class="hlt">air</span> quality in terms of volatile organic compound permeation have not been known. The data in this article help us to clarify the impacts on indoor VOC levels of membrane-based heat <span class="hlt">exchangers</span>. Guidelines for material selection can be obtained for future use total heat <span class="hlt">exchangers</span> for building ventilation. © 2011 John Wiley & Sons A/S.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://lofe.dukejournals.org/content/2/1.abstract','USGSPUBS'); return false;" href="http://lofe.dukejournals.org/content/2/1.abstract"><span><span class="hlt">Air</span>-water oxygen <span class="hlt">exchange</span> in a large whitewater river</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hall, Robert O.; Kennedy, Theodore A.; Rosi-Marshall, Emma J.</p> <p>2012-01-01</p> <p><span class="hlt">Air</span>-water gas <span class="hlt">exchange</span> governs fluxes of gas into and out of aquatic ecosystems. Knowing this flux is necessary to calculate gas budgets (i.e., O2) to estimate whole-ecosystem metabolism and basin-scale carbon budgets. Empirical data on rates of gas <span class="hlt">exchange</span> for streams, estuaries, and oceans are readily available. However, there are few data from large rivers and no data from whitewater rapids. We measured gas transfer velocity in the Colorado River, Grand Canyon, as decline in O2 saturation deficit, 7 times in a 28-km segment spanning 7 rapids. The O2 saturation deficit exists because of hypolimnetic discharge from Glen Canyon Dam, located 25 km upriver from Lees Ferry. Gas transfer velocity (k600) increased with slope of the immediate reach. k600 was -1 in flat reaches, while k600 for the steepest rapid ranged 3600-7700 cm h-1, an extremely high value of k600. Using the rate of gas <span class="hlt">exchange</span> per unit length of water <span class="hlt">surface</span> elevation (Kdrop, m-1), segment-integrated k600 varied between 74 and 101 cm h-1. Using Kdrop we scaled k600 to the remainder of the Colorado River in Grand Canyon. At the scale corresponding to the segment length where 80% of the O2 <span class="hlt">exchanged</span> with the atmosphere (mean length = 26.1 km), k600 varied 4.5-fold between 56 and 272 cm h-1 with a mean of 113 cm h-1. Gas transfer velocity for the Colorado River was higher than those from other aquatic ecosystems because of large rapids. Our approach of scaling k600 based on Kdrop allows comparing gas transfer velocity across rivers with spatially heterogeneous morphology.</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('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=214946&keyword=chemical+AND+pollution+AND+boundary&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=214946&keyword=chemical+AND+pollution+AND+boundary&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>Atmospheric Boundary Layer <span class="hlt">Modeling</span> for Combined Meteorology and <span class="hlt">Air</span> Quality Systems</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>Atmospheric Eulerian grid <span class="hlt">models</span> for mesoscale and larger applications require sub-grid <span class="hlt">models</span> for turbulent vertical <span class="hlt">exchange</span> processes, particularly within the Planetary Boundary Layer (PSL). In combined meteorology and <span class="hlt">air</span> quality <span class="hlt">modeling</span> systems consistent PSL <span class="hlt">modeling</span> of wi...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.5581L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.5581L"><span>Sum-Frequency Generation Spectroscopy for Studying Organic Layers at Water-<span class="hlt">Air</span> Interfaces: Microlayer Monitoring and <span class="hlt">Surface</span> Reactivity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Laß, Kristian; Kleber, Joscha; Bange, Hermann; Friedrichs, Gernot</p> <p>2015-04-01</p> <p>The sea <span class="hlt">surface</span> microlayer, according to commonly accepted terminology, comprises the topmost millimetre of the oceanic water column. It is often enriched with organic matter and is directly influenced by sunlight exposure and gas <span class="hlt">exchange</span> with the atmosphere, hence making it a place for active biochemistry and photochemistry as well as for heterogeneous reactions. In addition, <span class="hlt">surface</span> active material either is formed or accumulates directly at the <span class="hlt">air</span>-water interface and gives rise to very thin layers, sometimes down to monomolecular thickness. This "sea <span class="hlt">surface</span> nanolayer" determines the viscoelastic properties of the seawater <span class="hlt">surface</span> and thus may impact the turbulent <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> rates. To this effect, this small scale layer presumably plays an important role for large scale changes of atmospheric trace gas concentrations (e.g., by modulating the ocean carbon sink characteristics) with possible implications for coupled climate <span class="hlt">models</span>. To date, detailed knowledge about the composition, structure, and reactivity of the sea <span class="hlt">surface</span> nanolayer is still scarce. Due to its small vertical dimension and the small amount of material, this surfactant layer is very difficult to separate and analyse. A way out is the application of second-order nonlinear optical methods, which make a direct <span class="hlt">surface</span>-specific and background-free detection of this interfacial layer possible. In recent years, we have introduced the use of vibrational sum frequency generation (VSFG) spectroscopy to gain insight into natural and artificial organic monolayers at the <span class="hlt">air</span>-water interface. In this contribution, the application of VSFG spectroscopy for the analysis of the sea <span class="hlt">surface</span> nanolayer will be illustrated. Resulting spectra are interpreted in terms of layer composition and surfactant classes, in particular with respect to carbohydrate-containing molecules such as glycolipids. The partitioning of the detected surfactants into soluble and non-soluble ("wet" and "dry") surfactants will be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.H11B1297C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.H11B1297C"><span>Evaluate the Relative Importance of Subsurface Lateral Energy <span class="hlt">Exchange</span> to Ground Heat Flux and Energy Balance over the Heterogeneous <span class="hlt">Surface</span> of a Sub-tropical Wetland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>CUI, W.; Chui, T. F. M.</p> <p>2016-12-01</p> <p>Subsurface lateral water and energy <span class="hlt">exchanges</span> are often ignored in methods involving a <span class="hlt">surface</span> energy balance under the homogeneity assumption, which may affect the estimation of evapotranspiration over a heterogeneous <span class="hlt">surface</span>. Wetlands, however, are heterogeneous with vegetated areas and open water, making it difficult to accurately measure and estimate evapotranspiration. This study estimated the subsurface lateral energy <span class="hlt">exchange</span> between the reed bed and shallow open water of a wetland within Mai Po Nature Reserve in Hong Kong, and further discussed its relative importance to the ground heat flux and energy balance over the wetland <span class="hlt">surface</span>. An array of water level and temperature sensors were installed in the reed bed and the adjacent water, together with an eddy covariance system. The results suggested that the lateral energy <span class="hlt">exchange</span> was over 30% of ground heat flux for half of the monitoring period, and should therefore be accounted for during the measurement of ground heat flux. However, the lateral energy <span class="hlt">exchange</span> could not explain the energy balance disclosure at the site, as the variation was in phase with the residual of energy budget during the summer but was out of phase during the winter. Furthermore, this study developed a convolution <span class="hlt">model</span> to estimate the lateral energy <span class="hlt">exchange</span> based on <span class="hlt">air</span> temperature which is readily available at many sites worldwide. This study overall enhanced our understanding of the subsurface lateral energy <span class="hlt">exchange</span>, and possibly our estimation of evapotranspiration in heterogeneous environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EPJWC..2405004I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EPJWC..2405004I"><span>Time lag between the tropopause height and the levels of 7Be concentration in near <span class="hlt">surface</span> <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>Ioannidou, A.; Vasileiadis, A.; Melas, D.</p> <p>2012-04-01</p> <p>The concentration of 7Be at near <span class="hlt">surface</span> <span class="hlt">air</span> has been determined over 2009, a year of a deep solar minimum, in the region of Thessaloniki, Greece at 40°62' N, 22°95'E. In geomagnetic latitudes over 40° N, the elevation of the tropopause during the warm summer months and the vertical <span class="hlt">exchange</span> of <span class="hlt">air</span> masses within the troposphere cause greater mixture of the <span class="hlt">air</span> masses resulting in higher concentration levels for 7Be in <span class="hlt">surface</span> <span class="hlt">air</span>. The positive correlation between the monthly activity concentration of 7Be and the tropopause height (0.94, p < 0.0001), and also between 7Be concentration and the temperature T (°C) (R = 0.97, p < 0.001), confirm that the increased rate of vertical transport within the troposphere, especially during warmer summer months, has as a result the descent to <span class="hlt">surface</span> of <span class="hlt">air</span> masses enriched in 7Be. However, the 7Be concentration levels in near <span class="hlt">surface</span> <span class="hlt">air</span> are not expected to respond immediately to the change of elevation of the tropopause. It was found that there's a time lag of ~ 3 days between the change in the daily <span class="hlt">surface</span> concentrations of 7Be the change in the elevation of the tropopause.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1953j0089J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1953j0089J"><span>Experimental temperature analysis of simple & hybrid earth <span class="hlt">air</span> tunnel heat <span class="hlt">exchanger</span> in series connection at Bikaner Rajasthan India</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jakhar, O. P.; Sharma, Chandra Shekhar; Kukana, Rajendra</p> <p>2018-05-01</p> <p>The Earth <span class="hlt">Air</span> Tunnel Heat <span class="hlt">Exchanger</span> System is a passive <span class="hlt">air</span>-conditioning system which has no side effect on earth climate and produces better cooling effect and heating effect comfortable to human body. It produces heating effect in winter and cooling effect in summer with the minimum power consumption of energy as compare to other <span class="hlt">air</span>-conditioning devices. In this research paper Temperature Analysis was done on the two systems of Earth <span class="hlt">Air</span> Tunnel Heat <span class="hlt">Exchanger</span> experimentally for summer cooling purpose. Both the system was installed at Mechanical Engineering Department Government Engineering College Bikaner Rajasthan India. Experimental results concludes that the Average <span class="hlt">Air</span> Temperature Difference was found as 11.00° C and 16.27° C for the Simple and Hybrid Earth <span class="hlt">Air</span> Tunnel Heat <span class="hlt">Exchanger</span> in Series Connection System respectively. The Maximum <span class="hlt">Air</span> Temperature Difference was found as 18.10° C and 23.70° C for the Simple and Hybrid Earth <span class="hlt">Air</span> Tunnel Heat <span class="hlt">Exchanger</span> in Series Connection System respectively. The Minimum <span class="hlt">Air</span> Temperature Difference was found as 5.20° C and 11.70° C for the Simple and Hybrid Earth <span class="hlt">Air</span> Tunnel Heat <span class="hlt">Exchanger</span> in Series Connection System respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFD.E4003J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFD.E4003J"><span>Respiratory Mechanics and Gas <span class="hlt">Exchange</span>: The Effect of Surfactants</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jbaily, Abdulrahman; Szeri, Andrew J.</p> <p>2017-11-01</p> <p>The purpose of the lung is to <span class="hlt">exchange</span> gases, primarily oxygen and carbon dioxide, between the atmosphere and the circulatory system. To enable this <span class="hlt">exchange</span>, the airways in the lungs terminate in some 300 million alveoli that provide adequate <span class="hlt">surface</span> area for transport. During breathing, work must be done to stretch various tissues to accommodate a greater volume of gas. Considerable work must also be done to expand the liquid lining (hypophase) that coats the interior <span class="hlt">surfaces</span> of the alveoli. This is enabled by a <span class="hlt">surface</span> active lipo-protein complex, known as pulmonary surfactant, that modifies the <span class="hlt">surface</span> tension at the hypophase-<span class="hlt">air</span> interface. Surfactants also serve as physical barriers that modify the rate of gas transfer across interfaces. We develop a mathematical <span class="hlt">model</span> to study the action of pulmonary surfactant and its determinative contributions to breathing. The <span class="hlt">model</span> is used to explore the influence of surfactants on alveolar mechanics and on gas <span class="hlt">exchange</span>: it relates the work of respiration at the level of the alveolus to the gas <span class="hlt">exchange</span> rate through the changing influence of pulmonary surfactant over the breathing cycle. This work is motivated by a need to develop improved surfactant replacement therapies to treat serious medical conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17328184','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17328184"><span><span class="hlt">Air</span>-water <span class="hlt">exchange</span> and dry deposition of polybrominated diphenyl ethers at a coastal site in Izmir Bay, Turkey.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cetin, Banu; Odabasi, Mustafa</p> <p>2007-02-01</p> <p>The <span class="hlt">air</span>-water <span class="hlt">exchange</span> of polybrominated diphenyl ethers (PBDEs), an emerging class of persistent organic pollutants (POPs), was investigated using paired <span class="hlt">air</span>-water samples (n = 15) collected in July and December, 2005 from Guzelyali Port in Izmir Bay, Turkey. Total dissolved-phase water concentrations of PBDEs (sigma7PBDEs) were 212 +/- 65 and 87 +/- 57 pg L(-1) (average +/- SD) in summer and winter, respectively. BDE-209 was the most abundant congener in all samples, followed by BDE-99 and -47. Average ambient gas-phase sigma7PBDE concentrations were between 189 +/- 61 (summer) and 76 +/- 65 pg m(-3) (winter). Net <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes ranged from -0.9 +/- 1.0 (BDE-28) (volatilization) to 11.1 +/- 5.4 (BDE-209) ng m(-2) day(-1) (deposition). The BDE-28 fluxes were mainly volatilization while the other congeners were deposited. Gas- and dissolved-phase concentrations were significantly correlated (P = 0.33-0.55, p < 0.05, except for BDE-209, r = 0.05, p > 0.05) indicating thatthe atmosphere controls the <span class="hlt">surface</span> water PBDE levels in this coastal environment. Estimated particulate dry deposition fluxes ranged between 2.7 +/- 1.9 (BDE-154) and 116 +/- 84 ng m(-2) day(-1) (BDE-209) indicating that dry deposition is also a significant input to <span class="hlt">surface</span> waters in the study area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SurSR..71..367C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SurSR..71..367C"><span>The nature of the <span class="hlt">air</span>-cleaved mica <span class="hlt">surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Christenson, Hugo K.; Thomson, Neil H.</p> <p>2016-06-01</p> <p>The accepted image of muscovite mica is that of an inert and atomically smooth <span class="hlt">surface</span>, easily prepared by cleavage in an ambient atmosphere. Consequently, mica is extensively used a <span class="hlt">model</span> substrate in many fundamental studies of <span class="hlt">surface</span> phenomena and as a substrate for AFM imaging of biomolecules. In this review we present evidence from the literature that the above picture is not quite correct. The mica used in experimental work is almost invariably cleaved in laboratory <span class="hlt">air</span>, where a reaction between the mica <span class="hlt">surface</span>, atmospheric CO2 and water occurs immediately after cleavage. The evidence suggests very strongly that as a result the mica <span class="hlt">surface</span> becomes covered by up to one formula unit of K2CO3 per nm2, which is mobile under humid conditions, and crystallises under drier conditions. The properties of mica in <span class="hlt">air</span> or water vapour cannot be fully understood without reference to the <span class="hlt">surface</span> K2CO3, and many studies of the structure of adsorbed water on mica <span class="hlt">surfaces</span> may need to be revisited. With this new insight, however, the <span class="hlt">air</span>-cleaved mica should provide exciting opportunities to study phenomena such as two-dimensional ion diffusion, electrolyte effects on <span class="hlt">surface</span> conductivity, and two-dimensional crystal nucleation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-LRC-1957-B701_P-05383.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-LRC-1957-B701_P-05383.html"><span>Hot-<span class="hlt">Air</span> Jets/Ceramic Heat <span class="hlt">Exchangers</span>/ Materials for Nose Cones and Reentry Vehicles</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>1957-09-07</p> <p>L57-5383 Hot-<span class="hlt">air</span> jets employing ceramic heat <span class="hlt">exchangers</span> played an important role at Langley in the study of materials for ballistic missile nose cones and re-entry vehicles. Here a <span class="hlt">model</span> is being tested in one of theses jets at 4000 degrees Fahrenheit in 1957. Photograph published in Engineer in Charge: A History of the Langley Aeronautical Laboratory, 1917-1958 by James R. Hansen. Page 477.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E3SWC..2200027C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E3SWC..2200027C"><span>Industrial applications of the <span class="hlt">air</span> direct-contact, gravel, ground heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cepiński, Wojciech; Besler, Maciej</p> <p>2017-11-01</p> <p>The paper describes the analysis of possibility of using the <span class="hlt">air</span> direct-contact, gravel, ground heat <span class="hlt">exchanger</span> (Polish acronym BGWCiM), patented at the Wroclaw University of Science and Technology to prepare <span class="hlt">air</span> for conditioning rooms in the industry. Indicated the industry sectors where the application may be the most beneficial.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1437748-modeling-uranium-vi-adsorption-onto-montmorillonite-under-varying-carbonate-concentrations-surface-complexation-model-accounting-spillover-effect-surface-potential','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1437748-modeling-uranium-vi-adsorption-onto-montmorillonite-under-varying-carbonate-concentrations-surface-complexation-model-accounting-spillover-effect-surface-potential"><span><span class="hlt">Modeling</span> uranium(VI) adsorption onto montmorillonite under varying carbonate concentrations: A <span class="hlt">surface</span> complexation <span class="hlt">model</span> accounting for the spillover effect on <span class="hlt">surface</span> potential</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>Tournassat, C.; Tinnacher, R. M.; Grangeon, S.</p> <p></p> <p>The prediction of U(VI) adsorption onto montmorillonite clay is confounded by the complexities of: (1) the montmorillonite structure in terms of adsorption sites on basal and edge <span class="hlt">surfaces</span>, and the complex interactions between the electrical double layers at these <span class="hlt">surfaces</span>, and (2) U(VI) solution speciation, which can include cationic, anionic and neutral species. Previous U(VI)-montmorillonite adsorption and <span class="hlt">modeling</span> studies have typically expanded classical <span class="hlt">surface</span> complexation <span class="hlt">modeling</span> approaches, initially developed for simple oxides, to include both cation <span class="hlt">exchange</span> and <span class="hlt">surface</span> complexation reactions. However, previous <span class="hlt">models</span> have not taken into account the unique characteristics of electrostatic <span class="hlt">surface</span> potentials that occur at montmorillonitemore » edge sites, where the electrostatic <span class="hlt">surface</span> potential of basal plane cation <span class="hlt">exchange</span> sites influences the <span class="hlt">surface</span> potential of neighboring edge sites (‘spillover’ effect).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1437748-modeling-uranium-vi-adsorption-onto-montmorillonite-under-varying-carbonate-concentrations-surface-complexation-model-accounting-spillover-effect-surface-potential','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1437748-modeling-uranium-vi-adsorption-onto-montmorillonite-under-varying-carbonate-concentrations-surface-complexation-model-accounting-spillover-effect-surface-potential"><span><span class="hlt">Modeling</span> uranium(VI) adsorption onto montmorillonite under varying carbonate concentrations: A <span class="hlt">surface</span> complexation <span class="hlt">model</span> accounting for the spillover effect on <span class="hlt">surface</span> potential</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Tournassat, C.; Tinnacher, R. M.; Grangeon, S.; ...</p> <p>2017-10-06</p> <p>The prediction of U(VI) adsorption onto montmorillonite clay is confounded by the complexities of: (1) the montmorillonite structure in terms of adsorption sites on basal and edge <span class="hlt">surfaces</span>, and the complex interactions between the electrical double layers at these <span class="hlt">surfaces</span>, and (2) U(VI) solution speciation, which can include cationic, anionic and neutral species. Previous U(VI)-montmorillonite adsorption and <span class="hlt">modeling</span> studies have typically expanded classical <span class="hlt">surface</span> complexation <span class="hlt">modeling</span> approaches, initially developed for simple oxides, to include both cation <span class="hlt">exchange</span> and <span class="hlt">surface</span> complexation reactions. However, previous <span class="hlt">models</span> have not taken into account the unique characteristics of electrostatic <span class="hlt">surface</span> potentials that occur at montmorillonitemore » edge sites, where the electrostatic <span class="hlt">surface</span> potential of basal plane cation <span class="hlt">exchange</span> sites influences the <span class="hlt">surface</span> potential of neighboring edge sites (‘spillover’ effect).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1150902-multi-scale-modeling-approximation-assisted-optimization-bare-tube-heat-exchangers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1150902-multi-scale-modeling-approximation-assisted-optimization-bare-tube-heat-exchangers"><span>MULTI-SCALE <span class="hlt">MODELING</span> AND APPROXIMATION ASSISTED OPTIMIZATION OF BARE TUBE HEAT <span class="hlt">EXCHANGERS</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>Bacellar, Daniel; Ling, Jiazhen; Aute, Vikrant</p> <p>2014-01-01</p> <p><span class="hlt">Air</span>-to-refrigerant heat <span class="hlt">exchangers</span> are very common in <span class="hlt">air</span>-conditioning, heat pump and refrigeration applications. In these heat <span class="hlt">exchangers</span>, there is a great benefit in terms of size, weight, refrigerant charge and heat transfer coefficient, by moving from conventional channel sizes (~ 9mm) to smaller channel sizes (< 5mm). This work investigates new designs for <span class="hlt">air</span>-to-refrigerant heat <span class="hlt">exchangers</span> with tube outer diameter ranging from 0.5 to 2.0mm. The goal of this research is to develop and optimize the design of these heat <span class="hlt">exchangers</span> and compare their performance with existing state of the art designs. The <span class="hlt">air</span>-side performance of various tube bundle configurationsmore » are analyzed using a Parallel Parameterized CFD (PPCFD) technique. PPCFD allows for fast-parametric CFD analyses of various geometries with topology change. Approximation techniques drastically reduce the number of CFD evaluations required during optimization. Maximum Entropy Design method is used for sampling and Kriging method is used for metamodeling. Metamodels are developed for the <span class="hlt">air</span>-side heat transfer coefficients and pressure drop as a function of tube-bundle dimensions and <span class="hlt">air</span> velocity. The metamodels are then integrated with an <span class="hlt">air</span>-to-refrigerant heat <span class="hlt">exchanger</span> design code. This integration allows a multi-scale analysis of <span class="hlt">air</span>-side performance heat <span class="hlt">exchangers</span> including <span class="hlt">air</span>-to-refrigerant heat transfer and phase change. Overall optimization is carried out using a multi-objective genetic algorithm. The optimal designs found can exhibit 50 percent size reduction, 75 percent decrease in <span class="hlt">air</span> side pressure drop and doubled <span class="hlt">air</span> heat transfer coefficients compared to a high performance compact micro channel heat <span class="hlt">exchanger</span> with same capacity and flow rates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC51E0850G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC51E0850G"><span>The EUSTACE project: delivering global, daily information on <span class="hlt">surface</span> <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>Ghent, D.; Rayner, N. A.</p> <p>2017-12-01</p> <p>Day-to-day variations in <span class="hlt">surface</span> <span class="hlt">air</span> temperature affect society in many ways; however, daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements are not available everywhere. A global daily analysis cannot be achieved with measurements made in situ alone, so incorporation of satellite retrievals is needed. To achieve this, in the EUSTACE project (2015-2018, https://www.eustaceproject.eu) we have developed an understanding of the relationships between traditional (land and marine) <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements and retrievals of <span class="hlt">surface</span> skin temperature from satellite measurements, i.e. Land <span class="hlt">Surface</span> Temperature, Ice <span class="hlt">Surface</span> Temperature, Sea <span class="hlt">Surface</span> Temperature and Lake <span class="hlt">Surface</span> Water Temperature. Here we discuss the science needed to produce a fully-global daily analysis (or ensemble of analyses) of <span class="hlt">surface</span> <span class="hlt">air</span> temperature on the centennial scale, integrating different ground-based and satellite-borne data types. Information contained in the satellite retrievals is used to create globally-complete fields in the past, using statistical <span class="hlt">models</span> of how <span class="hlt">surface</span> <span class="hlt">air</span> temperature varies in a connected way from place to place. This includes developing new "Big Data" analysis methods as the data volumes involved are considerable. We will present recent progress along this road in the EUSTACE project, i.e.: • identifying inhomogeneities in daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurement series from weather stations and correcting for these over Europe; • estimating <span class="hlt">surface</span> <span class="hlt">air</span> temperature over all <span class="hlt">surfaces</span> of Earth from <span class="hlt">surface</span> skin temperature retrievals; • using new statistical techniques to provide information on higher spatial and temporal scales than currently available, making optimum use of information in data-rich eras. Information will also be given on how interested users can become involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JTST...25.1056H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JTST...25.1056H"><span>Fabrication of High-Temperature Heat <span class="hlt">Exchangers</span> by Plasma Spraying Exterior Skins on Nickel Foams</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hafeez, P.; Yugeswaran, S.; Chandra, S.; Mostaghimi, J.; Coyle, T. W.</p> <p>2016-06-01</p> <p>Thermal-sprayed heat <span class="hlt">exchangers</span> were tested at high temperatures (750 °C), and their performances were compared to the foam heat <span class="hlt">exchangers</span> made by brazing Inconel sheets to their <span class="hlt">surface</span>. Nickel foil was brazed to the exterior <span class="hlt">surface</span> of 10-mm-thick layers of 10 and 40 PPI nickel foam. A plasma torch was used to spray an Inconel coating on the <span class="hlt">surface</span> of the foil. A burner test rig was built to produce hot combustion gases that flowed over exposed face of the heat <span class="hlt">exchanger</span>. Cooling <span class="hlt">air</span> flowed through the foam heat <span class="hlt">exchanger</span> at rates of up to 200 SLPM. <span class="hlt">Surface</span> temperature and <span class="hlt">air</span> inlet/exit temperature were measured. Heat transfer to <span class="hlt">air</span> flowing through the foam was significantly higher for the thermally sprayed heat <span class="hlt">exchangers</span> than for the brazed heat <span class="hlt">exchangers</span>. On an average, thermally sprayed heat <span class="hlt">exchangers</span> show 36% higher heat transfer than conventionally brazed foam heat <span class="hlt">exchangers</span>. At low flow rates, the convective resistance is large (~4 × 10-2 m2 K/W), and the effect of thermal contact resistance is negligible. At higher flow rates, the convective resistance decreases (~2 × 10-3 m2 K/W), and the lower contact resistance of the thermally sprayed heat <span class="hlt">exchanger</span> provides better performance than the brazed heat <span class="hlt">exchangers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/834477','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/834477"><span>Chemical-Specific Representation of <span class="hlt">Air</span>-Soil <span class="hlt">Exchange</span> and Soil Penetration in Regional Multimedia <span class="hlt">Models</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>McKone, T.E.; Bennett, D.H.</p> <p>2002-08-01</p> <p>In multimedia mass-balance <span class="hlt">models</span>, the soil compartment is an important sink as well as a conduit for transfers to vegetation and shallow groundwater. Here a novel approach for constructing soil transport algorithms for multimedia fate <span class="hlt">models</span> is developed and evaluated. The resulting algorithms account for diffusion in gas and liquid components; advection in gas, liquid, or solid phases; and multiple transformation processes. They also provide an explicit quantification of the characteristic soil penetration depth. We construct a compartment <span class="hlt">model</span> using three and four soil layers to replicate with high reliability the flux and mass distribution obtained from the exact analyticalmore » solution describing the transient dispersion, advection, and transformation of chemicals in soil with fixed properties and boundary conditions. Unlike the analytical solution, which requires fixed boundary conditions, the soil compartment algorithms can be dynamically linked to other compartments (<span class="hlt">air</span>, vegetation, ground water, <span class="hlt">surface</span> water) in multimedia fate <span class="hlt">models</span>. We demonstrate and evaluate the performance of the algorithms in a <span class="hlt">model</span> with applications to benzene, benzo(a)pyrene, MTBE, TCDD, and tritium.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25686886','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25686886"><span>The effects of rice canopy on the <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of polycyclic aromatic hydrocarbons and organochlorine pesticides using paired passive <span class="hlt">air</span> samplers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Yan; Wang, Shaorui; Luo, Chunling; Li, Jun; Ming, Lili; Zhang, Gan; Li, Xiangdong</p> <p>2015-05-01</p> <p>The rice canopy in paddy fields can influence the <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of organic chemicals. We used paired passive <span class="hlt">air</span> samplers to assess the <span class="hlt">exchange</span> of polycyclic aromatic hydrocarbons (PAHs) and organochlorine pesticides (OCPs) in a paddy field, South China. Levels of OCPs and light PAHs were generally higher under the canopy than above it. We found that the rice canopy can physically obstruct the evaporation of most OCPs and light PAHs, and can also act as a barrier to the gaseous deposition of p,p'-DDT and heavy PAHs. Paddy fields can behave as a secondary source of OCPs and light PAHs. The homolog patterns of these two types of chemical varied slightly between the <span class="hlt">air</span> below and above the rice canopy, implying contributions of different sources. Paired passive <span class="hlt">air</span> samplers can be used effectively to assess the in situ <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of PAHs and OCPs in subtropical paddy fields. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3759556','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3759556"><span>Associations between PBDEs in Office <span class="hlt">Air</span>, Dust, and <span class="hlt">Surface</span> Wipes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Watkins, Deborah J.; McClean, Michael D.; Fraser, Alicia J.; Weinberg, Janice; Stapleton, Heather M.; Webster, Thomas F.</p> <p>2013-01-01</p> <p>Increased use of flame-retardants in office furniture may increase exposure to PBDEs in the office environment. However, partitioning of PBDEs within the office environment is not well understood. Our objectives were to examine relationships between concurrent measures of PBDEs in office <span class="hlt">air</span>, floor dust, and <span class="hlt">surface</span> wipes. We collected <span class="hlt">air</span>, dust, and <span class="hlt">surface</span> wipe samples from 31 offices in Boston, MA. Correlation and linear regression were used to evaluate associations between variables. Geometric mean (GM) concentrations of individual BDE congeners in <span class="hlt">air</span> and congener specific octanol-<span class="hlt">air</span> partition coefficients (Koa) were used to predict GM concentrations in dust and <span class="hlt">surface</span> wipes and compared to the measured concentrations. GM concentrations of PentaBDEs in office <span class="hlt">air</span>, dust, and <span class="hlt">surface</span> wipes were 472 pg/m3, 2411 ng/g, and 77 pg/cm2, respectively. BDE209 was detected in 100% of dust samples (GM=4202 ng/g), 93% of <span class="hlt">surface</span> wipes (GM=125 pg/cm2), and 39% of <span class="hlt">air</span> samples. PentaBDEs in dust and <span class="hlt">air</span> were moderately correlated with each other (r=0.60, p=0.0003), as well as with PentaBDEs in <span class="hlt">surface</span> wipes (r=0.51, p=0.003 for both dust and <span class="hlt">air</span>). BDE209 in dust was correlated with BDE209 in <span class="hlt">surface</span> wipes (r=0.69, p=0.007). Building (three categories) and PentaBDEs in dust were independent predictors of PentaBDEs in both <span class="hlt">air</span> and <span class="hlt">surface</span> wipes, together explaining 50% (p=0.0009) and 48% (p=0.001) of the variation respectively. Predicted and measured concentrations of individual BDE congeners were highly correlated in dust (r=0.98, p<0.0001) and <span class="hlt">surface</span> wipes (r=0.94, p=002). BDE209 provided an interesting test of this equilibrium partitioning <span class="hlt">model</span> as it is a low volatility compound. Associations between PentaBDEs in multiple sampling media suggest that collecting dust or <span class="hlt">surface</span> wipes may be a convenient method of characterizing exposure in the indoor environment. The volatility of individual congeners, as well as physical characteristics of the indoor environment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1339391-precise-determination-water-exchanges-mineral-surface','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1339391-precise-determination-water-exchanges-mineral-surface"><span>Precise determination of water <span class="hlt">exchanges</span> on a mineral <span class="hlt">surface</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Stack, Andrew G.; Borreguero, Jose M.; Prisk, Timothy R.; ...</p> <p>2016-10-03</p> <p>Solvent <span class="hlt">exchanges</span> on solid <span class="hlt">surfaces</span> and dissolved ions are a fundamental property important for understanding chemical reactions, but the rates of fast <span class="hlt">exchanges</span> are poorly constrained. In this paper, we probed the diffusional motions of water adsorbed onto nanoparticles of the mineral barite (BaSO 4) using quasi-elastic neutron scattering (QENS) and classical molecular dynamics (MD) to reveal the complex dynamics of water <span class="hlt">exchange</span> along mineral <span class="hlt">surfaces</span>. QENS data as a function of temperature and momentum transfer (Q) were fit using scattering functions derived from MD trajectories. The simulations reproduce the dynamics measured in the experiments at ambient temperatures, but asmore » temperature is lowered the simulations overestimate slower motions. Decomposition of the MD-computed QENS intensity into contributions from adsorbed and unbound water shows that the majority of the signal arises from adsorbed species, although the dynamics of unbound water cannot be dismissed. The mean residence times of water on each of the four <span class="hlt">surface</span> sites present on the barite {001} were calculated using MD: at room temperature the low barium site is 194 ps, whereas the high barium site contains two distributions of motions at 84 and 2.5 ps. These contrast to 13 ps residence time on both sulfate sites, with an additional <span class="hlt">surface</span> diffusion <span class="hlt">exchange</span> of 66 ps. <span class="hlt">Surface</span> <span class="hlt">exchanges</span> are similar to those of the aqueous ions calculated using the same force field: Ba aq 2+ is 208 ps and SO 4aq 2- is 5.8 ps. Finally, this work demonstrates how MD can be a reliable method to deconvolute solvent <span class="hlt">exchange</span> reactions when quantitatively validated by QENS measurements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ArTh...37..137A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ArTh...37..137A"><span>Performance analyses of helical coil heat <span class="hlt">exchangers</span>. The effect of external coil <span class="hlt">surface</span> modification on heat <span class="hlt">exchanger</span> effectiveness</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrzejczyk, Rafał; Muszyński, Tomasz</p> <p>2016-12-01</p> <p>The shell and coil heat <span class="hlt">exchangers</span> are commonly used in heating, ventilation, nuclear industry, process plant, heat recovery and <span class="hlt">air</span> conditioning systems. This type of recuperators benefits from simple construction, the low value of pressure drops and high heat transfer. In helical coil, centrifugal force is acting on the moving fluid due to the curvature of the tube results in the development. It has been long recognized that the heat transfer in the helical tube is much better than in the straight ones because of the occurrence of secondary flow in planes normal to the main flow inside the helical structure. Helical tubes show good performance in heat transfer enhancement, while the uniform curvature of spiral structure is inconvenient in pipe installation in heat <span class="hlt">exchangers</span>. Authors have presented their own construction of shell and tube heat <span class="hlt">exchanger</span> with intensified heat transfer. The purpose of this article is to assess the influence of the <span class="hlt">surface</span> modification over the performance coefficient and effectiveness. The experiments have been performed for the steady-state heat transfer. Experimental data points were gathered for both laminar and turbulent flow, both for co current- and countercurrent flow arrangement. To find optimal heat transfer intensification on the shell-side authors applied the number of transfer units analysis.</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/2017APS..DFDQ12005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDQ12005L"><span>Drop impact on a solid <span class="hlt">surface</span> at reduced <span class="hlt">air</span> pressure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Langley, Kenneth; Li, E. Q.; Tian, Y. S.; Hicks, P. D.; Thoroddsen, S. T.</p> <p>2017-11-01</p> <p>When a drop approaches a solid <span class="hlt">surface</span> at atmospheric pressure, the lubrication pressure within the <span class="hlt">air</span> forms a dimple in the bottom of the drop resulting in the entrainment of an <span class="hlt">air</span> disc upon impact. Reducing the ambient <span class="hlt">air</span> pressure below atmospheric has been shown to suppress splashing and the compression of the intervening <span class="hlt">air</span> could be significant on the <span class="hlt">air</span> disc formation; however, to date there have been no experimental studies showing how the entrainment of the <span class="hlt">air</span> disc is affected by reducing the ambient pressure. Using ultra-high-speed interferometry, at up to 5 Mfps, we investigate droplet impacts onto dry solid <span class="hlt">surfaces</span> in reduced ambient <span class="hlt">air</span> pressures with particular interest in what happens as rarified gas effects become important, i.e. when the thickness of the <span class="hlt">air</span> layer is of the same magnitude as the mean free path of the <span class="hlt">air</span> molecules. Experimental data will be presented showing novel phenomena and comparisons will be drawn with theoretical <span class="hlt">models</span> from the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24643387','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24643387"><span>Concentrations, atmospheric partitioning, and <span class="hlt">air</span>-water/soil <span class="hlt">surface</span> <span class="hlt">exchange</span> of polychlorinated dibenzo-p-dioxin and dibenzofuran along the upper reaches of the Haihe River basin, North China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nie, Zhiqiang; Die, Qingqi; Yang, Yufei; Tang, Zhenwu; Wang, Qi; Huang, Qifei</p> <p>2014-01-01</p> <p>Polychlorinated dibenzo-p-dioxin and dibenzofuran (PCDD/PCDF) were overall measured and compared in ambient <span class="hlt">air</span>, water, soils, and sediments along the upper reaches of the Haihe River of North China, so as to evaluate their concentrations, profiles, and to understand the processes of gas-particle partitioning and <span class="hlt">air</span>-water/soil <span class="hlt">exchange</span>. The following results were obtained: (1) The average concentrations (toxic equivalents, TEQs) of 2,3,7,8-PCDD/PCDF in <span class="hlt">air</span>, water, sediment, and soil samples were 4,855 fg/m(3), 9.5 pg/L, 99.2 pg/g dry weight (dw), and 56.4 pg/g (203 fg TEQ/m(3), 0.46 pg TEQ/L, 2.2 pg TEQ/g dw, and 1.3 pg TEQ/g, respectively), respectively. (2) Although OCDF, 1,2,3,4,6,7,8-HpCDF, OCDD, and 1,2,3,4,6,7,8-HpCDD were the dominant congeners among four environmental sinks, obvious discrepancies of these congener and homologue patterns of PCDD/PCDF were observed still. (3) Significant linear correlations for PCDD/PCDF were observed between the gas-particle partition coefficient (K p) and the subcooled liquid vapor pressure (P L (0)) and octanol-<span class="hlt">air</span> partition coefficient (K oa). (4) Fugacity fraction values of <span class="hlt">air</span>-water <span class="hlt">exchange</span> indicated that most of PCDD/PCDF homologues were dominated by net volatilization from water into <span class="hlt">air</span>. The low-chlorinated PCDD/PCDF (tetra- to hexa-) presented a strong net volatilization from the soil into <span class="hlt">air</span>, while high-chlorinated PCDD/PCDF (hepta- to octa-) were mainly close to equilibrium for <span class="hlt">air</span>-soil <span class="hlt">exchange</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e5129X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e5129X"><span>Thickened boundary layer theory for <span class="hlt">air</span> film drag reduction on a van body <span class="hlt">surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, Xiaopeng; Cao, Lifeng; Huang, Heng</p> <p>2018-05-01</p> <p>To elucidate drag reduction mechanism on a van body <span class="hlt">surface</span> under <span class="hlt">air</span> film condition, a thickened boundary layer theory was proposed and a frictional resistance calculation <span class="hlt">model</span> of the van body <span class="hlt">surface</span> was established. The frictional resistance on the van body <span class="hlt">surface</span> was calculated with different parameters of <span class="hlt">air</span> film thickness. In addition, the frictional resistance of the van body <span class="hlt">surface</span> under the <span class="hlt">air</span> film condition was analyzed by computational fluid dynamics (CFD) simulation and different <span class="hlt">air</span> film states that influenced the friction resistance on the van body <span class="hlt">surface</span> were discussed. As supported by the CFD simulation results, the thickened boundary layer theory may provide reference for practical application of <span class="hlt">air</span> film drag reduction on a van body <span class="hlt">surface</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20334101','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20334101"><span>Silica nano-particle super-hydrophobic <span class="hlt">surfaces</span>: the effects of <span class="hlt">surface</span> morphology and trapped <span class="hlt">air</span> pockets on hydrodynamic drainage forces.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chan, Derek Y C; Uddin, Md Hemayet; Cho, Kwun L; Liaw, Irving I; Lamb, Robert N; Stevens, Geoffrey W; Grieser, Franz; Dagastine, Raymond R</p> <p>2009-01-01</p> <p>We used atomic force microscopy to study dynamic forces between a rigid silica sphere (radius approximately 45 microm) and a silica nano-particle super-hydrophobic <span class="hlt">surface</span> (SNP-SHS) in aqueous electrolyte, in the presence and absence of surfactant. Characterization of the SNP-SHS <span class="hlt">surface</span> in <span class="hlt">air</span> showed a <span class="hlt">surface</span> roughness of up to two microns. When in contact with an aqueous phase, the SNP-SHS traps large, soft and stable <span class="hlt">air</span> pockets in the <span class="hlt">surface</span> interstices. The inherent roughness of the SNP-SHS together with the trapped <span class="hlt">air</span> pockets are responsible for the superior hydrophobic properties of SNP-SHS such as high equilibrium contact angle (> 140 degrees) of water sessile drops on these <span class="hlt">surfaces</span> and low hydrodynamic friction as observed in force measurements. We also observed that added surfactants adsorbed at the <span class="hlt">surface</span> of <span class="hlt">air</span> pockets magnified hydrodynamic interactions involving the SNP-SHS. The dynamic forces between the same silica sphere and a laterally smooth mica <span class="hlt">surface</span> showed that the fitted Navier slip lengths using the Reynolds lubrication <span class="hlt">model</span> were an order of magnitude larger than the length scale of the sphere <span class="hlt">surface</span> roughness. The <span class="hlt">surface</span> roughness and the lateral heterogeneity of the SNP-SHS hindered attempts to characterize the dynamic response using the Reynolds lubrication <span class="hlt">model</span> even when augmented with a Navier slip boundary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912697R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912697R"><span>The EUSTACE project: delivering global, daily information on <span class="hlt">surface</span> <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>Rayner, Nick</p> <p>2017-04-01</p> <p>Day-to-day variations in <span class="hlt">surface</span> <span class="hlt">air</span> temperature affect society in many ways; however, daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements are not available everywhere. A global daily analysis cannot be achieved with measurements made in situ alone, so incorporation of satellite retrievals is needed. To achieve this, in the EUSTACE project (2015-June 2018, https://www.eustaceproject.eu) we are developing an understanding of the relationships between traditional (land and marine) <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements and retrievals of <span class="hlt">surface</span> skin temperature from satellite measurements, i.e. Land <span class="hlt">Surface</span> Temperature, Ice <span class="hlt">Surface</span> Temperature, Sea <span class="hlt">Surface</span> Temperature and Lake <span class="hlt">Surface</span> Water Temperature. Here we discuss the science needed to produce a fully-global daily analysis (or ensemble of analyses) of <span class="hlt">surface</span> <span class="hlt">air</span> temperature on the centennial scale, integrating different ground-based and satellite-borne data types. Information contained in the satellite retrievals is used to create globally-complete fields in the past, using statistical <span class="hlt">models</span> of how <span class="hlt">surface</span> <span class="hlt">air</span> temperature varies in a connected way from place to place. As the data volumes involved are considerable, such work needs to include development of new "Big Data" analysis methods. We will present recent progress along this road in the EUSTACE project: 1. providing new, consistent, multi-component estimates of uncertainty in <span class="hlt">surface</span> skin temperature retrievals from satellites; 2. identifying inhomogeneities in daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurement series from weather stations and correcting for these over Europe; 3. estimating <span class="hlt">surface</span> <span class="hlt">air</span> temperature over all <span class="hlt">surfaces</span> of Earth from <span class="hlt">surface</span> skin temperature retrievals; 4. using new statistical techniques to provide information on higher spatial and temporal scales than currently available, making optimum use of information in data-rich eras. Information will also be given on how interested users can become involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC51D1201G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC51D1201G"><span>The EUSTACE project: delivering global, daily information on <span class="hlt">surface</span> <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>Ghent, D.; Rayner, N. A.</p> <p>2016-12-01</p> <p>Day-to-day variations in <span class="hlt">surface</span> <span class="hlt">air</span> temperature affect society in many ways; however, daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements are not available everywhere. A global daily analysis cannot be achieved with measurements made in situ alone, so incorporation of satellite retrievals is needed. To achieve this, in the EUSTACE project (2015-June 2018, https://www.eustaceproject.eu) we are developing an understanding of the relationships between traditional (land and marine) <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurements and retrievals of <span class="hlt">surface</span> skin temperature from satellite measurements, i.e. Land <span class="hlt">Surface</span> Temperature, Ice <span class="hlt">Surface</span> Temperature, Sea <span class="hlt">Surface</span> Temperature and Lake <span class="hlt">Surface</span> Water Temperature. Here we discuss the science needed to produce a fully-global daily analysis (or ensemble of analyses) of <span class="hlt">surface</span> <span class="hlt">air</span> temperature on the centennial scale, integrating different ground-based and satellite-borne data types. Information contained in the satellite retrievals is used to create globally-complete fields in the past, using statistical <span class="hlt">models</span> of how <span class="hlt">surface</span> <span class="hlt">air</span> temperature varies in a connected way from place to place. As the data volumes involved are considerable, such work needs to include development of new "Big Data" analysis methods. We will present recent progress along this road in the EUSTACE project, i.e.: • providing new, consistent, multi-component estimates of uncertainty in <span class="hlt">surface</span> skin temperature retrievals from satellites; • identifying inhomogeneities in daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature measurement series from weather stations and correcting for these over Europe; • estimating <span class="hlt">surface</span> <span class="hlt">air</span> temperature over all <span class="hlt">surfaces</span> of Earth from <span class="hlt">surface</span> skin temperature retrievals; • using new statistical techniques to provide information on higher spatial and temporal scales than currently available, making optimum use of information in data-rich eras. Information will also be given on how interested users can become involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1512690S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1512690S"><span>The <span class="hlt">Air</span>-Sea Interface and <span class="hlt">Surface</span> Stress under Tropical Cyclones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Soloviev, Alexander; Lukas, Roger; Donelan, Mark; Ginis, Isaac</p> <p>2013-04-01</p> <p> of the drag coefficient wind speed dependence around 65 m/s. This minimum may contribute to the rapid intensification of storms to major tropical cyclones. The subsequent slow increase of the drag coefficient with wind above 65 m/s serves as an obstacle for further intensification of tropical cyclones. Such dependence may explain the observed bi-modal distribution of tropical cyclone intensity. Implementation of the new parameterization into operational <span class="hlt">models</span> is expected to improve predictions of tropical cyclone intensity and the associated wave field. References: Donelan, M. A., B. K. Haus, N. Reul, W. Plant, M. Stiassnie, H. Graber, O. Brown, and E. Saltzman, 2004: On the limiting aerodynamic roughness of the ocean in very strong winds, Farrell, B.F, and P.J. Ioannou, 2008: The stochastic parametric mechanism for growth of wind-driven <span class="hlt">surface</span> water waves. Journal of Physical Oceanography 38, 862-879. Kelly, R.E., 1965: The stability of an unsteady Kelvin-Helmholtz flow. J. Fluid Mech. 22, 547-560. Koga, M., 1981: Direct production of droplets from breaking wind-waves-Its observation by a multi-colored overlapping exposure technique, Tellus 33, 552-563. Miles, J.W., 1959: On the generation of <span class="hlt">surface</span> waves by shear flows, part 3. J. Fluid. Mech. 6, 583-598. Soloviev, A.V. and R. Lukas, 2010: Effects of bubbles and sea spray on <span class="hlt">air</span>-sea <span class="hlt">exchanges</span> in hurricane conditions. Boundary-Layer Meteorology 136, 365-376. Soloviev, A., A. Fujimura, and S. Matt, 2012: <span class="hlt">Air</span>-sea interface in hurricane conditions. J. Geophys. Res. 117, C00J34.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890043107&hterms=surfactants&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsurfactants','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890043107&hterms=surfactants&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsurfactants"><span>Flow visualization study of grooved <span class="hlt">surface/surfactant/air</span> sheet interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reed, Jason C.; Weinstein, Leonard M.</p> <p>1989-01-01</p> <p>The effects of groove geometry, surfactants, and airflow rate have been ascertained by a flow-visualization study of grooved-<span class="hlt">surface</span> <span class="hlt">models</span> which addresses the possible conditions for skin friction-reduction in marine vehicles. It is found that the grooved <span class="hlt">surface</span> geometry holds the injected bubble stream near the wall and, in some cases, results in a 'tube' of <span class="hlt">air</span> which remains attached to the wall. It is noted that groove dimension and the use of surfactants can substantially affect the stability of this <span class="hlt">air</span> tube; deeper grooves, surfactants with high contact angles, and angled <span class="hlt">air</span> injection, are all found to increase the stability of the attached <span class="hlt">air</span> tube, while convected disturbances and high shear increase interfacial instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034286','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034286"><span>First-order <span class="hlt">exchange</span> coefficient coupling for simulating <span class="hlt">surface</span> water-groundwater interactions: Parameter sensitivity and consistency with a physics-based approach</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Ebel, B.A.; Mirus, B.B.; Heppner, C.S.; VanderKwaak, J.E.; Loague, K.</p> <p>2009-01-01</p> <p>Distributed hydrologic <span class="hlt">models</span> capable of simulating fully-coupled <span class="hlt">surface</span> water and groundwater flow are increasingly used to examine problems in the hydrologic sciences. Several techniques are currently available to couple the <span class="hlt">surface</span> and subsurface; the two most frequently employed approaches are first-order <span class="hlt">exchange</span> coefficients (a.k.a., the <span class="hlt">surface</span> conductance method) and enforced continuity of pressure and flux at the <span class="hlt">surface</span>-subsurface boundary condition. The effort reported here examines the parameter sensitivity of simulated hydrologic response for the first-order <span class="hlt">exchange</span> coefficients at a well-characterized field site using the fully coupled Integrated Hydrology <span class="hlt">Model</span> (InHM). This investigation demonstrates that the first-order <span class="hlt">exchange</span> coefficients can be selected such that the simulated hydrologic response is insensitive to the parameter choice, while simulation time is considerably reduced. Alternatively, the ability to choose a first-order <span class="hlt">exchange</span> coefficient that intentionally decouples the <span class="hlt">surface</span> and subsurface facilitates concept-development simulations to examine real-world situations where the <span class="hlt">surface</span>-subsurface <span class="hlt">exchange</span> is impaired. While the parameters comprising the first-order <span class="hlt">exchange</span> coefficient cannot be directly estimated or measured, the insensitivity of the simulated flow system to these parameters (when chosen appropriately) combined with the ability to mimic actual physical processes suggests that the first-order <span class="hlt">exchange</span> coefficient approach can be consistent with a physics-based framework. Copyright ?? 2009 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ACP....11.2127L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ACP....11.2127L"><span>Evaluation of urban <span class="hlt">surface</span> parameterizations in the WRF <span class="hlt">model</span> using measurements during the Texas <span class="hlt">Air</span> Quality Study 2006 field campaign</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, S.-H.; Kim, S.-W.; Angevine, W. M.; Bianco, L.; McKeen, S. A.; Senff, C. J.; Trainer, M.; Tucker, S. C.; Zamora, R. J.</p> <p>2011-03-01</p> <p>The performance of different urban <span class="hlt">surface</span> parameterizations in the WRF (Weather Research and Forecasting) in simulating urban boundary layer (UBL) was investigated using extensive measurements during the Texas <span class="hlt">Air</span> Quality Study 2006 field campaign. The extensive field measurements collected on <span class="hlt">surface</span> (meteorological, wind profiler, energy balance flux) sites, a research aircraft, and a research vessel characterized 3-dimensional atmospheric boundary layer structures over the Houston-Galveston Bay area, providing a unique opportunity for the evaluation of the physical parameterizations. The <span class="hlt">model</span> simulations were performed over the Houston metropolitan area for a summertime period (12-17 August) using a bulk urban parameterization in the Noah land <span class="hlt">surface</span> <span class="hlt">model</span> (original LSM), a modified LSM, and a single-layer urban canopy <span class="hlt">model</span> (UCM). The UCM simulation compared quite well with the observations over the Houston urban areas, reducing the systematic <span class="hlt">model</span> biases in the original LSM simulation by 1-2 °C in near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature and by 200-400 m in UBL height, on average. A more realistic turbulent (sensible and latent heat) energy partitioning contributed to the improvements in the UCM simulation. The original LSM significantly overestimated the sensible heat flux (~200 W m-2) over the urban areas, resulting in warmer and higher UBL. The modified LSM slightly reduced warm and high biases in near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature (0.5-1 °C) and UBL height (~100 m) as a result of the effects of urban vegetation. The relatively strong thermal contrast between the Houston area and the water bodies (Galveston Bay and the Gulf of Mexico) in the LSM simulations enhanced the sea/bay breezes, but the <span class="hlt">model</span> performance in predicting local wind fields was similar among the simulations in terms of statistical evaluations. These results suggest that a proper <span class="hlt">surface</span> representation (e.g. urban vegetation, <span class="hlt">surface</span> morphology) and explicit parameterizations of urban physical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JASTP..71..841K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JASTP..71..841K"><span>ARIMA representation for daily solar irradiance and <span class="hlt">surface</span> <span class="hlt">air</span> temperature time series</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kärner, Olavi</p> <p>2009-06-01</p> <p>Autoregressive integrated moving average (ARIMA) <span class="hlt">models</span> are used to compare long-range temporal variability of the total solar irradiance (TSI) at the top of the atmosphere (TOA) and <span class="hlt">surface</span> <span class="hlt">air</span> temperature series. The comparison shows that one and the same type of the <span class="hlt">model</span> is applicable to represent the TSI and <span class="hlt">air</span> temperature series. In terms of the <span class="hlt">model</span> type <span class="hlt">surface</span> <span class="hlt">air</span> temperature imitates closely that for the TSI. This may mean that currently no other forcing to the climate system is capable to change the random walk type variability established by the varying activity of the rotating Sun. The result should inspire more detailed examination of the dependence of various climate series on short-range fluctuations of TSI.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....9097L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....9097L"><span><span class="hlt">Modelling</span> of <span class="hlt">surface</span> fluxes and Urban Boundary Layer over an old mediterannean city core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lemonsu, A.; Masson, V.; Grimmond, Cs. B.</p> <p>2003-04-01</p> <p>In the frameworks of the UBL(Urban Boundary Layer)-ESCOMPTE campaign, the Town Energy Balance (TEB) <span class="hlt">model</span> was run in off-line mode for Marseille. TEB's performance is evaluated with observations of <span class="hlt">surface</span> temperatures and <span class="hlt">surface</span> energy balance fluxes collected during the campaign. Parameterization improvements allow to better represent the energy <span class="hlt">exchanges</span> between the <span class="hlt">air</span> inside the canyon and the atmosphere above the roof level. Then, high resolution Méso-NH simulations are done to study the 3-D structure and the evolution of the Urban Boundary Layer (UBL) over Marseille. Will will give a special attention to the impact of the seabord effects (sea-breeze circulation) on the UBL.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2889562','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2889562"><span>Universal <span class="hlt">model</span> for water costs of gas <span class="hlt">exchange</span> by animals and plants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Woods, H. Arthur; Smith, Jennifer N.</p> <p>2010-01-01</p> <p>For terrestrial animals and plants, a fundamental cost of living is water vapor lost to the atmosphere during <span class="hlt">exchange</span> of metabolic gases. Here, by bringing together previously developed <span class="hlt">models</span> for specific taxa, we integrate properties common to all terrestrial gas <span class="hlt">exchangers</span> into a universal <span class="hlt">model</span> of water loss. The <span class="hlt">model</span> predicts that water loss scales to gas <span class="hlt">exchange</span> with an exponent of 1 and that the amount of water lost per unit of gas <span class="hlt">exchanged</span> depends on several factors: the <span class="hlt">surface</span> temperature of the respiratory system near the outside of the organism, the gas consumed (oxygen or carbon dioxide), the steepness of the gradients for gas and vapor, and the transport mode (convective or diffusive). <span class="hlt">Model</span> predictions were largely confirmed by data on 202 species in five taxa—insects, birds, bird eggs, mammals, and plants—spanning nine orders of magnitude in rate of gas <span class="hlt">exchange</span>. Discrepancies between <span class="hlt">model</span> predictions and data seemed to arise from biologically interesting violations of <span class="hlt">model</span> assumptions, which emphasizes how poorly we understand gas <span class="hlt">exchange</span> in some taxa. The universal <span class="hlt">model</span> provides a unified conceptual framework for analyzing <span class="hlt">exchange</span>-associated water losses across taxa with radically different metabolic and <span class="hlt">exchange</span> systems. PMID:20404161</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20404161','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20404161"><span>Universal <span class="hlt">model</span> for water costs of gas <span class="hlt">exchange</span> by animals and plants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Woods, H Arthur; Smith, Jennifer N</p> <p>2010-05-04</p> <p>For terrestrial animals and plants, a fundamental cost of living is water vapor lost to the atmosphere during <span class="hlt">exchange</span> of metabolic gases. Here, by bringing together previously developed <span class="hlt">models</span> for specific taxa, we integrate properties common to all terrestrial gas <span class="hlt">exchangers</span> into a universal <span class="hlt">model</span> of water loss. The <span class="hlt">model</span> predicts that water loss scales to gas <span class="hlt">exchange</span> with an exponent of 1 and that the amount of water lost per unit of gas <span class="hlt">exchanged</span> depends on several factors: the <span class="hlt">surface</span> temperature of the respiratory system near the outside of the organism, the gas consumed (oxygen or carbon dioxide), the steepness of the gradients for gas and vapor, and the transport mode (convective or diffusive). <span class="hlt">Model</span> predictions were largely confirmed by data on 202 species in five taxa--insects, birds, bird eggs, mammals, and plants--spanning nine orders of magnitude in rate of gas <span class="hlt">exchange</span>. Discrepancies between <span class="hlt">model</span> predictions and data seemed to arise from biologically interesting violations of <span class="hlt">model</span> assumptions, which emphasizes how poorly we understand gas <span class="hlt">exchange</span> in some taxa. The universal <span class="hlt">model</span> provides a unified conceptual framework for analyzing <span class="hlt">exchange</span>-associated water losses across taxa with radically different metabolic and <span class="hlt">exchange</span> systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H22D..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H22D..06C"><span>Evaluating Predictive Uncertainty of Hyporheic <span class="hlt">Exchange</span> <span class="hlt">Modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chow, R.; Bennett, J.; Dugge, J.; Wöhling, T.; Nowak, W.</p> <p>2017-12-01</p> <p>Hyporheic <span class="hlt">exchange</span> is the interaction of water between rivers and groundwater, and is difficult to predict. One of the largest contributions to predictive uncertainty for hyporheic fluxes have been attributed to the representation of heterogeneous subsurface properties. This research aims to evaluate which aspect of the subsurface representation - the spatial distribution of hydrofacies or the <span class="hlt">model</span> for local-scale (within-facies) heterogeneity - most influences the predictive uncertainty. Also, we seek to identify data types that help reduce this uncertainty best. For this investigation, we conduct a <span class="hlt">modelling</span> study of the Steinlach River meander, in Southwest Germany. The Steinlach River meander is an experimental site established in 2010 to monitor hyporheic <span class="hlt">exchange</span> at the meander scale. We use HydroGeoSphere, a fully integrated <span class="hlt">surface</span> water-groundwater <span class="hlt">model</span>, to <span class="hlt">model</span> hyporheic <span class="hlt">exchange</span> and to assess the predictive uncertainty of hyporheic <span class="hlt">exchange</span> transit times (HETT). A highly parameterized complex <span class="hlt">model</span> is built and treated as `virtual reality', which is in turn <span class="hlt">modelled</span> with simpler subsurface parameterization schemes (Figure). Then, we conduct Monte-Carlo simulations with these <span class="hlt">models</span> to estimate the predictive uncertainty. Results indicate that: Uncertainty in HETT is relatively small for early times and increases with transit times. Uncertainty from local-scale heterogeneity is negligible compared to uncertainty in the hydrofacies distribution. Introducing more data to a poor <span class="hlt">model</span> structure may reduce predictive variance, but does not reduce predictive bias. Hydraulic head observations alone cannot constrain the uncertainty of HETT, however an estimate of hyporheic <span class="hlt">exchange</span> flux proves to be more effective at reducing this uncertainty. Figure: Approach for evaluating predictive <span class="hlt">model</span> uncertainty. A conceptual <span class="hlt">model</span> is first developed from the field investigations. A complex <span class="hlt">model</span> (`virtual reality') is then developed based on that conceptual <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol5/pdf/CFR-2013-title29-vol5-sec1910-425.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol5/pdf/CFR-2013-title29-vol5-sec1910-425.pdf"><span>29 CFR 1910.425 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 29 Labor 5 2013-07-01 2013-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1910.425 Section 1910.425... Procedures § 1910.425 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. (a) General. Employers engaged in <span class="hlt">surface</span>-supplied <span class="hlt">air</span>...-supplied <span class="hlt">air</span> diving shall not be conducted at depths deeper than 190 fsw, except that dives with bottom...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol5/pdf/CFR-2012-title29-vol5-sec1910-425.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol5/pdf/CFR-2012-title29-vol5-sec1910-425.pdf"><span>29 CFR 1910.425 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 29 Labor 5 2012-07-01 2012-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1910.425 Section 1910.425... Procedures § 1910.425 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. (a) General. Employers engaged in <span class="hlt">surface</span>-supplied <span class="hlt">air</span>...-supplied <span class="hlt">air</span> diving shall not be conducted at depths deeper than 190 fsw, except that dives with bottom...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol5/pdf/CFR-2010-title29-vol5-sec1910-425.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol5/pdf/CFR-2010-title29-vol5-sec1910-425.pdf"><span>29 CFR 1910.425 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 29 Labor 5 2010-07-01 2010-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1910.425 Section 1910.425... Procedures § 1910.425 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. (a) General. Employers engaged in <span class="hlt">surface</span>-supplied <span class="hlt">air</span>...-supplied <span class="hlt">air</span> diving shall not be conducted at depths deeper than 190 fsw, except that dives with bottom...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol5/pdf/CFR-2011-title29-vol5-sec1910-425.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol5/pdf/CFR-2011-title29-vol5-sec1910-425.pdf"><span>29 CFR 1910.425 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 29 Labor 5 2011-07-01 2011-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1910.425 Section 1910.425... Procedures § 1910.425 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. (a) General. Employers engaged in <span class="hlt">surface</span>-supplied <span class="hlt">air</span>...-supplied <span class="hlt">air</span> diving shall not be conducted at depths deeper than 190 fsw, except that dives with bottom...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70027017','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70027017"><span>Radon (222Rn) in ground water of fractured rocks: A diffusion/ion <span class="hlt">exchange</span> <span class="hlt">model</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>Wood, W.W.; Kraemer, T.F.; Shapiro, A.</p> <p>2004-01-01</p> <p>Ground waters from fractured igneous and high-grade sialic metamorphic rocks frequently have elevated activity of dissolved radon (222Rn). A chemically based <span class="hlt">model</span> is proposed whereby radium (226Ra) from the decay of uranium (238U) diffuses through the primary porosity of the rock to the water-transmitting fracture where it is sorbed on weathering products. Sorption of 226Ra on the fracture <span class="hlt">surface</span> maintains an activity gradient in the rock matrix, ensuring a continuous supply of 226Ra to fracture <span class="hlt">surfaces</span>. As a result of the relatively long half-life of 226Ra (1601 years), significant activity can accumulate on fracture <span class="hlt">surfaces</span>. The proximity of this sorbed 226Ra to the active ground water flow system allows its decay progeny 222Rn to enter directly into the water. Laboratory analyses of primary porosity and diffusion coefficients of the rock matrix, radon emanation, and ion <span class="hlt">exchange</span> at fracture <span class="hlt">surfaces</span> are consistent with the requirements of a diffusion/ion- <span class="hlt">exchange</span> <span class="hlt">model</span>. A dipole-brine injection/withdrawal experiment conducted between bedrock boreholes in the high-grade metamorphic and granite rocks at the Hubbard Brook Experimental Forest, Grafton County, New Hampshire, United States (42??56???N, 71??43???W) shows a large activity of 226Ra <span class="hlt">exchanged</span> from fracture <span class="hlt">surfaces</span> by a magnesium brine. The 226Ra activity removed by the <span class="hlt">exchange</span> process is 34 times greater than that of 238U activity. These observations are consistent with the diffusion/ion-<span class="hlt">exchange</span> <span class="hlt">model</span>. Elutriate isotopic ratios of 223Ra/226Ra and 238U/226Ra are also consistent with the proposed chemically based diffusion/ion-<span class="hlt">exchange</span> <span class="hlt">model</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_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.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec197-432.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec197-432.pdf"><span>46 CFR 197.432 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 7 2012-10-01 2012-10-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 197.432 Section 197.432...-supplied <span class="hlt">air</span> diving. The diving supervisor shall insure that— (a) <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving is conducted... space; and (f) The <span class="hlt">surface</span>-supplied <span class="hlt">air</span> diver has the equipment required by § 197.346 (b) or (d). ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec197-432.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec197-432.pdf"><span>46 CFR 197.432 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 7 2013-10-01 2013-10-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 197.432 Section 197.432...-supplied <span class="hlt">air</span> diving. The diving supervisor shall insure that— (a) <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving is conducted... space; and (f) The <span class="hlt">surface</span>-supplied <span class="hlt">air</span> diver has the equipment required by § 197.346 (b) or (d). ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec197-432.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec197-432.pdf"><span>46 CFR 197.432 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 197.432 Section 197.432...-supplied <span class="hlt">air</span> diving. The diving supervisor shall insure that— (a) <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving is conducted... space; and (f) The <span class="hlt">surface</span>-supplied <span class="hlt">air</span> diver has the equipment required by § 197.346 (b) or (d). ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec197-432.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec197-432.pdf"><span>46 CFR 197.432 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 7 2011-10-01 2011-10-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 197.432 Section 197.432...-supplied <span class="hlt">air</span> diving. The diving supervisor shall insure that— (a) <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving is conducted... space; and (f) The <span class="hlt">surface</span>-supplied <span class="hlt">air</span> diver has the equipment required by § 197.346 (b) or (d). ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=335749','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=335749"><span><span class="hlt">Modeling</span> green infrastructure land use changes on future <span class="hlt">air</span> ...</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>Green infrastructure can be a cost-effective approach for reducing stormwater runoff and improving water quality as a result, but it could also bring co-benefits for <span class="hlt">air</span> quality: less impervious <span class="hlt">surfaces</span> and more vegetation can decrease the urban heat island effect, and also result in more removal of <span class="hlt">air</span> pollutants via dry deposition with increased vegetative <span class="hlt">surfaces</span>. Cooler <span class="hlt">surface</span> temperatures can also decrease ozone formation through the increases of NOx titration; however, cooler <span class="hlt">surface</span> temperatures also lower the height of the boundary layer resulting in more concentrated pollutants within the same volume of <span class="hlt">air</span>, especially for primary emitted pollutants (e.g. NOx, CO, primary particulate matter). To better understand how green infrastructure impacts <span class="hlt">air</span> quality, the interactions between all of these processes must be considered collectively. In this study, we use a comprehensive coupled meteorology-<span class="hlt">air</span> quality <span class="hlt">model</span> (WRF-CMAQ) to simulate the influence of planned land use changes that include green infrastructure in Kansas City (KC) on regional meteorology and <span class="hlt">air</span> quality. Current and future land use data was provided by the Mid-America Regional Council for 2012 and 2040 (projected land use due to population growth, city planning and green infrastructure implementation). These land use datasets were incorporated into the WRF-CMAQ <span class="hlt">modeling</span> system allowing the <span class="hlt">modeling</span> system to propagate the changes in vegetation and impervious <span class="hlt">surface</span> coverage on meteoro</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=255244&keyword=temperature+AND+variability&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=255244&keyword=temperature+AND+variability&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>Identifying Housing and Meteorological Conditions Influencing Residential <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rates in the DEARS and RIOPA Studies: Development of Distributions for Human Exposure <span class="hlt">Modeling</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>Appropriate prediction of residential <span class="hlt">air</span> <span class="hlt">exchange</span> rate (AER) is important for estimating human exposures in the residential microenvironment, as AER drives the infiltration of outdoor-generated <span class="hlt">air</span> pollutants indoors. AER differences among homes may result from a number of fact...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992IJHMT..35.2683L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992IJHMT..35.2683L"><span>Steady state <span class="hlt">model</span> for the thermal regimes of shells of airships and hot <span class="hlt">air</span> balloons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luchev, Oleg A.</p> <p>1992-10-01</p> <p>A steady state <span class="hlt">model</span> of the temperature regime of airships and hot <span class="hlt">air</span> balloons shells is developed. The <span class="hlt">model</span> includes three governing equations: the equation of the temperature field of airships or balloons shell, the integral equation for the radiative fluxes on the internal <span class="hlt">surface</span> of the shell, and the integral equation for the natural convective heat <span class="hlt">exchange</span> between the shell and the internal gas. In the <span class="hlt">model</span> the following radiative fluxes on the shell external <span class="hlt">surface</span> are considered: the direct and the earth reflected solar radiation, the diffuse solar radiation, the infrared radiation of the earth <span class="hlt">surface</span> and that of the atmosphere. For the calculations of the infrared external radiation the <span class="hlt">model</span> of the plane layer of the atmosphere is used. The convective heat transfer on the external <span class="hlt">surface</span> of the shell is considered for the cases of the forced and the natural convection. To solve the mentioned set of the equations the numerical iterative procedure is developed. The <span class="hlt">model</span> and the numerical procedure are used for the simulation study of the temperature fields of an airship shell under the forced and the natural convective heat transfer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.745c2141B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.745c2141B"><span>A Numerical Analysis on a Compact Heat <span class="hlt">Exchanger</span> in Aluminum Foam</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buonomo, B.; Ercole, D.; Manca, O.; Nardini, S.</p> <p>2016-09-01</p> <p>A numerical investigation on a compact heat <span class="hlt">exchanger</span> in aluminum foam is carried out. The governing equations in two-dimensional steady state regime are written in local thermal non-equilibrium (LTNE). The geometrical domain under investigation is made up of a plate in aluminum foam with inside a single array of five circular tubes. The presence of the open-celled metal foam is <span class="hlt">modeled</span> as a porous media by means of the Darcy-Forchheimer law. The foam has a porosity of 0.93 with 20 pores per inch and the LTNE assumption is used to simulate the heat transfer between metal foam and <span class="hlt">air</span>. The compact heat <span class="hlt">exchanger</span> at different <span class="hlt">air</span> flow rates is studied with an assigned <span class="hlt">surface</span> tube temperature. The results in terms of local heat transfer coefficient and Nusselt number on the external <span class="hlt">surface</span> of the tubes are given. Moreover, local <span class="hlt">air</span> temperature and velocity profiles in the smaller cross section, between two consecutive tubes, as a function of Reynolds number are showed. The performance evaluation criteria (PEC) is assessed in order to evaluate the effectiveness of the metal foam.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1170410','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1170410"><span>Solid oxide fuel cell power plant having a fixed contact oxidation catalyzed section of a multi-section cathode <span class="hlt">air</span> heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Saito, Kazuo; Lin, Yao</p> <p>2015-02-17</p> <p>The multi-section cathode <span class="hlt">air</span> heat <span class="hlt">exchanger</span> (102) includes at least a first heat <span class="hlt">exchanger</span> section (104), and a fixed contact oxidation catalyzed section (126) secured adjacent each other in a stack association. Cool cathode inlet <span class="hlt">air</span> flows through cool <span class="hlt">air</span> channels (110) of the at least first (104) and oxidation catalyzed sections (126). Hot anode exhaust flows through hot <span class="hlt">air</span> channels (124) of the oxidation catalyzed section (126) and is combusted therein. The combusted anode exhaust then flows through hot <span class="hlt">air</span> channels (112) of the first section (104) of the cathode <span class="hlt">air</span> heat <span class="hlt">exchanger</span> (102). The cool and hot <span class="hlt">air</span> channels (110, 112) are secured in direct heat <span class="hlt">exchange</span> relationship with each other so that temperatures of the heat <span class="hlt">exchanger</span> (102) do not exceed 800.degree. C. to minimize requirements for using expensive, high-temperature alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27378004','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27378004"><span>A multiscale <span class="hlt">model</span> of placental oxygen <span class="hlt">exchange</span>: The effect of villous tree structure on <span class="hlt">exchange</span> efficiency.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lin, Mabelle; Mauroy, Benjamin; James, Joanna L; Tawhai, Merryn H; Clark, Alys R</p> <p>2016-11-07</p> <p>The placenta is critical to fetal health during pregnancy as it supplies oxygen and nutrients to maintain life. It has a complex structure, and alterations to this structure across spatial scales are associated with several pregnancy complications, including intrauterine growth restriction (IUGR). The relationship between placental structure and its efficiency as an oxygen <span class="hlt">exchanger</span> is not well understood in normal or pathological pregnancies. Here we present a computational framework that predicts oxygen transport in the placenta which accounts for blood and oxygen transport in the space around a placental functional unit (the villous tree). The <span class="hlt">model</span> includes the well-defined branching structure of the largest villous tree branches, as well as a smoothed representation of the small terminal villi that comprise the placenta's gas <span class="hlt">exchange</span> interfaces. The <span class="hlt">model</span> demonstrates that oxygen <span class="hlt">exchange</span> is sensitive to villous tree geometry, including the villous branch length and volume, which are seen to change in IUGR. This is because, to be an efficient <span class="hlt">exchanger</span>, the architecture of the villous tree must provide a balance between maximising the <span class="hlt">surface</span> area available for <span class="hlt">exchange</span>, and the opposing condition of allowing sufficient maternal blood flow to penetrate into the space surrounding the tree. The <span class="hlt">model</span> also predicts an optimum oxygen <span class="hlt">exchange</span> when the branch angle is 24 °, as villous branches and TBs are spread out sufficiently to channel maternal blood flow deep into the placental tissue for oxygen <span class="hlt">exchange</span> without being shunted directly into the DVs. Without concurrent change in the branch length and angles, the <span class="hlt">model</span> predicts that the number of branching generations has a small influence on oxygen <span class="hlt">exchange</span>. The <span class="hlt">modelling</span> framework is presented in 2D for simplicity but is extendible to 3D or to incorporate the high-resolution imaging data that is currently evolving to better quantify placental structure. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19766288','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19766288"><span><span class="hlt">Modelling</span> bioaccumulation of semi-volatile organic compounds (SOCs) from <span class="hlt">air</span> in plants based on allometric principles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Steyaert, Nils L L; Hauck, Mara; Van Hulle, Stijn W H; Hendriks, A Jan</p> <p>2009-10-01</p> <p>A <span class="hlt">model</span> was developed for gaseous plant-<span class="hlt">air</span> <span class="hlt">exchange</span> of semi-volatile organic compounds. Based on previous soil-plant <span class="hlt">modelling</span>, uptake and elimination kinetics were scaled as a function of plant mass and octanol-<span class="hlt">air</span> partition ratios. <span class="hlt">Exchange</span> of chemicals was assumed to be limited by resistances encountered during diffusion through a laminar boundary layer of <span class="hlt">air</span> and permeation through the cuticle of the leaf. The uptake rate constant increased and the elimination rate constant decreased with the octanol-<span class="hlt">air</span> partition ratio both apparently levelling off at high values. Differences in kinetics between species could be explained by their masses. Validation on independent data showed that bio-concentration factors of PCBs, chlorobenzenes and other chemicals were predicted well by the <span class="hlt">model</span>. For pesticides, polycyclic aromatic hydrocarbons and dioxins deviations occurred.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70164484','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70164484"><span>Gas <span class="hlt">exchange</span> rates across the sediment-water and <span class="hlt">air</span>-water interfaces in south San Francisco Bay</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hartman, Blayne; Hammond, Douglas E.</p> <p>1984-01-01</p> <p>Radon 222 concentrations in the water and sedimentary columns and radon <span class="hlt">exchange</span> rates across the sediment-water and <span class="hlt">air</span>-water interfaces have been measured in a section of south San Francisco Bay. Two independent methods have been used to determine sediment-water <span class="hlt">exchange</span> rates, and the annual averages of these methods agree within the uncertainty of the determinations, about 20%. The annual average of benthic fluxes from shoal areas is nearly a factor of 2 greater than fluxes from the channel areas. Fluxes from the shoal and channel areas exceed those expected from simple molecular diffusion by factors of 4 and 2, respectively, apparently due to macrofaunal irrigation. Values of the gas transfer coefficient for radon <span class="hlt">exchange</span> across the <span class="hlt">air</span>-water interface were determined by constructing a radon mass balance for the water column and by direct measurement using floating chambers. The chamber method appears to yield results which are too high. Transfer coefficients computed using the mass balance method range from 0.4 m/day to 1.8 m/day, with a 6-year average of 1.0 m/day. Gas <span class="hlt">exchange</span> is linearly dependent upon wind speed over a wind speed range of 3.2–6.4 m/s, but shows no dependence upon current velocity. Gas transfer coefficients predicted from an empirical relationship between gas <span class="hlt">exchange</span> rates and wind speed observed in lakes and the oceans are within 30% of the coefficients determined from the radon mass balance and are considerably more accurate than coefficients predicted from theoretical gas <span class="hlt">exchange</span> <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020058228','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020058228"><span>Laser Induced Aluminum <span class="hlt">Surface</span> Breakdown <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chen, Yen-Sen; Liu, Jiwen; Zhang, Sijun; Wang, Ten-See (Technical Monitor)</p> <p>2002-01-01</p> <p>Laser powered propulsion systems involve complex fluid dynamics, thermodynamics and radiative transfer processes. Based on an unstructured grid, pressure-based computational aerothermodynamics; platform, several sub-<span class="hlt">models</span> describing such underlying physics as laser ray tracing and focusing, thermal non-equilibrium, plasma radiation and <span class="hlt">air</span> spark ignition have been developed. This proposed work shall extend the numerical platform and existing sub-<span class="hlt">models</span> to include the aluminum wall <span class="hlt">surface</span> Inverse Bremsstrahlung (IB) effect from which <span class="hlt">surface</span> ablation and free-electron generation can be initiated without relying on the <span class="hlt">air</span> spark ignition sub-<span class="hlt">model</span>. The following tasks will be performed to accomplish the research objectives.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1247947','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1247947"><span>Kinetics of oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> on epitaxial Ruddlesden–Popper phases and correlations to first-principles descriptors</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, Yueh -Lin; Wang, Xiao Renshaw; Lee, Ho Nyung</p> <p>2015-12-17</p> <p>Through alignment of theoretical <span class="hlt">modeling</span> with experimental measurements of oxygen <span class="hlt">surface-exchange</span> kinetics on (001)-oriented La 2–xSr xMO 4+δ (M = Co, Ni, Cu) thin films, we demonstrate here the capability of the theoretical bulk O 2p-band centers to correlate with oxygen <span class="hlt">surface-exchange</span> kinetics of the Ruddlesden–Popper oxide (RP 214) (001)-oriented thin films. In addition, we demonstrate that the bulk O 2p-band centers can also correlate with the experimental activation energies for bulk oxygen transport and oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> of both the RP 214 and the perovskite polycrystalline materials reported in the literature, indicating the effectiveness of the bulk O 2p-bandmore » centers in describing the associated energetics and kinetics. Here, we propose that the opposite slopes of the bulk O 2p-band center correlations between the RP 214 and the perovskite materials are due to the intrinsic mechanistic differences of their oxygen <span class="hlt">surface-exchange</span> kinetics bulk anionic transport.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPS...326..417R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPS...326..417R"><span>Proton <span class="hlt">exchange</span> membrane fuel cell <span class="hlt">model</span> for aging predictions: Simulated equivalent active <span class="hlt">surface</span> area loss and comparisons with durability tests</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Robin, C.; Gérard, M.; Quinaud, M.; d'Arbigny, J.; Bultel, Y.</p> <p>2016-09-01</p> <p>The prediction of Proton <span class="hlt">Exchange</span> Membrane Fuel Cell (PEMFC) lifetime is one of the major challenges to optimize both material properties and dynamic control of the fuel cell system. In this study, by a multiscale <span class="hlt">modeling</span> approach, a mechanistic catalyst dissolution <span class="hlt">model</span> is coupled to a dynamic PEMFC cell <span class="hlt">model</span> to predict the performance loss of the PEMFC. Results are compared to two 2000-h experimental aging tests. More precisely, an original approach is introduced to estimate the loss of an equivalent active <span class="hlt">surface</span> area during an aging test. Indeed, when the computed Electrochemical Catalyst <span class="hlt">Surface</span> Area profile is fitted on the experimental measures from Cyclic Voltammetry, the computed performance loss of the PEMFC is underestimated. To be able to predict the performance loss measured by polarization curves during the aging test, an equivalent active <span class="hlt">surface</span> area is obtained by a <span class="hlt">model</span> inversion. This methodology enables to successfully find back the experimental cell voltage decay during time. The <span class="hlt">model</span> parameters are fitted from the polarization curves so that they include the global degradation. Moreover, the <span class="hlt">model</span> captures the aging heterogeneities along the <span class="hlt">surface</span> of the cell observed experimentally. Finally, a second 2000-h durability test in dynamic operating conditions validates the approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec57-5006.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec57-5006.pdf"><span>30 CFR 57.5006 - <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 30 Mineral Resources 1 2014-07-01 2014-07-01 false <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved] 57.5006... Quality, Radiation, Physical Agents, and Diesel Particulate Matter <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> and Underground...-Nitrosodimethylamine. <span class="hlt">Air</span> Quality—<span class="hlt">Surface</span> Only [Reserved] <span class="hlt">Air</span> Quality—Underground Only ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec57-5006.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec57-5006.pdf"><span>30 CFR 57.5006 - <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 30 Mineral Resources 1 2012-07-01 2012-07-01 false <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved] 57.5006... Quality, Radiation, Physical Agents, and Diesel Particulate Matter <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> and Underground...-Nitrosodimethylamine. <span class="hlt">Air</span> Quality—<span class="hlt">Surface</span> Only [Reserved] <span class="hlt">Air</span> Quality—Underground Only ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec57-5006.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec57-5006.pdf"><span>30 CFR 57.5006 - <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 30 Mineral Resources 1 2013-07-01 2013-07-01 false <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> Only [Reserved] 57.5006... Quality, Radiation, Physical Agents, and Diesel Particulate Matter <span class="hlt">Air</span> Quality-<span class="hlt">Surface</span> and Underground...-Nitrosodimethylamine. <span class="hlt">Air</span> Quality—<span class="hlt">Surface</span> Only [Reserved] <span class="hlt">Air</span> Quality—Underground Only ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15330437','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15330437"><span>[Comparison of <span class="hlt">air</span>/soil mercury <span class="hlt">exchange</span> between warm and cold season in Hongfeng Reservoir region].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Shao-feng; Feng, Xin-bin; Qiu, Guang-le; Fu, Xue-wu</p> <p>2004-01-01</p> <p>In July 2002 and March 2003, the mercury <span class="hlt">exchange</span> flux between soil and <span class="hlt">air</span> was measured using dynamic flux chamber method in Hongfeng Reservoir region. Mercury <span class="hlt">exchange</span> flux is (27.4 +/- 40.1) ng x (m2 x h)(-1) (n = 255) and (5.6 +/- 19.4) ng x (m2 x h)(-1) (n = 192) in summer and winter respectively. The correlation coefficient between mercury flux and solar radiation, <span class="hlt">air</span> temperature, soil temperature is 0.74, 0.83 and 0.80 in summer, and 0.88, 0.56 and 0.59 in winter. From the data, it was found that the mercury emission is stronger in summer than that in winter, and compared to winter, mercury <span class="hlt">exchange</span> between soil and <span class="hlt">air</span> depends more on meteorological conditions in summer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1358252','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1358252"><span>Miniaturized <span class="hlt">Air</span>-to-Refrigerant Heat <span class="hlt">Exchangers</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>Radermacher, Reinhard; Bacellar, Daniel; Aute, Vikrant</p> <p></p> <p><span class="hlt">Air</span>-to-refrigerant Heat <span class="hlt">eXchangers</span> (HX) are an essential component of Heating, Ventilation, <span class="hlt">Air</span>-Conditioning, and Refrigeration (HVAC&R) systems, serving as the main heat transfer component. The major limiting factor to HX performance is the large airside thermal resistance. Recent literature aims at improving heat transfer performance by utilizing enhancement methods such as fins and small tube diameters; this has lead to almost exhaustive research on the microchannel HX (MCHX). The objective of this project is to develop a miniaturized <span class="hlt">air</span>-to-refrigerant HX with at least 20% reduction in volume, material volume, and approach temperature compared to current state-of-the-art multiport flat tube designs andmore » also be capable of production within five years. Moreover, the proposed HX’s are expected to have good water drainage and should succeed in both evaporator and condenser applications. The project leveraged Parallel-Parametrized Computational Fluid Dynamics (PPCFD) and Approximation-Assisted Optimization (AAO) techniques to perform multi-scale analysis and shape optimization with the intent of developing novel HX designs whose thermal-hydraulic performance exceeds that of state-of-the-art MCHX. Nine heat <span class="hlt">exchanger</span> geometries were initially chosen for detailed analysis, selected from 35+ geometries which were identified in previous work at the University of Maryland, College Park. The newly developed optimization framework was exercised for three design optimization problems: (DP I) 1.0kW radiator, (DP II) 10kW radiator and (DP III) 10kW two-phase HX. DP I consisted of the design and optimization of 1.0kW <span class="hlt">air</span>-to-water HX’s which exceeded the project requirements of 20% volume/material reduction and 20% better performance. Two prototypes for the 1.0kW HX were prototyped, tested and validated using newly-designed airside and refrigerant side test facilities. DP II, a scaled version DP I for 10kW <span class="hlt">air</span>-to-water HX applications, also yielded optimized HX</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('https://www.ncbi.nlm.nih.gov/pubmed/21827644','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21827644"><span>Performance evaluation on an <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> for alumina nanofluid under laminar flow.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Teng, Tun-Ping; Hung, Yi-Hsuan; Teng, Tun-Chien; Chen, Jyun-Hong</p> <p>2011-08-09</p> <p>This study analyzes the characteristics of alumina (Al2O3)/water nanofluid to determine the feasibility of its application in an <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> for heat dissipation for PEMFC or electronic chip cooling. The experimental sample was Al2O3/water nanofluid produced by the direct synthesis method at three different concentrations (0.5, 1.0, and 1.5 wt.%). The experiments in this study measured the thermal conductivity and viscosity of nanofluid with weight fractions and sample temperatures (20-60°C), and then used the nanofluid in an actual <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> to assess its heat <span class="hlt">exchange</span> capacity and pressure drop under laminar flow. Experimental results show that the nanofluid has a higher heat <span class="hlt">exchange</span> capacity than water, and a higher concentration of nanoparticles provides an even better ratio of the heat <span class="hlt">exchange</span>. The maximum enhanced ratio of heat <span class="hlt">exchange</span> and pressure drop for all the experimental parameters in this study was about 39% and 5.6%, respectively. In addition to nanoparticle concentration, the temperature and mass flow rates of the working fluid can affect the enhanced ratio of heat <span class="hlt">exchange</span> and pressure drop of nanofluid. The cross-section aspect ratio of tube in the heat <span class="hlt">exchanger</span> is another important factor to be taken into consideration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3212002','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3212002"><span>Performance evaluation on an <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> for alumina nanofluid under laminar flow</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2011-01-01</p> <p>This study analyzes the characteristics of alumina (Al2O3)/water nanofluid to determine the feasibility of its application in an <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> for heat dissipation for PEMFC or electronic chip cooling. The experimental sample was Al2O3/water nanofluid produced by the direct synthesis method at three different concentrations (0.5, 1.0, and 1.5 wt.%). The experiments in this study measured the thermal conductivity and viscosity of nanofluid with weight fractions and sample temperatures (20-60°C), and then used the nanofluid in an actual <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> to assess its heat <span class="hlt">exchange</span> capacity and pressure drop under laminar flow. Experimental results show that the nanofluid has a higher heat <span class="hlt">exchange</span> capacity than water, and a higher concentration of nanoparticles provides an even better ratio of the heat <span class="hlt">exchange</span>. The maximum enhanced ratio of heat <span class="hlt">exchange</span> and pressure drop for all the experimental parameters in this study was about 39% and 5.6%, respectively. In addition to nanoparticle concentration, the temperature and mass flow rates of the working fluid can affect the enhanced ratio of heat <span class="hlt">exchange</span> and pressure drop of nanofluid. The cross-section aspect ratio of tube in the heat <span class="hlt">exchanger</span> is another important factor to be taken into consideration. PMID:21827644</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=322488&simplesearch=1&searchall=nitrogen+or+phosphorus+or+nutrient&noarchive=1&sitype=sa&sitype=pr','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=322488&simplesearch=1&searchall=nitrogen+or+phosphorus+or+nutrient&noarchive=1&sitype=sa&sitype=pr"><span>The Measurement and <span class="hlt">modeling</span> of the contribution of ...</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>In North America, ammonia (NH3) is increasingly being recognized not only for its role in atmospheric aerosol formation but also as an important component of atmospheric nitrogen deposition. This has been driven by the evolution of policies to protect ecosystems from nitrogen over-enrichment, an expansion of research underpinning these policy efforts, and technological advances in measurement and <span class="hlt">modeling</span> tools applied to these research needs. Ammonia measurements from satellites, nitrogen focused field campaigns, and the National Atmospheric Deposition Program’s Ammonia Monitoring Network (AMoN) have advanced understanding of the processes controlling NH3 <span class="hlt">air-surface</span> <span class="hlt">exchange</span> and the spatio-temporal behavior of NH3 in the atmosphere. These datasets have subsequently lead to improvements in NH3 <span class="hlt">air-surface</span> <span class="hlt">exchange</span> <span class="hlt">models</span> and therefore more accurate estimates of NH3 deposition. From a process standpoint, NH3 differs from other nitrogen compounds such as nitric acid in that NH3 is <span class="hlt">exchanged</span> bi-directionally between the <span class="hlt">surface</span> and atmosphere as regulated by a “compensation point”. Because natural <span class="hlt">surfaces</span> may be sources or sinks of atmospheric NH3, and may alternate between emission and deposition on a timescale as short as hours, the deposition velocity concept does not accurately describe NH3 <span class="hlt">air</span> <span class="hlt">surface</span> <span class="hlt">exchange</span>. Instead, a more mechanistic treatment of the nitrogen status and acidity of the <span class="hlt">surface</span> must be employed, typically as a bi-directional fr</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.1658C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.1658C"><span><span class="hlt">Modeling</span> the Physical Multi-Phase Interactions of HNO3 Between Snow and <span class="hlt">Air</span> on the Antarctic Plateau (Dome C) and coast (Halley)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chan, Hoi Ga; Frey, Markus M.; King, Martin D.</p> <p>2017-04-01</p> <p>Nitrogen oxides (NOx = NO + NO2) emissions from nitrate (NO3-) photolysis in snow affect the oxidising capacity of the lower troposphere especially in remote regions of the high latitudes with low pollution levels. The porous structure of snowpack allows the <span class="hlt">exchange</span> of gases with the atmosphere driven by physicochemical processes, and hence, snow can act as both source and sink of atmospheric chemical trace gases. Current <span class="hlt">models</span> are limited by poor process understanding and often require tuning parameters. Here, two multi-phase physical <span class="hlt">models</span> were developed from first principles constrained by observed atmospheric nitrate, HNO3, to describe the <span class="hlt">air</span>-snow interaction of nitrate. Similar to most of the previous approaches, the first <span class="hlt">model</span> assumes that below a threshold temperature, To, the <span class="hlt">air</span>-snow grain interface is pure ice and above To, a disordered interface (DI) emerges assumed to be covering the entire grain <span class="hlt">surface</span>. The second <span class="hlt">model</span> assumes that <span class="hlt">Air</span>-Ice interactions dominate over the entire temperature range below melting and that only above the eutectic temperature, liquid is present in the form of micropockets in grooves. The <span class="hlt">models</span> are validated with available year-round observations of nitrate in snow and <span class="hlt">air</span> at a cold site on the Antarctica Plateau (Dome C, 75°06'S, 123°33'E, 3233 m a.s.l.) and at a relatively warm site on the Antarctica coast (Halley, 75°35'S, 26°39'E, 35 m a.s.l). The first <span class="hlt">model</span> agrees reasonably well with observations at Dome C (Cv(RMSE) = 1.34), but performs poorly at Halley (Cv(RMSE) = 89.28) while the second <span class="hlt">model</span> reproduces with good agreement observations at both sites without any tuning (Cv(RMSE) = 0.84 at both sites). It is therefore suggested that <span class="hlt">air</span>-snow interactions of nitrate in the winter are determined by non-equilibrium <span class="hlt">surface</span> adsorption and co-condensation on ice coupled with solid-state diffusion inside the grain. In summer, however, the <span class="hlt">air</span>-snow <span class="hlt">exchange</span> of nitrate is mainly driven by solvation into liquid</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=180684&keyword=global+AND+water+AND+issues&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=180684&keyword=global+AND+water+AND+issues&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>ISSUES IN SIMULATING ELEMENTAL MERCURY <span class="hlt">AIR</span>/WATER <span class="hlt">EXCHANGE</span> AND AQUEOUS MONOMETHYLMERCURY SPECIATION</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>This presentation focuses on two areas relevant to assessing the global fate and bioavailability of mercury: elemental mercury <span class="hlt">air</span>/water <span class="hlt">exchange</span> and aqueous environmental monomethylmercury speciation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29627685','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29627685"><span>Structural equation <span class="hlt">modeling</span> of PAHs in ambient <span class="hlt">air</span>, dust fall, soil, and cabbage in vegetable bases of Northern China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, YunHui; Hou, DeYi; Xiong, GuanNan; Duan, YongHong; Cai, ChuanYang; Wang, Xin; Li, JingYa; Tao, Shu; Liu, WenXin</p> <p>2018-08-01</p> <p>A series of field samples including ambient <span class="hlt">air</span> (gaseous and particulate phases), dust fall, <span class="hlt">surface</span> soil, rhizosphere soil and cabbage tissues (leaf, root and core), were collected in vegetable bases near a large coking manufacturer in Shanxi Province, Northern China, during a harvest season. A factor analysis was employed to apportion the emission sources of polycyclic aromatic hydrocarbons (PAHs), and the statistical results indicated coal combustion was the dominant emission source that accounted for different environmental media and cabbage tissues, while road traffic, biomass burning and the coking industry contributed to a lesser extent. A structural equation <span class="hlt">model</span> was first developed to quantitatively explore the transport pathways of PAHs from surrounding media to cabbage tissues. The <span class="hlt">modeling</span> results showed that PAHs in ambient <span class="hlt">air</span> were positively associated with those in dust fall, and a close relationship was also true for PAHs in dust fall and in <span class="hlt">surface</span> soil due to <span class="hlt">air</span>-soil <span class="hlt">exchange</span> process. Furthermore, PAHs in <span class="hlt">surface</span> soil were correlated with those in rhizosphere soil and in the cabbage leaf with the path coefficients of 0.83 and 0.39, respectively. PAHs in the cabbage leaf may dominantly contribute to the accumulation of PAHs in the edible part of cabbages. Copyright © 2018 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016FrES...10..644W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016FrES...10..644W"><span>An assessment of precipitation and <span class="hlt">surface</span> <span class="hlt">air</span> temperature over China by regional climate <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Xueyuan; Tang, Jianping; Niu, Xiaorui; Wang, Shuyu</p> <p>2016-12-01</p> <p>An analysis of a 20-year summer time simulation of present-day climate (1989-2008) over China using four regional climate <span class="hlt">models</span> coupled with different land <span class="hlt">surface</span> <span class="hlt">models</span> is carried out. The climatic means, interannual variability, linear trends, and extremes are examined, with focus on precipitation and near <span class="hlt">surface</span> <span class="hlt">air</span> temperature. The <span class="hlt">models</span> are able to reproduce the basic features of the observed summer mean precipitation and temperature over China and the regional detail due to topographic forcing. Overall, the <span class="hlt">model</span> performance is better for temperature than that of precipitation. The <span class="hlt">models</span> reasonably grasp the major anomalies and standard deviations over China and the five subregions studied. The <span class="hlt">models</span> generally reproduce the spatial pattern of high interannual variability over wet regions, and low variability over the dry regions. The <span class="hlt">models</span> also capture well the variable temperature gradient increase to the north by latitude. Both the observed and simulated linear trend of precipitation shows a drying tendency over the Yangtze River Basin and wetting over South China. The <span class="hlt">models</span> capture well the relatively small temperature trends in large areas of China. The <span class="hlt">models</span> reasonably simulate the characteristics of extreme precipitation indices of heavy rain days and heavy precipitation fraction. Most of the <span class="hlt">models</span> also performed well in capturing both the sign and magnitude of the daily maximum and minimum temperatures over China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70155848','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70155848"><span>Groundwater and <span class="hlt">surface</span> water <span class="hlt">exchange</span> and resulting Nitrate dynamics in the Bogue Phalia Basin in northwestern Mississippi</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Barlow, Jeannie R.; Coupe, Richard H.</p> <p>2012-01-01</p> <p>During April 2007 through September 2008, the USGS collected hydrogeologic and water-quality data from a site on the Bogue Phalia to evaluate the role of groundwater and <span class="hlt">surface</span>-water interaction on the transport of nitrate to the shallow sand and gravel aquifer underlying the Mississippi Alluvial Plain in northwestern Mississippi. A two-dimensional groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> <span class="hlt">model</span> was developed using temperature and head data and VS2DH, a variably saturated flow and energy transport <span class="hlt">model</span>. Results from this <span class="hlt">model</span> showed that groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> at the site occurred regularly and recharge was laterally extensive into the alluvial aquifer. Nitrate was consistently reported in <span class="hlt">surface</span>-water samples (n = 52, median concentration = 39.8 μmol/L) although never detected in samples collected from in-stream piezometers or shallow monitoring wells adjacent to the stream (n = 46). These two facts, consistent detections of nitrate in <span class="hlt">surface</span> water and no detections of nitrate in groundwater, coupled with <span class="hlt">model</span> results that indicate large amounts of <span class="hlt">surface</span> water moving through an anoxic streambed, support the case for denitrification and nitrate loss through the streambed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.H54B..06K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.H54B..06K"><span>Upscaling and Downscaling of Land <span class="hlt">Surface</span> Fluxes with <span class="hlt">Surface</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>Kustas, W. P.; Anderson, M. C.; Hain, C.; Albertson, J. D.; Gao, F.; Yang, Y.</p> <p>2015-12-01</p> <p>Land <span class="hlt">surface</span> temperature (LST) is a key <span class="hlt">surface</span> boundary condition that is significantly correlated to <span class="hlt">surface</span> flux partitioning between latent and sensible heat. The spatial and temporal variation in LST is driven by radiation, wind, vegetation cover and roughness as well as soil moisture status in the <span class="hlt">surface</span> and root zone. Data from airborne and satellite-based platforms provide LST from ~10 km to sub meter resolutions. A land <span class="hlt">surface</span> scheme called the Two-Source Energy Balance (TSEB) <span class="hlt">model</span> has been incorporated into a multi-scale regional <span class="hlt">modeling</span> system ALEXI (Atmosphere Land <span class="hlt">Exchange</span> Inverse) and a disaggregation scheme (DisALEXI) using higher resolution LST. Results with this <span class="hlt">modeling</span> system indicates that it can be applied over heterogeneous land <span class="hlt">surfaces</span> and estimate reliable <span class="hlt">surface</span> fluxes with minimal in situ information. Consequently, this <span class="hlt">modeling</span> system allows for scaling energy fluxes from subfield to regional scales in regions with little ground data. In addition, the TSEB scheme has been incorporated into a large Eddy Simulation (LES) <span class="hlt">model</span> for investigating dynamic interactions between variations in the land <span class="hlt">surface</span> state reflected in the spatial pattern in LST and the lower atmospheric <span class="hlt">air</span> properties affecting energy <span class="hlt">exchange</span>. An overview of research results on scaling of fluxes and interactions with the lower atmosphere from the subfield level to regional scales using the TSEB, ALEX/DisALEX and the LES-TSEB approaches will be presented. Some unresolved issues in the use of LST at different spatial resolutions for estimating <span class="hlt">surface</span> energy balance and upscaling fluxes, particularly evapotranspiration, will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PSST...23f5036P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PSST...23f5036P"><span>Quantification of <span class="hlt">air</span> plasma chemistry for <span class="hlt">surface</span> disinfection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pavlovich, Matthew J.; Clark, Douglas S.; Graves, David B.</p> <p>2014-12-01</p> <p>Atmospheric-pressure <span class="hlt">air</span> plasmas, created by a variety of discharges, are promising sources of reactive species for the emerging field of plasma biotechnology because of their convenience and ability to operate at ambient conditions. One biological application of ambient-<span class="hlt">air</span> plasma is microbial disinfection, and the ability of <span class="hlt">air</span> plasmas to decontaminate both solid <span class="hlt">surfaces</span> and liquid volumes has been thoroughly established in the literature. However, the mechanism of disinfection and which reactive species most strongly correlate with antimicrobial effects are still not well understood. We describe quantitative gas-phase measurements of plasma chemistry via infrared spectroscopy in confined volumes, focusing on <span class="hlt">air</span> plasma generated via <span class="hlt">surface</span> micro-discharge (SMD). Previously, it has been shown that gaseous chemistry is highly sensitive to operating conditions, and the measurements we describe here extend those findings. We quantify the gaseous concentrations of ozone (O3) and nitrogen oxides (NO and NO2, or NOx) throughout the established ‘regimes’ for SMD <span class="hlt">air</span> plasma chemistry: the low-power, ozone-dominated mode; the high-power, nitrogen oxides-dominated mode; and the intermediate, unstable transition region. The results presented here are in good agreement with previously published experimental studies of aqueous chemistry and parameterized <span class="hlt">models</span> of gaseous chemistry. The principal finding of the present study is the correlation of bacterial inactivation on dry <span class="hlt">surfaces</span> with gaseous chemistry across these time and power regimes. Bacterial decontamination is most effective in ‘NOx mode’ and less effective in ‘ozone mode’, with the weakest antibacterial effects in the transition region. Our results underscore the dynamic nature of <span class="hlt">air</span> plasma chemistry and the importance of careful chemical characterization of plasma devices intended for biological applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27236846','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27236846"><span>Leaching heavy metals from the <span class="hlt">surface</span> soil of reclaimed tidal flat by alternating seawater inundation and <span class="hlt">air</span> drying.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guo, Shi-Hong; Liu, Zhen-Ling; Li, Qu-Sheng; Yang, Ping; Wang, Li-Li; He, Bao-Yan; Xu, Zhi-Min; Ye, Jin-Shao; Zeng, Eddy Y</p> <p>2016-08-01</p> <p>Leaching experiments were conducted in a greenhouse to simulate seawater leaching combined with alternating seawater inundation and <span class="hlt">air</span> drying. We investigated the heavy metal release of soils caused by changes associated with seawater inundation/<span class="hlt">air</span> drying cycles in the reclaimed soils. After the treatment, the contents of all heavy metals (Cd, Pb, Cr, and Cu), except Zn, in <span class="hlt">surface</span> soil significantly decreased (P < 0.05), with removal rates ranging from 10% to 51%. The amounts of the <span class="hlt">exchangeable</span>, carbonate, reducible, and oxidizable fractions also significantly decreased (P < 0.05). Moreover, prolonged seawater inundation enhanced the release of heavy metals. Measurement of diffusive gradients in thin films indicated that seawater inundation significantly increased the re-mobility of heavy metals. During seawater inundation, iron oxide reduction induced the release of heavy metals in the reducible fraction. Decomposition of organic matter, and complexation with dissolved organic carbon decreased the amount of heavy metals in the oxidizable fraction. Furthermore, complexation of chloride ions and competition of cations during seawater inundation and/or leaching decreased the levels of heavy metals in the <span class="hlt">exchangeable</span> fraction. By contrast, <span class="hlt">air</span> drying significantly enhanced the concentration of heavy metals in the <span class="hlt">exchangeable</span> fraction. Therefore, the removal of heavy metals in the <span class="hlt">exchangeable</span> fraction can be enhanced during subsequent leaching with seawater. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27461227','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27461227"><span><span class="hlt">Air</span> breathing and aquatic gas <span class="hlt">exchange</span> during hypoxia in armoured catfish.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Scott, Graham R; Matey, Victoria; Mendoza, Julie-Anne; Gilmour, Kathleen M; Perry, Steve F; Almeida-Val, Vera M F; Val, Adalberto L</p> <p>2017-01-01</p> <p><span class="hlt">Air</span> breathing in fish is commonly believed to have arisen as an adaptation to aquatic hypoxia. The effectiveness of <span class="hlt">air</span> breathing for tissue O 2 supply depends on the ability to avoid O 2 loss as oxygenated blood from the <span class="hlt">air</span>-breathing organ passes through the gills. Here, we evaluated whether the armoured catfish (Hypostomus aff. pyreneusi)-a facultative <span class="hlt">air</span> breather-can avoid branchial O 2 loss while <span class="hlt">air</span> breathing in aquatic hypoxia, and we measured various other respiratory and metabolic traits important for O 2 supply and utilization. Fish were instrumented with opercular catheters to measure the O 2 tension (PO 2 ) of expired water, and <span class="hlt">air</span> breathing and aquatic respiration were measured during progressive stepwise hypoxia in the water. Armoured catfish exhibited relatively low rates of O 2 consumption and gill ventilation, and gill ventilation increased in hypoxia due primarily to increases in ventilatory stroke volume. Armoured catfish began <span class="hlt">air</span> breathing at a water PO 2 of 2.5 kPa, and both <span class="hlt">air</span>-breathing frequency and hypoxia tolerance (as reflected by PO 2 at loss of equilibrium, LOE) was greater in individuals with a larger body mass. Branchial O 2 loss, as reflected by higher PO 2 in expired than in inspired water, was observed in a minority (4/11) of individuals as water PO 2 approached that at LOE. Armoured catfish also exhibited a gill morphology characterized by short filaments bearing short fused lamellae, large interlamellar cell masses, low <span class="hlt">surface</span> area, and a thick epithelium that increased water-to-blood diffusion distance. Armoured catfish had a relatively low blood-O 2 binding affinity when sampled in normoxia (P 50 of 3.1 kPa at pH 7.4), but were able to rapidly increase binding affinity during progressive hypoxia exposure (to a P 50 of 1.8 kPa). Armoured catfish also had low activities of several metabolic enzymes in white muscle, liver, and brain. Therefore, low rates of metabolism and gill ventilation, and a reduction in branchial gas-<span class="hlt">exchange</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040082134','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040082134"><span>Extratropical Stratosphere-Troposphere Mass <span class="hlt">Exchange</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schoeberl, Mark R.</p> <p>2004-01-01</p> <p>Understanding the <span class="hlt">exchange</span> of gases between the stratosphere and the troposphere is important for determining how pollutants enter the stratosphere and how they leave. This study does a global analysis of that the <span class="hlt">exchange</span> of mass between the stratosphere and the troposphere. While the <span class="hlt">exchange</span> of mass is not the same as the <span class="hlt">exchange</span> of constituents, you can t get the constituent <span class="hlt">exchange</span> right if you have the mass <span class="hlt">exchange</span> wrong. Thus this kind of calculation is an important test for <span class="hlt">models</span> which also compute trace gas transport. In this study I computed the mass <span class="hlt">exchange</span> for two assimilated data sets and a GCM. The <span class="hlt">models</span> all agree that amount of mass descending from the stratosphere to the troposphere in the Northern Hemisphere extra tropics is approx. 10(exp 10) kg/s averaged over a year. The value for the Southern Hemisphere by about a factor of two. ( 10(exp 10) kg of <span class="hlt">air</span> is the amount of <span class="hlt">air</span> in 100 km x 100 km area with a depth of 100 m - roughly the size of the D.C. metro area to a depth of 300 feet.) Most people have the idea that most of the mass enters the stratosphere through the tropics. But this study shows that almost 5 times more mass enters the stratosphere through the extra-tropics. This mass, however, is quickly recycled out again. Thus the lower most stratosphere is a mixture of upper stratospheric <span class="hlt">air</span> and tropospheric <span class="hlt">air</span>. This is an important result for understanding the chemistry of the lower stratosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DSRI..122...17M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DSRI..122...17M"><span>The <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of mercury in the low latitude Pacific and Atlantic Oceans</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mason, Robert P.; Hammerschmidt, Chad R.; Lamborg, Carl H.; Bowman, Katlin L.; Swarr, Gretchen J.; Shelley, Rachel U.</p> <p>2017-04-01</p> <p><span class="hlt">Air</span>-sea <span class="hlt">exchange</span> is an important component of the global mercury (Hg) cycle as it mediates the rate of increase in ocean Hg, and therefore the rate of change in levels of methylmercury (MeHg), the most toxic and bioaccumulative form of Hg in seafood and the driver of human health concerns. Gas evasion of elemental Hg (Hg0) from the ocean is an important sink for ocean Hg with previous studies suggesting that evasion is not uniform across ocean basins. To understand further the factors controlling Hg0 evasion, and its relationship to atmospheric Hg deposition, we made measurements of dissolved Hg0 (DHg0) in <span class="hlt">surface</span> waters, along with measurements of Hg in precipitation and on aerosols, and Hg0 in marine <span class="hlt">air</span>, during two GEOTRACES cruises; GP16 in the equatorial South Pacific and GA03 in the North Atlantic. We contrast the concentrations and estimated evasion fluxes of Hg0 during these cruises, and the factors influencing this <span class="hlt">exchange</span>. Concentrations of DHg0 and fluxes were lower during the GP16 cruise than during the GA03 cruise, and likely reflect the lower atmospheric deposition in the South Pacific. An examination of Hg/Al ratios for aerosols from the cruises suggests that they were anthropogenically-enriched relative to crustal material, although to a lesser degree for the South Pacific than the aerosols over the North Atlantic. Both regions appear to be net sources of Hg0 to the atmosphere (evasion>deposition) and the reasons for this are discussed. Overall, the studies reported here provide further clarification on the factors controlling evasion of Hg0 from the ocean <span class="hlt">surface</span>, and the role of anthropogenic inputs in influencing ocean Hg concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29801207','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29801207"><span>Photochemical <span class="hlt">model</span> evaluation of 2013 California wild fire <span class="hlt">air</span> quality impacts using <span class="hlt">surface</span>, aircraft, and satellite data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baker, K R; Woody, M C; Valin, L; Szykman, J; Yates, E L; Iraci, L T; Choi, H D; Soja, A J; Koplitz, S N; Zhou, L; Campuzano-Jost, Pedro; Jimenez, Jose L; Hair, J W</p> <p>2018-10-01</p> <p>The Rim Fire was one of the largest wildfires in California history, burning over 250,000 acres during August and September 2013 affecting <span class="hlt">air</span> quality locally and regionally in the western U.S. Routine <span class="hlt">surface</span> monitors, remotely sensed data, and aircraft based measurements were used to assess how well the Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) photochemical grid <span class="hlt">model</span> applied at 4 and 12 km resolution represented regional plume transport and chemical evolution during this extreme wildland fire episode. Impacts were generally similar at both grid resolutions although notable differences were seen in some secondary pollutants (e.g., formaldehyde and peroxyacyl nitrate) near the Rim fire. The <span class="hlt">modeling</span> system does well at capturing near-fire to regional scale smoke plume transport compared to remotely sensed aerosol optical depth (AOD) and aircraft transect measurements. Plume rise for the Rim fire was well characterized as the <span class="hlt">modeled</span> plume top was consistent with remotely sensed data and the altitude of aircraft measurements, which were typically made at the top edge of the plume. Aircraft-based lidar suggests O 3 downwind in the Rim fire plume was vertically stratified and tended to be higher at the plume top, while CMAQ estimated a more uniformly mixed column of O 3 . Predicted wildfire ozone (O 3 ) was overestimated both at the plume top and at nearby rural and urban <span class="hlt">surface</span> monitors. Photolysis rates were well characterized by the <span class="hlt">model</span> compared with aircraft measurements meaning aerosol attenuation was reasonably estimated and unlikely contributing to O 3 overestimates at the top of the plume. Organic carbon was underestimated close to the Rim fire compared to aircraft data, but was consistent with nearby <span class="hlt">surface</span> measurements. Periods of elevated <span class="hlt">surface</span> PM 2.5 at rural monitors near the Rim fire were not usually coincident with elevated O 3 . Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830026675','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830026675"><span>Use of cooling <span class="hlt">air</span> heat <span class="hlt">exchangers</span> as replacements for hot section strategic materials</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gauntner, J. W.</p> <p>1983-01-01</p> <p>Because of financial and political constraints, strategic aerospace materials required for the hot section of future engines might be in short supply. As an alternative to these strategic materials, this study examines the use of a cooling <span class="hlt">air</span> heat <span class="hlt">exchanger</span> in combination with less advanced hot section materials. Cycle calculations are presented for future turbofan systems with overall pressure ratios to 65, bypass ratios near 13, and combustor exit temperatures to 3260 R. These calculations quantify the effect on TSFC of using a decreased materials technology in a turbofan system. The calculations show that the cooling <span class="hlt">air</span> heat <span class="hlt">exchanger</span> enables the feasibility of these engines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=278574&Lab=NCEA&keyword=simulation+AND+processes&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=278574&Lab=NCEA&keyword=simulation+AND+processes&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>Estimating North American background ozone in U.S. <span class="hlt">surface</span> <span class="hlt">air</span> with two independent global <span class="hlt">models</span>: Variability, uncertainties, and recommendations</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>Accurate estimates for North American background (NAB) ozone (O3) in <span class="hlt">surface</span> <span class="hlt">air</span> over the United States are needed for setting and implementing an attainable national O3 standard. These estimates rely on simulations with atmospheric chemistry-transport <span class="hlt">models</span> that set North Amer...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CPL...695..240Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CPL...695..240Y"><span>A spin <span class="hlt">exchange</span> <span class="hlt">model</span> for singlet fission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yago, Tomoaki; Wakasa, Masanobu</p> <p>2018-03-01</p> <p>Singlet fission has been analyzed with the Dexter <span class="hlt">model</span> in which electron <span class="hlt">exchange</span> occurs between chromophores, conserving the spin for each electron. In the present study, we propose a spin <span class="hlt">exchange</span> <span class="hlt">model</span> for singlet fission. In the spin <span class="hlt">exchange</span> <span class="hlt">model</span>, spins are <span class="hlt">exchanged</span> by the <span class="hlt">exchange</span> interaction between two electrons. Our analysis with simple spin functions demonstrates that singlet fission is possible by spin <span class="hlt">exchange</span>. A necessary condition for spin <span class="hlt">exchange</span> is a variation in <span class="hlt">exchange</span> interactions. We also adapt the spin <span class="hlt">exchange</span> <span class="hlt">model</span> to triplet fusion and triplet energy transfer, which often occur after singlet fission in organic solids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.B11E..08C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.B11E..08C"><span>Process <span class="hlt">Model</span> for Studying Regional 13C Stable Isotope <span class="hlt">Exchange</span> between Vegetation and Atmosphere</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.; Chen, B.; Huang, L.; Tans, P.; Worthy, D.; Ishizawa, M.; Chan, D.</p> <p>2007-12-01</p> <p>The variation of the stable isotope 13CO2 in the <span class="hlt">air</span> in <span class="hlt">exchange</span> with land ecosystems results from fractionation processes in both plants and soil during photosynthesis and respiration. Its diurnal and seasonal variations therefore contain information on the carbon cycle. We developed a <span class="hlt">model</span> (BEPS-iso) to simulate its <span class="hlt">exchange</span> between vegetation and the atmosphere. To be useful for regional carbon cycle studies, the <span class="hlt">model</span> has the following characteristics: (i) it considers the turbulent mixing in the vertical profile from the soil <span class="hlt">surface</span> to the top of the planetary boundary layer (PBL); (ii) it scales individual leaf photosynthetic discrimination to the whole canopy through the separation of sunlit and shaded leaf groups; (iii) through simulating leaf-level photosynthetic processes, it has the capacity to mechanistically examine isotope discrimination resulting from meteorological forcings, such as radiation, precipitation and humidity; and (iv) through complete <span class="hlt">modeling</span> of radiation, energy and water fluxes, it also simulates soil moisture and temperature needed for estimating ecosystem respiration and the 13C signal from the soil. After validation using flask data acquired at 20 m level on a tower near Fraserdale, Ontario, Canada, during intensive campaigns (1998-2000), the <span class="hlt">model</span> has been used for several purposes: (i) to investigate the diurnal and seasonal variations in the disequilibrium in 13C fractionation between ecosystem respiration and photosynthesis, which is an important step in using 13C measurements to separate these carbon cycle components; (ii) to quantify the 13C rectification in the PBL, which differs significantly from CO2 rectification because of the diurnal and seasonal disequilibriums; and (iii) to <span class="hlt">model</span> the 13C spatial and temporal variations over the global land <span class="hlt">surface</span> for the purpose of CO2 inversion using 13C as an additional constraint.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=311934&Lab=NERL&keyword=simulation+AND+processes&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=311934&Lab=NERL&keyword=simulation+AND+processes&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>Development and Evaluation of a New <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rate Algorithm for the Stochastic Human Exposure and Dose Simulation <span class="hlt">Model</span> (ISES Presentation)</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>Previous exposure assessment panel studies have observed considerable seasonal, between-home and between-city variability in residential pollutant infiltration. This is likely a result of differences in home ventilation, or <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AER). The Stochastic Human Exposure ...</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/2015EGUGA..1714679M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714679M"><span>Carbon speciation at the <span class="hlt">air</span>-sea interface during rain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McGillis, Wade; Hsueh, Diana; Takeshita, Yui; Donham, Emily; Markowitz, Michele; Turk, Daniela; Martz, Todd; Price, Nicole; Langdon, Chris; Najjar, Raymond; Herrmann, Maria; Sutton, Adrienne; Loose, Brice; Paine, Julia; Zappa, Christopher</p> <p>2015-04-01</p> <p>This investigation demonstrates the <span class="hlt">surface</span> ocean dilution during rain events on the ocean and quantifies the lowering of <span class="hlt">surface</span> pCO2 affecting the <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of carbon dioxide. <span class="hlt">Surface</span> salinity was measured during rain events in Puerto Rico, the Florida Keys, East Coast USA, Panama, and the Palmyra Atoll. End-member analysis is used to determine the subsequent <span class="hlt">surface</span> ocean carbonate speciation. <span class="hlt">Surface</span> ocean carbonate chemistry was measured during rain events to verify any approximations made. The physical processes during rain (cold, fresh water intrusion and buoyancy, <span class="hlt">surface</span> waves and shear, microscale mixing) are described. The role of rain on <span class="hlt">surface</span> mixing, biogeochemistry, and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20001972-waking-sleeping-giant-introducing-new-heat-exchanger-technology-residential-air-conditioning-marketplace','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20001972-waking-sleeping-giant-introducing-new-heat-exchanger-technology-residential-air-conditioning-marketplace"><span>Waking the sleeping giant: Introducing new heat <span class="hlt">exchanger</span> technology into the residential <span class="hlt">air</span>-conditioning marketplace</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>Chapp, T.; Voss, M.; Stephens, C.</p> <p>1998-07-01</p> <p>The <span class="hlt">Air</span> Conditioning Industry has made tremendous strides in improvements to the energy efficiency and reliability of its product offerings over the past 40 years. These improvement can be attributed to enhancements of components, optimization of the energy cycle, and modernized and refined manufacturing techniques. During this same period, energy consumption for space cooling has grown significantly. In January of 1992, the minimum efficiency requirement for central <span class="hlt">air</span> conditioning equipment was raised to 10 SEER. This efficiency level is likely to increase further under the auspices of the National Appliance Energy Conservation Act (NAECA). A new type of heat exchangermore » was developed for <span class="hlt">air</span> conditioning equipment by Modine Manufacturing Company in the early 1990's. Despite significant advantages in terms of energy efficiency, dehumidification, durability, and refrigerant charge there has been little interest expressed by the <span class="hlt">air</span> conditioning industry. A cooperative effort between Modine, various utilities, and several state energy offices has been organized to test and demonstrate the viability of this heat <span class="hlt">exchanger</span> design throughout the nation. This paper will review the fundamentals of heat <span class="hlt">exchanger</span> design and document this simple, yet novel technology. These experiences involving equipment retrofits have been documented with respect to the performance potential of <span class="hlt">air</span> conditioning system constructed with PF{trademark} Heat <span class="hlt">Exchangers</span> (generically referred to as microchannel heat <span class="hlt">exchangers</span>) from both an energy efficiency as well as a comfort perspective. The paper will also detail the current plan to introduce 16 to 24 systems into an extended field test throughout the US which commenced in the Fall of 1997.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A43G2558W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A43G2558W"><span><span class="hlt">Air</span>-sea <span class="hlt">exchange</span> and gas-particle partitioning of polycyclic aromatic hydrocarbons over the northwestern Pacific Ocean: Role of East Asian continental outflow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Z.; Guo, Z.</p> <p>2017-12-01</p> <p>We measured 15 parent polycyclic aromatic hydrocarbons (PAHs) in atmosphere and water during a research cruise from the East China Sea (ECS) to the northwestern Pacific Ocean (NWP) in the spring of 2015 to investigate the occurrence, <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>, and gas-particle partitioning of PAHs with a particular focus on the influence of East Asian continental outflow. The gaseous PAH composition and identification of sources were consistent with PAHs from the upwind area, indicating that the gaseous PAHs (three- to five-ring PAHs) were influenced by upwind land pollution. In addition, <span class="hlt">air</span>-sea <span class="hlt">exchange</span> fluxes of gaseous PAHs were estimated to be -54.2 to 107.4 ng m-2 d-1, and was indicative of variations of land-based PAH inputs. The logarithmic gas-particle partition coefficient (logKp) of PAHs regressed linearly against the logarithmic subcooled liquid vapor pressure, with a slope of -0.25. This was significantly larger than the theoretical value (-1), implying disequilibrium between the gaseous and particulate PAHs over the NWP. The non-equilibrium of PAH gas-particle partitioning was shielded from the volatilization of three-ring gaseous PAHs from seawater and lower soot concentrations in particular when the oceanic <span class="hlt">air</span> masses prevailed. <span class="hlt">Modeling</span> PAH absorption into organic matter and adsorption onto soot carbon revealed that the status of PAH gas-particle partitioning deviated more from the <span class="hlt">modeling</span> Kp for oceanic <span class="hlt">air</span> masses than those for continental <span class="hlt">air</span> masses, which coincided with higher volatilization of three-ring PAHs and confirmed the influence of <span class="hlt">air</span>-sea <span class="hlt">exchange</span>. Meanwhile, significant linear regressions between logKp and logKoa (logKsa) for PAHs were observed for continental <span class="hlt">air</span> masses, suggesting the dominant effect of East Asian continental outflow on atmospheric PAHs over the NWP during the sampling campaign.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010MsT..........6R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010MsT..........6R"><span><span class="hlt">Air</span> and Ground <span class="hlt">Surface</span> Temperature Relations in a Mountainous Basin, Wolf Creek, Yukon Territory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roadhouse, Emily A.</p> <p></p> <p>The links between climate and permafrost are well known, but the precise nature of the relationship between <span class="hlt">air</span> and ground temperatures remains poorly understood, particularly in complex mountain environments. Although previous studies indicate that elevation and potential incoming solar radiation (PISR) are the two leading factors contributing to the existence of permafrost at a given location, additional factors may also contribute significantly to the existence of mountain permafrost, including vegetation cover, snow accumulation and the degree to which individual mountain landscapes are prone to <span class="hlt">air</span> temperature inversions. Current mountain permafrost <span class="hlt">models</span> consider only elevation and aspect, and have not been able to deal with inversion effects in a systematic fashion. This thesis explores the relationship between <span class="hlt">air</span> and ground <span class="hlt">surface</span> temperatures and the presence of <span class="hlt">surface</span>-based inversions at 27 sites within the Wolf Creek basin and surrounding area between 2001 and 2006, as a first step in developing an improved permafrost distribution TTOP <span class="hlt">model</span>. The TTOP <span class="hlt">model</span> describes the relationship between the mean annual <span class="hlt">air</span> temperature and the temperature at the top of permafrost in terms of the <span class="hlt">surface</span> and thermal offsets (Smith and Riseborough, 2002). Key components of this <span class="hlt">model</span> are n-factors which relate <span class="hlt">air</span> and ground climate by establishing the ratio between <span class="hlt">air</span> and <span class="hlt">surface</span> freezing (winter) and thawing (summer) degree-days, thus summarizing the <span class="hlt">surface</span> energy balance on a seasonal basis. Here we examine (1) <span class="hlt">surface</span> offsets and (2) freezing and thawing n-factor variability at a number of sites through altitudinal treeline in the southern Yukon. Thawing n-factors (nt) measured at individual sites remained relatively constant from one year to the next and may be related to land cover. During the winter, the insulating effect of a thick snow cover results in higher <span class="hlt">surface</span> temperatures, while thin snow cover results in low <span class="hlt">surface</span> temperatures more closely</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=volume+AND+concept&pg=7&id=EJ667010','ERIC'); return false;" href="https://eric.ed.gov/?q=volume+AND+concept&pg=7&id=EJ667010"><span>Authentic Assessment in the Geometry Classroom: Calculating the Classroom <span class="hlt">Air-Exchange</span> Rate.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Erich, David J.</p> <p>2002-01-01</p> <p>Introduces a room <span class="hlt">air-exchange</span> activity designed to assess student understanding of the concept of volume. Lists materials for the activity and its procedures. Includes the lesson plan and a student worksheet. (KHR)</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>Ice <span class="hlt">Surface</span> Temperature Variability in the Polar Regions and the Relationships to 2 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 <span class="hlt">surface</span> and near <span class="hlt">surface</span> <span class="hlt">air</span> temperature from <span class="hlt">models</span> or observations in the Polar Regions is challenging due to the extreme conditions and the lack of in situ observations. The errors in near <span class="hlt">surface</span> 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 <span class="hlt">models</span> for the relationship between the satellite observed skin ice temperatures and 2m <span class="hlt">air</span> temperatures. We use the Arctic and Antarctic Sea and sea ice <span class="hlt">Surface</span> Temperatures from thermal Infrared satellite sensors (AASTI) reanalysis to estimate daily <span class="hlt">surface</span> <span class="hlt">air</span> temperature over land ice and sea ice 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 <span class="hlt">models</span> and thus provides an important alternative to <span class="hlt">modelled</span> <span class="hlt">air</span> temperature estimates. The new <span class="hlt">surface</span> <span class="hlt">air</span> temperature data record has been validated against more than 58.000 independent in situ measurements for the four <span class="hlt">surface</span> types: Arctic sea ice, Greenland ice sheet, Antarctic sea ice and Antarctic ice sheet. The average correlations are 92-97% and average root mean square errors are 3.1-3.6°C for the four <span class="hlt">surface</span> types. The root mean square error includes the uncertainty of the in-situ measurement, which ranges from 0.5 to 2°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 ice 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 <span class="hlt">surface</span> <span class="hlt">air</span> temperature over</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.H13D1372V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.H13D1372V"><span>Numerical analysis of one-dimensional temperature data for groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> with 1DTempPro</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Voytek, E. B.; Drenkelfuss, A.; Day-Lewis, F. D.; Healy, R. W.; Lane, J. W.; Werkema, D. D.</p> <p>2012-12-01</p> <p>Temperature is a naturally occurring tracer, which can be exploited to infer the movement of water through the vadose and saturated zones, as well as the <span class="hlt">exchange</span> of water between aquifers and <span class="hlt">surface</span>-water bodies, such as estuaries, lakes, and streams. One-dimensional (1D) vertical temperature profiles commonly show thermal amplitude attenuation and increasing phase lag of diurnal or seasonal temperature variations with propagation into the subsurface. This behavior is described by the heat-transport equation (i.e., the convection-conduction-dispersion equation), which can be solved analytically in 1D under certain simplifying assumptions (e.g., sinusoidal or steady-state boundary conditions and homogeneous hydraulic and thermal properties). Analysis of 1D temperature profiles using analytical <span class="hlt">models</span> provides estimates of vertical groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span>. The utility of these estimates can be diminished when the <span class="hlt">model</span> assumptions are violated, as is common in field applications. Alternatively, analysis of 1D temperature profiles using numerical <span class="hlt">models</span> allows for consideration of more complex and realistic boundary conditions. However, such analyses commonly require <span class="hlt">model</span> calibration and the development of input files for finite-difference or finite-element codes. To address the calibration and input file requirements, a new computer program, 1DTempPro, is presented that facilitates numerical analysis of vertical 1D temperature profiles. 1DTempPro is a graphical user interface (GUI) to the USGS code VS2DH, which numerically solves the flow- and heat-transport equations. Pre- and post-processor features within 1DTempPro allow the user to calibrate VS2DH <span class="hlt">models</span> to estimate groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> and hydraulic conductivity in cases where hydraulic head is known. This approach improves groundwater/ <span class="hlt">surface</span>-water <span class="hlt">exchange</span>-rate estimates for real-world data with complexities ill-suited for examination with analytical methods. Additionally, the code</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914729D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914729D"><span>Observing mass <span class="hlt">exchange</span> with the Lofoten Basin using <span class="hlt">surface</span> drifters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dugstad, Johannes S.; LaCasce, Joe; Koszalka, Inga M.; Fer, Ilker</p> <p>2017-04-01</p> <p>The Lofoten Basin in the Nordic Seas plays a central role in the global overturning circulation, acting as a reservoir for northward-flowing Atlantic water. Substantial heat loss occurs here, permitting the waters to become denser and eventually sink nearer the Arctic. Idealized <span class="hlt">modeling</span> studies and theoretical arguments suggest the warm water enters the Lofoten Basin via eddy transport from the boundary current over the adjacent continental slope. But there is no observational evidence that this is the major contribution to mass <span class="hlt">exchange</span> between the warm Atlantic Current and the Basin. How the basin waters exit also remains a mystery. <span class="hlt">Surface</span> drifters offer an unique possibility to study the pathways of the boundary-basin <span class="hlt">exchange</span> of mass and heat. We thereby examine trajectories of <span class="hlt">surface</span> drifters released in the Nordic Seas in the POLEWARD and PROVOLO experiments, and supplemented by historical data from the Global Drifter Array. Contrary to the idea that the boundary current eddies are the main source, the results suggest that fluid is entering the Lofoten Basin from all sides. However, the drifters exit preferentially in the northeast corner of the basin. This asymmetry likely contributes to the extended residence times of the warm Atlantic waters in the Lofoten Basin. We consider various measures to quantify the effect, and test whether this is captured in a high resolution numerical <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=310516&noarchive=1&sitype=pr&fed_org_id=111','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=310516&noarchive=1&sitype=pr&fed_org_id=111"><span>“<span class="hlt">Modeling</span> Trends in <span class="hlt">Air</span> Pollutant Concentrations over the ...</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>Regional <span class="hlt">model</span> calculations over annual cycles have pointed to the need for accurately representing impacts of long-range transport. Linking regional and global scale <span class="hlt">models</span> have met with mixed success as biases in the global <span class="hlt">model</span> can propagate and influence regional calculations and often confound interpretation of <span class="hlt">model</span> results. Since transport is efficient in the free-troposphere and since simulations over Continental scales and annual cycles provide sufficient opportunity for “atmospheric turn-over”, i.e., <span class="hlt">exchange</span> between the free-troposphere and the boundary-layer, a conceptual framework is needed wherein interactions between processes occurring at various spatial and temporal scales can be consistently examined. The coupled WRF-CMAQ <span class="hlt">model</span> is expanded to hemispheric scales and <span class="hlt">model</span> simulations over period spanning 1990-current are analyzed to examine changes in hemispheric <span class="hlt">air</span> pollution resulting from changes in emissions over this period. The National Exposure Research Laboratory (NERL) Atmospheric <span class="hlt">Modeling</span> and Analysis Division (AMAD) conducts research in support of EPA mission to protect human health and the environment. AMAD research program is engaged in developing and evaluating predictive atmospheric <span class="hlt">models</span> on all spatial and temporal scales for forecasting the <span class="hlt">air</span> quality and for assessing changes in <span class="hlt">air</span> quality and <span class="hlt">air</span> pollutant exposures, as affected by changes in ecosystem management and regulatory decisions. AMAD is responsible for pr</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3403436','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3403436"><span>Protein hydrogen <span class="hlt">exchange</span>: Testing current <span class="hlt">models</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>Skinner, John J; Lim, Woon K; Bédard, Sabrina; Black, Ben E; Englander, S Walter</p> <p>2012-01-01</p> <p>To investigate the determinants of protein hydrogen <span class="hlt">exchange</span> (HX), HX rates of most of the backbone amide hydrogens of Staphylococcal nuclease were measured by NMR methods. A modified analysis was used to improve accuracy for the faster hydrogens. HX rates of both near <span class="hlt">surface</span> and well buried hydrogens are spread over more than 7 orders of magnitude. These results were compared with previous hypotheses for HX rate determination. Contrary to a common assumption, proximity to the <span class="hlt">surface</span> of the native protein does not usually produce fast <span class="hlt">exchange</span>. The slow HX rates for unprotected <span class="hlt">surface</span> hydrogens are not well explained by local electrostatic field. The ability of buried hydrogens to <span class="hlt">exchange</span> is not explained by a solvent penetration mechanism. The <span class="hlt">exchange</span> rates of structurally protected hydrogens are not well predicted by algorithms that depend only on local interactions or only on transient unfolding reactions. These observations identify some of the present difficulties of HX rate prediction and suggest the need for returning to a detailed hydrogen by hydrogen analysis to examine the bases of structure-rate relationships, as described in the companion paper (Skinner et al., Protein Sci 2012;21:996–1005). PMID:22544567</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.8177K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.8177K"><span>The boundary condition for vertical velocity and its interdependence with <span class="hlt">surface</span> gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kowalski, Andrew S.</p> <p>2017-07-01</p> <p>The law of conservation of linear momentum is applied to <span class="hlt">surface</span> gas <span class="hlt">exchanges</span>, employing scale analysis to diagnose the vertical velocity (w) in the boundary layer. Net upward momentum in the <span class="hlt">surface</span> layer is forced by evaporation (E) and defines non-zero vertical motion, with a magnitude defined by the ratio of E to the <span class="hlt">air</span> density, as w = <mstyle displaystyle="false">E/ρ</mstyle>. This is true even right down at the <span class="hlt">surface</span> where the boundary condition is w|0 = <mstyle displaystyle="false"><mfrac style="text">E/ρ|0</mfrac></mstyle> (where w|0 and ρ|0 represent the vertical velocity and density of <span class="hlt">air</span> at the <span class="hlt">surface</span>). This Stefan flow velocity implies upward transport of a non-diffusive nature that is a general feature of the troposphere but is of particular importance at the <span class="hlt">surface</span>, where it assists molecular diffusion with upward gas migration (of H2O, for example) but opposes that of downward-diffusing species like CO2 during daytime. The definition of flux-gradient relationships (eddy diffusivities) requires rectification to exclude non-diffusive transport, which does not depend on scalar gradients. At the microscopic scale, the role of non-diffusive transport in the process of evaporation from inside a narrow tube - with vapour transport into an overlying, horizontal airstream - was described long ago in classical mechanics and is routinely accounted for by chemical engineers, but has been neglected by scientists studying stomatal conductance. Correctly accounting for non-diffusive transport through stomata, which can appreciably reduce net CO2 transport and marginally boost that of water vapour, should improve characterisations of ecosystem and plant functioning.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARC37003B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARC37003B"><span>Biphilic <span class="hlt">Surfaces</span> for Enhanced Water Collection from Humid <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>Benkoski, Jason; Gerasopoulos, Konstantinos; Luedeman, William</p> <p></p> <p><span class="hlt">Surface</span> wettability plays an important role in water recovery, distillation, dehumidification, and heat transfer. The efficiency of each process depends on the rate of droplet nucleation, droplet growth, and mass transfer. Unfortunately, hydrophilic <span class="hlt">surfaces</span> are good at nucleation but poor at shedding. Hydrophobic <span class="hlt">surfaces</span> are the reverse. Many plants and animals overcome this tradeoff through biphilic <span class="hlt">surfaces</span> with patterned wettability. For example, the Stenocara beetle uses hydrophilic patches on a superhydrophobic background to collect fog from <span class="hlt">air</span>. Cribellate spiders similarly collect fog on their webs through periodic spindle-knot structures. In this study, we investigate the effects of wettability patterns on the rate of water collection from humid <span class="hlt">air</span>. The steady state rate of water collection per unit area is measured as a function of undercooling, angle of inclination, water contact angle, hydrophilic patch size, patch spacing, area fraction, and patch height relative to the hydrophobic background. We then <span class="hlt">model</span> each pattern by comparing the potential and kinetic energy of a droplet as it rolls downwards at a fixed angle. The results indicate that the design rules for collecting fog differ from those for condensation from humid <span class="hlt">air</span>. The authors gratefully acknowledge the Office of Naval Research for financial support through Grant Number N00014-15-1-2107.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1816764O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1816764O"><span>Developing multi-tracer approaches to constrain the parameterisation of leaf and soil CO2 and H2O <span class="hlt">exchange</span> in land <span class="hlt">surface</span> <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ogée, Jerome; Wehr, Richard; Commane, Roisin; Launois, Thomas; Meredith, Laura; Munger, Bill; Nelson, David; Saleska, Scott; Zahniser, Mark; Wofsy, Steve; Wingate, Lisa</p> <p>2016-04-01</p> <p>The net flux of carbon dioxide between the land <span class="hlt">surface</span> and the atmosphere is dominated by photosynthesis and soil respiration, two of the largest gross CO2 fluxes in the carbon cycle. More robust estimates of these gross fluxes could be obtained from the atmospheric budgets of other valuable tracers, such as carbonyl sulfide (COS) or the carbon and oxygen isotope compositions (δ13C and δ18O) of atmospheric CO2. Over the past decades, the global atmospheric flask network has measured the inter-annual and intra-annual variations in the concentrations of these tracers. However, knowledge gaps and a lack of high-resolution multi-tracer ecosystem-scale measurements have hindered the development of process-based <span class="hlt">models</span> that can simulate the behaviour of each tracer in response to environmental drivers. We present novel datasets of net ecosystem COS, 13CO2 and CO18O <span class="hlt">exchange</span> and vertical profile data collected over 3 consecutive growing seasons (2011-2013) at the Harvard forest flux site. We then used the process-based <span class="hlt">model</span> MuSICA (multi-layer Simulator of the Interactions between vegetation Canopy and the Atmosphere) to include the transport, reaction, diffusion and production of each tracer within the forest and <span class="hlt">exchanged</span> with the atmosphere. <span class="hlt">Model</span> simulations over the three years captured well the impact of diurnally and seasonally varying environmental conditions on the net ecosystem <span class="hlt">exchange</span> of each tracer. The <span class="hlt">model</span> also captured well the dynamic vertical features of tracer behaviour within the canopy. This unique dataset and <span class="hlt">model</span> sensitivity analysis highlights the benefit in the collection of multi-tracer high-resolution field datasets and the developement of multi-tracer land <span class="hlt">surface</span> <span class="hlt">models</span> to provide valuable constraints on photosynthesis and respiration across scales in the near future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840032418&hterms=financial+ratios&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfinancial%2Bratios','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840032418&hterms=financial+ratios&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfinancial%2Bratios"><span>Use of cooling <span class="hlt">air</span> heat <span class="hlt">exchangers</span> as replacements for hot section strategic materials</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gauntner, J. W.</p> <p>1983-01-01</p> <p>Because of financial and political constraints, strategic aerospace materials required for the hot section of future engines might be in short supply. As an alternative to these strategic materials, this study examines the use of a cooling <span class="hlt">air</span> heat <span class="hlt">exchanger</span> in combination with less advanced hot section materials. Cycle calculations are presented for future turbofan systems with overall pressure ratios to 65, bypass ratios near 13, and combustor exit temperatures to 3260 R. These calculations quantify the effect on TSFC of using a decreased materials technology in a turbofan system. The calculations show that the cooling <span class="hlt">air</span> heat <span class="hlt">exchanger</span> enables the feasibility of these engines. Previously announced in STAR as N83-34946</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BGeo...10.1379C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BGeo...10.1379C"><span>Technical Note: A simple method for <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> measurements in mesocosms and its application in carbon budgeting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Czerny, J.; Schulz, K. G.; Ludwig, A.; Riebesell, U.</p> <p>2013-03-01</p> <p>Mesocosms as large experimental units provide the opportunity to perform elemental mass balance calculations, e.g. to derive net biological turnover rates. However, the system is in most cases not closed at the water <span class="hlt">surface</span> and gases <span class="hlt">exchange</span> with the atmosphere. Previous attempts to budget carbon pools in mesocosms relied on educated guesses concerning the <span class="hlt">exchange</span> of CO2 with the atmosphere. Here, we present a simple method for precise determination of <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> in mesocosms using N2O as a deliberate tracer. Beside the application for carbon budgeting, transfer velocities can be used to calculate <span class="hlt">exchange</span> rates of any gas of known concentration, e.g. to calculate aquatic production rates of climate relevant trace gases. Using an arctic KOSMOS (Kiel Off Shore Mesocosms for future Ocean Simulation) experiment as an exemplary dataset, it is shown that the presented method improves accuracy of carbon budget estimates substantially. Methodology of manipulation, measurement, data processing and conversion to CO2 fluxes are explained. A theoretical discussion of prerequisites for precise gas <span class="hlt">exchange</span> measurements provides a guideline for the applicability of the method under various experimental conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.B32A..07K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.B32A..07K"><span>Process-based upscaling of <span class="hlt">surface</span>-atmosphere <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keenan, T. F.; Prentice, I. C.; Canadell, J.; Williams, C. A.; Wang, H.; Raupach, M. R.; Collatz, G. J.; Davis, T.; Stocker, B.; Evans, B. J.</p> <p>2015-12-01</p> <p>Empirical upscaling techniques such as machine learning and data-mining have proven invaluable tools for the global scaling of disparate observations of <span class="hlt">surface</span>-atmosphere <span class="hlt">exchange</span>, but are not based on a theoretical understanding of the key processes involved. This makes spatial and temporal extrapolation outside of the training domain difficult at best. There is therefore a clear need for the incorporation of knowledge of ecosystem function, in combination with the strength of data mining. Here, we present such an approach. We describe a novel diagnostic process-based <span class="hlt">model</span> of global photosynthesis and ecosystem respiration, which is directly informed by a variety of global datasets relevant to ecosystem state and function. We use the <span class="hlt">model</span> framework to estimate global carbon cycling both spatially and temporally, with a specific focus on the mechanisms responsible for long-term change. Our results show the importance of incorporating process knowledge into upscaling approaches, and highlight the effect of key processes on the terrestrial carbon cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4828238','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4828238"><span>The Pathway for Oxygen: Tutorial <span class="hlt">Modelling</span> on Oxygen Transport from <span class="hlt">Air</span> to Mitochondrion</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bassingthwaighte, James B.; Raymond, Gary M.; Dash, Ranjan K.; Beard, Daniel A.; Nolan, Margaret</p> <p>2016-01-01</p> <p>The ‘Pathway for Oxygen’ is captured in a set of <span class="hlt">models</span> describing quantitative relationships between fluxes and driving forces for the flux of oxygen from the external <span class="hlt">air</span> source to the mitochondrial sink at cytochrome oxidase. The intervening processes involve convection, membrane permeation, diffusion of free and heme-bound O2 and enzymatic reactions. While this system’s basic elements are simple: ventilation, alveolar gas <span class="hlt">exchange</span> with blood, circulation of the blood, perfusion of an organ, uptake by tissue, and consumption by chemical reaction, integration of these pieces quickly becomes complex. This complexity led us to construct a tutorial on the ideas and principles; these first PathwayO2 <span class="hlt">models</span> are simple but quantitative and cover: 1) a ‘one-alveolus lung’ with airway resistance, lung volume compliance, 2) bidirectional transport of solute gasses like O2 and CO2, 3) gas <span class="hlt">exchange</span> between alveolar <span class="hlt">air</span> and lung capillary blood, 4) gas solubility in blood, and circulation of blood through the capillary syncytium and back to the lung, and 5) blood-tissue gas <span class="hlt">exchange</span> in capillaries. These open-source <span class="hlt">models</span> are at Physiome.org and provide background for the many respiratory <span class="hlt">models</span> there. PMID:26782201</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23668111','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23668111"><span>[Characteristics of mercury <span class="hlt">exchange</span> flux between soil and atmosphere under the snow retention and snow melting control].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Gang; Wang, Ning; Ai, Jian-Chao; Zhang, Lei; Yang, Jing; Liu, Zi-Qi</p> <p>2013-02-01</p> <p>Jiapigou gold mine, located in the upper Songhua River, was once the largest mine in China due to gold output, where gold extraction with algamation was widely applied to extract gold resulting in severe mercury pollution to ambient environmental medium. In order to study the characteristics of mercury <span class="hlt">exchange</span> flux between soil (snow) and atmosphere under the snow retention and snow melting control, sampling sites were selected in equal distances along the slope which is situated in the typical hill-valley terrain unit. Mercury <span class="hlt">exchange</span> flux between soil (snow) and atmosphere was determined with the method of dynamic flux chamber and in all sampling sites the atmosphere concentration from 0 to 150 cm near to the earth in the vertical direction was measured. Furthermore, the impact factors including synchronous meteorology, the <span class="hlt">surface</span> characteristics under the snow retention and snow melting control and the mercury concentration in vertical direction were also investigated. The results are as follows: During the period of snow retention and melting the <span class="hlt">air</span> mercury tends to gather towards valley bottom along the slope and an obvious deposit tendency process was found from <span class="hlt">air</span> to the earth's <span class="hlt">surface</span> under the control of thermal inversion due to the underlying <span class="hlt">surface</span> of cold source (snow <span class="hlt">surface</span>). However, during the period of snow melting, mercury <span class="hlt">exchange</span> flux between the soil and atmosphere on the <span class="hlt">surface</span> of the earth with the snow being melted demonstrates alternative deposit and release processes. As for the earth with snow covered, the deposit level of mercury <span class="hlt">exchange</span> flux between soil and atmosphere is lower than that during the period of snow retention. The relationship between mercury <span class="hlt">exchange</span> flux and impact factors shows that in snow retention there is a remarkable negative linear correlation between mercury <span class="hlt">exchange</span> flux and <span class="hlt">air</span> mercury concentration as well as between the former and the <span class="hlt">air</span> temperature. In addition, in snow melting mercury <span class="hlt">exchange</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2629R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2629R"><span><span class="hlt">Air</span>- ice-snow interaction in the Northern Hemisphere under different stability conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Repina, Irina; Chechin, Dmitry; Artamonov, Arseny</p> <p>2013-04-01</p> <p>The traditional parameterizations of the atmospheric boundary layer are based on similarity theory and the coefficients of turbulent transfer, describing the atmospheric-<span class="hlt">surface</span> interaction and the diffusion of impurities in the operational <span class="hlt">models</span> of <span class="hlt">air</span> pollution, weather forecasting and climate change. Major drawbacks of these parameterizations is that they are not applicable for the extreme conditions of stratification and currents over complex <span class="hlt">surfaces</span> (such as sea ice, marginal ice zone or stormy sea). These problem could not be overcome within the framework of classical theory, i.e, by rectifying similarity functions or through the introduction of amendments to the traditional turbulent closure schemes. Lack of knowledge on the structure of the <span class="hlt">surface</span> <span class="hlt">air</span> layer and the <span class="hlt">exchange</span> of momentum, heat and moisture between the rippling water <span class="hlt">surface</span> and the atmosphere at different atmospheric stratifications is at present the major obstacle which impede proper functioning of the operational global and regional weather prediction <span class="hlt">models</span> and expert <span class="hlt">models</span> of climate and climate change. This is especially important for the polar regions, where in winter time the development of strong stable boundary layer in the presence of polynyas and leads usually occur. Experimental studies of atmosphere-ice-snow interaction under different stability conditions are presented. Strong stable and unstable conditions are discussed. Parametrizations of turbulent heat and gas <span class="hlt">exchange</span> at the atmosphere ocean interface are developed. The dependence of the <span class="hlt">exchange</span> coefficients and aerodynamic roughness on the atmospheric stratification over the snow and ice <span class="hlt">surface</span> is experimentally confirmed. The drag coefficient is reduced with increasing stability. The behavior of the roughness parameter is simple. This result was obtained in the Arctic from the measurements over hummocked <span class="hlt">surface</span>. The value of the roughness in the Arctic is much less than that observed over the snow in the middle and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1611486M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1611486M"><span>Wind variability and sheltering effects on measurements and <span class="hlt">modeling</span> of <span class="hlt">air</span>-water <span class="hlt">exchange</span> for a small lake</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Markfort, Corey D.; Resseger, Emily; Porté-Agel, Fernando; Stefan, Heinz</p> <p>2014-05-01</p> <p>Lakes with a <span class="hlt">surface</span> area of less than 10 km2 account for over 50% of the global cumulative lake <span class="hlt">surface</span> water area, and make up more than 99% of the total number of global lakes, ponds, and wetlands. Within the boreal regions as well as some temperate and tropical areas, a significant proportion of land cover is characterized by lakes or wetlands, which can have a dramatic effect on land-atmosphere fluxes as well as the local and regional energy budget. Many of these small water bodies are surrounded by complex terrain and forest, which cause the wind blowing over a small lake or wetland to be highly variable. Wind mixing of the lake <span class="hlt">surface</span> layer affects thermal stratification, <span class="hlt">surface</span> temperature and <span class="hlt">air</span>-water gas transfer, e.g. O2, CO2, and CH4. As the wind blows from the land to the lake, wake turbulence behind trees and other shoreline obstacles leads to a recirculation zone and enhanced turbulence. This wake flow results in the delay of the development of wind shear stress on the lake <span class="hlt">surface</span>, and the fetch required for <span class="hlt">surface</span> shear stress to fully develop may be ~O(1 km). Interpretation of wind measurements made on the lake is hampered by the unknown effect of wake turbulence. We present field measurements designed to quantify wind variability over a sheltered lake. The wind data and water column temperature profiles are used to evaluate a new method to quantify wind sheltering of lakes that takes into account lake size, shape and the surrounding landscape features. The <span class="hlt">model</span> is validated against field data for 36 Minnesota lakes. Effects of non-uniform sheltering and lake shape are also demonstrated. The effects of wind sheltering must be included in lake <span class="hlt">models</span> to determine the effect of wind-derived energy inputs on lake stratification, <span class="hlt">surface</span> gas transfer, lake water quality, and fish habitat. These effects are also important for correctly <span class="hlt">modeling</span> momentum, heat, moisture and trace gas flux to the atmosphere.</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://adsabs.harvard.edu/abs/2016ThEng..63..329M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ThEng..63..329M"><span>Startup of <span class="hlt">air</span>-cooled condensers and dry cooling towers at low temperatures of the cooling <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>Milman, O. O.; Ptakhin, A. V.; Kondratev, A. V.; Shifrin, B. A.; Yankov, G. G.</p> <p>2016-05-01</p> <p>The problems of startup and performance of <span class="hlt">air</span>-cooled condensers (ACC) and dry cooling towers (DCT) at low cooling <span class="hlt">air</span> temperatures are considered. Effects of the startup of the ACC at sub-zero temperatures are described. Different options of the ACC heating up are analyzed, and examples of existing technologies are presented (electric heating, heating up with hot <span class="hlt">air</span> or steam, and internal and external heating). The use of additional heat <span class="hlt">exchanging</span> sections, steam tracers, in the DCT design is described. The need for high power in cases of electric heating and heating up with hot <span class="hlt">air</span> is noted. An experimental stand for research and testing of the ACC startup at low temperatures is described. The design of the three-pass ACC unit is given, and its advantages over classical single-pass design at low temperatures are listed. The formation of ice plugs inside the heat <span class="hlt">exchanging</span> tubes during the start-up of ACC and DCT at low cooling <span class="hlt">air</span> temperatures is analyzed. Experimental data on the effect of the steam flow rate, steam nozzle distance from the heat-<span class="hlt">exchange</span> <span class="hlt">surface</span>, and their orientation in space on the metal temperature were collected, and test results are analyzed. It is noted that the <span class="hlt">surface</span> temperature at the end of the heat up is almost independent from its initial temperature. Recommendations for the safe start-up of ACCs and DCTs are given. The heating flow necessary to sufficiently heat up heat-<span class="hlt">exchange</span> <span class="hlt">surfaces</span> of ACCs and DCTs for the safe startup is estimated. The technology and the process of the heat up of the ACC with the heating steam external supply are described by the example of the startup of the full-scale section of the ACC at sub-zero temperatures of the cooling <span class="hlt">air</span>, and the advantages of the proposed start-up technology are confirmed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JPS...156..232B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JPS...156..232B"><span><span class="hlt">Modeling</span> and optimization of the <span class="hlt">air</span> system in polymer <span class="hlt">exchange</span> membrane fuel cell systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bao, Cheng; Ouyang, Minggao; Yi, Baolian</p> <p></p> <p>Stack and <span class="hlt">air</span> system are the two most important components in the fuel cell system (FCS). It is meaningful to study their properties and the trade-off between them. In this paper, a modified one-dimensional steady-state analytical fuel cell <span class="hlt">model</span> is used. The logarithmic mean of the inlet and the outlet oxygen partial pressure is adopted to avoid underestimating the effect of <span class="hlt">air</span> stoichiometry. And the pressure drop <span class="hlt">model</span> in the grid-distributed flow field is included in the stack analysis. Combined with the coordinate change preprocessing and analog technique, neural network is used to treat the MAP of compressor and turbine in the <span class="hlt">air</span> system. Three kinds of <span class="hlt">air</span> system topologies, the pure screw compressor, serial booster and exhaust expander are analyzed in this article. A real-code genetic algorithm is programmed to obtain the global optimum <span class="hlt">air</span> stoichiometric ratio and the cathode outlet pressure. It is shown that the serial booster and expander with the help of exhaust recycling, can improve more than 3% in the FCS efficiency comparing to the pure screw compressor. As the net power increases, the optimum cathode outlet pressure keeps rising and the <span class="hlt">air</span> stoichiometry takes on the concave trajectory. The working zone of the proportional valve is also discussed. This presented work is helpful to the design of the <span class="hlt">air</span> system in fuel cell system. The steady-state optimum can also be used in the dynamic control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRG..121.2216M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRG..121.2216M"><span><span class="hlt">Modeling</span> hydrological controls on variations in peat water content, water table depth, and <span class="hlt">surface</span> energy <span class="hlt">exchange</span> of a boreal western Canadian fen peatland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mezbahuddin, M.; Grant, R. F.; Flanagan, L. B.</p> <p>2016-08-01</p> <p>Improved predictive capacity of hydrology and <span class="hlt">surface</span> energy <span class="hlt">exchange</span> is critical for conserving boreal peatland carbon sequestration under drier and warmer climates. We represented basic processes for water and O2 transport and their effects on ecosystem water, energy, carbon, and nutrient cycling in a process-based <span class="hlt">model</span> ecosys to simulate effects of seasonal and interannual variations in hydrology on peat water content, water table depth (WTD), and <span class="hlt">surface</span> energy <span class="hlt">exchange</span> of a Western Canadian fen peatland. Substituting a van Genuchten <span class="hlt">model</span> (VGM) for a modified Campbell <span class="hlt">model</span> (MCM) in ecosys enabled a significantly better simulation of peat moisture retention as indicated by higher <span class="hlt">modeled</span> versus measured R2 and Willmot's index (d) with VGM (R2 0.7, d 0.8) than with MCM (R2 0.25, d 0.35) for daily peat water contents from a wetter year 2004 to a drier year 2009. With the improved peat moisture simulation, ecosys <span class="hlt">modeled</span> hourly WTD and energy fluxes reasonably well (<span class="hlt">modeled</span> versus measured R2: WTD 0.6, net radiation 0.99, sensible heat >0.8, and latent heat >0.85). Gradually declining ratios of precipitation to evapotranspiration and of lateral recharge to discharge enabled simulation of a gradual drawdown of growing season WTD and a consequent peat drying from 2004 to 2009. When WTD fell below a threshold of 0.35 m below the hollow <span class="hlt">surface</span>, intense drying of mosses in ecosys caused a simulated reduction in evapotranspiration and an increase in Bowen ratio during late growing season that were consistent with measurements. Hence, using appropriate water desorption curve coupled with vertical-lateral hydraulic schemes is vital to accurately simulate peatland hydrology and energy balance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21379833-experimental-investigation-modeling-direct-coupled-pv-air-collector','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21379833-experimental-investigation-modeling-direct-coupled-pv-air-collector"><span>Experimental investigation and <span class="hlt">modeling</span> of a direct-coupled PV/T <span class="hlt">air</span> collector</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>Shahsavar, A.; Ameri, M.; Energy and Environmental Engineering Research Center, Shahid Bahonar University, Kerman</p> <p>2010-11-15</p> <p>Photovoltaic/thermal (PV/T) systems refer to the integration of photovoltaic and solar thermal technologies into one single system, in that both useful heat energy and electricity are produced. The impetus of this paper is to <span class="hlt">model</span> a direct-coupled PV/T <span class="hlt">air</span> collector which is designed, built, and tested at a geographic location of Kerman, Iran. In this system, a thin aluminum sheet suspended at the middle of <span class="hlt">air</span> channel is used to increase the heat <span class="hlt">exchange</span> <span class="hlt">surface</span> and consequently improve heat extraction from PV panels. This PV/T system is tested in natural convection and forced convection (with two, four and eight fansmore » operating) and its unsteady results are presented in with and without glass cover cases. A theoretical <span class="hlt">model</span> is developed and validated against experimental data, where good agreement between the measured values and those calculated by the simulation <span class="hlt">model</span> were achieved. Comparisons are made between electrical performance of the different modes of operation, and it is concluded that there is an optimum number of fans for achieving maximum electrical efficiency. Also, results show that setting glass cover on photovoltaic panels leads to an increase in thermal efficiency and decrease in electrical efficiency of the system. (author)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A53F2321H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A53F2321H"><span>Indoor Levels of Formaldehyde and Other Pollutants and Relationship to <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rates and Human Activities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huangfu, Y.; O'Keeffe, P.; Kirk, M.; Walden, V. P.; Lamb, B. K.; Jobson, B. T.</p> <p>2017-12-01</p> <p>This paper reports results on an indoor <span class="hlt">air</span> quality study conducted on six homes in summer and winter, contrasting indoor and outdoor concentrations of O3, CO, CO2, NOx, PM2.5, and selected volatile organic hydrocarbons measured by PTR-MS. Data were collected as 1 minute averages. <span class="hlt">Air</span> <span class="hlt">exchange</span> rates of the homes were determined by CO2 tracer release. Smart home sensors, recording human activity level in various places in the home, and window and doors openings, were utilized to better understand the link between human activity and indoor <span class="hlt">air</span> pollution. From our study, averaged <span class="hlt">air</span> <span class="hlt">exchange</span> rates of the homes ranged from 0.2 to 1.2 hour-1 and were greatly affected by the ventilation system type and window and door openings. In general, a negative correlation between <span class="hlt">air</span> <span class="hlt">exchange</span> rate and indoor VOCs levels was observed, with large variation of pollutant levels between the homes. For most of the VOCs measured in the house, including formaldehyde and acetaldehyde, summer levels were much higher than winter levels. In some homes formaldehyde levels displayed a time of day variation that was linked to changes in indoor temperature. During a wildfire period in the summer of 2015, outdoor levels of PM2.5, formaldehyde, and benzene dramatically increased, significantly impacting indoor levels due to infiltration. Human activities, such as cooking, can significantly change the levels of most of the compounds measured in the house and the levels can be significantly elevated for short periods of time, with peak levels can be several orders higher compared with typical levels. The data suggest that an outcome of state energy codes that require new homes to be energy efficient, and as a consequence built with lower <span class="hlt">air</span> <span class="hlt">exchange</span> rates, will be unacceptable levels of <span class="hlt">air</span> toxics, notably formaldehyde.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740062566&hterms=air+contamination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dair%2Bcontamination','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740062566&hterms=air+contamination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dair%2Bcontamination"><span>Mathematical estimation of the level of microbial contamination on spacecraft <span class="hlt">surfaces</span> by volumetric <span class="hlt">air</span> sampling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oxborrow, G. S.; Roark, A. L.; Fields, N. D.; Puleo, J. R.</p> <p>1974-01-01</p> <p>Microbiological sampling methods presently used for enumeration of microorganisms on spacecraft <span class="hlt">surfaces</span> require contact with easily damaged components. Estimation of viable particles on <span class="hlt">surfaces</span> using <span class="hlt">air</span> sampling methods in conjunction with a mathematical <span class="hlt">model</span> would be desirable. Parameters necessary for the mathematical <span class="hlt">model</span> are the effect of angled <span class="hlt">surfaces</span> on viable particle collection and the number of viable cells per viable particle. Deposition of viable particles on angled <span class="hlt">surfaces</span> closely followed a cosine function, and the number of viable cells per viable particle was consistent with a Poisson distribution. Other parameters considered by the mathematical <span class="hlt">model</span> included deposition rate and fractional removal per unit time. A close nonlinear correlation between volumetric <span class="hlt">air</span> sampling and airborne fallout on <span class="hlt">surfaces</span> was established with all fallout data points falling within the 95% confidence limits as determined by the mathematical <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ThApC.105..357P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ThApC.105..357P"><span>Comparison of human radiation <span class="hlt">exchange</span> <span class="hlt">models</span> in outdoor areas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, Sookuk; Tuller, Stanton E.</p> <p>2011-10-01</p> <p>Results from the radiation components of seven different human thermal <span class="hlt">exchange</span> <span class="hlt">models</span>/methods are compared. These include the Burt, COMFA, MENEX, OUT_SET* and RayMan <span class="hlt">models</span>, the six-directional method and the new Park and Tuller <span class="hlt">model</span> employing projected area factors ( f p) and effective radiation area factors ( f eff) determined from a sample of normal- and over-weight Canadian Caucasian adults. Input data include solar and longwave radiation measured during a clear summer day in southern Ontario. Variations between <span class="hlt">models</span> came from differences in f p and f eff and different estimates of longwave radiation from the open sky. The ranges between <span class="hlt">models</span> for absorbed solar, net longwave and net all-wave radiation were 164, 31 and 187 W m-2, respectively. These differentials between <span class="hlt">models</span> can be significant in total human thermal <span class="hlt">exchange</span>. Therefore, proper f p and f eff values should be used to make accurate estimation of radiation on the human body <span class="hlt">surface</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PrOce.109..104C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PrOce.109..104C"><span>Sea <span class="hlt">surface</span> microlayers: A unified physicochemical and biological perspective of the <span class="hlt">air</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>Cunliffe, Michael; Engel, Anja; Frka, Sanja; Gašparović, Blaženka; Guitart, Carlos; Murrell, J. Colin; Salter, Matthew; Stolle, Christian; Upstill-Goddard, Robert; Wurl, Oliver</p> <p>2013-02-01</p> <p>The sea <span class="hlt">surface</span> microlayer (SML) covers more than 70% of the Earth's <span class="hlt">surface</span> and is the boundary layer interface between the ocean and the atmosphere. This important biogeochemical and ecological system is critical to a diverse range of Earth system processes, including the synthesis, transformation and cycling of organic material, and the <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of gases, particles and aerosols. In this review we discuss the SML paradigm, taking into account physicochemical and biological characteristics that define SML structure and function. These include enrichments in biogenic molecules such as carbohydrates, lipids and proteinaceous material that contribute to organic carbon cycling, distinct microbial assemblages that participate in <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>, the generation of climate-active aerosols and the accumulation of anthropogenic pollutants with potentially serious implications for the health of the ocean. Characteristically large physical, chemical and biological gradients thus separate the SML from the underlying water and the available evidence implies that the SML retains its integrity over wide ranging environmental conditions. In support of this we present previously unpublished time series data on bacterioneuston composition and SML surfactant activity immediately following physical SML disruption; these imply timescales of the order of minutes for the reestablishment of the SML following disruption. A progressive approach to understanding the SML and hence its role in global biogeochemistry can only be achieved by considering as an integrated whole, all the key components of this complex environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110000601','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110000601"><span><span class="hlt">Air</span> Circulation and Heat <span class="hlt">Exchange</span> Under Reduced Pressures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rygalov, V.; Wheeler, R.; Dixon, M.; Fowler, P.; Hillhouse, L.</p> <p>2010-01-01</p> <p>Heat <span class="hlt">exchange</span> rates decrease non-linearly with reductions in atmospheric pressure. This decrease creates risk of thermal stress (elevated leaf temperatures) for plants under reduced pressures. Forced convection (fans) significantly increases heat <span class="hlt">exchange</span> rate under almost all pressures except below 10 kPa. Plant cultivation techniques under reduced pressures will require forced convection. The cooling curve technique is a reliable means of assessing the influence of environmental variables like pressure and gravity on gas <span class="hlt">exchange</span> of plant. These results represent the extremes of gas <span class="hlt">exchange</span> conditions for simple systems under variable pressures. In reality, dense plant canopies will exhibit responses in between these extremes. More research is needed to understand the dependence of forced convection on atmospheric pressure. The overall thermal balance <span class="hlt">model</span> should include latent and radiative <span class="hlt">exchange</span> components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914688S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914688S"><span>Explicit <span class="hlt">modeling</span> of groundwater-<span class="hlt">surface</span> water interactions using a simple bucket-type <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Staudinger, Maria; Carlier, Claire; Brunner, Philip; Seibert, Jan</p> <p>2017-04-01</p> <p>Longer dry spells can become critical for water supply and groundwater dependent ecosystems. During these dry spells groundwater is often the most relevant source for streams. Hence, the hydrological behavior of a catchment is often dominated by groundwater <span class="hlt">surface</span> water interactions, which can vary considerably in space and time. While classical hydrological approaches hardly consider this spatial dependence, quantitative, hydrogeological <span class="hlt">modeling</span> approaches can couple <span class="hlt">surface</span> runoff processes and groundwater processes. Hydrogeological <span class="hlt">modeling</span> can help to gain an improved understanding of catchment processes during low flow. However, due to their complex parametrization and large computational requirements, such hydrogeological <span class="hlt">models</span> are difficult to employ at catchment scale, particularly for a larger set of catchments. Then bucket-type hydrological <span class="hlt">models</span> remain a practical alternative. In this study we combine the strengths of both the hydrogeological and bucket-type hydrological <span class="hlt">models</span> to better understand low flow processes and ultimately to use this knowledge for low flow projections. Bucket-type hydrological <span class="hlt">models</span> have traditionally not been developed with focus on the simulation of low flow. One consequence is that interactions between <span class="hlt">surface</span> and groundwater are not explicitly considered. Water fluxes in bucket-type hydrological <span class="hlt">models</span> are commonly simulated only in one direction, namely from the groundwater to the stream but not from the stream to the groundwater. This latter flux, however, can become more important during low flow situations. We therefore further developed the bucket-type hydrological <span class="hlt">model</span> HBV to simulate low flow situations by allowing for <span class="hlt">exchange</span> in both directions i.e. also from the stream to the groundwater. The additional HBV <span class="hlt">exchange</span> box is developed by using a variety of synthetic hydrogeological <span class="hlt">models</span> as training set that were generated using a fully coupled, physically based hydrogeological <span class="hlt">model</span>. In this way processes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.H51K0756H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.H51K0756H"><span>Uncertainty quantification of <span class="hlt">surface</span>-water/groundwater <span class="hlt">exchange</span> estimates in large wetland systems using Python</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hughes, J. D.; Metz, P. A.</p> <p>2014-12-01</p> <p>Most watershed studies include observation-based water budget analyses to develop first-order estimates of significant flow terms. <span class="hlt">Surface</span>-water/groundwater (SWGW) <span class="hlt">exchange</span> is typically assumed to be equal to the residual of the sum of inflows and outflows in a watershed. These estimates of SWGW <span class="hlt">exchange</span>, however, are highly uncertain as a result of the propagation of uncertainty inherent in the calculation or processing of the other terms of the water budget, such as stage-area-volume relations, and uncertainties associated with land-cover based evapotranspiration (ET) rate estimates. Furthermore, the uncertainty of estimated SWGW <span class="hlt">exchanges</span> can be magnified in large wetland systems that transition from dry to wet during wet periods. Although it is well understood that observation-based estimates of SWGW <span class="hlt">exchange</span> are uncertain it is uncommon for the uncertainty of these estimates to be directly quantified. High-level programming languages like Python can greatly reduce the effort required to (1) quantify the uncertainty of estimated SWGW <span class="hlt">exchange</span> in large wetland systems and (2) evaluate how different approaches for partitioning land-cover data in a watershed may affect the water-budget uncertainty. We have used Python with the Numpy, Scipy.stats, and pyDOE packages to implement an unconstrained Monte Carlo approach with Latin Hypercube sampling to quantify the uncertainty of monthly estimates of SWGW <span class="hlt">exchange</span> in the Floral City watershed of the Tsala Apopka wetland system in west-central Florida, USA. Possible sources of uncertainty in the water budget analysis include rainfall, ET, canal discharge, and land/bathymetric <span class="hlt">surface</span> elevations. Each of these input variables was assigned a probability distribution based on observation error or spanning the range of probable values. The Monte Carlo integration process exposes the uncertainties in land-cover based ET rate estimates as the dominant contributor to the uncertainty in SWGW <span class="hlt">exchange</span> estimates. We will discuss</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C13A0809M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C13A0809M"><span><span class="hlt">Modeling</span> of multi-phase interactions of reactive nitrogen between snow and <span class="hlt">air</span> in Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McCrystall, M.; Chan, H. G. V.; Frey, M. M.; King, M. D.</p> <p>2016-12-01</p> <p>In polar and snow-covered regions, the snowpack is an important link between atmospheric, terrestrial and oceanic systems. Trace gases, including nitrogen oxides, produced via photochemical reactions in snow are partially released to the lower atmosphere with considerable impact on its composition. However, the post-depositional processes that change the chemical composition and physical properties of the snowpack are still poorly understood. Most current snow chemistry <span class="hlt">models</span> oversimplify as they assume <span class="hlt">air</span>-liquid interactions and aqueous phase chemistry taking place at the interface between the snow grain and <span class="hlt">air</span>. Here, we develop a novel temperature dependent multi-phase (gas-liquid-ice) physical <span class="hlt">exchange</span> <span class="hlt">model</span> for reactive nitrogen. The <span class="hlt">model</span> is validated with existing year-round observations of nitrate in the top 0.5-2 cm of snow and the overlying atmosphere at two very different Antarctic locations: Dome C on the East Antarctic Plateau with very low annual mean temperature (-54ºC) and accumulation rate (<30 kg m-2 yr-1); and Halley, a coastal site with at times at or above freezing temperatures during summer, high accumulation rate and high background level of sea salt aerosol. We find that below the eutectic temperature of the H2O/dominant ion mixture the <span class="hlt">surface</span> snow nitrate is controlled by kinetic adsorption onto the <span class="hlt">surface</span> of snow grains followed by grain diffusion. Above the eutectic temperature, in addition to the former two processes, thermodynamic equilibrium of HNO3 between interstitial <span class="hlt">air</span> and liquid water pockets, possibly present at triple junctions or grooves at grain boundaries, greatly enhances the nitrate uptake by snow in agreement with the concentration peak observed in summer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GBioC..31..901E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GBioC..31..901E"><span>Impacts of ENSO on <span class="hlt">air</span>-sea oxygen <span class="hlt">exchange</span>: Observations and mechanisms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eddebbar, Yassir A.; Long, Matthew C.; Resplandy, Laure; Rödenbeck, Christian; Rodgers, Keith B.; Manizza, Manfredi; Keeling, Ralph F.</p> <p>2017-05-01</p> <p><span class="hlt">Models</span> and observations of atmospheric potential oxygen (APO ≃ O2 + 1.1 * CO2) are used to investigate the influence of El Niño-Southern Oscillation (ENSO) on <span class="hlt">air</span>-sea O2 <span class="hlt">exchange</span>. An atmospheric transport inversion of APO data from the Scripps flask network shows significant interannual variability in tropical APO fluxes that is positively correlated with the Niño3.4 index, indicating anomalous ocean outgassing of APO during El Niño. Hindcast simulations of the Community Earth System <span class="hlt">Model</span> (CESM) and the Institut Pierre-Simon Laplace <span class="hlt">model</span> show similar APO sensitivity to ENSO, differing from the Geophysical Fluid Dynamics Laboratory <span class="hlt">model</span>, which shows an opposite APO response. In all <span class="hlt">models</span>, O2 accounts for most APO flux variations. Detailed analysis in CESM shows that the O2 response is driven primarily by ENSO modulation of the source and rate of equatorial upwelling, which moderates the intensity of O2 uptake due to vertical transport of low-O2 waters. These upwelling changes dominate over counteracting effects of biological productivity and thermally driven O2 <span class="hlt">exchange</span>. During El Niño, shallower and weaker upwelling leads to anomalous O2 outgassing, whereas deeper and intensified upwelling during La Niña drives enhanced O2 uptake. This response is strongly localized along the central and eastern equatorial Pacific, leading to an equatorial zonal dipole in atmospheric anomalies of APO. This dipole is further intensified by ENSO-related changes in winds, reconciling apparently conflicting APO observations in the tropical Pacific. These findings suggest a substantial and complex response of the oceanic O2 cycle to climate variability that is significantly (>50%) underestimated in magnitude by ocean <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvB..85k5124Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvB..85k5124Q"><span>Asymptotic behavior of the Kohn-Sham <span class="hlt">exchange</span> potential at a metal <span class="hlt">surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qian, Zhixin</p> <p>2012-03-01</p> <p>The asymptotic structure of the Kohn-Sham <span class="hlt">exchange</span> potential vx(r) in the classically forbidden region of a metal <span class="hlt">surface</span> is investigated, together with that of the Slater <span class="hlt">exchange</span> potential VxS(r) and those of the approximate Krieger-Li-Iafrate VxKLI(r) and Harbola-Sahni Wx(r) <span class="hlt">exchange</span> potentials. Particularly, the former is shown to have the form of vx(z→∞)=-αx/z with αx a constant dependent only of bulk electron density. The same result in previous work is thus confirmed; in the meanwhile, a controversy raised recently gets resolved. The structure of the <span class="hlt">exchange</span> hole ρx(r,r') is examined, and the delocalization of it in the metal bulk when the electron is at large distance from the metal <span class="hlt">surface</span> is demonstrated with analytical expressions. The asymptotic structures of vx(r), VxS(r), VxKLI(r), and Wx(r) at a slab metal <span class="hlt">surface</span> are also investigated. Particularly, vx(z→∞)=-1/z in the slab case. The distinction, in this respect, between the semi-infinite and the slab metal <span class="hlt">surfaces</span> is elucidated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863488','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863488"><span>Fluidized bed heat <span class="hlt">exchanger</span> utilizing angularly extending heat <span class="hlt">exchange</span> tubes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Talmud, Fred M.; Garcia-Mallol, Juan-Antonio</p> <p>1980-01-01</p> <p>A fluidized bed heat <span class="hlt">exchanger</span> in which <span class="hlt">air</span> is passed through a bed of particulate material containing fuel disposed in a housing. A steam/water natural circulation system is provided and includes a steam drum disposed adjacent the fluidized bed and a series of tubes connected at one end to the steam drum. A portion of the tubes are connected to a water drum and in the path of the <span class="hlt">air</span> and the gaseous products of combustion exiting from the bed. Another portion of the tubes pass through the bed and extend at an angle to the upper <span class="hlt">surface</span> of the bed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=310793&keyword=ammonia&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=310793&keyword=ammonia&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><span class="hlt">Modelling</span> the Air–<span class="hlt">Surface</span> <span class="hlt">Exchange</span> of Ammonia from the Field to Global Scale</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>The Working Group addressed the current understanding and uncertainties in the processes controlling ammonia (NH3) bi-directional <span class="hlt">exchange</span>, and in the application of numerical <span class="hlt">models</span> to describe these processes. As a starting point for the discussion, the Working Group drew on th...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..442..461L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..442..461L"><span>Fabrication of a superhydrophobic <span class="hlt">surface</span> with fungus-cleaning properties on brazed aluminum for industrial application in heat <span class="hlt">exchangers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Jeong-Won; Hwang, Woonbong</p> <p>2018-06-01</p> <p>Extensive research has been carried out concerning the application of superhydrophobic coating in heat <span class="hlt">exchangers</span>, but little is known about the application of this technique to brazed aluminum heat <span class="hlt">exchangers</span> (BAHEs). In this work, we describe a new superhydrophobic coating method, which is suitable for BAHE use on an industrial scale. We first render the BAHE superhydrophobic by fabricating micro/nanostructures using solution dipping followed by fluorination. After the complete removal of the silicon residue, we verify using <span class="hlt">surface</span> analysis that the BAHE <span class="hlt">surface</span> is perfectly superhydrophobic. We also studied the fungus-cleaning properties of the superhydrophobic <span class="hlt">surface</span> by growing fungus for 4 weeks in a moist environment on BAHE fins with and without superhydrophobic coating. We observed that, whereas the fungus grown on the untreated fins is extremely difficult to remove, the fungus on the fins with the superhydrophobic coating can be removed easily with only a modest amount of water. We also found that the coated BAHE fins exhibit excellent resistance to moisture. The superhydrophobic coating method that we propose is therefore expected to have a major impact in the heating, ventilating and <span class="hlt">air</span> conditioning industry market.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870014174','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870014174"><span>Development of an <span class="hlt">air</span> ground data <span class="hlt">exchange</span> concept: Flight deck perspective</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flathers, G. W., II</p> <p>1987-01-01</p> <p>The planned modernization of the U.S. National Airspace System (NAS) includes the development and use of a digital data link as a means to <span class="hlt">exchange</span> information between aircraft and ground-based facilities. This report presents an operationally-oriented concept on how data link could be used for applications related directly to <span class="hlt">air</span> traffic control. The specific goal is to establish the role that data link could play in the <span class="hlt">air</span>-ground communications. Due regard is given to the unique characteristics of data link and voice communications, current principles of <span class="hlt">air</span> traffic control, operational procedures, human factors/man-machine interfaces, and the integration of data link with other <span class="hlt">air</span> and ground systems. The resulting concept is illustrated in the form of a paper-and-pencil simulation in which data link and voice communications during the course of a hypothetical flight are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=59576&keyword=film+AND+analysis&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=59576&keyword=film+AND+analysis&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>THE ROLE OF AQUEOUS THIN FILM EVAPORATIVE COOLING ON RATES OF ELEMENTAL MERCURY <span class="hlt">AIR</span>-WATER <span class="hlt">EXCHANGE</span> UNDER TEMPERATURE DISEQUILIBRIUM CONDITIONS</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>The technical conununity has only recently addressed the role of atmospheric temperature variations on rates of <span class="hlt">air</span>-water vapor phase toxicant <span class="hlt">exchange</span>. The technical literature has documented that: 1) day time rates of elemental mercury vapor phase <span class="hlt">air</span>-water <span class="hlt">exchange</span> can exceed ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3720057','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3720057"><span>Pan-Arctic <span class="hlt">modelling</span> of net ecosystem <span class="hlt">exchange</span> of CO2</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shaver, G. R.; Rastetter, E. B.; Salmon, V.; Street, L. E.; van de Weg, M. J.; Rocha, A.; van Wijk, M. T.; Williams, M.</p> <p>2013-01-01</p> <p>Net ecosystem <span class="hlt">exchange</span> (NEE) of C varies greatly among Arctic ecosystems. Here, we show that approximately 75 per cent of this variation can be accounted for in a single regression <span class="hlt">model</span> that predicts NEE as a function of leaf area index (LAI), <span class="hlt">air</span> temperature and photosynthetically active radiation (PAR). The <span class="hlt">model</span> was developed in concert with a survey of the light response of NEE in Arctic and subarctic tundras in Alaska, Greenland, Svalbard and Sweden. <span class="hlt">Model</span> parametrizations based on data collected in one part of the Arctic can be used to predict NEE in other parts of the Arctic with accuracy similar to that of predictions based on data collected in the same site where NEE is predicted. The principal requirement for the dataset is that it should contain a sufficiently wide range of measurements of NEE at both high and low values of LAI, <span class="hlt">air</span> temperature and PAR, to properly constrain the estimates of <span class="hlt">model</span> parameters. Canopy N content can also be substituted for leaf area in predicting NEE, with equal or greater accuracy, but substitution of soil temperature for <span class="hlt">air</span> temperature does not improve predictions. Overall, the results suggest a remarkable convergence in regulation of NEE in diverse ecosystem types throughout the Arctic. PMID:23836790</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3046576','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3046576"><span>A Three-Dimensional Multiscale <span class="hlt">Model</span> for Gas <span class="hlt">Exchange</span> in Fruit1[C][W][OA</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ho, Quang Tri; Verboven, Pieter; Verlinden, Bert E.; Herremans, Els; Wevers, Martine; Carmeliet, Jan; Nicolaï, Bart M.</p> <p>2011-01-01</p> <p>Respiration of bulky plant organs such as roots, tubers, stems, seeds, and fruit depends very much on oxygen (O2) availability and often follows a Michaelis-Menten-like response. A multiscale <span class="hlt">model</span> is presented to calculate gas <span class="hlt">exchange</span> in plants using the microscale geometry of the tissue, or vice versa, local concentrations in the cells from macroscopic gas concentration profiles. This approach provides a computationally feasible and accurate analysis of cell metabolism in any plant organ during hypoxia and anoxia. The predicted O2 and carbon dioxide (CO2) partial pressure profiles compared very well with experimental data, thereby validating the multiscale <span class="hlt">model</span>. The important microscale geometrical features are the shape, size, and three-dimensional connectivity of cells and <span class="hlt">air</span> spaces. It was demonstrated that the gas-<span class="hlt">exchange</span> properties of the cell wall and cell membrane have little effect on the cellular gas <span class="hlt">exchange</span> of apple (Malus × domestica) parenchyma tissue. The analysis clearly confirmed that cells are an additional route for CO2 transport, while for O2 the intercellular spaces are the main diffusion route. The simulation results also showed that the local gas concentration gradients were steeper in the cells than in the surrounding <span class="hlt">air</span> spaces. Therefore, to analyze the cellular metabolism under hypoxic and anoxic conditions, the microscale <span class="hlt">model</span> is required to calculate the correct intracellular concentrations. Understanding the O2 response of plants and plant organs thus not only requires knowledge of external conditions, dimensions, gas-<span class="hlt">exchange</span> properties of the tissues, and cellular respiration kinetics but also of microstructure. PMID:21224337</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GeoRL..40.5683H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeoRL..40.5683H"><span>Efficient gas <span class="hlt">exchange</span> between a boreal river and the atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huotari, Jussi; Haapanala, Sami; Pumpanen, Jukka; Vesala, Timo; Ojala, Anne</p> <p>2013-11-01</p> <p>largest uncertainties in accurately resolving the role of rivers and streams in carbon cycling stem from difficulties in determining gas <span class="hlt">exchange</span> between water and the atmosphere. So far, estimates for river-atmosphere gas <span class="hlt">exchange</span> have lacked direct ecosystem-scale flux measurements not disturbing gas <span class="hlt">exchange</span> across the <span class="hlt">air</span>-water interface. We conducted the first direct riverine gas <span class="hlt">exchange</span> measurements with eddy covariance in tandem with continuous <span class="hlt">surface</span> water CO2 measurements in a large boreal river for 30 days. Our measured gas transfer velocity was, on average, 20.8 cm h-1, which is clearly higher than the <span class="hlt">model</span> estimates based on river channel morphology and water velocity, whereas our floating chambers gave comparable values at 17.3 cm h-1. These results demonstrate that present estimates for riverine CO2 emissions are very likely too low. This result is also relevant to any other gases emitted, as their diffusive <span class="hlt">exchange</span> rates are similarly proportional to gas transfer velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRC..123..514M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRC..123..514M"><span><span class="hlt">Surface</span> Connectivity and Interocean <span class="hlt">Exchanges</span> From Drifter-Based Transition Matrices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McAdam, Ronan; van Sebille, Erik</p> <p>2018-01-01</p> <p>Global <span class="hlt">surface</span> transport in the ocean can be represented by using the observed trajectories of drifters to calculate probability distribution functions. The oceanographic applications of the Markov Chain approach to <span class="hlt">modeling</span> include tracking of floating debris and water masses, globally and on yearly-to-centennial time scales. Here we analyze the error inherent with mapping trajectories onto a grid and the consequences for ocean transport <span class="hlt">modeling</span> and detection of accumulation structures. A sensitivity analysis of Markov Chain parameters is performed in an idealized Stommel gyre and western boundary current as well as with observed ocean drifters, complementing previous studies on widespread floating debris accumulation. Focusing on two key areas of interocean exchange—the Agulhas system and the North Atlantic intergyre transport barrier—we assess the capacity of the Markov Chain methodology to detect <span class="hlt">surface</span> connectivity and dynamic transport barriers. Finally, we extend the methodology's functionality to separate the geostrophic and nongeostrophic contributions to interocean <span class="hlt">exchange</span> in these key regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993AtmEn..27.2085W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993AtmEn..27.2085W"><span>A continuous-flow denuder for the measurement of ambient concentrations and <span class="hlt">surface-exchange</span> fluxes of ammonia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wyers, G. P.; Otjes, R. P.; Slanina, J.</p> <p></p> <p>A new diffusion denuder is described for the continuous measurement of atmospheric ammonia. Ammonia is collected in an absorption solution in a rotating denuder, separated from interfering compounds by diffusion through a semi-permeable membrane and detected by conductometry. The method is free from interferences by other atmospheric gases, with the exception of volatile amines. The detection limit is 6 ng m -3 for a 30-min integration time. This compact instrument is fully automated and suited for routine deployment in field studies. The precision is sufficiently high for micrometeorological studies of <span class="hlt">air-surface</span> <span class="hlt">exchange</span> of ammonia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1416730','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1416730"><span>Group IV nanocrystals with ion-<span class="hlt">exchangeable</span> <span class="hlt">surface</span> ligands and methods of making the same</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>Wheeler, Lance M.; Nichols, Asa W.; Chernomordik, Boris D.</p> <p></p> <p>Methods are described that include reacting a starting nanocrystal that includes a starting nanocrystal core and a covalently bound <span class="hlt">surface</span> species to create an ion-<span class="hlt">exchangeable</span> (IE) nanocrystal that includes a <span class="hlt">surface</span> charge and a first ion-<span class="hlt">exchangeable</span> (IE) <span class="hlt">surface</span> ligand ionically bound to the <span class="hlt">surface</span> charge, where the starting nanocrystal core includes a group IV element.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1015c2072S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1015c2072S"><span><span class="hlt">Modeling</span> of Hydrate Formation Mode in Raw Natural Gas <span class="hlt">Air</span> Coolers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scherbinin, S. V.; Prakhova, M. Yu; Krasnov, A. N.; Khoroshavina, E. A.</p> <p>2018-05-01</p> <p><span class="hlt">Air</span> cooling units (ACU) are used at all the gas fields for cooling natural gas after compressing. When using ACUs on raw (wet) gas in a low temperature condition, there is a danger of hydrate plug formation in the heat <span class="hlt">exchanging</span> tubes of the ACU. To predict possible hydrate formation, a mathematical <span class="hlt">model</span> of the <span class="hlt">air</span> cooler thermal behavior used in the control system shall adequately calculate not only gas temperature at the cooler's outlet, but also a dew point value, a temperature at which condensation, as well as the gas hydrate formation point, onsets. This paper proposes a mathematical <span class="hlt">model</span> allowing one to determine the pressure in the <span class="hlt">air</span> cooler which makes hydrate formation for a given gas composition possible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol8/pdf/CFR-2013-title29-vol8-sec1926-1085.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol8/pdf/CFR-2013-title29-vol8-sec1926-1085.pdf"><span>29 CFR 1926.1085 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 29 Labor 8 2013-07-01 2013-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1926.1085 Section 1926.1085 Labor Regulations Relating to Labor (Continued) OCCUPATIONAL SAFETY AND HEALTH ADMINISTRATION... Procedures § 1926.1085 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. Note: The requirements applicable to construction work...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol8/pdf/CFR-2010-title29-vol8-sec1926-1085.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol8/pdf/CFR-2010-title29-vol8-sec1926-1085.pdf"><span>29 CFR 1926.1085 - <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 29 Labor 8 2010-07-01 2010-07-01 false <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. 1926.1085 Section 1926.1085 Labor Regulations Relating to Labor (Continued) OCCUPATIONAL SAFETY AND HEALTH ADMINISTRATION... Procedures § 1926.1085 <span class="hlt">Surface</span>-supplied <span class="hlt">air</span> diving. Note: The requirements applicable to construction work...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22103582','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22103582"><span>Distribution and <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of current-use pesticides (CUPs) from East Asia to the high Arctic Ocean.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhong, Guangcai; Xie, Zhiyong; Cai, Minghong; Möller, Axel; Sturm, Renate; Tang, Jianhui; Zhang, Gan; He, Jianfeng; Ebinghaus, Ralf</p> <p>2012-01-03</p> <p><span class="hlt">Surface</span> seawater and marine boundary layer <span class="hlt">air</span> samples were collected on the ice-breaker R/V Xuelong (Snow Dragon) from the East China Sea to the high Arctic (33.23-84.5° N) in July to September 2010 and have been analyzed for six current-use pesticides (CUPs): trifluralin, endosulfan, chlorothalonil, chlorpyrifos, dacthal, and dicofol. In all oceanic <span class="hlt">air</span> samples, the six CUPs were detected, showing highest level (>100 pg/m(3)) in the Sea of Japan. Gaseous CUPs basically decreased from East Asia (between 36.6 and 45.1° N) toward Bering and Chukchi Seas. The dissolved CUPs in ocean water ranged widely from <MDL to 111 pg/L. Latitudinal trends of α-endosulfan, chlorpyrifos, and dicofol in seawater were roughly consistent with their latitudinal trends in <span class="hlt">air</span>. Trifluralin in seawater was relatively high in the Sea of Japan (35.2° N) and evenly distributed between 36.9 and 72.5° N, but it remained below the detection limit at the highest northern latitudes in Chukchi Sea. In contrast with other CUPs, concentrations of chlorothalonil and dacthal were more abundant in Chukchi Sea and in East Asia. The <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> of CUPs was generally dominated by net deposition. Latitudinal trends of fugacity ratios of α-endosulfan, chlorothalonil, and dacthal showed stronger deposition of these compounds in East Asia than in Chukchi Sea, while trifluralin showed stronger deposition in Chukchi Sea (-455 ± 245 pg/m(2)/day) than in the North Pacific (-241 ± 158 pg/m(2)/day). <span class="hlt">Air</span>-sea gas <span class="hlt">exchange</span> of chlorpyrifos varied from net volatilizaiton in East Asia (<40° N) to equilibrium or net deposition in the North Pacific and the Arctic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995JCli....8.1360G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995JCli....8.1360G"><span>Observed Screen (<span class="hlt">Air</span>) and GCM <span class="hlt">Surface</span>/Screen Temperatures: Implications for Outgoing Longwave Fluxes at the <span class="hlt">Surface</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garratt, J. R.</p> <p>1995-05-01</p> <p>There is direct evidence that excess net radiation calculated in general circulation <span class="hlt">models</span> at continental <span class="hlt">surfaces</span> [of about 11-17 W m2 (20%-27%) on an annual ~1 is not only due to overestimates in annual incoming shortwave fluxes [of 9-18 W m2 (6%-9%)], but also to underestimates in outgoing longwave fluxes. The bias in the outgoing longwave flux is deduced from a comparison of screen-<span class="hlt">air</span> temperature observations, available as a global climatology of mean monthly values, and <span class="hlt">model</span>-calculated <span class="hlt">surface</span> and screen-<span class="hlt">air</span> temperatures. An underestimate in the screen temperature computed in general circulation <span class="hlt">models</span> over continents, of about 3 K on an annual basis, implies an underestimate in the outgoing longwave flux, averaged in six <span class="hlt">models</span> under study, of 11-15 W m2 (3%-4%). For a set of 22 inland stations studied previously, the residual bias on an annual basis (the residual is the net radiation minus incoming shortwave plus outgoing longwave) varies between 18 and 23 W m2 for the <span class="hlt">models</span> considered. Additional biases in one or both of the reflected shortwave and incoming longwave components cannot be ruled out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28675854','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28675854"><span><span class="hlt">Air</span>-sea <span class="hlt">exchange</span> and gas-particle partitioning of polycyclic aromatic hydrocarbons over the northwestern Pacific Ocean: Role of East Asian continental outflow.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Zilan; Lin, Tian; Li, Zhongxia; Jiang, Yuqing; Li, Yuanyuan; Yao, Xiaohong; Gao, Huiwang; Guo, Zhigang</p> <p>2017-11-01</p> <p>We measured 15 parent polycyclic aromatic hydrocarbons (PAHs) in atmosphere and water during a research cruise from the East China Sea (ECS) to the northwestern Pacific Ocean (NWP) in the spring of 2015 to investigate the occurrence, <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>, and gas-particle partitioning of PAHs with a particular focus on the influence of East Asian continental outflow. The gaseous PAH composition and identification of sources were consistent with PAHs from the upwind area, indicating that the gaseous PAHs (three-to five-ring PAHs) were influenced by upwind land pollution. In addition, <span class="hlt">air</span>-sea <span class="hlt">exchange</span> fluxes of gaseous PAHs were estimated to be -54.2-107.4 ng m -2 d -1 , and was indicative of variations of land-based PAH inputs. The logarithmic gas-particle partition coefficient (logK p ) of PAHs regressed linearly against the logarithmic subcooled liquid vapor pressure (logP L 0 ), with a slope of -0.25. This was significantly larger than the theoretical value (-1), implying disequilibrium between the gaseous and particulate PAHs over the NWP. The non-equilibrium of PAH gas-particle partitioning was shielded from the volatilization of three-ring gaseous PAHs from seawater and lower soot concentrations in particular when the oceanic <span class="hlt">air</span> masses prevailed. <span class="hlt">Modeling</span> PAH absorption into organic matter and adsorption onto soot carbon revealed that the status of PAH gas-particle partitioning deviated more from the <span class="hlt">modeling</span> K p for oceanic <span class="hlt">air</span> masses than those for continental <span class="hlt">air</span> masses, which coincided with higher volatilization of three-ring PAHs and confirmed the influence of <span class="hlt">air</span>-sea <span class="hlt">exchange</span>. Meanwhile, significant linear regressions between logK p and logK oa (logK sa ) for PAHs were observed for continental <span class="hlt">air</span> masses, suggesting the dominant effect of East Asian continental outflow on atmospheric PAHs over the NWP during the sampling campaign. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApSS..410..117G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApSS..410..117G"><span>A study on <span class="hlt">air</span> bubble wetting: Role of <span class="hlt">surface</span> wettability, <span class="hlt">surface</span> tension, and ionic surfactants</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>George, Jijo Easo; Chidangil, Santhosh; George, Sajan D.</p> <p>2017-07-01</p> <p>Fabrication of hydrophobic/hydrophilic <span class="hlt">surfaces</span> by biomimicking nature has attracted significant attention recently due to their potential usage in technologies, ranging from self-cleaning to DNA condensation. Despite the potential applications, compared to <span class="hlt">surfaces</span> of tailored wettability, less attention has been paid towards development and understanding of <span class="hlt">air</span> bubble adhesion and its dynamics on <span class="hlt">surfaces</span> with varying wettability. In this manuscript, following the commonly used approach of oxygen plasma treatment, polydimethylsiloxane <span class="hlt">surfaces</span> with tunable wettability are prepared. The role of plasma treatment conditions on the <span class="hlt">surface</span> hydrophilicity and the consequent effect on adhesion dynamics of an underwater <span class="hlt">air</span> bubble is explored for the first time. The ATR-FTIR spectroscopic analysis reveals that the change in hydrophilicity arises from the chemical modification of the <span class="hlt">surface</span>, manifested as Si-OH vibrations in the spectra. The thickness of the formed thin liquid film at the <span class="hlt">surface</span> responsible for the experimentally observed <span class="hlt">air</span> bubble repellency is estimated from the augmented Young-Laplace equation. The concentration dependent studies using cationic as well as anionic surfactant elucidate that the reduced <span class="hlt">surface</span> tension of the aqueous solution results in a stable thicker film and causes non-adherence of <span class="hlt">air</span> bubble to the aerophilic <span class="hlt">surface</span>. Furthermore, the study carried out to understand the combined effect of plasma treatment and surfactants reveals that even below critical micelle concentration, a negatively charged <span class="hlt">surface</span> results in <span class="hlt">air</span> bubble repellency for the anionic surfactant, whereas only enhanced <span class="hlt">air</span> bubble contact angle is observed for the cationic surfactant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002JGRC..107.3196S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002JGRC..107.3196S"><span>An Oceanic General Circulation <span class="hlt">Model</span> (OGCM) investigation of the Red Sea circulation, 1. <span class="hlt">Exchange</span> between the Red Sea and the Indian Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sofianos, Sarantis S.; Johns, William E.</p> <p>2002-11-01</p> <p>The mechanisms involved in the seasonal <span class="hlt">exchange</span> between the Red Sea and the Indian Ocean are studied using an Oceanic General Circulation <span class="hlt">Model</span> (OGCM), namely the Miami Isopycnic Coordinate Ocean <span class="hlt">Model</span> (MICOM). The <span class="hlt">model</span> reproduces the basic characteristics of the seasonal circulation observed in the area of the strait of Bab el Mandeb. There is good agreement between <span class="hlt">model</span> results and available observations on the strength of the <span class="hlt">exchange</span> and the characteristics of the water masses involved, as well as the seasonal flow pattern. During winter, this flow consists of a typical inverse estuarine circulation, while during summer, the <span class="hlt">surface</span> flow reverses, there is an intermediate inflow of relatively cold and fresh water, and the hypersaline outflow at the bottom of the strait is significantly reduced. Additional experiments with different atmospheric forcing (seasonal winds, seasonal thermohaline <span class="hlt">air</span>-sea fluxes, or combinations) were performed in order to assess the role of the atmospheric forcing fields in the <span class="hlt">exchange</span> flow at Bab el Mandeb. The results of both the wind- and thermohaline-driven experiments exhibit a strong seasonality at the area of the strait, which is in phase with the observations. However, it is the combination of both the seasonal pattern of the wind stress and the seasonal thermohaline forcing that can reproduce the observed seasonal variability at the strait. The importance of the seasonal cycle of the thermohaline forcing on the <span class="hlt">exchange</span> flow pattern is also emphasized by these results. In the experiment where the thermohaline forcing is represented by its annual mean, the strength of the <span class="hlt">exchange</span> is reduced almost by half.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810126C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810126C"><span>Towards constraining the stratosphere-troposphere <span class="hlt">exchange</span> of radiocarbon: strategies of stratospheric 14CO2 measurements using <span class="hlt">Air</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>Chen, Huilin; Paul, Dipayan; Meijer, Harro; Miller, John; Kivi, Rigel; Krol, Maarten</p> <p>2016-04-01</p> <p>Radiocarbon (14C) plays an important role in the carbon cycle studies to understand both natural and anthropogenic carbon fluxes, 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 stratosphere due to the cosmogenic production. To this end, better understanding the stratospheric radiocarbon source is very useful to advance the use of radiocarbon for these applications. However, stratospheric 14C observations have been very limited so that there are large uncertainties on 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 14C measurements using <span class="hlt">Air</span>Core samples from Sodankylä, Northern Finland. <span class="hlt">Air</span>Core is an innovative atmospheric sampling system, which passively collects atmospheric <span class="hlt">air</span> samples into a long piece of coiled stainless steel tubing during the descent of a balloon flight. Due to the relatively low cost of the consumables, there is a potential to make such <span class="hlt">Air</span>Core profiling in other parts of the world on a regular basis. In this study, we simulate the 14C in the atmosphere and assess the stratosphere-troposphere <span class="hlt">exchange</span> of radiocarbon using the TM5 <span class="hlt">model</span>. The Sodankylä radiocarbon measurements will be used to verify the performance of the <span class="hlt">model</span> at high latitude. Besides this, we will also 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 <span class="hlt">exchange</span>, and based on the results design a strategy to set up a 14C measurement program using <span class="hlt">Air</span>Core.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2954549','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2954549"><span>Modified Perfluorocarbon Tracer Method for Measuring Effective Multizone <span class="hlt">Air</span> <span class="hlt">Exchange</span> Rates</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shinohara, Naohide; Kataoka, Toshiyuki; Takamine, Koichi; Butsugan, Michio; Nishijima, Hirokazu; Gamo, Masashi</p> <p>2010-01-01</p> <p>A modified procedure was developed for the measurement of the effective <span class="hlt">air</span> <span class="hlt">exchange</span> rate, which represents the relationship between the pollutants emitted from indoor sources and the residents’ level of exposure, by placing the dosers of tracer gas at locations that resemble indoor emission sources. To measure the 24-h-average effective <span class="hlt">air</span> <span class="hlt">exchange</span> rates in future surveys based on this procedure, a low-cost, easy-to-use perfluorocarbon tracer (PFT) doser with a stable dosing rate was developed by using double glass vials, a needle, a polyethylene-sintered filter, and a diffusion tube. Carbon molecular sieve cartridges and carbon disulfide (CS2) were used for passive sampling and extraction of the tracer gas, respectively. Recovery efficiencies, sampling rates, and lower detection limits for 24-h sampling of hexafluorobenzene, octafluorotoluene, and perfluoroallylbenzene were 40% ± 3%, 72% ± 5%, and 84% ± 6%; 10.5 ± 1.1, 14.4 ± 1.4, and 12.2 ± 0.49 mL min−1; and 0.20, 0.17, and 0.26 μg m−3, respectively. PMID:20948928</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20948928','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20948928"><span>Modified perfluorocarbon tracer method for measuring effective multizone <span class="hlt">air</span> <span class="hlt">exchange</span> rates.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shinohara, Naohide; Kataoka, Toshiyuki; Takamine, Koichi; Butsugan, Michio; Nishijima, Hirokazu; Gamo, Masashi</p> <p>2010-09-01</p> <p>A modified procedure was developed for the measurement of the effective <span class="hlt">air</span> <span class="hlt">exchange</span> rate, which represents the relationship between the pollutants emitted from indoor sources and the residents' level of exposure, by placing the dosers of tracer gas at locations that resemble indoor emission sources. To measure the 24-h-average effective <span class="hlt">air</span> <span class="hlt">exchange</span> rates in future surveys based on this procedure, a low-cost, easy-to-use perfluorocarbon tracer (PFT) doser with a stable dosing rate was developed by using double glass vials, a needle, a polyethylene-sintered filter, and a diffusion tube. Carbon molecular sieve cartridges and carbon disulfide (CS₂) were used for passive sampling and extraction of the tracer gas, respectively. Recovery efficiencies, sampling rates, and lower detection limits for 24-h sampling of hexafluorobenzene, octafluorotoluene, and perfluoroallylbenzene were 40% ± 3%, 72% ± 5%, and 84% ± 6%; 10.5 ± 1.1, 14.4 ± 1.4, and 12.2 ± 0.49 mL min⁻¹; and 0.20, 0.17, and 0.26 μg m⁻³, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/46514','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/46514"><span>A physically based analytical spatial <span class="hlt">air</span> temperature and humidity <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Yang Yang; Theodore A. Endreny; David J. Nowak</p> <p>2013-01-01</p> <p>Spatial variation of urban <span class="hlt">surface</span> <span class="hlt">air</span> temperature and humidity influences human thermal comfort, the settling rate of atmospheric pollutants, and plant physiology and growth. Given the lack of observations, we developed a Physically based Analytical Spatial <span class="hlt">Air</span> Temperature and Humidity (PASATH) <span class="hlt">model</span>. The PASATH <span class="hlt">model</span> calculates spatial solar radiation and heat...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmEn.160...36H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmEn.160...36H"><span>Persistence of initial conditions in continental scale <span class="hlt">air</span> quality simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hogrefe, Christian; Roselle, Shawn J.; Bash, Jesse O.</p> <p>2017-07-01</p> <p>This study investigates the effect of initial conditions (IC) for pollutant concentrations in the atmosphere and soil on simulated <span class="hlt">air</span> quality for two continental-scale Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span> applications. One of these applications was performed for springtime and the second for summertime. Results show that a spin-up period of ten days commonly used in regional-scale applications may not be sufficient to reduce the effects of initial conditions to less than 1% of seasonally-averaged <span class="hlt">surface</span> ozone concentrations everywhere while 20 days were found to be sufficient for the entire domain for the spring case and almost the entire domain for the summer case. For the summer case, differences were found to persist longer aloft due to circulation of <span class="hlt">air</span> masses and even a spin-up period of 30 days was not sufficient to reduce the effects of ICs to less than 1% of seasonally-averaged layer 34 ozone concentrations over the southwestern portion of the <span class="hlt">modeling</span> domain. Analysis of the effect of soil initial conditions for the CMAQ bidirectional NH3 <span class="hlt">exchange</span> <span class="hlt">model</span> shows that during springtime they can have an important effect on simulated inorganic aerosols concentrations for time periods of one month or longer. The effects are less pronounced during other seasons. The results, while specific to the <span class="hlt">modeling</span> domain and time periods simulated here, suggest that <span class="hlt">modeling</span> protocols need to be scrutinized for a given application and that it cannot be assumed that commonly-used spin-up periods are necessarily sufficient to reduce the effects of initial conditions on <span class="hlt">model</span> results to an acceptable level. What constitutes an acceptable level of difference cannot be generalized and will depend on the particular application, time period and species of interest. Moreover, as the application of <span class="hlt">air</span> quality <span class="hlt">models</span> is being expanded to cover larger geographical domains and as these <span class="hlt">models</span> are increasingly being coupled with other <span class="hlt">modeling</span> systems to better represent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyA..491..271L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyA..491..271L"><span>Rethinking <span class="hlt">exchange</span> market <span class="hlt">models</span> as optimization algorithms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luquini, Evandro; Omar, Nizam</p> <p>2018-02-01</p> <p>The <span class="hlt">exchange</span> market <span class="hlt">model</span> has mainly been used to study the inequality problem. Although the human society inequality problem is very important, the <span class="hlt">exchange</span> market <span class="hlt">models</span> dynamics until stationary state and its capability of ranking individuals is interesting in itself. This study considers the hypothesis that the <span class="hlt">exchange</span> market <span class="hlt">model</span> could be understood as an optimization procedure. We present herein the implications for algorithmic optimization and also the possibility of a new family of <span class="hlt">exchange</span> market <span class="hlt">models</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26065326','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26065326"><span>Interaction between <span class="hlt">Air</span> Bubbles and Superhydrophobic <span class="hlt">Surfaces</span> in Aqueous Solutions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shi, Chen; Cui, Xin; Zhang, Xurui; Tchoukov, Plamen; Liu, Qingxia; Encinas, Noemi; Paven, Maxime; Geyer, Florian; Vollmer, Doris; Xu, Zhenghe; Butt, Hans-Jürgen; Zeng, Hongbo</p> <p>2015-07-07</p> <p>Superhydrophobic <span class="hlt">surfaces</span> are usually characterized by a high apparent contact angle of water drops in <span class="hlt">air</span>. Here we analyze the inverse situation: Rather than focusing on water repellency in <span class="hlt">air</span>, we measure the attractive interaction of <span class="hlt">air</span> bubbles and superhydrophobic <span class="hlt">surfaces</span> in water. Forces were measured between microbubbles with radii R of 40-90 μm attached to an atomic force microscope cantilever and submerged superhydrophobic <span class="hlt">surfaces</span>. In addition, forces between macroscopic bubbles (R = 1.2 mm) at the end of capillaries and superhydrophobic <span class="hlt">surfaces</span> were measured. As superhydrophobic <span class="hlt">surfaces</span> we applied soot-templated <span class="hlt">surfaces</span>, nanofilament <span class="hlt">surfaces</span>, micropillar arrays with flat top faces, and decorated micropillars. Depending on the specific structure of the superhydrophobic <span class="hlt">surfaces</span> and the presence and amount of entrapped <span class="hlt">air</span>, different interactions were observed. Soot-templated <span class="hlt">surfaces</span> in the Cassie state showed superaerophilic behavior: Once the electrostatic double-layer force and a hydrodynamic repulsion were overcome, bubbles jumped onto the <span class="hlt">surface</span> and fully merged with the entrapped <span class="hlt">air</span>. On nanofilaments and micropillar arrays we observed in addition the formation of sessile bubbles with finite contact angles below 90° or the attachment of bubbles, which retained their spherical shape.</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://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=64491&Lab=NERL&keyword=climatology&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=64491&Lab=NERL&keyword=climatology&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>DEVELOPMENT OF A LAND-<span class="hlt">SURFACE</span> <span class="hlt">MODEL</span> PART I: APPLICATION IN A MESOSCALE METEOROLOGY <span class="hlt">MODEL</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>Parameterization of land-<span class="hlt">surface</span> processes and consideration of <span class="hlt">surface</span> inhomogeneities are very important to mesoscale meteorological <span class="hlt">modeling</span> applications, especially those that provide information for <span class="hlt">air</span> quality <span class="hlt">modeling</span>. To provide crucial, reliable information on the diurn...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDL28002N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDL28002N"><span>Keeping warm with fur in cold water: entrainment of <span class="hlt">air</span> in hairy <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nasto, Alice; Regli, Marianne; Brun, Pierre-Thomas; Clanet, Christophe; Hosoi, Anette</p> <p>2015-11-01</p> <p>Instead of relying on a thick layer of body fat for insulation as many aquatic mammals do, fur seals and otters trap <span class="hlt">air</span> in their dense fur for insulation in cold water. Using a combination of <span class="hlt">model</span> experiments and theory, we rationalize this mechanism of <span class="hlt">air</span> trapping underwater for thermoregulation. For the <span class="hlt">model</span> experiments, hairy <span class="hlt">surfaces</span> are fabricated using laser cut molds and casting samples with PDMS. <span class="hlt">Modeling</span> the hairy texture as a network of capillary tubes, the imbibition speed of water into the hairs is obtained through a balance of hydrostatic pressure and viscous stress. In this scenario, the bending of the hairs and capillary forces are negligible. The maximum diving depth that can be achieved before the hairs are wetted to the roots is predicted from a comparison of the diving speed and imbibition speed. The amount of <span class="hlt">air</span> that is entrained in hairy <span class="hlt">surfaces</span> is greater than what is expected for classic Landau-Levich-Derjaguin plate plunging. A phase diagram with the parameters from experiments and biological data allows a comparison of the <span class="hlt">model</span> system and animals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170005914','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170005914"><span>Laser Processed Condensing Heat <span class="hlt">Exchanger</span> Technology Development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hansen, Scott; Wright, Sarah; Wallace, Sarah; Hamilton, Tanner; Dennis, Alexander; Zuhlke, Craig; Roth, Nick; Sanders, John</p> <p>2017-01-01</p> <p>The reliance on non-permanent coatings in Condensing Heat <span class="hlt">Exchanger</span> (CHX) designs is a significant technical issue to be solved before long-duration spaceflight can occur. Therefore, high reliability CHXs have been identified by the Evolvable Mars Campaign (EMC) as critical technologies needed to move beyond low earth orbit. The Laser Processed Condensing Heat <span class="hlt">Exchanger</span> project aims to solve these problems through the use of femtosecond laser processed <span class="hlt">surfaces</span>, which have unique wetting properties and potentially exhibit anti-microbial growth properties. These <span class="hlt">surfaces</span> were investigated to identify if they would be suitable candidates for a replacement CHX <span class="hlt">surface</span>. Among the areas researched in this project include microbial growth testing, siloxane flow testing in which laser processed <span class="hlt">surfaces</span> were exposed to siloxanes in an <span class="hlt">air</span> stream, and manufacturability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25827140','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25827140"><span><span class="hlt">Air</span>-Seawater <span class="hlt">Exchange</span> of Organochlorine Pesticides along the Sediment Plume of a Large Contaminated River.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lin, Tian; Guo, Zhigang; Li, Yuanyuan; Nizzetto, Luca; Ma, Chuanliang; Chen, Yingjun</p> <p>2015-05-05</p> <p>Gaseous <span class="hlt">exchange</span> fluxes of organochlorine pesticides (OCPs) across the <span class="hlt">air</span>-water interface of the coastal East China Sea were determined in order to assess whether the contaminated plume of the Yangtze River could be an important regional source of OCPs to the atmosphere. Hexachlorocyclohexanes (HCHs), chlordane compounds (CHLs), and dichlorodiphenyltrichloroethanes (DDTs) were the most frequently detected OCPs in <span class="hlt">air</span> and water. <span class="hlt">Air</span>-water <span class="hlt">exchange</span> was mainly characterized by net volatilization for all measured OCPs. The net gaseous <span class="hlt">exchange</span> flux ranged 10-240 ng/(m2·day) for γ-HCH, 60-370 ng/(m2·day) for trans-CHL, 97-410 ng/(m2·day) for cis-CHL, and ∼0 (e.g., equilibrium) to 490 ng/(m2·day) for p,p'-DDE. We found that the plume of the large contaminated river can serve as a significant regional secondary atmospheric source of legacy contaminants released in the catchment. In particular, the sediment plume represented the relevant source of DDT compounds (especially p,p'-DDE) sustaining net degassing when clean <span class="hlt">air</span> masses from the open ocean reached the plume area. In contrast, a mass balance showed that, for HCHs, contaminated river discharge (water and sediment) plumes were capable of sustaining volatilization throughout the year. These results demonstrate the inconsistencies in the fate of HCHs and DDTs in this large estuarine system with declining primary sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20180000782','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20180000782"><span><span class="hlt">Air</span> Quality Forecasts Using the NASA GEOS <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Keller, Christoph A.; Knowland, K. Emma; Nielsen, Jon E.; Orbe, Clara; Ott, Lesley; Pawson, Steven; Saunders, Emily; Duncan, Bryan; Follette-Cook, Melanie; Liu, Junhua; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20180000782'); toggleEditAbsImage('author_20180000782_show'); toggleEditAbsImage('author_20180000782_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20180000782_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20180000782_hide"></p> <p>2018-01-01</p> <p>We provide an introduction to a new high-resolution (0.25 degree) global composition forecast produced by NASA's Global <span class="hlt">Modeling</span> and Assimilation office. The NASA Goddard Earth Observing System version 5 (GEOS-5) <span class="hlt">model</span> has been expanded to provide global near-real-time forecasts of atmospheric composition at a horizontal resolution of 0.25 degrees (25 km). Previously, this combination of detailed chemistry and resolution was only provided by regional <span class="hlt">models</span>. This system combines the operational GEOS-5 weather forecasting <span class="hlt">model</span> with the state-of-the-science GEOS-Chem chemistry module (version 11) to provide detailed chemical analysis of a wide range of <span class="hlt">air</span> pollutants such as ozone, carbon monoxide, nitrogen oxides, and fine particulate matter (PM2.5). The resolution of the forecasts is the highest resolution compared to current, publically-available global composition forecasts. Evaluation and validation of <span class="hlt">modeled</span> trace gases and aerosols compared to <span class="hlt">surface</span> and satellite observations will be presented for constituents relative to health <span class="hlt">air</span> quality standards. Comparisons of <span class="hlt">modeled</span> trace gases and aerosols against satellite observations show that the <span class="hlt">model</span> produces realistic concentrations of atmospheric constituents in the free troposphere. <span class="hlt">Model</span> comparisons against <span class="hlt">surface</span> observations highlight the <span class="hlt">model</span>'s capability to capture the diurnal variability of <span class="hlt">air</span> pollutants under a variety of meteorological conditions. The GEOS-5 composition forecasting system offers a new tool for scientists and the public health community, and is being developed jointly with several government and non-profit partners. Potential applications include <span class="hlt">air</span> quality warnings, flight campaign planning and exposure studies using the archived analysis fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12578005','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12578005"><span>Effects of <span class="hlt">air</span> current speed on gas <span class="hlt">exchange</span> in plant leaves and plant canopies.</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; Tsuruyama, J; Shibuya, T; Yoshida, M; Kiyota, M</p> <p>2003-01-01</p> <p>To obtain basic data on adequate <span class="hlt">air</span> circulation to enhance plant growth in a closed plant culture system in a controlled ecological life support system (CELSS), an investigation was made of the effects of the <span class="hlt">air</span> current speed ranging from 0.01 to 1.0 m s-1 on photosynthesis and transpiration in sweetpotato leaves and photosynthesis in tomato seedlings canopies. The gas <span class="hlt">exchange</span> rates in leaves and canopies were determined by using a chamber method with an infrared gas analyzer. The net photosynthetic rate and the transpiration rate increased significantly as the <span class="hlt">air</span> current speeds increased from 0.01 to 0.2 m s-1. The transpiration rate increased gradually at <span class="hlt">air</span> current speeds ranging from 0.2 to 1.0 m s-1 while the net photosynthetic rate was almost constant at <span class="hlt">air</span> current speeds ranging from 0.5 to 1.0 m s-1. The increase in the net photosynthetic and transpiration rates were strongly dependent on decreased boundary-layer resistances against gas diffusion. The net photosynthetic rate of the plant canopy was doubled by an increased <span class="hlt">air</span> current speed from 0.1 to 1.0 m s-1 above the plant canopy. The results demonstrate the importance of <span class="hlt">air</span> movement around plants for enhancing the gas <span class="hlt">exchange</span> in the leaf, especially in plant canopies in the CELSS. c2002 COSPAR. Published by Elsevier Science Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmRe.196...62S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmRe.196...62S"><span>Intense <span class="hlt">air</span>-sea <span class="hlt">exchanges</span> and heavy orographic precipitation over Italy: The role of Adriatic sea <span class="hlt">surface</span> temperature uncertainty</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stocchi, Paolo; Davolio, Silvio</p> <p>2017-11-01</p> <p>Strong and persistent low-level winds blowing over the Adriatic basin are often associated with intense precipitation events over Italy. Typically, in case of moist southeasterly wind (Sirocco), rainfall affects northeastern Italy and the Alpine chain, while with cold northeasterly currents (Bora) precipitations are localized along the eastern slopes of the Apennines and central Italy coastal areas. These events are favoured by intense <span class="hlt">air</span>-sea interactions and it is reasonable to hypothesize that the Adriatic sea <span class="hlt">surface</span> temperature (SST) can affect the amount and location of precipitation. High-resolution simulations of different Bora and Sirocco events leading to severe precipitation are performed using a convection-permitting <span class="hlt">model</span> (MOLOCH). Sensitivity experiments varying the SST initialization field are performed with the aim of evaluating the impact of SST uncertainty on precipitation forecasts, which is a relevant topic for operational weather predictions, especially at local scales. Moreover, diagnostic tools to compute water vapour fluxes across the Italian coast and atmospheric water budget over the Adriatic Sea have been developed and applied in order to characterize the <span class="hlt">air</span> mass that feeds the precipitating systems. Finally, the investigation of the processes through which the SST influences location and intensity of heavy precipitation allows to gain a better understanding on mechanisms conducive to severe weather in the Mediterranean area and in the Adriatic basin in particular. Results show that the effect of the Adriatic SST (uncertainty) on precipitation is complex and can vary considerably among different events. For both Bora and Sirocco events, SST does not influence markedly the atmospheric water budget or the degree of moistening of <span class="hlt">air</span> that flows over the Adriatic Sea. SST mainly affects the stability of the atmospheric boundary layer, thus influencing the flow dynamics and the orographic flow regime, and in turn, the precipitation pattern.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060029193&hterms=air+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dair%2Bmeasurement','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060029193&hterms=air+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dair%2Bmeasurement"><span>Sea <span class="hlt">surface</span> temperature measurements with <span class="hlt">AIRS</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Aumann, H.</p> <p>2003-01-01</p> <p>The comparison of global sea <span class="hlt">surface</span> skin temperature derived from cloud-free <span class="hlt">AIRS</span> super window channel at 2616 cm-1 (sst2616) with the Real-Time Global Sea <span class="hlt">Surface</span> Temperature for September 2002 shows surprisingly small standard deviation of 0.44K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA502422','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA502422"><span>Stochastic Lanchester <span class="hlt">Air-to-Air</span> Campaign <span class="hlt">Model</span>: <span class="hlt">Model</span> Description and Users Guides</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2009-01-01</p> <p>STOCHASTIC LANCHESTER <span class="hlt">AIR-TO-AIR</span> CAMPAIGN <span class="hlt">MODEL</span> <span class="hlt">MODEL</span> DESCRIPTION AND USERS GUIDES—2009 REPORT PA702T1 Rober t V. Hemm Jr. Dav id A . Lee...LMI © 2009. ALL RIGHTS RESERVED. Stochastic Lanchester <span class="hlt">Air-to-Air</span> Campaign <span class="hlt">Model</span>: <span class="hlt">Model</span> Description and Users Guides—2009 PA702T1/JANUARY...2009 Executive Summary This report documents the latest version of the Stochastic Lanchester <span class="hlt">Air-to-Air</span> Campaign <span class="hlt">Model</span> (SLAACM), developed by LMI for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/514643-modeling-multicomponent-ion-exchange-equilibrium-utilizing-hydrous-crystalline-silicotitanates-multiple-interactive-ion-exchange-site-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/514643-modeling-multicomponent-ion-exchange-equilibrium-utilizing-hydrous-crystalline-silicotitanates-multiple-interactive-ion-exchange-site-model"><span><span class="hlt">Modeling</span> multicomponent ion <span class="hlt">exchange</span> equilibrium utilizing hydrous crystalline silicotitanates by a multiple interactive ion <span class="hlt">exchange</span> site <span class="hlt">model</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>Zheng, Z.; Anthony, R.G.; Miller, J.E.</p> <p>1997-06-01</p> <p>An equilibrium multicomponent ion <span class="hlt">exchange</span> <span class="hlt">model</span> is presented for the ion <span class="hlt">exchange</span> of group I metals by TAM-5, a hydrous crystalline silicotitanate. On the basis of the data from ion <span class="hlt">exchange</span> and structure studies, the solid phase is represented as Na{sub 3}X instead of the usual form of NaX. By using this solid phase representation, the solid can be considered as an ideal phase. A set of <span class="hlt">model</span> ion <span class="hlt">exchange</span> reactions is proposed for ion <span class="hlt">exchange</span> between H{sup +}, Na{sup +}, K{sup +}, Rb{sup +}, and Cs{sup +}. The equilibrium constants for these reactions were estimated from experiments with simplemore » ion <span class="hlt">exchange</span> systems. Bromley`s <span class="hlt">model</span> for activity coefficients of electrolytic solutions was used to account for liquid phase nonideality. Bromley`s <span class="hlt">model</span> parameters for CsOH at high ionic strength and for NO{sub 2}{sup {minus}} and Al(OH){sub 4}{sup {minus}} were estimated in order to apply the <span class="hlt">model</span> for complex waste simulants. The equilibrium compositions and distribution coefficients of counterions were calculated for complex simulants typical of DOE wastes by solving the equilibrium equations for the <span class="hlt">model</span> reactions and material balance equations. The predictions match the experimental results within 10% for all of these solutions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008APS..MARJ17010M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008APS..MARJ17010M"><span>Dynamics of Gas <span class="hlt">Exchange</span> through the Fractal Architecture of the Human Lung, <span class="hlt">Modeled</span> as an Exactly Solvable Hierarchical Tree</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mayo, Michael; Pfeifer, Peter; Gheorghiu, Stefan</p> <p>2008-03-01</p> <p>The acinar airways lie at the periphery of the human lung and are responsible for the transfer of oxygen from <span class="hlt">air</span> to the blood during respiration. This transfer occurs by the diffusion-reaction of oxygen over the irregular <span class="hlt">surface</span> of the alveolar membranes lining the acinar airways. We present an exactly solvable diffusion-reaction <span class="hlt">model</span> on a hierarchically branched tree, allowing a quantitative prediction of the oxygen current over the entire system of acinar airways responsible for the gas <span class="hlt">exchange</span>. We discuss the effect of diffusional screening, which is strongly coupled to oxygen transport in the human lung. We show that the oxygen current is insensitive to a loss of permeability of the alveolar membranes over a wide range of permeabilities, similar to a ``constant-current source'' in an electric network. Such fault tolerance has been observed in other treatments of the gas <span class="hlt">exchange</span> in the lung and is obtained here as a fully analytical result.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26479780','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26479780"><span>Biofouling on polymeric heat <span class="hlt">exchanger</span> <span class="hlt">surfaces</span> with E. coli and native biofilms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pohl, S; Madzgalla, M; Manz, W; Bart, H J</p> <p>2015-01-01</p> <p>The biofouling affinity of different polymeric <span class="hlt">surfaces</span> (polypropylene, polysulfone, polyethylene terephthalate, and polyether ether ketone) in comparison to stainless steel (SS) was studied for the <span class="hlt">model</span> bacterium Escherichia coli K12 DSM 498 and native biofilms originating from Rhine water. The biofilm mass deposited on the polymer <span class="hlt">surfaces</span> was minimized by several magnitudes compared to SS. The cell count and the accumulated biomass of E. coli on the polymer <span class="hlt">surfaces</span> showed an opposing linear trend. The promising low biofilm formation on the polymers is attributed to the combination of inherent <span class="hlt">surface</span> properties (roughness, <span class="hlt">surface</span> energy and hydrophobicity) when compared to SS. The fouling characteristics of E. coli biofilms show good conformity with the more complex native biofilms investigated. The results can be utilized for the development of new polymer heat <span class="hlt">exchangers</span> when using untreated river water as coolant or for other processes needing antifouling materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110022999','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110022999"><span>Improvement of the GEOS-5 AGCM upon Updating the <span class="hlt">Air</span>-Sea Roughness Parameterization</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Garfinkel, C. I.; Molod, A.; Oman, L. D.; Song, I.-S.</p> <p>2011-01-01</p> <p>The impact of an <span class="hlt">air</span>-sea roughness parameterization over the ocean that more closely matches recent observations of <span class="hlt">air</span>-sea <span class="hlt">exchange</span> is examined in the NASA Goddard Earth Observing System, version 5 (GEOS-5) atmospheric general circulation <span class="hlt">model</span>. <span class="hlt">Surface</span> wind biases in the GEOS-5 AGCM are decreased by up to 1.2m/s. The new parameterization also has implications aloft as improvements extend into the stratosphere. Many other GCMs (both for operational weather forecasting and climate) use a similar class of parameterization for their <span class="hlt">air</span>-sea roughness scheme. We therefore expect that results from GEOS-5 are relevant to other <span class="hlt">models</span> as well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5519K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5519K"><span><span class="hlt">Modelling</span> the urban <span class="hlt">air</span> quality in Hamburg with the new city-scale chemistry transport <span class="hlt">model</span> CityChem</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karl, Matthias; Ramacher, Martin; Aulinger, Armin; Matthias, Volker; Quante, Markus</p> <p>2017-04-01</p> <p> Health Organization (WHO) guideline concentration limits for O3 and of the regulatory limits for NO2. <span class="hlt">Model</span> tests were performed with CityChem to study the ozone formation rate with simultaneous variation of emissions of nitrogen oxides (NOx) and volatile organic compounds (VOC). Emissions of VOC in urban areas are not well quantified as they may originate from various sources, including solvent usage, industry, combustion plants and vehicular traffic. The employed chemical mechanism contains large uncertainties with respect to ozone formation. Observed high-O3 episodes were analyzed by comparing <span class="hlt">modelled</span> pollutant concentrations with concentration data from the Hamburg <span class="hlt">air</span> quality surveillance network (http://luft.hamburg.de/). The analysis inspected possible reasons for too low <span class="hlt">modelled</span> O3 in summer such as missing emissions of VOC from natural sources like green parks and the vertical <span class="hlt">exchange</span> of O3 towards the <span class="hlt">surface</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987JGR....92.1937J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987JGR....92.1937J"><span>On the parameters influencing <span class="hlt">air</span>-water gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>JäHne, Bernd; Münnich, Karl Otto; BöSinger, Rainer; Dutzi, Alfred; Huber, Werner; Libner, Peter</p> <p>1987-02-01</p> <p>Detailed gas <span class="hlt">exchange</span> measurements from two circular and one linear wind/wave tunnels are presented. Heat, He, CH4, CO2, Kr, and Xe have been used as tracers. The experiments show the central importance of waves for the water-side transfer process. With the onset of waves the Schmidt number dependence of the transfer velocity k changes from k ∝ Sc-⅔ to k ∝ Sc-½indicating a change in the boundary conditions at the <span class="hlt">surface</span>. Moreover, energy put into the wave field by wind is transferred to near-<span class="hlt">surface</span> turbulence enhancing gas transfer. The data show that the mean square slope of the waves is the best parameter to characterize the free wavy <span class="hlt">surface</span> with respect to water-side transfer processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080008474','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080008474"><span>3D <span class="hlt">Air</span> Quality and the Clean <span class="hlt">Air</span> Interstate Rule: Lagrangian Sampling of CMAQ <span class="hlt">Model</span> Results to Aid Regional Accountability Metrics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fairlie, T. D.; Szykman, Jim; Pierce, Robert B.; Gilliland, A. B.; Engel-Cox, Jill; Weber, Stephanie; Kittaka, Chieko; Al-Saadi, Jassim A.; Scheffe, Rich; Dimmick, Fred; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20080008474'); toggleEditAbsImage('author_20080008474_show'); toggleEditAbsImage('author_20080008474_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20080008474_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20080008474_hide"></p> <p>2008-01-01</p> <p>The Clean <span class="hlt">Air</span> Interstate Rule (CAIR) is expected to reduce transport of <span class="hlt">air</span> pollutants (e.g. fine sulfate particles) in nonattainment areas in the Eastern United States. CAIR highlights the need for an integrated <span class="hlt">air</span> quality observational and <span class="hlt">modeling</span> system to understand sulfate as it moves in multiple dimensions, both spatially and temporally. Here, we demonstrate how results from an <span class="hlt">air</span> quality <span class="hlt">model</span> can be combined with a 3d monitoring network to provide decision makers with a tool to help quantify the impact of CAIR reductions in SO2 emissions on regional transport contributions to sulfate concentrations at <span class="hlt">surface</span> monitors in the Baltimore, MD area, and help improve decision making for strategic implementation plans (SIPs). We sample results from the Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span> using ensemble back trajectories computed with the NASA Langley Research Center trajectory <span class="hlt">model</span> to provide Lagrangian time series and vertical profile information, that can be compared with NASA satellite (MODIS), EPA <span class="hlt">surface</span>, and lidar measurements. Results are used to assess the regional transport contribution to <span class="hlt">surface</span> SO4 measurements in the Baltimore MSA, and to characterize the dominant source regions for low, medium, and high SO4 episodes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDKP1130P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDKP1130P"><span>Nonlinear Acoustics at the <span class="hlt">Air</span>-Water Free <span class="hlt">Surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pree, Seth; Naranjo, Brian; Putterman, Seth</p> <p>2016-11-01</p> <p>According to linear acoustics, airborne sound incident on a water <span class="hlt">surface</span> transmits only a tenth of a percent of its energy. This difficulty of transmitting energy across the water <span class="hlt">surface</span> limits the feasibility of standoff ultrasound imaging. We propose to overcome this long standing problem by developing new methods of coupling into the medium at standoff. In particular, we believe that the acoustic nonlinearity of both the <span class="hlt">air</span> and the medium may yield a range of effects in the vicinity of the <span class="hlt">surface</span> permitting an efficient transmission of ultrasound from the <span class="hlt">air</span> into the medium. The recent commercial availability of parametric speakers that deliver modulated 100kHz ultrasound at 135dB to nonlinearly generate music at 95dB provides an interesting platform with which to revisit the transmission of sound across acoustic impedance mismatches. We show results of experimental studies of the behavior of the <span class="hlt">air</span>-water free <span class="hlt">surface</span> when subjected to large amplitude acoustic pressures from the <span class="hlt">air</span>. This work was supported by the ARO STIR program.</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 CO2 <span class="hlt">exchange</span> 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 CO2 <span class="hlt">exchange</span> in estuarine systems capture the relevant temporal variability and, as such, the temporal variability of bulk parameterized and directly measured CO2 fluxes was investigated in the Danish estuary, Roskilde Fjord. The <span class="hlt">air</span>-sea CO2 fluxes showed large temporal variability across seasons and between days and that more than 30% of the net CO2 emission in 2013 was a result of two large fall and winter storms. The diurnal variability of ΔpCO2 was up to 400 during summer changing the estuary from a source to a sink of CO2 within the day. Across seasons the system was suggested to change from a sink of atmospheric CO2 during spring to near neutral during summer and later to a source of atmospheric CO2 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 CO2 m-2 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 CO2 flux samples were filtered according to the H2Osbnd CO2 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 CO2 <span class="hlt">exchanges</span> and changed the net <span class="hlt">air</span>-sea CO2 <span class="hlt">exchange</span> from an uptake to a release. The CO2 gas transfer velocity was calculated from directly measured CO2 fluxes and ΔpCO2 and agreed to previous observations and parameterizations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17706251','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17706251"><span><span class="hlt">Air</span>--sea gaseous <span class="hlt">exchange</span> of PCB at the Venice lagoon (Italy).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Manodori, L; Gambaro, A; Moret, I; Capodaglio, G; Cescon, P</p> <p>2007-10-01</p> <p>Water bodies are important storage media for persistent organic pollutants (POPs) such as polychlorinated biphenyls (PCBs) and this function is increased in coastal regions because their inputs are higher than those to the open sea. The <span class="hlt">air</span>-water interface is extensively involved with the global cycling of PCBs because it is the place where they accumulate due to depositional processes and where they may be emitted by gaseous <span class="hlt">exchange</span>. In this work the parallel collection of <span class="hlt">air</span>, microlayer and sub-superficial water samples was performed in July 2005 at a site in the Venice lagoon to evaluate the summer gaseous flux of PCBs. The total concentration of PCBs (sum of 118 congeners) in <span class="hlt">air</span> varies from 87 to 273 pg m(-3), whereas in the operationally defined dissolved phase of microlayer and sub-superficial water samples it varies from 159 to 391 pg L(-1). No significant enrichment of dissolved PCB into the microlayer has been observed, although a preferential accumulation of most hydrophobic congeners occurs. Due to this behaviour, we believe that the modified two-layer <span class="hlt">model</span> was the most suitable approach for the evaluation of the flux at the <span class="hlt">air</span>-sea interface, because it takes into account the influence of the microlayer. From its application it appears that PCB volatilize from the lagoon waters with a net flux varying from 58 to 195 ng m(-2)d(-1) (uncertainty: +/-50-64%) due to the strong influence of wind speed. This flux is greater than those reported in the literature for the atmospheric deposition and rivers input and reveals that PCB are actively emitted from the Venice lagoon in summer months.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=210265&keyword=understanding+AND+human+AND+nature&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=210265&keyword=understanding+AND+human+AND+nature&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>A Comparison of Statistical Techniques for Combining <span class="hlt">Modeled</span> and Observed Concentrations to Create High-Resolution Ozone <span class="hlt">Air</span> Quality <span class="hlt">Surfaces</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><span class="hlt">Air</span> quality <span class="hlt">surfaces</span> representing pollutant concentrations across space and time are needed for many applications, including tracking trends and relating <span class="hlt">air</span> quality to human and ecosystem health. The spatial and temporal characteristics of these <span class="hlt">surfaces</span> may reveal new informat...</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('http://adsabs.harvard.edu/abs/2014PhDT.......101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......101S"><span>Ion <span class="hlt">Exchange</span> Formation via Sulfonated Bicomponent Nonwovens</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stoughton, Hannah L.</p> <p></p> <p>For many years ion <span class="hlt">exchange</span> resins were used to: remove heavy metals from water, recover materials from wastewater, and eliminate harmful gases from the <span class="hlt">air</span>. While use of these resin beads dominates the ion <span class="hlt">exchange</span> industry, the beads have limitations that should be considered when decisions are made to employ them. For instance, officials must balance the inherent zero sum <span class="hlt">surface</span> area and porosity of the materials. This series of studies investigates the use of bicomponent nonwovens as a base substrate for producing high <span class="hlt">surface</span> area ion <span class="hlt">exchange</span> materials for the removal of heavy metal ions. Functionalized materials were produced in a two-step process: (1) PET/PE spunbond bicomponent fibers were fractured completely, producing the high <span class="hlt">surface</span> area nonwoven to be used as the base ion <span class="hlt">exchange</span> material, and (2) the conditions for functionalizing the PET fibers of the nonwoven webs were investigated where an epoxy containing monomer was grafted to the <span class="hlt">surface</span> followed by sulfonation of the monomer. The functionalization reactions of the PET fibers were monitored based on: weight gain, FTIR, TOF-SIMS, and SEM. Ion <span class="hlt">exchange</span> properties were evaluated using titration and copper ion removal capacity from test solutions. The relationship between web structure and removal efficiency of the metal ions was defined through a comparison of the bicomponent and homocomponent nonwovens for copper ion removal efficiency. The investigation revealed that utilizing the high <span class="hlt">surface</span> area, fractured bicomponent nonwoven ion <span class="hlt">exchange</span> materials with capacities comparable to commercially available ion <span class="hlt">exchange</span> resins could be produced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070023751&hterms=air+asia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dair%2Basia','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070023751&hterms=air+asia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dair%2Basia"><span>High Lapse Rates in <span class="hlt">AIRS</span> Retrieved Temperatures in Cold <span class="hlt">Air</span> Outbreaks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fetzer, Eric J.; Kahn, Brian; Olsen, Edward T.; Fishbein, Evan</p> <p>2004-01-01</p> <p> atmosphere. We anticipate future improvements in the <span class="hlt">AIRS</span> retrieval algorithm will lead to improved understanding of the <span class="hlt">exchange</span> of sensible and latent heat from ocean to atmosphere, and more realistic near-<span class="hlt">surface</span> lapse rates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70099278','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70099278"><span>1DTempPro: analyzing temperature profiles for groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</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>Voytek, Emily B.; Drenkelfuss, Anja; Day-Lewis, Frederick D.; Healy, Richard; Lane, John W.; Werkema, Dale D.</p> <p>2014-01-01</p> <p>A new computer program, 1DTempPro, is presented for the analysis of vertical one-dimensional (1D) temperature profiles under saturated flow conditions. 1DTempPro is a graphical user interface to the U.S. Geological Survey code Variably Saturated 2-Dimensional Heat Transport (VS2DH), which numerically solves the flow and heat-transport equations. Pre- and postprocessor features allow the user to calibrate VS2DH <span class="hlt">models</span> to estimate vertical groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> and also hydraulic conductivity for cases where hydraulic head is known.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4310242','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4310242"><span>Computational fluid dynamics <span class="hlt">modeling</span> of transport and deposition of pesticides in an aircraft cabin</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Isukapalli, Sastry S.; Mazumdar, Sagnik; George, Pradeep; Wei, Binnian; Jones, Byron; Weisel, Clifford P.</p> <p>2015-01-01</p> <p>Spraying of pesticides in aircraft cabins is required by some countries as part of a disinsection process to kill insects that pose a public health threat. However, public health concerns remain regarding exposures of cabin crew and passengers to pesticides in aircraft cabins. While large scale field measurements of pesticide residues and <span class="hlt">air</span> concentrations in aircraft cabins scenarios are expensive and time consuming, Computational Fluid Dynamics (CFD) <span class="hlt">models</span> provide an effective alternative for characterizing concentration distributions and exposures. This study involved CFD <span class="hlt">modeling</span> of a twin-aisle 11 row cabin mockup with heated manikins, mimicking a part of a fully occupied Boeing 767 cabin. The <span class="hlt">model</span> was applied to study the flow and deposition of pesticides under representative scenarios with different spraying patterns (sideways and overhead) and cabin <span class="hlt">air</span> <span class="hlt">exchange</span> rates (low and high). Corresponding spraying experiments were conducted in the cabin mockup, and pesticide deposition samples were collected at the manikin’s lap and seat top for a limited set of five seats. The CFD <span class="hlt">model</span> performed well for scenarios corresponding to high <span class="hlt">air</span> <span class="hlt">exchange</span> rates, captured the concentration profiles for middle seats under low <span class="hlt">air</span> <span class="hlt">exchange</span> rates, and underestimated the concentrations at window seats under low <span class="hlt">air</span> <span class="hlt">exchange</span> rates. Additionally, both the CFD and experimental measurements showed no major variation in deposition characteristics between sideways and overhead spraying. The CFD <span class="hlt">model</span> can estimate concentration fields and deposition profiles at very high resolutions, which can be used for characterizing the overall variability in <span class="hlt">air</span> concentrations and <span class="hlt">surface</span> loadings. Additionally, these <span class="hlt">model</span> results can also provide a realistic range of <span class="hlt">surface</span> and <span class="hlt">air</span> concentrations of pesticides in the cabin that can be used to estimate potential exposures of cabin crew and passengers to these pesticides. PMID:25642134</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080045293&hterms=desertification&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Ddesertification','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080045293&hterms=desertification&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Ddesertification"><span>Impact of Asian Dust on Global <span class="hlt">Surface</span> <span class="hlt">Air</span> Quality and Radiation Budget</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chin, Mian; Diehl, Thomas; Yu, Hongbin; Ginoux, Paul</p> <p>2006-01-01</p> <p>Dust originating from Asian deserts and desertification areas can be transported regionally and globally to affect <span class="hlt">surface</span> <span class="hlt">air</span> quality, visibility, and radiation budget not only at immediate downwind locations (e.g., eastern Asia) but also regions far away from the sources (e.g., North America). Deposition of Asian dust to the North Pacific Ocean basin influences the ocean productivity. In this study, we will use the Goddard Chemistry Aerosol Radiation and Transport (GOCART) <span class="hlt">model</span>, remote sensing data form satellite and from the ground-based network, and in-situ data from aircraft and <span class="hlt">surface</span> observations to address the following questions: - What are the effects of Asian dust on the <span class="hlt">surface</span> <span class="hlt">air</span> quality and visibility over Asia and North America? - What are the seasonal and spatial variations of dust deposition to the North Pacific Ocean? How does the Asian dust affect <span class="hlt">surface</span> radiation budget?</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AtmEn.178...31J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AtmEn.178...31J"><span>Seasonal atmospheric deposition and <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> of polycyclic aromatic hydrocarbons over the Yangtze River Estuary, East China Sea: Implications for source-sink processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Yuqing; Lin, Tian; Wu, Zilan; Li, Yuanyuan; Li, Zhongxia; Guo, Zhigang; Yao, Xiaohong</p> <p>2018-04-01</p> <p>In this work, <span class="hlt">air</span> samples and <span class="hlt">surface</span> seawater samples covering four seasons from March 2014 to January 2015 were collected from a background receptor site in the YRE to explore the seasonal fluxes of <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> and dry and wet deposition of 15 polycyclic aromatic hydrocarbons (PAHs) and their source-sink processes at the <span class="hlt">air</span>-sea interface. The average dry and wet deposition fluxes of 15 PAHs were estimated as 879 ± 1393 ng m-2 d-1 and 755 ± 545 ng m-2 d-1, respectively. Gaseous PAH release from seawater to the atmosphere averaged 3114 ± 1999 ng m-2 d-1 in a year round. The <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> of PAHs was the dominant process at the <span class="hlt">air</span>-sea interface in the YRE as the magnitude of volatilization flux of PAHs exceeded that of total dry and wet deposition. The gas PAH <span class="hlt">exchange</span> flux was dominated by three-ring PAHs, with the highest value in summer and lowest in winter, indicating a marked seasonal variation owing to differences in Henry's law constants associated with temperature, as well as wind speed and gaseous-dissolved gradient among seasons. Based on the simplified mass balance estimation, a net 11 tons y-1 of PAHs (mainly three-ring PAHs) were volatilized from seawater to the atmosphere in a ∼20,000 km2 area in the YRE. Other than the year-round Yangtze River input and ocean ship emissions, the selective release of low-molecular-weight PAHs from bottom sediments in winter due to resuspension triggered by the East Asian winter monsoon is another potential source of PAHs. This work suggests that the source-sink processes of PAHs at the <span class="hlt">air</span>-sea interface in the YRE play a crucial role in regional cycling of PAHs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1989saei.confQ....C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1989saei.confQ....C"><span>Analytical methods to predict liquid congealing in ram <span class="hlt">air</span> heat <span class="hlt">exchangers</span> during cold operation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coleman, Kenneth; Kosson, Robert</p> <p>1989-07-01</p> <p>Ram <span class="hlt">air</span> heat <span class="hlt">exchangers</span> used to cool liquids such as lube oils or Ethylene-Glycol/water solutions can be subject to congealing in very cold ambients, resulting in a loss of cooling capability. Two-dimensional, transient analytical <span class="hlt">models</span> have been developed to explore this phenomenon with both continuous and staggered fin cores. Staggered fin predictions are compared to flight test data from the E-2C Allison T56 engine lube oil system during winter conditions. For simpler calculations, a viscosity ratio correction was introduced and found to provide reasonable cold ambient performance predictions for the staggered fin core, using a one-dimensional approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16846610','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16846610"><span>Incorporating water-release and lateral protein interactions in <span class="hlt">modeling</span> equilibrium adsorption for ion-<span class="hlt">exchange</span> chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thrash, Marvin E; Pinto, Neville G</p> <p>2006-09-08</p> <p>The equilibrium adsorption of two albumin proteins on a commercial ion <span class="hlt">exchanger</span> has been studied using a colloidal <span class="hlt">model</span>. The <span class="hlt">model</span> accounts for electrostatic and van der Waals forces between proteins and the ion <span class="hlt">exchanger</span> <span class="hlt">surface</span>, the energy of interaction between adsorbed proteins, and the contribution of entropy from water-release accompanying protein adsorption. Protein-<span class="hlt">surface</span> interactions were calculated using methods previously reported in the literature. Lateral interactions between adsorbed proteins were experimentally measured with microcalorimetry. Water-release was estimated by applying the preferential interaction approach to chromatographic retention data. The adsorption of ovalbumin and bovine serum albumin on an anion <span class="hlt">exchanger</span> at solution pH>pI of protein was measured. The experimental isotherms have been <span class="hlt">modeled</span> from the linear region to saturation, and the influence of three modulating alkali chlorides on capacity has been evaluated. The heat of adsorption is endothermic for all cases studied, despite the fact that the net charge on the protein is opposite that of the adsorbing <span class="hlt">surface</span>. Strong repulsive forces between adsorbed proteins underlie the endothermic heat of adsorption, and these forces intensify with protein loading. It was found that the driving force for adsorption is the entropy increase due to the release of water from the protein and adsorbent <span class="hlt">surfaces</span>. It is shown that the colloidal <span class="hlt">model</span> predicts protein adsorption capacity in both the linear and non-linear isotherm regions, and can account for the effects of modulating salt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/752138','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/752138"><span>SPEEDUP{trademark} ion <span class="hlt">exchange</span> column <span class="hlt">model</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>Hang, T.</p> <p>2000-03-06</p> <p>A transient <span class="hlt">model</span> to describe the process of loading a solute onto the granular fixed bed in an ion <span class="hlt">exchange</span> (IX) column has been developed using the SpeedUp{trademark} software package. SpeedUp offers the advantage of smooth integration into other existing SpeedUp flowsheet <span class="hlt">models</span>. The mathematical algorithm of a porous particle diffusion <span class="hlt">model</span> was adopted to account for convection, axial dispersion, film mass transfer, and pore diffusion. The method of orthogonal collocation on finite elements was employed to solve the governing transport equations. The <span class="hlt">model</span> allows the use of a non-linear Langmuir isotherm based on an effective binary ionic <span class="hlt">exchange</span> process.more » The SpeedUp column <span class="hlt">model</span> was tested by comparing to the analytical solutions of three transport problems from the ion <span class="hlt">exchange</span> literature. In addition, a sample calculation of a train of three crystalline silicotitanate (CST) IX columns in series was made using both the SpeedUp <span class="hlt">model</span> and Purdue University's VERSE-LC code. All test cases showed excellent agreement between the SpeedUp <span class="hlt">model</span> results and the test data. The <span class="hlt">model</span> can be readily used for SuperLig{trademark} ion <span class="hlt">exchange</span> resins, once the experimental data are complete.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1261476-surface-oxygen-exchange-rate-linked-bulk-ion-diffusivity-mixed-conducting-ruddlesdenpopper-phases','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1261476-surface-oxygen-exchange-rate-linked-bulk-ion-diffusivity-mixed-conducting-ruddlesdenpopper-phases"><span>Is the <span class="hlt">surface</span> oxygen <span class="hlt">exchange</span> rate linked to bulk ion diffusivity in mixed conducting Ruddlesden–Popper phases?</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Tomkiewicz, Alex C.; Tamimi, Mazin A.; Huq, Ashfia; ...</p> <p>2015-03-02</p> <p>There is a possible link between oxygen <span class="hlt">surface</span> <span class="hlt">exchange</span> rate and bulk oxygen anion diffusivity in mixed ionic and electronic conducting oxides; it is a topic of great interest and debate. While a large body of experimental evidence and theoretical analyses support a link, observed differences between bulk and <span class="hlt">surface</span> composition of these materials are hard to reconcile with this observation. This is further compounded by potential problems with simultaneous measurement of both parameters. Here we utilize separate techniques, in situ neutron diffraction and pulsed isotopic <span class="hlt">surface</span> <span class="hlt">exchange</span>, to examine bulk ion mobility and <span class="hlt">surface</span> oxygen <span class="hlt">exchange</span> rates of threemore » Ruddlesden-Popper phases, general form A n-1A 2'BnO 3n+1, A n-1A 2'BnX 3n+1; LaSrCo 0.5Fe 0.5O 4-δ (n = 1), La 0.3Sr 2.7CoFeO 7-δ (n = 2) and LaSr 3Co 1.5Fe 1.5O 10-δ (n = 3). These measurements are complemented by <span class="hlt">surface</span> composition determination via high sensitivity-low energy ion scattering. We observe a correlation between bulk ion mobility and <span class="hlt">surface</span> <span class="hlt">exchange</span> rate between materials. The <span class="hlt">surface</span> <span class="hlt">exchange</span> rates vary by more than one order of magnitude with high anion mobility in the bulk of an oxygen vacancy-rich n = 2 Ruddlesden-Popper material correlating with rapid oxygen <span class="hlt">exchange</span>. Furthermore this is in contrast with the similar <span class="hlt">surface</span> <span class="hlt">exchange</span> rates which we may expect due to similar <span class="hlt">surface</span> compositions across all three samples. This paper conclude that experimental limitations lead to inherent convolution of <span class="hlt">surface</span> and bulk rates, and that <span class="hlt">surface</span> <span class="hlt">exchange</span> steps are not likely to be rate limiting in oxygen incorporation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26642083','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26642083"><span>Gaseous and Freely-Dissolved PCBs in the Lower Great Lakes Based on Passive Sampling: Spatial Trends and <span class="hlt">Air</span>-Water <span class="hlt">Exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Ying; Wang, Siyao; McDonough, Carrie A; Khairy, Mohammed; Muir, Derek C G; Helm, Paul A; Lohmann, Rainer</p> <p>2016-05-17</p> <p>Polyethylene passive sampling was performed to quantify gaseous and freely dissolved polychlorinated biphenyls (PCBs) in the <span class="hlt">air</span> and water of Lakes Erie and Ontario during 2011-2012. In view of differing physical characteristics and the impacts of historical contamination by PCBs within these lakes, spatial variation of PCB concentrations and <span class="hlt">air</span>-water <span class="hlt">exchange</span> across these lakes may be expected. Both lakes displayed statistically similar aqueous and atmospheric PCB concentrations. Total aqueous concentrations of 29 PCBs ranged from 1.5 pg L(-1) in the open lake of Lake Erie (site E02) in 2011 spring to 105 pg L(-1) in Niagara (site On05) in 2012 summer, while total atmospheric concentrations were 7.7-634 pg m(-3) across both lakes. A west-to-east gradient was observed for aqueous PCBs in Lake Erie. River discharge and localized influences (e.g., sediment resuspension and regional alongshore transport) likely dominated spatial trends of aqueous PCBs in both lakes. <span class="hlt">Air</span>-water <span class="hlt">exchange</span> fluxes of Σ7PCBs ranged from -2.4 (±1.9) ng m(-2) day(-1) (deposition) in Sheffield (site E03) to 9.0 (±3.1) ng m(-2) day(-1) (volatilization) in Niagara (site On05). Net volatilization of PCBs was the primary trend across most sites and periods. Almost half of variation in <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes was attributed to the difference in aqueous concentrations of PCBs. Uncertainty analysis in fugacity ratios and mass fluxes in <span class="hlt">air</span>-water <span class="hlt">exchange</span> of PCBs indicated that PCBs have reached or approached equilibrium only at the eastern Lake Erie and along the Canadian shore of Lake Ontario sites, where <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes dominated atmospheric concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JPhCS.395a2048M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JPhCS.395a2048M"><span>A Novel Approach to <span class="hlt">Model</span> the <span class="hlt">Air</span>-Side Heat Transfer in Microchannel Condensers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martínez-Ballester, S.; Corberán, José-M.; Gonzálvez-Maciá, J.</p> <p>2012-11-01</p> <p>The work presents a <span class="hlt">model</span> (Fin1D×3) for microchannel condensers and gas coolers. The paper focusses on the description of the novel approach employed to <span class="hlt">model</span> the <span class="hlt">air</span>-side heat transfer. The <span class="hlt">model</span> applies a segment-by-segment discretization to the heat <span class="hlt">exchanger</span> adding, in each segment, a specific bi-dimensional grid to the <span class="hlt">air</span> flow and fin wall. Given this discretization, the fin theory is applied by using a continuous piecewise function for the fin wall temperature. It allows taking into account implicitly the heat conduction between tubes along the fin, and the unmixed <span class="hlt">air</span> influence on the heat capacity. The <span class="hlt">model</span> has been validated against experimental data resulting in predicted capacity errors within ± 5%. Differences on prediction results and computational cost were studied and compared with the previous authors' <span class="hlt">model</span> (Fin2D) and with other simplified <span class="hlt">model</span>. Simulation time of the proposed <span class="hlt">model</span> was reduced one order of magnitude respect the Fin2D's time retaining its same accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=64331&Lab=NERL&keyword=evapotranspiration&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=64331&Lab=NERL&keyword=evapotranspiration&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>A COUPLED LAND-<span class="hlt">SURFACE</span> AND DRY DEPOSITION <span class="hlt">MODEL</span> AND COMPARISON TO FIELD MEASUREMENTS OF <span class="hlt">SURFACE</span> HEAT, MOISTURE, AND OZONE FLUXES</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 have developed a coupled land-<span class="hlt">surface</span> and dry deposition <span class="hlt">model</span> for realistic treatment of <span class="hlt">surface</span> fluxes of heat, moisture, and chemical dry deposition within a comprehensive <span class="hlt">air</span> quality <span class="hlt">modeling</span> system. A new land-<span class="hlt">surface</span> <span class="hlt">model</span> (LSM) with explicit treatment of soil moisture...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A13G0307W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A13G0307W"><span>How important is getting the land <span class="hlt">surface</span> energy <span class="hlt">exchange</span> correct in WRF for wind energy forecasting?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wharton, S.; Simpson, M.; Osuna, J. L.; Newman, J. F.; Biraud, S.</p> <p>2013-12-01</p> <p>Wind power forecasting is plagued with difficulties in accurately predicting the occurrence and intensity of atmospheric conditions at the heights spanned by industrial-scale turbines (~ 40 to 200 m above ground level). Better simulation of the relevant physics would enable operational practices such as integration of large fractions of wind power into power grids, scheduling maintenance on wind energy facilities, and deciding design criteria based on complex loads for next-generation turbines and siting. Accurately simulating the <span class="hlt">surface</span> energy processes in numerical <span class="hlt">models</span> may be critically important for wind energy forecasting as energy <span class="hlt">exchange</span> at the <span class="hlt">surface</span> strongly drives atmospheric mixing (i.e., stability) in the lower layers of the planetary boundary layer (PBL), which in turn largely determines wind shear and turbulence at heights found in the turbine rotor-disk. We hypothesize that simulating accurate a <span class="hlt">surface</span>-atmosphere energy coupling should lead to more accurate predictions of wind speed and turbulence at heights within the turbine rotor-disk. Here, we tested 10 different land <span class="hlt">surface</span> <span class="hlt">model</span> configurations in the Weather Research and Forecasting (WRF) <span class="hlt">model</span> including Noah, Noah-MP, SSiB, Pleim-Xiu, RUC, and others to evaluate (1) the accuracy of simulated <span class="hlt">surface</span> energy fluxes to flux tower measurements, (2) the accuracy of forecasted wind speeds to observations at rotor-disk heights, and (3) the sensitivity of forecasting hub-height rotor disk wind speed to the choice of land <span class="hlt">surface</span> <span class="hlt">model</span>. WRF was run for four, two-week periods covering both summer and winter periods over the Southern Great Plains ARM site in Oklahoma. Continuous measurements of <span class="hlt">surface</span> energy fluxes and lidar-based wind speed, direction and turbulence were also available. The SGP ARM site provided an ideal location for this evaluation as it centrally located in the wind-rich Great Plains and multi-MW wind farms are rapidly expanding in the area. We found significant differences in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A21B0049O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A21B0049O"><span>Evaluation of Day and Nighttime Lower Tropospheric Ozone from <span class="hlt">Air</span> Quality <span class="hlt">Models</span> using TES and Ozonesondes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Osterman, G. B.; Neu, J. L.; Eldering, A.; Pinder, R. W.; Tang, Y.; McQueen, J.</p> <p>2012-12-01</p> <p>At night, ozone can be transported long distances above the <span class="hlt">surface</span> inversion layer without chemical destruction or deposition. As the boundary layer breaks up in the morning, this nocturnal ozone can be mixed down to the <span class="hlt">surface</span> and rapidly increase ozone concentrations at a rate that can rival chemical ozone production. Most regional scale <span class="hlt">models</span> that are used for <span class="hlt">air</span> quality forecasts and ozone source attribution do not adequately capture nighttime ozone concentrations and transport. We combine ozone profile data from the NASA Earth Observing System (EOS) Tropospheric Emission Spectrometer (TES) and other sensors, ozonesonde data collected during the INTEX Ozonesonde Network Study (IONS), EPA <span class="hlt">Air</span>Now ground station ozone data, the Community Multi-Scale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span>, and the National <span class="hlt">Air</span> Quality Forecast Capability (NAQFC) <span class="hlt">model</span> to examine <span class="hlt">air</span> quality events during August 2006. We present both aggregated statistics and case-study analyses that assess the relationship between the <span class="hlt">models</span>' ability to reproduce <span class="hlt">surface</span> <span class="hlt">air</span> quality events and their ability to capture the vertical distribution of ozone both during the day and at night. We perform the comparisons looking at the geospatial dependence in the differences between the measurements and <span class="hlt">models</span> under different <span class="hlt">surface</span> ozone conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26538177','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26538177"><span>Gas <span class="hlt">exchange</span> and dive characteristics of the free-swimming backswimmer Anisops deanei.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jones, Karl K; Snelling, Edward P; Watson, Amy P; Seymour, Roger S</p> <p>2015-11-01</p> <p>Many aquatic insects utilise <span class="hlt">air</span> bubbles on the <span class="hlt">surface</span> of their bodies to supply O2 while they dive. The bubbles can simply store O2, as in the case of an '<span class="hlt">air</span> store', or they can act as a physical 'gas gill', extracting O2 from the water. Backswimmers of the genus Anisops augment their <span class="hlt">air</span> store with O2 from haemoglobin cells located in the abdomen. The O2 release from the haemoglobin helps stabilise bubble volume, enabling backswimmers to remain near neutrally buoyant for a period of the dive. It is generally assumed that the backswimmer <span class="hlt">air</span> store does not act as a gas gill and that gas <span class="hlt">exchange</span> with the water is negligible. This study combines measurements of dive characteristics under different exotic gases (N2, He, SF6, CO) with mathematical <span class="hlt">modelling</span>, to show that the <span class="hlt">air</span> store of the backswimmer Anisops deanei does <span class="hlt">exchange</span> gases with the water. Our results indicate that approximately 20% of O2 consumed during a dive is obtained directly from the water. Oxygen from the water complements that released from the haemoglobin, extending the period of near-neutral buoyancy and increasing dive duration. © 2015. Published by The Company of Biologists Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869090','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869090"><span>Self-defrosting recuperative <span class="hlt">air-to-air</span> heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Drake, Richard L.</p> <p>1993-01-01</p> <p>A heat <span class="hlt">exchanger</span> includes a stationary spirally or concentrically wound heat <span class="hlt">exchanger</span> core with rotating baffles on upper and lower ends thereof. The rotating baffles include rotating inlets and outlets which are in communication with respective fixed inlets and outlets via annuli. The rotation of the baffles causes a concurrent rotation of the temperature distribution within the stationary <span class="hlt">exchanger</span> core, thereby preventing frost build-up in some applications and preventing the formation of hot spots in other applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C31D..01L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C31D..01L"><span>Gas <span class="hlt">exchange</span> in the ice zone: the role of small waves and big animals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loose, B.; Takahashi, A.; Bigdeli, A.</p> <p>2016-12-01</p> <p>The balance of <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> and net biological carbon fixation determine the transport and transformation of carbon dioxide and methane in the ocean. <span class="hlt">Air</span>-sea gas <span class="hlt">exchange</span> is mostly driven by upper ocean physics, but biology can also play a role. In the open ocean, gas <span class="hlt">exchange</span> increases proportionate to the square of wind speed. When sea ice is present, this dependence breaks down in part because breaking waves and <span class="hlt">air</span> bubble entrainment are damped out by interactions between sea ice and the wave field. At the same time, sea ice motions, formation, melt, and even sea ice-associated organisms can act to introduce turbulence and <span class="hlt">air</span> bubbles into the upper ocean, thereby enhancing <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span>. We take advantage of the knowledge advances of upper ocean physics including bubble dynamics to formulate a <span class="hlt">model</span> for <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> in the sea ice zone. Here, we use the <span class="hlt">model</span> to examine the role of small-scale waves and diving animals that trap <span class="hlt">air</span> for insulation, including penguins, seals and polar bears. We compare these processes to existing parameterizations of wave and bubble dynamics in the open ocean, to observe how sea ice both mitigates and locally enhances <span class="hlt">air</span>-sea gas transfer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGC51D0449R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGC51D0449R"><span>Trends in <span class="hlt">Surface</span> Temperature from <span class="hlt">AIRS</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruzmaikin, A.; Aumann, H. H.</p> <p>2014-12-01</p> <p>To address possible causes of the current hiatus in the Earth's global temperature we investigate the trends and variability in the <span class="hlt">surface</span> temperature using retrievals obtained from the measurements by the Atmospheric Infrared Sounder (<span class="hlt">AIRS</span>) and its companion instrument, the Advanced Microwave Sounding Unit (AMSU), onboard of Aqua spacecraft in 2002-2014. The data used are L3 monthly means on a 1x1degree spatial grid. We separate the land and ocean temperatures, as well as temperatures in Artic, Antarctic and desert regions. We find a monotonic positive trend for the land temperature but not for the ocean temperature. The difference in the regional trends can help to explain why the global <span class="hlt">surface</span> temperature remains almost unchanged but the frequency of occurrence of the extreme events increases under rising anthropogenic forcing. The results are compared with the <span class="hlt">model</span> studies. This work was supported by the Jet Propulsion Laboratory of the California Institute of Technology, under a contract with the National Aeronautics and Space Administration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/143941','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/143941"><span>Self-defrosting recuperative <span class="hlt">air-to-air</span> heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Drake, R.L.</p> <p>1993-12-28</p> <p>A heat <span class="hlt">exchanger</span> is described which includes a stationary spirally or concentrically wound heat <span class="hlt">exchanger</span> core with rotating baffles on upper and lower ends thereof. The rotating baffles include rotating inlets and outlets which are in communication with respective fixed inlets and outlets via annuli. The rotation of the baffles causes a concurrent rotation of the temperature distribution within the stationary <span class="hlt">exchanger</span> core, thereby preventing frost build-up in some applications and preventing the formation of hot spots in other applications. 3 figures.</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/2012EOSTr..93..213L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EOSTr..93..213L"><span>Developing <span class="hlt">air</span> quality forecasts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Pius; Saylor, Rick; Meagher, James</p> <p>2012-05-01</p> <p>Third International Workshop on <span class="hlt">Air</span> Quality Forecasting Research; Potomac, Maryland, 29 November to 1 December 2011 Elevated concentrations of both near-<span class="hlt">surface</span> ozone (O3) and fine particulate matter smaller than 2.5 micrometers in diameter have been implicated in increased mortality and other human health impacts. In light of these known influences on human health, many governments around the world have instituted <span class="hlt">air</span> quality forecasting systems to provide their citizens with advance warning of impending poor <span class="hlt">air</span> quality so that they can take actions to limit exposure. In an effort to improve the performance of <span class="hlt">air</span> quality forecasting systems and provide a forum for the <span class="hlt">exchange</span> of the latest research in <span class="hlt">air</span> quality <span class="hlt">modeling</span>, the International Workshop on <span class="hlt">Air</span> Quality Forecasting Research (IWAQFR) was established in 2009 and is cosponsored by the U.S. National Oceanic and Atmospheric Administration (NOAA), Environment Canada (EC), and the World Meteorological Organization (WMO). The steering committee for IWAQFR's establishment was composed of Véronique Bouchet, Mike Howe, and Craig Stoud (EC); Greg Carmichael (University of Iowa); Paula Davidson and Jim Meagher (NOAA); and Liisa Jalkanen (WMO). The most recent workshop took place in Maryland.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21175183','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21175183"><span>A generalized ligand-<span class="hlt">exchange</span> strategy enabling sequential <span class="hlt">surface</span> functionalization of colloidal nanocrystals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dong, Angang; Ye, Xingchen; Chen, Jun; Kang, Yijin; Gordon, Thomas; Kikkawa, James M; Murray, Christopher B</p> <p>2011-02-02</p> <p>The ability to engineer <span class="hlt">surface</span> properties of nanocrystals (NCs) is important for various applications, as many of the physical and chemical properties of nanoscale materials are strongly affected by the <span class="hlt">surface</span> chemistry. Here, we report a facile ligand-<span class="hlt">exchange</span> approach, which enables sequential <span class="hlt">surface</span> functionalization and phase transfer of colloidal NCs while preserving the NC size and shape. Nitrosonium tetrafluoroborate (NOBF4) is used to replace the original organic ligands attached to the NC <span class="hlt">surface</span>, stabilizing the NCs in various polar, hydrophilic media such as N,N-dimethylformamide for years, with no observed aggregation or precipitation. This approach is applicable to various NCs (metal oxides, metals, semiconductors, and dielectrics) of different sizes and shapes. The hydrophilic NCs obtained can subsequently be further functionalized using a variety of capping molecules, imparting different <span class="hlt">surface</span> functionalization to NCs depending on the molecules employed. Our work provides a versatile ligand-<span class="hlt">exchange</span> strategy for NC <span class="hlt">surface</span> functionalization and represents an important step toward controllably engineering the <span class="hlt">surface</span> properties of NCs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27136304','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27136304"><span>Soil concentrations, occurrence, sources and estimation of <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of polychlorinated biphenyls in Indian cities.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chakraborty, Paromita; Zhang, Gan; Li, Jun; Selvaraj, Sakthivel; Breivik, Knut; Jones, Kevin C</p> <p>2016-08-15</p> <p>Past studies have shown potentially increasing levels of polychlorinated biphenyls (PCBs) in the Indian environment. This is the first attempt to investigate the occurrence of PCBs in <span class="hlt">surface</span> soil and estimate diffusive <span class="hlt">air</span>-soil <span class="hlt">exchange</span>, both on a regional scale as well as at local level within the metropolitan environment of India. From the north, New Delhi and Agra, east, Kolkata, west, Mumbai and Goa and Chennai and Bangalore in the southern India were selected for this study. 33 PCB congeners were quantified in <span class="hlt">surface</span> soil and possible sources were derived using positive matrix factorization <span class="hlt">model</span>. Net flux directions of PCBs were estimated in seven major metropolitan cities of India along urban-suburban-rural transects. Mean Σ33PCBs concentration in soil (12ng/g dry weight) was nearly twice the concentration found in global background soil, but in line with findings from Pakistan and urban sites of China. Higher abundance of the heavier congeners (6CB-8CB) was prevalent mostly in the urban centers. Cities like Chennai, Mumbai and Kolkata with evidence of ongoing PCB sources did not show significant correlation with soil organic carbon (SOC). This study provides evidence that soil is acting as sink for heavy weight PCB congeners and source for lighter congeners. Atmospheric transport is presumably a controlling factor for occurrence of PCBs in less polluted sites of India. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060016349&hterms=urbanization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Durbanization','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060016349&hterms=urbanization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Durbanization"><span>The Atlanta Urban Heat Island Mitigation and <span class="hlt">Air</span> Quality <span class="hlt">Modeling</span> Project: How High-Resoution Remote Sensing Data Can Improve <span class="hlt">Air</span> Quality <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Quattrochi, Dale A.; Estes, Maurice G., Jr.; Crosson, William L.; Khan, Maudood N.</p> <p>2006-01-01</p> <p>The Atlanta Urban Heat Island and <span class="hlt">Air</span> Quality Project had its genesis in Project ATLANTA (ATlanta Land use Analysis: Temperature and <span class="hlt">Air</span> quality) that began in 1996. Project ATLANTA examined how high-spatial resolution thermal remote sensing data could be used to derive better measurements of the Urban Heat Island effect over Atlanta. We have explored how these thermal remote sensing, as well as other imaged datasets, can be used to better characterize the urban landscape for improved <span class="hlt">air</span> quality <span class="hlt">modeling</span> over the Atlanta area. For the <span class="hlt">air</span> quality <span class="hlt">modeling</span> project, the National Land Cover Dataset and the local scale Landpro99 dataset at 30m spatial resolutions have been used to derive land use/land cover characteristics for input into the MM5 mesoscale meteorological <span class="hlt">model</span> that is one of the foundations for the Community Multiscale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span> to assess how these data can improve output from CMAQ. Additionally, land use changes to 2030 have been predicted using a Spatial Growth <span class="hlt">Model</span> (SGM). SGM simulates growth around a region using population, employment and travel demand forecasts. <span class="hlt">Air</span> quality <span class="hlt">modeling</span> simulations were conducted using both current and future land cover. Meteorological <span class="hlt">modeling</span> simulations indicate a 0.5 C increase in daily maximum <span class="hlt">air</span> temperatures by 2030. <span class="hlt">Air</span> quality <span class="hlt">modeling</span> simulations show substantial differences in relative contributions of individual atmospheric pollutant constituents as a result of land cover change. Enhanced boundary layer mixing over the city tends to offset the increase in ozone concentration expected due to higher <span class="hlt">surface</span> temperatures as a result of urbanization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H23D1723L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H23D1723L"><span>3D numerical <span class="hlt">modeling</span> of hyporheic <span class="hlt">exchange</span> processes in fractal riverbed</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, A.; Aubeneau, A.</p> <p>2017-12-01</p> <p>The subsurface region receiving stream water is known as the hyporheic zone and the flow of water in and out of this zone is called hyporheic <span class="hlt">exchange</span>. The hyporheic zone is populated by biofilms and is a hotspot for nutrient uptake and contaminant transformation. Traditionally, pumping <span class="hlt">models</span> predicting the head distribution over the riverbed boundary are used to obtain the velocity field in the subsurface. However, past research has largely overlooked the nonlinearity of the turbulent flow above the bumpy riverbed. The main objective of this research is to investigate the effect of spatial and temporal heterogeneity created by turbulent flow on hyporheic <span class="hlt">exchange</span> and residence time distribution in fractal channel beds. The 3-D fractal riverbed is created from the power spectrum. Large-Eddy Simulation is used to provide the pressure field over the benthic boundary. Finally, Darcian fluxes in the sub-<span class="hlt">surface</span> are calculated and hyporheic travel times computed using random walks. <span class="hlt">Surface</span> and subsurface transport processes are represented explicitly and can be studied in detail. Our results suggest that (1) Eddies and wakes around the dunes force the <span class="hlt">exchange</span> (2) The bigger the dunes, the greater the influence of turbulence (3) Turbulence induces more <span class="hlt">exchange</span> than pumping predicts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150003353','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150003353"><span>Method and Apparatus for Measuring <span class="hlt">Surface</span> <span class="hlt">Air</span> Pressure</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lin, Bing (Inventor); Hu, Yongxiang (Inventor)</p> <p>2014-01-01</p> <p>The present invention is directed to an apparatus and method for remotely measuring <span class="hlt">surface</span> <span class="hlt">air</span> pressure. In one embodiment, the method of the present invention utilizes the steps of transmitting a signal having multiple frequencies into the atmosphere, measuring the transmitted/reflected signal to determine the relative received power level of each frequency and then determining the <span class="hlt">surface</span> <span class="hlt">air</span> pressure based upon the attenuation of the transmitted frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28186210','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28186210"><span>US residential building <span class="hlt">air</span> <span class="hlt">exchange</span> rates: new perspectives to improve decision making at vapor intrusion sites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Reichman, Rivka; Shirazi, Elham; Colliver, Donald G; Pennell, Kelly G</p> <p>2017-02-22</p> <p>Vapor intrusion (VI) is well-known to be difficult to characterize because indoor <span class="hlt">air</span> (IA) concentrations exhibit considerable temporal and spatial variability in homes throughout impacted communities. To overcome this and other limitations, most VI science has focused on subsurface processes; however there is a need to understand the role of aboveground processes, especially building operation, in the context of VI exposure risks. This tutorial review focuses on building <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) and provides a review of literature related building AERs to inform decision making at VI sites. Commonly referenced AER values used by VI regulators and practitioners do not account for the variability in AER values that have been published in indoor <span class="hlt">air</span> quality studies. The information presented herein highlights that seasonal differences, short-term weather conditions, home age and <span class="hlt">air</span> conditioning status, which are well known to influence AERs, are also likely to influence IA concentrations at VI sites. Results of a 3D VI <span class="hlt">model</span> in combination with relevant AER values reveal that IA concentrations can vary more than one order of magnitude due to <span class="hlt">air</span> conditioning status and one order of magnitude due to house age. Collectively, the data presented strongly support the need to consider AERs when making decisions at VI sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4198866','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4198866"><span>Uncoupled <span class="hlt">surface</span> spin induced <span class="hlt">exchange</span> bias in α-MnO2 nanowires</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Wenxian; Zeng, Rong; Sun, Ziqi; Tian, Dongliang; Dou, Shixue</p> <p>2014-01-01</p> <p>We have studied the microstructure, <span class="hlt">surface</span> states, valence fluctuations, magnetic properties, and <span class="hlt">exchange</span> bias effect in MnO2 nanowires. High purity α-MnO2 rectangular nanowires were synthesized by a facile hydrothermal method with microwave-assisted procedures. The microstructure analysis indicates that the nanowires grow in the [0 0 1] direction with the (2 1 0) plane as the <span class="hlt">surface</span>. Mn3+ and Mn2+ ions are not found in the system by X-ray photoelectron spectroscopy. The effective magnetic moment of the manganese ions fits in with the theoretical and experimental values of Mn4+ very well. The uncoupled spins in 3d3 orbitals of the Mn4+ ions in MnO6 octahedra on the rough <span class="hlt">surface</span> are responsible for the net magnetic moment. Spin glass behavior is observed through magnetic measurements. Furthermore, the <span class="hlt">exchange</span> bias effect is observed for the first time in pure α-MnO2 phase due to the coupling of the <span class="hlt">surface</span> spin glass with the antiferromagnetic α-MnO2 matrix. These α-MnO2 nanowires, with a spin-glass-like behavior and with an <span class="hlt">exchange</span> bias effect excited by the uncoupled <span class="hlt">surface</span> spins, should therefore inspire further study concerning the origin, theory, and applicability of <span class="hlt">surface</span> structure induced magnetism in nanostructures. PMID:25319531</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.146g4303L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.146g4303L"><span>Ab initio state-specific N2 + O dissociation and <span class="hlt">exchange</span> <span class="hlt">modeling</span> for molecular simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luo, Han; Kulakhmetov, Marat; Alexeenko, Alina</p> <p>2017-02-01</p> <p>Quasi-classical trajectory (QCT) calculations are used in this work to calculate state-specific N2(X1Σ ) +O(3P ) →2 N(4S ) +O(3P ) dissociation and N2(X1Σ ) +O(3P ) →NO(X2Π ) +N(4S ) <span class="hlt">exchange</span> cross sections and rates based on the 13A″ and 13A' ab initio potential energy <span class="hlt">surface</span> by Gamallo et al. [J. Chem. Phys. 119, 2545-2556 (2003)]. The calculations consider translational energies up to 23 eV and temperatures between 1000 K and 20 000 K. Vibrational favoring is observed for dissociation reaction at the whole range of collision energies and for <span class="hlt">exchange</span> reaction around the dissociation limit. For the same collision energy, cross sections for v = 30 are 4 to 6 times larger than those for the ground state. The <span class="hlt">exchange</span> reaction has an effective activation energy that is dependent on the initial rovibrational level, which is different from dissociation reaction. In addition, the <span class="hlt">exchange</span> cross sections have a maximum when the total collision energy (TCE) approaches dissociation energy. The calculations are used to generate compact QCT-derived state-specific dissociation (QCT-SSD) and QCT-derived state-specific <span class="hlt">exchange</span> (QCT-SSE) <span class="hlt">models</span>, which describe over 1 × 106 cross sections with about 150 <span class="hlt">model</span> parameters. The <span class="hlt">models</span> can be used directly within direct simulation Monte Carlo and computational fluid dynamics simulations. Rate constants predicted by the new <span class="hlt">models</span> are compared to the experimental measurements, direct QCT calculations and predictions by other <span class="hlt">models</span> that include: TCE <span class="hlt">model</span>, Bose-Candler QCT-based <span class="hlt">exchange</span> <span class="hlt">model</span>, Macheret-Fridman dissociation <span class="hlt">model</span>, Macheret's <span class="hlt">exchange</span> <span class="hlt">model</span>, and Park's two-temperature <span class="hlt">model</span>. The new <span class="hlt">models</span> match QCT-calculated and experimental rates within 30% under nonequilibrium conditions while other <span class="hlt">models</span> under predict by over an order of magnitude under vibrationally-cold conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.6352P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.6352P"><span>Importance of ocean mesoscale variability for <span class="hlt">air</span>-sea interactions in the Gulf of Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Putrasahan, D. A.; Kamenkovich, I.; Le Hénaff, M.; Kirtman, B. P.</p> <p>2017-06-01</p> <p>Mesoscale variability of currents in the Gulf of Mexico (GoM) can affect oceanic heat advection and <span class="hlt">air</span>-sea heat <span class="hlt">exchanges</span>, which can influence climate extremes over North America. This study is aimed at understanding the influence of the oceanic mesoscale variability on the lower atmosphere and <span class="hlt">air</span>-sea heat <span class="hlt">exchanges</span>. The study contrasts global climate <span class="hlt">model</span> (GCM) with 0.1° ocean resolution (high resolution; HR) with its low-resolution counterpart (1° ocean resolution with the same 0.5° atmosphere resolution; LR). The LR simulation is relevant to current generation of GCMs that are still unable to resolve the oceanic mesoscale. Similar to observations, HR exhibits positive correlation between sea <span class="hlt">surface</span> temperature (SST) and <span class="hlt">surface</span> turbulent heat flux anomalies, while LR has negative correlation. For HR, we decompose lateral advective heat fluxes in the upper ocean into mean (slowly varying) and mesoscale-eddy (fast fluctuations) components. We find that the eddy flux divergence/convergence dominates the lateral advection and correlates well with the SST anomalies and <span class="hlt">air</span>-sea latent heat <span class="hlt">exchanges</span>. This result suggests that oceanic mesoscale advection supports warm SST anomalies that in turn feed <span class="hlt">surface</span> heat flux. We identify anticyclonic warm-core circulation patterns (associated Loop Current and rings) which have an average diameter of 350 km. These warm anomalies are sustained by eddy heat flux convergence at submonthly time scales and have an identifiable imprint on <span class="hlt">surface</span> turbulent heat flux, atmospheric circulation, and convective precipitation in the northwest portion of an averaged anticyclone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019169','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019169"><span>Study of transient behavior of finned coil heat <span class="hlt">exchangers</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rooke, S. P.; Elissa, M. G.</p> <p>1993-01-01</p> <p>The status of research on the transient behavior of finned coil cross-flow heat <span class="hlt">exchangers</span> using single phase fluids is reviewed. Applications with available analytical or numerical solutions are discussed. Investigation of water-to-<span class="hlt">air</span> type cross-flow finned tube heat <span class="hlt">exchangers</span> is examined through the use of simplified governing equations and an up-wind finite difference scheme. The degenerate case of zero <span class="hlt">air</span>-side capacitance rate is compared with available exact solution. Generalization of the numerical <span class="hlt">model</span> is discussed for application to multi-row multi-circuit heat <span class="hlt">exchangers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26995905','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26995905"><span>[Effect of <span class="hlt">air</span> temperature and rainfall on wetland ecosystem CO2 <span class="hlt">exchange</span> in China].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chu, Xiao-jing; Han, Guang-xuan</p> <p>2015-10-01</p> <p>Wetland can be a potential efficient sink to reduce global warming due to its higher primary productivity and lower carbon decomposition rate. While there has been a series progress on the influence mechanism of ecosystem CO2 <span class="hlt">exchange</span> over China' s wetlands, a systematic metaanalysis of data still needs to be improved. We compiled data of ecosystem CO2 <span class="hlt">exchange</span> of 21 typical wetland vegetation types in China from 29 papers and carried out an integrated analysis of <span class="hlt">air</span> temperature and precipitation effects on net ecosystem CO2 <span class="hlt">exchange</span> (NEE), ecosystem respiration (Reco), gross primary productivity (GPP), the response of NEE to PAR, and the response of Reco to temperature. The results showed that there were significant responses (P<0.05) of NEE (R2 = 50%, R2=57%), GPP (R2 = 60%, R2 = 50%) Reco (R2 = 44%, R2=50%) with increasing <span class="hlt">air</span> temperature and enhanced precipitation on the annual scale. On the growing season scale, <span class="hlt">air</span> temperature accounted for 50% of the spatial variation of NEE, 36% of GPP and 19% of Reco, respectively. Both NEE (R2 = 33%) and GPP (R2 =25%) were correlated positively with precipitation (P<0.05). However, the relationship between Reco and precipitation was not significant (P>0.05). Across different Chinese wetlands, both precipitation and temperature had no significant effect on apparent quantum yield (α) or ecosystem respiration in the daytime (Reco,day, P>0.05). The maximum photosynthesis rate (Amax) was remarkably correlated with precipitation (P <0.01), but not with <span class="hlt">air</span> temperature. Besides, there was no significant correlation between basal respiration (Rref) and precipitation (P>0.05). Precipitation was negatively correlated with temperature sensitivity of Reco (Q10, P<0.05). Furthermore, temperature accounted for 35% and 46% of the variations in temperature sensitivity of Reco (Q10) and basal respiration (Rref P<0.05), respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1225372','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1225372"><span>External reflection FTIR of peptide monolayer films in situ at the <span class="hlt">air</span>/water interface: experimental design, spectra-structure correlations, and effects of hydrogen-deuterium <span class="hlt">exchange</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>Flach, C R; Brauner, J W; Taylor, J W; Baldwin, R C; Mendelsohn, R</p> <p>1994-01-01</p> <p>A Fourier transform infrared spectrometer has been interfaced with a <span class="hlt">surface</span> balance and a new external reflection infrared sampling accessory, which permits the acquisition of spectra from protein monolayers in situ at the <span class="hlt">air</span>/water interface. The accessory, a sample shuttle that permits the collection of spectra in alternating fashion from sample and background troughs, reduces interference from water vapor rotation-vibration bands in the amide I and amide II regions of protein spectra (1520-1690 cm-1) by nearly an order of magnitude. Residual interference from water vapor absorbance ranges from 50 to 200 microabsorbance units. The performance of the device is demonstrated through spectra of synthetic peptides designed to adopt alpha-helical, antiparallel beta-sheet, mixed beta-sheet/beta-turn, and unordered conformations at the <span class="hlt">air</span>/water interface. The extent of <span class="hlt">exchange</span> on the <span class="hlt">surface</span> can be monitored from the relative intensities of the amide II and amide I modes. Hydrogen-deuterium <span class="hlt">exchange</span> may lower the amide I frequency by as much as 11-12 cm-1 for helical secondary structures. This shifts the vibrational mode into a region normally associated with unordered structures and leads to uncertainties in the application of algorithms commonly used for determination of secondary structure from amide I contours of proteins in D2O solution. PMID:7919013</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHyd..552..421R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHyd..552..421R"><span>Experimental calibration and validation of sewer/<span class="hlt">surface</span> flow <span class="hlt">exchange</span> equations in steady and unsteady flow conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rubinato, Matteo; Martins, Ricardo; Kesserwani, Georges; Leandro, Jorge; Djordjević, Slobodan; Shucksmith, James</p> <p>2017-09-01</p> <p>The linkage between sewer pipe flow and floodplain flow is recognised to induce an important source of uncertainty within two-dimensional (2D) urban flood <span class="hlt">models</span>. This uncertainty is often attributed to the use of empirical hydraulic formulae (the one-dimensional (1D) weir and orifice steady flow equations) to achieve data-connectivity at the linking interface, which require the determination of discharge coefficients. Because of the paucity of high resolution localised data for this type of flows, the current understanding and quantification of a suitable range for those discharge coefficients is somewhat lacking. To fulfil this gap, this work presents the results acquired from an instrumented physical <span class="hlt">model</span> designed to study the interaction between a pipe network flow and a floodplain flow. The full range of sewer-to-<span class="hlt">surface</span> and <span class="hlt">surface</span>-to-sewer flow conditions at the <span class="hlt">exchange</span> zone are experimentally analysed in both steady and unsteady flow regimes. Steady state measured discharges are first analysed considering the relationship between the energy heads from the sewer flow and the floodplain flow; these results show that existing weir and orifice formulae are valid for describing the flow <span class="hlt">exchange</span> for the present physical <span class="hlt">model</span>, and yield new calibrated discharge coefficients for each of the flow conditions. The measured <span class="hlt">exchange</span> discharges are also integrated (as a source term) within a 2D numerical flood <span class="hlt">model</span> (a finite volume solver to the 2D Shallow Water Equations (SWE)), which is shown to reproduce the observed coefficients. This calibrated numerical <span class="hlt">model</span> is then used to simulate a series of unsteady flow tests reproduced within the experimental facility. Results show that the numerical <span class="hlt">model</span> overestimated the values of mean surcharge flow rate. This suggests the occurrence of additional head losses in unsteady conditions which are not currently accounted for within flood <span class="hlt">models</span> calibrated in steady flow conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950047978&hterms=urban+landscape&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Durban%2Blandscape','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950047978&hterms=urban+landscape&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Durban%2Blandscape"><span>Estimating the urban bias of <span class="hlt">surface</span> shelter temperatures using upper-<span class="hlt">air</span> and satellite data. Part 1: Development of <span class="hlt">models</span> predicting <span class="hlt">surface</span> shelter temperatures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Epperson, David L.; Davis, Jerry M.; Bloomfield, Peter; Karl, Thomas R.; Mcnab, Alan L.; Gallo, Kevin P.</p> <p>1995-01-01</p> <p>Multiple regression techniques were used to predict <span class="hlt">surface</span> shelter temperatures based on the time period 1986-89 using upper-<span class="hlt">air</span> data from the European Centre for Medium-Range Weather Forecasts (ECMWF) to represent the background climate and site-specific data to represent the local landscape. Global monthly mean temperature <span class="hlt">models</span> were developed using data from over 5000 stations available in the Global Historical Climate Network (GHCN). Monthly maximum, mean, and minimum temperature <span class="hlt">models</span> for the United States were also developed using data from over 1000 stations available in the U.S. Cooperative (COOP) Network and comparative monthly mean temperature <span class="hlt">models</span> were developed using over 1150 U.S. stations in the GHCN. Three-, six-, and full-variable <span class="hlt">models</span> were developed for comparative purposes. Inferences about the variables selected for the various <span class="hlt">models</span> were easier for the GHCN <span class="hlt">models</span>, which displayed month-to-month consistency in which variables were selected, than for the COOP <span class="hlt">models</span>, which were assigned a different list of variables for nearly every month. These and other results suggest that global calibration is preferred because data from the global spectrum of physical processes that control <span class="hlt">surface</span> temperatures are incorporated in a global <span class="hlt">model</span>. All of the <span class="hlt">models</span> that were developed in this study validated relatively well, especially the global <span class="hlt">models</span>. Recalibration of the <span class="hlt">models</span> with validation data resulted in only slightly poorer regression statistics, indicating that the calibration list of variables was valid. Predictions using data from the validation dataset in the calibrated equation were better for the GHCN <span class="hlt">models</span>, and the globally calibrated GHCN <span class="hlt">models</span> generally provided better U.S. predictions than the U.S.-calibrated COOP <span class="hlt">models</span>. Overall, the GHCN and COOP <span class="hlt">models</span> explained approximately 64%-95% of the total variance of <span class="hlt">surface</span> shelter temperatures, depending on the month and the number of <span class="hlt">model</span> variables. In addition, root</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvL.108g4503K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvL.108g4503K"><span>Skating on a Film of <span class="hlt">Air</span>: Drops Impacting on a <span class="hlt">Surface</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kolinski, John M.; Rubinstein, Shmuel M.; Mandre, Shreyas; Brenner, Michael P.; Weitz, David A.; Mahadevan, L.</p> <p>2012-02-01</p> <p>The commonly accepted description of drops impacting on a <span class="hlt">surface</span> typically ignores the essential role of the <span class="hlt">air</span> that is trapped between the impacting drop and the <span class="hlt">surface</span>. Here we describe a new imaging modality that is sensitive to the behavior right at the <span class="hlt">surface</span>. We show that a very thin film of <span class="hlt">air</span>, only a few tens of nanometers thick, remains trapped between the falling drop and the <span class="hlt">surface</span> as the drop spreads. The thin film of <span class="hlt">air</span> serves to lubricate the drop enabling the fluid to skate on the <span class="hlt">air</span> film laterally outward at surprisingly high velocities, consistent with theoretical predictions. Eventually this thin film of <span class="hlt">air</span> breaks down as the fluid wets the <span class="hlt">surface</span> via a spinodal-like mechanism. Our results show that the dynamics of impacting drops are much more complex than previously thought, with a rich array of unexpected phenomena that require rethinking classic paradigms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70157483','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70157483"><span>1DTempPro V2: new features for inferring groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</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>Koch, Franklin W.; Voytek, Emily B.; Day-Lewis, Frederick D.; Healy, Richard W.; Briggs, Martin A.; Lane, John W.; Werkema, Dale D.</p> <p>2016-01-01</p> <p>A new version of the computer program 1DTempPro extends the original code to include new capabilities for (1) automated parameter estimation, (2) layer heterogeneity, and (3) time-varying specific discharge. The code serves as an interface to the U.S. Geological Survey <span class="hlt">model</span> VS2DH and supports analysis of vertical one-dimensional temperature profiles under saturated flow conditions to assess groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> and estimate hydraulic conductivity for cases where hydraulic head is known.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12387399','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12387399"><span>Investigation into the importance of the stomatal pathway in the <span class="hlt">exchange</span> of PCBs between <span class="hlt">air</span> and plants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barber, Jonathan L; Kurt, Perihan B; Thomas, Gareth O; Kerstiens, Gerhard; Jones, Kevin C</p> <p>2002-10-15</p> <p>The transfer of persistent organic pollutants (POPs) from <span class="hlt">air</span> to vegetation is an important <span class="hlt">air-surface</span> <span class="hlt">exchange</span> process that affects global cycling and can result in human and wildlife exposure via the terrestrial food chain. To improve understanding of this process, the role of stomata in uptake of gas-phase polychlorinated biphenyls (PCBs) was investigated using Hemerocallis x hybrida "Black Eyed Stella", a plant with a high stomatal density. Uptake of PCBs was monitored over a 72-h period in the presence and absence of light. Uptake rates were significantly greater in illuminated (stomata open) plants than unilluminated (stomata closed) plants for 18 of the 28 measured PCB congeners (p < 0.05). Depuration of PCBs was monitored in a subsequent experiment over a period of 3 weeks. Levels after 3 weeks of depuration time were still much higher than the concentration prior to contamination. Tri- and tetrachlorinated PCBs showed the greatest depuration, with less than 20% and 50% of accumulated PCBs respectively remaining, while approximately 70% of higher chlorinated PCB congeners remained in the plants at the end of the experiment. Treatments with/without light (to control stomatal opening during uptake) and with/without abscisic acid (ABA) application (to control stomatal opening during depuration) were compared. After contamination indoors for 3 days, there was a significantly higher concentration of PCBs (p < 0.05) in the light contaminated plants than the dark-contaminated plants for 13 of the 28 measured PCB congeners. The ABA treatment affected depuration of PCB-18 only. "Light/ABA-treated" plants had a significantly slower depuration rate for PCB-18 than "light/untreated", "dark/ABA-treated", and "dark/untreated" plants (p < 0.05). The results of the study indicate that there is a stomatal effect on the rate of <span class="hlt">exchange</span> of PCBs between Hemerocallis leaves and <span class="hlt">air</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhA.121..505D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhA.121..505D"><span>Elasticity of the hair cover in <span class="hlt">air</span>-retaining Salvinia <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ditsche, Petra; Gorb, Elena; Mayser, Matthias; Gorb, Stanislav; Schimmel, Thomas; Barthlott, Wilhelm</p> <p>2015-11-01</p> <p>Immersed in water superhydrophobic <span class="hlt">surfaces</span> (e.g., lotus) maintain thin temporary <span class="hlt">air</span> films. In certain aquatic plants and animals, these films are thicker and more persistent. Floating ferns of the genus Salvinia show elaborated hierarchical superhydrophobic <span class="hlt">surface</span> structures: a hairy cover of complex trichomes. In the case of S. molesta, they are eggbeater shaped and topped by hydrophilic tips, which pin the <span class="hlt">air</span>-water interface and prevent rupture of contact. It has been proposed that these trichomes can oscillate with the <span class="hlt">air</span>-water interface, when turbulences occur and thereby stabilize the <span class="hlt">air</span> film. The deformability of such arrays of trichomes requires a certain elasticity of the structures. In this study, we determined the stiffness of the trichome coverage of S. molesta and three other Salvinia species. Our results confirm the elasticity of the trichome coverage in all investigated Salvinia species. We did not reveal a clear relationship between the time of <span class="hlt">air</span> retention and stiffness of the trichome coverage, which means that the <span class="hlt">air</span> retention function is additionally dependent on different parameters, e.g., the trichome shape and <span class="hlt">surface</span> free energy. These data are not only interesting for Salvinia biology, but also important for the development of biomimetic <span class="hlt">air</span>-retaining <span class="hlt">surfaces</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.18002011B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.18002011B"><span>The influence of flow modification on <span class="hlt">air</span> and PCM temperatures in an accumulative heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borcuch, Marcin; Musiał, Michał; Sztekler, Karol; Kalawa, Wojciech; Gumuła, Stanisław; Stefański, Sebastian</p> <p>2018-06-01</p> <p>The paper presents the influence of flow modification on the operation of an accumulative heat <span class="hlt">exchanger</span>. This device can be used as a regenerator in ventilation and <span class="hlt">air</span> supply systems. A heat <span class="hlt">exchanger</span> uses ceresine (a mixture of paraffins) as a phase change material (PCM). The aim of this research was to determine the effect of flow modification on temperature distribution and pressure drops in the device. The introduction contains a short description of the test stand used, including the accumulative heat <span class="hlt">exchanger</span>, the guide vanes, and the locations of measurement and control equipment. We found that additional objects limited vortex structures, increased the inside temperature, and dropped the pressure along the heat <span class="hlt">exchanger</span>. Guidelines for further research are proposed and briefly discussed.</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('https://www.ncbi.nlm.nih.gov/pubmed/26782201','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26782201"><span>The Pathway for Oxygen: Tutorial <span class="hlt">Modelling</span> on Oxygen Transport from <span class="hlt">Air</span> to Mitochondrion: The Pathway for Oxygen.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bassingthwaighte, James B; Raymond, Gary M; Dash, Ranjan K; Beard, Daniel A; Nolan, Margaret</p> <p>2016-01-01</p> <p>The 'Pathway for Oxygen' is captured in a set of <span class="hlt">models</span> describing quantitative relationships between fluxes and driving forces for the flux of oxygen from the external <span class="hlt">air</span> source to the mitochondrial sink at cytochrome oxidase. The intervening processes involve convection, membrane permeation, diffusion of free and heme-bound O2 and enzymatic reactions. While this system's basic elements are simple: ventilation, alveolar gas <span class="hlt">exchange</span> with blood, circulation of the blood, perfusion of an organ, uptake by tissue, and consumption by chemical reaction, integration of these pieces quickly becomes complex. This complexity led us to construct a tutorial on the ideas and principles; these first PathwayO2 <span class="hlt">models</span> are simple but quantitative and cover: (1) a 'one-alveolus lung' with airway resistance, lung volume compliance, (2) bidirectional transport of solute gasses like O2 and CO2, (3) gas <span class="hlt">exchange</span> between alveolar <span class="hlt">air</span> and lung capillary blood, (4) gas solubility in blood, and circulation of blood through the capillary syncytium and back to the lung, and (5) blood-tissue gas <span class="hlt">exchange</span> in capillaries. These open-source <span class="hlt">models</span> are at Physiome.org and provide background for the many respiratory <span class="hlt">models</span> there.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150006832','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150006832"><span>Impact of Bay-Breeze Circulations on <span class="hlt">Surface</span> <span class="hlt">Air</span> Quality and Boundary Layer Export</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Loughner, Christopher P.; Tzortziou, Maria; Follette-Cook, Melanie; Pickering, Kenneth E.; Goldberg, Daniel; Satam, Chinmay; Weinheimer, Andrew; Crawford, James H.; Knapp, David J.; Montzka, Denise D.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150006832'); toggleEditAbsImage('author_20150006832_show'); toggleEditAbsImage('author_20150006832_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150006832_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150006832_hide"></p> <p>2014-01-01</p> <p>Meteorological and <span class="hlt">air</span>-quality <span class="hlt">model</span> simulations are analyzed alongside observations to investigate the role of the Chesapeake Bay breeze on <span class="hlt">surface</span> <span class="hlt">air</span> quality, pollutant transport, and boundary layer venting. A case study was conducted to understand why a particular day was the only one during an 11-day ship-based field campaign on which <span class="hlt">surface</span> ozone was not elevated in concentration over the Chesapeake Bay relative to the closest upwind site and why high ozone concentrations were observed aloft by in situ aircraft observations. Results show that southerly winds during the overnight and early-morning hours prevented the advection of <span class="hlt">air</span> pollutants from the Washington, D.C., and Baltimore, Maryland, metropolitan areas over the <span class="hlt">surface</span> waters of the bay. A strong and prolonged bay breeze developed during the late morning and early afternoon along the western coastline of the bay. The strength and duration of the bay breeze allowed pollutants to converge, resulting in high concentrations locally near the bay-breeze front within the Baltimore metropolitan area, where they were then lofted to the top of the planetary boundary layer (PBL). Near the top of the PBL, these pollutants were horizontally advected to a region with lower PBL heights, resulting in pollution transport out of the boundary layer and into the free troposphere. This elevated layer of <span class="hlt">air</span> pollution aloft was transported downwind into New England by early the following morning where it likely mixed down to the <span class="hlt">surface</span>, affecting <span class="hlt">air</span> quality as the boundary layer grew.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DPS....4920301P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DPS....4920301P"><span><span class="hlt">Surface</span> Modification and <span class="hlt">Surface</span> - Subsurface <span class="hlt">Exchange</span> Processes on Europa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phillips, Cynthia B.; Molaro, Jamie; Hand, Kevin P.</p> <p>2017-10-01</p> <p>The <span class="hlt">surface</span> of Jupiter’s moon Europa is modified by exogenic processes such as sputtering, gardening, radiolysis, sulfur ion implantation, and thermal processing, as well as endogenic processes including tidal shaking, mass wasting, and the effects of subsurface tectonic and perhaps cryovolcanic activity. New materials are created or deposited on the <span class="hlt">surface</span> (radiolysis, micrometeorite impacts, sulfur ion implantation, cryovolcanic plume deposits), modified in place (thermal segregation, sintering), transported either vertically or horizontally (sputtering, gardening, mass wasting, tectonic and cryovolcanic activity), or lost from Europa completely (sputtering, plumes, larger impacts). Some of these processes vary spatially, as visible in Europa’s leading-trailing hemisphere brightness asymmetry.Endogenic geologic processes also vary spatially, depending on terrain type. The <span class="hlt">surface</span> can be classified into general landform categories that include tectonic features (ridges, bands, cracks); disrupted “chaos-type” terrain (chaos blocks, matrix, domes, pits, spots); and impact craters (simple, complex, multi-ring). The spatial distribution of these terrain types is relatively random, with some differences in apex-antiapex cratering rates and latitudinal variation in chaos vs. tectonic features.In this work, we extrapolate <span class="hlt">surface</span> processes and rates from the top meter of the <span class="hlt">surface</span> in conjunction with global estimates of transport and resurfacing rates. We combine near-<span class="hlt">surface</span> modification with an estimate of <span class="hlt">surface</span>-subsurface (and vice versa) transport rates for various geologic terrains based on an average of proposed formation mechanisms, and a spatial distribution of each landform type over Europa’s <span class="hlt">surface</span> area.Understanding the rates and mass balance for each of these processes, as well as their spatial and temporal variability, allows us to estimate <span class="hlt">surface</span> - subsurface <span class="hlt">exchange</span> rates over the average <span class="hlt">surface</span> age (~50myr) of Europa. Quantifying the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P52B..08P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P52B..08P"><span><span class="hlt">Surface</span> Modification and <span class="hlt">Surface</span> - Subsurface <span class="hlt">Exchange</span> Processes on Europa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phillips, C. B.; Molaro, J.; Hand, K. P.</p> <p>2017-12-01</p> <p>The <span class="hlt">surface</span> of Jupiter's moon Europa is modified by exogenic processes such as sputtering, gardening, radiolysis, sulfur ion implantation, and thermal processing, as well as endogenic processes including tidal shaking, mass wasting, and the effects of subsurface tectonic and perhaps cryovolcanic activity. New materials are created or deposited on the <span class="hlt">surface</span> (radiolysis, micrometeorite impacts, sulfur ion implantation, cryovolcanic plume deposits), modified in place (thermal segregation, sintering), transported either vertically or horizontally (sputtering, gardening, mass wasting, tectonic and cryovolcanic activity), or lost from Europa completely (sputtering, plumes, larger impacts). Some of these processes vary spatially, as visible in Europa's leading-trailing hemisphere brightness asymmetry. Endogenic geologic processes also vary spatially, depending on terrain type. The <span class="hlt">surface</span> can be classified into general landform categories that include tectonic features (ridges, bands, cracks); disrupted "chaos-type" terrain (chaos blocks, matrix, domes, pits, spots); and impact craters (simple, complex, multi-ring). The spatial distribution of these terrain types is relatively random, with some differences in apex-antiapex cratering rates and latitudinal variation in chaos vs. tectonic features. In this work, we extrapolate <span class="hlt">surface</span> processes and rates from the top meter of the <span class="hlt">surface</span> in conjunction with global estimates of transport and resurfacing rates. We combine near-<span class="hlt">surface</span> modification with an estimate of <span class="hlt">surface</span>-subsurface (and vice versa) transport rates for various geologic terrains based on an average of proposed formation mechanisms, and a spatial distribution of each landform type over Europa's <span class="hlt">surface</span> area. Understanding the rates and mass balance for each of these processes, as well as their spatial and temporal variability, allows us to estimate <span class="hlt">surface</span> - subsurface <span class="hlt">exchange</span> rates over the average <span class="hlt">surface</span> age ( 50myr) of Europa. Quantifying the timescale</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810068621','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810068621"><span>Investigation of Effectiveness of <span class="hlt">Air</span>-Heating a Hollow Steel Propeller for Protection Against Icing. 3: 25% Partitioned Blades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mulholland, Donald R.; Perkins, Porter J.</p> <p>1948-01-01</p> <p>The icing protection obtained from an internally <span class="hlt">air</span>-heated propeller blade partitioned to confine the heated <span class="hlt">air</span> forward of 25-percent chord was investigated in the NACA Cleveland icing research tunnel. A production-<span class="hlt">model</span> hollow steel propeller was modified with an Internal radial partition at 25-percent chord and with shank and tip openings to admit and exhaust the heated <span class="hlt">air</span>. Temperatures were measured on the blade <span class="hlt">surfaces</span> and in the heated-<span class="hlt">air</span> system during tunnel icing conditions. Heat-<span class="hlt">exchanger</span> effectiveness and photographs of Ice formations on the blades were obtained. <span class="hlt">Surface</span> temperature measurements indicated that confining the heated <span class="hlt">air</span> forward of the 25-percent chord gave.a more economical distribution of the applied heat as compared with unpartitioned and 50-percent partitioned blades, by dissipating a greater percentage of the available heat at the leading edge. At a propeller speed of 850 rpm, a heating rate of 7000 Btu per hour per blade at a shank <span class="hlt">air</span> temperature of 400 F provided adequate Icing protection at ambient-<span class="hlt">air</span> temperatures of 23 F but not at temperatures as low as 15 F. With the heating rate used, a heat-<span class="hlt">exchanger</span> effectiveness of 77 percent was obtained as compared to 56 percent for 50-percent partitioned and 47 percent for unpartitioned blades.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26436513','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26436513"><span>Concentrations, Trends, and <span class="hlt">Air</span>-Water <span class="hlt">Exchange</span> of PAHs and PBDEs Derived from Passive Samplers in Lake Superior in 2011.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ruge, Zoe; Muir, Derek; Helm, Paul; Lohmann, Rainer</p> <p>2015-12-01</p> <p>Polycyclic aromatic hydrocarbons (PAHs) and polybrominated diphenylethers (PBDEs) are both currently released into the environment from anthropogenic activity. Both are hence primarily associated with populated or industrial areas, although wildfires can be an important source of PAHs, as well. Polyethylene passive samplers (PEs) were simultaneously deployed in <span class="hlt">surface</span> water and near <span class="hlt">surface</span> atmosphere to determine spatial trends and <span class="hlt">air</span>-water gaseous <span class="hlt">exchange</span> of 21 PAHs and 11 PBDEs at 19 sites across Lake Superior in 2011. <span class="hlt">Surface</span> water and atmospheric PAH concentrations were greatest at urban sites (up to 65 ng L(-1) and 140 ng m(-3), respectively, averaged from June to October). Near populated regions, PAHs displayed net <span class="hlt">air</span>-to-water deposition, but were near equilibrium off-shore. Retene, probably depositing following major wildfires in the region, dominated dissolved PAH concentrations at most Lake Superior sites. Atmospheric and dissolved PBDEs were greatest near urban and populated sites (up to 6.8 pg L(-1) and 15 pg m(-3), respectively, averaged from June to October), dominated by BDE-47. At most coastal sites, there was net gaseous deposition of BDE-47, with less brominated congeners contributing to Sault Ste. Marie and eastern open lake fluxes. Conversely, the central open lake and Eagle Harbor sites generally displayed volatilization of PBDEs into the atmosphere, mainly BDE-47.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/12353','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/12353"><span>Focus State Roadway Departure Safety Plans and High Friction <span class="hlt">Surface</span> Treatments Peer <span class="hlt">Exchange</span> : an RPSCB Peer <span class="hlt">Exchange</span></span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2014-08-01</p> <p>This report summarizes the Focus State Roadway Departure Safety Plans and High Friction <span class="hlt">Surface</span> Treatments Peer <span class="hlt">Exchange</span>, held in Birmingham, Alabama, sponsored by the Federal Highway Administration (FHWA) Office of Safetys Roadway Safety Professi...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JAtS...60.2429M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JAtS...60.2429M"><span>Cooperative Atmosphere-<span class="hlt">Surface</span> <span class="hlt">Exchange</span> Study-1999.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moeng, Chin-Hoh; Poulos, Gregory S.; Lemone, Margaret A.</p> <p>2003-10-01</p> <p><span class="hlt">Surface</span>-station, radiosonde, and Doppler minisodar data from the Cooperative Atmosphere-<span class="hlt">Surface</span> <span class="hlt">Exchange</span> Study-1997 (CASES-97) field project, collected in a 60-km-wide array in the lower Walnut River watershed (terrain variation 150 m) southeast of Wichita, Kansas, are used to study the relationship of the change of the 2-m potential temperature 2m with station elevation ze, 2m/ze ,ze to the ambient wind and thermal stratification /z ,z during fair-weather nights. As in many previous studies, predawn 2m varies linearly with ze, and ,ze ,z over a depth h that represents the maximum elevation range of the stations. Departures from the linear 2m-elevation relationship (<IMG border="0" src="/charent/GREEK/UNACCENTED/CAP/Theta.gif">,ze line) are related to vegetation (cool for vegetation, warm for bare ground), local terrain (drainage flows from nearby hills, although a causal relationship is not established), and the formation of a cold pool at lower elevations on some days.<IMG SRC="/images/indent.gif" WIDTH=15 HEIGHT=10 BORDER=0 ALT="">The near-<span class="hlt">surface</span> flow and its evolution are functions of the Froude number Fr = S/(Nh), where S is the mean wind speed from the <span class="hlt">surface</span> to h, and N is the corresponding Brunt-Väisälä frequency. The near-<span class="hlt">surface</span> wind is coupled to the ambient flow for Fr = 3.3, based on where the straight line relating <IMG border="0" src="/charent/GREEK/UNACCENTED/CAP/Theta.gif">,ze to ln Fr intersects the ln Fr axis. Under these conditions, <IMG border="0" src="/charent/GREEK/UNACCENTED/CAP/Theta.gif">2m is constant horizontally even though <IMG border="0" src="/charent/GREEK/UNACCENTED/CAP/Theta.gif">,z > 0, suggesting that near-<span class="hlt">surface</span> <span class="hlt">air</span> moves up- and downslope dry adiabatically. However, <IMG border="0" src="/charent/GREEK/UNACCENTED/CAP/Theta.gif">2m cools (or warms) everywhere at the same rate. The lowest Froude numbers are associated with drainage flows, while intermediate values characterize regimes with intermediate behavior. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23157102','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23157102"><span>[Use of the <span class="hlt">air</span>-Q laryngeal airway and tube <span class="hlt">exchanger</span> in a case of difficult tracheal extubation after maxillectomy].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Komasawa, Nobuyasu; Ueki, Ryusuke; Iwasaki, Yohei; Tatara, Tsuneo; Tashiro, Chikara; Kaminoh, Yoshiroh</p> <p>2012-10-01</p> <p>A 79-year-old man was diagnosed with maxillary cancer and underwent total maxillectomy under general anesthesia. The oropharyngeal airway was needed for efficient mask ventilation during anesthesia induction. The maxilla was totally resected and reconstructed with skin from a femoral flap. Tracheal extubation was considered to be difficult given that mask ventilation was contraindicated due to reconstruction of the maxilla. After inserting a tube <span class="hlt">exchanger</span> (TE) into the trachea, the tracheal tube was <span class="hlt">exchanged</span> with an <span class="hlt">air</span>-Q laryngeal airway through the TE. After confirming effective ventilation with the <span class="hlt">air</span>-Q mask, the patient was awakened from anesthesia. We confirmed sufficient spontaneous breathing and no active bleeding in the pharynx. After re-inserting the TE thorough <span class="hlt">air</span>-Q, the <span class="hlt">air</span>-Q was removed, followed by removal of the TE. These findings suggest that the <span class="hlt">air</span>-Q and TE were effective in a case of difficult extubation after maxillectomy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18640753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18640753"><span>Dry deposition and soil-<span class="hlt">air</span> gas <span class="hlt">exchange</span> of polychlorinated biphenyls (PCBs) in an industrial area.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bozlaker, Ayse; Odabasi, Mustafa; Muezzinoglu, Aysen</p> <p>2008-12-01</p> <p>Ambient <span class="hlt">air</span> and dry deposition, and soil samples were collected at the Aliaga industrial site in Izmir, Turkey. Atmospheric total (particle+gas) Sigma(41)-PCB concentrations were higher in summer (3370+/-1617 pg m(-3), average+SD) than in winter (1164+/-618 pg m(-3)), probably due to increased volatilization with temperature. Average particulate Sigma(41)-PCBs dry deposition fluxes were 349+/-183 and 469+/-328 ng m(-2) day(-1) in summer and winter, respectively. Overall average particulate deposition velocity was 5.5+/-3.5 cm s(-1). The spatial distribution of Sigma(41)-PCB soil concentrations (n=48) showed that the iron-steel plants, ship dismantling facilities, refinery and petrochemicals complex are the major sources in the area. Calculated <span class="hlt">air</span>-soil <span class="hlt">exchange</span> fluxes indicated that the contaminated soil is a secondary source to the atmosphere for lighter PCBs and as a sink for heavier ones. Comparable magnitude of gas <span class="hlt">exchange</span> and dry particle deposition fluxes indicated that both mechanisms are equally important for PCB movement between <span class="hlt">air</span> and soil in Aliaga.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22894100','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22894100"><span>Measurement of <span class="hlt">air</span> <span class="hlt">exchange</span> rates in different indoor environments using continuous CO2 sensors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>You, Yan; Niu, Can; Zhou, Jian; Liu, Yating; Bai, Zhipeng; Zhang, Jiefeng; He, Fei; Zhang, Nan</p> <p>2012-01-01</p> <p>A new <span class="hlt">air</span> <span class="hlt">exchange</span> rate (AER) monitoring method using continuous CO2 sensors was developed and validated through both laboratory experiments and field studies. Controlled laboratory simulation tests were conducted in a 1-m3 environmental chamber at different AERs (0.1-10.0 hr(-1)). AERs were determined using the decay method based on box <span class="hlt">model</span> assumptions. Field tests were conducted in classrooms, dormitories, meeting rooms and apartments during 2-5 weekdays using CO2 sensors coupled with data loggers. Indoor temperature, relative humidity (RH), and CO2 concentrations were continuously monitored while outdoor parameters combined with on-site climate conditions were recorded. Statistical results indicated that good laboratory performance was achieved: duplicate precision was within 10%, and the measured AERs were 90%-120% of the real AERs. Average AERs were 1.22, 1.37, 1.10, 1.91 and 0.73 hr(-1) in dormitories, <span class="hlt">air</span>-conditioned classrooms, classrooms with an <span class="hlt">air</span> circulation cooling system, reading rooms, and meeting rooms, respectively. In an elderly particulate matter exposure study, all the homes had AER values ranging from 0.29 to 3.46 hr(-1) in fall, and 0.12 to 1.39 hr(-1) in winter with a median AER of 1.15.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H41M..03L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H41M..03L"><span>Atmospheric sensitivity to land <span class="hlt">surface</span> changes: comparing the impact of albedo, roughness, and evaporative resistance on near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature using an idealized land <span class="hlt">model</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lague, M. M.; Swann, A. L. S.; Bonan, G. B.</p> <p>2017-12-01</p> <p>Past studies have demonstrated how changes in vegetation can impact the atmosphere; however, it is often difficult to identify the exact physical pathway through which vegetation changes drive an atmospheric response. <span class="hlt">Surface</span> properties (such as vegetation color, or height) control <span class="hlt">surface</span> energy fluxes, which feed back on the atmosphere on both local and global scales by modifying temperatures, cloud cover, and energy gradients. Understanding how land <span class="hlt">surface</span> properties influence energy fluxes is crucial for improving our understanding of how vegetation change - past, present, and future - impacts the atmosphere, global climate, and people. We explore the sensitivity of the atmosphere to perturbations of three land <span class="hlt">surface</span> properties - albedo, roughness, and evaporative resistance - using an idealized land <span class="hlt">model</span> coupled to an Earth System <span class="hlt">Model</span>. We derive a relationship telling us how large a change in each <span class="hlt">surface</span> property is required to drive a local 0.1 K change in 2m <span class="hlt">air</span> temperature. Using this idealized framework, we are able to separate the influence on the atmosphere of each individual <span class="hlt">surface</span> property. We demonstrate that the impact of each <span class="hlt">surface</span> property on the atmosphere is spatially variable - that is, a similar change in vegetation can have different climate impacts if made in different locations. This analysis not only improves our understanding of how the land system can influence climate, but also provides us with a set of theoretical limits on the potential climate impact of arbitrary vegetation change (natural or anthropogenic).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70177056','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70177056"><span>Water levels and groundwater and <span class="hlt">surface</span>-water <span class="hlt">exchanges</span> in lakes of the northeast Twin Cities Metropolitan Area, Minnesota, 2002 through 2015</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Jones, Perry M.; Trost, Jared J.; Erickson, Melinda L.</p> <p>2016-10-19</p> <p>OverviewThis study assessed lake-water levels and regional and local groundwater and <span class="hlt">surface</span>-water <span class="hlt">exchanges</span> near northeast Twin Cities Metropolitan Area lakes applying three approaches: statistical analysis, field study, and groundwater-flow <span class="hlt">modeling</span>.  Statistical analyses of lake levels were completed to assess the effect of physical setting and climate on lake-level fluctuations of selected lakes. A field study of groundwater and <span class="hlt">surface</span>-water interactions in selected lakes was completed to (1) estimate potential percentages of <span class="hlt">surface</span>-water contributions to well water across the northeast Twin Cities Metropolitan Area, (2) estimate general ages for waters extracted from the wells, and (3) assess groundwater inflow to lakes and lake-water outflow to aquifers downgradient from White Bear Lake.  Groundwater flow was simulated using a steady-state, groundwater-flow <span class="hlt">model</span> to assess regional groundwater and <span class="hlt">surface</span>-water <span class="hlt">exchanges</span> and the effects of groundwater withdrawals, climate, and other factors on water levels of northeast Twin Cities Metropolitan Area lakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=88581&keyword=e+AND+commerce&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=88581&keyword=e+AND+commerce&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>LINKING ETA <span class="hlt">MODEL</span> WITH THE COMMUNITY MULTISCALE <span class="hlt">AIR</span> QUALITY (CMAQ) <span class="hlt">MODELING</span> SYSTEM: OZONE BOUNDARY CONDITIONS</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>A prototype <span class="hlt">surface</span> ozone concentration forecasting <span class="hlt">model</span> system for the Eastern U.S. has been developed. The <span class="hlt">model</span> system is consisting of a regional meteorological and a regional <span class="hlt">air</span> quality <span class="hlt">model</span>. It demonstrated a strong prediction dependence on its ozone boundary conditions....</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006GeoRL..3314803Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006GeoRL..3314803Z"><span>Impacts of winter storms on <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Weiqing; Perrie, Will; Vagle, Svein</p> <p>2006-07-01</p> <p>The objective of this study is to investigate <span class="hlt">air</span>-sea gas <span class="hlt">exchange</span> during winter storms, using field measurements from Ocean Station Papa in the Northeast Pacific (50°N, 145°W). We show that increasing gas transfer rates are coincident with increasing winds and deepening depth of bubble penetration, and that this process depends on sea state. Wave-breaking is shown to be an important factor in the gas transfer velocity during the peaks of the storms, increasing the flux rates by up to 20%. Gas transfer rates and concentrations can exhibit asymmetry, reflecting a sudden increase with the onset of a storm, and gradual recovery stages.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018HMT....54..305C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018HMT....54..305C"><span>Experimental study on heat transfer performance of fin-tube <span class="hlt">exchanger</span> and PSHE for waste heat recovery</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Ting; Bae, Kyung Jin; Kwon, Oh Kyung</p> <p>2018-02-01</p> <p>In this paper, heat transfer characteristics of fin-tube heat <span class="hlt">exchanger</span> and primary <span class="hlt">surface</span> heat <span class="hlt">exchanger</span> (PSHE) used in waste heat recovery were investigated experimentally. The flow in the fin-tube heat <span class="hlt">exchanger</span> is cross flow and in PSHE counter flow. The variations of friction factor and Colburn j factor with <span class="hlt">air</span> mass flow rate, and Nu number with Re number are presented. Various comparison methods are used to evaluate heat transfer performance, and the results show that the heat transfer rate of the PSHE is on average 17.3% larger than that of fin-tube heat <span class="hlt">exchanger</span> when <span class="hlt">air</span> mass flow rate is ranging from 1.24 to 3.45 kg/min. However, the PSHE causes higher pressure drop, and the fin-tube heat <span class="hlt">exchanger</span> has a wider application range which leads to a 31.7% higher value of maximum heat transfer rate compared to that of the PSHE. Besides, under the same fan power per unit frontal <span class="hlt">surface</span>, a higher heat transfer rate value is given in the fin-tube heat <span class="hlt">exchanger</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1042892','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1042892"><span>Foundation Heat <span class="hlt">Exchanger</span> Final Report: Demonstration, Measured Performance, and Validated <span class="hlt">Model</span> and Design Tool</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>Hughes, Patrick; Im, Piljae</p> <p>2012-04-01</p> <p> <span class="hlt">exchanger</span> (FHX) has been coined to refer exclusively to ground heat <span class="hlt">exchangers</span> installed in the overcut around the basement walls. The primary technical challenge undertaken by this project was the development and validation of energy performance <span class="hlt">models</span> and design tools for FHX. In terms of performance <span class="hlt">modeling</span> and design, ground heat <span class="hlt">exchangers</span> in other construction excavations (e.g., utility trenches) are no different from conventional HGHX, and <span class="hlt">models</span> and design tools for HGHX already exist. This project successfully developed and validated energy performance <span class="hlt">models</span> and design tools so that FHX or hybrid FHX/HGHX systems can be engineered with confidence, enabling this technology to be applied in residential and light commercial buildings. The validated energy performance <span class="hlt">model</span> also addresses and solves another problem, the longstanding inadequacy in the way ground-building thermal interaction is represented in building energy <span class="hlt">models</span>, whether or not there is a ground heat <span class="hlt">exchanger</span> nearby. Two side-by-side, three-level, unoccupied research houses with walkout basements, identical 3,700 ft{sup 2} floor plans, and hybrid FHX/HGHX systems were constructed to provide validation data sets for the energy performance <span class="hlt">model</span> and design tool. The envelopes of both houses are very energy efficient and airtight, and the HERS ratings of the homes are 44 and 45 respectively. Both houses are mechanically ventilated with energy recovery ventilators, with space conditioning provided by water-to-<span class="hlt">air</span> heat pumps with 2 ton nominal capacities. Separate water-to-water heat pumps with 1.5 ton nominal capacities were used for water heating. In these unoccupied research houses, human impact on energy use (hot water draw, etc.) is simulated to match the national average. At House 1 the hybrid FHX/HGHX system was installed in 300 linear feet of excavation, and 60% of that was construction excavation (needed to construct the home). At House 2 the hybrid FHX/HGHX system was installed in 360 feet of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A53E2309Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A53E2309Y"><span>Effects of Northern Hemisphere Sea <span class="hlt">Surface</span> Temperature Changes on the Global <span class="hlt">Air</span> Quality</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yi, K.; Liu, J.</p> <p>2017-12-01</p> <p>The roles of regional sea <span class="hlt">surface</span> temperature (SST) variability on modulating the climate system and consequently the <span class="hlt">air</span> quality are investigated using the Community Earth System <span class="hlt">Model</span> (CESM). Idealized, spatially uniform SST anomalies of +/- 1 °C are superimposed onto the North Pacific, North Atlantic, and North Indian Oceans individually. Ignoring the response of natural emissions, our simulations suggest large seasonal and regional variability of <span class="hlt">surface</span> O3 and PM2.5 concentrations in response to SST anomalies, especially during boreal summers. Increasing the SST by 1 °C in one of the oceans generally decreases the <span class="hlt">surface</span> O3 concentrations from 1 to 5 ppbv while increases the anthropogenic PM2.5 concentrations from 0.5 to 3 µg m-3. We implement the integrated process rate (IPR) analysis in CESM and find that meteorological transport in response to SST changes is the key process causing <span class="hlt">air</span> pollutant perturbations in most cases. During boreal summers, the increase in tropical SST over different ocean basins enhances deep convection, which significantly increases the <span class="hlt">air</span> temperature over the upper troposphere and trigger large-scale subsidence over nearby and remote regions. These processes tend to increase tropospheric stability and suppress rainfall at lower mid-latitudes. Consequently, it reduces the vertical transport of O3 to the <span class="hlt">surface</span> while facilitating the accumulation of PM2.5 concentrations over most regions. In addition, this regional SST warming may also considerably suppress intercontinental transport of <span class="hlt">air</span> pollution as confirmed with idealized CO-like tracers. Our findings indicate a robust linkage between basin-scale SST variability and regional <span class="hlt">air</span> quality, which can help local <span class="hlt">air</span> quality management.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70102289','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70102289"><span><span class="hlt">Air</span>-water gas <span class="hlt">exchange</span> and CO2 flux in a mangrove-dominated estuary</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Ho, David T.; Ferrón, Sara; Engel, Victor C.; Larsen, Laurel G.; Barr, Jordan G.</p> <p>2014-01-01</p> <p>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 <span class="hlt">air</span>-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 <span class="hlt">air</span>-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 <span class="hlt">exchange</span> than predicted by commonly used wind speed/gas <span class="hlt">exchange</span> parameterizations. The results have important implications for carbon fluxes in mangrove ecosystems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://edg.epa.gov/metadata/catalog/search/resource/details.page?uuid=%7Ba7fd531c-b6ed-4edd-8b6d-20a28d71270f%7D','PESTICIDES'); return false;" href="https://edg.epa.gov/metadata/catalog/search/resource/details.page?uuid=%7Ba7fd531c-b6ed-4edd-8b6d-20a28d71270f%7D"><span>US EPA 2012 <span class="hlt">Air</span> Quality Fused <span class="hlt">Surface</span> for the Conterminous U.S. Map Service</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>This web service contains a polygon layer that depicts fused <span class="hlt">air</span> quality predictions for 2012 for census tracts in the conterminous United States. Fused <span class="hlt">air</span> quality predictions (for ozone and PM2.5) are <span class="hlt">modeled</span> using a Bayesian space-time downscaling fusion <span class="hlt">model</span> approach described in a series of three published journal papers: 1) (Berrocal, V., Gelfand, A. E. and Holland, D. M. (2012). Space-time fusion under error in computer <span class="hlt">model</span> output: an application to <span class="hlt">modeling</span> <span class="hlt">air</span> quality. Biometrics 68, 837-848; 2) Berrocal, V., Gelfand, A. E. and Holland, D. M. (2010). A bivariate space-time downscaler under space and time misalignment. The Annals of Applied Statistics 4, 1942-1975; and 3) Berrocal, V., Gelfand, A. E., and Holland, D. M. (2010). A spatio-temporal downscaler for output from numerical <span class="hlt">models</span>. J. of Agricultural, Biological,and Environmental Statistics 15, 176-197) is used to provide daily, predictive PM2.5 (daily average) and O3 (daily 8-hr maximum) <span class="hlt">surfaces</span> for 2012. Summer (O3) and annual (PM2.5) means calculated and published. The downscaling fusion <span class="hlt">model</span> uses both <span class="hlt">air</span> quality monitoring data from the National <span class="hlt">Air</span> Monitoring Stations/State and Local <span class="hlt">Air</span> Monitoring Stations (NAMS/SLAMS) and numerical output from the <span class="hlt">Models</span>-3/Community Multiscale <span class="hlt">Air</span> Quality (CMAQ). Currently, predictions at the US census tract centroid locations within the 12 km CMAQ domain are archived. Predictions at the CMAQ grid cell centroids, or any desired set of locations co</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://adsabs.harvard.edu/abs/2013JPS...243..946K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JPS...243..946K"><span>Numerical investigation of interfacial transport resistance due to water droplets in proton <span class="hlt">exchange</span> membrane fuel cell <span class="hlt">air</span> channels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koz, Mustafa; Kandlikar, Satish G.</p> <p>2013-12-01</p> <p>Oxygen transport resistance at the <span class="hlt">air</span> flow channel and gas diffusion layer (GDL) interface is needed in <span class="hlt">modelling</span> the performance of a proton <span class="hlt">exchange</span> membrane fuel cell (PEMFC). This resistance is expressed through the non-dimensional Sherwood number (Sh). The effect of the presence of a droplet on Sh is studied numerically in an isolated <span class="hlt">air</span> flow channel using a commercially available package, COMSOL Multiphysics®. A droplet is represented as a solid obstruction placed on the GDL-channel interface and centred along the channel width. The effect of a single droplet is first studied for a range of superficial mean <span class="hlt">air</span> velocities and droplet sizes. Secondly, the effect of droplet spacing on Sh is studied through simulations of two consecutive droplets. Lastly, multiple droplets in a row are studied as a more representative case of a PEMFC <span class="hlt">air</span> flow channel. The results show that the droplets significantly increase Sh above the fully developed value in the wake region. This enhancement increases with the number of droplets, droplet size, and superficial mean <span class="hlt">air</span> velocity. Moreover, the analogy between mass and heat transfer is investigated by comparing Sh to the equivalent Nusselt number.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920013253','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920013253"><span><span class="hlt">Modelling</span> and simulation of a heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Xia, Lei; Deabreu-Garcia, J. Alex; Hartley, Tom T.</p> <p>1991-01-01</p> <p>Two <span class="hlt">models</span> for two different control systems are developed for a parallel heat <span class="hlt">exchanger</span>. First by spatially lumping a heat <span class="hlt">exchanger</span> <span class="hlt">model</span>, a good approximate <span class="hlt">model</span> which has a high system order is produced. <span class="hlt">Model</span> reduction techniques are applied to these to obtain low order <span class="hlt">models</span> that are suitable for dynamic analysis and control design. The simulation method is discussed to ensure a valid simulation result.</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 fluxes and climate to orbital forcing changes in the Community Climate System <span class="hlt">Model</span></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 <span class="hlt">model</span> coupled to an ocean ecosystem <span class="hlt">model</span> is used to quantify the response of carbon fluxes 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 ice 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 fluxes of the same order. However, the differences in global net <span class="hlt">air</span>-sea carbon fluxes are small, which is due to several effects, two of which stand out: first, colder sea <span class="hlt">surface</span> temperature leads to a more effective solubility pump but also to increased sea ice concentration which blocks <span class="hlt">air</span>-sea <span class="hlt">exchange</span>, 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://hdl.handle.net/2060/20060021945','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060021945"><span>Conceptual Design of a Condensing Heat <span class="hlt">Exchanger</span> for Space Systems Using Porous Media</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hasan, Mohammad M.; Khan, Lutful I.; Nayagam, Vedha; Balasubramaniam, Ramaswamy</p> <p>2006-01-01</p> <p>Condensing heat <span class="hlt">exchangers</span> are used in many space applications in the thermal and humidity control systems. In the International Space Station (ISS), humidity control is achieved by using a water cooled fin <span class="hlt">surface</span> over which the moist <span class="hlt">air</span> condenses, followed by "slurper bars" that take in both the condensate and <span class="hlt">air</span> into a rotary separator and separates the water from <span class="hlt">air</span>. The use of a cooled porous substrate as the condensing <span class="hlt">surface</span> provides and attractive alternative that combines both heat removal as well as liquid/gas separation into a single unit. By selecting the pore sizes of the porous substrate a gravity independent operation may also be possible with this concept. Condensation of vapor into and on the porous <span class="hlt">surface</span> from the flowing <span class="hlt">air</span> and the removal of condensate from the porous substrate are the critical processes involved in the proposed concept. This paper describes some preliminary results of the proposed condensate withdrawal process and discusses the on-going design and development work of a porous media based condensing heat <span class="hlt">exchanger</span> at the NASA Glenn Research Center in collaboration with NASA Johnson Space Center.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AtmEn..43.3630B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AtmEn..43.3630B"><span><span class="hlt">Modelling</span> pesticide volatilization after soil application using the mechanistic <span class="hlt">model</span> Volt'<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>Bedos, Carole; Génermont, Sophie; Le Cadre, Edith; Garcia, Lucas; Barriuso, Enrique; Cellier, Pierre</p> <p></p> <p>Volatilization of pesticides participates in atmospheric contamination and affects environmental ecosystems including human welfare. <span class="hlt">Modelling</span> at relevant time and spatial scales is needed to better understand the complex processes involved in pesticide volatilization. Volt'<span class="hlt">Air</span>-Pesticides has been developed following a two-step procedure to study pesticide volatilization at the field scale and at a quarter time step. Firstly, Volt'<span class="hlt">Air</span>-NH 3 was adapted by extending the initial transfer of solutes to pesticides and by adding specific calculations for physico-chemical equilibriums as well as for the degradation of pesticides in soil. Secondly, the <span class="hlt">model</span> was evaluated in terms of 3 pesticides applied on bare soil (atrazine, alachlor, and trifluralin) which display a wide range of volatilization rates. A sensitivity analysis confirmed the relevance of tuning to K h. Then, using Volt'<span class="hlt">Air</span>-Pesticides, environmental conditions and emission fluxes of the pesticides were compared to fluxes measured under 2 environmental conditions. The <span class="hlt">model</span> fairly well described water temporal dynamics, soil <span class="hlt">surface</span> temperature, and energy budget. Overall, Volt'<span class="hlt">Air</span>-Pesticides estimates of the order of magnitude of the volatilization flux of all three compounds were in good agreement with the field measurements. The <span class="hlt">model</span> also satisfactorily simulated the decrease in the volatilization rate of the three pesticides during night-time as well as the decrease in the soil <span class="hlt">surface</span> residue of trifluralin before and after incorporation. However, the timing of the maximum flux rate during the day was not correctly described, thought to be linked to an increased adsorption under dry soil conditions. Thanks to Volt'<span class="hlt">Air</span>'s capacity to deal with pedo-climatic conditions, several existing parameterizations describing adsorption as a function of soil water content could be tested. However, this point requires further investigation. Practically speaking, Volt'<span class="hlt">Air</span>-Pesticides can be a useful tool to make</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACPD...1025033L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACPD...1025033L"><span>Evaluation of urban <span class="hlt">surface</span> parameterizations in the WRF <span class="hlt">model</span> using measurements during the Texas <span class="hlt">Air</span> Quality Study 2006 field campaign</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, S.-H.; Kim, S.-W.; Angevine, W. M.; Bianco, L.; McKeen, S. A.; Senff, C. J.; Trainer, M.; Tucker, S. C.; Zamora, R. J.</p> <p>2010-10-01</p> <p>The impact of urban <span class="hlt">surface</span> parameterizations in the WRF (Weather Research and Forecasting) <span class="hlt">model</span> on the simulation of local meteorological fields is investigated. The Noah land <span class="hlt">surface</span> <span class="hlt">model</span> (LSM), a modified LSM, and a single-layer urban canopy <span class="hlt">model</span> (UCM) have been compared, focusing on urban patches. The <span class="hlt">model</span> simulations were performed for 6 days from 12 August to 17 August during the Texas <span class="hlt">Air</span> Quality Study 2006 field campaign. Analysis was focused on the Houston-Galveston metropolitan area. The <span class="hlt">model</span> simulated temperature, wind, and atmospheric boundary layer (ABL) height were compared with observations from <span class="hlt">surface</span> meteorological stations (Continuous Ambient Monitoring Stations, CAMS), wind profilers, the NOAA Twin Otter aircraft, and the NOAA Research Vessel Ronald H. Brown. The UCM simulation showed better results in the comparison of ABL height and <span class="hlt">surface</span> temperature than the LSM simulations, whereas the original LSM overestimated both the <span class="hlt">surface</span> temperature and ABL height significantly in urban areas. The modified LSM, which activates hydrological processes associated with urban vegetation mainly through transpiration, slightly reduced warm and high biases in <span class="hlt">surface</span> temperature and ABL height. A comparison of <span class="hlt">surface</span> energy balance fluxes in an urban area indicated the UCM reproduces a realistic partitioning of sensible heat and latent heat fluxes, consequently improving the simulation of urban boundary layer. However, the LSMs have a higher Bowen ratio than the observation due to significant suppression of latent heat flux. The comparison results suggest that the subgrid heterogeneity by urban vegetation and urban morphological characteristics should be taken into account along with the associated physical parameterizations for accurate simulation of urban boundary layer if the region of interest has a large fraction of vegetation within the urban patch. <span class="hlt">Model</span> showed significant discrepancies in the specific meteorological conditions when nocturnal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23550960','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23550960"><span>1DTempPro: analyzing temperature profiles for groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Voytek, Emily B; Drenkelfuss, Anja; Day-Lewis, Frederick D; Healy, Richard; Lane, John W; Werkema, Dale</p> <p>2014-01-01</p> <p>A new computer program, 1DTempPro, is presented for the analysis of vertical one-dimensional (1D) temperature profiles under saturated flow conditions. 1DTempPro is a graphical user interface to the U.S. Geological Survey code Variably Saturated 2-Dimensional Heat Transport (VS2DH), which numerically solves the flow and heat-transport equations. Pre- and postprocessor features allow the user to calibrate VS2DH <span class="hlt">models</span> to estimate vertical groundwater/<span class="hlt">surface</span>-water <span class="hlt">exchange</span> and also hydraulic conductivity for cases where hydraulic head is known. Published 2013. This article is a U.S. Government work and is in the public domain in the USA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26931659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26931659"><span><span class="hlt">Air</span>-sea <span class="hlt">exchange</span> of gaseous mercury in the tropical coast (Luhuitou fringing reef) of the South China Sea, the Hainan Island, China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ci, Zhijia; Zhang, Xiaoshan; Wang, Zhangwei</p> <p>2016-06-01</p> <p>The <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of gaseous mercury (mainly Hg(0)) in the tropical ocean is an important part of the global Hg biogeochemical cycle, but the related investigations are limited. In this study, we simultaneously measured Hg(0) concentrations in <span class="hlt">surface</span> waters and overlaying <span class="hlt">air</span> in the tropical coast (Luhuitou fringing reef) of the South China Sea (SCS), Hainan Island, China, for 13 days on January-February 2015. The purpose of this study was to explore the temporal variation of Hg(0) concentrations in <span class="hlt">air</span> and <span class="hlt">surface</span> waters, estimate the <span class="hlt">air</span>-sea Hg(0) flux, and reveal their influencing factors in the tropical coastal environment. The mean concentrations (±SD) of Hg(0) in <span class="hlt">air</span> and total Hg (THg) in waters were 2.34 ± 0.26 ng m(-3) and 1.40 ± 0.48 ng L(-1), respectively. Both Hg(0) concentrations in waters (53.7 ± 18.8 pg L(-1)) and Hg(0)/THg ratios (3.8 %) in this study were significantly higher than those of the open water of the SCS in winter. Hg(0) in waters usually exhibited a clear diurnal variation with increased concentrations in daytime and decreased concentrations in nighttime, especially in cloudless days with low wind speed. Linear regression analysis suggested that Hg(0) concentrations in waters were positively and significantly correlated to the photosynthetically active radiation (PAR) (R (2) = 0.42, p < 0.001). <span class="hlt">Surface</span> waters were always supersaturated with Hg(0) compared to <span class="hlt">air</span> (the degree of saturation, 2.46 to 13.87), indicating that the <span class="hlt">surface</span> water was one of the atmospheric Hg(0) sources. The <span class="hlt">air</span>-sea Hg(0) fluxes were estimated to be 1.73 ± 1.25 ng m(-2) h(-1) with a large range between 0.01 and 6.06 ng m(-2) h(-1). The high variation of Hg(0) fluxes was mainly attributed to the greatly temporal variation of wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20355819','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20355819"><span>New insights into proton <span class="hlt">surface</span> mobility processes in PEMFC catalysts using isotopic <span class="hlt">exchange</span> methods.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ferreira-Aparicio, Paloma</p> <p>2009-09-01</p> <p>The <span class="hlt">surface</span> chemistry and the adsorption/desorption/<span class="hlt">exchange</span> behavior of a proton-<span class="hlt">exchange</span> membrane fuel cell catalyst are analyzed as a case study for the development of tailor-made support materials of enhanced performance and stability. By using H2, D2, and CO as probe molecules, the relevance of some <span class="hlt">surface</span> functional groups of the catalyst support on several diffusion processes taking place during the adsorption is shown. Sulfonic groups associated with the vulcanized carbon black <span class="hlt">surface</span> have been detected by means of spectroscopic techniques (X-ray photoelectron spectroscopy and Fourier transform infrared spectroscopy) and by analysis of the desorbed products during temperature-programmed desorption tests by mass spectrometry. Such hydrophilic species have been observed to favor proton <span class="hlt">surface</span> mobility and <span class="hlt">exchange</span> with Pt-adsorbed deuterium even in the presence of adsorbed CO. This behavior is relevant both for the proper characterization of these kinds of catalysts using adsorption probes and for the design of new <span class="hlt">surface</span>-modified carbon supports, enabling alternative proton-transfer pathways throughout the catalytic layers toward the membrane.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/7785756','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/7785756"><span>[Heat and moisture <span class="hlt">exchangers</span> for conditioning of inspired <span class="hlt">air</span> of intubated patients in intensive care. The humidification properties of passive <span class="hlt">air</span> <span class="hlt">exchangers</span> under clinical conditions].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rathgeber, J; Züchner, K; Kietzmann, D; Weyland, W</p> <p>1995-04-01</p> <p>Heat and moisture <span class="hlt">exchangers</span> (HME) are used as artificial noses for intubated patients to prevent tracheo-bronchial or pulmonary damage resulting from dry and cold inspired gases. HME are mounted directly on the tracheal tube, where they collect a large fraction of the heat and moisture of the expired <span class="hlt">air</span>, adding this to the subsequent inspired breath. The effective performance depends on the water-retention capacity of the HME: the amount of water added to the inspired gas cannot exceed the stored water uptake of the previous breath. This study evaluates the efficiency of four different HME under laboratory and clinical conditions using a new moisture-measuring device. METHODS. In a first step, the absolute efficiency of four different HME (DAR Hygrobac, Gibeck Humid-Vent 2P, Pall BB 22-15 T, and Pall BB 100) was evaluated using a lung <span class="hlt">model</span> simulating physiological heat and humidity conditions of the upper airways. The <span class="hlt">model</span> was ventilated with tidal volumes of 500, 1,000, and 1,500 ml and different flow rates. The water content of the ventilated <span class="hlt">air</span> was determined between tracheal tube and HME using a new high-resolution humidity meter and compared with the absolute water loss of the exhaled <span class="hlt">air</span> at the gas outlet of a Siemens Servo C ventilator measured with a dew-point hygrometer. Secondly, the moisturizing efficiency was evaluated under clinical conditions in an intensive care unit with 25 intubated patients. Maintaining the ventilatory conditions for each patient, the HME were randomly changed. The humidity data were determined as described above and compared with the laboratory findings. RESULTS AND DISCUSSION. The water content at the respirator outlet is inversely equivalent to the humidity of the inspired gases and represents the water loss from the respiratory tract if the patient is ventilated with dry gases. Moisture retention and heating capacity decreased with higher volumes and higher flow rates. These data are simple to obtain without affecting the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A52E..05L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A52E..05L"><span>Atlantic Meridional Overturning Circulation Influence on North Atlantic Sector <span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature and its Predictability in the Kiel Climate <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Latif, M.</p> <p>2017-12-01</p> <p>We investigate the influence of the Atlantic Meridional Overturning Circulation (AMOC) on the North Atlantic sector <span class="hlt">surface</span> <span class="hlt">air</span> temperature (SAT) in two multi-millennial control integrations of the Kiel Climate <span class="hlt">Model</span> (KCM). One <span class="hlt">model</span> version employs a freshwater flux correction over the North Atlantic, while the other does not. A clear influence of the AMOC on North Atlantic sector SAT only is simulated in the corrected <span class="hlt">model</span> that depicts much reduced upper ocean salinity and temperature biases in comparison to the uncorrected <span class="hlt">model</span>. Further, the <span class="hlt">model</span> with much reduced biases depicts significantly enhanced multiyear SAT predictability in the North Atlantic sector relative to the uncorrected <span class="hlt">model</span>. The enhanced SAT predictability in the corrected <span class="hlt">model</span> is due to a stronger and more variable AMOC and its enhanced influence on North Atlantic sea <span class="hlt">surface</span> temperature (SST). Results obtained from preindustrial control integrations of <span class="hlt">models</span> participating in the Coupled <span class="hlt">Model</span> Intercomparison Project Phase 5 (CMIP5) support the findings obtained from the KCM: <span class="hlt">models</span> with large North Atlantic biases tend to have a weak AMOC influence on SST and exhibit a smaller SAT predictability over the North Atlantic sector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100026667','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100026667"><span>A Mass Computation <span class="hlt">Model</span> for Lightweight Brayton Cycle Regenerator Heat <span class="hlt">Exchangers</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Juhasz, Albert J.</p> <p>2010-01-01</p> <p>Based on a theoretical analysis of convective heat transfer across large internal <span class="hlt">surface</span> areas, this paper discusses the design implications for generating lightweight gas-gas heat <span class="hlt">exchanger</span> designs by packaging such areas into compact three-dimensional shapes. Allowances are made for hot and cold inlet and outlet headers for assembly of completed regenerator (or recuperator) heat <span class="hlt">exchanger</span> units into closed cycle gas turbine flow ducting. <span class="hlt">Surface</span> area and resulting volume and mass requirements are computed for a range of heat <span class="hlt">exchanger</span> effectiveness values and internal heat transfer coefficients. Benefit cost curves show the effect of increasing heat <span class="hlt">exchanger</span> effectiveness on Brayton cycle thermodynamic efficiency on the plus side, while also illustrating the cost in heat <span class="hlt">exchanger</span> required <span class="hlt">surface</span> area, volume, and mass requirements as effectiveness is increased. The equations derived for counterflow and crossflow configurations show that as effectiveness values approach unity, or 100 percent, the required <span class="hlt">surface</span> area, and hence heat <span class="hlt">exchanger</span> volume and mass tend toward infinity, since the implication is that heat is transferred at a zero temperature difference. To verify the dimensional accuracy of the regenerator mass computational procedure, calculation of a regenerator specific mass, that is, heat <span class="hlt">exchanger</span> weight per unit working fluid mass flow, is performed in both English and SI units. Identical numerical values for the specific mass parameter, whether expressed in lb/(lb/sec) or kg/(kg/sec), show the dimensional consistency of overall results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100037206','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100037206"><span>A Mass Computation <span class="hlt">Model</span> for Lightweight Brayton Cycle Regenerator Heat <span class="hlt">Exchangers</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Juhasz, Albert J.</p> <p>2010-01-01</p> <p>Based on a theoretical analysis of convective heat transfer across large internal <span class="hlt">surface</span> areas, this paper discusses the design implications for generating lightweight gas-gas heat <span class="hlt">exchanger</span> designs by packaging such areas into compact three-dimensional shapes. Allowances are made for hot and cold inlet and outlet headers for assembly of completed regenerator (or recuperator) heat <span class="hlt">exchanger</span> units into closed cycle gas turbine flow ducting. <span class="hlt">Surface</span> area and resulting volume and mass requirements are computed for a range of heat <span class="hlt">exchanger</span> effectiveness values and internal heat transfer coefficients. Benefit cost curves show the effect of increasing heat <span class="hlt">exchanger</span> effectiveness on Brayton cycle thermodynamic efficiency on the plus side, while also illustrating the cost in heat <span class="hlt">exchanger</span> required <span class="hlt">surface</span> area, volume, and mass requirements as effectiveness is increased. The equations derived for counterflow and crossflow configurations show that as effectiveness values approach unity, or 100 percent, the required <span class="hlt">surface</span> area, and hence heat <span class="hlt">exchanger</span> volume and mass tend toward infinity, since the implication is that heat is transferred at a zero temperature difference. To verify the dimensional accuracy of the regenerator mass computational procedure, calculation of a regenerator specific mass, that is, heat <span class="hlt">exchanger</span> weight per unit working fluid mass flow, is performed in both English and SI units. Identical numerical values for the specific mass parameter, whether expressed in lb/(lb/sec) or kg/ (kg/sec), show the dimensional consistency of overall results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.5784F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.5784F"><span>Short-term Rn-222 concentration changes in underground spaces with limited <span class="hlt">air</span> <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fijałkowska-Lichwa, Lidia; Przylibski, Tadeusz A.</p> <p>2010-05-01</p> <p>Authors conducted research on radon concentration in two underground structures located in the vicinity of Kletno (Sudety Mts., SW Poland), which are accessible for visitors. One of these structures is Niedźwiedzia (Bear) Cave, and the second one is the part of former uranium mine - Fluorite Adit. Both selected underground structures are characterized by almost constant temperature, changing within the range from +5 to +7° C and also constant relative humidity, close to 100%. Both these parameters testify that <span class="hlt">air</span> <span class="hlt">exchange</span> with the atmosphere is very limited. <span class="hlt">Air</span> <span class="hlt">exchange</span> is limited particularly in Niedźwiedzia Cave, which microclimate is protected i.e. by applying of locks at the entrance and exit of tourist route. The measurements were conducted between 16.05.2008. and 15.11.2009., by the use of a new Polish equipment - SRDN-3 devices with semiconductor detector. SRDN-3 device records every hour radon concentration as well as atmospheric parameters - relative humidity and temperature. At the same time authors conducted measurements of basic parameters in the open atmosphere close to Niedźwiedzia Cave. Obtained results of atmospheric parameters measurements may be used for both underground structures; because they are located within the distance of about 1 km. Atmospheric parameters were measured by the use of automatic weather station VantagePro2. On the base of conducted research authors corroborate, that the differences of radon concentration in both underground structures reach three orders of magnitude during a year. In Niedźwiedzia Cave these values are in the range from below 88 Bq/m3 (detection limit of the SRDN-3 device) up to 12 kBq/m3. Related values in Fluorite Adit are between < 88 Bq/m3 and 35 kBq/m3. It was observed also the different course of daily radon concentration changes in both structures. Additionally, authors registered that daily course of radon concentration changes differs due to season of the year. Such changes are observed in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090015376','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090015376"><span>Investigation of Liquid Metal Heat <span class="hlt">Exchanger</span> Designs for Fission <span class="hlt">Surface</span> Power</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dyson, Rodger W.; Penswick, Barry; Robbie, Malcolm; Geng, Steven M.</p> <p>2009-01-01</p> <p>Fission <span class="hlt">surface</span> power is an option for future Moon and Mars <span class="hlt">surface</span> missions. High power nuclear reactor heated Stirling convertors are an option to provide reliable power for long duration outpost operations. This report investigates various design approaches for the liquid metal to acceptor heat <span class="hlt">exchange</span> and clarifies the details used in the analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51I..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51I..01H"><span>Updating representation of land <span class="hlt">surface</span>-atmosphere feedbacks in airborne campaign <span class="hlt">modeling</span> analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, M.; Carmichael, G. R.; Crawford, J. H.; Chan, S.; Xu, X.; Fisher, J. A.</p> <p>2017-12-01</p> <p>An updated <span class="hlt">modeling</span> system to support airborne field campaigns is being built at NASA Ames Pleiades, with focus on adjusting the representation of land <span class="hlt">surface</span>-atmosphere feedbacks. The main updates, referring to previous experiences with ARCTAS-CARB and CalNex in the western US to study <span class="hlt">air</span> pollution inflows, include: 1) migrating the WRF (Weather Research and Forecasting) coupled land <span class="hlt">surface</span> <span class="hlt">model</span> from Noah to improved/more complex <span class="hlt">models</span> especially Noah-MP and Rapid Update Cycle; 2) enabling the WRF land initialization with suitably spun-up land <span class="hlt">model</span> output; 3) incorporating satellite land cover, vegetation dynamics, and soil moisture data (i.e., assimilating Soil Moisture Active Passive data using the ensemble Kalman filter approach) into WRF. Examples are given of comparing the <span class="hlt">model</span> fields with available aircraft observations during spring-summer 2016 field campaigns taken place at the eastern side of continents (KORUS-AQ in South Korea and ACT-America in the eastern US), the <span class="hlt">air</span> pollution export regions. Under fair weather and stormy conditions, <span class="hlt">air</span> pollution vertical distributions and column amounts, as well as the impact from land <span class="hlt">surface</span>, are compared. These help identify challenges and opportunities for LEO/GEO satellite remote sensing and <span class="hlt">modeling</span> of <span class="hlt">air</span> quality in the northern hemisphere. Finally, we briefly show applications of this system on simulating Australian conditions, which would explore the needs for further development of the observing system in the southern hemisphere and inform the Clean <span class="hlt">Air</span> and Urban Landscapes (https://www.nespurban.edu.au) <span class="hlt">modelers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995WRR....31..619B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995WRR....31..619B"><span>An Analytic Approach to <span class="hlt">Modeling</span> Land-Atmosphere Interaction: 1. Construct and Equilibrium Behavior</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brubaker, Kaye L.; Entekhabi, Dara</p> <p>1995-03-01</p> <p>A four-variable land-atmosphere <span class="hlt">model</span> is developed to investigate the coupled <span class="hlt">exchanges</span> of water and energy between the land <span class="hlt">surface</span> and atmosphere and the role of these <span class="hlt">exchanges</span> in the statistical behavior of continental climates. The land-atmosphere system is substantially simplified and formulated as a set of ordinary differential equations that, with the addition of random noise, are suitable for analysis in the form of the multivariate Îto equation. The <span class="hlt">model</span> treats the soil layer and the near-<span class="hlt">surface</span> atmosphere as reservoirs with storage capacities for heat and water. The transfers between these reservoirs are regulated by four states: soil saturation, soil temperature, <span class="hlt">air</span> specific humidity, and <span class="hlt">air</span> potential temperature. The atmospheric reservoir is treated as a turbulently mixed boundary layer of fixed depth. Heat and moisture advection, precipitation, and layer-top <span class="hlt">air</span> entrainment are parameterized. The system is forced externally by solar radiation and the lateral advection of <span class="hlt">air</span> and water mass. The remaining energy and water mass <span class="hlt">exchanges</span> are expressed in terms of the state variables. The <span class="hlt">model</span> development and equilibrium solutions are presented. Although comparisons between observed data and steady state <span class="hlt">model</span> results re inexact, the <span class="hlt">model</span> appears to do a reasonable job of partitioning net radiation into sensible and latent heat flux in appropriate proportions for bare-soil midlatitude summer conditions. Subsequent work will introduce randomness into the forcing terms to investigate the effect of water-energy coupling and land-atmosphere interaction on variability and persistence in the climatic system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...1313285B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...1313285B"><span><span class="hlt">Air</span>/sea DMS gas transfer in the North Atlantic: evidence for limited interfacial gas <span class="hlt">exchange</span> at high wind speed</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bell, T. G.; De Bruyn, W.; Miller, S. D.; Ward, B.; Christensen, K.; Saltzman, E. S.</p> <p>2013-05-01</p> <p>Shipboard measurements of eddy covariance DMS <span class="hlt">air</span>/sea fluxes and seawater concentration were carried out in the North Atlantic bloom region in June/July 2011. Gas transfer coefficients (k660) show a linear dependence on mean horizontal wind speed at wind speeds up to 11 m s-1. At higher wind speeds the relationship between k660 and wind speed weakens. At high winds, measured DMS fluxes were lower than predicted based on the linear relationship between wind speed and interfacial stress extrapolated from low to intermediate wind speeds. In contrast, the transfer coefficient for sensible heat did not exhibit this effect. The apparent suppression of <span class="hlt">air</span>/sea gas flux at higher wind speeds appears to be related to sea state, as determined from shipboard wave measurements. These observations are consistent with the idea that long waves suppress near <span class="hlt">surface</span> water side turbulence, and decrease interfacial gas transfer. This effect may be more easily observed for DMS than for less soluble gases, such as CO2, because the <span class="hlt">air</span>/sea <span class="hlt">exchange</span> of DMS is controlled by interfacial rather than bubble-mediated gas transfer under high wind speed conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5855873','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5855873"><span>Acoustic Sensors for <span class="hlt">Air</span> and <span class="hlt">Surface</span> Navigation Applications</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kapoor, Rohan; Ramasamy, Subramanian; Schyndel, Ron Van</p> <p>2018-01-01</p> <p>This paper presents the state-of-the-art and reviews the state-of-research of acoustic sensors used for a variety of navigation and guidance applications on <span class="hlt">air</span> and <span class="hlt">surface</span> vehicles. In particular, this paper focuses on echolocation, which is widely utilized in nature by certain mammals (e.g., cetaceans and bats). Although acoustic sensors have been extensively adopted in various engineering applications, their use in navigation and guidance systems is yet to be fully exploited. This technology has clear potential for applications in <span class="hlt">air</span> and <span class="hlt">surface</span> navigation/guidance for intelligent transport systems (ITS), especially considering <span class="hlt">air</span> and <span class="hlt">surface</span> operations indoors and in other environments where satellite positioning is not available. Propagation of sound in the atmosphere is discussed in detail, with all potential attenuation sources taken into account. The errors introduced in echolocation measurements due to Doppler, multipath and atmospheric effects are discussed, and an uncertainty analysis method is presented for ranging error budget prediction in acoustic navigation applications. Considering the design challenges associated with monostatic and multi-static sensor implementations and looking at the performance predictions for different possible configurations, acoustic sensors show clear promises in navigation, proximity sensing, as well as obstacle detection and tracking. The integration of acoustic sensors in multi-sensor navigation systems is also considered towards the end of the paper and a low Size, Weight and Power, and Cost (SWaP-C) sensor integration architecture is presented for possible introduction in <span class="hlt">air</span> and <span class="hlt">surface</span> navigation systems. PMID:29414894</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5071885','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5071885"><span>Gold Nanoparticle Monolayers from Sequential Interfacial Ligand <span class="hlt">Exchange</span> and Migration in a Three-Phase 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>Yang, Guang; Hallinan, Daniel T.</p> <p>2016-01-01</p> <p>Using a three-phase system, centimeter-scale monolayer gold nanoparticle (Au NP) films have been prepared that have long-range order and hydrophobic ligands. The system contains an interface between an aqueous phase containing Au NPs and an oil phase containing one of various types of amine ligands, and a water/<span class="hlt">air</span> interface. As the Au NPs diffuse to the water/oil interface, ligand <span class="hlt">exchange</span> takes place which temporarily traps them at the water/oil interface. The ligand-<span class="hlt">exchanged</span> particles then spontaneously migrate to the <span class="hlt">air</span>/water interface, where they self-assemble, forming a monolayer under certain conditions. The spontaneous formation of the NP film at the <span class="hlt">air</span>/water interface was due to the minimization of the system Helmholtz free energy. However, the extent of <span class="hlt">surface</span> functionalization was dictated by kinetics. This decouples interfacial ligand <span class="hlt">exchange</span> from interfacial self-assembly, while maintaining the simplicity of a single system. The interparticle center-to-center distance was dictated by the amine ligand length. The Au NP monolayers exhibit tunable <span class="hlt">surface</span> plasma resonance and excellent spatial homogeneity, which is useful for <span class="hlt">surface</span>-enhanced Raman scattering. The “<span class="hlt">air</span>/water/oil” self-assembly method developed here not only benefits the fundamental understanding of NP ligand conformations, but is also applicable to the manufacture of plasmonic nanoparticle devices with precisely designed optical properties. PMID:27762394</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://adsabs.harvard.edu/abs/2008ACPD....8.2163E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ACPD....8.2163E"><span>Global ozone and <span class="hlt">air</span> quality: a multi-<span class="hlt">model</span> assessment of risks to human health and crops</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ellingsen, K.; Gauss, M.; van Dingenen, R.; Dentener, F. J.; Emberson, L.; Fiore, A. M.; Schultz, M. G.; Stevenson, D. S.; Ashmore, M. R.; Atherton, C. S.; Bergmann, D. J.; Bey, I.; Butler, T.; Drevet, J.; Eskes, H.; Hauglustaine, D. A.; Isaksen, I. S. A.; Horowitz, L. W.; Krol, M.; Lamarque, J. F.; Lawrence, M. G.; van Noije, T.; Pyle, J.; Rast, S.; Rodriguez, J.; Savage, N.; Strahan, S.; Sudo, K.; Szopa, S.; Wild, O.</p> <p>2008-02-01</p> <p>Within ACCENT, a European Network of Excellence, eighteen atmospheric <span class="hlt">models</span> from the U.S., Europe, and Japan calculated present (2000) and future (2030) concentrations of ozone at the Earth's <span class="hlt">surface</span> with hourly temporal resolution. Comparison of <span class="hlt">model</span> results with <span class="hlt">surface</span> ozone measurements in 14 world regions indicates that levels and seasonality of <span class="hlt">surface</span> ozone in North America and Europe are characterized well by global <span class="hlt">models</span>, with annual average biases typically within 5-10 nmol/mol. However, comparison with rather sparse observations over some regions suggest that most <span class="hlt">models</span> overestimate annual ozone by 15-20 nmol/mol in some locations. Two scenarios from the International Institute for Applied Systems Analysis (IIASA) and one from the Intergovernmental Panel on Climate Change Special Report on Emissions Scenarios (IPCC SRES) have been implemented in the <span class="hlt">models</span>. This study focuses on changes in near-<span class="hlt">surface</span> ozone and their effects on human health and vegetation. Different indices and <span class="hlt">air</span> quality standards are used to characterise <span class="hlt">air</span> quality. We show that often the calculated changes in the different indices are closely inter-related. Indices using lower thresholds are more consistent between the <span class="hlt">models</span>, and are recommended for global <span class="hlt">model</span> analysis. Our analysis indicates that currently about two-thirds of the regions considered do not meet health <span class="hlt">air</span> quality standards, whereas only 2-4 regions remain below the threshold. Calculated <span class="hlt">air</span> quality exceedances show moderate deterioration by 2030 if current emissions legislation is followed and slight improvements if current emissions reduction technology is used optimally. For the "business as usual" scenario severe <span class="hlt">air</span> quality problems are predicted. We show that <span class="hlt">model</span> simulations of <span class="hlt">air</span> quality indices are particularly sensitive to how well ozone is represented, and improved accuracy is needed for future projections. Additional measurements are needed to allow a more quantitative assessment of the risks to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060004052','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060004052"><span>Updraft <span class="hlt">Model</span> for Development of Autonomous Soaring Uninhabited <span class="hlt">Air</span> Vehicles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Allen, Michael J.</p> <p>2006-01-01</p> <p>Large birds and glider pilots commonly use updrafts caused by convection in the lower atmosphere to extend flight duration, increase cross-country speed, improve range, or simply to conserve energy. Uninhabited <span class="hlt">air</span> vehicles may also have the ability to exploit updrafts to improve performance. An updraft <span class="hlt">model</span> was developed at NASA Dryden Flight Research Center (Edwards, California) to investigate the use of convective lift for uninhabited <span class="hlt">air</span> vehicles in desert regions. Balloon and <span class="hlt">surface</span> measurements obtained at the National Oceanic and Atmospheric Administration <span class="hlt">Surface</span> Radiation station (Desert Rock, Nevada) enabled the <span class="hlt">model</span> development. The data were used to create a statistical representation of the convective velocity scale, w*, and the convective mixing-layer thickness, zi. These parameters were then used to determine updraft size, vertical velocity profile, spacing, and maximum height. This paper gives a complete description of the updraft <span class="hlt">model</span> and its derivation. Computer code for running the <span class="hlt">model</span> is also given in conjunction with a check case for <span class="hlt">model</span> verification.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008919','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008919"><span>Microgravity condensing heat <span class="hlt">exchanger</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thomas, Christopher M. (Inventor); Ma, Yonghui (Inventor); North, Andrew (Inventor); Weislogel, Mark M. (Inventor)</p> <p>2011-01-01</p> <p>A heat <span class="hlt">exchanger</span> having a plurality of heat <span class="hlt">exchanging</span> aluminum fins with hydrophilic condensing <span class="hlt">surfaces</span> which are stacked and clamped between two cold plates. The cold plates are aligned radially along a plane extending through the axis of a cylindrical duct and hold the stacked and clamped portions of the heat <span class="hlt">exchanging</span> fins along the axis of the cylindrical duct. The fins extend outwardly from the clamped portions along approximately radial planes. The spacing between fins is symmetric about the cold plates, and are somewhat more closely spaced as the angle they make with the cold plates approaches 90.degree.. Passageways extend through the fins between vertex spaces which provide capillary storage and communicate with passageways formed in the stacked and clamped portions of the fins, which communicate with water drains connected to a pump externally to the duct. Water with no entrained <span class="hlt">air</span> is drawn from the capillary spaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915477O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915477O"><span>Advancing land <span class="hlt">surface</span> <span class="hlt">model</span> development with satellite-based Earth observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Orth, Rene; Dutra, Emanuel; Trigo, Isabel F.; Balsamo, Gianpaolo</p> <p>2017-04-01</p> <p>The land <span class="hlt">surface</span> forms an essential part of the climate system. It interacts with the atmosphere through the <span class="hlt">exchange</span> of water and energy and hence influences weather and climate, as well as their predictability. Correspondingly, the land <span class="hlt">surface</span> <span class="hlt">model</span> (LSM) is an essential part of any weather forecasting system. LSMs rely on partly poorly constrained parameters, due to sparse land <span class="hlt">surface</span> observations. With the use of newly available land <span class="hlt">surface</span> temperature observations, we show in this study that novel satellite-derived datasets help to improve LSM configuration, and hence can contribute to improved weather predictability. We use the Hydrology Tiled ECMWF Scheme of <span class="hlt">Surface</span> <span class="hlt">Exchanges</span> over Land (HTESSEL) and validate it comprehensively against an array of Earth observation reference datasets, including the new land <span class="hlt">surface</span> temperature product. This reveals satisfactory <span class="hlt">model</span> performance in terms of hydrology, but poor performance in terms of land <span class="hlt">surface</span> temperature. This is due to inconsistencies of process representations in the <span class="hlt">model</span> as identified from an analysis of perturbed parameter simulations. We show that HTESSEL can be more robustly calibrated with multiple instead of single reference datasets as this mitigates the impact of the structural inconsistencies. Finally, performing coupled global weather forecasts we find that a more robust calibration of HTESSEL also contributes to improved weather forecast skills. In summary, new satellite-based Earth observations are shown to enhance the multi-dataset calibration of LSMs, thereby improving the representation of insufficiently captured processes, advancing weather predictability and understanding of climate system feedbacks. Orth, R., E. Dutra, I. F. Trigo, and G. Balsamo (2016): Advancing land <span class="hlt">surface</span> <span class="hlt">model</span> development with satellite-based Earth observations. Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2016-628</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H23I1785B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H23I1785B"><span>Groundwater Discharge of Legacy Nitrogen to River Networks: Linking Regional Groundwater <span class="hlt">Models</span> to Streambed Groundwater-<span class="hlt">Surface</span> Water <span class="hlt">Exchange</span> and Nitrogen Processing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barclay, J. R.; Helton, A. M.; Briggs, M. A.; Starn, J. J.; Hunt, A.</p> <p>2017-12-01</p> <p>Despite years of management, excess nitrogen (N) is a pervasive problem in many aquatic ecosystems. More than half of <span class="hlt">surface</span> water in the United States is derived from groundwater, and widespread N contamination in aquifers from decades of watershed N inputs suggest legacy N discharging from groundwater may contribute to contemporary N pollution problems in <span class="hlt">surface</span> waters. Legacy N loads to streams and rivers are controlled by both regional scale flow paths and fine-scale processes that drive N transformations, such as groundwater-<span class="hlt">surface</span> water <span class="hlt">exchange</span> across steep redox gradients that occur at stream bed interfaces. Adequately incorporating these disparate scales is a challenge, but it is essential to understanding legacy N transport and making informed management decisions. We developed a regional groundwater flow <span class="hlt">model</span> for the Farmington River, a HUC-8 basin that drains to the Long Island Sound, a coastal estuary that suffers from elevated N loads despite decades of management, to understand broad patterns of regional transport. To evaluate and refine the regional <span class="hlt">model</span>, we used thermal infrared imagery paired with vertical temperature profiling to estimate groundwater discharge at the streambed interface. We also analyzed discharging groundwater for multiple N species to quantify fine scale patterns of N loading and transformation via denitrification at the streambed interface. Integrating regional and local estimates of groundwater discharge of legacy N to river networks should improve our ability to predict spatiotemporal patterns of legacy N loading to and transformation within <span class="hlt">surface</span> waters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA587111','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA587111"><span>Military Airlift: DOD Plans to Participate in Multi-National Program to <span class="hlt">Exchange</span> <span class="hlt">Air</span> Services with European Nations</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-10-30</p> <p><span class="hlt">Air</span> Transport, <span class="hlt">Air-to-Air</span> Refueling and Other <span class="hlt">Exchange</span> of Services ( ATARES ) program.1 ATARES is a European program through which member nations use a... ATARES is managed by the Movement Coordination Centre Europe (MCCE), a multi-national organization established in July 2007 to coordinate and optimize...of ATARES but is seeking to join the program. DOD is a member of MCCE and pays a fee for this membership; there is no additional fee to become a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800058489&hterms=modeling+reactions+chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmodeling%2Breactions%2Bchemical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800058489&hterms=modeling+reactions+chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmodeling%2Breactions%2Bchemical"><span>Meteorological and <span class="hlt">air</span> pollution <span class="hlt">modeling</span> for an urban airport</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Swan, P. R.; Lee, I. Y.</p> <p>1980-01-01</p> <p>Results are presented of numerical experiments <span class="hlt">modeling</span> meteorology, multiple pollutant sources, and nonlinear photochemical reactions for the case of an airport in a large urban area with complex terrain. A planetary boundary-layer <span class="hlt">model</span> which predicts the mixing depth and generates wind, moisture, and temperature fields was used; it utilizes only <span class="hlt">surface</span> and synoptic boundary conditions as input data. A version of the Hecht-Seinfeld-Dodge chemical kinetics <span class="hlt">model</span> is integrated with a new, rapid numerical technique; both the San Francisco Bay Area <span class="hlt">Air</span> Quality Management District source inventory and the San Jose Airport aircraft inventory are utilized. The <span class="hlt">air</span> quality <span class="hlt">model</span> results are presented in contour plots; the combined results illustrate that the highly nonlinear interactions which are present require that the chemistry and meteorology be considered simultaneously to make a valid assessment of the effects of individual sources on regional <span class="hlt">air</span> quality.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AtmEn.174..194K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AtmEn.174..194K"><span>Constraining the uncertainty in emissions over India with a regional <span class="hlt">air</span> quality <span class="hlt">model</span> evaluation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karambelas, Alexandra; Holloway, Tracey; Kiesewetter, Gregor; Heyes, Chris</p> <p>2018-02-01</p> <p>To evaluate uncertainty in the spatial distribution of <span class="hlt">air</span> emissions over India, we compare satellite and <span class="hlt">surface</span> observations with simulations from the U.S. Environmental Protection Agency (EPA) Community Multi-Scale <span class="hlt">Air</span> Quality (CMAQ) <span class="hlt">model</span>. Seasonally representative simulations were completed for January, April, July, and October 2010 at 36 km × 36 km using anthropogenic emissions from the Greenhouse Gas-<span class="hlt">Air</span> Pollution Interaction and Synergies (GAINS) <span class="hlt">model</span> following version 5a of the Evaluating the Climate and <span class="hlt">Air</span> Quality Impacts of Short-Lived Pollutants project (ECLIPSE v5a). We use both tropospheric columns from the Ozone Monitoring Instrument (OMI) and <span class="hlt">surface</span> observations from the Central Pollution Control Board (CPCB) to closely examine <span class="hlt">modeled</span> nitrogen dioxide (NO2) biases in urban and rural regions across India. Spatial average evaluation with satellite retrievals indicate a low bias in the <span class="hlt">modeled</span> tropospheric column (-63.3%), which reflects broad low-biases in majority non-urban regions (-70.1% in rural areas) across the sub-continent to slightly lesser low biases reflected in semi-urban areas (-44.7%), with the threshold between semi-urban and rural defined as 400 people per km2. In contrast, <span class="hlt">modeled</span> <span class="hlt">surface</span> NO2 concentrations exhibit a slight high bias of +15.6% when compared to <span class="hlt">surface</span> CPCB observations predominantly located in urban areas. Conversely, in examining extremely population dense urban regions with more than 5000 people per km2 (dense-urban), we find <span class="hlt">model</span> overestimates in both the column (+57.8) and at the <span class="hlt">surface</span> (+131.2%) compared to observations. Based on these results, we find that existing emission fields for India may overestimate urban emissions in densely populated regions and underestimate rural emissions. However, if we rely on <span class="hlt">model</span> evaluation with predominantly urban <span class="hlt">surface</span> observations from the CPCB, comparisons reflect <span class="hlt">model</span> high biases, contradictory to the knowledge gained using satellite observations. Satellites thus</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25350507','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25350507"><span><span class="hlt">Modeling</span> apple <span class="hlt">surface</span> temperature dynamics based on weather data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Lei; Peters, Troy; Zhang, Qin; Zhang, Jingjin; Huang, Danfeng</p> <p>2014-10-27</p> <p>The exposure of fruit <span class="hlt">surfaces</span> to direct sunlight during the summer months can result in sunburn damage. Losses due to sunburn damage are a major economic problem when marketing fresh apples. The objective of this study was to develop and validate a <span class="hlt">model</span> for simulating fruit <span class="hlt">surface</span> temperature (FST) dynamics based on energy balance and measured weather data. A series of weather data (<span class="hlt">air</span> temperature, humidity, solar radiation, and wind speed) was recorded for seven hours between 11:00-18:00 for two months at fifteen minute intervals. To validate the <span class="hlt">model</span>, the FSTs of "Fuji" apples were monitored using an infrared camera in a natural orchard environment. The FST dynamics were measured using a series of thermal images. For the apples that were completely exposed to the sun, the RMSE of the <span class="hlt">model</span> for estimating FST was less than 2.0 °C. A sensitivity analysis of the emissivity of the apple <span class="hlt">surface</span> and the conductance of the fruit <span class="hlt">surface</span> to water vapour showed that accurate estimations of the apple <span class="hlt">surface</span> emissivity were important for the <span class="hlt">model</span>. The validation results showed that the <span class="hlt">model</span> was capable of accurately describing the thermal performances of apples under different solar radiation intensities. Thus, this <span class="hlt">model</span> could be used to more accurately estimate the FST relative to estimates that only consider the <span class="hlt">air</span> temperature. In addition, this <span class="hlt">model</span> provides useful information for sunburn protection management.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4279478','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4279478"><span><span class="hlt">Modeling</span> Apple <span class="hlt">Surface</span> Temperature Dynamics Based on Weather Data</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Lei; Peters, Troy; Zhang, Qin; Zhang, Jingjin; Huang, Danfeng</p> <p>2014-01-01</p> <p>The exposure of fruit <span class="hlt">surfaces</span> to direct sunlight during the summer months can result in sunburn damage. Losses due to sunburn damage are a major economic problem when marketing fresh apples. The objective of this study was to develop and validate a <span class="hlt">model</span> for simulating fruit <span class="hlt">surface</span> temperature (FST) dynamics based on energy balance and measured weather data. A series of weather data (<span class="hlt">air</span> temperature, humidity, solar radiation, and wind speed) was recorded for seven hours between 11:00–18:00 for two months at fifteen minute intervals. To validate the <span class="hlt">model</span>, the FSTs of “Fuji” apples were monitored using an infrared camera in a natural orchard environment. The FST dynamics were measured using a series of thermal images. For the apples that were completely exposed to the sun, the RMSE of the <span class="hlt">model</span> for estimating FST was less than 2.0 °C. A sensitivity analysis of the emissivity of the apple <span class="hlt">surface</span> and the conductance of the fruit <span class="hlt">surface</span> to water vapour showed that accurate estimations of the apple <span class="hlt">surface</span> emissivity were important for the <span class="hlt">model</span>. The validation results showed that the <span class="hlt">model</span> was capable of accurately describing the thermal performances of apples under different solar radiation intensities. Thus, this <span class="hlt">model</span> could be used to more accurately estimate the FST relative to estimates that only consider the <span class="hlt">air</span> temperature. In addition, this <span class="hlt">model</span> provides useful information for sunburn protection management. PMID:25350507</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28493625','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28493625"><span>Significant OH production under <span class="hlt">surface</span> cleaning and <span class="hlt">air</span> cleaning conditions: Impact on indoor <span class="hlt">air</span> quality.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carslaw, N; Fletcher, L; Heard, D; Ingham, T; Walker, H</p> <p>2017-11-01</p> <p>We report measurements of hydroxyl (OH) and hydroperoxy (HO 2 ) radicals made by laser-induced fluorescence spectroscopy in a computer classroom (i) in the absence of indoor activities (ii) during desk cleaning with a limonene-containing cleaner (iii) during operation of a commercially available "<span class="hlt">air</span> cleaning" device. In the unmanipulated environment, the one-minute averaged OH concentration remained close to or below the limit of detection (6.5×10 5  molecule cm -3 ), whilst that of HO 2 was 1.3×10 7  molecule cm -3 . These concentrations increased to ~4×10 6 and 4×10 8  molecule cm -3 , respectively during desk cleaning. During operation of the <span class="hlt">air</span> cleaning device, OH and HO 2 concentrations reached ~2×10 7 and ~6×10 8  molecule cm -3 respectively. The potential of these OH concentrations to initiate chemical processing is explored using a detailed chemical <span class="hlt">model</span> for indoor <span class="hlt">air</span> (the INDCM). The <span class="hlt">model</span> can reproduce the measured OH and HO 2 concentrations to within 50% and often within a few % and demonstrates that the resulting secondary chemistry varies with the cleaning activity. Whilst terpene reaction products dominate the product composition following <span class="hlt">surface</span> cleaning, those from aromatics and other VOCs are much more important during the use of the <span class="hlt">air</span> cleaning device. © 2017 John Wiley & Sons A/S. Published by John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..4412527S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..4412527S"><span>Strong Dependence of U.S. Summertime <span class="hlt">Air</span> Quality on the Decadal Variability of Atlantic Sea <span class="hlt">Surface</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>Shen, Lu; Mickley, Loretta J.; Leibensperger, Eric M.; Li, Mingwei</p> <p>2017-12-01</p> <p>We find that summertime <span class="hlt">air</span> quality in the eastern U.S. displays strong dependence on North Atlantic sea <span class="hlt">surface</span> temperatures, resulting from large-scale ocean-atmosphere interactions. Using observations, reanalysis data sets, and climate <span class="hlt">model</span> simulations, we further identify a multidecadal variability in <span class="hlt">surface</span> <span class="hlt">air</span> quality driven by the Atlantic Multidecadal Oscillation (AMO). In one-half cycle ( 35 years) of the AMO from cold to warm phase, summertime maximum daily 8 h ozone concentrations increase by 1-4 ppbv and PM2.5 concentrations increase by 0.3-1.0 μg m-3 over much of the east. These <span class="hlt">air</span> quality changes are related to warmer, drier, and more stagnant weather in the AMO warm phase, together with anomalous circulation patterns at the <span class="hlt">surface</span> and aloft. If the AMO shifts to the cold phase in future years, it could partly offset the climate penalty on U.S. <span class="hlt">air</span> quality brought by global warming, an effect which should be considered in long-term <span class="hlt">air</span> quality planning.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1425654','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1425654"><span>User-Oriented <span class="hlt">Modeling</span> Tools for Advanced Hybrid and Climate-Appropriate Rooftop <span class="hlt">Air</span> Conditioners</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>Woolley, Jonathan; Univ. of California, Davis, CA; Modera, Mark</p> <p></p> <p>Hybrid unitary <span class="hlt">air</span> conditioning systems offer a pathway to substantially reduce energy use and peak electrical demand for cooling, heating, and ventilation in commercial buildings. Hybrid <span class="hlt">air</span> conditioners incorporate multiple subsystems that are carefully orchestrated to provide climate- and application-specific efficiency advantages. There are a multitude of hybrid system architectures, but common subsystems include: heat recovery ventilation, indirect evaporative cooling, desiccant dehumidification, variable speed fans, modulating dampers, and multi-stage or variable-speed vapor compression cooling. Categorically, hybrid systems can operate in numerous discrete modes. For example: indirect evaporative cooling may operate for periods when the subsystem provides adequate sensible cooling, thenmore » vapor compression cooling will be included when more cooling or dehumidification is necessary. Laboratory assessments, field studies, and simulations have demonstrated that hybrid unitary <span class="hlt">air</span> conditioners could reduce energy use for cooling and ventilation by 30-90% depending on climate and application. Heretofore, it has been challenging - if not impossible - for practitioners to <span class="hlt">model</span> hybrid <span class="hlt">air</span> conditioners as part of building energy simulations; and the limitation has severely obstructed broader adoption of technologies in this class. In this project, we developed a new feature for EnergyPlus that enables <span class="hlt">modeling</span> hybrid unitary <span class="hlt">air</span> conditioning equipment for building energy simulations. This is a significant advancement for both theory and practice, and confers public benefit by enabling practitioners to evaluate this compelling efficiency technology as a part of building energy simulations. The feature is a black-box <span class="hlt">model</span> that requires extensive performance data for each hybrid unitary product. In parallel, we also developed new features for the Technology Performance <span class="hlt">Exchange</span> to enable manufacturers to submit performance data in a standard format that can be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17..985C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17..985C"><span>From watershed- to stream-reach-scale: the influence of multiple spatial scales on <span class="hlt">surface</span> water-groundwater <span class="hlt">exchange</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caruso, Alice; Boano, Fulvio; Ridolfi, Luca</p> <p>2015-04-01</p> <p><span class="hlt">Surface</span> water bodies continuously interact with the subsurface and it is by now widely known that the hyporheic zone plays a key role in the mixing of river water with shallow groundwater. Hyporheic <span class="hlt">exchange</span> occurs over a very wide range of spatial and temporal scales and the <span class="hlt">exchange</span> processes at different scales interact and determine a complex system of nested flow cells. This intricacy results from the multiplicity of spatial scale that characterize landscape and river morphology. In the last years, many processes that regulate the <span class="hlt">surface</span>-groundwater interactions have been elucidated and a more holistic view of groundwater and <span class="hlt">surface</span> water has been adopted. However, despite several insights on the mechanisms of hyporheic <span class="hlt">exchange</span> have been achieved, many important aspects remain to be clarified, i.e. how <span class="hlt">surface</span>-groundwater interactions influence solute transport, microbial activity and biogeochemical transformations at the scale of entire watersheds. To date a deep knowledge of small-scale processes has been developed but what is lacking is a unifying overview of the role of <span class="hlt">surface</span> water-groundwater <span class="hlt">exchange</span> for the health of the whole water system at larger scales, i.e. the scale of the entire basin. In order to better understand the complex multiscale nature of spatial patterns of <span class="hlt">surface</span>-subsurface <span class="hlt">exchange</span>, we aim to assess the importance of the individual scales included in the range between watershed scale to stream reach scale. Hence, we study the large-scale subsurface flow field taking into account the <span class="hlt">surface</span>-groundwater interactions induced by landscape topography from the basin scale to smaller scales ranging from tens of kilometers to tens of meters. The aim of this research is to analyze how individual topographic scales affect the flow field and to understand which ones are the most important and should be focused on. To study the impact of various scales of landscape topography we apply an analytical <span class="hlt">model</span> that provides an exact solution of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27458653','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27458653"><span>Spatial Distribution and <span class="hlt">Air</span>-Water <span class="hlt">Exchange</span> of Organic Flame Retardants in the Lower Great Lakes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McDonough, Carrie A; Puggioni, Gavino; Helm, Paul A; Muir, Derek; Lohmann, Rainer</p> <p>2016-09-06</p> <p>Organic flame retardants (OFRs) such as polybrominated diphenyl ethers (PBDEs) and novel halogenated flame retardants (NHFRs) are ubiquitous, persistent, and bioaccumulative contaminants that have been used in consumer goods to slow combustion. In this study, polyethylene passive samplers (PEs) were deployed throughout the lower Great Lakes (Lake Erie and Lake Ontario) to measure OFRs in <span class="hlt">air</span> and water, calculate <span class="hlt">air</span>-water <span class="hlt">exchange</span> fluxes, and investigate spatial trends. Dissolved Σ12BDE was greatest in Lake Ontario near Toronto (18 pg/L), whereas gaseous Σ12BDE was greatest on the southern shoreline of Lake Erie (11 pg/m(3)). NHFRs were generally below detection limits. <span class="hlt">Air</span>-water <span class="hlt">exchange</span> was dominated by absorption of BDEs 47 and 99, ranging from -964 pg/m(2)/day to -30 pg/m(2)/day. Σ12BDE in <span class="hlt">air</span> and water was significantly correlated with surrounding population density, suggesting that phased-out PBDEs continued to be emitted from population centers along the Great Lakes shoreline in 2012. Correlation with dissolved Σ12BDE was strongest when considering population within 25 km while correlation with gaseous Σ12BDE was strongest when using population within 3 km to the south of each site. Bayesian kriging was used to predict dissolved Σ12BDE over the lakes, illustrating the utility of relatively highly spatially resolved measurements in identifying potential hot spots for future study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ThApC.132.1057Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ThApC.132.1057Y"><span>Multi-criterion <span class="hlt">model</span> ensemble of CMIP5 <span class="hlt">surface</span> <span class="hlt">air</span> temperature over China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Tiantian; Tao, Yumeng; Li, Jingjing; Zhu, Qian; Su, Lu; He, Xiaojia; Zhang, Xiaoming</p> <p>2018-05-01</p> <p>The global circulation <span class="hlt">models</span> (GCMs) are useful tools for simulating climate change, projecting future temperature changes, and therefore, supporting the preparation of national climate adaptation plans. However, different GCMs are not always in agreement with each other over various regions. The reason is that GCMs' configurations, module characteristics, and dynamic forcings vary from one to another. <span class="hlt">Model</span> ensemble techniques are extensively used to post-process the outputs from GCMs and improve the variability of <span class="hlt">model</span> outputs. Root-mean-square error (RMSE), correlation coefficient (CC, or R) and uncertainty are commonly used statistics for evaluating the performances of GCMs. However, the simultaneous achievements of all satisfactory statistics cannot be guaranteed in using many <span class="hlt">model</span> ensemble techniques. In this paper, we propose a multi-<span class="hlt">model</span> ensemble framework, using a state-of-art evolutionary multi-objective optimization algorithm (termed MOSPD), to evaluate different characteristics of ensemble candidates and to provide comprehensive trade-off information for different <span class="hlt">model</span> ensemble solutions. A case study of optimizing the <span class="hlt">surface</span> <span class="hlt">air</span> temperature (SAT) ensemble solutions over different geographical regions of China is carried out. The data covers from the period of 1900 to 2100, and the projections of SAT are analyzed with regard to three different statistical indices (i.e., RMSE, CC, and uncertainty). Among the derived ensemble solutions, the trade-off information is further analyzed with a robust Pareto front with respect to different statistics. The comparison results over historical period (1900-2005) show that the optimized solutions are superior over that obtained simple <span class="hlt">model</span> average, as well as any single GCM output. The improvements of statistics are varying for different climatic regions over China. Future projection (2006-2100) with the proposed ensemble method identifies that the largest (smallest) temperature changes will happen in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17379807','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17379807"><span>Bottom-up determination of <span class="hlt">air</span>-sea momentum <span class="hlt">exchange</span> under a major tropical cyclone.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jarosz, Ewa; Mitchell, Douglas A; Wang, David W; Teague, William J</p> <p>2007-03-23</p> <p>As a result of increasing frequency and intensity of tropical cyclones, an accurate forecasting of cyclone evolution and ocean response is becoming even more important to reduce threats to lives and property in coastal regions. To improve predictions, accurate evaluation of the <span class="hlt">air</span>-sea momentum <span class="hlt">exchange</span> is required. Using current observations recorded during a major tropical cyclone, we have estimated this momentum transfer from the ocean side of the <span class="hlt">air</span>-sea interface, and we discuss it in terms of the drag coefficient. For winds between 20 and 48 meters per second, this coefficient initially increases and peaks at winds of about 32 meters per second before decreasing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=211903&keyword=Biosphere&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=211903&keyword=Biosphere&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>Description and Initial Simulation of a Dynamic Bidirectional <span class="hlt">Air-Surface</span> <span class="hlt">Exchange</span> <span class="hlt">Model</span> for Mercury in Community Multiscale <span class="hlt">Air</span> Quality <span class="hlt">Model</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>Emissions of elemental mercury (Hg<SUP>0</SUP>) from natural processes are believed to be as large as anthropogenic mercury emissions and are a critical source required to <span class="hlt">model</span> the transport and fate of mercury. Recent ecosystem scale measurements indicate that a fraction of rec...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A53F2339R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A53F2339R"><span>Satellite skill in detecting extreme episodes in near-<span class="hlt">surface</span> <span class="hlt">air</span> quality</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruiz, D. J.; Prather, M. J.</p> <p>2017-12-01</p> <p>Ozone (O3) contributes to ambient <span class="hlt">air</span> pollution, adversely affecting public health, agriculture, and ecosystems. Reliable, long-term, densely distributed <span class="hlt">surface</span> networks are required to establish the scale, intensity and repeatability of major pollution events (designated here in a climatological sense as <span class="hlt">air</span> quality extremes, AQX as defined in Schnell's work). Regrettably, such networks are only available for North America (NA) and Europe (EU), which does not include many populated regions where the deaths associated with <span class="hlt">air</span> pollution exposure are alarmingly high. Directly measuring <span class="hlt">surface</span> pollutants from space without lidar is extremely difficult. Mapping of daily pollution events requires cross-track nadir scanners and these have limited sensitivity to <span class="hlt">surface</span> O3 levels. This work examines several years of coincident <span class="hlt">surface</span> and OMI satellite measurements over NA-EU, in combination with a chemistry-transport <span class="hlt">model</span> (CTM) hindcast of that period to understand how the large-scale AQX episodes may extend into the free troposphere and thus be more amenable to satellite mapping. We show how extreme NA-EU episodes are measured from OMI and then look for such patterns over other polluted regions of the globe. We gather individual high-quality O3 <span class="hlt">surface</span> site measurements from these other regions, to check on our satellite detection. Our approach with global satellite detection would avoid issues associated with regional variations in seasonality, chemical regime, data product biases; and it does not require defining a separate absolute threshold for each data product (<span class="hlt">surface</span> site and satellite). This also enables coherent linking of the extreme events into large-scale pollution episodes whose magnitude evolves over 100's of km for several days. Tools used here include the UC Irvine CTM, which shows that much of the O3 <span class="hlt">surface</span> variability is lost at heights above 2 km, but AQX local events are readily seen in a 0-3 km column average. The OMI data are taken from X</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=338083&Lab=NERL&keyword=quality+AND+life&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=338083&Lab=NERL&keyword=quality+AND+life&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><span class="hlt">Modeling</span> the <span class="hlt">Air</span>-Vegetation-Soil <span class="hlt">Exchange</span> of Reactive Nitrogen</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>Nitrogen is an essential building block of all proteins and thus an essential nutrient for all life. However, in excess reactive nitrogen can lead to poor <span class="hlt">air</span> or water quality, loss of biodiversity, and impact respiratory and cardiac health. Human activity has perturbed this cycl...</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/2006IJCli..26.1671E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006IJCli..26.1671E"><span>Simulating <span class="hlt">air</span> temperature in an urban street canyon in all weather conditions using measured data at a reference meteorological station</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Erell, E.; Williamson, T.</p> <p>2006-10-01</p> <p>A <span class="hlt">model</span> is proposed that adapts data from a standard meteorological station to provide realistic site-specific <span class="hlt">air</span> temperature in a city street exposed to the same meso-scale environment. In addition to a rudimentary description of the two sites, the canyon <span class="hlt">air</span> temperature (CAT) <span class="hlt">model</span> requires only inputs measured at standard weather stations; yet it is capable of accurately predicting the evolution of <span class="hlt">air</span> temperature in all weather conditions for extended periods. It simulates the effect of urban geometry on radiant <span class="hlt">exchange</span>; the effect of moisture availability on latent heat flux; energy stored in the ground and in building <span class="hlt">surfaces</span>; <span class="hlt">air</span> flow in the street based on wind above roof height; and the sensible heat flux from individual <span class="hlt">surfaces</span> and from the street canyon as a whole. The CAT <span class="hlt">model</span> has been tested on field data measured in a monitoring program carried out in Adelaide, Australia, in 2000-2001. After calibrating the <span class="hlt">model</span>, predicted <span class="hlt">air</span> temperature correlated well with measured data in all weather conditions over extended periods. The experimental validation provides additional evidence in support of a number of parameterisation schemes incorporated in the <span class="hlt">model</span> to account for sensible heat and storage flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/874378','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874378"><span>Heat <span class="hlt">exchanger</span> with transpired, highly porous fins</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Kutscher, Charles F.; Gawlik, Keith</p> <p>2002-01-01</p> <p>The heat <span class="hlt">exchanger</span> includes a fin and tube assembly with increased heat transfer <span class="hlt">surface</span> area positioned within a hollow chamber of a housing to provide effective heat transfer between a gas flowing within the hollow chamber and a fluid flowing in the fin and tube assembly. A fan is included to force a gas, such as <span class="hlt">air</span>, to flow through the hollow chamber and through the fin and tube assembly. The fin and tube assembly comprises fluid conduits to direct the fluid through the heat <span class="hlt">exchanger</span>, to prevent mixing with the gas, and to provide a heat transfer <span class="hlt">surface</span> or pathway between the fluid and the gas. A heat transfer element is provided in the fin and tube assembly to provide extended heat transfer <span class="hlt">surfaces</span> for the fluid conduits. The heat transfer element is corrugated to form fins between alternating ridges and grooves that define flow channels for directing the gas flow. The fins are fabricated from a thin, heat conductive material containing numerous orifices or pores for transpiring the gas out of the flow channel. The grooves are closed or only partially open so that all or substantially all of the gas is transpired through the fins so that heat is <span class="hlt">exchanged</span> on the front and back <span class="hlt">surfaces</span> of the fins and also within the interior of the orifices, thereby significantly increasing the available the heat transfer <span class="hlt">surface</span> of the heat <span class="hlt">exchanger</span>. The transpired fins also increase heat transfer effectiveness of the heat <span class="hlt">exchanger</span> by increasing the heat transfer coefficient by disrupting boundary layer development on the fins and by establishing other beneficial gas flow patterns, all at desirable pressure drops.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SuTMP...5b4002O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SuTMP...5b4002O"><span>Interpreting contact angle results under <span class="hlt">air</span>, water and oil for the same <span class="hlt">surfaces</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ozkan, Orkun; Yildirim Erbil, H.</p> <p>2017-06-01</p> <p>Under-water and under-oil superhydropobicity and superhydrophilicity have gained significant attention over the last few years. In this study, contact angles on five flat <span class="hlt">surfaces</span> (polypropylene, poly(methyl methacrylate), polycarbonate, TEFLON-FEP and glass slide) were measured in water drop-in-<span class="hlt">air</span>, <span class="hlt">air</span> bubble-under-water, oil drop-in-<span class="hlt">air</span>, <span class="hlt">air</span> bubble-under-oil, oil drop-under-water and water drop-under-oil conditions. Heptane, octane, nonane, decane, dodecane, and hexadecane hydrocarbons were used as oils. Immiscible water/oil pairs were previously mutually saturated to provide thermodynamical equilibrium conditions and their <span class="hlt">surface</span> and interfacial tensions were determined experimentally. These pairs were used in the two-liquid contact angle measurements. <span class="hlt">Surface</span> free energies of the solid <span class="hlt">surfaces</span> in <span class="hlt">air</span> were determined independently by using the van Oss-Good method, using the contact angle results of pure water, ethylene glycol, formamide, methylene iodide and α-bromonaphalene. In addition, Zisman’s ‘critical <span class="hlt">surface</span> tension’ values were also determined for comparison. In theory, the summation of contact angle results in a complementary case would give a total of 180° for ideal <span class="hlt">surfaces</span>. However, it was determined that there are large deviations from this rule in practical cases and these deviations depend on <span class="hlt">surface</span> free energies of solids. Three complementary cases of (water-in-<span class="hlt">air</span> with <span class="hlt">air</span> bubble-under-water); (oil-in-<span class="hlt">air</span> with <span class="hlt">air</span> bubble-under-oil); and (oil-under-water with water-under-oil) were investigated in particular to determine the deviations from ideality. A novel approach, named ‘complementary hysteresis’ [γ WA(cosθ 1  -  cosθ 2) and γ OW(cosθ 6  -  cosθ 5)] was developed where γ WA and γ OW represent the interfacial tensions of water/<span class="hlt">air</span> and oil/water, and θ 1, θ 2, θ 5, and θ 6 were the contact angles of water/<span class="hlt">air</span>, <span class="hlt">air</span> bubble/water, oil/water and water/oil respectively. It was experimentally determined that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140005396','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140005396"><span><span class="hlt">Surface</span> Ocean pCO2 Seasonality and Sea-<span class="hlt">Air</span> CO2 Flux Estimates for the North American East Coast</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Signorini, Sergio; Mannino, Antonio; Najjar, Raymond G., Jr.; Friedrichs, Marjorie A. M.; Cai, Wei-Jun; Salisbury, Joe; Wang, Zhaohui Aleck; Thomas, Helmuth; Shadwick, Elizabeth</p> <p>2013-01-01</p> <p>Underway and in situ observations of <span class="hlt">surface</span> ocean pCO2, combined with satellite data, were used to develop pCO2 regional algorithms to analyze the seasonal and interannual variability of <span class="hlt">surface</span> ocean pCO2 and sea-<span class="hlt">air</span> 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-<span class="hlt">air</span> CO2 flux were derived from the available pCO2 data, as well as from the pCO2 reconstructed by the algorithm. Two different gas <span class="hlt">exchange</span> 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 <span class="hlt">surface</span> ocean pCO2 from the data or algorithm, as well as with the use of the two different gas <span class="hlt">exchange</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27785157','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27785157"><span>Multi-pollutant <span class="hlt">surface</span> objective analyses and mapping of <span class="hlt">air</span> quality health index over North America.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Robichaud, Alain; Ménard, Richard; Zaïtseva, Yulia; Anselmo, David</p> <p>2016-01-01</p> <p><span class="hlt">Air</span> quality, like weather, can affect everyone, but responses differ depending on the sensitivity and health condition of a given individual. To help protect exposed populations, many countries have put in place real-time <span class="hlt">air</span> quality nowcasting and forecasting capabilities. We present in this paper an optimal combination of <span class="hlt">air</span> quality measurements and <span class="hlt">model</span> outputs and show that it leads to significant improvements in the spatial representativeness of <span class="hlt">air</span> quality. The product is referred to as multi-pollutant <span class="hlt">surface</span> objective analyses (MPSOAs). Moreover, based on MPSOA, a geographical mapping of the Canadian <span class="hlt">Air</span> Quality Health Index (AQHI) is also presented which provides users (policy makers, public, <span class="hlt">air</span> quality forecasters, and epidemiologists) with a more accurate picture of the health risk anytime and anywhere in Canada and the USA. Since pollutants can also behave as passive atmospheric tracers, they provide information about transport and dispersion and, hence, reveal synoptic and regional meteorological phenomena. MPSOA could also be used to build <span class="hlt">air</span> pollution climatology, compute local and national trends in <span class="hlt">air</span> quality, and detect systematic biases in numerical <span class="hlt">air</span> quality (AQ) <span class="hlt">models</span>. Finally, initializing AQ <span class="hlt">models</span> at regular time intervals with MPSOA can produce more accurate <span class="hlt">air</span> quality forecasts. It is for these reasons that the Canadian Meteorological Centre (CMC) in collaboration with the <span class="hlt">Air</span> Quality Research Division (AQRD) of Environment Canada has recently implemented MPSOA in their daily operations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70157933','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70157933"><span>Natural radium and radon tracers to quantify water <span class="hlt">exchange</span> and movement in reservoirs</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Smith, Christopher G.; Baskaran, Mark</p> <p>2011-01-01</p> <p>Radon and radium isotopes are routinely used to quantify <span class="hlt">exchange</span> rates between different hydrologic reservoirs. Since their recognition as oceanic tracers in the 1960s, both radon and radium have been used to examine processes such as <span class="hlt">air</span>-sea <span class="hlt">exchange</span>, deep oceanic mixing, benthic inputs, and many others. Recently, the application of radon-222 and the radium-quartet (223,224,226,228Ra) as coastal tracers has seen a revelation with the growing interest in coastal groundwater dynamics. The enrichment of these isotopes in benthic fluids including groundwater makes both radium and radon ideal tracers of coastal benthic processes (e.g. submarine groundwater discharge). In this chapter we review traditional and recent advances in the application of radon and radium isotopes to understand mixing and <span class="hlt">exchange</span> between various hydrologic reservoirs, specifically: (1) atmosphere and ocean, (2) deep and shallow oceanic water masses, (3) coastal groundwater/benthic pore waters and <span class="hlt">surface</span> ocean, and (4) aquifer-lakes. While the isotopes themselves and their distribution in the environment provide qualitative information about the <span class="hlt">exchange</span> processes, it is mixing/<span class="hlt">exchange</span> and transport <span class="hlt">models</span> for these isotopes that provide specific quantitative information about these processes. Brief introductions of these <span class="hlt">models</span> and mixing parameters are provided for both historical and more recent studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25399878','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25399878"><span>Estimation of bias with the single-zone assumption in measurement of residential <span class="hlt">air</span> <span class="hlt">exchange</span> using the perfluorocarbon tracer gas method.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Van Ryswyk, K; Wallace, L; Fugler, D; MacNeill, M; Héroux, M È; Gibson, M D; Guernsey, J R; Kindzierski, W; Wheeler, A J</p> <p>2015-12-01</p> <p>Residential <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) are vital in understanding the temporal and spatial drivers of indoor <span class="hlt">air</span> quality (IAQ). Several methods to quantify AERs have been used in IAQ research, often with the assumption that the home is a single, well-mixed <span class="hlt">air</span> zone. Since 2005, Health Canada has conducted IAQ studies across Canada in which AERs were measured using the perfluorocarbon tracer (PFT) gas method. Emitters and detectors of a single PFT gas were placed on the main floor to estimate a single-zone AER (AER(1z)). In three of these studies, a second set of emitters and detectors were deployed in the basement or second floor in approximately 10% of homes for a two-zone AER estimate (AER(2z)). In total, 287 daily pairs of AER(2z) and AER(1z) estimates were made from 35 homes across three cities. In 87% of the cases, AER(2z) was higher than AER(1z). Overall, the AER(1z) estimates underestimated AER(2z) by approximately 16% (IQR: 5-32%). This underestimate occurred in all cities and seasons and varied in magnitude seasonally, between homes, and daily, indicating that when measuring residential <span class="hlt">air</span> <span class="hlt">exchange</span> using a single PFT gas, the assumption of a single well-mixed <span class="hlt">air</span> zone very likely results in an under prediction of the AER. The results of this study suggest that the long-standing assumption that a home represents a single well-mixed <span class="hlt">air</span> zone may result in a substantial negative bias in <span class="hlt">air</span> <span class="hlt">exchange</span> estimates. Indoor <span class="hlt">air</span> quality professionals should take this finding into consideration when developing study designs or making decisions related to the recommendation and installation of residential ventilation systems. © 2014 Her Majesty the Queen in Right of Canada. Indoor <span class="hlt">Air</span> published by John Wiley & Sons Ltd Reproduced with the permission of the Minister of Health Canada.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29501890','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29501890"><span>Distribution, sources, and <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of OCPs, PCBs and PAHs in urban soils of Nepal.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pokhrel, Balram; Gong, Ping; Wang, Xiaoping; Chen, Mengke; Wang, Chuanfei; Gao, Shaopeng</p> <p>2018-06-01</p> <p>Due to the high temperature and extensive use of organochlorine pesticides (OCPs), polychlorinated biphenyls (PCBs) and polycyclic aromatic hydrocarbons (PAHs), tropical cities could act as secondary sources of these pollutants and therefore received global concern. As compared with other tropical cities, studies on the <span class="hlt">air</span>-soil <span class="hlt">exchange</span> of OCPs, PCBs and PAHs in tropical Nepali cities remained limited. In the present study, 39 soil samples from Kathmandu (capital of Nepal) and 21 soil samples from Pokhara (second largest city in Nepal) were collected The soil concentrations of the sum of endosulfans (α- and β-endosulfans) ranged from 0.01 to 16.4 ng/g dw. Meanwhile, ∑dichlorodiphenyltrichloroethane (DDTs) ranged from 0.01 to 6.5 ng/g dw; ∑6PCBs from 0.01 to 9.7 ng/g dw; and ∑15PAHs from 17.1 to 6219 ng/g dw. High concentrations of OCPs were found in the soil of commercial land, while, high soil PAH concentrations were found on tourist/religious and commercial land. Combined the published <span class="hlt">air</span> concentrations, and the soil data of this study, the directions and fluxes of <span class="hlt">air</span>-soil <span class="hlt">exchange</span> were estimated using a fugacity <span class="hlt">model</span>. It is clear that Nepal is a country contributing prominently to secondary emissions of endosulfans, hexachlorobenzene (HCB), and low molecular weight (LMW) PCBs and PAHs. The flux for all the pollutants in Kathmandu, with ∑endosulfans up to 3553; HCB up to 5263; and ∑LMW-PAHs up to 24378 ng m -2  h -1 , were higher than those in Pokhara. These high flux values indicated the high strength of Nepali soils to act as a source. Copyright © 2018 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910007372','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910007372"><span><span class="hlt">Air</span>-ground interface: <span class="hlt">Surface</span> waves, <span class="hlt">surface</span> impedance and acoustic-to-seismic coupling coefficient</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Daigle, Gilles; Embleton, Tony</p> <p>1990-01-01</p> <p>In atmospheric acoustics, the subject of <span class="hlt">surface</span> waves has been an area of discussion for many years. The existence of an acoustic <span class="hlt">surface</span> wave is now well established theoretically. The mathematical solution for spherical wave propagation above an impedance boundary includes the possibility of a contribution that possesses all the standard properties for a <span class="hlt">surface</span> wave. <span class="hlt">Surface</span> waves exist when the <span class="hlt">surface</span> is sufficiently porous, relative to its acoustical resistance, that it can influence the airborne particle velocity near the <span class="hlt">surface</span> and reduce the phase velocity of sound waves in <span class="hlt">air</span> at the <span class="hlt">surface</span>. This traps some of the sound energy in the <span class="hlt">air</span> to remain near the <span class="hlt">surface</span> as it propagates. Above porous grounds, the existence of <span class="hlt">surface</span> waves has eluded direct experimental confirmation (pulse experiments have failed to show a separate arrival expected from the reduced phase speed) and indirect evidence for its existence has appeared contradictory. The experimental evidence for the existence of an acoustical <span class="hlt">surface</span> wave above porous boundaries is reviewed. Recent measurements including pulse experiments are also described. A few years ago the acoustic impedance of a grass-covered <span class="hlt">surface</span> was measured in the frequency range 30 to 300 Hz. Here, further measurements on the same site are discussed. These measurements include core samples, a shallow refractive survey to determine the seismic velocities, and measurements of the acoustic-to-seismic coupling coefficient.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC33E1118L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC33E1118L"><span>Evaluation of CMIP5 Ability to Reproduce 20th Century Regional Trends in <span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature and Precipitation over CONUS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, J.; Waliser, D. E.; Lee, H.; Loikith, P. C.; Kunkel, K.</p> <p>2017-12-01</p> <p>Monitoring temporal changes in key climate variables, such as <span class="hlt">surface</span> <span class="hlt">air</span> temperature and precipitation, is an integral part of the ongoing efforts of the United States National Climate Assessment (NCA). Climate <span class="hlt">models</span> participating in CMIP5 provide future trends for four different emissions scenarios. In order to have confidence in the future projections of <span class="hlt">surface</span> <span class="hlt">air</span> temperature and precipitation, it is crucial to evaluate the ability of CMIP5 <span class="hlt">models</span> to reproduce observed trends for three different time periods (1895-1939, 1940-1979, and 1980-2005). Towards this goal, trends in <span class="hlt">surface</span> <span class="hlt">air</span> temperature and precipitation obtained from the NOAA nClimGrid 5 km gridded station observation-based product are compared during all three time periods to the 206 CMIP5 historical simulations from 48 unique GCMs and their multi-<span class="hlt">model</span> ensemble (MME) for NCA-defined climate regions during summer (JJA) and winter (DJF). This evaluation quantitatively examines the biases of simulated trends of the spatially averaged temperature and precipitation in the NCA climate regions. The CMIP5 MME reproduces historical <span class="hlt">surface</span> <span class="hlt">air</span> temperature trends for JJA for all time period and all regions, except the Northern Great Plains from 1895-1939 and Southeast during 1980-2005. Likewise, for DJF, the MME reproduces historical <span class="hlt">surface</span> <span class="hlt">air</span> temperature trends across all time periods over all regions except the Southeast from 1895-1939 and the Midwest during 1940-1979. The Regional Climate <span class="hlt">Model</span> Evaluation System (RCMES), an analysis tool which supports the NCA by providing access to data and tools for regional climate <span class="hlt">model</span> validation, facilitates the comparisons between the <span class="hlt">models</span> and observation. The RCMES Toolkit is designed to assist in the analysis of climate variables and the procedure of the evaluation of climate projection <span class="hlt">models</span> to support the decision-making processes. This tool is used in conjunction with the above analysis and results will be presented to demonstrate its capability to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACP....1311073B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACP....1311073B"><span><span class="hlt">Air</span>-sea dimethylsulfide (DMS) gas transfer in the North Atlantic: evidence for limited interfacial gas <span class="hlt">exchange</span> at high wind speed</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bell, T. G.; De Bruyn, W.; Miller, S. D.; Ward, B.; Christensen, K.; Saltzman, E. S.</p> <p>2013-11-01</p> <p>Shipboard measurements of eddy covariance dimethylsulfide (DMS) <span class="hlt">air</span>-sea fluxes and seawater concentration were carried out in the North Atlantic bloom region in June/July 2011. Gas transfer coefficients (k660) show a linear dependence on mean horizontal wind speed at wind speeds up to 11 m s-1. At higher wind speeds the relationship between k660 and wind speed weakens. At high winds, measured DMS fluxes were lower than predicted based on the linear relationship between wind speed and interfacial stress extrapolated from low to intermediate wind speeds. In contrast, the transfer coefficient for sensible heat did not exhibit this effect. The apparent suppression of <span class="hlt">air</span>-sea gas flux at higher wind speeds appears to be related to sea state, as determined from shipboard wave measurements. These observations are consistent with the idea that long waves suppress near-<span class="hlt">surface</span> water-side turbulence, and decrease interfacial gas transfer. This effect may be more easily observed for DMS than for less soluble gases, such as CO2, because the <span class="hlt">air</span>-sea <span class="hlt">exchange</span> of DMS is controlled by interfacial rather than bubble-mediated gas transfer under high wind speed conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/944434','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/944434"><span>Reaction chemistry and ligand <span class="hlt">exchange</span> at cadmium selenide nanocrystal <span class="hlt">surfaces</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>Owen, Jonathan; Park, Jungwon; Trudeau, Paul-Emile</p> <p></p> <p>Chemical modification of nanocrystal <span class="hlt">surfaces</span> is fundamentally important to their assembly, their implementation in biology and medicine, and greatly impacts their electrical and optical properties. However, it remains a major challenge owing to a lack of analytical tools to directly determine nanoparticle <span class="hlt">surface</span> structure. Early nuclear magnetic resonance (NMR) and X-ray photoelectron spectroscopy (XPS) studies of CdSe nanocrystals prepared in tri-n-octylphosphine oxide (1) and tri-n-octylphosphine (2), suggested these coordinating solvents are datively bound to the particle <span class="hlt">surface</span>. However, assigning the broad NMR resonances of <span class="hlt">surface</span>-bound ligands is complicated by significant concentrations of phosphorus-containing impurities in commercial sources of 1, andmore » XPS provides only limited information about the nature of the phosphorus containing molecules in the sample. More recent reports have shown the <span class="hlt">surface</span> ligands of CdSe nanocrystals prepared in technical grade 1, and in the presence of alkylphosphonic acids, include phosphonic and phosphinic acids. These studies do not, however, distinguish whether these ligands are bound datively, as neutral, L-type ligands, or by X-type interaction of an anionic phosphonate/phosphinate moiety with a <span class="hlt">surface</span> Cd{sup 2+} ion. Answering this question would help clarify why ligand <span class="hlt">exchange</span> with such particles does not proceed generally as expected based on a L-type ligand <span class="hlt">model</span>. By using reagents with reactive silicon-chalcogen and silicon-chlorine bonds to cleave the ligands from the nanocrystal <span class="hlt">surface</span>, we show that our CdSe and CdSe/ZnS core-shell nanocrystal <span class="hlt">surfaces</span> are likely terminated by X-type binding of alkylphosphonate ligands to a layer of Cd{sup 2+}/Zn{sup 2+} ions, rather than by dative interactions. Further, we provide spectroscopic evidence that 1 and 2 are not coordinated to our purified nanocrystals.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110016312','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110016312"><span>Thermoelectric <span class="hlt">Air</span>/Soil Energy-Harvesting Device</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Snyder, Jeffrey; Fleurial, Jean-Pierre; Lawrence, Eric</p> <p>2005-01-01</p> <p>A proposed thermoelectric device would exploit natural temperature differences between <span class="hlt">air</span> and soil to harvest small amounts of electric energy. Because the <span class="hlt">air</span>/soil temperature difference fluctuates between nighttime and daytime, it is almost never zero, and so there is almost always some energy available for harvesting. Unlike photovoltaic cells, the proposed device could operate in the absence of sunlight. Unlike a Stirling engine, which could be designed to extract energy from the <span class="hlt">air</span>/soil temperature difference, the proposed device would contain no moving parts. The main attractive feature of the proposed device would be high reliability. In a typical application, this device would be used for low-power charging of a battery that would, in turn, supply high power at brief, infrequent intervals for operating an instrumentation package containing sensors and communication circuits. The device (see figure) would include a heat <span class="hlt">exchanger</span> buried in soil and connected to a heat pipe extending up to a short distance above the ground <span class="hlt">surface</span>. A thermoelectric microgenerator (TEMG) would be mounted on top of the heat pipe. The TEMG could be of an advanced type, now under development, that could maintain high (relative to prior thermoelectric generators) power densities at small temperature differentials. A heat <span class="hlt">exchanger</span> exposed to the <span class="hlt">air</span> would be mounted on top of the TEMG. It would not matter whether the <span class="hlt">air</span> was warmer than the soil or the soil warmer than the <span class="hlt">air</span>: as long as there was a nonzero temperature difference, heat would flow through the device and electricity would be generated. A study of factors that could affect the design and operation of the device has been performed. These factors include the thermal conductances of the soil, the components of the device, the contacts between the components of the device, and the interfaces between the heat <span class="hlt">exchangers</span> and their environments. The study included experiments that were performed on a <span class="hlt">model</span> of the device</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26ES...33a2015A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26ES...33a2015A"><span>Thermodynamic <span class="hlt">model</span> of Ak-Tuz deposit <span class="hlt">surface</span> water formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alekhina, V. M.; Tokaver, I. V.; Ryzhenko, B. N.; Cherkasova, E. V.</p> <p>2016-03-01</p> <p>In Ak-Tuz deposit <span class="hlt">surface</span> water macro and micro components concentrations are measured. Thermodynamic <span class="hlt">model</span> is developed for aqueous composition prognosis at variation of water <span class="hlt">exchange</span>. The concentration of n×10-8 mg Th / kg H2O and more testifies about Th containing colloid species in aqueous solution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H43B1623L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H43B1623L"><span>Assessment of <span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature over China Using Multi-criterion <span class="hlt">Model</span> Ensemble Framework</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, J.; Zhu, Q.; Su, L.; He, X.; Zhang, X.</p> <p>2017-12-01</p> <p>The General Circulation <span class="hlt">Models</span> (GCMs) are designed to simulate the present climate and project future trends. It has been noticed that the performances of GCMs are not always in agreement with each other over different regions. <span class="hlt">Model</span> ensemble techniques have been developed to post-process the GCMs' outputs and improve their prediction reliabilities. To evaluate the performances of GCMs, root-mean-square error, correlation coefficient, and uncertainty are commonly used statistical measures. However, the simultaneous achievements of these satisfactory statistics cannot be guaranteed when using many <span class="hlt">model</span> ensemble techniques. Meanwhile, uncertainties and future scenarios are critical for Water-Energy management and operation. In this study, a new multi-<span class="hlt">model</span> ensemble framework was proposed. It uses a state-of-art evolutionary multi-objective optimization algorithm, termed Multi-Objective Complex Evolution Global Optimization with Principle Component Analysis and Crowding Distance (MOSPD), to derive optimal GCM ensembles and demonstrate the trade-offs among various solutions. Such trade-off information was further analyzed with a robust Pareto front with respect to different statistical measures. A case study was conducted to optimize the <span class="hlt">surface</span> <span class="hlt">air</span> temperature (SAT) ensemble solutions over seven geographical regions of China for the historical period (1900-2005) and future projection (2006-2100). The results showed that the ensemble solutions derived with MOSPD algorithm are superior over the simple <span class="hlt">model</span> average and any single <span class="hlt">model</span> output during the historical simulation period. For the future prediction, the proposed ensemble framework identified that the largest SAT change would occur in the South Central China under RCP 2.6 scenario, North Eastern China under RCP 4.5 scenario, and North Western China under RCP 8.5 scenario, while the smallest SAT change would occur in the Inner Mongolia under RCP 2.6 scenario, South Central China under RCP 4.5 scenario, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25741459','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25741459"><span><span class="hlt">Modeling</span> inflation rates and <span class="hlt">exchange</span> rates in Ghana: application of multivariate GARCH <span class="hlt">models</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nortey, Ezekiel Nn; Ngoh, Delali D; Doku-Amponsah, Kwabena; Ofori-Boateng, Kenneth</p> <p>2015-01-01</p> <p>This paper was aimed at investigating the volatility and conditional relationship among inflation rates, <span class="hlt">exchange</span> rates and interest rates as well as to construct a <span class="hlt">model</span> using multivariate GARCH DCC and BEKK <span class="hlt">models</span> using Ghana data from January 1990 to December 2013. The study revealed that the cumulative depreciation of the cedi to the US dollar from 1990 to 2013 is 7,010.2% and the yearly weighted depreciation of the cedi to the US dollar for the period is 20.4%. There was evidence that, the fact that inflation rate was stable, does not mean that <span class="hlt">exchange</span> rates and interest rates are expected to be stable. Rather, when the cedi performs well on the forex, inflation rates and interest rates react positively and become stable in the long run. The BEKK <span class="hlt">model</span> is robust to <span class="hlt">modelling</span> and forecasting volatility of inflation rates, <span class="hlt">exchange</span> rates and interest rates. The DCC <span class="hlt">model</span> is robust to <span class="hlt">model</span> the conditional and unconditional correlation among inflation rates, <span class="hlt">exchange</span> rates and interest rates. The BEKK <span class="hlt">model</span>, which forecasted high <span class="hlt">exchange</span> rate volatility for the year 2014, is very robust for <span class="hlt">modelling</span> the <span class="hlt">exchange</span> rates in Ghana. The mean equation of the DCC <span class="hlt">model</span> is also robust to forecast inflation rates in Ghana.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21669328','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21669328"><span>Atmospheric concentrations and <span class="hlt">air</span>-soil gas <span class="hlt">exchange</span> of polycyclic aromatic hydrocarbons (PAHs) in remote, rural village and urban areas of Beijing-Tianjin region, North 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, Wentao; Simonich, Staci; Giri, Basant; Chang, Ying; Zhang, Yuguang; Jia, Yuling; Tao, Shu; Wang, Rong; Wang, Bin; Li, Wei; Cao, Jun; Lu, Xiaoxia</p> <p>2011-07-01</p> <p>Forty passive <span class="hlt">air</span> samplers were deployed to study the occurrence of gas and particulate phase PAHs in remote, rural village and urban areas of Beijing-Tianjin region, North China for four seasons (spring, summer, fall and winter) from 2007 to 2008. The influence of emissions on the spatial distribution pattern of <span class="hlt">air</span> PAH concentrations was addressed. In addition, the <span class="hlt">air</span>-soil gas <span class="hlt">exchange</span> of PAHs was studied using fugacity calculations. The median gaseous and particulate phase PAH concentrations were 222 ng/m³ and 114 ng/m³, respectively, with a median total PAH concentration of 349 ng/m³. Higher PAH concentrations were measured in winter than in other seasons. <span class="hlt">Air</span> PAH concentrations measured at the rural villages and urban sites in the northern mountain region were significantly lower than those measured at sites in the southern plain during all seasons. However, there was no significant difference in PAH concentrations between the rural villages and urban sites in the northern and southern areas. This urban-rural PAH distribution pattern was related to the location of PAH emission sources and the population distribution. The location of PAH emission sources explained 56%-77% of the spatial variation in ambient <span class="hlt">air</span> PAH concentrations. The annual median <span class="hlt">air</span>-soil gas <span class="hlt">exchange</span> flux of PAHs was 42.2 ng/m²/day from soil to <span class="hlt">air</span>. Among the 15 PAHs measured, acenaphthylene (ACY) and acenaphthene (ACE) contributed to more than half of the total <span class="hlt">exchange</span> flux. Furthermore, the <span class="hlt">air</span>-soil gas <span class="hlt">exchange</span> fluxes of PAHs at the urban sites were higher than those at the remote and rural sites. In summer, more gaseous PAHs volatilized from soil to <span class="hlt">air</span> because of higher temperatures and increased rainfall. However, in winter, more gaseous PAHs deposited from <span class="hlt">air</span> to soil due to higher PAH emissions and lower temperatures. The soil TOC concentration had no significant influence on the <span class="hlt">air</span>-soil gas <span class="hlt">exchange</span> of PAHs. Copyright © 2011 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.B43D2148B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.B43D2148B"><span>Assessing Near-<span class="hlt">surface</span> Heat, Water Vapor and Carbon Dioxide <span class="hlt">Exchange</span> Over a Coastal Salt-marsh</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.; O'Halloran, T. L.; LeMoine, J.</p> <p>2017-12-01</p> <p>Coastal ecosystems play an important role in mitigating the effects of climate change by storing significant quantities of carbon. A growing number of studies suggest that vegetated estuarine habitats, specifically salt marshes, have high long-term rates of carbon sequestration, perhaps even higher than mature tropical and temperate forests. Large amounts of carbon, accumulated over thousands of years, are stored in the plant materials and sediment. Improved understanding of the factors that control energy and carbon <span class="hlt">exchange</span> is needed to better guide restoration and conservation management practices. To that end, we recently established an observation system to study marsh-atmosphere interactions within the North Inlet-Winyah Bay National Estuarine Research Reserve. Near-<span class="hlt">surface</span> fluxes of heat, water vapor (H2O) and carbon dioxide (CO2) were measured by an eddy-covariance system consisting of an aerodynamic open-path H2O / CO2 gas analyzer with a spatially integrated 3D sonic anemometer/thermometer (IRGASON). The IRGASON instrument provides co-located and highly synchronized, fast response H2O, CO2 and <span class="hlt">air</span>- temperature measurements, which eliminates the need for spectral corrections associated with the separation between the sonic anemometer and the gas analyzer. This facilitates calculating the instantaneous CO2 molar mixing ratio relative to dry <span class="hlt">air</span>. Fluxes computed from CO2 and H2O mixing ratios, which are conserved quantities, do not require post-processing corrections for <span class="hlt">air</span>-density changes associated with temperature and water vapor fluctuations. These corrections are particularly important for CO2, because they could be even larger than the measured flux. Here we present the normalized frequency spectra of <span class="hlt">air</span> temperature, water vapor and CO2, as well as their co-spectra with the co-located vertical wind. We also show mean daily cycles of sensible, latent and CO2 fluxes and analyze correlations with <span class="hlt">air</span>/water temperature, wind speed and light availability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1214990','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1214990"><span><span class="hlt">Air</span>-Cooled Heat <span class="hlt">Exchanger</span> for High-Temperature Power Electronics: Preprint</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>Waye, S. K.; Lustbader, J.; Musselman, M.</p> <p>2015-05-06</p> <p>This work demonstrates a direct <span class="hlt">air</span>-cooled heat <span class="hlt">exchanger</span> strategy for high-temperature power electronic devices with an application specific to automotive traction drive inverters. We present experimental heat dissipation and system pressure curves versus flow rate for baseline and optimized sub-module assemblies containing two ceramic resistance heaters that provide device heat fluxes. The maximum allowable junction temperature was set to 175 deg.C. Results were extrapolated to the inverter scale and combined with balance-of-inverter components to estimate inverter power density and specific power. The results exceeded the goal of 12 kW/L and 12 kW/kg for power density and specific power, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A11H3088O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A11H3088O"><span>Evaluating the Vertical Distribution of Ozone and its Relationship to Pollution Events in <span class="hlt">Air</span> Quality <span class="hlt">Models</span> using Satellite Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Osterman, G. B.; Neu, J. L.; Eldering, A.; Pinder, R. W.; Tang, Y.; McQueen, J.</p> <p>2014-12-01</p> <p>Most regional scale <span class="hlt">models</span> that are used for <span class="hlt">air</span> quality forecasts and ozone source attribution do not adequately capture the distribution of ozone in the mid- and upper troposphere, but it is unclear how this shortcoming relates to their ability to simulate <span class="hlt">surface</span> ozone. We combine ozone profile data from the NASA Earth Observing System (EOS) Tropospheric Emission Spectrometer (TES) and a new joint product from TES and the Ozone Monitoring Instrument along with ozonesonde measurements and EPA <span class="hlt">Air</span>Now ground station ozone data to examine <span class="hlt">air</span> quality events during August 2006 in the Community Multi-Scale <span class="hlt">Air</span> Quality (CMAQ) and National <span class="hlt">Air</span> Quality Forecast Capability (NAQFC) <span class="hlt">models</span>. We present both aggregated statistics and case-study analyses with the goal of assessing the relationship between the <span class="hlt">models</span>' ability to reproduce <span class="hlt">surface</span> <span class="hlt">air</span> quality events and their ability to capture the vertical distribution of ozone. We find that the <span class="hlt">models</span> lack the mid-tropospheric ozone variability seen in TES and the ozonesonde data, and discuss the conditions under which this variability appears to be important for <span class="hlt">surface</span> <span class="hlt">air</span> quality.</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('http://adsabs.harvard.edu/abs/2011EPJAP..5423406Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011EPJAP..5423406Z"><span>Steady state macroscopic <span class="hlt">model</span> of the influence of water on the performances of a micro <span class="hlt">air</span>-breathing fuel cell</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zeidan, M.; Turpin, Ch.; Cantin, F.; Astier, S.</p> <p>2011-05-01</p> <p>Water management is one of the most crucial issues to drive PEM fuel cells. The challenge is enhanced in the case of micro <span class="hlt">air</span>-breathing proton <span class="hlt">exchange</span> membrane fuel cells (μABFC): their thinness and their reduced <span class="hlt">surface</span> indeed make their hydration state fast changing and very sensitive to the experimental conditions (temperature and relative humidity (RH)). It can lead to strong flooding or drying out issues. Firstly, this study highlights this sensitivity by various measurements. Then a steady state macroscopic <span class="hlt">model</span> for the μABFC is proposed, focusing on the cathode, using a rather original approach for diffusion in porous media. Finally, a literal steady state formula for the water content is provided, and its influences on the performances of the μABFC are explicitly proposed. The <span class="hlt">model</span> is parameterized and compared to measures in several atmospheric conditions.</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 CO2 <span class="hlt">exchange</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>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 CO2 flux was directly measured above a small, woodland lake using the eddy covariance technique and compared with fluxes deduced from changes in measured lake-water CO2 storage and with flux predictions from boundary-layer and <span class="hlt">surface</span>-renewal <span class="hlt">models</span>. Over a 3-yr period, lake-atmosphere <span class="hlt">exchanges</span> of CO2 were measured over 5 weeks in spring, summer, and fall. Observed springtime CO2 efflux was large (2.3-2.7 ??mol m-2 s-1) immediately after lake-thaw. That efflux decreased exponentially with time to less than 0.2 ??mol m-2 s-1 within 2 weeks. Substantial interannual variability was found in the magnitudes of springtime efflux, <span class="hlt">surface</span> water CO2 concentrations, lake CO2 storage, and meteorological conditions. Summertime measurements show a weak diurnal trend with a small average downward flux (-0.17 ??mol m-2 s-1) to the lake's <span class="hlt">surface</span>, while late fall flux was trendless and smaller (-0.0021 ??mol m-2 s-1). Large springtime efflux afforded an opportunity to make direct measurement of lake-atmosphere fluxes well above the detection limits of eddy covariance instruments, facilitating the testing of different gas flux methodologies and <span class="hlt">air</span>-water gas-transfer <span class="hlt">models</span>. Although there was an overall agreement in fluxes determined by eddy covariance and those calculated from lake-water storage change in CO2, agreement was inconsistent between eddy covariance flux measurements and fluxes predicted by boundary-layer and <span class="hlt">surface</span>-renewal <span class="hlt">models</span>. Comparison of measured and <span class="hlt">modeled</span> transfer velocities for CO2, along with measured and <span class="hlt">modeled</span> cumulative CO2 flux, indicates that in most instances the <span class="hlt">surface</span>-renewal <span class="hlt">model</span> underpredicts actual flux. Greater underestimates were found with comparisons involving homogeneous boundary-layer <span class="hlt">models</span>. No physical mechanism responsible for the inconsistencies was identified by analyzing coincidentally measured environmental variables.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990019562&hterms=skin+sensors&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dskin%2Bsensors','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990019562&hterms=skin+sensors&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dskin%2Bsensors"><span>Assimilation of Goes-Derived Skin Temperature Tendencies into Mesoscale <span class="hlt">Models</span> to Improve Forecasts of near <span class="hlt">Surface</span> <span class="hlt">Air</span> Temperature and Mixing Ratio</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lapenta, William M.; McNider, Richard T.; Suggs, Ron; Jedlovec, Gary; Robertson, Franklin R.</p> <p>1998-01-01</p> <p>A technique has been developed for assimilating GOES-FR skin temperature tendencies into the <span class="hlt">surface</span> energy budget equation of a mesoscale <span class="hlt">model</span> so that the simulated rate of temperature chance closely agrees with the satellite observations. A critical assumption of the technique is that the availability of moisture (either from the soil or vegetation) is the least known term in the <span class="hlt">model</span>'s <span class="hlt">surface</span> energy budget. Therefore, the simulated latent heat flux, which is a function of <span class="hlt">surface</span> moisture availability, is adjusted based upon differences between the <span class="hlt">modeled</span> and satellite-observed skin temperature tendencies. An advantage of this technique is that satellite temperature tendencies are assimilated in an energetically consistent manner that avoids energy imbalances and <span class="hlt">surface</span> stability problems that arise from direct assimilation of <span class="hlt">surface</span> shelter temperatures. The fact that the rate of change of the satellite skin temperature is used rather than the absolute temperature means that sensor calibration is not as critical. An advantage of this technique for short-range forecasts (0-48 h) is that it does not require a complex land-<span class="hlt">surface</span> formulation within the atmospheric <span class="hlt">model</span>. As a result, the need to specify poorly known soil and vegetative characteristics is eliminated. The GOES assimilation technique has been incorporated into the PSU/NCAR MM5. Results will be presented to demonstrate the ability of the assimilation scheme to improve short- term (0-48h) simulations of near-<span class="hlt">surface</span> <span class="hlt">air</span> temperature and mixing ratio during the warm season for several selected cases which exhibit a variety of atmospheric and land-<span class="hlt">surface</span> conditions. In addition, validation of terms in the simulated <span class="hlt">surface</span> energy budget will be presented using in situ data collected at the Southern Great Plains (SGP) Cloud And Radiation Testbed (CART) site as part of the Atmospheric Radiation Measurements Program (ARM).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012WRR....48.9530B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012WRR....48.9530B"><span>A physically based <span class="hlt">model</span> of global freshwater <span class="hlt">surface</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>Beek, Ludovicus P. H.; Eikelboom, Tessa; Vliet, Michelle T. H.; Bierkens, Marc F. P.</p> <p>2012-09-01</p> <p>Temperature determines a range of physical properties of water and exerts a strong control on <span class="hlt">surface</span> water biogeochemistry. Thus, in freshwater ecosystems the thermal regime directly affects the geographical distribution of aquatic species through their growth and metabolism and indirectly through their tolerance to parasites and diseases. <span class="hlt">Models</span> used to predict <span class="hlt">surface</span> water temperature range between physically based deterministic <span class="hlt">models</span> and statistical approaches. Here we present the initial results of a physically based deterministic <span class="hlt">model</span> of global freshwater <span class="hlt">surface</span> temperature. The <span class="hlt">model</span> adds a <span class="hlt">surface</span> water energy balance to river discharge <span class="hlt">modeled</span> by the global hydrological <span class="hlt">model</span> PCR-GLOBWB. In addition to advection of energy from direct precipitation, runoff, and lateral <span class="hlt">exchange</span> along the drainage network, energy is <span class="hlt">exchanged</span> between the water body and the atmosphere by shortwave and longwave radiation and sensible and latent heat fluxes. Also included are ice formation and its effect on heat storage and river hydraulics. We use the coupled <span class="hlt">surface</span> water and energy balance <span class="hlt">model</span> to simulate global freshwater <span class="hlt">surface</span> temperature at daily time steps with a spatial resolution of 0.5° on a regular grid for the period 1976-2000. We opt to parameterize the <span class="hlt">model</span> with globally available data and apply it without calibration in order to preserve its physical basis with the outlook of evaluating the effects of atmospheric warming on freshwater <span class="hlt">surface</span> temperature. We validate our simulation results with daily temperature data from rivers and lakes (U.S. Geological Survey (USGS), limited to the USA) and compare mean monthly temperatures with those recorded in the Global Environment Monitoring System (GEMS) data set. Results show that the <span class="hlt">model</span> is able to capture the mean monthly <span class="hlt">surface</span> temperature for the majority of the GEMS stations, while the interannual variability as derived from the USGS and NOAA data was captured reasonably well. Results are poorest for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080039287','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080039287"><span>Improved <span class="hlt">Surface</span> Parameter Retrievals using <span class="hlt">AIRS</span>/AMSU Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Susskind, Joel; Blaisdell, John</p> <p>2008-01-01</p> <p>The <span class="hlt">AIRS</span> Science Team Version 5.0 retrieval algorithm became operational at the Goddard DAAC in July 2007 generating near real-time products from analysis of <span class="hlt">AIRS</span>/AMSU sounding data. This algorithm contains many significant theoretical advances over the <span class="hlt">AIRS</span> Science Team Version 4.0 retrieval algorithm used previously. Two very significant developments of Version 5 are: 1) the development and implementation of an improved Radiative Transfer Algorithm (RTA) which allows for accurate treatment of non-Local Thermodynamic Equilibrium (non-LTE) effects on shortwave sounding channels; and 2) the development of methodology to obtain very accurate case by case product error estimates which are in turn used for quality control. These theoretical improvements taken together enabled a new methodology to be developed which further improves soundings in partially cloudy conditions. In this methodology, longwave C02 channel observations in the spectral region 700 cm(exp -1) to 750 cm(exp -1) are used exclusively for cloud clearing purposes, while shortwave C02 channels in the spectral region 2195 cm(exp -1) 2395 cm(exp -1) are used for temperature sounding purposes. This allows for accurate temperature soundings under more difficult cloud conditions. This paper further improves on the methodology used in Version 5 to derive <span class="hlt">surface</span> skin temperature and <span class="hlt">surface</span> spectral emissivity from <span class="hlt">AIRS</span>/AMSU observations. Now, following the approach used to improve tropospheric temperature profiles, <span class="hlt">surface</span> skin temperature is also derived using only shortwave window channels. This produces improved <span class="hlt">surface</span> parameters, both day and night, compared to what was obtained in Version 5. These in turn result in improved boundary layer temperatures and retrieved total O3 burden.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15244753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15244753"><span>Ultrashort laser pulses and electromagnetic pulse generation in <span class="hlt">air</span> and on dielectric <span class="hlt">surfaces</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sprangle, P; Peñano, J R; Hafizi, B; Kapetanakos, C A</p> <p>2004-06-01</p> <p>Intense, ultrashort laser pulses propagating in the atmosphere have been observed to emit sub-THz electromagnetic pulses (EMPS). The purpose of this paper is to analyze EMP generation from the interaction of ultrashort laser pulses with <span class="hlt">air</span> and with dielectric <span class="hlt">surfaces</span> and to determine the efficiency of conversion of laser energy to EMP energy. In our self-consistent <span class="hlt">model</span> the laser pulse partially ionizes the medium, forms a plasma filament, and through the ponderomotive forces associated with the laser pulse, drives plasma currents which are the source of the EMP. The propagating laser pulse evolves under the influence of diffraction, Kerr focusing, plasma defocusing, and energy depletion due to electron collisions and ionization. Collective effects and recombination processes are also included in the <span class="hlt">model</span>. The duration of the EMP in <span class="hlt">air</span>, at a fixed point, is found to be a few hundred femtoseconds, i.e., on the order of the laser pulse duration plus the electron collision time. For steady state laser pulse propagation the flux of EMP energy is nonradiative and axially directed. Radiative EMP energy is present only for nonsteady state or transient laser pulse propagation. The analysis also considers the generation of EMP on the <span class="hlt">surface</span> of a dielectric on which an ultrashort laser pulse is incident. For typical laser parameters, the power and energy conversion efficiency from laser radiation to EMP radiation in both <span class="hlt">air</span> and from dielectric <span class="hlt">surfaces</span> is found to be extremely small, < 10(-8). Results of full-scale, self-consistent, numerical simulations of atmospheric and dielectric <span class="hlt">surface</span> EMP generation are presented. A recent experiment on atmospheric EMP generation is also simulated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24433879','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24433879"><span>Impact of indoor <span class="hlt">surface</span> material on perceived <span class="hlt">air</span> quality.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Senitkova, I</p> <p>2014-03-01</p> <p>The material combination impact on perceived indoor <span class="hlt">air</span> quality for various <span class="hlt">surface</span> interior materials is presented in this paper. The chemical analysis and sensory assessments identifies health adverse of indoor <span class="hlt">air</span> pollutants (TVOCs). In this study, emissions and odors from different common indoor <span class="hlt">surface</span> materials were investigated in glass test chamber under standardized conditions. Chemical measurements (TVOC concentration) and sensory assessments (odor intensity, <span class="hlt">air</span> acceptability) were done after building materials exposure to standardized conditions. The results of the chemical and sensory assessment of individual materials and their combinations are compared and discussed within the paper. The using possibility of individual material <span class="hlt">surface</span> sorption ability was investigated. The knowledge of targeted sorption effects can be used in the interior design phase. The results demonstrate the various sorption abilities of various indoor materials as well as the various sorption abilities of the same indoor material in various combinations. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1917789G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1917789G"><span>Assessment of the uncertainties in <span class="hlt">air</span> mass and pollutants transboundary <span class="hlt">exchange</span> over the continental part of the EANET region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gromov, Sergey S.; Trifonova-Yakovleva, Alisa; Gromov, Sergey A.</p> <p>2017-04-01</p> <p>In this study, we attempt to quantify the uncertainties in <span class="hlt">air</span> mass <span class="hlt">exchange</span> in the lower troposphere across two regions of the Russian border in Eastern Siberia and the Russian Far East in 2000-2015. We use meteorological data from long-term <span class="hlt">air</span> sound data (ASD) on mean layer winds [1] and from the ERA INTERIM re-analysis (EIR) project [2]. Using a transboundary <span class="hlt">exchange</span> <span class="hlt">model</span>, we estimate the total and net amounts of <span class="hlt">air</span> crossing the boundary segments around Irkutsk (IR) and Vladivostok (VL) aerological stations. We compare transport terms derived (i) from the long-term wind statistics based on both ASD and EIR data, and (ii) from integrating 6h meteorological winds from EIR directly over the border segments cells. We find similar wind direction statistics in both meteorological datasets, however EIR favours stronger westerly winds at VL in summer, which results in more often <span class="hlt">air</span> export from China to Russia in the Far East. There is less agreement on the wind strengths than wind directions between the datasets, with EIR often providing slower wind speeds. The resulting climatic (ASD) and directly (from EIR 6h terms) calculated non-equilibrium (net) transport terms are comparable in orders (tens of million km3/month), however may differ substantially in temporal evolution or/and magnitude. Thus, EIR net transport over the IR segment has similar annual dynamics but is higher by a factor of ˜ 4 (maxima of 3.6 vs. 12 of 106 km3/month in December, respectively). An opposite ratio is derived for the VL segment (average ˜ 6 vs. 13 of 106 km3/month), with a distinct seasonality in the ASD but not in the EIR data. We attribute this discrepancy to the variations in wind direction with altitude, which cannot be resolved in the <span class="hlt">model</span> fed with the ASD data. Calculated transport in the boundary layer (BL, provided by the EIR) supports this inference. Thus, the BL net transport temporal dynamics differ substantially from that within the 3 km layer, owing to the BL diurnal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920022003','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920022003"><span>Computer program to solve two-dimensional shock-wave interference problems with an equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Glass, Christopher E.</p> <p>1990-01-01</p> <p>The computer program EASI, an acronym for Equilibrium <span class="hlt">Air</span> Shock Interference, was developed to calculate the inviscid flowfield, the maximum <span class="hlt">surface</span> pressure, and the maximum heat flux produced by six shock wave interference patterns on a 2-D, cylindrical configuration. Thermodynamic properties of the inviscid flowfield are determined using either an 11-specie, 7-reaction equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span> or a calorically perfect <span class="hlt">air</span> <span class="hlt">model</span>. The inviscid flowfield is solved using the integral form of the conservation equations. <span class="hlt">Surface</span> heating calculations at the impingement point for the equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span> use variable transport properties and specific heat. However, for the calorically perfect <span class="hlt">air</span> <span class="hlt">model</span>, heating rate calculations use a constant Prandtl number. Sample calculations of the six shock wave interference patterns, a listing of the computer program, and flowcharts of the programming logic are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990STIN...9231247G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990STIN...9231247G"><span>Computer program to solve two-dimensional shock-wave interference problems with an equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Glass, Christopher E.</p> <p>1990-08-01</p> <p>The computer program EASI, an acronym for Equilibrium <span class="hlt">Air</span> Shock Interference, was developed to calculate the inviscid flowfield, the maximum <span class="hlt">surface</span> pressure, and the maximum heat flux produced by six shock wave interference patterns on a 2-D, cylindrical configuration. Thermodynamic properties of the inviscid flowfield are determined using either an 11-specie, 7-reaction equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span> or a calorically perfect <span class="hlt">air</span> <span class="hlt">model</span>. The inviscid flowfield is solved using the integral form of the conservation equations. <span class="hlt">Surface</span> heating calculations at the impingement point for the equilibrium chemically reacting <span class="hlt">air</span> <span class="hlt">model</span> use variable transport properties and specific heat. However, for the calorically perfect <span class="hlt">air</span> <span class="hlt">model</span>, heating rate calculations use a constant Prandtl number. Sample calculations of the six shock wave interference patterns, a listing of the computer program, and flowcharts of the programming logic are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4490136','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4490136"><span><span class="hlt">Air</span> <span class="hlt">exchange</span> rates and migration of VOCs in basements and residences</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Du, Liuliu; Batterman, Stuart; Godwin, Christopher; Rowe, Zachary; Chin, Jo-Yu</p> <p>2015-01-01</p> <p>Basements can influence indoor <span class="hlt">air</span> quality by affecting <span class="hlt">air</span> <span class="hlt">exchange</span> rates (AERs) and by the presence of emission sources of volatile organic compounds (VOCs) and other pollutants. We characterized VOC levels, AERs and interzonal flows between basements and occupied spaces in 74 residences in Detroit, Michigan. Flows were measured using a steady-state multi-tracer system, and 7-day VOC measurements were collected using passive samplers in both living areas and basements. A walkthrough survey/inspection was conducted in each residence. AERs in residences and basements averaged 0.51 and 1.52 h−1, respectively, and had strong and opposite seasonal trends, e.g., AERs were highest in residences during the summer, and highest in basements during the winter. <span class="hlt">Air</span> flows from basements to occupied spaces also varied seasonally. VOC concentration distributions were right-skewed, e.g., 90th percentile benzene, toluene, naphthalene and limonene concentrations were 4.0, 19.1, 20.3 and 51.0 μg m−3, respectively; maximum concentrations were 54, 888, 1117 and 134 μg m−3. Identified VOC sources in basements included solvents, household cleaners, <span class="hlt">air</span> fresheners, smoking, and gasoline-powered equipment. The number and type of potential VOC sources found in basements are significant and problematic, and may warrant advisories regarding the storage and use of potentially strong VOCs sources in basements. PMID:25601281</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JQSRT.195..119T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JQSRT.195..119T"><span>Effects of ice crystal <span class="hlt">surface</span> roughness and <span class="hlt">air</span> bubble inclusions on cirrus cloud radiative properties from remote sensing perspective</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Guanglin; Panetta, R. Lee; Yang, Ping; Kattawar, George W.; Zhai, Peng-Wang</p> <p>2017-07-01</p> <p>We study the combined effects of <span class="hlt">surface</span> roughness and inhomogeneity on the optical scattering properties of ice crystals and explore the consequent implications to remote sensing of cirrus cloud properties. Specifically, <span class="hlt">surface</span> roughness and inhomogeneity are added to the Moderate Resolution Imaging Spectroradiometer (MODIS) collection 6 (MC6) cirrus cloud particle habit <span class="hlt">model</span>. Light scattering properties of the new habit <span class="hlt">model</span> are simulated using a modified version of the Improved Geometric Optics Method (IGOM). Both inhomogeneity and <span class="hlt">surface</span> roughness affect the single scattering properties significantly. In visible bands, inhomogeneity and <span class="hlt">surface</span> roughness both tend to smooth the phase function and eliminate halos and the backscattering peak. The asymmetry parameter varies with the degree of <span class="hlt">surface</span> roughness following a U shape - decreases and then increases - with a minimum at around 0.15, whereas it decreases monotonically with the <span class="hlt">air</span> bubble volume fraction. <span class="hlt">Air</span> bubble inclusions significantly increase phase matrix element -P12 for scattering angles between 20°-120°, whereas <span class="hlt">surface</span> roughness has a much weaker effect, increasing -P12 slightly from 60°-120°. Radiative transfer simulations and cirrus cloud property retrievals are conducted by including both the factors. In terms of <span class="hlt">surface</span> roughness and <span class="hlt">air</span> bubble volume fraction, retrievals of cirrus cloud optical thickness or the asymmetry parameter using solar bands show similar patterns of variation. Polarimetric simulations using the MC6 cirrus cloud particle habit <span class="hlt">model</span> are shown to be more consistent with observations when both <span class="hlt">surface</span> roughness and inhomogeneity are simultaneously considered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=60376&keyword=high+AND+flow+AND+oxygen&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=60376&keyword=high+AND+flow+AND+oxygen&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>GROUNDWATER-<span class="hlt">SURFACE</span> WATER <span class="hlt">EXCHANGE</span> AND IMPLICATIONS FOR LARGE RIVER RESTORATION</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>Movement of river water into and out of high-porosity alluvial deposits can have an important influence on <span class="hlt">surface</span> water quality and aquatic habitat. In our study of a 60-km reach of the Willamette River in Oregon, USA, we: 1) used tracers to estimate the rate of <span class="hlt">exchange</span> betw...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS11A1775K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS11A1775K"><span>Atmospheric Transference of the Toxic Burden of Atmosphere-<span class="hlt">Surface</span> <span class="hlt">Exchangeable</span> Pollutants to the Great Lakes Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, A.; Perlinger, J. A.; Giang, A.; Zhang, H.; Selin, N. E.; Wu, S.</p> <p>2016-12-01</p> <p>Toxic pollutants that share certain chemical properties undergo repeated emission and deposition between Earth's <span class="hlt">surfaces</span> and the atmosphere. Following their emission through anthropogenic activities, they are transported locally, regionally or globally through the atmosphere, are deposited, and impact local ecosystems, in some cases as a result of bioaccumulation in food webs. We call them atmosphere-<span class="hlt">surface</span> <span class="hlt">exchangeable</span> pollutants or "ASEPs", wherein this group is comprised of thousands of chemicals. We are studying potential future contamination in the Great Lakes region by <span class="hlt">modeling</span> scenarios of the future for three compounds/compound classes, mercury, polychlorinated biphenyl compounds, and polycyclic aromatic hydrocarbons. In this presentation we focus on mercury and future scenarios of contamination of the Great Lake region. The atmospheric transport of mercury under specific scenarios will be discussed. The global 3-D chemical transport <span class="hlt">model</span> GEOS-Chem has been applied to estimate future atmospheric concentrations and deposition rates of mercury in the Great Lakes region for selected future scenarios of emissions and climate. We find that, assuming no changes in climate, annual mean net deposition flux of mercury to the Great Lakes Region may increase by approximately 50% over 2005 levels by 2050, without global or regional policies addressing mercury, <span class="hlt">air</span> pollution, and climate. In contrast, we project that the combination of global and North American action on mercury could lead to a 21% reduction in deposition from 2005 levels by 2050. US action alone results in a projected 18% reduction over 2005 levels by 2050. We also find that, assuming no changes in anthropogenic emissions, climate change and biomass burning emissions would, respectively, cause annual mean net deposition flux of mercury to the Great Lakes Region to increase by approximately 5% and decrease by approximately 2% over 2000 levels by 2050.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS23B2025O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS23B2025O"><span>Field Observations of Coastal <span class="hlt">Air</span>-Sea Interaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ortiz-Suslow, D. G.; Haus, B. K.; Williams, N. J.; Graber, H. C.</p> <p>2016-12-01</p> <p>In the nearshore zone wind, waves, and currents generated from different forcing mechanisms converge in shallow water. This can profoundly affect the physical nature of the ocean <span class="hlt">surface</span>, which can significantly modulate the <span class="hlt">exchange</span> of momentum, heat, and mass across the <span class="hlt">air</span>-sea interface. For decades, the focus of <span class="hlt">air</span>-sea interaction research has been on the open ocean while the shallow water regime has been relatively under-explored. This bears implications for efforts to understand and <span class="hlt">model</span> various coastal processes, such as mixing, <span class="hlt">surface</span> transport, and <span class="hlt">air</span>-sea gas flux. The results from a recent study conducted at the New River Inlet in North Carolina showed that directly measured <span class="hlt">air</span>-sea flux parameters, such as the atmospheric drag coefficient, are strong functions of space as well as the ambient conditions (i.e. wind speed and direction). The drag is typically used to parameterize the wind stress magnitude. It is generally assumed that the wind direction is the direction of the atmospheric forcing (i.e. wind stress), however significant wind stress steering off of the azimuthal wind direction was observed and was found to be related to the horizontal <span class="hlt">surface</span> current shear. The authors have just returned from a field campaign carried out within Monterey Bay in California. <span class="hlt">Surface</span> observations made from two research vessels were complimented by an array of beach and inland flux stations, high-resolution wind forecasts, and satellite image acquisitions. This is a rich data set and several case studies will be analyzed to highlight the importance of various processes for understanding the <span class="hlt">air</span>-sea fluxes. Preliminary findings show that interactions between the local wind-sea and the shoaling, incident swell can have a profound effect on the wind stress magnitude. The Monterey Bay coastline contains a variety of topographical features and the importance of land-<span class="hlt">air</span>-sea interactions will also be investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003148','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003148"><span>Brief Communication: Upper <span class="hlt">Air</span> Relaxation in RACMO2 Significantly Improves <span class="hlt">Modelled</span> Interannual <span class="hlt">Surface</span> Mass Balance Variability in Antarctica</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>van de Berg, W. J.; Medley, B.</p> <p>2016-01-01</p> <p>The Regional Atmospheric Climate <span class="hlt">Model</span> (RACMO2) has been a powerful tool for improving <span class="hlt">surface</span> mass balance (SMB) estimates from GCMs or reanalyses. However, new yearly SMB observations for West Antarctica show that the <span class="hlt">modelled</span> interannual variability in SMB is poorly simulated by RACMO2, in contrast to ERA-Interim, which resolves this variability well. In an attempt to remedy RACMO2 performance, we included additional upper-<span class="hlt">air</span> relaxation (UAR) in RACMO2. With UAR, the correlation to observations is similar for RACMO2 and ERA-Interim. The spatial SMB patterns and ice-sheet-integrated SMB <span class="hlt">modelled</span> using UAR remain very similar to the estimates of RACMO2 without UAR. We only observe an upstream smoothing of precipitation in regions with very steep topography like the Antarctic Peninsula. We conclude that UAR is a useful improvement for regional climate <span class="hlt">model</span> simulations, although results in regions with steep topography should be treated with care.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993ONERA..75.....A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993ONERA..75.....A"><span>High temperature heat <span class="hlt">exchangers</span> for gas turbines and future hypersonic <span class="hlt">air</span> breathing propulsion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Avran, Patrick; Bernard, Pierre</p> <p></p> <p>After surveying the results of ONERA's investigations to date of metallic and ceramic heat <span class="hlt">exchangers</span> applicable to automotive and aircraft powerplants, which are primarily of finned-tube counterflow configuration, attention is given to the influence of heat-<span class="hlt">exchanger</span> effectiveness on fuel consumption and <span class="hlt">exchanger</span> dimensions and weight. Emphasis is placed on the results of studies of cryogenic heat <span class="hlt">exchangers</span> used by airbreathing hypersonic propulsion systems. The numerical codes developed by ONERA for the <span class="hlt">modeling</span> of heat <span class="hlt">exchanger</span> thermodynamics are evaluated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860034311&hterms=current+feedback&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcurrent%2Bfeedback','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860034311&hterms=current+feedback&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcurrent%2Bfeedback"><span>Sea <span class="hlt">surface</span> temperature anomalies, planetary waves, and <span class="hlt">air</span>-sea feedback in the middle latitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Frankignoul, C.</p> <p>1985-01-01</p> <p>Current analytical <span class="hlt">models</span> for large-scale <span class="hlt">air</span>-sea interactions in the middle latitudes are reviewed in terms of known sea-<span class="hlt">surface</span> temperature (SST) anomalies. The scales and strength of different atmospheric forcing mechanisms are discussed, along with the damping and feedback processes controlling the evolution of the SST. Difficulties with effective SST <span class="hlt">modeling</span> are described in terms of the techniques and results of case studies, numerical simulations of mixed-layer variability and statistical <span class="hlt">modeling</span>. The relationship between SST and diabatic heating anomalies is considered and a linear <span class="hlt">model</span> is developed for the response of the stationary atmosphere to the <span class="hlt">air</span>-sea feedback. The results obtained with linear wave <span class="hlt">models</span> are compared with the linear <span class="hlt">model</span> results. Finally, sample data are presented from experiments with general circulation <span class="hlt">models</span> into which specific SST anomaly data for the middle latitudes were introduced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980004095','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980004095"><span>Assimilation of Satellite Data in Regional <span class="hlt">Air</span> Quality <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mcnider, Richard T.; Norris, William B.; Casey, Daniel; Pleim, Jonathan E.; Roselle, Shawn J.; Lapenta, William M.</p> <p>1997-01-01</p> <p>In terms of important uncertainty in regional-scale <span class="hlt">air</span>-pollution <span class="hlt">models</span>, probably no other aspect ranks any higher than the current ability to specify clouds and soil moisture on the regional scale. Because clouds in <span class="hlt">models</span> are highly parameterized, the ability of <span class="hlt">models</span> to predict the correct spatial and radiative characteristics is highly suspect and subject to large error. The poor representation of cloud fields from point measurements at National Weather Services stations and the almost total absence of <span class="hlt">surface</span> moisture availability observations has made assimilation of these variables difficult to impossible. Yet, the correct inclusion of clouds and <span class="hlt">surface</span> moisture are of first-order importance in regional-scale photochemistry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15737155','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15737155"><span>The effectiveness of stand alone <span class="hlt">air</span> cleaners for shelter-in-place.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ward, M; Siegel, J A; Corsi, R L</p> <p>2005-04-01</p> <p>Stand-alone <span class="hlt">air</span> cleaners may be efficient for rapid removal of indoor fine particles and have potential use for shelter-in-place (SIP) strategies following acts of bioterrorism. A screening <span class="hlt">model</span> was employed to ascertain the potential significance of size-resolved particle (0.1-2 microm) removal using portable high efficiency particle arresting (HEPA) <span class="hlt">air</span> cleaners in residential buildings following an outdoor release of particles. The number of stand-alone <span class="hlt">air</span> cleaners, <span class="hlt">air</span> <span class="hlt">exchange</span> rate, volumetric flow rate through the heating, ventilating and <span class="hlt">air</span>-conditioning (HVAC) system, and size-resolved particle removal efficiency in the HVAC filter were varied. The effectiveness of <span class="hlt">air</span> cleaners for SIP was evaluated in terms of the outdoor and the indoor particle concentration with <span class="hlt">air</span> cleaner(s) relative to the indoor concentration without <span class="hlt">air</span> cleaners. Through transient and steady-state analysis of the <span class="hlt">model</span> it was determined that one to three portable HEPA <span class="hlt">air</span> cleaners can be effective for SIP following outdoor bioaerosol releases, with maximum reductions in particle concentrations as high as 90% relative to conditions in which an <span class="hlt">air</span> cleaner is not employed. The relative effectiveness of HEPA <span class="hlt">air</span> cleaners vs. other removal mechanisms was predicted to decrease with increasing particle size, because of increasing competition by particle deposition with indoor <span class="hlt">surfaces</span> and removal to HVAC filters. However, the effect of particle size was relatively small for most scenarios considered here. The results of a screening analysis suggest that stand-alone (portable) <span class="hlt">air</span> cleaners that contain high efficiency particle arresting (HEPA) filters can be effective for reducing indoor fine particle concentrations in residential dwellings during outdoor releases of biological warfare agents. The relative effectiveness of stand-alone <span class="hlt">air</span> cleaners for reducing occupants' exposure to particles of outdoor origin depends on several factors, including the type of heating, ventilating and <span class="hlt">air</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_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/2017AGUFM.H33B1669L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H33B1669L"><span>Turbulent water vapor <span class="hlt">exchanges</span> and two source energy balance <span class="hlt">model</span> estimated fluxes of heterogeneous vineyard canopies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Los, S.; Hipps, L.; Alfieri, J. G.; Prueger, J. H.; Kustas, W. P.</p> <p>2017-12-01</p> <p>Agriculture in semi-arid regions is globally facing increasing stress on water resources. Hence, knowledge of water used in irrigated crops is essential for water resource management. However, quantifying spatial and temporal distribution of evapotranspiration (ET) has proven difficult because of the inherent complexities involved. Understanding of the complex biophysical relationships that govern ET is incomplete, particularly for heterogeneous vegetation. The USDA-ARS is developing a remotely-sensed ET <span class="hlt">modeling</span> system that utilizes a two-source energy balance (TSEB) <span class="hlt">model</span> capable of simulating turbulent water and energy <span class="hlt">exchange</span> from measurements of radiometric land <span class="hlt">surface</span> temperature. The <span class="hlt">modeling</span> system has been tested over a number of vegetated <span class="hlt">surfaces</span> and is currently being validated for vineyard sites in the Central Valley of California through the Grape Remote sensing Atmospheric Profiling & Evapotranspiration eXperiment (GRAPEX). The highly variable, elevated canopy structure and semi-arid climatic conditions of these sites give the opportunity to gain knowledge of both turbulent <span class="hlt">exchange</span> processes and the TSEB <span class="hlt">model</span>'s ability to simulate turbulent fluxes for heterogeneous vegetation. Analyzed are fast-response (20 Hz) 3-D velocity, temperature, and humidity measurements gathered over 4 years at two vineyard sites. These data were collected at a height of 5 m, within the <span class="hlt">surface</span> layer but above the canopy, and at 1.5 m, below the canopy top. Power spectra and cross-spectra are used to study behavior of turbulent water vapor <span class="hlt">exchanges</span> and coupling between the canopy layer and <span class="hlt">surface</span> layer under various atmospheric conditions. Frequent light winds and unstable daytime conditions, combined with the complicated canopy structure, often induce intermittent and episodic turbulence transport. This resulted in a modal behavior alternating between periods of more continuous canopy venting and periods where water vapor fluxes are dominated by transient, low</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.epa.gov/airmarkets/clean-air-markets-monitoring-surface-water-chemistry','PESTICIDES'); return false;" href="https://www.epa.gov/airmarkets/clean-air-markets-monitoring-surface-water-chemistry"><span>Clean <span class="hlt">Air</span> Markets - Monitoring <span class="hlt">Surface</span> Water Chemistry</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>Learn about how EPA uses Long Term Monitoring (LTM) and Temporily Integrated Monitoring of Ecosystems (TIME) to track the effect of the Clean <span class="hlt">Air</span> Act Amendments on acidity of <span class="hlt">surface</span> waters in the eastern U.S.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H33F1758A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H33F1758A"><span>Data Assimilation of <span class="hlt">Air</span>SWOT and Synthetically Derived SWOT Observations of Water <span class="hlt">Surface</span> Elevation in a Multichannel River</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Altenau, E. H.; Pavelsky, T.; Andreadis, K.; Bates, P. D.; Neal, J. C.</p> <p>2017-12-01</p> <p>Multichannel rivers continue to be challenging features to quantify, especially at regional and global scales, which is problematic because accurate representations of such environments are needed to properly monitor the earth's water cycle as it adjusts to climate change. It has been demonstrated that higher-complexity, 2D <span class="hlt">models</span> outperform lower-complexity, 1D <span class="hlt">models</span> in simulating multichannel river hydraulics at regional scales due to the inclusion of the channel network's connectivity. However, new remote sensing measurements from the future <span class="hlt">Surface</span> Water and Ocean Topography (SWOT) mission and it's airborne analog <span class="hlt">Air</span>SWOT offer new observations that can be used to try and improve the lower-complexity, 1D <span class="hlt">models</span> to achieve accuracies closer to the higher-complexity, 2D codes. Here, we use an Ensemble Kalman Filter (EnKF) to assimilate <span class="hlt">Air</span>SWOT water <span class="hlt">surface</span> elevation (WSE) measurements from a 2015 field campaign into a 1D hydrodynamic <span class="hlt">model</span> along a 90 km reach of Tanana River, AK. This work is the first to test data assimilation methods using real SWOT-like data from <span class="hlt">Air</span>SWOT. Additionally, synthetic SWOT observations of WSE are generated across the same study site using a fine-resolution 2D <span class="hlt">model</span> and assimilated into the coarser-resolution 1D <span class="hlt">model</span>. Lastly, we compare the abilities of <span class="hlt">Air</span>SWOT and the synthetic-SWOT observations to improve spatial and temporal <span class="hlt">model</span> outputs in WSEs. Results indicate 1D <span class="hlt">model</span> outputs of spatially distributed WSEs improve as observational coverage increases, and improvements in temporal fluctuations in WSEs depend on the number of observations. Furthermore, results reveal that assimilation of <span class="hlt">Air</span>SWOT observations produce greater error reductions in 1D <span class="hlt">model</span> outputs compared to synthetic SWOT observations due to lower measurement errors. Both <span class="hlt">Air</span>SWOT and the synthetic SWOT observations significantly lower spatial and temporal errors in 1D <span class="hlt">model</span> outputs of WSEs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22599927-generation-large-area-glow-like-surface-discharge-atmospheric-pressure-air','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22599927-generation-large-area-glow-like-surface-discharge-atmospheric-pressure-air"><span>Generation of large-area and glow-like <span class="hlt">surface</span> discharge in atmospheric pressure <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>Song, Ying; Bi, Zhenhua; Wang, Xueyang</p> <p>2016-08-15</p> <p>A large-area (6 cm × 6 cm) <span class="hlt">air</span> <span class="hlt">surface</span> dielectric barrier discharge has been generated at atmospheric pressure by using well-aligned and micron-sized dielectric tubes with tungsten wire electrodes. Intensified CCD images with an exposure time of 5 ns show that the uniform <span class="hlt">surface</span> <span class="hlt">air</span> discharge can be generated during the rising and falling time of pulsed DC voltage. Current and voltage and optical measurements confirm the formation of glow-like <span class="hlt">air</span> discharges on the <span class="hlt">surface</span> of micron-sized dielectric tubes. Simulation results indicate that the microelectrode configuration contributes to the formation of strong <span class="hlt">surface</span> electric field and plays an important role in the generation of uniformmore » <span class="hlt">surface</span> <span class="hlt">air</span> discharge.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4580M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4580M"><span>Simulation of infiltration and redistribution of intense rainfall using Land <span class="hlt">Surface</span> <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mueller, Anna; Verhoef, Anne; Cloke, Hannah</p> <p>2016-04-01</p> <p>Flooding from intense rainfall (FFIR) can cause widespread damage and disruption. Numerical Weather Prediction (NWP) <span class="hlt">models</span> provide distributed information about atmospheric conditions, such as precipitation, that can lead to a flooding event. Short duration, high intensity rainfall events are generally poorly predicted by NWP <span class="hlt">models</span>, because of the high spatiotemporal resolution required and because of the way the convective rainfall is described in the <span class="hlt">model</span>. The resolution of NWP <span class="hlt">models</span> is ever increasing. Better understanding of complex hydrological processes and the effect of scale is important in order to improve the prediction of magnitude and duration of such events, in the context of disaster management. Working as part of the NERC SINATRA project, we evaluated how the Land <span class="hlt">Surface</span> <span class="hlt">Model</span> (LSM) components of NWP <span class="hlt">models</span> cope with high intensity rainfall input and subsequent infiltration problems. Both in terms of the amount of water infiltrated in the soil store, as well as the timing and the amount of <span class="hlt">surface</span> and subsurface runoff generated. The <span class="hlt">models</span> investigated are SWAP (Soil Water <span class="hlt">Air</span> Plant, Alterra, the Netherlands, van Dam 1997), JULES (Joint UK Land Environment Simulator a component of Unified <span class="hlt">Model</span> in UK Met Office, Best et al. 2011) and CHTESSEL (Carbon and Hydrology- Tiled ECMWF Scheme for <span class="hlt">Surface</span> <span class="hlt">Exchanges</span> over Land, Balsamo et al. 2009) We analysed the numerical aspects arising from discontinuities (or sharp gradients) in forcing and/or the <span class="hlt">model</span> solution. These types of infiltration configurations were tested in the laboratory (Vachaud 1971), for some there are semi-analytical solutions (Philip 1957, Parlange 1972, Vanderborght 2005) or reference numerical solutions (Haverkamp 1977, van Dam 2000, Vanderborght 2005). The maximum infiltration by the <span class="hlt">surface</span>, Imax, is in general dependent on atmospheric conditions, <span class="hlt">surface</span> type, soil type, soil moisture content θ, and <span class="hlt">surface</span> orographic factor σ. The <span class="hlt">models</span> used differ in their approach to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15683168','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15683168"><span><span class="hlt">Air</span>-water gas <span class="hlt">exchange</span> of chlorinated pesticides in four lakes spanning a 1,205 meter elevation range in the Canadian Rocky Mountains.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wilkinson, Andrew C; Kimpe, Lynda E; Blais, Jules M</p> <p>2005-01-01</p> <p>Concentrations of selected persistent organic pollutants (POPs) in <span class="hlt">air</span> and water were measured from four lakes that transect the Canadian Rocky Mountains. These data were used in combination with wind velocity and temperature-adjusted Henry's law constants to estimate the direction and magnitude of chemical <span class="hlt">exchange</span> across the <span class="hlt">air</span>-water interface of these lakes. Bow Lake (1,975 m above sea level [masl]) was studied during the summers of 1998 through 2000; Donald (770 masl) was studied during the summer of 1999; Dixon Dam Lake (946 masl) and Kananaskis Lake (1,667 masl) were studied during the summer of 2000. Hexachlorobenzene (HCB) and dieldrin volatilized from Bow Lake in spring and summer of 1998 to 2000 at a rate of 0.92 +/-1.1 and 0.55+/-0.37 ng m(-2) d(-1), respectively. The alpha-endosulfan deposited to Bow Lake at a rate of 3.4+/-2.2 ng m(-2) d(-1). Direction of gas <span class="hlt">exchange</span> for gamma-hexachlorocyclohexane (gamma-HCH) changed from net deposition in 1998 to net volatilization in 1999, partly because of a surge in y-HCH concentrations in the water at Bow Lake in 1999. Average gamma-HCH concentrations in <span class="hlt">air</span> declined steadily over the three-year period, from 0.021 ng m(-3) in 1998, to 0.0023 ng m(-3) in 2000, and to volatilization in 1999 and 2000. Neither the concentrations of organochlorine compounds (OCs) in <span class="hlt">air</span> and water, nor the direction and rate of <span class="hlt">air</span>-water gas <span class="hlt">exchange</span> correlate with temperature or elevation. In general, losses of pesticides by outflow were greater than the amount <span class="hlt">exchanged</span> across the <span class="hlt">air</span>-water interface in these lakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000AtmEn..34.4667D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AtmEn..34.4667D"><span>Uncertainty, ensembles and <span class="hlt">air</span> quality dispersion <span class="hlt">modeling</span>: applications and challenges</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dabberdt, Walter F.; Miller, Erik</p> <p></p> <p>The past two decades have seen significant advances in mesoscale meteorological <span class="hlt">modeling</span> research and applications, such as the development of sophisticated and now widely used advanced mesoscale prognostic <span class="hlt">models</span>, large eddy simulation <span class="hlt">models</span>, four-dimensional data assimilation, adjoint <span class="hlt">models</span>, adaptive and targeted observational strategies, and ensemble and probabilistic forecasts. Some of these advances are now being applied to urban <span class="hlt">air</span> quality <span class="hlt">modeling</span> and applications. Looking forward, it is anticipated that the high-priority <span class="hlt">air</span> quality issues for the near-to-intermediate future will likely include: (1) routine operational forecasting of adverse <span class="hlt">air</span> quality episodes; (2) real-time high-level support to emergency response activities; and (3) quantification of <span class="hlt">model</span> uncertainty. Special attention is focused here on the quantification of <span class="hlt">model</span> uncertainty through the use of ensemble simulations. Application to emergency-response dispersion <span class="hlt">modeling</span> is illustrated using an actual event that involved the accidental release of the toxic chemical oleum. Both <span class="hlt">surface</span> footprints of mass concentration and the associated probability distributions at individual receptors are seen to provide valuable quantitative indicators of the range of expected concentrations and their associated uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRD..11912338L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRD..11912338L"><span>Effects of trans-Eurasian transport of <span class="hlt">air</span> pollutants on <span class="hlt">surface</span> ozone concentrations over Western China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xiaoyuan; Liu, Junfeng; Mauzerall, Denise L.; Emmons, Louisa K.; Walters, Stacy; Horowitz, Larry W.; Tao, Shu</p> <p>2014-11-01</p> <p>Due to a lack of industrialization in Western China, <span class="hlt">surface</span> <span class="hlt">air</span> there was, until recently, believed to be relatively unpolluted. However, recent measurements and <span class="hlt">modeling</span> studies have found high levels of ozone (O3) there. Based on the state-of-the-science global chemical transport <span class="hlt">model</span> MOZART-4, we identify the origin, pathway, and mechanism of trans-Eurasian transport of <span class="hlt">air</span> pollutants to Western China in 2000. MOZART-4 generally simulates well the observed <span class="hlt">surface</span> O3 over inland areas of China. Simulations find <span class="hlt">surface</span> ozone concentrations over Western China on average to be about 10 ppbv higher than Eastern China. Using sensitivity studies, we find that anthropogenic emissions from all Eurasian regions except China contribute 10-15 ppbv <span class="hlt">surface</span> O3 over Western China, superimposed upon a 35-40 ppbv natural background. Transport from European anthropogenic sources to Northwestern China results in 2-6 ppbv O3 enhancements in spring and summer. Indian anthropogenic sources strongly influence O3 over the Tibetan Plateau during the summer monsoon. Transport of O3 originating from emissions in the Middle East occasionally reach Western China and increase <span class="hlt">surface</span> ozone there by about 1-4 ppbv. These influences are of similar magnitude as trans-Pacific and transatlantic transport of O3 and its precursors, indicating the significance of trans-Eurasian ozone transport in hemispheric transport of <span class="hlt">air</span> pollution. Our study further indicates that mitigation of anthropogenic emissions from Europe, the Indian subcontinent, and the Middle East could benefit public health and agricultural productivity in Western China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810068620','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810068620"><span>Investigation of Effectiveness of <span class="hlt">Air</span>-Heating a Hollow Steel Propeller for Protection Against Icing. 2: 50% Impartitioned Blades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Perkins, Porter J.; Mulholland, Donald R.</p> <p>1948-01-01</p> <p>The icing protection afforded an internal <span class="hlt">air</span>-heated propeller blade by radial partitioning at 50-percent chord to confine the heated <span class="hlt">air</span> to the forward half of the blade was determined in the NACA Cleveland icing research tunnel. A modified production-<span class="hlt">model</span> hollow steel propeller, was used for the investigation. Temperatures of the blade <span class="hlt">surfaces</span> for several heating rates were measured under various tunnel Icing' conditions. Photographic observations of ice formations on blade <span class="hlt">surfaces</span> and blade heat-<span class="hlt">exchanger</span> effectiveness were obtained. With 50-percent partitioning of the blades, adequate icing protection at 1050 rpm was obtained with a heating rate of 26,000 Btu per hour per blade at the blade shank using an <span class="hlt">air</span> temperature of 400 F with a flow rate of 280 pounds per hour per blade, which is one-third less heat than was found necessary for similar Ice protection with unpartitioned blades. The chordwise distribution of the applied heat, as determined by <span class="hlt">surface</span> temperature measurements, was considered unsatisfactory with much of the heat dissipated well back of the leading edge. Heat-<span class="hlt">exchanger</span> effectiveness of approximately 56 percent also Indicated poor utilization of available heat. This effectiveness was, however, 9 percent greater than that obtained from unpartitioned blades.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/911006','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/911006"><span>INEEL <span class="hlt">AIR</span> <span class="hlt">MODELING</span> PROTOCOL ext</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>C. S. Staley; M. L. Abbott; P. D. Ritter</p> <p>2004-12-01</p> <p>Various laws stemming from the Clean <span class="hlt">Air</span> Act of 1970 and the Clean <span class="hlt">Air</span> Act amendments of 1990 require <span class="hlt">air</span> emissions <span class="hlt">modeling</span>. <span class="hlt">Modeling</span> is used to ensure that <span class="hlt">air</span> emissions from new projects and from modifications to existing facilities do not exceed certain standards. For radionuclides, any new airborne release must be <span class="hlt">modeled</span> to show that downwind receptors do not receive exposures exceeding the dose limits and to determine the requirements for emissions monitoring. For criteria and toxic pollutants, emissions usually must first exceed threshold values before <span class="hlt">modeling</span> of downwind concentrations is required. This document was prepared to provide guidancemore » for performing environmental compliance-driven <span class="hlt">air</span> <span class="hlt">modeling</span> of emissions from Idaho National Engineering and Environmental Laboratory facilities. This document assumes that the user has experience in <span class="hlt">air</span> <span class="hlt">modeling</span> and dose and risk assessment. It is not intended to be a "cookbook," nor should all recommendations herein be construed as requirements. However, there are certain procedures that are required by law, and these are pointed out. It is also important to understand that <span class="hlt">air</span> emissions <span class="hlt">modeling</span> is a constantly evolving process. This document should, therefore, be reviewed periodically and revised as needed. The document is divided into two parts. Part A is the protocol for radiological assessments, and Part B is for nonradiological assessments. This document is an update of and supersedes document INEEL/INT-98-00236, Rev. 0, INEEL <span class="hlt">Air</span> <span class="hlt">Modeling</span> Protocol. This updated document incorporates changes in some of the rules, procedures, and <span class="hlt">air</span> <span class="hlt">modeling</span> codes that have occurred since the protocol was first published in 1998.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhRvE..89f2804P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvE..89f2804P"><span>Axelrod's <span class="hlt">model</span> with <span class="hlt">surface</span> tension</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pace, Bruno; Prado, Carmen P. C.</p> <p>2014-06-01</p> <p>In this work we propose a subtle change in Axelrod's <span class="hlt">model</span> for the dissemination of culture. The mechanism consists of excluding from the set of potentially interacting neighbors those that would never possibly <span class="hlt">exchange</span>. Although the alteration proposed does not alter the state space topologically, it yields significant qualitative changes, specifically the emergence of <span class="hlt">surface</span> tension, driving the system in some cases to metastable states. The transient behavior is considerably richer, and cultural regions become stable leading to the formation of different spatiotemporal patterns. A metastable "glassy" phase emerges between the globalized phase and the disordered, multicultural phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC21C0953M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC21C0953M"><span>CMIP5 land <span class="hlt">surface</span> <span class="hlt">models</span> systematically underestimate inter-annual variability of net ecosystem <span class="hlt">exchange</span> in semi-arid southwestern North America.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>MacBean, N.; Scott, R. L.; Biederman, J. A.; Vuichard, N.; Hudson, A.; Barnes, M.; Fox, A. M.; Smith, W. K.; Peylin, P. P.; Maignan, F.; Moore, D. J.</p> <p>2017-12-01</p> <p>Recent studies based on analysis of atmospheric CO2 inversions, satellite data and terrestrial biosphere <span class="hlt">model</span> simulations have suggested that semi-arid ecosystems play a dominant role in the interannual variability and long-term trend in the global carbon sink. These studies have largely cited the response of vegetation activity to changing moisture availability as the primary mechanism of variability. However, some land <span class="hlt">surface</span> <span class="hlt">models</span> (LSMs) used in these studies have performed poorly in comparison to satellite-based observations of vegetation dynamics in semi-arid regions. Further analysis is therefore needed to ensure semi-arid carbon cycle processes are well represented in global scale LSMs before we can fully establish their contribution to the global carbon cycle. In this study, we evaluated annual net ecosystem <span class="hlt">exchange</span> (NEE) simulated by CMIP5 land <span class="hlt">surface</span> <span class="hlt">models</span> using observations from 20 Ameriflux sites across semi-arid southwestern North America. We found that CMIP5 <span class="hlt">models</span> systematically underestimate the magnitude and sign of NEE inter-annual variability; therefore, the true role of semi-arid regions in the global carbon cycle may be even more important than previously thought. To diagnose the factors responsible for this bias, we used the ORCHIDEE LSM to test different climate forcing data, prescribed vegetation fractions and <span class="hlt">model</span> structures. Climate and prescribed vegetation do contribute to uncertainty in annual NEE simulations, but the bias is primarily caused by incorrect timing and magnitude of peak gross carbon fluxes. Modifications to the hydrology scheme improved simulations of soil moisture in comparison to data. This in turn improved the seasonal cycle of carbon uptake due to a more realistic limitation on photosynthesis during water stress. However, the peak fluxes are still too low, and phenology is poorly represented for desert shrubs and grasses. We provide suggestions on <span class="hlt">model</span> developments needed to tackle these issues in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000117692','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000117692"><span>BOREAS AFM-08 ECMWF Hourly <span class="hlt">Surface</span> and Upper <span class="hlt">Air</span> Data for the SSA and NSA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Viterbo, Pedro; Betts, Alan; Hall, Forrest G. (Editor); Newcomer, Jeffrey A.; Smith, David E. (Technical Monitor)</p> <p>2000-01-01</p> <p>The Boreal Ecosystem-Atmosphere Study (BOREAS) Airborne Fluxes and Meteorology (AFM)-8 team focused on <span class="hlt">modeling</span> efforts to improve the understanding of the diurnal evolution of the convective boundary layer over the boreal forest. This data set contains hourly data from the European Center for for Medium-Range Weather Forecasts (ECMWF) operational <span class="hlt">model</span> from below the <span class="hlt">surface</span> to the top of the atmosphere, including the <span class="hlt">model</span> fluxes at the <span class="hlt">surface</span>. Spatially, the data cover a pair of the points that enclose the rawinsonde sites at Candle Lake, Saskatchewan, in the Southern Study Area (SSA) and Thompson, Manitoba, in the Northern Study Area (NSA). Temporally, the data include the two time periods of 13 May 1994 to 30 Sept 1994 and 01 Mar 1996 to 31 Mar 1997. The data are stored in tabular ASCII files. The number of records in the upper <span class="hlt">air</span> data files may exceed 20,000, causing a problem for some software packages. The ECMWF hourly <span class="hlt">surface</span> and upper <span class="hlt">air</span> data are available from the Earth Observing System Data and Information System (EOSDIS) Oak Ridge National Laboratory (ORNL) Distributed Active Archive Center (DAAC). The data files are available on a CD-ROM (see document number 20010000884).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHyd..555...15W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHyd..555...15W"><span>Integrated hydrologic and hydrodynamic <span class="hlt">modeling</span> to assess water <span class="hlt">exchange</span> in a data-scarce reservoir</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Binbin; Wang, Guoqiang; Wang, Zhonggen; Liu, Changming; Ma, Jianming</p> <p>2017-12-01</p> <p>Integrated hydrologic and hydrodynamic <span class="hlt">modeling</span> is useful in evaluating hydrodynamic characteristics (e.g. water <span class="hlt">exchange</span> processes) in data-scarce water bodies, however, most studies lack verification of the hydrologic <span class="hlt">model</span>. Here, water <span class="hlt">exchange</span> (represented by water age) was investigated through integrated hydrologic and hydrodynamic <span class="hlt">modeling</span> of the Hongfeng Reservoir, a poorly gauged reservoir in southwest China. The performance of the hydrologic <span class="hlt">model</span> and parameter replacement among sub-basins with hydrological similarity was verified by historical data. Results showed that hydrological similarity based on the hierarchical cluster analysis and topographic index probability density distribution was reliable with satisfactory performance of parameter replacement. The hydrodynamic <span class="hlt">model</span> was verified using daily water levels and water temperatures from 2009 and 2010. The water <span class="hlt">exchange</span> processes in the Hongfeng Reservoir are very complex with temporal, vertical, and spatial variations. The temporal water age was primarily controlled by the variable inflow and outflow, and the maximum and minimum ages for the site near the dam were 406.10 d (15th June) and 90.74 d (3rd August), respectively, in 2010. Distinct vertical differences in water age showed that <span class="hlt">surface</span> flow, interflow, and underflow appeared alternately, depending on the season and water depth. The worst water <span class="hlt">exchange</span> situation was found in the central areas of the North Lake with the highest water ages in the bottom on both 15th June and 3rd August, in 2010. Comparison of the spatial water ages revealed that the more favorable hydraulic conditions on 3rd August mainly improved the water <span class="hlt">exchange</span> in the dam areas and most areas of the South Lake, but had little effect on the bottom layers of the other deepest areas in the South and North Lakes. The presented framework can be applied in other data-scarce waterbodies worldwide to provide better understanding of water <span class="hlt">exchange</span> processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/515513','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/515513"><span>Speciation of uranium in <span class="hlt">surface</span>-modified, hydrothermally treated, (UO{sub 2}){sup 2+}-<span class="hlt">exchanged</span> smectite clays</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>Giaquinta, D.M.; Soderholm, L.; Yuchs, S.E.</p> <p>1997-08-01</p> <p>A successful solution to the problem of disposal and permanent storage of water soluble radioactive species must address two issues: exclusion of the radionuclides from the environment and the prevention of leaching from the storage media into the environment. Immobilization of radionuclides in clay minerals has been studied. In addition to the use of clays as potential waste forms, information about the interactions of radionuclides with clays and how such interactions affect their speciations is crucial for successful <span class="hlt">modeling</span> of actinide-migration. X-ray absorption spectroscopy (XAS) is used to determine the uranium speciation in <span class="hlt">exchanged</span> and <span class="hlt">surface</span>-modified clays. The XAS datamore » from uranyl-loaded bentonite clay are compared with those obtained after the particle <span class="hlt">surfaces</span> have been coated with alkylsilanes. These silane films, which render the <span class="hlt">surface</span> of the clay hydrophobic, are added in order to minimize the ability of external water to <span class="hlt">exchange</span> with the water in the clay interlayer, thereby decreasing the release rate of the <span class="hlt">exchanged</span>-uranium species. Mild hydrothermal conditions are used in an effort to mimic potential geologic conditions that may occur during long-term radioactive waste storage. The XAS spectra indicate that the uranyl monomer species remain unchanged in most samples, except in those samples that were both coated with an alkylsilane and hydrothermally treated. When the clay was coated with an organic film, formed by the acidic deposition of octadecyltrimethoxysilane, hydrothermal treatment results in the formation of aggregated uranium species in which the uranium is reduced from U{sup VI} to U{sup IV}.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.epa.gov/csapr/air-quality-modeling','PESTICIDES'); return false;" href="https://www.epa.gov/csapr/air-quality-modeling"><span><span class="hlt">Air</span> Quality <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>In this technical support document (TSD) EPA describes the <span class="hlt">air</span> quality <span class="hlt">modeling</span> performed to support the Environmental Protection Agency’s Transport Rule proposal (now known as the Cross-State <span class="hlt">Air</span> Pollution Rule).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SurSc.667...79Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SurSc.667...79Z"><span>Spin-wave resonance frequency in ferromagnetic thin film with interlayer <span class="hlt">exchange</span> coupling and <span class="hlt">surface</span> anisotropy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Shuhui; Rong, Jianhong; Wang, Huan; Wang, Dong; Zhang, Lei</p> <p>2018-01-01</p> <p>We have investigated the dependence of spin-wave resonance(SWR) frequency on the <span class="hlt">surface</span> anisotropy, the interlayer <span class="hlt">exchange</span> coupling, the ferromagnetic layer thickness, the mode number and the external magnetic field in a ferromagnetic superlattice film by means of the linear spin-wave approximation and Green's function technique. The SWR frequency of the ferromagnetic thin film is shifted to higher values corresponding to those of above factors, respectively. It is found that the linear behavior of SWR frequency curves of all modes in the system is observed as the external magnetic field is increasing, however, SWR frequency curves are nonlinear with the lower and the higher modes for different <span class="hlt">surface</span> anisotropy and interlayer <span class="hlt">exchange</span> coupling in the system. In addition, the SWR frequency of the lowest (highest) mode is shifted to higher (lower) values when the film thickness is thinner. The interlayer <span class="hlt">exchange</span> coupling is more important for the energetically higher modes than for the energetically lower modes. The <span class="hlt">surface</span> anisotropy has a little effect on the SWR frequency of the highest mode, when the <span class="hlt">surface</span> anisotropy field is further increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16774763','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16774763"><span>Dynamics of water droplets detached from porous <span class="hlt">surfaces</span> of relevance to PEM fuel cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Theodorakakos, A; Ous, T; Gavaises, M; Nouri, J M; Nikolopoulos, N; Yanagihara, H</p> <p>2006-08-15</p> <p>The detachment of liquid droplets from porous material <span class="hlt">surfaces</span> used with proton <span class="hlt">exchange</span> membrane (PEM) fuel cells under the influence of a cross-flowing <span class="hlt">air</span> is investigated computationally and experimentally. CCD images taken on a purpose-built transparent fuel cell have revealed that the water produced within the PEM is forming droplets on the <span class="hlt">surface</span> of the gas-diffusion layer. These droplets are swept away if the velocity of the flowing <span class="hlt">air</span> is above a critical value for a given droplet size. Static and dynamic contact angle measurements for three different carbon gas-diffusion layer materials obtained inside a transparent <span class="hlt">air</span>-channel test <span class="hlt">model</span> have been used as input to the numerical <span class="hlt">model</span>; the latter is based on a Navier-Stokes equations flow solver incorporating the volume of fluid (VOF) two-phase flow methodology. Variable contact angle values around the gas-liquid-solid contact-line as well as their dynamic change during the droplet shape deformation process, have allowed estimation of the adhesion force between the liquid droplet and the solid <span class="hlt">surface</span> and successful prediction of the separation line at which droplets loose their contact from the solid <span class="hlt">surface</span> under the influence of the <span class="hlt">air</span> stream flowing around them. Parametric studies highlight the relevant importance of various factors affecting the detachment of the liquid droplets from the solid <span class="hlt">surface</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.H13J..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.H13J..06G"><span>Measuring and <span class="hlt">modeling</span> changes in land-atmosphere <span class="hlt">exchanges</span> and hydrologic response in forests undergoing insect-driven mortality</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gochis, D. J.; Brooks, P. D.; Harpold, A. A.; Ewers, B. E.; Pendall, E.; Barnard, H. R.; Reed, D.; Harley, P. C.; Hu, J.; Biederman, J.</p> <p>2010-12-01</p> <p>Given the magnitude and spatial extent of recent forest mortality in the western U.S. there is a pressing need to improve representation of such influences on the <span class="hlt">exchange</span> of energy, water, biogeochemical and momentum fluxes in land-atmosphere parameterizations coupled to weather and climate <span class="hlt">models</span>. In this talk we present observational data and <span class="hlt">model</span> results from a new study aimed at improving understanding the impacts of mountain pine beetle-induced forest mortality in the central Rocky Mountains. Baseline observations and <span class="hlt">model</span> runs from undisturbed lodgepole pine forest conditions are developed as references against which new observations and <span class="hlt">model</span> runs from infested stands are compared. We will specifically look at the structure and evolution of sub-canopy energy <span class="hlt">exchange</span> variables such as shortwave and longwave radiation and sub-canopy turbulence as well as sub-canopy precipitation, sapflow fluxes, canopy-scale fluxes and soil moisture and temperature. In this manner we seek to lay the ground work for evaluating the recent generation of land <span class="hlt">surface</span> <span class="hlt">model</span> changes aimed at representing insect-related forest dynamics in the CLM-C/N and Noah land <span class="hlt">surface</span> <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=307557&keyword=Pollution+AND+Soil&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=307557&keyword=Pollution+AND+Soil&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><span class="hlt">Model</span>-measurement comparison of ammonia bi-directional <span class="hlt">air-surface</span> <span class="hlt">exchange</span> fluxes over agricultural fields</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><span class="hlt">Modeling</span> of the bi-directional fluxes (BDFs) of ammonia (NH3) over fertilized soybean and corn canopies was evaluated for three intensive sampling periods: the first, during the summer of 2002 in Warsaw, North Carolina (NC), USA; and the second and third during the summer of 2007...</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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