Sample records for aerosol scale height

  1. Retrieving Smoke Aerosol Height from DSCOVR/EPIC

    NASA Astrophysics Data System (ADS)

    Xu, X.; Wang, J.; Wang, Y.

    2017-12-01

    Unlike industrial pollutant particles that are often confined within the planetary boundary layer, smoke from forest and agriculture fires can inject massive carbonaceous aerosols into the upper troposphere due to the intense pyro-convection. Sensitivity of weather and climate to absorbing carbonaceous aerosols is regulated by the altitude of those aerosol layers. However, aerosol height information remains limited from passive satellite sensors. Here we present an algorithm to estimate smoke aerosol height from radiances in the oxygen A and B bands measured by the Earth Polychromatic Imaging Camera (EPIC) from the Deep Space Climate Observatory (DSCOVR). With a suit of case studies and validation efforts, we demonstrate that smoke aerosol height can be well retrieved over both ocean and land surfaces multiple times daily.

  2. Aerosol layer height from synergistic use of VIIRS and OMPS

    NASA Astrophysics Data System (ADS)

    Lee, J.; Hsu, N. Y. C.; Sayer, A. M.; Kim, W.; Seftor, C. J.

    2017-12-01

    This study presents an Aerosol Single-scattering albedo and Height Estimation (ASHE) algorithm, which retrieves the height of UV-absorbing aerosols by synergistically using the Visible Infrared Imaging Radiometer Suite (VIIRS) and the Ozone Mapping and Profiler Suite (OMPS). ASHE provides height information over a much broader area than ground-based or spaceborne lidar measurements by benefitting from the wide swaths of the two instruments used. As determination of single-scattering albedo (SSA) of the aerosol layer is the most critical part for the performance and coverage of ASHE, here we demonstrate three different strategies to constrain the SSA. First, ASHE is able to retrieve the SSA of UV-absorbing aerosols when Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) provides vertical profiles of the aerosol layer of interest. Second, Aerosol Robotic Network (AERONET) inversions can directly constrain the SSA of the aerosol layer when collocated with VIIRS or OMPS. Last, a SSA climatology from ASHE, AERONET, or other data sources can be used for large-scale, aged aerosol events, for which climatological SSA is well-known, at the cost of a slight decrease in retrieval accuracy. The same algorithm can be applied to measurements of similar type, such as those made by the Moderate Resolution Imaging Spectroradiometer (MODIS) and Ozone Monitoring Instrument (OMI), for a long-term, consistent data record.

  3. Height Dependency of Aerosol-Cloud Interaction Regimes: Height Dependency of ACI Regime

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

    Chen, Jingyi; Liu, Yangang; Zhang, Minghua

    This study investigates the height dependency of aerosol-cloud interaction regimes in terms of the joint dependence of the key cloud microphysical properties (e.g. cloud droplet number concentration, cloud droplet relative dispersion, etc.) on aerosol number concentration (N a) and vertical velocity (w). The three distinct regimes with different microphysical features are the aerosol-limited regime, the updraft-limited regime, and the transitional regime. The results reveal two new phenomena in updraft-limited regime: 1) The “condensational broadening” of cloud droplet size distribution in contrast to the well-known “condensational narrowing” in the aerosol-limited regime; 2) Above the level of maximum supersaturation, some cloud dropletsmore » are deactivated into interstitial aerosols in the updraft-limited regime whereas all droplets remain activated in the aerosol-limited regime. Further analysis shows that the particle equilibrium supersaturation plays important role in understanding these unique features. Also examined is the height of warm rain initiation and its dependence on N a and w. The rain initiation height is found to depend primarily on either N a or w or both in different N a-w regimes, thus suggesting a strong regime dependence of the second aerosol indirect effect.« less

  4. Height Dependency of Aerosol-Cloud Interaction Regimes: Height Dependency of ACI Regime

    DOE PAGES

    Chen, Jingyi; Liu, Yangang; Zhang, Minghua; ...

    2018-01-10

    This study investigates the height dependency of aerosol-cloud interaction regimes in terms of the joint dependence of the key cloud microphysical properties (e.g. cloud droplet number concentration, cloud droplet relative dispersion, etc.) on aerosol number concentration (N a) and vertical velocity (w). The three distinct regimes with different microphysical features are the aerosol-limited regime, the updraft-limited regime, and the transitional regime. The results reveal two new phenomena in updraft-limited regime: 1) The “condensational broadening” of cloud droplet size distribution in contrast to the well-known “condensational narrowing” in the aerosol-limited regime; 2) Above the level of maximum supersaturation, some cloud dropletsmore » are deactivated into interstitial aerosols in the updraft-limited regime whereas all droplets remain activated in the aerosol-limited regime. Further analysis shows that the particle equilibrium supersaturation plays important role in understanding these unique features. Also examined is the height of warm rain initiation and its dependence on N a and w. The rain initiation height is found to depend primarily on either N a or w or both in different N a-w regimes, thus suggesting a strong regime dependence of the second aerosol indirect effect.« less

  5. Retrieving the Height of Smoke and Dust Aerosols by Synergistic Use of Multiple Satellite Sensors

    NASA Technical Reports Server (NTRS)

    Lee, Jaehwa; Hsu, N. Christina; Bettenhausen, Corey; Sayer, Andrew M.; Seftor, Colin J.; Jeong, Myeong-Jae

    2016-01-01

    The Aerosol Single scattering albedo and Height Estimation (ASHE) algorithm was first introduced in Jeong and Hsu (2008) to provide aerosol layer height and single scattering albedo (SSA) for biomass burning smoke aerosols. By using multiple satellite sensors synergistically, ASHE can provide the height information over much broader areas than lidar observations alone. The complete ASHE algorithm uses aerosol data from MODIS or VIIRS, OMI or OMPS, and CALIOP. A simplified algorithm also exists that does not require CALIOP data as long as the SSA of the aerosol layer is provided by another source. Several updates have recently been made: inclusion of dust layers in the retrieval process, better determination of the input aerosol layer height from CALIOP, improvement in aerosol optical depth (AOD) for nonspherical dust, development of quality assurance (QA) procedure, etc.

  6. Determining Aerosol Plume Height from Two GEO Imagers: Lessons from MISR and GOES

    NASA Technical Reports Server (NTRS)

    Wu, Dong L.

    2012-01-01

    Aerosol plume height is a key parameter to determine impacts of particulate matters generated from biomass burning, wind-blowing dust, and volcano eruption. Retrieving cloud top height from stereo imageries from two GOES (Geostationary Operational Environmental Satellites) have been demonstrated since 1970's and the principle should work for aerosol plumes if they are optically thick. The stereo technique has also been used by MISR (Multiangle Imaging SpectroRadiometer) since 2000 that has nine look angles along track to provide aerosol height measurements. Knowing the height of volcano aerosol layers is as important as tracking the ash plume flow for aviation safety. Lack of knowledge about ash plume height during the 2010 Eyja'rjallajokull eruption resulted in the largest air-traffic shutdown in Europe since World War II. We will discuss potential applications of Asian GEO satellites to make stereo measurements for dust and volcano plumes.

  7. Retrieving the Height of Smoke and Dust Aerosols by Synergistic Use of VIIRS, OMPS, and CALIOP Observations

    NASA Technical Reports Server (NTRS)

    Lee, Jaehwa; Hsu, N. Christina; Bettenhausen, Corey; Sayer, Andrew M.; Seftor, Colin J.; Jeong, Myeong-Jae

    2015-01-01

    Aerosol Single scattering albedo and Height Estimation (ASHE) algorithm was first introduced in Jeong and Hsu (2008) to provide aerosol layer height as well as single scattering albedo (SSA) for biomass burning smoke aerosols. One of the advantages of this algorithm was that the aerosol layer height can be retrieved over broad areas, which had not been available from lidar observations only. The algorithm utilized aerosol properties from three different satellite sensors, i.e., aerosol optical depth (AOD) and Ångström exponent (AE) from Moderate Resolution Imaging Spectroradiometer (MODIS), UV aerosol index (UVAI) from Ozone Monitoring Instrument (OMI), and aerosol layer height from Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP). Here, we extend the application of the algorithm to Visible Infrared Imaging Radiometer Suite (VIIRS) and Ozone Mapping and Profiler Suite (OMPS) data. We also now include dust layers as well as smoke. Other updates include improvements in retrieving the AOD of nonspherical dust from VIIRS, better determination of the aerosol layer height from CALIOP, and more realistic input aerosol profiles in the forward model for better accuracy.

  8. Passive remote sensing of aerosol layer height using near-UV multiangle polarization measurements

    NASA Astrophysics Data System (ADS)

    Wu, Lianghai; Hasekamp, Otto; van Diedenhoven, Bastiaan; Cairns, Brian; Yorks, John E.; Chowdhary, Jacek

    2016-08-01

    We demonstrate that multiangle polarization measurements in the near-UV and blue part of the spectrum are very well suited for passive remote sensing of aerosol layer height. For this purpose we use simulated measurements with different setups (different wavelength ranges, with and without polarization, different polarimetric accuracies) as well as airborne measurements from the Research Scanning Polarimeter (RSP) obtained over the continental USA. We find good agreement of the retrieved aerosol layer height from RSP with measurements from the Cloud Physics Lidar showing a mean absolute difference of less than 1 km. Furthermore, we found that the information on aerosol layer height is provided for large part by the multiangle polarization measurements with high accuracy rather than the multiangle intensity measurements. The information on aerosol layer height is significantly decreased when the shortest RSP wavelength (410 nm) is excluded from the retrieval and is virtually absent when 550 nm is used as shortest wavelength.

  9. Ceilometer signal performance with height in high aerosol loads

    NASA Astrophysics Data System (ADS)

    Bachour, D.; Perez-Astudillo, D.

    2016-02-01

    This paper is dedicated to the study of the Vaisala CL51 ceilometer backscatter signals during a one-year period, in particular the study of the noise embedded in the signals measured by the ceilometer, under cloudless conditions. The noise analysis is done to provide indication about the maximum atmospheric height up to which the ceilometer signal is still reliable enough in clear-sky conditions, for the detection of changing aerosol contents. The experiment was carried out in Doha, Qatar, for a period of 12 months, from December 2012 to November 2013. 214 clear days were selected during this year. Several tests were performed in order to assess the variability of the backscatter signals from day to day and between different heights in the atmosphere. To the authors' knowledge, it is the first time that the signal performance of a ceilometer is studied in a highly aerosol-loaded region, and for a relatively extended period of time. Considering the whole year, it is found that a height of 5 or 6 km represents a good compromise between including the signals arising from the dynamicity of the atmosphere and removing as much as possible the signal dominated by noise at higher heights. In winter months, however, this limit can be extended up to a height of 7 km.

  10. On the Specification of Smoke Injection Heights for Aerosol Forecasting

    NASA Astrophysics Data System (ADS)

    da Silva, A.; Schaefer, C.; Randles, C. A.

    2014-12-01

    The proper forecasting of biomass burning (BB) aerosols in global or regional transport models requires not only the specification of emission rates with sufficient temporal resolution but also the injection layers of such emissions. While current near realtime biomass burning inventories such as GFAS, QFED, FINN, GBBEP and FLAMBE provide such emission rates, it is left for each modeling system to come up with its own scheme for distributing these emissions in the vertical. A number of operational aerosol forecasting models deposits BB emissions in the near surface model layers, relying on the model's parameterization of turbulent and convective transport to determine the vertical mass distribution of BB aerosols. Despite their simplicity such schemes have been relatively successful reproducing the vertical structure of BB aerosols, except for those large fires that produce enough buoyancy to puncture the PBL and deposit the smoke at higher layers. Plume Rise models such as the so-called 'Freitas model', parameterize this sub-grid buoyancy effect, but require the specification of fire size and heat fluxes, none of which is readily available in near real-time from current remotely-sensed products. In this talk we will introduce a bayesian algorithm for estimating file size and heat fluxes from MODIS brightness temperatures. For small to moderate fires the Freitas model driven by these heat flux estimates produces plume tops that are highly correlated with the GEOS-5 model estimate of PBL height. Comparison to MINX plume height estimates from MISR indicates moderate skill of this scheme predicting the injection height of large fires. As an alternative, we make use of OMPS UV aerosol index data in combination with estimates of Overshooting Convective Tops (from MODIS and Geo-stationary satellites) to detect PyCu events and specify the BB emission vertical mass distribution in such cases. We will present a discussion of case studies during the SEAC4RS field campaign in

  11. Measurements of aerosol layer height and vertical profiles by lidar over Jinhua City

    NASA Astrophysics Data System (ADS)

    Yu, Siqi; Liu, Dong; Wang, Zhenzhu; Xu, Jiwei; Tian, Xiaomin; Wu, Decheng; Xie, Chenbo; Wang, Yingjian

    2018-03-01

    The vertical distribution of the aerosol layers is depicted by using the lidar data in Jinhua city from 2013 to 2014. The lidar installed in Jinhua is a dual-wavelength Mie polarization Raman lidar. Aerosol layers are searched through gradient method. At the same time, HYSPLIT model is used to tracing the aerosol trajectories. The results show that different heights of aerosol layers have different transportation route. By a case study, the lidar data on December 30, 2013 and May 1, 2014 reveal several vertical aerosol layers. According to the 24-hour backward trajectory of HYSPLIT model, different aerosol layers comes from different places, and this may relate to the winter monsoon in China.

  12. The role of cloud contamination, aerosol layer height and aerosol model in the assessment of the OMI near-UV retrievals over the ocean

    NASA Astrophysics Data System (ADS)

    Gassó, Santiago; Torres, Omar

    2016-07-01

    Retrievals of aerosol optical depth (AOD) at 388 nm over the ocean from the Ozone Monitoring Instrument (OMI) two-channel near-UV algorithm (OMAERUV) have been compared with independent AOD measurements. The analysis was carried out over the open ocean (OMI and MODerate-resolution Imaging Spectrometer (MODIS) AOD comparisons) and over coastal and island sites (OMI and AERONET, the AErosol RObotic NETwork). Additionally, a research version of the retrieval algorithm (using MODIS and CALIOP (Cloud-Aerosol Lidar with Orthogonal Polarization) information as constraints) was utilized to evaluate the sensitivity of the retrieval to different assumed aerosol properties. Overall, the comparison resulted in differences (OMI minus independent measurements) within the expected levels of uncertainty for the OMI AOD retrievals (0.1 for AOD < 0.3, 30 % for AOD > 0.3). Using examples from case studies with outliers, the reasons that led to the observed differences were examined with specific purpose to determine whether they are related to instrument limitations (i.e., pixel size, calibration) or algorithm assumptions (such as aerosol shape, aerosol height). The analysis confirms that OMAERUV does an adequate job at rejecting cloudy scenes within the instrument's capabilities. There is a residual cloud contamination in OMI pixels with quality flag 0 (the best conditions for aerosol retrieval according to the algorithm), resulting in a bias towards high AODs in OMAERUV. This bias is more pronounced at low concentrations of absorbing aerosols (AOD 388 nm ˜ < 0.5). For higher aerosol loadings, the bias remains within OMI's AOD uncertainties. In pixels where OMAERUV assigned a dust aerosol model, a fraction of them (< 20 %) had retrieved AODs significantly lower than AERONET and MODIS AODs. In a case study, a detailed examination of the aerosol height from CALIOP and the AODs from MODIS, along with sensitivity tests, was carried out by varying the different assumed parameters in the

  13. The Role of Cloud Contamination, Aerosol Layer Height and Aerosol Model in the Assessment of the OMI Near-UV Retrievals Over the Ocean

    NASA Technical Reports Server (NTRS)

    Gasso, Santiago; Torres, Omar

    2016-01-01

    Retrievals of aerosol optical depth (AOD) at 388 nm over the ocean from the Ozone Monitoring Instrument (OMI) two-channel near-UV algorithm (OMAERUV) have been compared with independent AOD measurements. The analysis was carried out over the open ocean (OMI and MODerate-resolution Imaging Spectrometer (MODIS) AOD comparisons) and over coastal and island sites (OMI and AERONET, the AErosol RObotic NETwork). Additionally, a research version of the retrieval algorithm (using MODIS and CALIOP (Cloud-Aerosol Lidar with Orthogonal Polarization) information as constraints) was utilized to evaluate the sensitivity of the retrieval to different assumed aerosol properties. Overall, the comparison resulted in differences (OMI minus independent measurements) within the expected levels of uncertainty for the OMI AOD retrievals (0.1 for AOD less than 0.3, 30% for AOD greater than 0.3). Using examples from case studies with outliers, the reasons that led to the observed differences were examined with specific purpose to determine whether they are related to instrument limitations (i.e., pixel size, calibration) or algorithm assumptions (such as aerosol shape, aerosol height). The analysis confirms that OMAERUV does an adequate job at rejecting cloudy scenes within the instrument's capabilities. There is a residual cloud contamination in OMI pixels with quality flag 0 (the best conditions for aerosol retrieval according to the algorithm), resulting in a bias towards high AODs in OMAERUV. This bias is more pronounced at low concentrations of absorbing aerosols (AOD 388 nm approximately less than 0.5). For higher aerosol loadings, the bias remains within OMI's AOD uncertainties. In pixels where OMAERUV assigned a dust aerosol model, a fraction of them (less than 20 %) had retrieved AODs significantly lower than AERONET and MODIS AODs. In a case study, a detailed examination of the aerosol height from CALIOP and the AODs from MODIS, along with sensitivity tests, was carried out by

  14. Height Distribution Between Cloud and Aerosol Layers from the GLAS Spaceborne Lidar in the Indian Ocean Region

    NASA Technical Reports Server (NTRS)

    Hart, William D.; Spinhirne, James D.; Palm, Steven P.; Hlavka, Dennis L.

    2005-01-01

    The Geoscience Laser Altimeter System (GLAS), a nadir pointing lidar on the Ice Cloud and land Elevation Satellite (ICESat) launched in 2003, now provides important new global measurements of the relationship between the height distribution of cloud and aerosol layers. GLAS data have the capability to detect, locate, and distinguish between cloud and aerosol layers in the atmosphere up to 40 km altitude. The data product algorithm tests the product of the maximum attenuated backscatter coefficient b'(r) and the vertical gradient of b'(r) within a layer against a predetermined threshold. An initial case result for the critical Indian Ocean region is presented. From the results the relative height distribution between collocated aerosol and cloud shows extensive regions where cloud formation is well within dense aerosol scattering layers at the surface. Citation: Hart, W. D., J. D. Spinhime, S. P. Palm, and D. L. Hlavka (2005), Height distribution between cloud and aerosol layers from the GLAS spaceborne lidar in the Indian Ocean region,

  15. Developments in the Aerosol Layer Height Retrieval Algorithm for the Copernicus Sentinel-4/UVN Instrument

    NASA Astrophysics Data System (ADS)

    Nanda, Swadhin; Sanders, Abram; Veefkind, Pepijn

    2016-04-01

    The Sentinel-4 mission is a part of the European Commission's Copernicus programme, the goal of which is to provide geo-information to manage environmental assets, and to observe, understand and mitigate the effects of the changing climate. The Sentinel-4/UVN instrument design is motivated by the need to monitor trace gas concentrations and aerosols in the atmosphere from a geostationary orbit. The on-board instrument is a high resolution UV-VIS-NIR (UVN) spectrometer system that provides hourly radiance measurements over Europe and northern Africa with a spatial sampling of 8 km. The main application area of Sentinel-4/UVN is air quality. One of the data products that is being developed for Sentinel-4/UVN is the Aerosol Layer Height (ALH). The goal is to determine the height of aerosol plumes with a resolution of better than 0.5 - 1 km. The ALH product thus targets aerosol layers in the free troposphere, such as desert dust, volcanic ash and biomass during plumes. KNMI is assigned with the development of the Aerosol Layer Height (ALH) algorithm. Its heritage is the ALH algorithm developed by Sanders and De Haan (ATBD, 2016) for the TROPOMI instrument on board the Sentinel-5 Precursor mission that is to be launched in June or July 2016 (tentative date). The retrieval algorithm designed so far for the aerosol height product is based on the absorption characteristics of the oxygen-A band (759-770 nm). The algorithm has heritage to the ALH algorithm developed for TROPOMI on the Sentinel 5 precursor satellite. New aspects for Sentinel-4/UVN include the higher resolution (0.116 nm compared to 0.4 for TROPOMI) and hourly observation from the geostationary orbit. The algorithm uses optimal estimation to obtain a spectral fit of the reflectance across absorption band, while assuming a single uniform layer with fixed width to represent the aerosol vertical distribution. The state vector includes amongst other elements the height of this layer and its aerosol optical

  16. Utilization of O4 slant column density to derive aerosol layer height from a spaceborne UV-visible hyperspectral sensor: sensitivity and case study

    NASA Astrophysics Data System (ADS)

    Park, S. S.; Kim, J.; Lee, H.; Torres, O.; Lee, K.-M.; Lee, S. D.

    2015-03-01

    The sensitivities of oxygen-dimer (O4) slant column densities (SCDs) to changes in aerosol layer height are investigated using simulated radiances by a radiative transfer model, Linearized Discrete Ordinate Radiative Transfer (LIDORT), and Differential Optical Absorption Spectroscopy (DOAS) technique. The sensitivities of the O4 SCDs to aerosol types and optical properties are also evaluated and compared. Among the O4 absorption bands at 340, 360, 380, and 477 nm, the O4 absorption band at 477 nm is found to be the most suitable to retrieve the aerosol effective height. However, the O4 SCD at 477 nm is significantly influenced not only by the aerosol layer effective height but also by aerosol vertical profiles, optical properties including single scattering albedo (SSA), aerosol optical depth (AOD), and surface albedo. Overall, the error of the retrieved aerosol effective height is estimated to be 414 m (16.5%), 564 m (22.4%), and 1343 m (52.5%) for absorbing, dust, and non-absorbing aerosol, respectively, assuming knowledge on the aerosol vertical distribution type. Using radiance data from the Ozone Monitoring Instrument (OMI), a new algorithm is developed to derive the aerosol effective height over East Asia after the determination of the aerosol type and AOD from the MODerate resolution Imaging Spectroradiometer (MODIS). The retrieved aerosol effective heights are lower by approximately 300 m (27 %) compared to those obtained from the ground-based LIDAR measurements.

  17. Utilization of O4 Slant Column Density to Derive Aerosol Layer Height from a Spaceborne UV-Visible Hyperspectral Sensor: Sensitivity and Case Study

    NASA Technical Reports Server (NTRS)

    Park, Sang Seo; Kim, Jhoon; Lee, Hanlim; Torres, Omar; Lee, Kwang-Mog; Lee, Sang Deok

    2016-01-01

    The sensitivities of oxygen-dimer (O4) slant column densities (SCDs) to changes in aerosol layer height are investigated using the simulated radiances by a radiative transfer model, the linearized pseudo-spherical vector discrete ordinate radiative transfer (VLIDORT), and the Differential Optical Absorption Spectroscopy (DOAS) technique. The sensitivities of the O4 index (O4I), which is defined as dividing O4 SCD by 10(exp 40) sq molecules cm(exp -5), to aerosol types and optical properties are also evaluated and compared. Among the O4 absorption bands at 340, 360, 380, and 477 nm, the O4 absorption band at 477 nm is found to be the most suitable to retrieve the aerosol effective height. However, the O4I at 477 nm is significantly influenced not only by the aerosol layer effective height but also by aerosol vertical profiles, optical properties including single scattering albedo (SSA), aerosol optical depth (AOD), particle size, and surface albedo. Overall, the error of the retrieved aerosol effective height is estimated to be 1276, 846, and 739 m for dust, non-absorbing, and absorbing aerosol, respectively, assuming knowledge on the aerosol vertical distribution shape. Using radiance data from the Ozone Monitoring Instrument (OMI), a new algorithm is developed to derive the aerosol effective height over East Asia after the determination of the aerosol type and AOD from the MODerate resolution Imaging Spectroradiometer (MODIS). About 80% of retrieved aerosol effective heights are within the error range of 1 km compared to those obtained from the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) measurements on thick aerosol layer cases.

  18. Pulse height response of an optical particle counter to monodisperse aerosols

    NASA Technical Reports Server (NTRS)

    Wilmoth, R. G.; Grice, S. S.; Cuda, V.

    1976-01-01

    The pulse height response of a right angle scattering optical particle counter has been investigated using monodisperse aerosols of polystyrene latex spheres, di-octyl phthalate and methylene blue. The results confirm previous measurements for the variation of mean pulse height as a function of particle diameter and show good agreement with the relative response predicted by Mie scattering theory. Measured cumulative pulse height distributions were found to fit reasonably well to a log normal distribution with a minimum geometric standard deviation of about 1.4 for particle diameters greater than about 2 micrometers. The geometric standard deviation was found to increase significantly with decreasing particle diameter.

  19. Large-Scale Covariability Between Aerosol and Precipitation Over the 7-SEAS Region: Observations and Simulations

    NASA Technical Reports Server (NTRS)

    Huang, Jingfeng; Hsu, N. Christina; Tsay, Si-Chee; Zhang, Chidong; Jeong, Myeong Jae; Gautam, Ritesh; Bettenhausen, Corey; Sayer, Andrew M.; Hansell, Richard A.; Liu, Xiaohong; hide

    2012-01-01

    One of the seven scientific areas of interests of the 7-SEAS field campaign is to evaluate the impact of aerosol on cloud and precipitation (http://7-seas.gsfc.nasa.gov). However, large-scale covariability between aerosol, cloud and precipitation is complicated not only by ambient environment and a variety of aerosol effects, but also by effects from rain washout and climate factors. This study characterizes large-scale aerosol-cloud-precipitation covariability through synergy of long-term multi ]sensor satellite observations with model simulations over the 7-SEAS region [10S-30N, 95E-130E]. Results show that climate factors such as ENSO significantly modulate aerosol and precipitation over the region simultaneously. After removal of climate factor effects, aerosol and precipitation are significantly anti-correlated over the southern part of the region, where high aerosols loading is associated with overall reduced total precipitation with intensified rain rates and decreased rain frequency, decreased tropospheric latent heating, suppressed cloud top height and increased outgoing longwave radiation, enhanced clear-sky shortwave TOA flux but reduced all-sky shortwave TOA flux in deep convective regimes; but such covariability becomes less notable over the northern counterpart of the region where low ]level stratus are found. Using CO as a proxy of biomass burning aerosols to minimize the washout effect, large-scale covariability between CO and precipitation was also investigated and similar large-scale covariability observed. Model simulations with NCAR CAM5 were found to show similar effects to observations in the spatio-temporal patterns. Results from both observations and simulations are valuable for improving our understanding of this region's meteorological system and the roles of aerosol within it. Key words: aerosol; precipitation; large-scale covariability; aerosol effects; washout; climate factors; 7- SEAS; CO; CAM5

  20. Utilization of O4 slant column density to derive aerosol layer height from a space-borne UV-visible hyperspectral sensor: sensitivity and case study

    NASA Astrophysics Data System (ADS)

    Park, Sang Seo; Kim, Jhoon; Lee, Hanlim; Torres, Omar; Lee, Kwang-Mog; Lee, Sang Deok

    2016-02-01

    The sensitivities of oxygen-dimer (O4) slant column densities (SCDs) to changes in aerosol layer height are investigated using the simulated radiances by a radiative transfer model, the linearized pseudo-spherical vector discrete ordinate radiative transfer (VLIDORT), and the differential optical absorption spectroscopy (DOAS) technique. The sensitivities of the O4 index (O4I), which is defined as dividing O4 SCD by 1040 molecules2 cm-5, to aerosol types and optical properties are also evaluated and compared. Among the O4 absorption bands at 340, 360, 380, and 477 nm, the O4 absorption band at 477 nm is found to be the most suitable to retrieve the aerosol effective height. However, the O4I at 477 nm is significantly influenced not only by the aerosol layer effective height but also by aerosol vertical profiles, optical properties including single scattering albedo (SSA), aerosol optical depth (AOD), particle size, and surface albedo. Overall, the error of the retrieved aerosol effective height is estimated to be 1276, 846, and 739 m for dust, non-absorbing, and absorbing aerosol, respectively, assuming knowledge on the aerosol vertical distribution shape. Using radiance data from the Ozone Monitoring Instrument (OMI), a new algorithm is developed to derive the aerosol effective height over East Asia after the determination of the aerosol type and AOD from the MODerate resolution Imaging Spectroradiometer (MODIS). About 80 % of retrieved aerosol effective heights are within the error range of 1 km compared to those obtained from the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) measurements on thick aerosol layer cases.

  1. Evaluation of the operational Aerosol Layer Height retrieval algorithm for Sentinel-5 Precursor: application to O2 A band observations from GOME-2A

    NASA Astrophysics Data System (ADS)

    Sanders, A. F. J.; de Haan, J. F.; Sneep, M.; Apituley, A.; Stammes, P.; Vieitez, M. O.; Tilstra, L. G.; Tuinder, O. N. E.; Koning, C. E.; Veefkind, J. P.

    2015-06-01

    .e., layer high in the atmosphere) to the extent that retrieved values are not realistically representing actual extinction profiles anymore. When the surface albedo is fixed in retrievals with GOME-2A spectra, convergence deteriorates as expected, but retrieved aerosol layer pressures become much higher (i.e., layer lower in atmosphere). The comparison with lidar measurements indicates that retrieved aerosol layer heights are indeed representative of the underlying profile in that case. Finally, subsequent retrieval simulations with two-layer aerosol profiles show that a model error in the assumed profile (two layers in the simulation but only one in the retrieval) is partly absorbed by the surface albedo when this parameter is fitted. This is expected in view of the correlations between errors in fit parameters and the effect is relatively small for elevated layers (less than 100 hPa). In case one of the scattering layers is near the surface (boundary layer aerosols), the effect becomes surprisingly large such that the retrieved height of the single layer is above the two-layer profile. Furthermore, we find that the retrieval solution, once retrieval converges, hardly depends on the starting values for the fit. Sensitivity experiments with GOME-2A spectra also show that aerosol layer height is indeed relatively robust against inaccuracies in the assumed aerosol model, even when the surface albedo is not fitted. We show spectral fit residuals, which can be used for further investigations. Fit residuals may be partly explained by spectroscopic uncertainties, which is suggested by an experiment showing the improvement of convergence when the absorption cross section is scaled in agreement with Butz et al. (2012) and Crisp et al. (2012) and a temperature offset to the a priori ECMWF temperature profile is fitted. Retrieved temperature offsets are always negative and quite large (ranging between -4 and -8 K), which is not expected if temperature offsets absorb remaining

  2. Evaluation of the operational Aerosol Layer Height retrieval algorithm for Sentinel-5 Precursor: application to O2 A band observations from GOME-2A

    NASA Astrophysics Data System (ADS)

    Sanders, A. F. J.; de Haan, J. F.; Sneep, M.; Apituley, A.; Stammes, P.; Vieitez, M. O.; Tilstra, L. G.; Tuinder, O. N. E.; Koning, C. E.; Veefkind, J. P.

    2015-11-01

    .e., layer high in the atmosphere) to the extent that retrieved values no longer realistically represent actual extinction profiles. When the surface albedo is fixed in retrievals with GOME-2A spectra, convergence deteriorates as expected, but retrieved aerosol layer pressures become much higher (i.e., layer lower in atmosphere). The comparison with lidar measurements indicates that retrieved aerosol layer heights are indeed representative of the underlying profile in that case. Finally, subsequent retrieval simulations with two-layer aerosol profiles show that a model error in the assumed profile (two layers in the simulation but only one in the retrieval) is partly absorbed by the surface albedo when this parameter is fitted. This is expected in view of the correlations between errors in fit parameters and the effect is relatively small for elevated layers (less than 100 hPa). If one of the scattering layers is near the surface (boundary layer aerosols), the effect becomes surprisingly large, in such a way that the retrieved height of the single layer is above the two-layer profile. Furthermore, we find that the retrieval solution, once retrieval converges, hardly depends on the starting values for the fit. Sensitivity experiments with GOME-2A spectra also show that aerosol layer height is indeed relatively robust against inaccuracies in the assumed aerosol model, even when the surface albedo is not fitted. We show spectral fit residuals, which can be used for further investigations. Fit residuals may be partly explained by spectroscopic uncertainties, which is suggested by an experiment showing the improvement of convergence when the absorption cross section is scaled in agreement with Butz et al. (2013) and Crisp et al. (2012), and a temperature offset to the a priori ECMWF temperature profile is fitted. Retrieved temperature offsets are always negative and quite large (ranging between -4 and -8 K), which is not expected if temperature offsets absorb remaining

  3. Utilization of O4 Slant Column Density to Derive Aerosol Layer Height from a Space-Borne UV-Visible Hyperspectral Sensor: Sensitivity and Case Study

    NASA Technical Reports Server (NTRS)

    Park, Sang Seo; Kim, Jhoon; Lee, Hanlim; Torres, Omar; Lee, Kwang-Mog; Lee, Sang Deok

    2016-01-01

    The sensitivities of oxygen-dimer (O4) slant column densities (SCDs) to changes in aerosol layer height are investigated using the simulated radiances by a radiative transfer model, the linearized pseudo-spherical vector discrete ordinate radiative transfer (VLIDORT), and the differential optical absorption spectroscopy (DOAS) technique. The sensitivities of the O4 index (O4I), which is defined as dividing O4 SCD by 10(sup 40) molecules (sup 2) per centimeters(sup -5), to aerosol types and optical properties are also evaluated and compared. Among the O4 absorption bands at 340, 360, 380, and 477 nanometers, the O4 absorption band at 477 nanometers is found to be the most suitable to retrieve the aerosol effective height. However, the O4I at 477 nanometers is significantly influenced not only by the aerosol layer effective height but also by aerosol vertical profiles, optical properties including single scattering albedo (SSA), aerosol optical depth (AOD), particle size, and surface albedo. Overall, the error of the retrieved aerosol effective height is estimated to be 1276, 846, and 739 meters for dust, non-absorbing, and absorbing aerosol, respectively, assuming knowledge on the aerosol vertical distribution shape. Using radiance data from the Ozone Monitoring Instrument (OMI), a new algorithm is developed to derive the aerosol effective height over East Asia after the determination of the aerosol type and AOD from the MODerate resolution Imaging Spectroradiometer (MODIS). About 80 percent of retrieved aerosol effective heights are within the error range of 1 kilometer compared to those obtained from the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) measurements on thick aerosol layer cases.

  4. Forest fires in Himalayan region during 2016 - Aerosol load and smoke plume heights detection by multi sensor observations

    NASA Astrophysics Data System (ADS)

    Kumar, S.; Dumka, U. C.

    2017-12-01

    The forest fires are common events over the Central Himalayan region during the pre-monsoon season (March - June) of every year. Forest fire plays a crucial role in governing the vegetation structure, ecosystem, climate change as well as in atmospheric chemistry. In regional and global scales, the combustion of forest and grassland vegetation releases large volumes of smoke, aerosols, and other chemically active species that significantly influence Earth's radiative budget and atmospheric chemistry, impacting air quality and risks to human health. During the year 2016, massive forest fires have been recorded over the Central Himalayan region of Uttarakhand which continues for several weeks. To study this event we used the multi-satellite observations of aerosols and pollutants during pre-fire, fire and post-fire period over the central Himalayan region. The data used in this study are active fire count and aerosol optical depth (AOD) from MODerate-resolution Imaging Spectroradiometer (MODIS), aerosol index and gases pollutants from Ozone Monitoring Instrument (OMI), along with vertical profiles of aerosols and smoke plume height information from Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO). The result shows that the mean fire counts were maximum in April. The daily average AOD value shows an increasing trend during the fire events. The mean value of AOD before the massive fire (25 April), during the fire (30 April) and post fire (5 May) periods are 0.3, 1.2 and 0.6 respectively. We find an increasing trend of total columnar NO2 over the Uttarakhand region during the massive fire event. Space-born Lidar (CALIPSO) retrievals show the extent of smoke plume heights beyond the planetary boundary layer up to 6 km during the peak burning day (April 30). The HYSPLIT air mass forward trajectory shows the long-range transportation of smoke plumes. The results of the present study provide valuable information for addressing smoke plume and

  5. Stereoscopic Height and Wind Retrievals for Aerosol Plumes with the MISR INteractive eXplorer (MINX)

    NASA Technical Reports Server (NTRS)

    Nelson, D.L.; Garay, M.J.; Kahn, Ralph A.; Dunst, Ben A.

    2013-01-01

    The Multi-angle Imaging SpectroRadiometer (MISR) instrument aboard the Terra satellite acquires imagery at 275-m resolution at nine angles ranging from 0deg (nadir) to 70deg off-nadir. This multi-angle capability facilitates the stereoscopic retrieval of heights and motion vectors for clouds and aerosol plumes. MISR's operational stereo product uses this capability to retrieve cloud heights and winds for every satellite orbit, yielding global coverage every nine days. The MISR INteractive eXplorer (MINX) visualization and analysis tool complements the operational stereo product by providing users the ability to retrieve heights and winds locally for detailed studies of smoke, dust and volcanic ash plumes, as well as clouds, at higher spatial resolution and with greater precision than is possible with the operational product or with other space-based, passive, remote sensing instruments. This ability to investigate plume geometry and dynamics is becoming increasingly important as climate and air quality studies require greater knowledge about the injection of aerosols and the location of clouds within the atmosphere. MINX incorporates features that allow users to customize their stereo retrievals for optimum results under varying aerosol and underlying surface conditions. This paper discusses the stereo retrieval algorithms and retrieval options in MINX, and provides appropriate examples to explain how the program can be used to achieve the best results.

  6. Relationship Between Aerosol Optical Depth and Particulate Matter Over Singapore: Effects of Aerosol Vertical Distributions

    NASA Technical Reports Server (NTRS)

    Chew, Boo Ning; Campbell, James; Hyer, Edward J.; Salinas, Santo V.; Reid, Jeffrey S.; Welton, Ellsworth J.; Holben, Brent N.; Liew, Soo Chin

    2016-01-01

    As part of the Seven Southeast Asian Studies (7SEAS) program, an Aerosol Robotic Network (AERONET) sun photometer and a Micro-Pulse Lidar Network (MPLNET) instrument have been deployed at Singapore to study the regional aerosol environment of the Maritime Continent (MC). In addition, the Navy Aerosol Analysis and Prediction System (NAAPS) is used to model aerosol transport over the region. From 24 September 2009 to 31 March 2011, the relationships between ground-, satellite- and model-based aerosol optical depth (AOD) and particulate matter with aerodynamic equivalent diameters less than 2.5 microns (PM2.5) for air quality applications are investigated. When MPLNET-derived aerosol scale heights are applied to normalize AOD for comparison with surface PM2.5 data, the empirical relationships are shown to improve with an increased 11%, 10% and 5% in explained variances, for AERONET, MODIS and NAAPS respectively. The ratios of root mean square errors to standard deviations for the relationships also show corresponding improvements of 8%, 6% and 2%. Aerosol scale heights are observed to be bimodal with a mode below and another above the strongly-capped/deep near-surface layer (SCD; 0-1.35 km). Aerosol extinctions within the SCD layer are well-correlated with surface PM2.5 concentrations, possibly due to strong vertical mixing in the region.

  7. Spatial distribution analysis of the OMI aerosol layer height: a pixel-by-pixel comparison to CALIOP observations

    NASA Astrophysics Data System (ADS)

    Chimot, Julien; Pepijn Veefkind, J.; Vlemmix, Tim; Levelt, Pieternel F.

    2018-04-01

    A global picture of atmospheric aerosol vertical distribution with a high temporal resolution is of key importance not only for climate, cloud formation, and air quality research studies but also for correcting scattered radiation induced by aerosols in absorbing trace gas retrievals from passive satellite sensors. Aerosol layer height (ALH) was retrieved from the OMI 477 nm O2 - O2 band and its spatial pattern evaluated over selected cloud-free scenes. Such retrievals benefit from a synergy with MODIS data to provide complementary information on aerosols and cloudy pixels. We used a neural network approach previously trained and developed. Comparison with CALIOP aerosol level 2 products over urban and industrial pollution in eastern China shows consistent spatial patterns with an uncertainty in the range of 462-648 m. In addition, we show the possibility to determine the height of thick aerosol layers released by intensive biomass burning events in South America and Russia from OMI visible measurements. A Saharan dust outbreak over sea is finally discussed. Complementary detailed analyses show that the assumed aerosol properties in the forward modelling are the key factors affecting the accuracy of the results, together with potential cloud residuals in the observation pixels. Furthermore, we demonstrate that the physical meaning of the retrieved ALH scalar corresponds to the weighted average of the vertical aerosol extinction profile. These encouraging findings strongly suggest the potential of the OMI ALH product, and in more general the use of the 477 nm O2 - O2 band from present and future similar satellite sensors, for climate studies as well as for future aerosol correction in air quality trace gas retrievals.

  8. A study of aerosol absorption and height retrievals with a hyperspectral (UV to NIR) passive sensor

    NASA Astrophysics Data System (ADS)

    Gasso, S.

    2017-12-01

    With the deployment of the first sensor (TOMS, in 1978) with capabilities to detect aerosol absorption (AA) from space, there has been a continuous evolution in hardware and algorithms used to measured this property. Although with TOMS and its more advanced successors (such as OMI) made significant progress in globally characterizing AA , there is room for improvement especially by taking advantage of sensors with extended spectral coverage (UV to NIR) and high spatial resolution (<1 km). While such unique sensor does not exist yet, the collocation of observations from different platforms that jointly fulfill those characteristics (e.g. A-Train, S-NPP) confirm that it is possible to fully retrieve all AA parameters that modulate absorption in the upwelling radiance (AOD, SSA and aerosol layer height). However, such combined approaches still have some drawbacks such as the difficulty to account for cloud contamination. The upcoming deployment of satellite detectors with the desired features all in one sensor (PACE, TropOMI, GEMS) prompt a revision of the AA retrieval technique used in past approaches. In particular,the TropOMI mission, a hyperspectral UV-to-NIR sensor with moderate ( 5km nadir pixel) spatial resolution to be launched in Fall 2017. In addition , the sensor will include sensing capabilities for the wavelength range of the Oxygen bands A and B at very high wavelength resolution. This study will be centered on the aerosol detection capabilities of TropOMI. Because the spectral range covered, it is theoretically possible to simultaneously retrieve the aerosol optical depth, the single scattering albedo and aerosol mean height without assuming any of them as it was the case with previous retrieval approaches. Specifically, we intend to present a theoretical study based on simulated radiances at selected UV, VIS and near-IR bands (including the Oxygen bands) and evaluate the sensitivity of this sensor to different levels of aerosol concentration, height

  9. Observation-based estimation of aerosol-induced reduction of planetary boundary layer height

    NASA Astrophysics Data System (ADS)

    Zou, Jun; Sun, Jianning; Ding, Aijun; Wang, Minghuai; Guo, Weidong; Fu, Congbin

    2017-09-01

    Radiative aerosols are known to influence the surface energy budget and hence the evolution of the planetary boundary layer. In this study, we develop a method to estimate the aerosol-induced reduction in the planetary boundary layer height (PBLH) based on two years of ground-based measurements at a site, the Station for Observing Regional Processes of the Earth System (SORPES), at Nanjing University, China, and radiosonde data from the meteorological station of Nanjing. The observations show that increased aerosol loads lead to a mean decrease of 67.1 W m-2 for downward shortwave radiation (DSR) and a mean increase of 19.2 W m-2 for downward longwave radiation (DLR), as well as a mean decrease of 9.6 Wm-2 for the surface sensible heat flux (SHF) in the daytime. The relative variations of DSR, DLR and SHF are shown as a function of the increment of column mass concentration of particulate matter (PM2.5). High aerosol loading can significantly increase the atmospheric stability in the planetary boundary layer during both daytime and nighttime. Based on the statistical relationship between SHF and PM2.5 column mass concentrations, the SHF under clean atmospheric conditions (same as the background days) is derived. In this case, the derived SHF, together with observed SHF, are then used to estimate changes in the PBLH related to aerosols. Our results suggest that the PBLH decreases more rapidly with increasing aerosol loading at high aerosol loading. When the daytime mean column mass concentration of PM2.5 reaches 200 mg m-2, the decrease in the PBLH at 1600 LST (local standard time) is about 450 m.

  10. Ionospheric scale height from the refraction of satellite signals.

    NASA Technical Reports Server (NTRS)

    Heron, M. L.; Titheridge, J. E.

    1972-01-01

    Accurate observations of the elevation angle of arrival of 20 MHz signals from the polar orbiting satellite Beacon-B for a 20 month period have provided transmission ionograms which may be reduced to give Hp the scale height at the peak of the ionosphere. Noon seasonal averages of Hp are 1.35 (in winter) to 1.55 (in summer) times greater than the scale height obtained from bottom-side ionograms. A comparison of scale height at the peak with routine measurements of total content and peak electron density indicates that the O+/H+ transition level is above 1000 km during the day but comes down to about 630 km on winter nights. A predawn peak in the overall scale height is caused by a lowering of the layer to a region of increased recombination and is magnified in winter by low O+/H+ transition levels.

  11. Aerosol-cloud interactions in a multi-scale modeling framework

    NASA Astrophysics Data System (ADS)

    Lin, G.; Ghan, S. J.

    2017-12-01

    Atmospheric aerosols play an important role in changing the Earth's climate through scattering/absorbing solar and terrestrial radiation and interacting with clouds. However, quantification of the aerosol effects remains one of the most uncertain aspects of current and future climate projection. Much of the uncertainty results from the multi-scale nature of aerosol-cloud interactions, which is very challenging to represent in traditional global climate models (GCMs). In contrast, the multi-scale modeling framework (MMF) provides a viable solution, which explicitly resolves the cloud/precipitation in the cloud resolved model (CRM) embedded in the GCM grid column. In the MMF version of community atmospheric model version 5 (CAM5), aerosol processes are treated with a parameterization, called the Explicit Clouds Parameterized Pollutants (ECPP). It uses the cloud/precipitation statistics derived from the CRM to treat the cloud processing of aerosols on the GCM grid. However, this treatment treats clouds on the CRM grid but aerosols on the GCM grid, which is inconsistent with the reality that cloud-aerosol interactions occur on the cloud scale. To overcome the limitation, here, we propose a new aerosol treatment in the MMF: Explicit Clouds Explicit Aerosols (ECEP), in which we resolve both clouds and aerosols explicitly on the CRM grid. We first applied the MMF with ECPP to the Accelerated Climate Modeling for Energy (ACME) model to have an MMF version of ACME. Further, we also developed an alternative version of ACME-MMF with ECEP. Based on these two models, we have conducted two simulations: one with the ECPP and the other with ECEP. Preliminary results showed that the ECEP simulations tend to predict higher aerosol concentrations than ECPP simulations, because of the more efficient vertical transport from the surface to the higher atmosphere but the less efficient wet removal. We also found that the cloud droplet number concentrations are also different between the

  12. Fractional solubility of aerosol iron: Synthesis of a global-scale data set

    NASA Astrophysics Data System (ADS)

    Sholkovitz, Edward R.; Sedwick, Peter N.; Church, Thomas M.; Baker, Alexander R.; Powell, Claire F.

    2012-07-01

    Aerosol deposition provides a major input of the essential micronutrient iron to the open ocean. A critical parameter with respect to biological availability is the proportion of aerosol iron that enters the oceanic dissolved iron pool - the so-called fractional solubility of aerosol iron (%FeS). Here we present a global-scale compilation of total aerosol iron loading (FeT) and estimated %FeS values for ∼1100 samples collected over the open ocean, the coastal ocean, and some continental sites, including a new data set from the Atlantic Ocean. Despite the wide variety of methods that have been used to define 'soluble' aerosol iron, our global-scale compilation reveals a remarkably consistent trend in the fractional solubility of aerosol iron as a function of total aerosol iron loading, with the great bulk of the data defining an hyperbolic trend. The hyperbolic trends that we observe for both global- and regional-scale data are adequately described by a simple two-component mixing model, whereby the fractional solubility of iron in the bulk aerosol reflects the conservative mixing of 'lithogenic' mineral dust (high FeT and low %FeS) and non-lithogenic 'combustion' aerosols (low FeT and high %FeS). An increasing body of empirical and model-based evidence points to anthropogenic fuel combustion as the major source of these non-lithogenic 'combustion' aerosols, implying that human emissions are a major determinant of the fractional solubility of iron in marine aerosols. The robust global-scale relationship between %FeS and FeT provides a simple heuristic method for estimating aerosol iron solubility at the regional to global scale.

  13. Evaluating the Height of Biomass Burning Smoke Aerosols Retrieved from Synergistic Use of Multiple Satellite Sensors Over Southeast Asia

    NASA Technical Reports Server (NTRS)

    Lee, Jaehwa; Hsu, N. Christina; Bettenhausen, Corey; Sayer, Andrew M.; Seftor, Colin J.; Jeong, Myeong-Jae; Tsay, Si-Chee; Welton, Ellsworth J.; Wang, Sheng-Hsiang; Chen, Wei-Nai

    2016-01-01

    This study evaluates the height of biomass burning smoke aerosols retrieved from a combined use of Visible Infrared Imaging Radiometer Suite (VIIRS), Ozone Mapping and Profiler Suite (OMPS), and Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) observations. The retrieved heights are compared against space borne and ground-based lidar measurements during the peak biomass burning season (March and April) over Southeast Asia from 2013 to 2015. Based on the comparison against CALIOP, a quality assurance (QA) procedure is developed. It is found that 74 (8184) of the retrieved heights fall within 1 km of CALIOP observations for unfiltered (QA-filtered) data, with root-mean-square error (RMSE) of 1.1 km (0.81.0 km). Eliminating the requirement of CALIOP observations from the retrieval process significantly increases the temporal coverage with only a slight decrease in the retrieval accuracy; for best QA data, 64 of data fall within 1 km of CALIOP observations with RMSE of 1.1 km. When compared with Micro-Pulse Lidar Network (MPLNET) measurements deployed at Doi Ang Khang, Thailand, the retrieved heights show RMSE of 1.7 km (1.1 km) for unfiltered (QA-filtered) data for the complete algorithm, and 0.9 km (0.8 km) for the simplified algorithm.

  14. A review of approaches to estimate wildfire plume injection height within large-scale atmospheric chemical transport models

    NASA Astrophysics Data System (ADS)

    Paugam, R.; Wooster, M.; Freitas, S.; Martin, M. Val

    2016-01-01

    Landscape fires produce smoke containing a very wide variety of chemical species, both gases and aerosols. For larger, more intense fires that produce the greatest amounts of emissions per unit time, the smoke tends initially to be transported vertically or semi-vertically close by the source region, driven by the intense heat and convective energy released by the burning vegetation. The column of hot smoke rapidly entrains cooler ambient air, forming a rising plume within which the fire emissions are transported. The characteristics of this plume, and in particular the height to which it rises before releasing the majority of the smoke burden into the wider atmosphere, are important in terms of how the fire emissions are ultimately transported, since for example winds at different altitudes may be quite different. This difference in atmospheric transport then may also affect the longevity, chemical conversion, and fate of the plumes chemical constituents, with for example very high plume injection heights being associated with extreme long-range atmospheric transport. Here we review how such landscape-scale fire smoke plume injection heights are represented in larger-scale atmospheric transport models aiming to represent the impacts of wildfire emissions on component of the Earth system. In particular we detail (i) satellite Earth observation data sets capable of being used to remotely assess wildfire plume height distributions and (ii) the driving characteristics of the causal fires. We also discuss both the physical mechanisms and dynamics taking place in fire plumes and investigate the efficiency and limitations of currently available injection height parameterizations. Finally, we conclude by suggesting some future parameterization developments and ideas on Earth observation data selection that may be relevant to the instigation of enhanced methodologies aimed at injection height representation.

  15. Informing Aerosol Transport Models With Satellite Multi-Angle Aerosol Measurements

    NASA Technical Reports Server (NTRS)

    Limbacher, J.; Patadia, F.; Petrenko, M.; Martin, M. Val; Chin, M.; Gaitley, B.; Garay, M.; Kalashnikova, O.; Nelson, D.; Scollo, S.

    2011-01-01

    As the aerosol products from the NASA Earth Observing System's Multi-angle Imaging SpectroRadiometer (MISR) mature, we are placing greater focus on ways of using the aerosol amount and type data products, and aerosol plume heights, to constrain aerosol transport models. We have demonstrated the ability to map aerosol air-mass-types regionally, and have identified product upgrades required to apply them globally, including the need for a quality flag indicating the aerosol type information content, that varies depending upon retrieval conditions. We have shown that MISR aerosol type can distinguish smoke from dust, volcanic ash from sulfate and water particles, and can identify qualitative differences in mixtures of smoke, dust, and pollution aerosol components in urban settings. We demonstrated the use of stereo imaging to map smoke, dust, and volcanic effluent plume injection height, and the combination of MISR and MODIS aerosol optical depth maps to constrain wildfire smoke source strength. This talk will briefly highlight where we stand on these application, with emphasis on the steps we are taking toward applying the capabilities toward constraining aerosol transport models, planet-wide.

  16. Comparison of dust-layer heights from active and passive satellite sensors

    NASA Astrophysics Data System (ADS)

    Kylling, Arve; Vandenbussche, Sophie; Capelle, Virginie; Cuesta, Juan; Klüser, Lars; Lelli, Luca; Popp, Thomas; Stebel, Kerstin; Veefkind, Pepijn

    2018-05-01

    Aerosol-layer height is essential for understanding the impact of aerosols on the climate system. As part of the European Space Agency Aerosol_cci project, aerosol-layer height as derived from passive thermal and solar satellite sensors measurements have been compared with aerosol-layer heights estimated from CALIOP measurements. The Aerosol_cci project targeted dust-type aerosol for this study. This ensures relatively unambiguous aerosol identification by the CALIOP processing chain. Dust-layer height was estimated from thermal IASI measurements using four different algorithms (from BIRA-IASB, DLR, LMD, LISA) and from solar GOME-2 (KNMI) and SCIAMACHY (IUP) measurements. Due to differences in overpass time of the various satellites, a trajectory model was used to move the CALIOP-derived dust heights in space and time to the IASI, GOME-2 and SCIAMACHY dust height pixels. It is not possible to construct a unique dust-layer height from the CALIOP data. Thus two CALIOP-derived layer heights were used: the cumulative extinction height defined as the height where the CALIOP extinction column is half of the total extinction column, and the geometric mean height, which is defined as the geometrical mean of the top and bottom heights of the dust layer. In statistical average over all IASI data there is a general tendency to a positive bias of 0.5-0.8 km against CALIOP extinction-weighted height for three of the four algorithms assessed, while the fourth algorithm has almost no bias. When comparing geometric mean height there is a shift of -0.5 km for all algorithms (getting close to zero for the three algorithms and turning negative for the fourth). The standard deviation of all algorithms is quite similar and ranges between 1.0 and 1.3 km. When looking at different conditions (day, night, land, ocean), there is more detail in variabilities (e.g. all algorithms overestimate more at night than during the day). For the solar sensors it is found that on average SCIAMACHY data

  17. Small-scale Scheimpflug lidar for aerosol extinction coefficient and vertical atmospheric transmittance detection.

    PubMed

    Sun, Guodong; Qin, Laian; Hou, Zaihong; Jing, Xu; He, Feng; Tan, Fengfu; Zhang, Silong

    2018-03-19

    In this paper, a new prototypical Scheimpflug lidar capable of detecting the aerosol extinction coefficient and vertical atmospheric transmittance at 1 km above the ground is described. The lidar system operates at 532 nm and can be used to detect aerosol extinction coefficients throughout an entire day. Then, the vertical atmospheric transmittance can be determined from the extinction coefficients with the equation of numerical integration in this area. CCD flat fielding of the image data is used to mitigate the effects of pixel sensitivity variation. An efficient method of two-dimensional wavelet transform according to a local threshold value has been proposed to reduce the Gaussian white noise in the lidar signal. Furthermore, a new iteration method of backscattering ratio based on genetic algorithm is presented to calculate the aerosol extinction coefficient and vertical atmospheric transmittance. Some simulations are performed to reduce the different levels of noise in the simulated signal in order to test the precision of the de-noising method and inversion algorithm. The simulation result shows that the root-mean-square errors of extinction coefficients are all less than 0.02 km -1 , and that the relative errors of the atmospheric transmittance between the model and inversion data are below 0.56% for all cases. The feasibility of the instrument and the inversion algorithm have also been verified by an optical experiment. The average relative errors of aerosol extinction coefficients between the Scheimpflug lidar and the conventional backscattering elastic lidar are 3.54% and 2.79% in the full overlap heights of two time points, respectively. This work opens up new possibilities of using a small-scale Scheimpflug lidar system for the remote sensing of atmospheric aerosols.

  18. Radiative Effects of Aerosol in the Marine Environment: Tales from the Two-Column Aerosol Project

    NASA Astrophysics Data System (ADS)

    Berg, L. K.; Fast, J. D.; Barnard, J.; Chand, D.; Chapman, E. G.; Comstock, J. M.; Ferrare, R. A.; Flynn, C. J.; Hair, J. W.; Hostetler, C. A.; Hubbe, J.; Johnson, R.; Kassianov, E.; Kluzek, C.; Laskin, A.; Lee, Y.; Mei, F.; Michalsky, J. J.; Redemann, J.; Rogers, R. R.; Russell, P. B.; Sedlacek, A. J.; Schmid, B.; Shilling, J. E.; Shinozuka, Y.; Springston, S. R.; Tomlinson, J. M.; Wilson, J. M.; Zelenyuk, A.; Berkowitz, C. M.

    2013-12-01

    There is still uncertainty associated with the direct radiative forcing by atmospheric aerosol and its representation in atmospheric models. This is particularly true in marine environments near the coast where the aerosol loading is a function of both naturally occurring and anthropogenic aerosol. These regions are also subject to variable synoptic and thermally driven flows (land-sea breezes) that transport aerosol between the continental and marine environments. The situation is made more complicated due to seasonal changes in aerosol emissions. Given these differences in emissions, we expect significant differences in the aerosol intensive and extensive properties between summer and winter and data is needed to evaluate models over the wide range of conditions. To address this issue, the recently completed Two Column Aerosol Project (TCAP) was designed to measure the key aerosol parameters in two atmospheric columns, one located over Cape Cod, Massachusetts and another approximately 200 km from the coast over the Atlantic Ocean. Measurements included aerosol size distribution, chemical composition, optical properties and vertical distribution. Several aspects make TCAP unique, including the year-long deployment of a suite of surface-based instruments by the US Department of Energy's Atmospheric Radiation Measurement (ARM) Climate Research Facility and two aircraft intensive operations periods supported by the ARM Airborne Facility, one conducted in July 2012 and a second in February 2013. The presentation will include a discussion of the impact of the aerosol optical properties and their uncertainty on simulations of the radiation budget within the TCAP domain in the context of both single column and regional scale models. Data from TCAP will be used to highlight a number of important factors, including diurnal variation in aerosol optical depth measured at the surface site, systematic changes in aerosol optical properties (including scattering, absorption, and

  19. Global View of Aerosol Vertical Distributions from CALIPSO Lidar Measurements and GOCART Simulations: Regional and Seasonal Variations

    NASA Technical Reports Server (NTRS)

    Yu, Hongbin; Chin, Mian; Winker, David M.; Omar, Ali H.; Liu, Zhaoyan; Kittaka, Chieko; Diehl, Thomas

    2010-01-01

    This study examines seasonal variations of the vertical distribution of aerosols through a statistical analysis of the Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) lidar observations from June 2006 to November 2007. A data-screening scheme is developed to attain good quality data in cloud-free conditions, and the polarization measurement is used to separate dust from non-dust aerosol. The CALIPSO aerosol observations are compared with aerosol simulations from the Goddard Chemistry Aerosol Radiation Transport (GOCART) model and aerosol optical depth (AOD) measurements from the MODerate resolution Imaging Spectroradiometer (MODIS). The CALIPSO observations of geographical patterns and seasonal variations of AOD are generally consistent with GOCART simulations and MODIS retrievals especially near source regions, while the magnitude of AOD shows large discrepancies in most regions. Both the CALIPSO observation and GOCART model show that the aerosol extinction scale heights in major dust and smoke source regions are generally higher than that in industrial pollution source regions. The CALIPSO aerosol lidar ratio also generally agrees with GOCART model within 30% on regional scales. Major differences between satellite observations and GOCART model are identified, including (1) an underestimate of aerosol extinction by GOCART over the Indian sub-continent, (2) much larger aerosol extinction calculated by GOCART than observed by CALIPSO in dust source regions, (3) much weaker in magnitude and more concentrated aerosol in the lower atmosphere in CALIPSO observation than GOCART model over transported areas in midlatitudes, and (4) consistently lower aerosol scale height by CALIPSO observation than GOCART model. Possible factors contributing to these differences are discussed.

  20. Cloud-top height retrieval from polarizing remote sensor POLDER

    NASA Astrophysics Data System (ADS)

    He, Xianqiang; Pan, Delu; Yan, Bai; Mao, Zhihua

    2006-10-01

    A new cloud-top height retrieval method is proposed by using polarizing remote sensing. In cloudy conditions, it shows that, in purple and blue bands, linear polarizing radiance at the top-of-atmosphere (TOA) is mainly contributed by Rayleigh scattering of the atmosphere's molecules above cloud, and the contribution by cloud reflection and aerosol scattering can be neglected. With such characteristics, the basis principle and method of cloud-top height retrieval using polarizing remote sensing are presented in detail, and tested by the polarizing remote sensing data of POLDER. The satellite-derived cloud-top height product can not only show the distribution of global cloud-top height, but also obtain the cloud-top height distribution of moderate-scale meteorological phenomena like hurricanes and typhoons. This new method is promising to become the operational algorithm for cloud-top height retrieval for POLDER and the future polarizing remote sensing satellites.

  1. A study of regional-scale aerosol assimilation using a Stretch-NICAM

    NASA Astrophysics Data System (ADS)

    Misawa, S.; Dai, T.; Schutgens, N.; Nakajima, T.

    2013-12-01

    Although aerosol is considered to be harmful to human health and it became a social issue, aerosol models and emission inventories include large uncertainties. In recent studies, data assimilation is applied to aerosol simulation to get more accurate aerosol field and emission inventory. Most of these studies, however, are carried out only on global scale, and there are only a few researches about regional scale aerosol assimilation. In this study, we have created and verified an aerosol assimilation system on regional scale, in hopes to reduce an error associated with the aerosol emission inventory. Our aerosol assimilation system has been developed using an atmospheric climate model, NICAM (Non-hydrostaric ICosahedral Atmospheric Model; Satoh et al., 2008) with a stretch grid system and coupled with an aerosol transport model, SPRINTARS (Takemura et al., 2000). Also, this assimilation system is based on local ensemble transform Kalman filter (LETKF). To validate this system, we used a simulated observational data by adding some artificial errors to the surface aerosol fields constructed by Stretch-NICAM-SPRINTARS. We also included a small perturbation in original emission inventory. This assimilation with modified observational data and emission inventory was performed in Kanto-plane region around Tokyo, Japan, and the result indicates the system reducing a relative error of aerosol concentration by 20%. Furthermore, we examined a sensitivity of the aerosol assimilation system by varying the number of total ensemble (5, 10 and 15 ensembles) and local patch (domain) size (radius of 50km, 100km and 200km), both of which are the tuning parameters in LETKF. The result of the assimilation with different ensemble number 5, 10 and 15 shows that the larger the number of ensemble is, the smaller the relative error become. This is consistent with ensemble Kalman filter theory and imply that this assimilation system works properly. Also we found that assimilation system

  2. CRISM Limb Observations of Aerosols and Water Vapor

    NASA Technical Reports Server (NTRS)

    Smith, Michael D.; Wolff, M.J.; Clancy, R.T.; Seelos, F.; Murchie, S.L.

    2009-01-01

    Near-infrared spectra taken in a limb-viewing geometry by the Compact Reconnaissance Imaging Spectrometer for Mars (CRISM) on-board the Mars Reconnaissance Orbiter (MRO) provide a useful tool for probing atmospheric structure. Here we describe preliminary work on the retrieval of vertical profiles of aerosols and water vapor from the CRISM limb observations. The first full set of CRISM limb observations was taken in July 2009, with subsequent limb observations planned once every two months. Each set of limb observations contains about four dozen scans across the limb giving pole-to-pole coverage for two orbits at roughly 100 and 290 W longitude. Radiative transfer modeling taking account of aerosol scattering in the limb-viewing geometry is used to model the observations. The retrievals show the height to which dust and water vapor extend and the location and height of water ice clouds. Results from the First set of CRISM limb observations (July 2009, Ls=300) show dust aerosol well-mixed to about three scale heights above the surface with thin water ice clouds above the dust near the equator and at mid-northern latitudes. Water vapor is concentrated at high southern latitudes.

  3. Dissemination of aerosol and splatter during ultrasonic scaling: a pilot study.

    PubMed

    Veena, H R; Mahantesha, S; Joseph, Preethi A; Patil, Sudhir R; Patil, Suvarna H

    2015-01-01

    Routine dental procedures produce aerosol and splatter, which pose a potential risk to the clinician and dental personnel, as well as the immunocompromised patient. Reports indicate that the ultrasonic scaler is the greatest producer of aerosol and splatter. The study aimed to evaluate the contamination distance, contamination amount and contamination duration of aerosol produced during ultrasonic scaling. The study was performed on a mannequin fitted with phantom jaws on a dental chair. Mock scaling was done for 15 min using an auto-tuned magnetostrictive ultrasonic scaler with the simultaneous use of a low volume saliva ejector. An ultrafiltrate-containing fluorescent dye was used in the reservoir supplying the scaler unit. Filter paper discs were placed in different positions and distances in the operatory. Immediately following scaling, the filter paper discs were replaced with new ones. This was done every 30 min for a total duration of 90 min. Maximum contamination was found on the right arm of the operator and left arm of the assistant. Contamination was also found on the head, chest and inner surface of the face mask of the operator and of the assistant. The aerosol was found to remain in the air up to 30 min after scaling. The occupational health hazards of dental aerosols can be minimized by following simple, inexpensive precautions. Copyright © 2014 King Saud Bin Abdulaziz University for Health Sciences. Published by Elsevier Ltd. All rights reserved.

  4. A weighted least squares approach to retrieve aerosol layer height over bright surfaces applied to GOME-2 measurements of the oxygen A band for forest fire cases over Europe

    NASA Astrophysics Data System (ADS)

    Nanda, Swadhin; Pepijn Veefkind, J.; de Graaf, Martin; Sneep, Maarten; Stammes, Piet; de Haan, Johan F.; Sanders, Abram F. J.; Apituley, Arnoud; Tuinder, Olaf; Levelt, Pieternel F.

    2018-06-01

    This paper presents a weighted least squares approach to retrieve aerosol layer height from top-of-atmosphere reflectance measurements in the oxygen A band (758-770 nm) over bright surfaces. A property of the measurement error covariance matrix is discussed, due to which photons travelling from the surface are given a higher preference over photons that scatter back from the aerosol layer. This is a potential source of biases in the estimation of aerosol properties over land, which can be mitigated by revisiting the design of the measurement error covariance matrix. The alternative proposed in this paper, which we call the dynamic scaling method, introduces a scene-dependent and wavelength-dependent modification in the measurement signal-to-noise ratio in order to influence this matrix. This method is generally applicable to other retrieval algorithms using weighted least squares. To test this method, synthetic experiments are done in addition to application to GOME-2A and GOME-2B measurements of the oxygen A band over the August 2010 Russian wildfires and the October 2017 Portugal wildfire plume over western Europe.

  5. New Measurements of Aerosol Vertical Structure from Space Using the NASA Geoscience Laser Altimeter System (GLAS): Applications for Aerosol Transport Models

    NASA Technical Reports Server (NTRS)

    Welton, Ellsworth J.; Ginoux, Paul; Colarco, Peter; Chin, Mian; Spinhirne, James D.; Palm, Steven P.; Hlavka, Dennis; Hart, William

    2003-01-01

    In the past, satellite measurements of aerosols have only been possible using passive sensors. Analysis of passive satellite data has lead to an improved understanding of aerosol properties, spatial distribution, and their effect on the earth s climate. However, direct measurement of aerosol vertical distribution has not been possible using only the passive data. Knowledge of aerosol vertical distribution is important to correctly assess the impact of aerosol absorption, for certain atmospheric correction procedures, and to help constrain height profiles in aerosol transport models. On January 12,2003 NASA launched the first satellite-based lidar, the Geoscience Laser Altimeter System (GLAS), onboard the ICESat spacecraft. GLAS is both an altimeter and an atmospheric lidar, and obtains direct measurements of aerosol and cloud heights. Here we show an overview of GLAS, provide an update of its current status, and discuss how GUS data will be useful for modeling efforts. In particular, a strategy of using GLAS to characterize the height profile of dust plumes over source regions will be presented, along with initial results. Such information can be used to validate and improve output from aerosol transport models. Aerosol height profile comparisons between GLAS and transport models will be shown for regions downwind of aerosol sources. We will also discuss the feasibility of assimilating GLAS profiles into the models in order to improve their output,

  6. New Measurements of Aerosol Vertical Structure from Space using the NASA Geoscience Laser Altimeter System (GLAS): Applications for Aerosol Transport Models

    NASA Technical Reports Server (NTRS)

    Welton, E. J.; Spinhime, J.; Palm, S.; Hlavka, D.; Hart, W.; Ginoux, P.; Chin, M.; Colarco, P.

    2004-01-01

    In the past, satellite measurements of aerosols have only been possible using passive sensors. Analysis of passive satellite data has lead to an improved understanding of aerosol properties, spatial distribution, and their effect on the earth,s climate. However, direct measurement of aerosol vertical distribution has not been possible using only the passive data. Knowledge of aerosol vertical distribution is important to correctly assess the impact of aerosol absorption, for certain atmospheric correction procedures, and to help constrain height profiles in aerosol transport models. On January 12,2003 NASA launched the first satellite-based lidar, the Geoscience Laser Altimeter System (GLAS), onboard the ICESat spacecraft. GLAS is both an altimeter and an atmospheric lidar, and obtains direct measurements of aerosol and cloud heights. Here we show an overview of GLAS, provide an update of its current status, and discuss how GLAS data will be useful for modeling efforts. In particular, a strategy of using GLAS to characterize the height profile of dust plumes over source regions will be presented, along with initial results. Such information can be used to validate and improve output from aerosol transport models. Aerosol height profile comparisons between GLAS and transport models will be shown for regions downwind of aerosol sources. We will also discuss the feasibility of assimilating GLAS profiles into the models in order to improve their output.

  7. Small-scale open ocean currents have large effects on wind wave heights

    NASA Astrophysics Data System (ADS)

    Ardhuin, Fabrice; Gille, Sarah T.; Menemenlis, Dimitris; Rocha, Cesar B.; Rascle, Nicolas; Chapron, Bertrand; Gula, Jonathan; Molemaker, Jeroen

    2017-06-01

    Tidal currents and large-scale oceanic currents are known to modify ocean wave properties, causing extreme sea states that are a hazard to navigation. Recent advances in the understanding and modeling capability of open ocean currents have revealed the ubiquitous presence of eddies, fronts, and filaments at scales 10-100 km. Based on realistic numerical models, we show that these structures can be the main source of variability in significant wave heights at scales less than 200 km, including important variations down to 10 km. Model results are consistent with wave height variations along satellite altimeter tracks, resolved at scales larger than 50 km. The spectrum of significant wave heights is found to be of the order of 70>>2/>(g2>>2>) times the current spectrum, where >> is the spatially averaged significant wave height, >> is the energy-averaged period, and g is the gravity acceleration. This variability induced by currents has been largely overlooked in spite of its relevance for extreme wave heights and remote sensing.Plain Language SummaryWe show that the variations in currents at <span class="hlt">scales</span> 10 to 100 km are the main source of variations in wave <span class="hlt">heights</span> at the same <span class="hlt">scales</span>. Our work uses a combination of realistic numerical models for currents and waves and data from the Jason-3 and SARAL/AltiKa satellites. This finding will be of interest for the investigation of extreme wave <span class="hlt">heights</span>, remote sensing, and air-sea interactions. As an immediate application, the present results will help constrain the error budget of the up-coming satellite missions, in particular the Surface Water and Ocean Topography (SWOT) mission, and decide how the data will have to be processed to arrive at accurate sea level and wave measurements. It will also help in the analysis of wave measurements by the CFOSAT satellite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000013623&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DTOM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000013623&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DTOM"><span>Current Status of <span class="hlt">Aerosol</span> Retrievals from TOMS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Torres, O.; Herman, J. R.; Bhartia, P. K.; Ginoux, P.</p> <p>1999-01-01</p> <p>Properties of atmospheric <span class="hlt">aerosols</span> over all land and water surfaces are retrieved from TOMS measurements of backscattered radiances. The TOMS technique, uses observations at two wavelengths. In the near ultraviolet (330-380 nm) range, where the effects of gaseous absorption are negligible. The retrieved properties are optical depth and a measure of <span class="hlt">aerosol</span> absorptivity, generally expressed as single scattering albedo. The main sources of error of the TOMS <span class="hlt">aerosol</span> products are sub-pixel cloud contamination and uncertainty on the <span class="hlt">height</span> above the surface of UV-absorbing <span class="hlt">aerosol</span> layers. The first error source is related to the large footprint (50 x 50 km at nadir) of the sensor, and the lack of detection capability of sub-pixel size clouds. The uncertainty associated with the <span class="hlt">height</span> of the absorbing <span class="hlt">aerosol</span> layers, on the other hand, is related to the pressure dependence of the molecular scattering process, which is the basis of the near-UV method of absorbing <span class="hlt">aerosol</span> detection. The detection of non-absorbing <span class="hlt">aerosols</span> is not sensitive to <span class="hlt">aerosol</span> layer <span class="hlt">height</span>. We will report on the ongoing work to overcome both of these difficulties. Coincident measurements of high spatial resolution thermal infrared radiances are used to address the cloud contamination issue. Mostly clear scenes for <span class="hlt">aerosol</span> retrieval are selected by examining the spatial homogeneity of the IR radiance measurements within a TOMS pixel. The approach to reduce the uncertainty associated with the <span class="hlt">height</span> of the <span class="hlt">aerosol</span> layer by making use of a chemical transport model will also be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860007278','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860007278"><span>Airborne Lidar measurements of <span class="hlt">aerosols</span>, mixed layer <span class="hlt">heights</span>, and ozone during the 1980 PEPE/NEROS summer field experiment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Browell, E. V.; Shipley, S. T.; Butler, C. F.; Ismail, S.</p> <p>1985-01-01</p> <p>A detailed summary of the NASA Ultraviolet Differential Absorption Lidar (UV DIAL) data archive obtained during the EPA Persistent Elevated Pollution Episode/Northeast Regional Oxidant Study (PEPE/NEROS) Summer Field Experiment Program (July through August 1980) is presented. The UV dial data set consists of remote measurements of mixed layer <span class="hlt">heights</span>, <span class="hlt">aerosol</span> backscatter cross sections, and sequential ozone profiles taken during 14 long-range flights onboard the NASA Wallops Flight Center Electra aircraft. These data are presented in graphic and tabular form, and they have been submitted to the PEPE/NEROS data archive on digital magnetic tape. The derivation of mixing <span class="hlt">heights</span> and ozone profiles from UV Dial signals is discussed, and detailed intercomparisons with measurements obtained by in situ sensors are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005543','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005543"><span><span class="hlt">Aerosol</span> Mapping From Space: Strengths, Limitations, and Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kahn, Ralph</p> <p>2010-01-01</p> <p>The <span class="hlt">aerosol</span> data products from the NASA Earth Observing System's MISR and MODIS instruments provide significant advances in regional and global <span class="hlt">aerosol</span> optical depth (AOD) mapping, <span class="hlt">aerosol</span> type measurement, and source plume characterization from space. These products have been and are being used for many applications, ranging from regional air quality assessment, to <span class="hlt">aerosol</span> air mass type identification and evolution, to wildfire smoke injection <span class="hlt">height</span> and <span class="hlt">aerosol</span> transport model validation. However, retrieval uncertainties and coverage gaps still limit the quantitative constraints these satellite data place on some important questions, such as global-<span class="hlt">scale</span> long-term trends and direct <span class="hlt">aerosol</span> radiative forcing. Major advances in these areas seem to require a different paradigm, involving the integration of satellite with suborbital data and with models. This presentation will briefly summarize where we stand, and what incremental improvements we can expect, with the current MISR and MODIS <span class="hlt">aerosol</span> products, and will then elaborate on some initial steps aimed at the necessary integration of satellite data with data from other sources and with chemical transport models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150005512&hterms=Organic+Chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DOrganic%2BChemical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150005512&hterms=Organic+Chemical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DOrganic%2BChemical"><span>The Organic <span class="hlt">Aerosols</span> of Titan's Atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sotin, Christophe; Lawrence, Kenneth; Beauchamp, Patricia M.; Zimmerman, Wayne</p> <p>2012-01-01</p> <p>One of Titan's many characteristics is the presence of a haze that veils its surface. This haze is composed of heavy organic particles and determining the chemical composition of these particles is a primary objective for future probes that would conduct in situ analysis. Meanwhile, solar occultations provide constraints on the optical characteristics of the haze layer. This paper describes solar occultation observations obtained by the Visual and Infrared Mapping Spectrometer (VIMS) onboard the Cassini spacecraft. These observations strongly constrain the optical characteristics of the haze layer. We detail the different steps involved in the processing of these data and apply them to two occultations that were observed at the South Pole and at the equator in order to investigate the latitudinal dependence of optical properties. The light curves obtained in seven atmospheric windows between 0.933-microns to 5-microns allow us to characterize atmospheric layers from 300 km to the surface. Very good fits of the light curves are obtained using a simple profile of number density of <span class="hlt">aerosols</span> that is characterized by a <span class="hlt">scale</span> <span class="hlt">height</span>. The main difference between the South Pole and the equator is that the value of the <span class="hlt">scale</span> <span class="hlt">height</span> increases with altitude at the South Pole whereas it decreases at the equator. The vertically integrated amount of <span class="hlt">aerosols</span> is similar at the two locations. The curve describing the cross-section versus wavelength is identical at the two locations suggesting that the <span class="hlt">aerosols</span> have similar characteristics. Finally, we find that the two-way vertical transmission at 5-microns is as large as 80% at both locations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A..72K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A..72K"><span>CHANG-ES. IX. Radio <span class="hlt">scale</span> <span class="hlt">heights</span> and <span class="hlt">scale</span> lengths of a consistent sample of 13 spiral galaxies seen edge-on and their correlations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krause, Marita; Irwin, Judith; Wiegert, Theresa; Miskolczi, Arpad; Damas-Segovia, Ancor; Beck, Rainer; Li, Jiang-Tao; Heald, George; Müller, Peter; Stein, Yelena; Rand, Richard J.; Heesen, Volker; Walterbos, Rene A. M.; Dettmar, Ralf-Jürgen; Vargas, Carlos J.; English, Jayanne; Murphy, Eric J.</p> <p>2018-03-01</p> <p>Aim. The vertical halo <span class="hlt">scale</span> <span class="hlt">height</span> is a crucial parameter to understand the transport of cosmic-ray electrons (CRE) and their energy loss mechanisms in spiral galaxies. Until now, the radio <span class="hlt">scale</span> <span class="hlt">height</span> could only be determined for a few edge-on galaxies because of missing sensitivity at high resolution. Methods: We developed a sophisticated method for the <span class="hlt">scale</span> <span class="hlt">height</span> determination of edge-on galaxies. With this we determined the <span class="hlt">scale</span> <span class="hlt">heights</span> and radial <span class="hlt">scale</span> lengths for a sample of 13 galaxies from the CHANG-ES radio continuum survey in two frequency bands. Results: The sample average values for the radio <span class="hlt">scale</span> <span class="hlt">heights</span> of the halo are 1.1 ± 0.3 kpc in C-band and 1.4 ± 0.7 kpc in L-band. From the frequency dependence analysis of the halo <span class="hlt">scale</span> <span class="hlt">heights</span> we found that the wind velocities (estimated using the adiabatic loss time) are above the escape velocity. We found that the halo <span class="hlt">scale</span> <span class="hlt">heights</span> increase linearly with the radio diameters. In order to exclude the diameter dependence, we defined a normalized <span class="hlt">scale</span> <span class="hlt">height</span> h˜ which is quite similar for all sample galaxies at both frequency bands and does not depend on the star formation rate or the magnetic field strength. However, h˜ shows a tight anticorrelation with the mass surface density. Conclusions: The sample galaxies with smaller <span class="hlt">scale</span> lengths are more spherical in the radio emission, while those with larger <span class="hlt">scale</span> lengths are flatter. The radio <span class="hlt">scale</span> <span class="hlt">height</span> depends mainly on the radio diameter of the galaxy. The sample galaxies are consistent with an escape-dominated radio halo with convective cosmic ray propagation, indicating that galactic winds are a widespread phenomenon in spiral galaxies. While a higher star formation rate or star formation surface density does not lead to a higher wind velocity, we found for the first time observational evidence of a gravitational deceleration of CRE outflow, e.g. a lowering of the wind velocity from the galactic disk.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A24C..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A24C..01H"><span>The DRAGON <span class="hlt">scale</span> concept and results for remote sensing of <span class="hlt">aerosol</span> properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Holben, B. N.; Eck, T. F.; Schafer, J.; Giles, D. M.; Kim, J.; Sano, I.; Mukai, S.; Kim, Y. J.; Reid, J. S.; Pickering, K. E.; Crawford, J. H.; Smirnov, A.; Sinyuk, A.; Slutsker, I.; Sorokin, M.; Rodriguez, J.; Liew, S.; Trevino, N.; Lim, H.; Lefer, B. L.; Nadkarni, R.; Macke, A.; Kinne, S. A.; Anderson, B. E.; Russell, P. B.; Maring, H. B.; Welton, E. J.; da Silva, A.; Toon, O. B.; Redemann, J.</p> <p>2013-12-01</p> <p><span class="hlt">Aerosol</span> processes occur at microscales but are typically observed and reported at continental to global <span class="hlt">scales</span>. Often observable <span class="hlt">aerosol</span> processes that have significant anthropogenic impact occur on spatial <span class="hlt">scales</span> of tens to a few hundred km, representative of convective cloud processing, urban/megacity sources, anthropogenic burning and natural wildfires, dry lakebed dust sources etc. Historically remote sensing of <span class="hlt">aerosols</span> has relied on relatively coarse temporal and spatial resolution satellite observations or high temporal resolution point observations from ground-based monitoring sites from networks such as AERONET, SKYNET, MPLNET and many other surface observation platforms. Airborne remote and in situ observations combined with assimilation models were/are to be the mesoscale link between the ground- and space-based RS <span class="hlt">scales</span>. However clearly the in situ and ground-based RS characterizations of <span class="hlt">aerosols</span> require a convergence of thought, parameterization and actual <span class="hlt">scale</span> measurements in order to advance this goal. This has been served by periodic multidisciplinary field campaigns yet only recently has a concerted effort been made to establish these ground-based networks in an effort to capture the mesoscale processes through measurement programs such as DISCOVER AQ and NASA AERONET's effort to foster such measurements and analysis through the Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON), short term meso-networks, with partners in Asia and Europe and N. America. This talk will review the historical need for such networks and discuss some of the results and in some cases unexpected findings from the eight DRAGON campaigns conducted the last several years. Emphasis will be placed on the most recent DISCOVER AQ campaign conducted in Houston TX and the synergism with a regional to global network plan through the SEAC4RS US campaign.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Ap%26SS.362..201M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Ap%26SS.362..201M"><span>Analysis of the temporal-spatial distribution of ionosphere <span class="hlt">scale</span> <span class="hlt">height</span> based on COSMIC occultation data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ma, Xin-Xin; Lin, Zhan; Jin, Hong-Lin; Chen, Hua-Ran; Jiao, Li-Guo</p> <p>2017-11-01</p> <p>In this study, the distribution characteristics of <span class="hlt">scale</span> <span class="hlt">height</span> at various solar activity levels were statistically analyzed using the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC) radio occultation data for 2007-2013. The results show that: (1) in the mid-high latitude region, the daytime (06-17LT) <span class="hlt">scale</span> <span class="hlt">height</span> exhibits annual variations in the form of a single peak structure with the crest appearing in summer. At the high latitude region, an annual variation is also observed for nighttime (18-05LT) <span class="hlt">scale</span> <span class="hlt">height</span>; (2) changes in the spatial distribution of the <span class="hlt">scale</span> <span class="hlt">height</span> occur. The crests are deflected towards the north during daytime (12-14LT) at a geomagnetic longitude of 60°W-180°W, and they are distributed roughly along the geomagnetic equator at 60°W-180°E. In the approximate region of 120°W-150°E and 50°S-80°S, the <span class="hlt">scale</span> <span class="hlt">height</span> values are significantly higher than those in other mid-latitude areas. This region enlarges with increased solar activity, and shows an approximately symmetric distribution about 0° geomagnetic longitude. Nighttime (00-02LT) <span class="hlt">scale</span> <span class="hlt">height</span> values in the high-latitude region are larger than those in the low-mid latitude region. These results could serve as reference for the study of ionosphere distribution and construction of the corresponding profile model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820017701&hterms=time+series+forecasting&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtime%2Bseries%2Bforecasting','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820017701&hterms=time+series+forecasting&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtime%2Bseries%2Bforecasting"><span>Spatial and Temporal <span class="hlt">scales</span> of time-averaged 700 MB <span class="hlt">height</span> anomalies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gutzler, D.</p> <p>1981-01-01</p> <p>The monthly and seasonal forecasting technique is based to a large extent on the extrapolation of trends in the positions of the centers of time averaged geopotential <span class="hlt">height</span> anomalies. The complete forecasted <span class="hlt">height</span> pattern is subsequently drawn around the forecasted anomaly centers. The efficacy of this technique was tested and time series of observed monthly mean and 5 day mean 700 mb geopotential <span class="hlt">heights</span> were examined. Autocorrelation statistics are generated to document the tendency for persistence of anomalies. These statistics are compared to a red noise hypothesis to check for evidence of possible preferred time <span class="hlt">scales</span> of persistence. Space-time spectral analyses at middle latitudes are checked for evidence of periodicities which could be associated with predictable month-to-month trends. A local measure of the average spatial <span class="hlt">scale</span> of anomalies is devised for guidance in the completion of the anomaly pattern around the forecasted centers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020023967&hterms=MPL&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DMPL','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020023967&hterms=MPL&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DMPL"><span><span class="hlt">Aerosol</span> Measurements by the Globally Distributed Micro Pulse Lidar Network</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spinhirne, James; Welton, Judd; Campbell, James; Berkoff, Tim; Starr, David (Technical Monitor)</p> <p>2001-01-01</p> <p>Full time measurements of the vertical distribution of <span class="hlt">aerosol</span> are now being acquired at a number of globally distributed MP (micro pulse) lidar sites. The MP lidar systems provide full time profiling of all significant cloud and <span class="hlt">aerosol</span> to the limit of signal attenuation from compact, eye safe instruments. There are currently eight sites in operation and over a dozen planned. At all sited there are also passive <span class="hlt">aerosol</span> and radiation measurements supporting the lidar data. Four of the installations are at Atmospheric Radiation Measurement program sites. The network operation includes instrument operation and calibration and the processing of <span class="hlt">aerosol</span> measurements with standard retrievals and data products from the network sites. Data products include optical thickness and extinction cross section profiles. Application of data is to supplement satellite <span class="hlt">aerosol</span> measurements and to provide a climatology of the <span class="hlt">height</span> distribution of <span class="hlt">aerosol</span>. The <span class="hlt">height</span> distribution of <span class="hlt">aerosol</span> is important for <span class="hlt">aerosol</span> transport and the direct scattering and absorption of shortwave radiation in the atmosphere. Current satellite and other data already provide a great amount of information on <span class="hlt">aerosol</span> distribution, but no passive technique can adequately resolve the <span class="hlt">height</span> profile of <span class="hlt">aerosol</span>. The Geoscience Laser Altimeter System (GLAS) is an orbital lidar to be launched in early 2002. GLAS will provide global measurements of the <span class="hlt">height</span> distribution of <span class="hlt">aerosol</span>. The MP lidar network will provide ground truth and analysis support for GLAS and other NASA Earth Observing System data. The instruments, sites, calibration procedures and standard data product algorithms for the MPL network will be described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT........28D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT........28D"><span>Connecting Water Quality With Air Quality Through Microbial <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dueker, M. Elias</p> <p></p> <p><span class="hlt">Aerosol</span> production from surface waters results in the transfer of aquatic materials (including nutrients and bacteria) to air. These materials can then be transported by onshore winds to land, representing a biogeochemical connection between aquatic and terrestrial systems not normally considered. In urban waterfront environments, this transfer could result in emissions of pathogenic bacteria from contaminated waters. Despite the potential importance of this link, sources, near-shore deposition, identity and viability of microbial <span class="hlt">aerosols</span> are largely uncharacterized. This dissertation focuses on the environmental and biological mechanisms that define this water-air connection, as a means to build our understanding of the biogeochemical, biogeographical, and public health implications of the transfer of surface water materials to the near-shore environment in both urban and non-urban environments. The effects of tidal <span class="hlt">height</span>, wind speed and fog on coastal <span class="hlt">aerosols</span> and microbial content were first quantified on a non-urban coast of Maine, USA. Culture-based, culture-independent, and molecular methods were used to simultaneously sample microbial <span class="hlt">aerosols</span> while monitoring meteorological parameters. <span class="hlt">Aerosols</span> at this site displayed clear marine influence and high concentrations of ecologically-relevant nutrients. Coarse <span class="hlt">aerosol</span> concentrations significantly increased with tidal <span class="hlt">height</span>, onshore wind speed, and fog presence. Tidal <span class="hlt">height</span> and fog presence did not significantly influence total microbial <span class="hlt">aerosol</span> concentrations, but did have a significant effect on culturable microbial <span class="hlt">aerosol</span> fallout. Molecular analyses of the microbes settling out of near-shore <span class="hlt">aerosols</span> provided further evidence of local ocean to terrestrial transport of microbes. <span class="hlt">Aerosol</span> and surface ocean bacterial communities shared species and in general were dominated by organisms previously sampled in marine environments. Fog presence strengthened the microbial connection between water and land through</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AtmEn.145..135C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AtmEn.145..135C"><span>Impact of meteorology on fine <span class="hlt">aerosols</span> at Lucas <span class="hlt">Heights</span>, Australia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crawford, Jagoda; Chambers, Scott; Cohen, David D.; Williams, Alastair; Griffiths, Alan; Stelcer, Eduard; Dyer, Leisa</p> <p>2016-11-01</p> <p>Ion Beam Analysis (IBA) techniques were used to assign nine years of PM2.5 observations to seven source types, at Lucas <span class="hlt">Heights</span>, a topographically complex urban fringe site of Sydney. The highest contributions to total PM2.5 were from motor vehicles (Autos, 26.3%), secondary sulfur (2ndryS, 23.7%), a mixture of industry and aged sea air (IndSaged, 20.6%), and smoke (Smoke, 13.7%). The Autos contribution was highest in winter, whereas 2ndryS was highest in summer, indicating that mitigation measures targeting SO2 release in summer and vehicle exhaust in winter would be most effective in reducing the PM2.5 concentrations at this site. Since concentrations of particulate matter can be significantly affected by local meteorology, generalised additive model (GAM) techniques were employed to investigate relationships between PM2.5 source types and meteorological conditions. The GAM predictors used included: time (seasonal to inter-annual variations), mixing layer depth, temperature, relative humidity, wind speed, wind direction, and atmospheric pressure. Meteorological influences on PM2.5 variability were found to be 58% for soil dust, 46% for Autos, 41% for total PM2.5, and 35% for 2ndryS. Effects were much smaller for other source types. Temperature was found to be an important variable for the determination of total PM2.5, 2ndryS, IndSaged, Soil and Smoke, indicating that future changes in temperature are likely to have an associated change in <span class="hlt">aerosol</span> concentrations. However, the impact on different source types varied. Temperature had the highest impact on 2ndryS (sometimes more than a factor of 4 increase for temperatures above 25 °C compared to temperatures under 10 °C) and IndSaged, being predominantly secondary <span class="hlt">aerosols</span> formed in the atmosphere from precursors, whereas wind speed and wind direction were more important for the determination of vehicle exhaust and fresh sea salt concentrations. The marginal effect of relative humidity on 2ndryS increased up to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003268&hterms=meteorology&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmeteorology','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003268&hterms=meteorology&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmeteorology"><span><span class="hlt">Aerosol</span> Meteorology of Maritime Continent for the 2012 7SEAS Southwest Monsoon Intensive Study - Part 2: Philippine Receptor Observations of Fine-<span class="hlt">Scale</span> <span class="hlt">Aerosol</span> Behavior</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reid, Jeffrey S.; Lagrosas, Nofel D.; Jonsson, Haflidi H.; Reid, Elizabeth A.; Atwood, Samuel A.; Boyd, Thomas J.; Ghate, Virendra P.; Xian, Peng; Posselt, Derek J.; Simpas, James B.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003268'); toggleEditAbsImage('author_20170003268_show'); toggleEditAbsImage('author_20170003268_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003268_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003268_hide"></p> <p>2016-01-01</p> <p>The largest 7 Southeast Asian Studies (7SEAS) operations period within the Maritime Continent (MC) occurred in the August-September 2012 biomass burning season. Data included were observations aboard the MY Vasco, dispatched to the Palawan Archipelago and Sulu Sea of the Philippines for September 2012. At these locations, the Vasco observed MC smoke and pollution entering the southwest monsoon (SWM) monsoonal trough. Here we describe the research cruise findings and the finer-<span class="hlt">scale</span> <span class="hlt">aerosol</span> meteorology of this convectively active region. This 2012 cruise complemented a 2-week cruise in 2011 and was generally consistent with previous findings in terms of how smoke emission and transport related to monsoonal flows, tropical cyclones (TC), and the covariance between smoke transport events and the atmosphere's thermodynamic structure. Biomass burning plumes were usually mixed with significant amounts of anthropogenic pollution. Also key to <span class="hlt">aerosol</span> behavior were squall lines and cold pools propagating across the South China Sea (SCS) and scavenging <span class="hlt">aerosol</span> particles in their path. However, the 2012 cruise showed much higher modulation in <span class="hlt">aerosol</span> frequency than its 2011 counterpart. Whereas in 2011 large synoptic-<span class="hlt">scale</span> <span class="hlt">aerosol</span> events transported high concentrations of smoke into the Philippines over days, in 2012 measured <span class="hlt">aerosol</span> events exhibited a much shorter-term variation, sometimes only 312h. Strong monsoonal flow reversals were also experienced in 2012. Nucleation events in cleaner and polluted conditions, as well as in urban plumes, were observed. Perhaps most interestingly, several cases of squall lines preceding major <span class="hlt">aerosol</span> events were observed, as opposed to 2011 observations where these lines largely scavenged <span class="hlt">aerosol</span> particles from the marine boundary layer. Combined, these observations indicate pockets of high and low particle counts that are not uncommon in the region. These perturbations are difficult to observe by satellite and very difficult to model</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....1614057R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....1614057R"><span><span class="hlt">Aerosol</span> meteorology of Maritime Continent for the 2012 7SEAS southwest monsoon intensive study - Part 2: Philippine receptor observations of fine-<span class="hlt">scale</span> <span class="hlt">aerosol</span> behavior</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reid, Jeffrey S.; Lagrosas, Nofel D.; Jonsson, Haflidi H.; Reid, Elizabeth A.; Atwood, Samuel A.; Boyd, Thomas J.; Ghate, Virendra P.; Xian, Peng; Posselt, Derek J.; Simpas, James B.; Uy, Sherdon N.; Zaiger, Kimo; Blake, Donald R.; Bucholtz, Anthony; Campbell, James R.; Chew, Boon Ning; Cliff, Steven S.; Holben, Brent N.; Holz, Robert E.; Hyer, Edward J.; Kreidenweis, Sonia M.; Kuciauskas, Arunas P.; Lolli, Simone; Oo, Min; Perry, Kevin D.; Salinas, Santo V.; Sessions, Walter R.; Smirnov, Alexander; Walker, Annette L.; Wang, Qing; Yu, Liya; Zhang, Jianglong; Zhao, Yongjing</p> <p>2016-11-01</p> <p>The largest 7 Southeast Asian Studies (7SEAS) operations period within the Maritime Continent (MC) occurred in the August-September 2012 biomass burning season. Data included were observations aboard the M/Y Vasco, dispatched to the Palawan Archipelago and Sulu Sea of the Philippines for September 2012. At these locations, the Vasco observed MC smoke and pollution entering the southwest monsoon (SWM) monsoonal trough. Here we describe the research cruise findings and the finer-<span class="hlt">scale</span> <span class="hlt">aerosol</span> meteorology of this convectively active region. This 2012 cruise complemented a 2-week cruise in 2011 and was generally consistent with previous findings in terms of how smoke emission and transport related to monsoonal flows, tropical cyclones (TC), and the covariance between smoke transport events and the atmosphere's thermodynamic structure. Biomass burning plumes were usually mixed with significant amounts of anthropogenic pollution. Also key to <span class="hlt">aerosol</span> behavior were squall lines and cold pools propagating across the South China Sea (SCS) and scavenging <span class="hlt">aerosol</span> particles in their path. However, the 2012 cruise showed much higher modulation in <span class="hlt">aerosol</span> frequency than its 2011 counterpart. Whereas in 2011 large synoptic-<span class="hlt">scale</span> <span class="hlt">aerosol</span> events transported high concentrations of smoke into the Philippines over days, in 2012 measured <span class="hlt">aerosol</span> events exhibited a much shorter-term variation, sometimes only 3-12 h. Strong monsoonal flow reversals were also experienced in 2012. Nucleation events in cleaner and polluted conditions, as well as in urban plumes, were observed. Perhaps most interestingly, several cases of squall lines preceding major <span class="hlt">aerosol</span> events were observed, as opposed to 2011 observations where these lines largely scavenged <span class="hlt">aerosol</span> particles from the marine boundary layer. Combined, these observations indicate pockets of high and low particle counts that are not uncommon in the region. These perturbations are difficult to observe by satellite and very difficult to model</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710651S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710651S"><span><span class="hlt">Scale</span> <span class="hlt">Height</span> variations with solar cycle in the ionosphere of Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sanchez-Cano, Beatriz; Lester, Mark; Witasse, Olivier; Milan, Stephen E.; Hall, Benjamin E. S.; Cartacci, Marco; Radicella, Sandro M.; Blelly, Pierre-Louis</p> <p>2015-04-01</p> <p>The Mars Advanced Radar for Subsurface and Ionospheric Sounding (MARSIS) on board the Mars Express spacecraft has been probing the topside of the ionosphere of Mars since June 2005, covering currently almost one solar cycle. A good knowledge of the behaviour of the ionospheric variability for a whole solar period is essential since the ionosphere is strongly dependent on solar activity. Using part of this dataset, covering the years 2005 - 2012, differences in the shape of the topside electron density profiles have been observed. These variations seem to be linked to changes in the ionospheric temperature due to the solar cycle variation. In particular, Mars' ionospheric response to the extreme solar minimum between end-2007 and end-2009 followed a similar pattern to the response observed in the Earth's ionosphere, despite the large differences related to internal origin of the magnetic field between both planets. Plasma parameters such as the <span class="hlt">scale</span> <span class="hlt">height</span> as a function of altitude, the main peak characteristics (altitude, density), the total electron content (TEC), the temperatures, and the ionospheric thermal pressures show variations related to the solar cycle. The main changes in the topside ionosphere are detected during the period of very low solar minimum, when ionospheric cooling occurs. The effect on the <span class="hlt">scale</span> <span class="hlt">height</span> is analysed in detail. In contrast, a clear increase of the <span class="hlt">scale</span> <span class="hlt">height</span> is observed during the high solar activity period due to enhanced ionospheric heating. The <span class="hlt">scale</span> <span class="hlt">height</span> variation during the solar cycle has been empirically modelled. The results have been compared with other datasets such as radio-occultation and retarding potential analyser data from old missions, especially in low solar activity periods (e.g. Mariner 4, Viking 1 and 2 landers), as well as with numerical modelling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A33A..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A33A..07L"><span>Sea-State Dependence of <span class="hlt">Aerosol</span> Concentration in the Marine Atmospheric Boundary Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lenain, L.; Melville, W. K.</p> <p>2016-02-01</p> <p>While sea spray <span class="hlt">aerosols</span> represent a large portion of the <span class="hlt">aerosols</span> present in the marine environment, and despite evidence of the importance of surface wave and wave-breaking related processes in the coupling of the ocean with the atmosphere, sea spray source generation functions are traditionally parameterized by the wind speed at 10m. It is clear that unless the wind and wave field are fully developed, the source function will be a function of both wind and wave parameters. In this study, we report on an air-sea interaction experiment, the ONR phase-resolved High-Resolution Air-Sea Interaction experiments (HIRES), conducted off the coast of Northern California in June 2010. Detailed measurements of <span class="hlt">aerosol</span> number concentration in the Marine Atmospheric Boundary Layer (MABL), at altitudes ranging from as low as 30m and up to 800m AMSL over a broad range of environmental conditions (significant wave <span class="hlt">height</span>, Hs, of 2 to 4.5m and wind speed at 10m <span class="hlt">height</span>, U10, of 10 to 18 m/s) collected from an instrumented research aircraft, are presented. <span class="hlt">Aerosol</span> number densities and volume are computed over a range of particle diameters from 0.1 to 200 µm, while the surface conditions, i.e. significant wave <span class="hlt">height</span>, moments of the breaker length distribution Λ(c), and wave breaking dissipation, were measured by a suite of electro-optical sensors that included the NASA Airborne Topographic Mapper (ATM). The sea-state dependence of the <span class="hlt">aerosol</span> concentration in the MABL is evident, ultimately stressing the need to incorporate wave and wave kinematics in the spray source generation functions that are traditionally primarily parameterized by surface winds. A <span class="hlt">scaling</span> of the measured <span class="hlt">aerosol</span> volume distribution by wave and atmospheric state variables is proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.3119M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.3119M"><span><span class="hlt">Aerosol</span>-cloud interactions in mixed-phase convective clouds - Part 1: <span class="hlt">Aerosol</span> perturbations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miltenberger, Annette K.; Field, Paul R.; Hill, Adrian A.; Rosenberg, Phil; Shipway, Ben J.; Wilkinson, Jonathan M.; Scovell, Robert; Blyth, Alan M.</p> <p>2018-03-01</p> <p>Changes induced by perturbed <span class="hlt">aerosol</span> conditions in moderately deep mixed-phase convective clouds (cloud top <span class="hlt">height</span> ˜ 5 km) developing along sea-breeze convergence lines are investigated with high-resolution numerical model simulations. The simulations utilise the newly developed Cloud-AeroSol Interacting Microphysics (CASIM) module for the Unified Model (UM), which allows for the representation of the two-way interaction between cloud and <span class="hlt">aerosol</span> fields. Simulations are evaluated against observations collected during the COnvective Precipitation Experiment (COPE) field campaign over the southwestern peninsula of the UK in 2013. The simulations compare favourably with observed thermodynamic profiles, cloud base cloud droplet number concentrations (CDNC), cloud depth, and radar reflectivity statistics. Including the modification of <span class="hlt">aerosol</span> fields by cloud microphysical processes improves the correspondence with observed CDNC values and spatial variability, but reduces the agreement with observations for average cloud size and cloud top <span class="hlt">height</span>. Accumulated precipitation is suppressed for higher-<span class="hlt">aerosol</span> conditions before clouds become organised along the sea-breeze convergence lines. Changes in precipitation are smaller in simulations with <span class="hlt">aerosol</span> processing. The precipitation suppression is due to less efficient precipitation production by warm-phase microphysics, consistent with parcel model predictions. In contrast, after convective cells organise along the sea-breeze convergence zone, accumulated precipitation increases with <span class="hlt">aerosol</span> concentrations. Condensate production increases with the <span class="hlt">aerosol</span> concentrations due to higher vertical velocities in the convective cores and higher cloud top <span class="hlt">heights</span>. However, for the highest-<span class="hlt">aerosol</span> scenarios, no further increase in the condensate production occurs, as clouds grow into an upper-level stable layer. In these cases, the reduced precipitation efficiency (PE) dominates the precipitation response and no further</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1232651','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1232651"><span>Holistic Interactions of Shallow Clouds, <span class="hlt">Aerosols</span>, and Land-Ecosystems (HI-<span class="hlt">SCALE</span>) Science Plan</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>Fast, JD; Berg, LK</p> <p></p> <p>Cumulus convection is an important component in the atmospheric radiation budget and hydrologic cycle over the Southern Great Plains and over many regions of the world, particularly during the summertime growing season when intense turbulence induced by surface radiation couples the land surface to clouds. Current convective cloud parameterizations contain uncertainties resulting in part from insufficient coincident data that couples cloud macrophysical and microphysical properties to inhomogeneities in boundary layer and <span class="hlt">aerosol</span> properties. The Holistic Interactions of Shallow Clouds, <span class="hlt">Aerosols</span>, and Land-Ecosystems (HI-<span class="hlt">SCALE</span>) campaign is designed to provide a detailed set of measurements that are needed to obtain a moremore » complete understanding of the life cycle of shallow clouds by coupling cloud macrophysical and microphysical properties to land surface properties, ecosystems, and <span class="hlt">aerosols</span>. HI-<span class="hlt">SCALE</span> consists of 2, 4-week intensive observational periods, one in the spring and the other in the late summer, to take advantage of different stages and distribution of “greenness” for various types of vegetation in the vicinity of the Atmospheric Radiation and Measurement (ARM) Climate Research Facility’s Southern Great Plains (SGP) site as well as <span class="hlt">aerosol</span> properties that vary during the growing season. Most of the proposed instrumentation will be deployed on the ARM Aerial Facility (AAF) Gulfstream 1 (G-1) aircraft, including those that measure atmospheric turbulence, cloud water content and drop size distributions, <span class="hlt">aerosol</span> precursor gases, <span class="hlt">aerosol</span> chemical composition and size distributions, and cloud condensation nuclei concentrations. Routine ARM <span class="hlt">aerosol</span> measurements made at the surface will be supplemented with <span class="hlt">aerosol</span> microphysical properties measurements. The G-1 aircraft will complete transects over the SGP Central Facility at multiple altitudes within the boundary layer, within clouds, and above clouds.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE10226E..0YP','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE10226E..0YP"><span>Lidar measurements of wildfire smoke <span class="hlt">aerosols</span> in the atmosphere above Sofia, Bulgaria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peshev, Zahary Y.; Deleva, Atanaska D.; Dreischuh, Tanja N.; Stoyanov, Dimitar V.</p> <p>2016-01-01</p> <p>Presented are results of lidar measurements and characterization of wildfire caused smoke <span class="hlt">aerosols</span> observed in the atmosphere above the city of Sofia, Bulgaria, related to two local wildfires raging in forest areas near the city. A lidar systems based on a frequency-doubled Nd:YAG laser operated at 532 nm and 1064 nm is used in the smoke <span class="hlt">aerosol</span> observations. It belongs to the Sofia LIDAR Station (at Laser Radars Laboratory, Institute of Electronics, Bulgarian Academy of Sciences), being a part of the European <span class="hlt">Aerosol</span> Lidar Network. Optical, dynamical, microphysical, and geometrical properties and parameters of the observed smoke <span class="hlt">aerosol</span> particles and layers are displayed and analyzed, such as: range/<span class="hlt">height</span>-resolved profiles of the <span class="hlt">aerosol</span> backscatter coefficient; integral <span class="hlt">aerosol</span> backscattering; sets of colormaps displaying time series of the <span class="hlt">height</span> distribution of the <span class="hlt">aerosol</span> density; topologic, geometric, and volumetric properties of the smoke <span class="hlt">aerosol</span> layers; time-averaged <span class="hlt">height</span> profiles of backscatter-related Ångström exponent (BAE). Obtained results of retrieving and profiling smoke <span class="hlt">aerosols</span> are commented in their relations to available meteorological and air-mass-transport forecasting and modelling data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040141567&hterms=devices+eye&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddevices%2Beye','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040141567&hterms=devices+eye&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddevices%2Beye"><span>Eye <span class="hlt">height</span> <span class="hlt">scaling</span> of absolute size in immersive and nonimmersive displays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dixon, M. W.; Wraga, M.; Proffitt, D. R.; Williams, G. C.; Kaiser, M. K. (Principal Investigator)</p> <p>2000-01-01</p> <p>Eye-<span class="hlt">height</span> (EH) <span class="hlt">scaling</span> of absolute <span class="hlt">height</span> was investigated in three experiments. In Experiment 1, standing observers viewed cubes in an immersive virtual environment. Observers' center of projection was placed at actual EH and at 0.7 times actual EH. Observers' size judgments revealed that the EH manipulation was 76.8% effective. In Experiment 2, seated observers viewed the same cubes on an interactive desktop display; however, no effect of EH was found in response to the simulated EH manipulation. Experiment 3 tested standing observers in the immersive environment with the field of view reduced to match that of the desktop. Comparable to Experiment 1, the effect of EH was 77%. These results suggest that EH <span class="hlt">scaling</span> is not generally used when people view an interactive desktop display because the altitude of the center of projection is indeterminate. EH <span class="hlt">scaling</span> is spontaneously evoked, however, in immersive environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7033854-relationship-between-fluid-bed-aerosol-generator-operation-aerosol-produced','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7033854-relationship-between-fluid-bed-aerosol-generator-operation-aerosol-produced"><span>Relationship between fluid bed <span class="hlt">aerosol</span> generator operation and the <span class="hlt">aerosol</span> produced</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>Carpenter, R.L.; Yerkes, K.</p> <p>1980-12-01</p> <p>The relationships between bed operation in a fluid bed <span class="hlt">aerosol</span> generator and <span class="hlt">aerosol</span> output were studied. A two-inch diameter fluid bed <span class="hlt">aerosol</span> generator (FBG) was constructed using stainless steel powder as a fluidizing medium. Fly ash from coal combustion was <span class="hlt">aerosolized</span> and the influence of FBG operating parameters on <span class="hlt">aerosol</span> mass median aerodynamic diameter (MMAD), geometric standard deviation (sigma/sub g/) and concentration was examined. In an effort to extend observations on large fluid beds to small beds using fine bed particles, minimum fluidizing velocities and elutriation constant were computed. Although FBG minimum fluidizing velocity agreed well with calculations, FBG elutriationmore » constant did not. The results of this study show that the properties of <span class="hlt">aerosols</span> produced by a FBG depend on fluid bed <span class="hlt">height</span> and air flow through the bed after the minimum fluidizing velocity is exceeded.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800015419','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800015419"><span>Shuttle program: Computing atmospheric <span class="hlt">scale</span> <span class="hlt">height</span> for refraction corrections</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lear, W. M.</p> <p>1980-01-01</p> <p>Methods for computing the atmospheric <span class="hlt">scale</span> <span class="hlt">height</span> to determine radio wave refraction were investigated for different atmospheres, and different angles of elevation. Tables of refractivity versus altitude are included. The equations used to compute the refraction corrections are given. It is concluded that very accurate corrections are determined with the assumption of an exponential atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1392040-aerosol-meteorology-maritime-continent-southwest-monsoon-intensive-study-part-philippine-receptor-observations-fine-scale-aerosol-behavior','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1392040-aerosol-meteorology-maritime-continent-southwest-monsoon-intensive-study-part-philippine-receptor-observations-fine-scale-aerosol-behavior"><span><span class="hlt">Aerosol</span> meteorology of Maritime Continent for the 2012 7SEAS southwest monsoon intensive study – Part 2: Philippine receptor observations of fine-<span class="hlt">scale</span> <span class="hlt">aerosol</span> behavior</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>Reid, Jeffrey S.; Lagrosas, Nofel D.; Jonsson, Haflidi H.</p> <p></p> <p>The largest 7 Southeast Asian Studies (7SEAS) operations period within the Maritime Continent (MC) occurred in the August–September 2012 biomass burning season. Data included were observations aboard the M/Y Vasco, dispatched to the Palawan Archipelago and Sulu Sea of the Philippines for September 2012. At these locations, the Vasco observed MC smoke and pollution entering the southwest monsoon (SWM) monsoonal trough. Here we describe the research cruise findings and the finer-<span class="hlt">scale</span> <span class="hlt">aerosol</span> meteorology of this convectively active region. This 2012 cruise complemented a 2-week cruise in 2011 and was generally consistent with previous findings in terms of how smoke emission and transportmore » related to monsoonal flows, tropical cyclones (TC), and the covariance between smoke transport events and the atmosphere's thermodynamic structure. Biomass burning plumes were usually mixed with significant amounts of anthropogenic pollution. Also key to <span class="hlt">aerosol</span> behavior were squall lines and cold pools propagating across the South China Sea (SCS) and scavenging <span class="hlt">aerosol</span> particles in their path. However, the 2012 cruise showed much higher modulation in <span class="hlt">aerosol</span> frequency than its 2011 counterpart. Whereas in 2011 large synoptic-<span class="hlt">scale</span> <span class="hlt">aerosol</span> events transported high concentrations of smoke into the Philippines over days, in 2012 measured <span class="hlt">aerosol</span> events exhibited a much shorter-term variation, sometimes only 3$-$12 h. Strong monsoonal flow reversals were also experienced in 2012. Nucleation events in cleaner and polluted conditions, as well as in urban plumes, were observed. Perhaps most interestingly, several cases of squall lines preceding major <span class="hlt">aerosol</span> events were observed, as opposed to 2011 observations where these lines largely scavenged <span class="hlt">aerosol</span> particles from the marine boundary layer. Combined, these observations indicate pockets of high and low particle counts that are not uncommon in the region. These perturbations are difficult to observe by satellite and very</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A42C..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A42C..02S"><span>CALIOP-based Biomass Burning Smoke Plume Injection <span class="hlt">Height</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Soja, A. J.; Choi, H. D.; Fairlie, T. D.; Pouliot, G.; Baker, K. R.; Winker, D. M.; Trepte, C. R.; Szykman, J.</p> <p>2017-12-01</p> <p>Carbon and <span class="hlt">aerosols</span> are cycled between terrestrial and atmosphere environments during fire events, and these emissions have strong feedbacks to near-field weather, air quality, and longer-term climate systems. Fire severity and burned area are under the control of weather and climate, and fire emissions have the potential to alter numerous land and atmospheric processes that, in turn, feedback to and interact with climate systems (e.g., changes in patterns of precipitation, black/brown carbon deposition on ice/snow, alteration in landscape and atmospheric/cloud albedo). If plume injection <span class="hlt">height</span> is incorrectly estimated, then the transport and deposition of those emissions will also be incorrect. The <span class="hlt">heights</span> to which smoke is injected governs short- or long-range transport, which influences surface pollution, cloud interaction (altered albedo), and modifies patterns of precipitation (cloud condensation nuclei). We are working with the Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) science team and other stakeholder agencies, primarily the Environmental Protection Agency and regional partners, to generate a biomass burning (BB) plume injection <span class="hlt">height</span> database using multiple platforms, sensors and models (CALIOP, MODIS, NOAA HMS, Langley Trajectory Model). These data have the capacity to provide enhanced smoke plume injection <span class="hlt">height</span> parameterization in regional, national and international scientific and air quality models. Statistics that link fire behavior and weather to plume rise are crucial for verifying and enhancing plume rise parameterization in local-, regional- and global-<span class="hlt">scale</span> models used for air quality, chemical transport and climate. Specifically, we will present: (1) a methodology that links BB injection <span class="hlt">height</span> and CALIOP air parcels to specific fires; (2) the daily evolution of smoke plumes for specific fires; (3) plumes transport and deposited on the Greenland Ice Sheet; and (4) compare CALIOP-derived smoke plume injection</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120003726','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120003726"><span>Assessing Impact of <span class="hlt">Aerosol</span> Intercontinental Transport on Regional Air Quality and Climate: What Satellites Can Help</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, Hongbin</p> <p>2011-01-01</p> <p>Mounting evidence for intercontinental transport of <span class="hlt">aerosols</span> suggests that <span class="hlt">aerosols</span> from a region could significantly affect climate and air quality in downwind regions and continents. Current assessment of these impacts for the most part has been based on global model simulations that show large variability. The <span class="hlt">aerosol</span> intercontinental transport and its influence on air quality and climate involve many processes at local, regional, and intercontinental <span class="hlt">scales</span>. There is a pressing need to establish modeling systems that bridge the wide range of <span class="hlt">scales</span>. The modeling systems need to be evaluated and constrained by observations, including satellite measurements. Columnar loadings of dust and combustion <span class="hlt">aerosols</span> can be derived from the MODIS and MISR measurements of total <span class="hlt">aerosol</span> optical depth and particle size and shape information. Characteristic transport <span class="hlt">heights</span> of dust and combustion <span class="hlt">aerosols</span> can be determined from the CALIPSO lidar and AIRS measurements. CALIPSO liar and OMI UV technique also have a unique capability of detecting <span class="hlt">aerosols</span> above clouds, which could offer some insights into <span class="hlt">aerosol</span> lofting processes and the importance of above-cloud transport pathway. In this presentation, I will discuss our efforts of integrating these satellite measurements and models to assess the significance of intercontinental transport of dust and combustion <span class="hlt">aerosols</span> on regional air quality and climate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1354732','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1354732"><span>Holistic Interactions of Shallow Clouds, <span class="hlt">Aerosols</span>, and Land-Ecosystems (HI-<span class="hlt">SCALE</span>) Field Campaign Report</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>Fast, J. D.; Berg, L. K.; Burleyson, C.</p> <p></p> <p>Cumulus convection is an important component in the atmospheric radiation budget and hydrologic cycle over the southern Great Plains and over many regions of the world, particularly during the summertime growing season when intense turbulence induced by surface radiation couples the land surface to clouds. Current convective cloud parameterizations contain uncertainties resulting in part from insufficient coincident data that couples cloud macrophysical and microphysical properties to inhomogeneities in land surface, boundary layer, and <span class="hlt">aerosol</span> properties. The Holistic Interactions of Shallow Clouds, <span class="hlt">Aerosols</span>, and Land-Ecosystems (HI-<span class="hlt">SCALE</span>) campaign was designed to provide a detailed set of measurements that are needed to obtainmore » a more complete understanding of the lifecycle of shallow clouds by coupling cloud macrophysical and microphysical properties to land surface properties, ecosystems, and <span class="hlt">aerosols</span>. Some of the land-atmosphere-cloud interactions that can be studied using HI-<span class="hlt">SCALE</span> data are shown in Figure 1. HI-<span class="hlt">SCALE</span> consisted of two 4-week intensive operation periods (IOPs), one in the spring (April 24-May 21) and the other in the late summer (August 28-September 24) of 2016, to take advantage of different stages of the plant lifecycle, the distribution of “greenness” for various types of vegetation in the vicinity of the U.S. Department of Energy (DOE) Atmospheric Radiation Measurement (ARM) Climate Research Facility Southern Great Plains (SGP) site, and <span class="hlt">aerosol</span> properties that vary during the growing season. As expected, satellite measurements indicated that the Normalized Difference Vegetation Index (NDVI) was much “greener” in the vicinity of the SGP site during the spring IOP than the late summer IOP as a result of winter wheat maturing in the spring and being harvested in the early summer. As shown in Figure 2, temperatures were cooler than average and soil moisture was high during the spring IOP, while temperatures were warmer than</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25569495','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25569495"><span>Comparison of suction device with saliva ejector for <span class="hlt">aerosol</span> and spatter reduction during ultrasonic <span class="hlt">scaling</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Holloman, Jessica L; Mauriello, Sally M; Pimenta, Luiz; Arnold, Roland R</p> <p>2015-01-01</p> <p><span class="hlt">Aerosols</span> and spatter are concerns in health care owing to their potential adverse health effects. The Isolite illuminated isolation system (Isolite Systems) and a saliva ejector were compared for <span class="hlt">aerosol</span> and spatter reduction during and after ultrasonic <span class="hlt">scaling</span>. Fifty participants were randomized to control (n = 25, saliva ejector) or test (n = 25, Isolite) groups and received a prophylaxis with an ultrasonic scaler. <span class="hlt">Aerosols</span> were collected in a petri dish containing transport media, dispersed, and plated to anaerobic blood agar to determine colony-forming units (CFUs). The authors analyzed the data using a t test. No significant difference occurred between groups in <span class="hlt">aerosol</span> and spatter reduction (P = .25). Mean (standard deviation) of log10 CFUs per milliliter collected during ultrasonic <span class="hlt">scaling</span> in the control and test groups were 3.61 (0.95) and 3.30 (0.88), respectively. All samples contained α-hemolytic streptococci, and many samples contained strictly oral anaerobes. A significant amount of contamination occurred during ultrasonic <span class="hlt">scaling</span> in both groups, as indicated by high numbers of CFUs and the identification of strictly oral anaerobes in all plates. Neither device reduced <span class="hlt">aerosols</span> and spatter effectively, and there was no significant difference in reduction between the 2 devices. Additional measures should be taken with these devices to reduce the likelihood of disease transmission. Copyright © 2015 American Dental Association. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308468&keyword=Scheme&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=308468&keyword=Scheme&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>Introducing Subgrid-<span class="hlt">scale</span> convective cloud and <span class="hlt">aerosol</span> interactions to the WRF-CMAQ integrated modeling system</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>Many regional and global climate models include <span class="hlt">aerosol</span> indirect effects (AIE) on grid-<span class="hlt">scale</span>/resolved clouds. However, the interaction between <span class="hlt">aerosols</span> and convective clouds remains highly uncertain, as noted in the IPCC AR4 report. The objective of this work is to help fill in ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25411280','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25411280"><span><span class="hlt">Scaling</span> of adult body weight to <span class="hlt">height</span> across sex and race/ethnic groups: relevance to BMI.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heymsfield, Steven B; Peterson, Courtney M; Thomas, Diana M; Heo, Moonseong; Schuna, John M; Hong, Sangmo; Choi, Woong</p> <p>2014-12-01</p> <p>Body mass index (BMI) is formulated on the assumption that body weight (BW) <span class="hlt">scales</span> to <span class="hlt">height</span> with a power of 2 (BW∝<span class="hlt">height</span>(2)), independent of sex and race-ethnicity. Powers differing from 2 are observed in studies of selected samples, thus raising the question if BMI is a generalizable metric that makes BW independent of <span class="hlt">height</span> across populations. The objectives were to test the hypothesis that adult BW <span class="hlt">scales</span> to <span class="hlt">height</span> with a power of 2 independent of sex and race-ethnicity and to advance an understanding of BMI as a measure of shape by extending allometric analyses to waist circumference (WC). We conducted cross-sectional subject evaluations, including body composition, from the NHANES and the Korean NHANES (KNHANES). Variations of the allometric model (Y = αX(β)) were used to establish <span class="hlt">height</span> <span class="hlt">scaling</span> powers (β ± SE) across non-Hispanic white and black, Mexican American, and Korean men and women. Exploratory analyses in population samples established age and adiposity as important independent determinants of <span class="hlt">height</span> <span class="hlt">scaling</span> powers (i.e., β). After age and adiposity in the next series of analyses were controlled for, BW <span class="hlt">scaling</span> powers were nonsignificantly different between race/ethnic groups within each sex group; WC findings were similar in women, whereas small but significant between-race differences were observed in the men. Sex differences in β values were nonsignificant except for BW in non-Hispanic blacks and WC in Koreans (P < 0.05). Nationally representative powers for BW were (NHANES/KNHANES) 2.12 ± 0.05/2.11 ± 0.06 for men and 2.02 ± 0.04/1.99 ± 0.06 for women and for WC were 0.66 ± 0.03/0.67 ± 0.05 for men and 0.61 ± 0.04/0.56 ± 0.05 for women. Adult BW <span class="hlt">scales</span> to <span class="hlt">height</span> with a power of ∼2 across the 8 sex and race/ethnic groups, an observation that makes BMI a generalizable <span class="hlt">height</span>-independent measure of shape across most populations. WC also follows generalizable <span class="hlt">scaling</span> rules, a finding that has implications for defining body shape in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRA..121.5675W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRA..121.5675W"><span>Topside correction of IRI by global modeling of ionospheric <span class="hlt">scale</span> <span class="hlt">height</span> using COSMIC radio occultation data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, M. J.; Guo, P.; Fu, N. F.; Xu, T. L.; Xu, X. S.; Jin, H. L.; Hu, X. G.</p> <p>2016-06-01</p> <p>The ionosphere <span class="hlt">scale</span> <span class="hlt">height</span> is one of the most significant ionospheric parameters, which contains information about the ion and electron temperatures and dynamics in upper ionosphere. In this paper, an empirical orthogonal function (EOF) analysis method is applied to process all the ionospheric radio occultations of GPS/COSMIC (Constellation Observing System for Meteorology, Ionosphere, and Climate) from the year 2007 to 2011 to reconstruct a global ionospheric <span class="hlt">scale</span> <span class="hlt">height</span> model. This monthly medium model has spatial resolution of 5° in geomagnetic latitude (-87.5° ~ 87.5°) and temporal resolution of 2 h in local time. EOF analysis preserves the characteristics of <span class="hlt">scale</span> <span class="hlt">height</span> quite well in the geomagnetic latitudinal, anural, seasonal, and diurnal variations. In comparison with COSMIC measurements of the year of 2012, the reconstructed model indicates a reasonable accuracy. In order to improve the topside model of International Reference Ionosphere (IRI), we attempted to adopt the <span class="hlt">scale</span> <span class="hlt">height</span> model in the Bent topside model by applying a <span class="hlt">scale</span> factor q as an additional constraint. With the factor q functioning in the exponent profile of topside ionosphere, the IRI <span class="hlt">scale</span> <span class="hlt">height</span> should be forced equal to the precise COSMIC measurements. In this way, the IRI topside profile can be improved to get closer to the realistic density profiles. Internal quality check of this approach is carried out by comparing COSMIC realistic measurements and IRI with or without correction, respectively. In general, the initial IRI model overestimates the topside electron density to some extent, and with the correction introduced by COSMIC <span class="hlt">scale</span> <span class="hlt">height</span> model, the deviation of vertical total electron content (VTEC) between them is reduced. Furthermore, independent validation with Global Ionospheric Maps VTEC implies a reasonable improvement in the IRI VTEC with the topside model correction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020005893&hterms=sampling+distribution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsampling%2Bdistribution','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020005893&hterms=sampling+distribution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsampling%2Bdistribution"><span>Measurement of the Vertical Distribution of <span class="hlt">Aerosol</span> by Globally Distributed MP Lidar Network Sites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spinhirne, James; Welton, Judd; Campbell, James; Starr, David OC. (Technical Monitor)</p> <p>2001-01-01</p> <p>The global distribution of <span class="hlt">aerosol</span> has an important influence on climate through the scattering and absorption of shortwave radiation and through modification of cloud optical properties. Current satellite and other data already provide a great amount of information on <span class="hlt">aerosol</span> distribution. However there are critical parameters that can only be obtained by active optical profiling. For <span class="hlt">aerosol</span>, no passive technique can adequately resolve the <span class="hlt">height</span> profile of <span class="hlt">aerosol</span>. The <span class="hlt">aerosol</span> <span class="hlt">height</span> distribution is required for any model for <span class="hlt">aerosol</span> transport and the <span class="hlt">height</span> resolved radiative heating/cooling effect of <span class="hlt">aerosol</span>. The Geoscience Laser Altimeter System (GLAS) is an orbital lidar to be launched by 2002. GLAS will provide global measurements of the <span class="hlt">height</span> distribution of <span class="hlt">aerosol</span>. The sampling will be limited by nadir only coverage. There is a need for local sites to address sampling, and accuracy factors. Full time measurements of the vertical distribution of <span class="hlt">aerosol</span> are now being acquired at a number of globally distributed MP (micro pulse) lidar sites. The MP lidar systems provide profiling of all significant cloud and <span class="hlt">aerosol</span> to the limit of signal attenuation from compact, eye safe instruments. There are currently six sites in operation and over a dozen planned. At all sites there are a complement of passive <span class="hlt">aerosol</span> and radiation measurements supporting the lidar data. Four of the installations are at Atmospheric Radiation Measurement program sites. The <span class="hlt">aerosol</span> measurements, retrievals and data products from the network sites will be discussed. The current and planned application of data to supplement satellite <span class="hlt">aerosol</span> measurements is covered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A24F..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A24F..06G"><span>From Global to Cloud Resolving <span class="hlt">Scale</span>: Experiments with a <span class="hlt">Scale</span>- and <span class="hlt">Aerosol</span>-Aware Physics Package and Impact on Tracer Transport</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grell, G. A.; Freitas, S. R.; Olson, J.; Bela, M.</p> <p>2017-12-01</p> <p>We will start by providing a summary of the latest cumulus parameterization modeling efforts at NOAA's Earth System Research Laboratory (ESRL) will be presented on both regional and global <span class="hlt">scales</span>. The physics package includes a <span class="hlt">scale</span>-aware parameterization of subgrid cloudiness feedback to radiation (coupled PBL, microphysics, radiation, shallow and congestus type convection), the stochastic Grell-Freitas (GF) <span class="hlt">scale</span>- and <span class="hlt">aerosol</span>-aware convective parameterization, and an <span class="hlt">aerosol</span> aware microphysics package. GF is based on a stochastic approach originally implemented by Grell and Devenyi (2002) and described in more detail in Grell and Freitas (2014, ACP). It was expanded to include PDF's for vertical mass flux, as well as modifications to improve the diurnal cycle. This physics package will be used on different <span class="hlt">scales</span>, spanning global to cloud resolving, to look at the impact on scalar transport and numerical weather prediction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870000906','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870000906"><span>Observations of stratospheric <span class="hlt">aerosols</span> associated with the El Chichon eruption</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thomas, L.; Vaughan, G.; Jenkins, D. B.; Wareing, D.; Farrington, M.</p> <p>1986-01-01</p> <p>Lidar observations of <span class="hlt">aerosols</span> were carried out at Aberystwyth between Nov. 1982 and Dec. 1985 using a frequency doubled and frequency tripled Nd/Yag laser and a receiver incorporating a 1 m diameter in a Newtonian telescope configuration. In analyses of the experimental data attention is paid to the magnitude of the coefficient relating extinction and backscatter, the choice being related to the possible presence of <span class="hlt">aerosols</span> in the upper troposphere and the atmospheric densities employed in the normalisation procedure. The <span class="hlt">aerosol</span> loading showed marked day to day changes in early months and an overall decay was apparent only after April 1983, this decay being consistent with an e sup -1 time of about 7 months. The general decay was accompanied by a lowering of the layer but layers of <span class="hlt">aerosols</span> were shown intermittently at <span class="hlt">heights</span> above the main layer in winter months. The <span class="hlt">height</span> variations of photon counts corrected for range, or of <span class="hlt">aerosol</span> backscatter ratio, showed clear signatures of the tropopause. A strong correlation was found between the <span class="hlt">heights</span> of the tropopause identified from the lidar measurements and from radiosonde-borne temperature measurements. A notable feature of the observations is the appearance of very sharp <span class="hlt">height</span> gradients of backscatter ratio which seem to be produced by differential advection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.P24A..08S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.P24A..08S"><span>Vertical Distribution of <span class="hlt">Aerosols</span> and Water Vapor Using CRISM Limb Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, M. D.; Wolff, M. J.; Clancy, R. T.; CRISM Science; Operations Teams</p> <p>2011-12-01</p> <p>Near-infrared spectra taken in a limb-viewing geometry by the Compact Reconnaissance Imaging Spectrometer for Mars (CRISM) on-board the Mars Reconnaissance Orbiter (MRO) provide a useful tool for probing atmospheric structure. Specifically, the observed radiance as a function of wavelength and <span class="hlt">height</span> above the limb allows the vertical distribution of both dust and ice <span class="hlt">aerosols</span> to be retrieved. These data serve as an important supplement to the <span class="hlt">aerosol</span> profiling provided by the MRO/MCS instrument allowing independent validation and giving additional information on particle physical and scattering properties through multi-wavelength studies. A total of at least ten CRISM limb observations have been taken so far covering a full Martian year. Each set of limb observations nominally contains about four dozen scans across the limb giving pole-to-pole coverage for two orbits at roughly 100 and 290 W longitude over the Tharsis and Syrtis/Hellas regions, respectively. At each longitude, limb scans are spaced roughly 10 degrees apart in latitude, with a vertical spatial resolution on the limb of roughly 800 m. Radiative transfer modeling is used to model the observations. We compute synthetic CRISM limb spectra using a discrete-ordinates radiative transfer code that accounts for multiple scattering from <span class="hlt">aerosols</span> and accounts for spherical geometry of the limb observations by integrating the source functions along curved paths in that coordinate system. Retrieved are 14-point vertical profiles for dust and water ice <span class="hlt">aerosols</span> with resolution of 0.4 <span class="hlt">scale</span> <span class="hlt">heights</span> between one and six <span class="hlt">scale</span> <span class="hlt">heights</span> above the surface. After the <span class="hlt">aerosol</span> retrieval is completed, the abundances of CO2 (or surface pressure) and H2O gas are retrieved by matching the depth of absorption bands at 2000 nm for carbon dioxide and at 2600 nm for water vapor. In addition to the column abundance of water vapor, limited information on its vertical structure can also be retrieved depending on the signal available</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/2014AtmEn..96..405P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AtmEn..96..405P"><span>Physicochemical characterization of smoke <span class="hlt">aerosol</span> during large-<span class="hlt">scale</span> wildfires: Extreme event of August 2010 in Moscow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popovicheva, O.; Kistler, M.; Kireeva, E.; Persiantseva, N.; Timofeev, M.; Kopeikin, V.; Kasper-Giebl, A.</p> <p>2014-10-01</p> <p>Enhancement of biomass burning-related research is essential for the assessment of large-<span class="hlt">scale</span> wildfires impact on pollution at regional and global <span class="hlt">scale</span>. Starting since 6 August 2010 Moscow was covered with thick smoke of unusually high PM10 and BC concentrations, considerably affected by huge forest and peat fires around megacity. This work presents the first comprehensive physico-chemical characterization of <span class="hlt">aerosols</span> during extreme smoke event in Moscow in August 2010. Sampling was performed in the Moscow center and suburb as well as one year later, in August 2011 during a period when no biomass burning was observed. Small-<span class="hlt">scale</span> experimental fires of regional biomass were conducted in the Moscow region. Carbon content, functionalities of organic/inorganic compounds, tracers of biomass burning (anhydrosaccharides), ionic composition, and structure of smoke were analyzed by thermal-optical analysis, FTIR spectroscopy, liquid and ion chromatography, and electron microscopy. Carbonaceous <span class="hlt">aerosol</span> in August 2010 was dominated by organic species with elemental carbon (EC) as minor component. High average OC/EC near 27.4 is found, comparable to smoke of regional biomass smoldering fire, and exceeded 3 times the value observed in August 2011. Organic functionalities of Moscow smoke <span class="hlt">aerosols</span> were hydroxyl, aliphatic, aromatic, acid and non-acid carbonyl, and nitro compound groups, almost all of them indicate wildfires around city as the source of smoke. The ratio of levoglucosan (LG) to mannosan near 5 confirms the origin of smoke from coniferous forest fires around megacity. Low ratio of LG/OC near 0.8% indicates the degradation of major molecular tracer of biomass burning in urban environment. Total concentration of inorganic ions dominated by sulfates SO4 2 - and ammonium NH4+ was found about 5 times higher during large-<span class="hlt">scale</span> wildfires than in August 2011. Together with strong sulfate and ammonium absorbance in smoke <span class="hlt">aerosols</span>, these observations prove the formation of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1038638-evaluating-wrf-chem-aerosol-indirect-effects-southeast-pacific-marine-stratocumulus-during-vocals-rex','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1038638-evaluating-wrf-chem-aerosol-indirect-effects-southeast-pacific-marine-stratocumulus-during-vocals-rex"><span>Evaluating WRF-Chem <span class="hlt">aerosol</span> indirect effects in Southeast Pacific marine stratocumulus during VOCALS-REx</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>Saide, Pablo; Spak, S. N.; Carmichael, Gregory</p> <p>2012-03-30</p> <p>We evaluate a regional-<span class="hlt">scale</span> simulation with the WRF-Chem model for the VAMOS (Variability of the American Monsoon Systems) Ocean-Cloud-Atmosphere-Land Study Regional Experiment (VOCALS-REx), which sampled the Southeast Pacific's persistent stratocumulus deck. Evaluation of VOCALS-REx ship-based and aircraft observations focuses on analyzing how <span class="hlt">aerosol</span> loading affects marine boundary layer (MBL) dynamics and cloud microphysics. We compare local time series and campaign averaged longitudinal gradients, and highlight differences in model simulations with (W) and without wet (NW) deposition processes. The higher <span class="hlt">aerosol</span> loadings in the NW case produce considerable changes in MBL dynamics and cloud microphysics, in accordance with the established conceptualmore » model of <span class="hlt">aerosol</span> indirect effects. These include increase in cloud albedo, increase in MBL and cloud <span class="hlt">heights</span>, drizzle suppression, increase in liquid water content, and increase in cloud lifetime. Moreover, better statistical representation of <span class="hlt">aerosol</span> mass and number concentration improves model fidelity in reproducing observed spatial and temporal variability in cloud properties, including top and base <span class="hlt">height</span>, droplet concentration, water content, rain rate, optical depth (COD) and liquid water path (LWP). Together, these help to quantify confidence in WRF-Chem's modeled <span class="hlt">aerosol</span>-cloud interactions, while identifying structural and parametric uncertainties including: irreversibility in rain wet removal; overestimation of marine DMS and sea salt emissions and accelerated aqueous sulfate conversion. Our findings suggest that WRF-Chem simulates marine cloud-<span class="hlt">aerosol</span> interactions at a level sufficient for applications in forecasting weather and air quality and studying <span class="hlt">aerosol</span> climate forcing, including the reliability required for policy analysis and geo-engineering applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960027888','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960027888"><span>Theoretical and global <span class="hlt">scale</span> model studies of the atmospheric sulfur/<span class="hlt">aerosol</span> system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kasibhatla, Prasad</p> <p>1996-01-01</p> <p>The primary focus during the third-phase of our on-going multi-year research effort has been on 3 activities. These are: (1) a global-<span class="hlt">scale</span> model study of the anthropogenic component of the tropospheric sulfur cycle; (2) process-<span class="hlt">scale</span> model studies of the factors influencing the distribution of <span class="hlt">aerosols</span> in the remote marine atmosphere; and (3) an investigation of the mechanism of the OH-initiated oxidation of DMS in the remote marine boundary layer. In this paper, we describe in more detail our research activities in each of these areas. A major portion of our activities during the fourth and final phase of this project will involve the preparation and submission of manuscripts describing the results from our model studies of marine boundary-layer <span class="hlt">aerosols</span> and DMS-oxidation mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4923863','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4923863"><span>Quantifying the effect of organic <span class="hlt">aerosol</span> aging and intermediate-volatility emissions on regional-<span class="hlt">scale</span> <span class="hlt">aerosol</span> pollution in China</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zhao, Bin; Wang, Shuxiao; Donahue, Neil M.; Jathar, Shantanu H.; Huang, Xiaofeng; Wu, Wenjing; Hao, Jiming; Robinson, Allen L.</p> <p>2016-01-01</p> <p>Secondary organic <span class="hlt">aerosol</span> (SOA) is one of the least understood constituents of fine particles; current widely-used models cannot predict its loadings or oxidation state. Recent laboratory experiments demonstrated the importance of several new processes, including aging of SOA from traditional precursors, aging of primary organic <span class="hlt">aerosol</span> (POA), and photo-oxidation of intermediate volatility organic compounds (IVOCs). However, evaluating the effect of these processes in the real atmosphere is challenging. Most models used in previous studies are over-simplified and some key reaction trajectories are not captured, and model parameters are usually phenomenological and lack experimental constraints. Here we comprehensively assess the effect of organic <span class="hlt">aerosol</span> (OA) aging and intermediate-volatility emissions on regional-<span class="hlt">scale</span> OA pollution with a state-of-the-art model framework and experimentally constrained parameters. We find that OA aging and intermediate-volatility emissions together increase OA and SOA concentrations in Eastern China by about 40% and a factor of 10, respectively, thereby improving model-measurement agreement significantly. POA and IVOCs both constitute over 40% of OA concentrations, and IVOCs constitute over half of SOA concentrations; this differs significantly from previous apportionment of SOA sources. This study facilitates an improved estimate of <span class="hlt">aerosol</span>-induced climate and health impacts, and implies a shift from current fine-particle control policies. PMID:27350423</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1511300W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1511300W"><span>Global <span class="hlt">aerosol</span> effects on convective clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wagner, Till; Stier, Philip</p> <p>2013-04-01</p> <p>Atmospheric <span class="hlt">aerosols</span> affect cloud properties, and thereby the radiation balance of the planet and the water cycle. The influence of <span class="hlt">aerosols</span> on clouds is dominated by increase of cloud droplet and ice crystal numbers (CDNC/ICNC) due to enhanced <span class="hlt">aerosols</span> acting as cloud condensation and ice nuclei. In deep convective clouds this increase in CDNC/ICNC is hypothesised to increase precipitation because of cloud invigoration through enhanced freezing and associated increased latent heat release caused by delayed warm rain formation. Satellite studies robustly show an increase of cloud top <span class="hlt">height</span> (CTH) and precipitation with increasing <span class="hlt">aerosol</span> optical depth (AOD, as proxy for <span class="hlt">aerosol</span> amount). To represent <span class="hlt">aerosol</span> effects and study their influence on convective clouds in the global climate <span class="hlt">aerosol</span> model ECHAM-HAM, we substitute the standard convection parameterisation, which uses one mean convective cloud for each grid column, with the convective cloud field model (CCFM), which simulates a spectrum of convective clouds, each with distinct values of radius, mixing ratios, vertical velocity, <span class="hlt">height</span> and en/detrainment. <span class="hlt">Aerosol</span> activation and droplet nucleation in convective updrafts at cloud base is the primary driver for microphysical <span class="hlt">aerosol</span> effects. To produce realistic estimates for vertical velocity at cloud base we use an entraining dry parcel sub cloud model which is triggered by perturbations of sensible and latent heat at the surface. <span class="hlt">Aerosol</span> activation at cloud base is modelled with a mechanistic, Köhler theory based, scheme, which couples the <span class="hlt">aerosols</span> to the convective microphysics. Comparison of relationships between CTH and AOD, and precipitation and AOD produced by this novel model and satellite based estimates show general agreement. Through model experiments and analysis of the model cloud processes we are able to investigate the main drivers for the relationship between CTH / precipitation and AOD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyA..501...86Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyA..501...86Y"><span><span class="hlt">Height</span> conditions salary expectations: Evidence from large-<span class="hlt">scale</span> data 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>Yang, Xiao; Gao, Jian; Liu, Jin-Hu; Zhou, Tao</p> <p>2018-07-01</p> <p><span class="hlt">Height</span> premium has been revealed by extensive literature, however, evidence from China based on large-<span class="hlt">scale</span> data remains still lacking. In this paper, we study how <span class="hlt">height</span> conditions salary expectations by exploring a dataset covering over 140,000 Chinese job seekers. By using graphical and regression models, we find evidence in support of <span class="hlt">height</span> premium that tall people expect a significantly higher salary in career development. In particular, regression results suggest stronger effects of <span class="hlt">height</span> premium on female than on male, however, the gender differences decrease as the education level increases and become insignificant after holding all control variables fixed. Further, results from graphical models suggest three promising ways in helping short people: (i) to accumulate more working experiences, since one year seniority can respectively make up about 3 cm and 7 cm shortness for female and male; (ii) to increase the level of education, since one higher academic degree may eliminate all disadvantages that brought by shortness; (iii) to target jobs in regions with a higher level of development. Our work provides a cross-culture supportive evidence of <span class="hlt">height</span> premium and contributes two novel features to the literature: the compensation story in helping short people, and the focus on salary expectations in isolation from discrimination channels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29902747','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29902747"><span>Elucidating the relationship between <span class="hlt">aerosol</span> concentration and summertime boundary layer structure in central China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Lin; Guo, Jianping; Miao, Yucong; Liu, Lin; Li, Jian; Chen, Dandan; He, Jing; Cui, Chunguang</p> <p>2018-06-11</p> <p>Wuhan, a megacity in central China, suffers from frequent <span class="hlt">aerosol</span> pollution and is accompanied by meteorological factors at both synoptic and local <span class="hlt">scales</span>. Partly due to the lack of appropriate observations of planetary boundary layer (PBL), the associations between synoptic conditions, PBL, and pollution there are not yet fully understood. Thus, systematic analyses were conducted using the fine-resolution soundings, surface meteorological measurements, and <span class="hlt">aerosol</span> observations in Wuhan during summer for the period 2013-2016, in combination with T-mode principal component analysis and simulations of backward trajectory. The results showed that the variations of boundary layer <span class="hlt">height</span> (BLH) not only modulated the diurnal variation of PM 2.5 concentration in Wuhan, but also the daily pollution level. Five different synoptic patterns during summer in Wuhan were identified from reanalysis geopotential <span class="hlt">height</span> fields. Among these synoptic patterns, two types characterized by northeasterly prevailing winds, were found to be associated with heavy pollution in Wuhan. Driven by the northeasterly winds, the polluted air mass from the heavily polluted regions could be easily transported to Wuhan, such as North China Plain and Yangtze River Delta. Such regional transports of pollutants must be partly responsible for the <span class="hlt">aerosol</span> pollution in Wuhan. In addition, these two synoptic patterns were also featured by the relatively high cloud cover and low boundary layer <span class="hlt">height</span> in Wuhan, which would favor the occurrence of pollution there. Overall, this study has important implications for understanding the important roles of meteorological factors in modulating <span class="hlt">aerosol</span> pollution in central China. Copyright © 2018 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E1103G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E1103G"><span>Real-time reconstruction of topside ionosphere <span class="hlt">scale</span> <span class="hlt">height</span> from coordinated GPS-TEC and ionosonde observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gulyaeva, Tamara; Poustovalova, Ljubov</p> <p></p> <p>The International Reference Ionosphere model extended to the plasmasphere, IRI-Plas, has been recently updated for assimilation of total electron content, TEC, derived from observations with Global Navigation Satellite System, GNSS. The ionosonde products of the F2 layer peak density (NmF2) and <span class="hlt">height</span> (hmF2) ensure true electron density maximum at the F2 peak. The daily solar and magnetic indices used by IRI-Plas code are compiled in data files including the 3-hour ap and kp magnetic index from 1958 onward, 12-monthly smoothed sunspot number R12 and Global Electron Content GEC12, daily solar radio flux F10.7 and daily sunspot number Ri. The 3-h ap-index is available in Real Time, RT, mode from GFZ, Potsdam, Germany, daily update of F10.7 is provided by Space Weather Canada service, and daily estimated international sunspot number Ri is provided by Solar Influences Data Analysis Center, SIDC, Belgium. For IRI-Plas-RT operation in regime of the daily update and prediction of the F2 layer peak parameters, the proxy kp and ap forecast for 3 to 24 hours ahead based on data for preceding 12 hours is applied online at http://www.izmiran.ru/services/iweather/. The topside electron density profile of IRI-Plas code is expressed with complementary half-peak density anchor <span class="hlt">height</span> above hmF2 which corresponds to transition O+/H+ <span class="hlt">height</span>. The present investigation is focused on reconstruction of topside ionosphere <span class="hlt">scale</span> <span class="hlt">height</span> using vertical total electron content (TEC) data derived from the Global Positioning System GPS observations and the ionosonde derived F2 layer peak parameters from 25 observatories ingested into IRI-Plas model. GPS-TEC and ionosonde measurements at solar maximum (September, 2002, and October, 2003) for quiet, positively disturbed, and negatively disturbed days of the month are used to obtain the topside <span class="hlt">scale</span> <span class="hlt">height</span>, Htop, representing the range of altitudes from hmF2 to the <span class="hlt">height</span> where NmF2 decay by e times occurs. Mapping of the F2 layer peak parameters</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050139744&hterms=date+palm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Ddate%2Bpalm','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050139744&hterms=date+palm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Ddate%2Bpalm"><span><span class="hlt">Aerosol</span> and Cloud Observations and Data Products by the GLAS Polar Orbiting Lidar Instrument</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spinhirne, J. D.; Palm, S. P.; Hlavka, D. L.; Hart, W. D.; Mahesh, A.; Welton, E. J.</p> <p>2005-01-01</p> <p>The Geoscience Laser Altimeter System (GLAS) launched in 2003 is the first polar orbiting satellite lidar. The instrument was designed for high performance observations of the distribution and optical scattering cross sections of clouds and <span class="hlt">aerosol</span>. The backscatter lidar operates at two wavelengths, 532 and 1064 nm. Both receiver channels meet and exceed their design goals, and beginning with a two month period through October and November 2003, an excellent global lidar data set now exists. The data products for atmospheric observations include the calibrated, attenuated backscatter cross section for cloud and <span class="hlt">aerosol</span>; <span class="hlt">height</span> detection for multiple cloud layers; planetary boundary layer <span class="hlt">height</span>; cirrus and <span class="hlt">aerosol</span> optical depth and the <span class="hlt">height</span> distribution of <span class="hlt">aerosol</span> and cloud scattering cross section profiles. The data sets are now in open release through the NASA data distribution system. The initial results on global statistics for cloud and <span class="hlt">aerosol</span> distribution has been produced and in some cases compared to other satellite observations. The sensitivity of the cloud measurements is such that the 70% global cloud coverage result should be the most accurate to date. Results on the global distribution of <span class="hlt">aerosol</span> are the first that produce the true <span class="hlt">height</span> distribution for model inter-comparison.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1044745-evaluating-wrf-chem-aerosol-indirect-effects-southeast-pacific-marine-stratocumulus-during-vocals-rex','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1044745-evaluating-wrf-chem-aerosol-indirect-effects-southeast-pacific-marine-stratocumulus-during-vocals-rex"><span>Evaluating WRF-Chem <span class="hlt">aerosol</span> indirect effects in Southeast Pacific marine stratocumulus during VOCALS-REx</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>Saide P. E.; Springston S.; Spak, S. N.</p> <p>2012-03-29</p> <p>We evaluate a regional-<span class="hlt">scale</span> simulation with the WRF-Chem model for the VAMOS (Variability of the American Monsoon Systems) Ocean-Cloud-Atmosphere-Land Study Regional Experiment (VOCALS-REx), which sampled the Southeast Pacific's persistent stratocumulus deck. Evaluation of VOCALS-REx ship-based and three aircraft observations focuses on analyzing how <span class="hlt">aerosol</span> loading affects marine boundary layer (MBL) dynamics and cloud microphysics. We compare local time series and campaign-averaged longitudinal gradients, and highlight differences in model simulations with (W) and without (NW) wet deposition processes. The higher <span class="hlt">aerosol</span> loadings in the NW case produce considerable changes in MBL dynamics and cloud microphysics, in accordance with the established conceptualmore » model of <span class="hlt">aerosol</span> indirect effects. These include increase in cloud albedo, increase in MBL and cloud <span class="hlt">heights</span>, drizzle suppression, increase in liquid water content, and increase in cloud lifetime. Moreover, better statistical representation of <span class="hlt">aerosol</span> mass and number concentration improves model fidelity in reproducing observed spatial and temporal variability in cloud properties, including top and base <span class="hlt">height</span>, droplet concentration, water content, rain rate, optical depth (COD) and liquid water path (LWP). Together, these help to quantify confidence in WRF-Chem's modeled <span class="hlt">aerosol</span>-cloud interactions, especially in the activation parameterization, while identifying structural and parametric uncertainties including: irreversibility in rain wet removal; overestimation of marine DMS and sea salt emissions, and accelerated aqueous sulfate conversion. Our findings suggest that WRF-Chem simulates marine cloud-<span class="hlt">aerosol</span> interactions at a level sufficient for applications in forecasting weather and air quality and studying <span class="hlt">aerosol</span> climate forcing, and may do so with the reliability required for policy analysis.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFD.E4004G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFD.E4004G"><span>On the Physics of Fizziness: How liquid properties control bursting bubble <span class="hlt">aerosol</span> production?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghabache, Elisabeth; Antkowiak, Arnaud; Josserand, Christophe; Seon, Thomas</p> <p>2014-11-01</p> <p>Either in a champagne glass or at the oceanic <span class="hlt">scales</span>, the tiny capillary bubbles rising at the surface burst in ejecting myriads of droplets. Focusing on the ejected droplets produced by a single bubble, we investigate experimentally how liquid properties and bubble size affect their characteristics: number, ejection velocities, sizes and ejection <span class="hlt">heights</span>. These results allow us to finely tune the bursting bubble <span class="hlt">aerosol</span> production. In the context of champagne industry, <span class="hlt">aerosols</span> play a major role by spreading wine aroma above the glass. We demonstrate that this champagne fizz can be enhanced by selecting the wine viscosity and the bubble size, thanks to specially designed glass.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NatGe..11...44S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NatGe..11...44S"><span>Substantial large-<span class="hlt">scale</span> feedbacks between natural <span class="hlt">aerosols</span> and climate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scott, C. E.; Arnold, S. R.; Monks, S. A.; Asmi, A.; Paasonen, P.; Spracklen, D. V.</p> <p>2018-01-01</p> <p>The terrestrial biosphere is an important source of natural <span class="hlt">aerosol</span>. Natural <span class="hlt">aerosol</span> sources alter climate, but are also strongly controlled by climate, leading to the potential for natural <span class="hlt">aerosol</span>-climate feedbacks. Here we use a global <span class="hlt">aerosol</span> model to make an assessment of terrestrial natural <span class="hlt">aerosol</span>-climate feedbacks, constrained by observations of <span class="hlt">aerosol</span> number. We find that warmer-than-average temperatures are associated with higher-than-average number concentrations of large (>100 nm diameter) particles, particularly during the summer. This relationship is well reproduced by the model and is driven by both meteorological variability and variability in natural <span class="hlt">aerosol</span> from biogenic and landscape fire sources. We find that the calculated extratropical annual mean <span class="hlt">aerosol</span> radiative effect (both direct and indirect) is negatively related to the observed global temperature anomaly, and is driven by a positive relationship between temperature and the emission of natural <span class="hlt">aerosol</span>. The extratropical <span class="hlt">aerosol</span>-climate feedback is estimated to be -0.14 W m-2 K-1 for landscape fire <span class="hlt">aerosol</span>, greater than the -0.03 W m-2 K-1 estimated for biogenic secondary organic <span class="hlt">aerosol</span>. These feedbacks are comparable in magnitude to other biogeochemical feedbacks, highlighting the need for natural <span class="hlt">aerosol</span> feedbacks to be included in climate simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003106&hterms=algorithm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dalgorithm','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003106&hterms=algorithm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dalgorithm"><span>A New Algorithm for Detecting Cloud <span class="hlt">Height</span> using OMPS/LP Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chen, Zhong; DeLand, Matthew; Bhartia, Pawan K.</p> <p>2016-01-01</p> <p>The Ozone Mapping and Profiler Suite Limb Profiler (OMPS/LP) ozone product requires the determination of cloud <span class="hlt">height</span> for each event to establish the lower boundary of the profile for the retrieval algorithm. We have created a revised cloud detection algorithm for LP measurements that uses the spectral dependence of the vertical gradient in radiance between two wavelengths in the visible and near-IR spectral regions. This approach provides better discrimination between clouds and <span class="hlt">aerosols</span> than results obtained using a single wavelength. Observed LP cloud <span class="hlt">height</span> values show good agreement with coincident Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/45755-climatology-stratospheric-aerosol','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/45755-climatology-stratospheric-aerosol"><span>A climatology of stratospheric <span class="hlt">aerosol</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>Hitchman, M.H.; Mckay, M.; Trepte, C.R.</p> <p>1994-10-01</p> <p>A global climatology of stratospheric <span class="hlt">aerosol</span> is created by combining nearly a decade (1979-1981 and 1984-1990) of contemporaneous observations from the Stratospheric <span class="hlt">Aerosol</span> and Gas Experiment (SAGE I and II) and Stratospheric <span class="hlt">Aerosol</span> Measurement (SAM II) instruments. One goal of this work is to provide a representative distribution of the <span class="hlt">aerosol</span> layer for use in radiative and chemical modeling. A table of decadal average 1 micron extinction values is included, extending from the tropopause to 35 km and 80 deg S to 85 deg N, which allows estimation of surface area density. We find that the <span class="hlt">aerosol</span> layer is distinctlymore » volcanic in nature and suggest that the decadal average is a more useful estimate of future <span class="hlt">aerosol</span> loading than a `background` loading, which is never clearly achieved during the data record. This climatology lends insight into the general circulation of the stratosphere. Latitude - altitude sections of extinction radio at 1 micron are shown, average by decade, season, and phase of the quasi-biennial oscillation (QBO). A tropical reservoir region is diagnosed, with an `upper` and a `lower` transport regime. In the tropics above 22 km (upper regime), enhanced lofting occurs in the summer, with suppressed lofting or eddy dilution in the winter. In the extratropics within two <span class="hlt">scale</span> <span class="hlt">heights</span> of the tropopause (lower regime), poleward and downward transport is most robust during winter, especially in the northern hemisphere. The transport patterns persist into the subsequent equinoctial season. Ascent associated with QBO easterly shear favors detrainment in the upper regime, while relative descent and poleward spreading during QBO westerly shear favors detrainment in the lower regime. Extinction radio differences between the winter-spring and summer-fall hemispheres, and differences between the two phases of the QBO, are typically 20-50%.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACPD...1432177B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACPD...1432177B"><span>Using the OMI <span class="hlt">Aerosol</span> Index and Absorption <span class="hlt">Aerosol</span> Optical Depth to evaluate the NASA MERRA <span class="hlt">Aerosol</span> Reanalysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buchard, V.; da Silva, A. M.; Colarco, P. R.; Darmenov, A.; Randles, C. A.; Govindaraju, R.; Torres, O.; Campbell, J.; Spurr, R.</p> <p>2014-12-01</p> <p>A radiative transfer interface has been developed to simulate the UV <span class="hlt">Aerosol</span> Index (AI) from the NASA Goddard Earth Observing System version 5 (GEOS-5) <span class="hlt">aerosol</span> assimilated fields. The purpose of this work is to use the AI and <span class="hlt">Aerosol</span> Absorption Optical Depth (AAOD) derived from the Ozone Monitoring Instrument (OMI) measurements as independent validation for the Modern Era Retrospective analysis for Research and Applications <span class="hlt">Aerosol</span> Reanalysis (MERRAero). MERRAero is based on a version of the GEOS-5 model that is radiatively coupled to the Goddard Chemistry, <span class="hlt">Aerosol</span>, Radiation, and Transport (GOCART) <span class="hlt">aerosol</span> module and includes assimilation of <span class="hlt">Aerosol</span> Optical Depth (AOD) from the Moderate Resolution Imaging Spectroradiometer (MODIS) sensor. Since AI is dependent on <span class="hlt">aerosol</span> concentration, optical properties and altitude of the <span class="hlt">aerosol</span> layer, we make use of complementary observations to fully diagnose the model, including AOD from the Multi-angle Imaging SpectroRadiometer (MISR), <span class="hlt">aerosol</span> retrievals from the <span class="hlt">Aerosol</span> Robotic Network (AERONET) and attenuated backscatter coefficients from the Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) mission to ascertain potential misplacement of plume <span class="hlt">height</span> by the model. By sampling dust, biomass burning and pollution events in 2007 we have compared model produced AI and AAOD with the corresponding OMI products, identifying regions where the model representation of absorbing <span class="hlt">aerosols</span> was deficient. As a result of this study over the Saharan dust region, we have obtained a new set of dust <span class="hlt">aerosol</span> optical properties that retains consistency with the MODIS AOD data that were assimilated, while resulting in better agreement with <span class="hlt">aerosol</span> absorption measurements from OMI. The analysis conducted over the South African and South American biomass burning regions indicates that revising the spectrally-dependent <span class="hlt">aerosol</span> absorption properties in the near-UV region improves the modeled-observed AI comparisons</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ACP....15.5743B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ACP....15.5743B"><span>Using the OMI <span class="hlt">aerosol</span> index and absorption <span class="hlt">aerosol</span> optical depth to evaluate the NASA MERRA <span class="hlt">Aerosol</span> Reanalysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buchard, V.; da Silva, A. M.; Colarco, P. R.; Darmenov, A.; Randles, C. A.; Govindaraju, R.; Torres, O.; Campbell, J.; Spurr, R.</p> <p>2015-05-01</p> <p>A radiative transfer interface has been developed to simulate the UV <span class="hlt">aerosol</span> index (AI) from the NASA Goddard Earth Observing System version 5 (GEOS-5) <span class="hlt">aerosol</span> assimilated fields. The purpose of this work is to use the AI and <span class="hlt">aerosol</span> absorption optical depth (AAOD) derived from the Ozone Monitoring Instrument (OMI) measurements as independent validation for the Modern Era Retrospective analysis for Research and Applications <span class="hlt">Aerosol</span> Reanalysis (MERRAero). MERRAero is based on a version of the GEOS-5 model that is radiatively coupled to the Goddard Chemistry, <span class="hlt">Aerosol</span>, Radiation, and Transport (GOCART) <span class="hlt">aerosol</span> module and includes assimilation of <span class="hlt">aerosol</span> optical depth (AOD) from the Moderate Resolution Imaging Spectroradiometer (MODIS) sensor. Since AI is dependent on <span class="hlt">aerosol</span> concentration, optical properties and altitude of the <span class="hlt">aerosol</span> layer, we make use of complementary observations to fully diagnose the model, including AOD from the Multi-angle Imaging SpectroRadiometer (MISR), <span class="hlt">aerosol</span> retrievals from the <span class="hlt">AErosol</span> RObotic NETwork (AERONET) and attenuated backscatter coefficients from the Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) mission to ascertain potential misplacement of plume <span class="hlt">height</span> by the model. By sampling dust, biomass burning and pollution events in 2007 we have compared model-produced AI and AAOD with the corresponding OMI products, identifying regions where the model representation of absorbing <span class="hlt">aerosols</span> was deficient. As a result of this study over the Saharan dust region, we have obtained a new set of dust <span class="hlt">aerosol</span> optical properties that retains consistency with the MODIS AOD data that were assimilated, while resulting in better agreement with <span class="hlt">aerosol</span> absorption measurements from OMI. The analysis conducted over the southern African and South American biomass burning regions indicates that revising the spectrally dependent <span class="hlt">aerosol</span> absorption properties in the near-UV region improves the modeled-observed AI comparisons</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.5364Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.5364Z"><span>Retrieval of volcanic ash <span class="hlt">height</span> from satellite-based infrared measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Lin; Li, Jun; Zhao, Yingying; Gong, He; Li, Wenjie</p> <p>2017-05-01</p> <p>A new algorithm for retrieving volcanic ash cloud <span class="hlt">height</span> from satellite-based measurements is presented. This algorithm, which was developed in preparation for China's next-generation meteorological satellite (FY-4), is based on volcanic ash microphysical property simulation and statistical optimal estimation theory. The MSG satellite's main payload, a 12-channel Spinning Enhanced Visible and Infrared Imager, was used as proxy data to test this new algorithm. A series of eruptions of Iceland's Eyjafjallajökull volcano during April to May 2010 and the Puyehue-Cordón Caulle volcanic complex eruption in the Chilean Andes on 16 June 2011 were selected as two typical cases for evaluating the algorithm under various meteorological backgrounds. Independent volcanic ash simulation training samples and satellite-based Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization data were used as validation data. It is demonstrated that the statistically based volcanic ash <span class="hlt">height</span> algorithm is able to rapidly retrieve volcanic ash <span class="hlt">heights</span>, globally. The retrieved ash <span class="hlt">heights</span> show comparable accuracy with both independent training data and the lidar measurements, which is consistent with previous studies. However, under complicated background, with multilayers in vertical <span class="hlt">scale</span>, underlying stratus clouds tend to have detrimental effects on the final retrieval accuracy. This is an unresolved problem, like many other previously published methods using passive satellite sensors. Compared with previous studies, the FY-4 ash <span class="hlt">height</span> algorithm is independent of simultaneous atmospheric profiles, providing a flexible way to estimate volcanic ash <span class="hlt">height</span> using passive satellite infrared measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130000601','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130000601"><span>Mixed Layer <span class="hlt">Heights</span> Derived from the NASA Langley Research Center Airborne High Spectral Resolution Lidar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scarino, Amy J.; Burton, Sharon P.; Ferrare, Rich A.; Hostetler, Chris A.; Hair, Johnathan W.; Obland, Michael D.; Rogers, Raymond R.; Cook, Anthony L.; Harper, David B.; Fast, Jerome; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20130000601'); toggleEditAbsImage('author_20130000601_show'); toggleEditAbsImage('author_20130000601_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20130000601_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20130000601_hide"></p> <p>2012-01-01</p> <p>The NASA airborne High Spectral Resolution Lidar (HSRL) has been deployed on board the NASA Langley Research Center's B200 aircraft to several locations in North America from 2006 to 2012 to aid in characterizing <span class="hlt">aerosol</span> properties for over fourteen field missions. Measurements of <span class="hlt">aerosol</span> extinction (532 nm), backscatter (532 and 1064 nm), and depolarization (532 and 1064 nm) during 349 science flights, many in coordination with other participating research aircraft, satellites, and ground sites, constitute a diverse data set for use in characterizing the spatial and temporal distribution of <span class="hlt">aerosols</span>, as well as properties and variability of the Mixing Layer (ML) <span class="hlt">height</span>. We describe the use of the HSRL data collected during these missions for computing ML <span class="hlt">heights</span> and show how the HSRL data can be used to determine the fraction of <span class="hlt">aerosol</span> optical thickness within and above the ML, which is important for air quality assessments. We describe the spatial and temporal variations in ML <span class="hlt">heights</span> found in the diverse locations associated with these experiments. We also describe how the ML <span class="hlt">heights</span> derived from HSRL have been used to help assess simulations of Planetary Boundary Layer (PBL) derived using various models, including the Weather Research and Forecasting Chemistry (WRF-Chem), NASA GEOS-5 model, and the ECMWF/MACC models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5364465','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5364465"><span>Contrasting influences of <span class="hlt">aerosols</span> on cloud properties during deficient and abundant monsoon years</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Patil, Nitin; Dave, Prashant; Venkataraman, Chandra</p> <p>2017-01-01</p> <p>Direct <span class="hlt">aerosol</span> radiative forcing facilitates the onset of Indian monsoon rainfall, based on synoptic <span class="hlt">scale</span> fast responses acting over timescales of days to a month. Here, we examine relationships between <span class="hlt">aerosols</span> and coincident clouds over the Indian subcontinent, using observational data from 2000 to 2009, from the core monsoon region. Season mean and daily timescales were considered. The correlation analyses of cloud properties with <span class="hlt">aerosol</span> optical depth revealed that deficient monsoon years were characterized by more frequent and larger decreases in cloud drop size and ice water path, but increases in cloud top pressure, with increases in <span class="hlt">aerosol</span> abundance. The opposite was observed during abundant monsoon years. The correlations of greater <span class="hlt">aerosol</span> abundance, with smaller cloud drop size, lower evidence of ice processes and shallower cloud <span class="hlt">height</span>, during deficient rainfall years, imply cloud inhibition; while those with larger cloud drop size, greater ice processes and a greater cloud vertical extent, during abundant rainfall years, suggest cloud invigoration. The study establishes that continental <span class="hlt">aerosols</span> over India alter cloud properties in diametrically opposite ways during contrasting monsoon years. The mechanisms underlying these effects need further analysis. PMID:28337991</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28337991','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28337991"><span>Contrasting influences of <span class="hlt">aerosols</span> on cloud properties during deficient and abundant monsoon years.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Patil, Nitin; Dave, Prashant; Venkataraman, Chandra</p> <p>2017-03-24</p> <p>Direct <span class="hlt">aerosol</span> radiative forcing facilitates the onset of Indian monsoon rainfall, based on synoptic <span class="hlt">scale</span> fast responses acting over timescales of days to a month. Here, we examine relationships between <span class="hlt">aerosols</span> and coincident clouds over the Indian subcontinent, using observational data from 2000 to 2009, from the core monsoon region. Season mean and daily timescales were considered. The correlation analyses of cloud properties with <span class="hlt">aerosol</span> optical depth revealed that deficient monsoon years were characterized by more frequent and larger decreases in cloud drop size and ice water path, but increases in cloud top pressure, with increases in <span class="hlt">aerosol</span> abundance. The opposite was observed during abundant monsoon years. The correlations of greater <span class="hlt">aerosol</span> abundance, with smaller cloud drop size, lower evidence of ice processes and shallower cloud <span class="hlt">height</span>, during deficient rainfall years, imply cloud inhibition; while those with larger cloud drop size, greater ice processes and a greater cloud vertical extent, during abundant rainfall years, suggest cloud invigoration. The study establishes that continental <span class="hlt">aerosols</span> over India alter cloud properties in diametrically opposite ways during contrasting monsoon years. The mechanisms underlying these effects need further 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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....16.4817K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....16.4817K"><span>Modeling and measurements of urban <span class="hlt">aerosol</span> processes on the neighborhood <span class="hlt">scale</span> in Rotterdam, Oslo and Helsinki</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; Kukkonen, Jaakko; Keuken, Menno P.; Lützenkirchen, Susanne; Pirjola, Liisa; Hussein, Tareq</p> <p>2016-04-01</p> <p>This study evaluates the influence of <span class="hlt">aerosol</span> processes on the particle number (PN) concentrations in three major European cities on the temporal <span class="hlt">scale</span> of 1 h, i.e., on the neighborhood and city <span class="hlt">scales</span>. We have used selected measured data of particle size distributions from previous campaigns in the cities of Helsinki, Oslo and Rotterdam. The <span class="hlt">aerosol</span> transformation processes were evaluated using the <span class="hlt">aerosol</span> dynamics model MAFOR, combined with a simplified treatment of roadside and urban atmospheric dispersion. We have compared the model predictions of particle number size distributions with the measured data, and conducted sensitivity analyses regarding the influence of various model input variables. We also present a simplified parameterization for <span class="hlt">aerosol</span> processes, which is based on the more complex <span class="hlt">aerosol</span> process computations; this simple model can easily be implemented to both Gaussian and Eulerian urban dispersion models. <span class="hlt">Aerosol</span> processes considered in this study were (i) the coagulation of particles, (ii) the condensation and evaporation of two organic vapors, and (iii) dry deposition. The chemical transformation of gas-phase compounds was not taken into account. By choosing concentrations and particle size distributions at roadside as starting point of the computations, nucleation of gas-phase vapors from the exhaust has been regarded as post tail-pipe emission, avoiding the need to include nucleation in the process analysis. Dry deposition and coagulation of particles were identified to be the most important <span class="hlt">aerosol</span> dynamic processes that control the evolution and removal of particles. The error of the contribution from dry deposition to PN losses due to the uncertainty of measured deposition velocities ranges from -76 to +64 %. The removal of nanoparticles by coagulation enhanced considerably when considering the fractal nature of soot aggregates and the combined effect of van der Waals and viscous interactions. The effect of condensation and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eosweb.larc.nasa.gov/project/misr/gallery/aerosols_europe','SCIGOV-ASDC'); return false;" href="https://eosweb.larc.nasa.gov/project/misr/gallery/aerosols_europe"><span><span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://eosweb.larc.nasa.gov/">Atmospheric Science Data Center </a></p> <p></p> <p>2013-04-17</p> <p>... depth. A color <span class="hlt">scale</span> is used to represent this quantity, and high <span class="hlt">aerosol</span> amount is indicated by yellow or green pixels, and clearer skies ... out most clearly, whereas MISR's oblique cameras enhance sensitivity to even thin layers of <span class="hlt">aerosols</span>. In the March image, the only ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51E2119L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51E2119L"><span>Sources and Variability of <span class="hlt">Aerosols</span> and <span class="hlt">Aerosol</span>-Cloud Interactions in the Arctic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, H.; Zhang, B.; Taylor, P. C.; Moore, R.; Barahona, D.; Fairlie, T. D.; Chen, G.; Ham, S. H.; Kato, S.</p> <p>2017-12-01</p> <p>Arctic sea ice in recent decades has significantly declined. This requires understanding of the Arctic surface energy balance, of which clouds are a major driver. However, the mechanisms for the formation and evolution of clouds in the Arctic and the roles of <span class="hlt">aerosols</span> therein are highly uncertain. Here we conduct data analysis and global model simulations to examine the sources and variability of <span class="hlt">aerosols</span> and <span class="hlt">aerosol</span>-cloud interactions in the Arctic. We use the MERRA-2 reanalysis data (2006-present) from the NASA Global Modeling and Assimilation Office (GMAO) to (1) quantify contributions of different <span class="hlt">aerosol</span> types to the <span class="hlt">aerosol</span> budget and <span class="hlt">aerosol</span> optical depths in the Arctic, (2) ­examine <span class="hlt">aerosol</span> distributions and variability and diagnose the major pathways for mid-latitude pollution transport to the Arctic, including their seasonal and interannual variability, and (3) characterize the distribution and variability of clouds (cloud optical depth, cloud fraction, cloud liquid and ice water path, cloud top <span class="hlt">height</span>) in the Arctic. We compare MERRA-2 <span class="hlt">aerosol</span> and cloud properties with those from C3M, a 3-D <span class="hlt">aerosol</span> and cloud data product developed at NASA Langley Research Center and merged from multiple A-Train satellite (CERES, CloudSat, CALIPSO, and MODIS) observations. We also conduct perturbation experiments using the NASA GEOS-5 chemistry-climate model (with GOCART <span class="hlt">aerosol</span> module coupled with two-moment cloud microphysics), and discuss the roles of various types of <span class="hlt">aerosols</span> in the formation and evolution of clouds in the Arctic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26512347','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26512347"><span>Body mass index and body composition <span class="hlt">scaling</span> to <span class="hlt">height</span> in children and adolescent.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chung, Sochung</p> <p>2015-09-01</p> <p>Childhood obesity prevalence has been increased and known to be related to various diseases and mortality in adult and body mass index (BMI) has been widely used as a screening tool in children with obesity. It is important to understand what BMI is and its limitations. BMI is a measure of weight adjusted for <span class="hlt">height</span>. Weight <span class="hlt">scales</span> to <span class="hlt">height</span> with a power of about 2, is the basis of BMI (weight/<span class="hlt">height</span>(2)) as the <span class="hlt">scaling</span> of body weight to <span class="hlt">height</span> across adults provides powers rounded to 2. BMI has the advantage of a simple and noninvasive surrogate measure of body fat, but it has limitation in differentiating body fat from lean (fat free) mass and low-moderate sensitivity is problematic for clinical applications. Among overweight children higher BMI levels can be a result of increased either fat or fat-free mass. BMI could be divided into fat-free mass index and fat mass index. Monitoring of the changes in body composition is important as distinguishing changes in each component occur with rapid growth in adolescents as it is occur in concert with changes in the hormonal environment. Reference values for each body composition indexes and chart created with selected percentiles of a normal adolescent population could be helpful in growth assessment and health risk evaluation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70115119','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70115119"><span>Modeling vegetation <span class="hlt">heights</span> from high resolution stereo aerial photography: an application for broad-<span class="hlt">scale</span> rangeland monitoring</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Gillan, Jeffrey K.; Karl, Jason W.; Duniway, Michael; Elaksher, Ahmed</p> <p>2014-01-01</p> <p>Vertical vegetation structure in rangeland ecosystems can be a valuable indicator for assessing rangeland health and monitoring riparian areas, post-fire recovery, available forage for livestock, and wildlife habitat. Federal land management agencies are directed to monitor and manage rangelands at landscapes <span class="hlt">scales</span>, but traditional field methods for measuring vegetation <span class="hlt">heights</span> are often too costly and time consuming to apply at these broad <span class="hlt">scales</span>. Most emerging remote sensing techniques capable of measuring surface and vegetation <span class="hlt">height</span> (e.g., LiDAR or synthetic aperture radar) are often too expensive, and require specialized sensors. An alternative remote sensing approach that is potentially more practical for managers is to measure vegetation <span class="hlt">heights</span> from digital stereo aerial photographs. As aerial photography is already commonly used for rangeland monitoring, acquiring it in stereo enables three-dimensional modeling and estimation of vegetation <span class="hlt">height</span>. The purpose of this study was to test the feasibility and accuracy of estimating shrub <span class="hlt">heights</span> from high-resolution (HR, 3-cm ground sampling distance) digital stereo-pair aerial images. Overlapping HR imagery was taken in March 2009 near Lake Mead, Nevada and 5-cm resolution digital surface models (DSMs) were created by photogrammetric methods (aerial triangulation, digital image matching) for twenty-six test plots. We compared the <span class="hlt">heights</span> of individual shrubs and plot averages derived from the DSMs to field measurements. We found strong positive correlations between field and image measurements for several metrics. Individual shrub <span class="hlt">heights</span> tended to be underestimated in the imagery, however, accuracy was higher for dense, compact shrubs compared with shrubs with thin branches. Plot averages of shrub <span class="hlt">height</span> from DSMs were also strongly correlated to field measurements but consistently underestimated. Grasses and forbs were generally too small to be detected with the resolution of the DSMs. Estimates of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013033','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013033"><span>Improvements to the OMI Near-uv <span class="hlt">Aerosol</span> Algorithm Using A-train CALIOP and AIRS Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Torres, O.; Ahn, C.; Zhong, C.</p> <p>2014-01-01</p> <p>The <span class="hlt">height</span> of desert dust and carbonaceous <span class="hlt">aerosols</span> layers and, to a lesser extent, the difficulty in assessing the predominant size mode of these absorbing <span class="hlt">aerosol</span> types, are sources of uncertainty in the retrieval of <span class="hlt">aerosol</span> properties from near UV satellite observations. The availability of independent, near-simultaneous measurements of <span class="hlt">aerosol</span> layer <span class="hlt">height</span>, and <span class="hlt">aerosol</span>-type related parameters derived from observations by other A-train sensors, makes possible the direct use of these parameters as input to the OMI (Ozone Monitoring Instrument) near UV retrieval algorithm. A monthly climatology of <span class="hlt">aerosol</span> layer <span class="hlt">height</span> derived from observations by the CALIOP (Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization) sensor, and real-time AIRS (Atmospheric Infrared Sounder) CO observations are used in an upgraded version of the OMI near UV <span class="hlt">aerosol</span> algorithm. AIRS CO measurements are used as a reliable tracer of carbonaceous <span class="hlt">aerosols</span>, which allows the identification of smoke layers in areas and times of the year where the dust-smoke differentiation is difficult in the near-UV. The use of CO measurements also enables the identification of elevated levels of boundary layer pollution undetectable by near UV observations alone. In this paper we discuss the combined use of OMI, CALIOP and AIRS observations for the characterization of <span class="hlt">aerosol</span> properties, and show a significant improvement in OMI <span class="hlt">aerosol</span> retrieval capabilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27237206','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27237206"><span><span class="hlt">Aerosol</span>, a health hazard during ultrasonic <span class="hlt">scaling</span>: A clinico-microbiological study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Singh, Akanksha; Shiva Manjunath, R G; Singla, Deepak; Bhattacharya, Hirak S; Sarkar, Arijit; Chandra, Neeraj</p> <p>2016-01-01</p> <p>Ultrasonic <span class="hlt">scaling</span> is a routinely used treatment to remove plaque and calculus from tooth surfaces. These scalers use water as a coolant which is splattered during the vibration of the tip. The splatter when mixed with saliva and plaque of the patients causes the <span class="hlt">aerosol</span> highly infectious and acts as a major risk factor for transmission of the disease. In spite of necessary protection, sometimes, the operator might get infected because of the infectious nature of the splatter. To evaluate the <span class="hlt">aerosol</span> contamination produced during ultrasonic <span class="hlt">scaling</span> by the help of microbiological analysis. This clinico-microbiological study consisted of twenty patients. Two agar plates were used for each patient; the first was kept at the center of the operatory room 20 min before the treatment while the second agar plate was kept 40 cm away from the patient's chest during the treatment. Both the agar plates were sent for microbiological analysis. The statistical analysis was done with the help of STATA 11.0 (StataCorp. 2013. Stata Statistical Software, Release 13. College Station, TX: StataCorp LP, 4905 Lakeway Drive College Station, Texas, USA). Statistical software was used for data analysis and the P < 0.001 was considered to be statistically significant. The results for bacterial count were highly significant when compared before and during the treatment. The Gram staining showed the presence of Staphylococcus and Streptococcus species in high numbers. The <span class="hlt">aerosols</span> and splatters produced during dental procedures have the potential to spread infection to dental personnel. Therefore, proper precautions should be taken to minimize the risk of infection to the operator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1815332M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1815332M"><span><span class="hlt">Aerosol</span> typing - key information from <span class="hlt">aerosol</span> studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mona, Lucia; Kahn, Ralph; Papagiannopoulos, Nikolaos; Holzer-Popp, Thomas; Pappalardo, Gelsomina</p> <p>2016-04-01</p> <p><span class="hlt">Aerosol</span> typing is a key source of <span class="hlt">aerosol</span> information from ground-based and satellite-borne instruments. Depending on the specific measurement technique, <span class="hlt">aerosol</span> typing can be used as input for retrievals or represents an output for other applications. Typically <span class="hlt">aerosol</span> retrievals require some a priori or external <span class="hlt">aerosol</span> type information. The accuracy of the derived <span class="hlt">aerosol</span> products strongly depends on the reliability of these assumptions. Different sensors can make use of different <span class="hlt">aerosol</span> type inputs. A critical review and harmonization of these procedures could significantly reduce related uncertainties. On the other hand, satellite measurements in recent years are providing valuable information about the global distribution of <span class="hlt">aerosol</span> types, showing for example the main source regions and typical transport paths. Climatological studies of <span class="hlt">aerosol</span> load at global and regional <span class="hlt">scales</span> often rely on inferred <span class="hlt">aerosol</span> type. There is still a high degree of inhomogeneity among satellite <span class="hlt">aerosol</span> typing schemes, which makes the use different sensor datasets in a consistent way difficult. Knowledge of the 4d <span class="hlt">aerosol</span> type distribution at these <span class="hlt">scales</span> is essential for understanding the impact of different <span class="hlt">aerosol</span> sources on climate, precipitation and air quality. All this information is needed for planning upcoming <span class="hlt">aerosol</span> emissions policies. The exchange of expertise and the communication among satellite and ground-based measurement communities is fundamental for improving long-term dataset consistency, and for reducing <span class="hlt">aerosol</span> type distribution uncertainties. <span class="hlt">Aerosol</span> typing has been recognized as one of its high-priority activities of the AEROSAT (International Satellite <span class="hlt">Aerosol</span> Science Network, http://aero-sat.org/) initiative. In the AEROSAT framework, a first critical review of <span class="hlt">aerosol</span> typing procedures has been carried out. The review underlines the high heterogeneity in many aspects: approach, nomenclature, assumed number of components and parameters used for the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19008483','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19008483"><span>Differences between brain mass and body weight <span class="hlt">scaling</span> to <span class="hlt">height</span>: potential mechanism of reduced mass-specific resting energy expenditure of taller adults.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heymsfield, Steven B; Chirachariyavej, Thamrong; Rhyu, Im Joo; Roongpisuthipong, Chulaporn; Heo, Moonseong; Pietrobelli, Angelo</p> <p>2009-01-01</p> <p>Adult resting energy expenditure (REE) <span class="hlt">scales</span> as <span class="hlt">height</span>( approximately 1.5), whereas body weight (BW) <span class="hlt">scales</span> as <span class="hlt">height</span>( approximately 2). Mass-specific REE (i.e., REE/BW) is thus lower in tall subjects compared with their shorter counterparts, the mechanism of which is unknown. We evaluated the hypothesis that high-metabolic-rate brain mass <span class="hlt">scales</span> to <span class="hlt">height</span> with a power significantly less than that of BW, a theory that if valid would provide a potential mechanism for <span class="hlt">height</span>-related REE effects. The hypothesis was tested by measuring brain mass on a large (n = 372) postmortem sample of Thai men. Since brain mass-body size relations may be influenced by age, the hypothesis was secondarily explored in Thai men age < or =45 yr (n = 299) and with brain magnetic resonance imaging (MRI) studies in Korean men (n = 30) age > or =20<30 yr. The <span class="hlt">scaling</span> of large body compartments was examined in a third group of Asian men living in New York (NY, n = 28) with MRI and dual-energy X-ray absorptiometry. Brain mass <span class="hlt">scaled</span> to <span class="hlt">height</span> with a power (mean +/- SEE; 0.46 +/- 0.13) significantly smaller (P < 0.001) than that of BW <span class="hlt">scaled</span> to <span class="hlt">height</span> (2.36 +/- 0.19) in the whole group of Thai men; brain mass/BW <span class="hlt">scaled</span> negatively to <span class="hlt">height</span> (-1.94 +/- 0.20, P < 0.001). Similar results were observed in younger Thai men, and results for brain mass/BW vs. <span class="hlt">height</span> were directionally the same (P = 0.09) in Korean men. Skeletal muscle and bone <span class="hlt">scaled</span> to <span class="hlt">height</span> with powers similar to that of BW (i.e., approximately 2-3) in the NY Asian men. Models developed using REE estimates in Thai men suggest that brain accounts for most of the REE/BW <span class="hlt">height</span> dependency. Tall and short men thus differ in relative brain mass, but the proportions of BW as large compartments appear independent of <span class="hlt">height</span>, observations that provide a potential mechanistic basis for related differences in REE and that have implications for the study of adult energy requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GMD.....9.4049T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GMD.....9.4049T"><span>Easy Volcanic <span class="hlt">Aerosol</span> (EVA v1.0): an idealized forcing generator for 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>Toohey, Matthew; Stevens, Bjorn; Schmidt, Hauke; Timmreck, Claudia</p> <p>2016-11-01</p> <p>Stratospheric sulfate <span class="hlt">aerosols</span> from volcanic eruptions have a significant impact on the Earth's climate. To include the effects of volcanic eruptions in climate model simulations, the Easy Volcanic <span class="hlt">Aerosol</span> (EVA) forcing generator provides stratospheric <span class="hlt">aerosol</span> optical properties as a function of time, latitude, <span class="hlt">height</span>, and wavelength for a given input list of volcanic eruption attributes. EVA is based on a parameterized three-box model of stratospheric transport and simple <span class="hlt">scaling</span> relationships used to derive mid-visible (550 nm) <span class="hlt">aerosol</span> optical depth and <span class="hlt">aerosol</span> effective radius from stratospheric sulfate mass. Precalculated look-up tables computed from Mie theory are used to produce wavelength-dependent <span class="hlt">aerosol</span> extinction, single scattering albedo, and scattering asymmetry factor values. The structural form of EVA and the tuning of its parameters are chosen to produce best agreement with the satellite-based reconstruction of stratospheric <span class="hlt">aerosol</span> properties following the 1991 Pinatubo eruption, and with prior millennial-timescale forcing reconstructions, including the 1815 eruption of Tambora. EVA can be used to produce volcanic forcing for climate models which is based on recent observations and physical understanding but internally self-consistent over any timescale of choice. In addition, EVA is constructed so as to allow for easy modification of different aspects of <span class="hlt">aerosol</span> properties, in order to be used in model experiments to help advance understanding of what aspects of the volcanic <span class="hlt">aerosol</span> are important for the climate system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT........76Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT........76Z"><span>Spatio-temporal variability of <span class="hlt">aerosols</span> in the tropics relationship with atmospheric and oceanic environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zuluaga-Arias, Manuel D.</p> <p>2011-12-01</p> <p> of surface temperature, atmospheric wind, geopotential <span class="hlt">height</span>, outgoing longwave radiation, water vapor and precipitation together with the climatology of <span class="hlt">aerosols</span> provide insight on how the variables interact. Different modes of variability, especially in intraseasonal time <span class="hlt">scales</span> appear as strong modulators of the <span class="hlt">aerosol</span> distribution. In particular, we investigate how two modes of variability related to the westward propagating synoptic African Easterly Waves of the Tropical Atlantic Ocean affect the horizontal and vertical structure of the environment. The statistical significance of these two modes is tested with the use of two different spectral techniques. The pattern of propagation of <span class="hlt">aerosol</span> load shows good correspondence with the progression of the atmospheric and oceanic conditions suitable for dust mobilization over the Atlantic Ocean. We present extensions to previous studies related with dust variability over the Atlantic region by evaluating the performance of the long period satellite <span class="hlt">aerosol</span> retrievals in determining modes of <span class="hlt">aerosol</span> variability. Results of the covariability between <span class="hlt">aerosols</span>-environment motivate the use of statistical regression models to test the significance of the forecasting skill of daily AOD time series. The regression models are calibrated using atmospheric variables as predictors from the reanalysis variables. The results show poor forecasting skill with significant error growing after the 3 rd day of the prediction. It is hypothesized that the simplicity of linear models results in an inability to provide a useful forecast.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5441M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5441M"><span>Atmosphere <span class="hlt">aerosol</span> satellite project <span class="hlt">Aerosol</span>-UA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Milinevsky, Gennadi; Yatskiv, Yaroslav; Syniavskyi, Ivan; Bovchaliuk, Andrii; Degtyaryov, Oleksandr; Sosonkin, Mikhail; Mishchenko, Michael; Danylevsky, Vassyl; Ivanov, Yury; Oberemok, Yevgeny; Masley, Volodymyr; Rosenbush, Vera; Moskalev, Sergii</p> <p>2017-04-01</p> <p>The experiment <span class="hlt">Aerosol</span>-UA is Ukrainian space mission aimed to the terrestrial atmospheric <span class="hlt">aerosol</span> spatial distribution and microphysics investigations. The experiment concept is based on idea of Glory/APS mission of precise orbital measurements of polarization and intensity of the sunlight scattered by the atmosphere, <span class="hlt">aerosol</span> and the surface the multichannel Scanning Polarimeter (ScanPol) with narrow field-of-view. ScanPol measurements will be accompanied by the wide-angle MultiSpectral Imager-Polarimeter (MSIP). The ScanPol is designed to measure Stokes parameters I, Q, U within the spectral range from the UV to the SWIR in a wide range of phase angles along satellite ground path. Expected ScanPol polarimetric accuracy is 0.15%. A high accuracy measurement of the degree of linear polarization is provided by on-board calibration of the ScanPol polarimeter. On-board calibration is performed for each scan of the mirror scanning system. A set of calibrators is viewed during the part of the scan range when the ScanPol polarimeter looks in the direction opposite to the Earth's surface. These reference assemblies provide calibration of the zero of the polarimetric <span class="hlt">scale</span> (unpolarized reference assembly) and the <span class="hlt">scale</span> factor for the polarimetric <span class="hlt">scale</span> (polarized reference assembly). The zero of the radiometric <span class="hlt">scale</span> is provided by the dark reference assembly.The spectral channels of the ScanPol are used to estimate the tropospheric <span class="hlt">aerosol</span> absorption, the <span class="hlt">aerosol</span> over the ocean and the land surface, the signals from cirrus clouds, stratospheric <span class="hlt">aerosols</span> caused by major volcanic eruptions, and the contribution of the Earth's surface. The imager-polarimeter MSIP will collect 60°x60° field-of-view images on the state of the atmosphere and surface in the area, where the ScanPol polarimeter will measure, to retrieve <span class="hlt">aerosol</span> optical depth and polarization properties of <span class="hlt">aerosol</span> by registration of three Stokes parameters simultaneously in three spectral channels. The two more</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900002762','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900002762"><span><span class="hlt">Aerosol</span> in the Pacific troposphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clarke, Antony D.</p> <p>1989-01-01</p> <p>The use of near real-time optical techniques is emphasized for the measurement of mid-tropospheric <span class="hlt">aerosol</span> over the Central Pacific. The primary focus is on measurement of the <span class="hlt">aerosol</span> size distribution over the range of particle diameters from 0.15 to 5.0 microns that are essential for modeling CO2 backscatter values in support of the laser atmospheric wind sounder (LAWS) program. The measurement system employs a LAS-X (Laser <span class="hlt">Aerosol</span> Spectrometer-PMS, Boulder, CO) with a custom 256 channel pulse <span class="hlt">height</span> analyzer and software for detailed measurement and analysis of <span class="hlt">aerosol</span> size distributions. A thermal preheater system (Thermo Optic <span class="hlt">Aerosol</span> Descriminator (TOAD) conditions the <span class="hlt">aerosol</span> in a manner that allows the discrimination of the size distribution of individual <span class="hlt">aerosol</span> components such as sulfuric acid, sulfates and refractory species. This allows assessment of the relative contribution of each component to the BCO2 signal. This is necessary since the different components have different sources, exhibit independent variability and provide different BCO2 signals for a given mass and particle size. Field activities involve experiments designed to examine both temporal and spatial variability of these <span class="hlt">aerosol</span> components from ground based and aircraft platforms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24733923','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24733923"><span>Assessing the effects of anthropogenic <span class="hlt">aerosols</span> on Pacific storm track using a multiscale global climate model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Yuan; Wang, Minghuai; Zhang, Renyi; Ghan, Steven J; Lin, Yun; Hu, Jiaxi; Pan, Bowen; Levy, Misti; Jiang, Jonathan H; Molina, Mario J</p> <p>2014-05-13</p> <p>Atmospheric <span class="hlt">aerosols</span> affect weather and global general circulation by modifying cloud and precipitation processes, but the magnitude of cloud adjustment by <span class="hlt">aerosols</span> remains poorly quantified and represents the largest uncertainty in estimated forcing of climate change. Here we assess the effects of anthropogenic <span class="hlt">aerosols</span> on the Pacific storm track, using a multiscale global <span class="hlt">aerosol</span>-climate model (GCM). Simulations of two <span class="hlt">aerosol</span> scenarios corresponding to the present day and preindustrial conditions reveal long-range transport of anthropogenic <span class="hlt">aerosols</span> across the north Pacific and large resulting changes in the <span class="hlt">aerosol</span> optical depth, cloud droplet number concentration, and cloud and ice water paths. Shortwave and longwave cloud radiative forcing at the top of atmosphere are changed by -2.5 and +1.3 W m(-2), respectively, by emission changes from preindustrial to present day, and an increased cloud top <span class="hlt">height</span> indicates invigorated midlatitude cyclones. The overall increased precipitation and poleward heat transport reflect intensification of the Pacific storm track by anthropogenic <span class="hlt">aerosols</span>. Hence, this work provides, for the first time to the authors' knowledge, a global perspective of the effects of Asian pollution outflows from GCMs. Furthermore, our results suggest that the multiscale modeling framework is essential in producing the <span class="hlt">aerosol</span> invigoration effect of deep convective clouds on a global <span class="hlt">scale</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1020967','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1020967"><span><span class="hlt">Aerosol</span> synthesis of nano and micro-<span class="hlt">scale</span> zero valent metal particles from oxide precursors</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>Phillips, Jonathan; Luhrs, Claudia; Lesman, Zayd</p> <p>2010-01-01</p> <p>In this work a novel <span class="hlt">aerosol</span> method, derived form the batch Reduction/Expansion Synthesis (RES) method, for production of nano / micro-<span class="hlt">scale</span> metal particles from oxides and hydroxides is presented. In the <span class="hlt">Aerosol</span>-RES (A-RES) method, an <span class="hlt">aerosol</span>, consisting of a physical mixture of urea and metal oxide or hydroxides, is passed through a heated oven (1000 C) with a residence time of the order of 1 second, producing pure (zero valent) metal particles. It appears that the process is flexible regarding metal or alloy identity, allows control of particle size and can be readily <span class="hlt">scaled</span> to very large throughput. Current workmore » is focused on creating nanoparticles of metal and metal alloy using this method. Although this is primarily a report on observations, some key elements of the chemistry are clear. In particular, the reducing species produced by urea decomposition are the primary agents responsible for reduction of oxides and hydroxides to metal. It is also likely that the rapid expansion that takes place when solid/liquid urea decomposes to form gas species influences the final morphology of the particles.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24973611','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24973611"><span>Modeling vegetation <span class="hlt">heights</span> from high resolution stereo aerial photography: an application for broad-<span class="hlt">scale</span> rangeland monitoring.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gillan, Jeffrey K; Karl, Jason W; Duniway, Michael; Elaksher, Ahmed</p> <p>2014-11-01</p> <p>Vertical vegetation structure in rangeland ecosystems can be a valuable indicator for assessing rangeland health and monitoring riparian areas, post-fire recovery, available forage for livestock, and wildlife habitat. Federal land management agencies are directed to monitor and manage rangelands at landscapes <span class="hlt">scales</span>, but traditional field methods for measuring vegetation <span class="hlt">heights</span> are often too costly and time consuming to apply at these broad <span class="hlt">scales</span>. Most emerging remote sensing techniques capable of measuring surface and vegetation <span class="hlt">height</span> (e.g., LiDAR or synthetic aperture radar) are often too expensive, and require specialized sensors. An alternative remote sensing approach that is potentially more practical for managers is to measure vegetation <span class="hlt">heights</span> from digital stereo aerial photographs. As aerial photography is already commonly used for rangeland monitoring, acquiring it in stereo enables three-dimensional modeling and estimation of vegetation <span class="hlt">height</span>. The purpose of this study was to test the feasibility and accuracy of estimating shrub <span class="hlt">heights</span> from high-resolution (HR, 3-cm ground sampling distance) digital stereo-pair aerial images. Overlapping HR imagery was taken in March 2009 near Lake Mead, Nevada and 5-cm resolution digital surface models (DSMs) were created by photogrammetric methods (aerial triangulation, digital image matching) for twenty-six test plots. We compared the <span class="hlt">heights</span> of individual shrubs and plot averages derived from the DSMs to field measurements. We found strong positive correlations between field and image measurements for several metrics. Individual shrub <span class="hlt">heights</span> tended to be underestimated in the imagery, however, accuracy was higher for dense, compact shrubs compared with shrubs with thin branches. Plot averages of shrub <span class="hlt">height</span> from DSMs were also strongly correlated to field measurements but consistently underestimated. Grasses and forbs were generally too small to be detected with the resolution of the DSMs. Estimates of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhDT.........3W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhDT.........3W"><span>Interactions Between Atmospheric <span class="hlt">Aerosols</span> and Marine Boundary Layer Clouds on Regional and Global <span class="hlt">Scales</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, Zhen</p> <p></p> <p>Airborne <span class="hlt">aerosols</span> are crucial atmospheric constituents that are involved in global climate change and human life qualities. Understanding the nature and magnitude of <span class="hlt">aerosol</span>-cloud-precipitation interactions is critical in model predictions for atmospheric radiation budget and the water cycle. The interactions depend on a variety of factors including <span class="hlt">aerosol</span> physicochemical complexity, cloud types, meteorological and thermodynamic regimes and data processing techniques. This PhD work is an effort to quantify the relationships among <span class="hlt">aerosol</span>, clouds, and precipitation on both global and regional <span class="hlt">scales</span> by using satellite retrievals and aircraft measurements. The first study examines spatial distributions of conversion rate of cloud water to rainwater in warm maritime clouds over the globe by using NASA A-Train satellite data. This study compares the time <span class="hlt">scale</span> of the onset of precipitation with different <span class="hlt">aerosol</span> categories defined by values of <span class="hlt">aerosol</span> optical depth, fine mode fraction, and Angstrom Exponent. The results indicate that conversion time <span class="hlt">scales</span> are actually quite sensitive to lower tropospheric static stability (LTSS) and cloud liquid water path (LWP), in addition to <span class="hlt">aerosol</span> type. Analysis shows that tropical Pacific Ocean is dominated by the highest average conversion rate while subtropical warm cloud regions (far northeastern Pacific Ocean, far southeastern Pacific Ocean, Western Africa coastal area) exhibit the opposite result. Conversion times are mostly shorter for lower LTSS regimes. When LTSS condition is fixed, higher conversion rates coincide with higher LWP and lower <span class="hlt">aerosol</span> index categories. After a general global view of physical property quantifications, the rest of the presented PhD studies is focused on regional airborne observations, especially bulk cloud water chemistry and <span class="hlt">aerosol</span> aqueous-phase reactions during the summertime off the California coast. Local air mass origins are categorized into three distinct types (ocean, ships, and land</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020041485&hterms=air+asia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dair%2Basia','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020041485&hterms=air+asia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dair%2Basia"><span>Overview of ACE-Asia Spring 2001 Investigations on <span class="hlt">Aerosol</span> Radiative Effects and Related <span class="hlt">Aerosol</span> Properties</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Russell, Philip B.; Valero, F. P. J.; Flatau, P. J.; Bergin, M.; Holben, B.; Nakajima, T.; Pilewskie, P.; Bergstrom, R.; Hipskind, R. Stephen (Technical Monitor)</p> <p>2001-01-01</p> <p> depth gradient, with AOD(500 nm) extremes from 0.1 to 1.1. On the Pacific transit from Honolulu to Hachijo AOD(500 nm) averaged 0.2, including increases to 0.4 after several storms, suggesting the strong impact of wind-generated seasalt. The AOD maximum, found in the Sea of Japan, was influenced by dust and anthropogenic sources. (4) In Beijing, single scattering albedo retrieved from AERONET sun-sky radiometry yielded midvisible SSA=0.88 with strong wavelength dependence, suggesting a significant black carbon component. SSA retrieved during dust episodes was approx. 0.90 and variable but wavelength neutral reflecting the presence of urban haze with the dust. Downwind at Anmyon Island SSA was considerably higher, approx. 0.94, but wavelength neutral for dust episodes and spectrally dependent during non dust periods. (5) Satellite retrievals show major <span class="hlt">aerosol</span> features moving from Asia over the Pacific; however, determining seasonal-average <span class="hlt">aerosol</span> effects is hampered by sampling frequency and large-<span class="hlt">scale</span> cloud systems that obscure key parts of <span class="hlt">aerosol</span> patterns. Preliminary calculations using, satellite-retrieved AOD fields and initial ACE-Asia <span class="hlt">aerosol</span> properties (including sulfates, soot, and dust) yield clear-sky <span class="hlt">aerosol</span> radiative effects in the seasonal-average ACE-Asia plume exceeding those of manmade greenhouse gases. Quantifying all-sky direct <span class="hlt">aerosol</span> radiative effects is complicated by the need to define the <span class="hlt">height</span> of absorbing <span class="hlt">aerosols</span> with respect to cloud decks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26348650','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26348650"><span>Real-Time Characterization of <span class="hlt">Aerosol</span> Particle Composition above the Urban Canopy in Beijing: Insights into the Interactions between the Atmospheric Boundary Layer and <span class="hlt">Aerosol</span> Chemistry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sun, Yele; Du, Wei; Wang, Qingqing; Zhang, Qi; Chen, Chen; Chen, Yong; Chen, Zhenyi; Fu, Pingqing; Wang, Zifa; Gao, Zhiqiu; Worsnop, Douglas R</p> <p>2015-10-06</p> <p>Despite extensive efforts into the characterization of air pollution during the past decade, real-time characterization of <span class="hlt">aerosol</span> particle composition above the urban canopy in the megacity Beijing has never been performed to date. Here we conducted the first simultaneous real-time measurements of <span class="hlt">aerosol</span> composition at two different <span class="hlt">heights</span> at the same location in urban Beijing from December 19, 2013 to January 2, 2014. The nonrefractory submicron <span class="hlt">aerosol</span> (NR-PM1) species were measured in situ by a high-resolution <span class="hlt">aerosol</span> mass spectrometer at near-ground level and an <span class="hlt">aerosol</span> chemical speciation monitor at 260 m on a 325 m meteorological tower in Beijing. Secondary <span class="hlt">aerosol</span> showed similar temporal variations between ground level and 260 m, whereas much weaker correlations were found for the primary <span class="hlt">aerosol</span>. The diurnal evolution of the ratios and correlations of <span class="hlt">aerosol</span> species between 260 m and the ground level further illustrated a complex interaction between vertical mixing processes and local source emissions on <span class="hlt">aerosol</span> chemistry in the atmospheric boundary layer. As a result, the <span class="hlt">aerosol</span> compositions at the two <span class="hlt">heights</span> were substantially different. Organic <span class="hlt">aerosol</span> (OA), mainly composed of primary OA (62%), at the ground level showed a higher contribution to NR-PM1 (65%) than at 260 m (54%), whereas a higher concentration and contribution (15%) of nitrate was observed at 260 m, probably due to the favorable gas-particle partitioning under lower temperature conditions. In addition, two different boundary layer structures were observed, each interacting differently with the evolution processes of <span class="hlt">aerosol</span> chemistry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1324897-evaluation-aerosol-vertical-distribution-global-aerosol-models-through-comparison-against-caliop-measurements-aerocom-phase-ii-results-aerosol-profiles-aerocom-ii-gcm','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1324897-evaluation-aerosol-vertical-distribution-global-aerosol-models-through-comparison-against-caliop-measurements-aerocom-phase-ii-results-aerosol-profiles-aerocom-ii-gcm"><span>Evaluation of the <span class="hlt">aerosol</span> vertical distribution in global <span class="hlt">aerosol</span> models through comparison against CALIOP measurements: AeroCom phase II results: <span class="hlt">AEROSOL</span> PROFILES IN AEROCOM II GCM</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>Koffi, Brigitte; Schulz, Michael; Bréon, François-Marie</p> <p>2016-06-27</p> <p>The ability of eleven models in simulating the <span class="hlt">aerosol</span> vertical distribution from regional to global <span class="hlt">scales</span>, as part of the second phase of the AeroCom model inter-comparison initiative (AeroCom II) is assessed and compared to results of the first phase. The evaluation is performed using a global monthly gridded dataset of <span class="hlt">aerosol</span> extinction profiles built on purpose from the CALIOP (Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization) Layer Product 3.01. Results over 12 sub-continental regions show that five models improved whereas three degraded in reproducing the Zα 0-6 km mean extinction <span class="hlt">height</span> diagnostic, which is computed over the 0-6 km altitude rangemore » for each studied region and season. While the models’ performance remains highly variable, it has generally improved in terms of inter-regional diversity and seasonality. The biases in Zα 0-6 km have notably decreased in the U.S. and European industrial and downwind maritime regions, whereas the timing of the Zα 0-6 km peak season has improved for all but two models. However, most of the models now show a Zα 0-6 km underestimation over land, notably in the dust and biomass burning regions in Asia and Africa. At global <span class="hlt">scale</span>, the AeroCom II models better reproduce the Zα 0-6 km latitudinal variability over ocean than over land. Hypotheses for the (changes in the) the performance of the individual models and for the inter-model diversity are discussed. We also provide an analysis of the CALIOP limitations and uncertainties that can contribute to the differences between the simulations and observations.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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/2010APJAS..46..279Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010APJAS..46..279Y"><span>Regional-<span class="hlt">scale</span> relationships between <span class="hlt">aerosol</span> and summer monsoon circulation, and precipitation over northeast Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yoon, Soon-Chang; Kim, Sang-Woo; Choi, Suk-Jin; Choi, In-Jin</p> <p>2010-08-01</p> <p>We investigated the regional-<span class="hlt">scale</span> relationships between columnar <span class="hlt">aerosol</span> loads and summer monsoon circulation, and also the precipitation over northeast Asia using <span class="hlt">aerosol</span> optical depth (AOD) data obtained from the 8-year MODIS, AERONET Sun/sky radiometer, and precipitation data acquired under the Global Precipitation Climatology Project (GPCP). These high-quality data revealed the regional-<span class="hlt">scale</span> link between AOD and summer monsoon circulation, precipitation in July over northeast Asian countries, and their distinct spatial and annual variabilities. Compared to the mean AOD for the entire period of 2001-2008, the increase of almost 40-50% in the AOD value in July 2005 and July 2007 was found over the downwind regions of China (Yellow Sea, Korean peninsula, and East Sea), with negative precipitation anomalies. This can be attributable to the strong westerly confluent flows, between cyclone flows by continental thermal low centered over the northern China and anticyclonic flows by the western North Pacific High, which transport anthropogenic pollution <span class="hlt">aerosols</span> emitted from east China to aforementioned downwind high AOD regions along the rim of the Pacific marine airmass. In July 2002, however, the easterly flows transported anthropogenic <span class="hlt">aerosols</span> from east China to the southwestern part of China in July 2002. As a result, the AOD off the coast of China was dramatically reduced in spite of decreasing rainfall. From the calculation of the cross-correlation coefficient between MODIS-derived AOD anomalies and GPCP precipitation anomalies in July over the period 2001-2008, we found negative correlations over the areas encompassed by 105-115°E and 30-35°N and by 120-140°E and 35-40°N (Yellow Sea, Korean peninsula, and East Sea). This suggests that <span class="hlt">aerosol</span> loads over these regions are easily influenced by the Asian monsoon flow system and associated precipitation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CG....109..216R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CG....109..216R"><span>A continuous <span class="hlt">scale</span>-space method for the automated placement of spot <span class="hlt">heights</span> on maps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rocca, Luigi; Jenny, Bernhard; Puppo, Enrico</p> <p>2017-12-01</p> <p>Spot <span class="hlt">heights</span> and soundings explicitly indicate terrain elevation on cartographic maps. Cartographers have developed design principles for the manual selection, placement, labeling, and generalization of spot <span class="hlt">height</span> locations, but these processes are work-intensive and expensive. Finding an algorithmic criterion that matches the cartographers' judgment in ranking the significance of features on a terrain is a difficult endeavor. This article proposes a method for the automated selection of spot <span class="hlt">heights</span> locations representing natural features such as peaks, saddles and depressions. A lifespan of critical points in a continuous <span class="hlt">scale</span>-space model is employed as the main measure of the importance of features, and an algorithm and a data structure for its computation are described. We also introduce a method for the comparison of algorithmically computed spot <span class="hlt">height</span> locations with manually produced reference compilations. The new method is compared with two known techniques from the literature. Results show spot <span class="hlt">height</span> locations that are closer to reference spot <span class="hlt">heights</span> produced manually by swisstopo cartographers, compared to previous techniques. The introduced method can be applied to elevation models for the creation of topographic and bathymetric maps. It also ranks the importance of extracted spot <span class="hlt">height</span> locations, which allows for a variation in the size of symbols and labels according to the significance of represented features. The importance ranking could also be useful for adjusting spot <span class="hlt">height</span> density of zoomable maps in real time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050156624&hterms=climate+effect+black+carbon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dclimate%2Beffect%2Bblack%2Bcarbon','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050156624&hterms=climate+effect+black+carbon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dclimate%2Beffect%2Bblack%2Bcarbon"><span>Effects of <span class="hlt">Aerosol</span> on Atmospheric Dynamics and Hydrologic Processes During Boreal Spring and Summer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lau, William K. M.; Kim, M. K.; Kim, K. M.; Chin, Mian</p> <p>2005-01-01</p> <p>Global and regional climate impacts of present-day <span class="hlt">aerosol</span> loading during boreal spring are investigated using the NASA finite volume General Circulation Model (fvGCM). Three-dimensional distributions of loadings of five species of tropospheric <span class="hlt">aerosols</span>, i.e., sulfate, black carbon, organic carbon, soil dust, and sea salt are prescribed from outputs of the Goddard Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport model (GOCART). The <span class="hlt">aerosol</span> loadings are used to calculate the extinction coefficient, single scattering albedo, and asymmetric factor at eleven spectral wavelengths in the radiative transfer code. We find that <span class="hlt">aerosol</span>-radiative forcing during boreal spring excites a wavetrain-like pattern in tropospheric temperature and geopotential <span class="hlt">height</span> that emanates from Northern Africa, through Eurasia, to northeastern Pacific. Associated with the teleconnection is strong surface cooling over regions with large <span class="hlt">aerosol</span> loading, i.e., China, India, and Africa. Low-to-mid tropospheric heating due to shortwave absorption is found in regions with large loading of dust (Northern Africa, and central East Asia), and black carbon (South and East Asia). In addition pronounced surface cooling is found over the Caspian Sea and warming over Eurasian and northeastern Asia, where <span class="hlt">aerosol</span> loadings are relatively low. These warming and cooling are components of teleconnection pattern produced primarily by atmospheric heating from absorbing <span class="hlt">aerosols</span>, i.e., dust from North Africa and black carbon from South and East Asia. Effects of <span class="hlt">aerosols</span> on atmospheric hydrologic cycle in the Asian monsoon region are also investigated. Results show that absorbing <span class="hlt">aerosols</span>, i.e., black carbon and dust, induce large-<span class="hlt">scale</span> upper-level heating anomaly over the Tibetan Plateau in April and May, ushering in an early onset of the Indian summer monsoon. Absorbing <span class="hlt">aerosols</span> also enhance lower-level heating and anomalous ascent over northern India, intensifying the Indian monsoon. Overall, the <span class="hlt">aerosol</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050071095&hterms=climate+effect+black+carbon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dclimate%2Beffect%2Bblack%2Bcarbon','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050071095&hterms=climate+effect+black+carbon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dclimate%2Beffect%2Bblack%2Bcarbon"><span>Effects of <span class="hlt">Aerosol</span> on Atmospheric Dynamics and Hydrologic Processes during Boreal Spring and Summer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lau, William K. M.; Kim, M. K.; Chin, Mian; Kim, K. M.</p> <p>2005-01-01</p> <p>Global and regional climate impacts of present-day <span class="hlt">aerosol</span> loading during boreal spring are investigated using the NASA finite volume General Circulation Model (fvGCM). Three-dimensional distributions of loadings of five species of tropospheric <span class="hlt">aerosols</span>, i.e., sulfate, black carbon, organic carbon, soil dust, and sea salt are prescribed from outputs of the Goddard Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport model (GOCART). The <span class="hlt">aerosol</span> loadings are used to calculate the extinction coefficient, single scattering albedo, and asymmetric factor at eleven spectral wavelengths in the radiative transfer code. We find that <span class="hlt">aerosol</span>-radiative forcing during boreal spring excites a wavetrain-like pattern in tropospheric temperature and geopotential <span class="hlt">height</span> that emanates from Northern Africa, through Eurasia, to northeastern Pacific. Associated with the teleconnection is strong surface cooling over regions with large <span class="hlt">aerosol</span> loading, i.e., China, India, and Africa. Low-to-mid tropospheric heating due to shortwave absorption is found in regions with large loading of dust (Northern Africa, and central East Asia), and black carbon (South and East Asia). In addition pronounced surface cooling is found over the Caspian Sea and warming over Eurasian and northeastern Asia, where <span class="hlt">aerosol</span> loadings are relatively low. These warming and cooling are components of teleconnection pattern produced primarily by atmospheric heating from absorbing <span class="hlt">aerosols</span>, i.e., dust from North Africa and.black carbon from South and East Asia. Effects of <span class="hlt">aerosols</span> on atmospheric hydrologic cycle in the Asian monsoon region are also investigated. Results show that absorbing <span class="hlt">aerosols</span>, i.e., black carbon and dust, induce large-<span class="hlt">scale</span> upper-level heating anomaly over the Tibetan Plateau in April and May, ushering in an early onset of the Indian summer monsoon. Absorbing <span class="hlt">aerosols</span> also enhance lower-level heating and anomalous ascent over northern India, intensifying the Indian monsoon. Overall, the <span class="hlt">aerosol</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1032685-assessing-regional-scale-predictions-aerosols-marine-stratocumulus-interactions-during-vocals-rex-using-wrf-chem','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1032685-assessing-regional-scale-predictions-aerosols-marine-stratocumulus-interactions-during-vocals-rex-using-wrf-chem"><span>Assessing regional <span class="hlt">scale</span> predictions of <span class="hlt">aerosols</span>, marine stratocumulus, and their interactions during VOCALS-REx using WRF-Chem</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>Yang, Qing; Gustafson, William I.; Fast, Jerome D.</p> <p>2011-12-02</p> <p>In the recent chemistry version (v3.3) of the Weather Research and Forecasting (WRF-Chem) model, we have coupled the Morrison double-moment microphysics scheme with interactive <span class="hlt">aerosols</span> so that full two-way <span class="hlt">aerosol</span>-cloud interactions are included in simulations. We have used this new WRF-Chem functionality in a study focused on assessing predictions of <span class="hlt">aerosols</span>, marine stratocumulus clouds, and their interactions over the Southeast Pacific using measurements from the VAMOS Ocean-Cloud-Atmosphere-Land Study Regional Experiment (VOCALS-REx) and satellite retrievals. This study also serves as a detailed analysis of our WRF-Chem simulations contributed to the VOCALS model Assessment (VOCA) project. The WRF-Chem 31-day (October 15-November 16,more » 2008) simulation with <span class="hlt">aerosol</span>-cloud interactions (AERO hereafter) is also compared to a simulation (MET hereafter) with fixed cloud droplet number concentrations assumed by the default in Morrison microphysics scheme with no interactive <span class="hlt">aerosols</span>. The well-predicted <span class="hlt">aerosol</span> properties such as number, mass composition, and optical depth lead to significant improvements in many features of the predicted stratocumulus clouds: cloud optical properties and microphysical properties such as cloud top effective radius, cloud water path, and cloud optical thickness, and cloud macrostructure such as cloud depth and cloud base <span class="hlt">height</span>. These improvements in addition to the <span class="hlt">aerosol</span> direct and semi-direct effects, in turn, feed back to the prediction of boundary-layer characteristics and energy budgets. Particularly, inclusion of interactive <span class="hlt">aerosols</span> in AERO strengths temperature and humidity gradients within capping inversion layer and lowers the MBL depth by 150 m from that of the MET simulation. Mean top-of-the-atmosphere outgoing shortwave fluxes, surface latent heat, and surface downwelling longwave fluxes are in better agreement with observations in AERO, compared to the MET simulation. Nevertheless, biases in some of the simulated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040171165&hterms=date+palm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddate%2Bpalm','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040171165&hterms=date+palm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Ddate%2Bpalm"><span>Cloud and <span class="hlt">Aerosol</span> Measurements from the GLAS Polar Orbiting Lidar: First Year Results</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spinhirne, J. D.; Palm, S. P.; Hlavka, D. L.; Hart, W. D.; Mahesh, A.; Welton, E. J.</p> <p>2004-01-01</p> <p>The Geoscience Laser Altimeter System (GLAS) launched in 2003 is the first polar orbiting satellite lidar. The instrument was designed for high performance observations of the distribution and optical scattering cross sections of clouds and <span class="hlt">aerosol</span>. GLAS is approaching six months of on orbit data operation. These data from thousands of orbits illustrate the ability of space lidar to accurately and dramatically measure the <span class="hlt">height</span> distribution of global cloud and <span class="hlt">aerosol</span> to an unprecedented degree. There were many intended science applications of the GLAS data and significant results have already been realized. One application is the accurate <span class="hlt">height</span> distribution and coverage of global cloud cover with one goal of defining the limitation and inaccuracies of passive retrievals. Comparison to MODIS cloud retrievals shows notable discrepancies. Initial comparisons to NOAA 14&15 satellite cloud retrievals show basic similarity in overall cloud coverage, but important differences in <span class="hlt">height</span> distribution. Because of the especially poor performance of passive cloud retrievals in polar regions, and partly because of high orbit track densities, the GLAS measurements are by far the most accurate measurement of Arctic and Antarctica cloud cover from space to date. Global <span class="hlt">aerosol</span> <span class="hlt">height</span> profiling is a fundamentally new measurement from space with multiple applications. A most important <span class="hlt">aerosol</span> application is providing input to global <span class="hlt">aerosol</span> generation and transport models. Another is improved measurement of <span class="hlt">aerosol</span> optical depth. Oceanic surface energy flux derivation from PBL and LCL <span class="hlt">height</span> measurements is another application of GLAS data that is being pursued. A special area of work for GLAS data is the correction and application of multiple scattering effects. Stretching of surface return pulses in excess of 40 m from cloud propagation effects and other interesting multiple scattering phenomena have been observed. As an EOS project instrument, GLAS data products are openly</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1184894-new-wrf-chem-treatment-studying-regional-scale-impacts-cloud-aerosol-interactions-parameterized-cumuli','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1184894-new-wrf-chem-treatment-studying-regional-scale-impacts-cloud-aerosol-interactions-parameterized-cumuli"><span>A New WRF-Chem Treatment for Studying Regional <span class="hlt">Scale</span> Impacts of Cloud-<span class="hlt">Aerosol</span> Interactions in Parameterized Cumuli</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>Berg, Larry K.; Shrivastava, ManishKumar B.; Easter, Richard C.</p> <p></p> <p>A new treatment of cloud-<span class="hlt">aerosol</span> interactions within parameterized shallow and deep convection has been implemented in WRF-Chem that can be used to better understand the <span class="hlt">aerosol</span> lifecycle over regional to synoptic <span class="hlt">scales</span>. The modifications to the model to represent cloud-<span class="hlt">aerosol</span> interactions include treatment of the cloud dropletnumber mixing ratio; key cloud microphysical and macrophysical parameters (including the updraft fractional area, updraft and downdraft mass fluxes, and entrainment) averaged over the population of shallow clouds, or a single deep convective cloud; and vertical transport, activation/resuspension, aqueous chemistry, and wet removal of <span class="hlt">aerosol</span> and trace gases in warm clouds. Thesechanges have beenmore » implemented in both the WRF-Chem chemistry packages as well as the Kain-Fritsch cumulus parameterization that has been modified to better represent shallow convective clouds. Preliminary testing of the modified WRF-Chem has been completed using observations from the Cumulus Humilis <span class="hlt">Aerosol</span> Processing Study (CHAPS) as well as a high-resolution simulation that does not include parameterized convection. The simulation results are used to investigate the impact of cloud-<span class="hlt">aerosol</span> interactions on the regional <span class="hlt">scale</span> transport of black carbon (BC), organic <span class="hlt">aerosol</span> (OA), and sulfate <span class="hlt">aerosol</span>. Based on the simulations presented here, changes in the column integrated BC can be as large as -50% when cloud-<span class="hlt">aerosol</span> interactions are considered (due largely to wet removal), or as large as +35% for sulfate in non-precipitating conditions due to the sulfate production in the parameterized clouds. The modifications to WRF-Chem version 3.2.1 are found to account for changes in the cloud drop number concentration (CDNC) and changes in the chemical composition of cloud-drop residuals in a way that is consistent with observations collected during CHAPS. Efforts are currently underway to port the changes described here to WRF-Chem version 3.5, and it is anticipated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4024913','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4024913"><span>Assessing the effects of anthropogenic <span class="hlt">aerosols</span> on Pacific storm track using a multiscale global climate model</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wang, Yuan; Wang, Minghuai; Zhang, Renyi; Ghan, Steven J.; Lin, Yun; Hu, Jiaxi; Pan, Bowen; Levy, Misti; Jiang, Jonathan H.; Molina, Mario J.</p> <p>2014-01-01</p> <p>Atmospheric <span class="hlt">aerosols</span> affect weather and global general circulation by modifying cloud and precipitation processes, but the magnitude of cloud adjustment by <span class="hlt">aerosols</span> remains poorly quantified and represents the largest uncertainty in estimated forcing of climate change. Here we assess the effects of anthropogenic <span class="hlt">aerosols</span> on the Pacific storm track, using a multiscale global aerosol–climate model (GCM). Simulations of two <span class="hlt">aerosol</span> scenarios corresponding to the present day and preindustrial conditions reveal long-range transport of anthropogenic <span class="hlt">aerosols</span> across the north Pacific and large resulting changes in the <span class="hlt">aerosol</span> optical depth, cloud droplet number concentration, and cloud and ice water paths. Shortwave and longwave cloud radiative forcing at the top of atmosphere are changed by −2.5 and +1.3 W m−2, respectively, by emission changes from preindustrial to present day, and an increased cloud top <span class="hlt">height</span> indicates invigorated midlatitude cyclones. The overall increased precipitation and poleward heat transport reflect intensification of the Pacific storm track by anthropogenic <span class="hlt">aerosols</span>. Hence, this work provides, for the first time to the authors’ knowledge, a global perspective of the effects of Asian pollution outflows from GCMs. Furthermore, our results suggest that the multiscale modeling framework is essential in producing the <span class="hlt">aerosol</span> invigoration effect of deep convective clouds on a global <span class="hlt">scale</span>. PMID:24733923</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70047368','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70047368"><span>Integrating disparate lidar data at the national <span class="hlt">scale</span> to assess the relationships between <span class="hlt">height</span> above ground, land cover and ecoregions</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Stoker, Jason M.; Cochrane, Mark A.; Roy, David P.</p> <p>2013-01-01</p> <p>With the acquisition of lidar data for over 30 percent of the US, it is now possible to assess the three-dimensional distribution of features at the national <span class="hlt">scale</span>. This paper integrates over 350 billion lidar points from 28 disparate datasets into a national-<span class="hlt">scale</span> database and evaluates if <span class="hlt">height</span> above ground is an important variable in the context of other nationalscale layers, such as the US Geological Survey National Land Cover Database and the US Environmental Protection Agency ecoregions maps. While the results were not homoscedastic and the available data did not allow for a complete <span class="hlt">height</span> census in any of the classes, it does appear that where lidar data were used, there were detectable differences in <span class="hlt">heights</span> among many of these national classification schemes. This study supports the hypothesis that there were real, detectable differences in <span class="hlt">heights</span> in certain national-<span class="hlt">scale</span> classification schemes, despite <span class="hlt">height</span> not being a variable used in any of the classification routines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A23L..03P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A23L..03P"><span><span class="hlt">Aerosol</span> Climate Time Series Evaluation In ESA <span class="hlt">Aerosol</span>_cci</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popp, T.; de Leeuw, G.; Pinnock, S.</p> <p>2015-12-01</p> <p>Within the ESA Climate Change Initiative (CCI) <span class="hlt">Aerosol</span>_cci (2010 - 2017) conducts intensive work to improve algorithms for the retrieval of <span class="hlt">aerosol</span> information from European sensors. By the end of 2015 full mission time series of 2 GCOS-required <span class="hlt">aerosol</span> parameters are completely validated and released: <span class="hlt">Aerosol</span> Optical Depth (AOD) from dual view ATSR-2 / AATSR radiometers (3 algorithms, 1995 - 2012), and stratospheric extinction profiles from star occultation GOMOS spectrometer (2002 - 2012). Additionally, a 35-year multi-sensor time series of the qualitative Absorbing <span class="hlt">Aerosol</span> Index (AAI) together with sensitivity information and an AAI model simulator is available. Complementary <span class="hlt">aerosol</span> properties requested by GCOS are in a "round robin" phase, where various algorithms are inter-compared: fine mode AOD, mineral dust AOD (from the thermal IASI spectrometer), absorption information and <span class="hlt">aerosol</span> layer <span class="hlt">height</span>. As a quasi-reference for validation in few selected regions with sparse ground-based observations the multi-pixel GRASP algorithm for the POLDER instrument is used. Validation of first dataset versions (vs. AERONET, MAN) and inter-comparison to other satellite datasets (MODIS, MISR, SeaWIFS) proved the high quality of the available datasets comparable to other satellite retrievals and revealed needs for algorithm improvement (for example for higher AOD values) which were taken into account for a reprocessing. The datasets contain pixel level uncertainty estimates which are also validated. The paper will summarize and discuss the results of major reprocessing and validation conducted in 2015. The focus will be on the ATSR, GOMOS and IASI datasets. Pixel level uncertainties validation will be summarized and discussed including unknown components and their potential usefulness and limitations. Opportunities for time series extension with successor instruments of the Sentinel family will be described and the complementarity of the different satellite <span class="hlt">aerosol</span> products</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.2949S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.2949S"><span><span class="hlt">Aerosol</span> optical characteristics and their vertical distributions under enhanced haze pollution events: effect of the regional transport of different <span class="hlt">aerosol</span> types over eastern China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Tianze; Che, Huizheng; Qi, Bing; Wang, Yaqiang; Dong, Yunsheng; Xia, Xiangao; Wang, Hong; Gui, Ke; Zheng, Yu; Zhao, Hujia; Ma, Qianli; Du, Rongguang; Zhang, Xiaoye</p> <p>2018-03-01</p> <p>The climatological variation of <span class="hlt">aerosol</span> properties and the planetary boundary layer (PBL) during 2013-2015 over the Yangtze River Delta (YRD) region were investigated by employing ground-based Micro Pulse Lidar (MPL) and CE-318 sun-photometer observations. Combining Moderate Resolution Imaging Spectroradiometer (MODIS) and Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) satellite products, enhanced haze pollution events affected by different types of <span class="hlt">aerosol</span> over the YRD region were analyzed through vertical structures, spatial distributions, backward trajectories, and the potential source contribution function (PSCF) model. The results show that <span class="hlt">aerosols</span> in the YRD are dominated by fine-mode particles, except in March. The <span class="hlt">aerosol</span> optical depth (AOD) in June and September is higher due to high single scattering albedo (SSA) from hygroscopic growth, but it is lower in July and August due to wet deposition from precipitation. The PBL <span class="hlt">height</span> (PBLH) is greater (means ranging from 1.23 to 1.84 km) and more variable in the warmer months of March to August, due to the stronger diurnal cycle and exchange of heat. Northern fine-mode pollutants are brought to the YRD at a <span class="hlt">height</span> of 1.5 km. The SSA increases, blocking the radiation to the surface, and cooling the surface, thereby weakening turbulence, lowering the PBL, and in turn accelerating the accumulation of pollutants, creating a feedback to the cooling effect. Originated from the deserts in Xinjiang and Inner Mongolia, long-range transported dust masses are seen at <span class="hlt">heights</span> of about 2 km over the YRD region with an SSA440 nm below 0.84, which heat air and raise the PBL, accelerating the diffusion of dust particles. Regional transport from biomass-burning spots to the south of the YRD region bring mixed <span class="hlt">aerosol</span> particles at a <span class="hlt">height</span> below 1.5 km, resulting in an SSA440 nm below 0.89. During the winter, the accumulation of the local emission layer is facilitated by stable weather conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=235326&keyword=european+AND+journal&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=235326&keyword=european+AND+journal&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>Trace Gas/<span class="hlt">Aerosol</span> Boundary Concentrations and their Impacts on Continental-<span class="hlt">scale</span> AQMEII Modelling Domains</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>Over twenty modeling groups are participating in the Air Quality Model Evaluation International Initiative (AQMEII) in which a variety of mesoscale photochemical and <span class="hlt">aerosol</span> air quality modeling systems are being applied to continental-<span class="hlt">scale</span> domains in North America and Europe fo...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050180337','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050180337"><span>Atmospheric Teleconnection over Eurasia Induced by <span class="hlt">Aerosol</span> Radiative Forcing During Boreal Spring</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, Maeng-Ki; Lau, K. M.; Chin, Mian; Kim, Kyu-Myong; Sud, Y. C.; Walker, Greg K.</p> <p>2005-01-01</p> <p>The direct effects of <span class="hlt">aerosols</span> on global and regional climate during boreal spring are investigated based on simulations using the NASA Global Modeling and Assimilation Office (GMAO) finite-volume general circulation model (fvGCM) with Microphyics of clouds in Relaxed Arakawa Schubert Scheme (McRAS). The <span class="hlt">aerosol</span> loading are prescribed from three-dimensional monthly distribution of tropospheric <span class="hlt">aerosols</span> viz., sulfate, black carbon, organic carbon, soil dust, and sea salt from output of the Goddard Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport model (GOCART). The <span class="hlt">aerosol</span> extinction coefficient, single scattering albedo, and asymmetric factor are computed as wavelength-dependent radiative forcing in the radiative transfer scheme of the fvGCM, and as a function of the <span class="hlt">aerosol</span> loading and ambient relative humidity. We find that anomalous atmospheric heat sources induced by absorbing <span class="hlt">aerosols</span> (dust and black carbon) excites a planetary <span class="hlt">scale</span> teleconnection pattern in sea level pressure, temperature and geopotential <span class="hlt">height</span> spanning North Africa through Eurasia to the North Pacific. Surface cooling due to direct effects of <span class="hlt">aerosols</span> is found in the vicinity and downstream of the <span class="hlt">aerosol</span> source regions, i.e., South Asia, East Asia, and northern and western Africa. Additionally, atmospheric heating is found in regions with large loading of dust (over Northern Africa, and Middle East), and black carbon (over South-East Asia). Paradoxically, the most pronounced feature in <span class="hlt">aerosol</span>-induced surface temperature is an east-west dipole anomaly with strong cooling over the Caspian Sea, and warming over central and northeastern Asia, where <span class="hlt">aerosol</span> concentration are low. Analyses of circulation anomalies show that the dipole anomaly is a part of an atmospheric teleconnection driven by atmospheric heating anomalies induced by absorbing <span class="hlt">aerosols</span> in the source regions, but the influence was conveyed globally through barotropic energy dispersion and sustained by feedback processes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JASS...32..311P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JASS...32..311P"><span>Vertical <span class="hlt">Scale</span> <span class="hlt">Height</span> of the Topside Ionosphere Around the Korean Peninsula: Estimates from Ionosondes and the Swarm Constellation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, Jaeheung; Kwak, Young-Sil; Mun, Jun-Chul; Min, Kyoung-Wook</p> <p>2015-12-01</p> <p>In this study, we estimated the topside <span class="hlt">scale</span> <span class="hlt">height</span> of plasma density (Hm) using the Swarm constellation and ionosondes in Korea. The Hm above Korean Peninsula is generally around 50 km. Statistical distributions of the topside <span class="hlt">scale</span> <span class="hlt">height</span> exhibited a complex dependence upon local time and season. The results were in general agreement with those of Tulasi Ram et al. (2009), who used the same method to calculate the topside <span class="hlt">scale</span> <span class="hlt">height</span> in a mid-latitude region. On the contrary, our results did not fully coincide with those obtained by Liu et al. (2007), who used electron density profiles from Arecibo Incoherent Scatter Radar (ISR) between 1966 and 2002. The disagreement may result from the limitations in our approximation method and data coverage used for estimations, as well as the inherent dependence of Hm on Geographic LONgitude (GLON).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009ACPD....921619M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ACPD....921619M"><span>Recent increase in <span class="hlt">aerosol</span> loading over the Australian arid zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitchell, R. M.; Campbell, S. K.; Qin, Y.</p> <p>2009-10-01</p> <p>Collocated sun photometer and nephelometer measurements at Tinga Tingana in the Australian Outback over the decade 1997-2007 show a significant increase in <span class="hlt">aerosol</span> loading following the onset of severe drought conditions in 2002. The mean mid-visible scattering coefficient obtained from nephelometer measurements over the period 2003-2007 is approximately double that recorded over the preceding 5 yr, with consistent trends in the column <span class="hlt">aerosol</span> optical depth derived from the sun photometer. This increase is confined to the season of dust activity, particularly September to March. In contrast, background <span class="hlt">aerosol</span> levels during May, June and July remained stable. The enhanced <span class="hlt">aerosol</span> loadings during the latter 5 yr of the study period can be understood as a combination of dune destabilisation through loss of ephemeral vegetation and surface crust, and the changing supply of fluvial sediments to ephemeral lakes and floodplains within the Lake Eyre Basin. Major dust outbreaks are generally highly localised, although significant dust activity was observed at Tinga Tingana on 50% of days when a major event occurred elsewhere in the Lake Eyre Basin, suggesting frequent basin-wide dust mobilisation. Combined analysis of <span class="hlt">aerosol</span> optical depth and scattering coefficient shows weak correlation between the surface and column <span class="hlt">aerosol</span> (R2=0.24). The <span class="hlt">aerosol</span> <span class="hlt">scale</span> <span class="hlt">height</span> is broadly distributed with a mode typically between 2-3 km, with clearly defined seasonal variation. Climatological analysis reveals bimodal structure in the annual cycle of <span class="hlt">aerosol</span> optical depth, with a summer peak related to maximal dust activity, and a spring peak related to lofted fine-mode <span class="hlt">aerosol</span>. There is evidence for an increase in near-surface <span class="hlt">aerosol</span> during the period 2003-2007 relative to 1997-2002, consistent with an increase in dust activity. This accords with an independent finding of increasing <span class="hlt">aerosol</span> loading over the Australian region as a whole, suggesting that rising dust activity over the Lake</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.7994M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.7994M"><span>Variation of <span class="hlt">aerosol</span> characteristics in the detail <span class="hlt">scale</span> of time and space</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukai, S.; Nakata, M.; Sano, I.</p> <p>2012-04-01</p> <p>-Osaka. We guess dust <span class="hlt">aerosols</span> are transported over the mountains because dust <span class="hlt">aerosols</span> exist higher than usual. In order to investigate change of <span class="hlt">aerosol</span> properties before and after dust event, we analyze particulate matter with scanning electron microscope (SEM) coupled with energy dispersive X-ray analyzer (EDX). It is found from the <span class="hlt">scaling</span> of particle size and ratio of major and minor axis for PM2.5 sampling on 21 March, 2010 when dust event occurred that at the peak of dust event nonspherical particles with large particle size are dominant. A componential analysis also presents temporal variation of <span class="hlt">aerosol</span> properties. Sulfur is major component before dust comes but Si becomes major component with dust event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23013157','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23013157"><span><span class="hlt">Aerosols</span> from fires: an examination of the effects on ozone photochemistry in the Western United States.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jiang, Xiaoyan; Wiedinmyer, Christine; Carlton, Annmarie G</p> <p>2012-11-06</p> <p>This study presents a first attempt to investigate the roles of fire <span class="hlt">aerosols</span> in ozone (O(3)) photochemistry using an online coupled meteorology-chemistry model, the Weather Research and Foresting model with Chemistry (WRF-Chem). Four 1-month WRF-Chem simulations for August 2007, with and without fire emissions, were carried out to assess the sensitivity of O(3) predictions to the emissions and subsequent radiative feedbacks associated with large-<span class="hlt">scale</span> fires in the Western United States (U.S.). Results show that decreases in planetary boundary layer <span class="hlt">height</span> (PBLH) resulting from the radiative effects of fire <span class="hlt">aerosols</span> and increases in emissions of nitrogen oxides (NO(x)) and volatile organic compounds (VOCs) from the fires tend to increase modeled O(3) concentrations near the source. Reductions in downward shortwave radiation reaching the surface and surface temperature due to fire <span class="hlt">aerosols</span> cause decreases in biogenic isoprene emissions and J(NO(2)) photolysis rates, resulting in reductions in O(3) concentrations by as much as 15%. Thus, the results presented in this study imply that considering the radiative effects of fire <span class="hlt">aerosols</span> may reduce O(3) overestimation by traditional photochemical models that do not consider fire-induced changes in meteorology; implementation of coupled meteorology-chemistry models are required to simulate the atmospheric chemistry impacted by large-<span class="hlt">scale</span> fires.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4254P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4254P"><span><span class="hlt">Aerosol</span> Climate Time Series in ESA <span class="hlt">Aerosol</span>_cci</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popp, Thomas; de Leeuw, Gerrit; Pinnock, Simon</p> <p>2016-04-01</p> <p>Within the ESA Climate Change Initiative (CCI) <span class="hlt">Aerosol</span>_cci (2010 - 2017) conducts intensive work to improve algorithms for the retrieval of <span class="hlt">aerosol</span> information from European sensors. Meanwhile, full mission time series of 2 GCOS-required <span class="hlt">aerosol</span> parameters are completely validated and released: <span class="hlt">Aerosol</span> Optical Depth (AOD) from dual view ATSR-2 / AATSR radiometers (3 algorithms, 1995 - 2012), and stratospheric extinction profiles from star occultation GOMOS spectrometer (2002 - 2012). Additionally, a 35-year multi-sensor time series of the qualitative Absorbing <span class="hlt">Aerosol</span> Index (AAI) together with sensitivity information and an AAI model simulator is available. Complementary <span class="hlt">aerosol</span> properties requested by GCOS are in a "round robin" phase, where various algorithms are inter-compared: fine mode AOD, mineral dust AOD (from the thermal IASI spectrometer, but also from ATSR instruments and the POLDER sensor), absorption information and <span class="hlt">aerosol</span> layer <span class="hlt">height</span>. As a quasi-reference for validation in few selected regions with sparse ground-based observations the multi-pixel GRASP algorithm for the POLDER instrument is used. Validation of first dataset versions (vs. AERONET, MAN) and inter-comparison to other satellite datasets (MODIS, MISR, SeaWIFS) proved the high quality of the available datasets comparable to other satellite retrievals and revealed needs for algorithm improvement (for example for higher AOD values) which were taken into account for a reprocessing. The datasets contain pixel level uncertainty estimates which were also validated and improved in the reprocessing. For the three ATSR algorithms the use of an ensemble method was tested. The paper will summarize and discuss the status of dataset reprocessing and validation. The focus will be on the ATSR, GOMOS and IASI datasets. Pixel level uncertainties validation will be summarized and discussed including unknown components and their potential usefulness and limitations. Opportunities for time series extension</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A23E0317D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A23E0317D"><span><span class="hlt">Aerosol</span> Activation Properties within and above Mixing Layer in the North China Plain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deng, Z.; Ran, L.</p> <p>2013-12-01</p> <p><span class="hlt">Aerosol</span> particles, serving as cloud condensation nuclei (CCN), may modify the properties of clouds and have an impact on climate. The vertical distribution of <span class="hlt">aerosols</span> and their activation properties is critical to quantify the effect of <span class="hlt">aerosols</span> on clouds. An intensive field campaign, Vertical Observations of trace Gases and <span class="hlt">Aerosols</span> in the North China Plain (VOGA-NCP 2013), was conducted in the North China Plain during the late July and early August 2013 to measure the vertical profiles of atmospheric components in this polluted region and estimate their effects on atmospheric environment and climate. <span class="hlt">Aerosols</span> were measured with in-situ instruments and Lidar. Particularly, the <span class="hlt">aerosols</span> were collected at 1000 m <span class="hlt">height</span> with a 1 m3 bag sampler attached to a tethered balloon, and subsequently measured with combined scanning mobility particle sizer (SMPS) and CCN counter. Comparisons of size-resolved activation ratios at ground level and 1000 m <span class="hlt">height</span> showed that <span class="hlt">aerosols</span> in upper atmosphere were not only less concentrated, but also less CCN-active than those at the surface. The difference in <span class="hlt">aerosol</span> properties between upper atmosphere and the ground indicates that the analysis of impacts of <span class="hlt">aerosols</span> on cloud might be misleading in heavily polluted region based on the relationship of cloud properties and surface <span class="hlt">aerosols</span> or column without considering the vertical distribution of <span class="hlt">aerosol</span> activation abilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACP....1011459G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACP....1011459G"><span>A critical look at spatial <span class="hlt">scale</span> choices in satellite-based <span class="hlt">aerosol</span> indirect effect studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grandey, B. S.; Stier, P.</p> <p>2010-12-01</p> <p>Analysing satellite datasets over large regions may introduce spurious relationships between <span class="hlt">aerosol</span> and cloud properties due to spatial variations in <span class="hlt">aerosol</span> type, cloud regime and synoptic regime climatologies. Using MODerate resolution Imaging Spectroradiometer data, we calculate relationships between <span class="hlt">aerosol</span> optical depth τa derived liquid cloud droplet effective number concentration Ne and liquid cloud droplet effective radius re at different spatial <span class="hlt">scales</span>. Generally, positive values of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: 10px; color: #000;">dlnNe<span style="margin-left: -3em; margin-right: .5em; vertical-align: -15%; font-size: 10px; color: #000;">dlnτa are found for ocean regions, whilst negative values occur for many land regions. The spatial distribution of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: 10px; color: #000;">dlnre<span style="margin-left: -2.7em; margin-right: .5em; vertical-align: -15%; font-size: 10px; color: #000;">dlnτa shows approximately the opposite pattern, with generally postive values for land regions and negative values for ocean regions. We find that for region sizes larger than 4° × 4°, spurious spatial variations in retrieved cloud and <span class="hlt">aerosol</span> properties can introduce widespread significant errors to calculations of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: 10px; color: #000;">dlnNe<span style="margin-left: -3em; margin-right: .5em; vertical-align: -15%; font-size: 10px; color: #000;">dlnτa and <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: 10px; color: #000;">dlnre<span style="margin-left: -2.7em; margin-right: .5em; vertical-align: -15%; font-size: 10px; color: #000;">dlnτa. For regions on the <span class="hlt">scale</span> of 60° × 60°, these methodological errors may lead to an overestimate in global cloud albedo effect radiative forcing of order 80% relative to that calculated for regions on the <span class="hlt">scale</span> of</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('https://ntrs.nasa.gov/search.jsp?R=19920065078&hterms=McCormick&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DMcCormick','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920065078&hterms=McCormick&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DMcCormick"><span>Background stratospheric <span class="hlt">aerosol</span> and polar stratospheric cloud reference models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mccormick, M. P.; Wang, P.-H.; Pitts, M. C.</p> <p>1993-01-01</p> <p>A global <span class="hlt">aerosol</span> climatology is evolving from the NASA satellite experiments SAM II, SAGE I, and SAGE II. In addition, polar stratospheric cloud (PSC) data have been obtained from these experiments over the last decade. An undated reference model of the optical characteristics of the background <span class="hlt">aerosol</span> is described and a new <span class="hlt">aerosol</span> reference model derived from the latest available data is proposed. The <span class="hlt">aerosol</span> models are referenced to the <span class="hlt">height</span> above the tropopause. The impact of a number of volcanic eruptions is described. In addition, a model describing the seasonal, longitudinal, and interannual variations in PSCs is presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080023775','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080023775"><span>The <span class="hlt">Aerosol</span>/Cloud/Ecosystems Mission (ACE)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schoeberl, Mark</p> <p>2008-01-01</p> <p>The goals and measurement strategy of the <span class="hlt">Aerosol</span>/Cloud/Ecosystems Mission (ACE) are described. ACE will help to answer fundamental science questions associated with <span class="hlt">aerosols</span>, clouds, air quality and global ocean ecosystems. Specifically, the goals of ACE are: 1) to quantify <span class="hlt">aerosol</span>-cloud interactions and to assess the impact of <span class="hlt">aerosols</span> on the hydrological cycle and 2) determine Ocean Carbon Cycling and other ocean biological processes. It is expected that ACE will: narrow the uncertainty in <span class="hlt">aerosol</span>-cloud-precipitation interaction and quantify the role of <span class="hlt">aerosols</span> in climate change; measure the ocean ecosystem changes and precisely quantify ocean carbon uptake; and, improve air quality forecasting by determining the <span class="hlt">height</span> and type of <span class="hlt">aerosols</span> being transported long distances. Overviews are provided of the <span class="hlt">aerosol</span>-cloud community measurement strategy, <span class="hlt">aerosol</span> and cloud observations over South Asia, and ocean biology research goals. Instruments used in the measurement strategy of the ACE mission are also highlighted, including: multi-beam lidar, multiwavelength high spectra resolution lidar, the ocean color instrument (ORCA)--a spectroradiometer for ocean remote sensing, dual frequency cloud radar and high- and low-frequency micron-wave radiometer. Future steps for the ACE mission include refining measurement requirements and carrying out additional instrument and payload studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120009839','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009839"><span>Integrated Modeling of <span class="hlt">Aerosol</span>, Cloud, Precipitation and Land Processes at Satellite-Resolved <span class="hlt">Scales</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peters-Lidard, Christa; Tao, Wei-Kuo; Chin, Mian; Braun, Scott; Case, Jonathan; Hou, Arthur; Kumar, Anil; Kumar, Sujay; Lau, William; Matsui, Toshihisa; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20120009839'); toggleEditAbsImage('author_20120009839_show'); toggleEditAbsImage('author_20120009839_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20120009839_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20120009839_hide"></p> <p>2012-01-01</p> <p>In this talk, I will present recent results from a project led at NASA/GSFC, in collaboration with NASA/MSFC and JHU, focused on the development and application of an observation-driven integrated modeling system that represents <span class="hlt">aerosol</span>, cloud, precipitation and land processes at satellite-resolved <span class="hlt">scales</span>. The project, known as the NASA Unified WRF (NU-WRF), is funded by NASA's Modeling and Analysis Program, and leverages prior investments from the Air Force Weather Agency and NASA's Earth Science Technology Office (ESTO). We define "satellite-resolved" <span class="hlt">scales</span> as being within a typical mesoscale atmospheric modeling grid (roughly 1-25 km), although this work is designed to bridge the continuum between local (microscale), regional (mesoscale) and global (synoptic) processes. NU-WRF is a superset of the standard NCAR Advanced Research WRF model, achieved by fully integrating the GSFC Land Information System (LIS, already coupled to WRF), the WRF/Chem enabled version of the Goddard Chemistry <span class="hlt">Aerosols</span> Radiation Transport (GOCART) model, the Goddard Satellite Data Simulation Unit (SDSU), and boundary/initial condition preprocessors for MERRA and GEOS-5 into a single software release (with source code available by agreement with NASA/GSFC). I will show examples where the full coupling between <span class="hlt">aerosol</span>, cloud, precipitation and land processes is critical for predicting local, regional, and global water and energy cycles, including some high-impact phenomena such as floods, hurricanes, mesoscale convective systems, droughts, and monsoons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007187','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007187"><span>The Invigoration of Deep Convective Clouds Over the Atlantic: <span class="hlt">Aerosol</span> Effect, Meteorology or Retrieval Artifact?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Koren, Ilan; Feingold, Graham; Remer, Lorraine A.</p> <p>2010-01-01</p> <p>Associations between cloud properties and <span class="hlt">aerosol</span> loading are frequently observed in products derived from satellite measurements. These observed trends between clouds and <span class="hlt">aerosol</span> optical depth suggest <span class="hlt">aerosol</span> modification of cloud dynamics, yet there are uncertainties involved in satellite retrievals that have the potential to lead to incorrect conclusions. Two of the most challenging problems are addressed here: the potential for retrieved <span class="hlt">aerosol</span> optical depth to be cloud-contaminated, and as a result, artificially correlated with cloud parameters; and the potential for correlations between <span class="hlt">aerosol</span> and cloud parameters to be erroneously considered to be causal. Here these issues are tackled directly by studying the effects of the <span class="hlt">aerosol</span> on convective clouds in the tropical Atlantic Ocean using satellite remote sensing, a chemical transport model, and a reanalysis of meteorological fields. Results show that there is a robust positive correlation between cloud fraction or cloud top <span class="hlt">height</span> and the <span class="hlt">aerosol</span> optical depth, regardless of whether a stringent filtering of <span class="hlt">aerosol</span> measurements in the vicinity of clouds is applied, or not. These same positive correlations emerge when replacing the observed <span class="hlt">aerosol</span> field with that derived from a chemical transport model. Model-reanalysis data is used to address the causality question by providing meteorological context for the satellite observations. A correlation exercise between the full suite of meteorological fields derived from model reanalysis and satellite-derived cloud fields shows that observed cloud top <span class="hlt">height</span> and cloud fraction correlate best with model pressure updraft velocity and relative humidity. Observed <span class="hlt">aerosol</span> optical depth does correlate with meteorological parameters but usually different parameters from those that correlate with observed cloud fields. The result is a near-orthogonal influence of <span class="hlt">aerosol</span> and meteorological fields on cloud top <span class="hlt">height</span> and cloud fraction. The results strengthen the case</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911801A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911801A"><span>Small <span class="hlt">scale</span> currents and ocean wave <span class="hlt">heights</span>: from today's models to future satellite observations with CFOSAT and SKIM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ardhuin, Fabrice; Gille, Sarah; Menemenlis, Dimitris; Rocha, Cesar; Rascle, Nicolas; Gula, Jonathan; Chapron, Bertrand</p> <p>2017-04-01</p> <p>Tidal currents and large oceanic currents, such as the Agulhas, Gulf Stream and Kuroshio, are known to modify ocean wave properties, causing extreme sea states that are a hazard to navigation. Recent advances in the understanding and modeling capability of ocean currents at <span class="hlt">scales</span> of 10 km or less have revealed the ubiquitous presence of fronts and filaments. Based on realistic numerical models, we show that these structures can be the main source of variability in significant wave <span class="hlt">heights</span> at <span class="hlt">scales</span> less than 200 km, including important variations at 10 km. This current-induced variability creates gradients in wave <span class="hlt">heights</span> that were previously overlooked and are relevant for extreme wave <span class="hlt">heights</span> and remote sensing. The spectrum of significant wave <span class="hlt">heights</span> is found to be of the order of 70⟨Hs ⟩2/(g2⟨Tm0,-1⟩2) times the current spectrum, where ⟨Hs ⟩ is the spatially-averaged significant wave <span class="hlt">height</span>, ⟨Tm0,-1⟩ is the average energy period, and g is the gravity acceleration. This small <span class="hlt">scale</span> variability is consistent with Jason-3 and SARAL along-track variability. We will discuss how future satellite mission with wave spectrometers can help observe these wave-current interactions. CFOSAT is due for launch in 2018, and SKIM is a proposal for ESA Earth Explorer 9.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....1714433C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....1714433C"><span>Further evidence for CCN <span class="hlt">aerosol</span> concentrations determining the <span class="hlt">height</span> of warm rain and ice initiation in convective clouds over the Amazon basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Campos Braga, Ramon; Rosenfeld, Daniel; Weigel, Ralf; Jurkat, Tina; Andreae, Meinrat O.; Wendisch, Manfred; Pöschl, Ulrich; Voigt, Christiane; Mahnke, Christoph; Borrmann, Stephan; Albrecht, Rachel I.; Molleker, Sergej; Vila, Daniel A.; Machado, Luiz A. T.; Grulich, Lucas</p> <p>2017-12-01</p> <p>We have investigated how <span class="hlt">aerosols</span> affect the <span class="hlt">height</span> above cloud base of rain and ice hydrometeor initiation and the subsequent vertical evolution of cloud droplet size and number concentrations in growing convective cumulus. For this purpose we used in situ data of hydrometeor size distributions measured with instruments mounted on HALO aircraft during the ACRIDICON-CHUVA campaign over the Amazon during September 2014. The results show that the <span class="hlt">height</span> of rain initiation by collision and coalescence processes (Dr, in units of meters above cloud base) is linearly correlated with the number concentration of droplets (Nd in cm-3) nucleated at cloud base (Dr ≈ 5 ṡ Nd). Additional cloud processes associated with Dr, such as GCCN, cloud, and mixing with ambient air and other processes, produce deviations of ˜ 21 % in the linear relationship, but it does not mask the clear relationship between Dr and Nd, which was also found at different regions around the globe (e.g., Israel and India). When Nd exceeded values of about 1000 cm-3, Dr became greater than 5000 m, and the first observed precipitation particles were ice hydrometeors. Therefore, no liquid water raindrops were observed within growing convective cumulus during polluted conditions. Furthermore, the formation of ice particles also took place at higher altitudes in the clouds in polluted conditions because the resulting smaller cloud droplets froze at colder temperatures compared to the larger drops in the unpolluted cases. The measured vertical profiles of droplet effective radius (re) were close to those estimated by assuming adiabatic conditions (rea), supporting the hypothesis that the entrainment and mixing of air into convective clouds is nearly inhomogeneous. Additional CCN activation on <span class="hlt">aerosol</span> particles from biomass burning and air pollution reduced re below rea, which further inhibited the formation of raindrops and ice particles and resulted in even higher altitudes for rain and ice initiation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.7345T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.7345T"><span>Global-<span class="hlt">scale</span> combustion sources of organic <span class="hlt">aerosols</span>: sensitivity to formation and removal mechanisms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsimpidi, Alexandra P.; Karydis, Vlassis A.; Pandis, Spyros N.; Lelieveld, Jos</p> <p>2017-06-01</p> <p>Organic compounds from combustion sources such as biomass burning and fossil fuel use are major contributors to the global atmospheric load of <span class="hlt">aerosols</span>. We analyzed the sensitivity of model-predicted global-<span class="hlt">scale</span> organic <span class="hlt">aerosols</span> (OA) to parameters that control primary emissions, photochemical aging, and the scavenging efficiency of organic vapors. We used a computationally efficient module for the description of OA composition and evolution in the atmosphere (ORACLE) of the global chemistry-climate model EMAC (ECHAM/MESSy Atmospheric Chemistry). A global dataset of <span class="hlt">aerosol</span> mass spectrometer (AMS) measurements was used to evaluate simulated primary (POA) and secondary (SOA) OA concentrations. Model results are sensitive to the emission rates of intermediate-volatility organic compounds (IVOCs) and POA. Assuming enhanced reactivity of semi-volatile organic compounds (SVOCs) and IVOCs with OH substantially improved the model performance for SOA. The use of a hybrid approach for the parameterization of the aging of IVOCs had a small effect on predicted SOA levels. The model performance improved by assuming that freshly emitted organic compounds are relatively hydrophobic and become increasingly hygroscopic due to oxidation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090020627','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090020627"><span>Estimating Mixing <span class="hlt">Heights</span> Using Microwave Temperature Profiler</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nielson-Gammon, John; Powell, Christina; Mahoney, Michael; Angevine, Wayne</p> <p>2008-01-01</p> <p>A paper describes the Microwave Temperature Profiler (MTP) for making measurements of the planetary boundary layer thermal structure data necessary for air quality forecasting as the Mixing Layer (ML) <span class="hlt">height</span> determines the volume in which daytime pollution is primarily concentrated. This is the first time that an airborne temperature profiler has been used to measure the mixing layer <span class="hlt">height</span>. Normally, this is done using a radar wind profiler, which is both noisy and large. The MTP was deployed during the Texas 2000 Air Quality Study (TexAQS-2000). An objective technique was developed and tested for estimating the ML <span class="hlt">height</span> from the MTP vertical temperature profiles. In order to calibrate the technique and evaluate the usefulness of this approach, estimates from a variety of measurements during the TexAQS-2000 were compared. Estimates of ML <span class="hlt">height</span> were used from radiosondes, radar wind profilers, an <span class="hlt">aerosol</span> backscatter lidar, and in-situ aircraft measurements in addition to those from the MTP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...1330453M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...1330453M"><span>Impacts of increasing the <span class="hlt">aerosol</span> complexity in the Met Office global NWP model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulcahy, J. P.; Walters, D. N.; Bellouin, N.; Milton, S. F.</p> <p>2013-11-01</p> <p>Inclusion of the direct and indirect radiative effects of <span class="hlt">aerosols</span> in high resolution global numerical weather prediction (NWP) models is being increasingly recognised as important for the improved accuracy of short-range weather forecasts. In this study the impacts of increasing the <span class="hlt">aerosol</span> complexity in the global NWP configuration of the Met Office Unified Model (MetUM) are investigated. A hierarchy of <span class="hlt">aerosol</span> representations are evaluated including three dimensional monthly mean speciated <span class="hlt">aerosol</span> climatologies, fully prognostic <span class="hlt">aerosols</span> modelled using the CLASSIC <span class="hlt">aerosol</span> scheme and finally, initialised <span class="hlt">aerosols</span> using assimilated <span class="hlt">aerosol</span> fields from the GEMS project. The prognostic <span class="hlt">aerosol</span> schemes are better able to predict the temporal and spatial variation of atmospheric <span class="hlt">aerosol</span> optical depth, which is particularly important in cases of large sporadic <span class="hlt">aerosol</span> events such as large dust storms or forest fires. Including the direct effect of <span class="hlt">aerosols</span> improves model biases in outgoing longwave radiation over West Africa due to a better representation of dust. However, uncertainties in dust optical properties propogate to its direct effect and the subsequent model response. Inclusion of the indirect <span class="hlt">aerosol</span> effects improves surface radiation biases at the North Slope of Alaska ARM site due to lower cloud amounts in high latitude clean air regions. This leads to improved temperature and <span class="hlt">height</span> forecasts in this region. Impacts on the global mean model precipitation and large-<span class="hlt">scale</span> circulation fields were found to be generally small in the short range forecasts. However, the indirect <span class="hlt">aerosol</span> effect leads to a strengthening of the low level monsoon flow over the Arabian Sea and Bay of Bengal and an increase in precipitation over Southeast Asia. Regional impacts on the African Easterly Jet (AEJ) are also presented with the large dust loading in the <span class="hlt">aerosol</span> climatology enhancing of the heat low over West Africa and weakening the AEJ. This study highlights the importance</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ERL....12e4021Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ERL....12e4021Z"><span>Decadal-<span class="hlt">scale</span> trends in regional <span class="hlt">aerosol</span> particle properties and their linkage to emission changes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Bin; Jiang, Jonathan H.; Gu, Yu; Diner, David; Worden, John; Liou, Kuo-Nan; Su, Hui; Xing, Jia; Garay, Michael; Huang, Lei</p> <p>2017-05-01</p> <p>Understanding long-term trends in <span class="hlt">aerosol</span> loading and properties is essential for evaluating the health and climatic effects of these airborne particulates as well as the effectiveness of pollution control policies. While many studies have used satellite data to examine the trends in <span class="hlt">aerosol</span> optical depth (AOD), very few have investigated the trends in <span class="hlt">aerosol</span> properties associated with particle size, morphology, and light absorption. In this study, we investigate decadal-<span class="hlt">scale</span> (13-15 year) trends in <span class="hlt">aerosol</span> loading and properties during 2001-2015 over three populous regions: the Eastern United States (EUS), Western Europe (WEU), and Eastern and Central China (ECC). We use observations from MISR (Multi-angle Imaging SpectroRadiometer) and MODIS (Moderate resolution Imaging Spectroradiometer). Relationships between <span class="hlt">aerosol</span> property trends and air pollutant emission changes are examined. We find that annual mean AOD shows pronounced decreasing trends over EUS and WEU regions, as a result of considerable emission reductions in all major pollutants except for mineral dust and ammonia (NH3). Over the ECC region, AOD increases before 2006 due to emission increases induced by rapid economic development, fluctuates between 2006 and 2011, and subsequently decreases after 2011 in conjunction with effective emission reduction in anthropogenic primary <span class="hlt">aerosols</span>, sulfur dioxide (SO2), and nitrogen oxides (NOx). The fraction of small-size AOD (<0.7 μm diameter), Ångstrom exponent and single-scattering albedo have generally decreased, while the fractions of large-size (>1.4 μm diameter), nonspherical and absorbing AOD have generally shown increasing trends over EUS and WEU regions, indicating that fine and light-scattering <span class="hlt">aerosol</span> constituents have been more effectively reduced than coarse and light-absorbing constituents. These trends are consistent with the larger reduction ratios in SO2 and NOx emissions than in primary <span class="hlt">aerosols</span>, including mineral dust and black carbon (BC</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.2175M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.2175M"><span>Impacts of increasing the <span class="hlt">aerosol</span> complexity in the Met Office global NWP model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulcahy, Jane; Walters, David; Bellouin, Nicolas; Milton, Sean</p> <p>2014-05-01</p> <p>Inclusion of the direct and indirect radiative effects of <span class="hlt">aerosols</span> in high resolution global numerical weather prediction (NWP) models is being increasingly recognised as important for the improved accuracy of short-range weather forecasts. In this study the impacts of increasing the <span class="hlt">aerosol</span> complexity in the global NWP configuration of the Met Office Unified Model (MetUM) are investigated. A hierarchy of <span class="hlt">aerosol</span> representations are evaluated including three dimensional monthly mean speciated <span class="hlt">aerosol</span> climatologies, fully prognostic <span class="hlt">aerosols</span> modelled using the CLASSIC <span class="hlt">aerosol</span> scheme and finally, initialised <span class="hlt">aerosols</span> using assimilated <span class="hlt">aerosol</span> fields from the GEMS project. The prognostic <span class="hlt">aerosol</span> schemes are better able to predict the temporal and spatial variation of atmospheric <span class="hlt">aerosol</span> optical depth, which is particularly important in cases of large sporadic <span class="hlt">aerosol</span> events such as large dust storms or forest fires. Including the direct effect of <span class="hlt">aerosols</span> improves model biases in outgoing longwave radiation over West Africa due to a better representation of dust. Inclusion of the indirect <span class="hlt">aerosol</span> effects has significant impacts on the SW radiation particularly at high latitudes due to lower cloud amounts in high latitude clean air regions. This leads to improved surface radiation biases at the North Slope of Alaska ARM site. Verification of temperature and <span class="hlt">height</span> forecasts is also improved in this region. Impacts on the global mean model precipitation and large-<span class="hlt">scale</span> circulation fields were found to be generally small in the short range forecasts. However, the indirect <span class="hlt">aerosol</span> effect leads to a strengthening of the low level monsoon flow over the Arabian Sea and Bay of Bengal and an increase in precipitation over Southeast Asia. This study highlights the importance of including a more realistic treatment of <span class="hlt">aerosol</span>-cloud interactions in global NWP models and the potential for improved global environmental prediction systems through the incorporation of more complex</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910016141','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910016141"><span>Tropospheric ozone and <span class="hlt">aerosols</span> measured by airborne lidar during the 1988 Arctic boundary layer experiment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Browell, Edward V.; Butler, Carolyn F.; Kooi, Susan A.</p> <p>1991-01-01</p> <p>Ozone (O3) and <span class="hlt">aerosol</span> distributions were measured from an aircraft using a differential absorption lidar (DIAL) system as part of the 1988 NASA Global Tropospheric Experiment - Arctic Boundary Layer Experiment (ABLE-3A) to study the sources and sinks of gases and <span class="hlt">aerosols</span> over the tundra regions of Alaska during the summer. The tropospheric O3 budget over the Arctic was found to be strongly influenced by stratospheric intrusions. Regions of low <span class="hlt">aerosol</span> scattering and enhanced O3 mixing ratios were usually correlated with descending air from the upper troposphere or lower stratosphere. Several cases of continental polar air masses were examined during the experiment. The <span class="hlt">aerosol</span> scattering associated with these air masses was very low, and the atmospheric distribution of <span class="hlt">aerosols</span> was quite homogeneous for those air masses that had been transported over the ice for greater than or = 3 days. The transition in O3 and <span class="hlt">aerosol</span> distributions from tundra to marine conditions was examined several times. The <span class="hlt">aerosol</span> data clearly show an abrupt change in <span class="hlt">aerosol</span> scattering properties within the mixed layer from lower values over the tundra to generally higher values over the water. The distinct differences in the <span class="hlt">heights</span> of the mixed layers in the two regions was also readily apparent. Several cases of enhanced O3 were observed during ABLE-3 in conjunction with enhanced <span class="hlt">aerosol</span> scattering in layers in the free atmosphere. Examples are presented of the large <span class="hlt">scale</span> variations of O3 and <span class="hlt">aerosols</span> observed with the airborne lidar system from near the surface to above the tropopause over the Arctic during ABLE-3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A31E2228A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A31E2228A"><span>Probing <span class="hlt">aerosol</span> indirect effect on deep convection using idealized cloud-resolving simulations with parameterized large-<span class="hlt">scale</span> dynamics.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anber, U.; Wang, S.; Gentine, P.; Jensen, M. P.</p> <p>2017-12-01</p> <p>A framework is introduced to investigate the indirect impact of <span class="hlt">aerosol</span> loading on tropical deep convection using 3-dimentional idealized cloud-system resolving simulations with coupled large-<span class="hlt">scale</span> circulation. The large <span class="hlt">scale</span> dynamics is parameterized using a spectral weak temperature gradient approximation that utilizes the dominant balance in the tropics between adiabatic cooling and diabatic heating. <span class="hlt">Aerosol</span> loading effect is examined by varying the number concentration of nuclei (CCN) to form cloud droplets in the bulk microphysics scheme over a wide range from 30 to 5000 without including any radiative effect as the radiative cooling is prescribed at a constant rate, to isolate the microphysical effect. Increasing <span class="hlt">aerosol</span> number concentration causes mean precipitation to decrease monotonically, despite the increase in cloud condensates. Such reduction in precipitation efficiency is attributed to reduction in the surface enthalpy fluxes, and not to the divergent circulation, as the gross moist stability remains unchanged. We drive a simple <span class="hlt">scaling</span> argument based on the moist static energy budget, that enables a direct estimation of changes in precipitation given known changes in surfaces enthalpy fluxes and the constant gross moist stability. The impact on cloud hydrometers and microphysical properties is also examined and is consistent with the macro-physical picture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.A23A0265M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.A23A0265M"><span>MISR Stereo-<span class="hlt">heights</span> of Grassland Fire Smoke Plumes 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>Mims, S. R.; Kahn, R. A.; Moroney, C. M.; Gaitley, B. J.; Nelson, D. L.; Garay, M. J.</p> <p>2008-12-01</p> <p>Plume <span class="hlt">heights</span> from wildfires are used in climate modeling to predict and understand trends in <span class="hlt">aerosol</span> transport. This study examines whether smoke from grassland fires in the desert region of Western and central Australia ever rises above the relatively stable atmospheric boundary layer and accumulates in higher layers of relative atmospheric stability. Several methods for deriving plume <span class="hlt">heights</span> from the Multi-angle Imaging SpectroRadiometer (MISR) instrument are examined for fire events during the summer 2000 and 2002 burning seasons. Using MISR's multi-angle stereo-imagery from its three near-nadir-viewing cameras, an automatic algorithm routinely derives the stereo-<span class="hlt">heights</span> above the geoid of the level-of-maximum-contrast for the entire global data set, which often correspond to the <span class="hlt">heights</span> of clouds and <span class="hlt">aerosol</span> plumes. Most of the fires that occur in the cases studied here are small, diffuse, and difficult to detect. To increase the signal from these thin hazes, the MISR enhanced stereo product that computes stereo <span class="hlt">heights</span> from the most steeply viewing MISR cameras is used. For some cases, a third approach to retrieving plume <span class="hlt">heights</span> from MISR stereo imaging observations, the MISR Interactive Explorer (MINX) tool, is employed to help differentiate between smoke and cloud. To provide context and to search for correlative factors, stereo-<span class="hlt">heights</span> are combined with data providing fire strength from the Moderate-resolution Imaging Spectroradiometer (MODIS) instrument, atmospheric structure from the NCEP/NCAR Reanalysis Project, surface cover from the Australia National Vegetation Information System, and forward and backward trajectories from the NOAA HYSPLIT model. Although most smoke plumes concentrate in the near-surface boundary layer, as expected, some appear to rise higher. These findings suggest that a closer examination of grassland fire energetics may be warranted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.2921R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.2921R"><span>Two global data sets of daily fire emission injection <span class="hlt">heights</span> since 2003</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rémy, Samuel; Veira, Andreas; Paugam, Ronan; Sofiev, Mikhail; Kaiser, Johannes W.; Marenco, Franco; Burton, Sharon P.; Benedetti, Angela; Engelen, Richard J.; Ferrare, Richard; Hair, Jonathan W.</p> <p>2017-02-01</p> <p>The Global Fire Assimilation System (GFAS) assimilates fire radiative power (FRP) observations from satellite-based sensors to produce daily estimates of biomass burning emissions. It has been extended to include information about injection <span class="hlt">heights</span> derived from fire observations and meteorological information from the operational weather forecasts of ECMWF. Injection <span class="hlt">heights</span> are provided by two distinct methods: the Integrated Monitoring and Modelling System for wildland fires (IS4FIRES) parameterisation and the one-dimensional plume rise model (PRM). A global database of daily biomass burning emissions and injection <span class="hlt">heights</span> at 0.1° resolution has been produced for 2003-2015 and is continuously extended in near-real time with the operational GFAS service of the Copernicus Atmospheric Monitoring Service (CAMS). In this study, the two injection <span class="hlt">height</span> data sets were compared with the new MPHP2 (MISR Plume <span class="hlt">Height</span> Project 2) satellite-based plume <span class="hlt">height</span> retrievals. The IS4FIRES parameterisation showed a better overall agreement than the observations, while the PRM was better at capturing the variability of injection <span class="hlt">heights</span>. The performance of both parameterisations is also dependent on the type of vegetation. Furthermore, the use of biomass burning emission <span class="hlt">heights</span> from GFAS in atmospheric composition forecasts was assessed in two case studies: the South AMerican Biomass Burning Analysis (SAMBBA) campaign which took place in September 2012 in Brazil, and a series of large fire events in the western USA in August 2013. For these case studies, forecasts of biomass burning <span class="hlt">aerosol</span> species by the Composition Integrated Forecasting System (C-IFS) of CAMS were found to better reproduce the observed vertical distribution when using PRM injection <span class="hlt">heights</span> from GFAS compared to <span class="hlt">aerosols</span> emissions being prescribed at the surface. The globally available GFAS injection <span class="hlt">heights</span> introduced and evaluated in this study provide a comprehensive data set for future fire and atmospheric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33B2362L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33B2362L"><span><span class="hlt">Aerosol</span> Extinction Profile Mapping with Lognormal Distribution Based on MPL Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, T. H.; Lee, T. T.; Chang, K. E.; Lien, W. H.; Liu, G. R.; Liu, C. Y.</p> <p>2017-12-01</p> <p>This study intends to challenge the profile mapping of <span class="hlt">aerosol</span> vertical distribution by mathematical function. With the similarity in distribution pattern, lognormal distribution is examined for mapping the <span class="hlt">aerosol</span> extinction profile based on MPL (Micro Pulse LiDAR) in situ measurements. The variables of lognormal distribution are log mean (μ) and log standard deviation (σ), which will be correlated with the parameters of <span class="hlt">aerosol</span> optical depht (AOD) and planetary boundary layer <span class="hlt">height</span> (PBLH) associated with the altitude of extinction peak (Mode) defined in this study. On the base of 10 years MPL data with single peak, the mapping results showed that the mean error of Mode and σ retrievals are 16.1% and 25.3%, respectively. The mean error of σ retrieval can be reduced to 16.5% under the cases of larger distance between PBLH and Mode. The proposed method is further applied to MODIS AOD product in mapping extinction profile for the retrieval of PM2.5 in terms of satellite observations. The results indicated well agreement between retrievals and ground measurements when <span class="hlt">aerosols</span> under 525 meters are well-mixed. The feasibility of proposed method to satellite remote sensing is also suggested by the case study. Keyword: <span class="hlt">Aerosol</span> extinction profile, Lognormal distribution, MPL, Planetary boundary layer <span class="hlt">height</span> (PBLH), <span class="hlt">Aerosol</span> optical depth (AOD), Mode</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.7095B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.7095B"><span>Vertical distribution of <span class="hlt">aerosols</span> over the Maritime Continent during El Niño</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blake Cohen, Jason; Loong Ng, Daniel Hui; Lun Lim, Alan Wei; Chua, Xin Rong</p> <p>2018-05-01</p> <p>The vertical distribution of <span class="hlt">aerosols</span> over Southeast Asia, a critical factor impacting <span class="hlt">aerosol</span> lifetime, radiative forcing, and precipitation, is examined for the 2006 post El Niño fire burning season. Combining these measurements with remotely sensed land, fire, and meteorological measurements, and fire plume modeling, we have reconfirmed that fire radiative power (FRP) is underestimated over Southeast Asia by MODIS measurements. These results are derived using a significantly different approach from other previously attempted approaches found in the literature. The horizontally constrained Maritime Continent's fire plume median <span class="hlt">height</span>, using the maximum variance of satellite observed <span class="hlt">aerosol</span> optical depth as the spatial and temporal constraint, is found to be 2.04 ± 1.52 km during the entirety of the 2006 El Niño fire season, and 2.19±1.50 km for October 2006. This is 0.83 km (0.98 km) higher than random sampling and all other past studies. Additionally, it is determined that 61 (+6-10) % of the bottom of the smoke plume and 83 (+8-11) % of the median of the smoke plume is in the free troposphere during the October maximum; while 49 (+7-9) % and 75 (+12-12) % of the total <span class="hlt">aerosol</span> plume and the median of the <span class="hlt">aerosol</span> plume, are correspondingly found in the free troposphere during the entire fire season. This vastly different vertical distribution will have impacts on <span class="hlt">aerosol</span> lifetime and dispersal. Application of a simple plume rise model using measurements of fire properties underestimates the median plume <span class="hlt">height</span> by 0.26 km over the entire fire season and 0.34 km over the maximum fire period. It is noted that the model underestimation over the bottom portions of the plume are much larger. The center of the plume can be reproduced when fire radiative power is increased by 20 % (with other parts of the plume ranging from an increase of 0 to 60 % depending on the portion of the plume and the length of the fire season considered). However, to reduce the biases</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26233420','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26233420"><span>Note: Design and development of wireless controlled <span class="hlt">aerosol</span> sampling network for large <span class="hlt">scale</span> <span class="hlt">aerosol</span> dispersion experiments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gopalakrishnan, V; Subramanian, V; Baskaran, R; Venkatraman, B</p> <p>2015-07-01</p> <p>Wireless based custom built <span class="hlt">aerosol</span> sampling network is designed, developed, and implemented for environmental <span class="hlt">aerosol</span> sampling. These <span class="hlt">aerosol</span> sampling systems are used in field measurement campaign, in which sodium <span class="hlt">aerosol</span> dispersion experiments have been conducted as a part of environmental impact studies related to sodium cooled fast reactor. The sampling network contains 40 <span class="hlt">aerosol</span> sampling units and each contains custom built sampling head and the wireless control networking designed with Programmable System on Chip (PSoC™) and Xbee Pro RF modules. The base station control is designed using graphical programming language LabView. The sampling network is programmed to operate in a preset time and the running status of the samplers in the network is visualized from the base station. The system is developed in such a way that it can be used for any other environment sampling system deployed in wide area and uneven terrain where manual operation is difficult due to the requirement of simultaneous operation and status logging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22483271-note-design-development-wireless-controlled-aerosol-sampling-network-large-scale-aerosol-dispersion-experiments','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22483271-note-design-development-wireless-controlled-aerosol-sampling-network-large-scale-aerosol-dispersion-experiments"><span>Note: Design and development of wireless controlled <span class="hlt">aerosol</span> sampling network for large <span class="hlt">scale</span> <span class="hlt">aerosol</span> dispersion experiments</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>Gopalakrishnan, V.; Subramanian, V.; Baskaran, R.</p> <p>2015-07-15</p> <p>Wireless based custom built <span class="hlt">aerosol</span> sampling network is designed, developed, and implemented for environmental <span class="hlt">aerosol</span> sampling. These <span class="hlt">aerosol</span> sampling systems are used in field measurement campaign, in which sodium <span class="hlt">aerosol</span> dispersion experiments have been conducted as a part of environmental impact studies related to sodium cooled fast reactor. The sampling network contains 40 <span class="hlt">aerosol</span> sampling units and each contains custom built sampling head and the wireless control networking designed with Programmable System on Chip (PSoC™) and Xbee Pro RF modules. The base station control is designed using graphical programming language LabView. The sampling network is programmed to operate in amore » preset time and the running status of the samplers in the network is visualized from the base station. The system is developed in such a way that it can be used for any other environment sampling system deployed in wide area and uneven terrain where manual operation is difficult due to the requirement of simultaneous operation and status logging.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRD..12113628C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRD..12113628C"><span>Estimation of columnar concentrations of absorbing and scattering fine mode <span class="hlt">aerosol</span> components using AERONET data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, Yongjoo; Ghim, Young Sung</p> <p>2016-11-01</p> <p>Columnar concentrations of absorbing and scattering components of fine mode <span class="hlt">aerosols</span> were estimated using <span class="hlt">Aerosol</span> Robotic Network (AERONET) data for a site downwind of Seoul. The study period was between March 2012 and April 2013 including the period of the Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON)-Asia campaign in March to May 2012. The Maxwell Garnett mixing rule was assumed for insoluble components embedded in a host solution, while the volume average mixing rule was assumed for the aqueous solution of soluble components. During the DRAGON-Asia campaign the surface concentrations of major components of fine particles were measured. The columnar mass fractions of black carbon (BC), organic carbon (OC), mineral dust (MD), and ammonium sulfate (AS) were 1.5, 5.9, 6.6, and 52%, respectively, which were comparable to the mass fractions measured at the surface for BC, OC, and secondary inorganic <span class="hlt">aerosols</span> at 2.3, 18, and 55%. The vertical distributions of BC and AS were investigated by employing the concept of a column <span class="hlt">height</span>. While the column <span class="hlt">height</span> for BC was similar to the planetary boundary layer (PBL) <span class="hlt">height</span>, that for AS was 4.4 times higher than the PBL <span class="hlt">height</span> and increased with air temperature from March to May. The monthly variations of the columnar mass concentrations during the study period were generally well explained in term of meteorology and emission characteristics. However, certain variations of MD were different from those typically observed primarily because only fine mode <span class="hlt">aerosols</span> were considered.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.8365K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.8365K"><span>Large-<span class="hlt">scale</span> connection between <span class="hlt">aerosol</span> optical depth and summer monsoon circulation, and precipitation over northeast Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Sang-Woo; Yoon, Soon-Chang; Choi, Suk-Jin; Choi, In-Jin</p> <p>2010-05-01</p> <p>We investigated the large-<span class="hlt">scale</span> connection between columnar <span class="hlt">aerosol</span> loads and summer monsoon circulation, and also the precipitation over northeast Asia using <span class="hlt">aerosol</span> optical depth (AOD) data obtained from the 8-year MODIS, AERONET Sun/sky radiometer, and precipitation data acquired under the Global Precipitation Climatology Project (GPCP). These high-quality data revealed the large-<span class="hlt">scale</span> link between AOD and summer monsoon circulation, precipitation in July over northeast Asian countries, and their distinct spatial and annual variabilities. Compared to the mean AOD for the entire period of 2001-2008, the increase of almost 40-50% in the AOD value in July 2005 and July 2007 was found over the downwind regions of China (Yellow Sea, Korean peninsula, and East Sea), with negative precipitation anomalies. This can be attributable to the strong westerly confluent flows, between cyclone flows by continental thermal low centered over the northern China and anti-cyclonic flows by the western North Pacific High, which transport anthropogenic pollution <span class="hlt">aerosols</span> emitted from east China to aforementioned downwind high AOD regions along the rim of the Pacific marine airmass. In July 2002, however, the easterly flows transported anthropogenic <span class="hlt">aerosols</span> from east China to the southwestern part of China in July 2002. As a result, the AOD off the coast of China was dramatically reduced in spite of decreasing rainfall. From the calculation of the cross-correlation coefficient between MODIS-derived AOD anomalies and GPCP precipitation anomalies over the period 2001-2008, we found negative correlations over the areas encompassed by 105-115E and 30-35N and by 120-140E and 35-40N (Yellow Sea, Korean peninsula, and East Sea). This suggests that <span class="hlt">aerosol</span> loads over these regions are easily influenced by the Asian monsoon flow system and associated precipitation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140008990','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140008990"><span>Constraints on Smoke Injection <span class="hlt">Height</span>, Source Strength, and Transports from MISR and MODIS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kahn, Ralph A.; Petrenko, Mariya; Val Martin, Maria; Chin, Mian</p> <p>2014-01-01</p> <p>The AeroCom BB (Biomass Burning) Experiment AOD (<span class="hlt">Aerosol</span> Optical Depth) motivation: We have a substantial set of satellite wildfire plume AOD snapshots and injection <span class="hlt">heights</span> to help calibrate model/inventory performance; We are 1) adding more fire source-strength cases 2) using MISR to improve the AOD constrains and 3) adding 2008 global injection <span class="hlt">heights</span>; We selected GFED3-daily due to good overall source strength performance, but any inventory can be tested; Joint effort to test multiple, global models, to draw robust BB injection <span class="hlt">height</span> and emission strength conclusions. We provide satellite-based injection <span class="hlt">height</span> and smoke plume AOD climatologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38..955R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38..955R"><span>The topside ionospheric effective <span class="hlt">scale</span> <span class="hlt">heights</span> (HT) derived with ROCSAT-1 and ground-based Ionosonde observations at equatorial and mid-latitude stations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ram Sudarsanam, Tulasi; Su, Shin-Yi; Liu, C. H.; Reinisch, Bodo</p> <p></p> <p>In this study, we propose the assimilation of topside in situ electron density data from ROCSAT-1 satellite along with the ionosonde measurements for accurate determination of topside iono-spheric effective <span class="hlt">scale</span> <span class="hlt">heights</span> (HT) using -Chapman function. The reconstructed topside elec-tron density profiles using these <span class="hlt">scale</span> <span class="hlt">heights</span> exhibit an excellent similitude with Jicamarca Incoherent Scatter Radar (ISR) profiles, and are much better representations than the existing methods of Reinisch-Huang method and/or the empirical IRI-2007 model. The main advan-tage with this method is that it allows the precise determination of the effective <span class="hlt">scale</span> <span class="hlt">height</span> (HT) and the topside electron density profiles at a dense network of ionosonde/digisonde sta-tions where no ISR facilities are available. The demonstration of the method is applied by investigating the diurnal, seasonal and solar activity variations of HT over the dip-equatorial station Jicamarca and the mid-latitude station Grahamstown. The diurnal variation of <span class="hlt">scale</span> <span class="hlt">heights</span> over Jicamarca consistently exhibits a morning time descent followed by a minimum around 0700-0800 LT and a pronounced maximum at noon during all the seasons of both high and moderate solar activity periods. Further, the <span class="hlt">scale</span> <span class="hlt">heights</span> exhibit a secondary maximum during the post-sunset hours of equinoctial and summer months, whereas the post-sunset peak is absent during the winter months. These typical features are further investigated using the topside ion properties obtained by ROCSAT-1 as well as SAMI2 model simulations. The re-sults consistently indicate that the diurnal variation of the effective <span class="hlt">scale</span> <span class="hlt">height</span> (HT) does not closely follow the plasma temperature variation and at equatorial latitudes is largely controlled by the vertical ExB drift.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110006994','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110006994"><span>What We are Learning from (and About) the 10 Plus Year MISR <span class="hlt">Aerosol</span> Data Record</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kahn, Ralph A.</p> <p>2010-01-01</p> <p>Having a 10+ year data record from the Multi-angle Imaging SpectroRadiometer (MISR) significantly improves our opportunities to validate the retrieved <span class="hlt">aerosol</span> optical depth (AOD) and especially particle microphysical property products. It also begins to raise the possibility of using the data to look for changes or even trends, at least on a regional basis. Further, we have had the opportunity to expand the database of wildfire smoke plume <span class="hlt">heights</span> derived from the multiangle observations. This presentation will review the latest <span class="hlt">aerosol</span> validation results and algorithm upgrades under consideration by the MISR team, and will summarize the current status of MISR global <span class="hlt">aerosol</span> air mass type, and regional dust transport and smoke injection <span class="hlt">height</span> products. The strengths and limitations of these data for constraining <span class="hlt">aerosol</span> transport model simulations will receive special emphasis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=128915&keyword=accounting+AND+system&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=128915&keyword=accounting+AND+system&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>MULTICOMPONENT <span class="hlt">AEROSOL</span> DYNAMICS OF THE PB-O2 SYSTEM IN A BENCH <span class="hlt">SCALE</span> FLAME INCINERATOR</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 study was carried out to understand the formation and growth of lead particles in a flame incinerator. A bench <span class="hlt">scale</span> flame incinerator was used to perform controlled experiments with lead acetate as a test compound. A dilution probe in conjunction with real-time <span class="hlt">aerosol</span> instrum...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1365568','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1365568"><span>Collaborative Research: Quantifying the Uncertainties of <span class="hlt">Aerosol</span> Indirect Effects and Impacts on Decadal-<span class="hlt">Scale</span> Climate Variability in NCAR CAM5 and CESM1</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>Nenes, Athanasios</p> <p></p> <p>The goal of this proposed project is to assess the climatic importance and sensitivity of <span class="hlt">aerosol</span> indirect effect (AIE) to cloud and <span class="hlt">aerosol</span> processes and feedbacks, which include organic <span class="hlt">aerosol</span> hygroscopicity, cloud condensation nuclei (CCN) activation kinetics, Giant CCN, cloud-<span class="hlt">scale</span> entrainment, ice nucleation in mixed-phase and cirrus clouds, and treatment of subgrid variability of vertical velocity. A key objective was to link <span class="hlt">aerosol</span>, cloud microphysics and dynamics feedbacks in CAM5 with a suite of internally consistent and integrated parameterizations that provide the appropriate degrees of freedom to capture the various aspects of the <span class="hlt">aerosol</span> indirect effect. The proposal integrated newmore » parameterization elements into the cloud microphysics, moist turbulence and <span class="hlt">aerosol</span> modules used by the NCAR Community Atmospheric Model version 5 (CAM5). The CAM5 model was then used to systematically quantify the uncertainties of <span class="hlt">aerosol</span> indirect effects through a series of sensitivity tests with present-day and preindustrial <span class="hlt">aerosol</span> emissions. New parameterization elements were developed as a result of these efforts, and new diagnostic tools & methodologies were also developed to quantify the impacts of <span class="hlt">aerosols</span> on clouds and climate within fully coupled models. Observations were used to constrain key uncertainties in the <span class="hlt">aerosol</span>-cloud links. Advanced sensitivity tools were developed and implements to probe the drivers of cloud microphysical variability with unprecedented temporal and spatial <span class="hlt">scale</span>. All these results have been published in top and high impact journals (or are in the final stages of publication). This proposal has also supported a number of outstanding graduate students.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AMT....11..161N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AMT....11..161N"><span>Error sources in the retrieval of <span class="hlt">aerosol</span> information over bright surfaces from satellite measurements in the oxygen A band</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nanda, Swadhin; de Graaf, Martin; Sneep, Maarten; de Haan, Johan F.; Stammes, Piet; Sanders, Abram F. J.; Tuinder, Olaf; Pepijn Veefkind, J.; Levelt, Pieternel F.</p> <p>2018-01-01</p> <p><p class="p">Retrieving <span class="hlt">aerosol</span> optical thickness and <span class="hlt">aerosol</span> layer <span class="hlt">height</span> over a bright surface from measured top-of-atmosphere reflectance spectrum in the oxygen A band is known to be challenging, often resulting in large errors. In certain atmospheric conditions and viewing geometries, a loss of sensitivity to <span class="hlt">aerosol</span> optical thickness has been reported in the literature. This loss of sensitivity has been attributed to a phenomenon known as critical surface albedo regime, which is a range of surface albedos for which the top-of-atmosphere reflectance has minimal sensitivity to <span class="hlt">aerosol</span> optical thickness. This paper extends the concept of critical surface albedo for <span class="hlt">aerosol</span> layer <span class="hlt">height</span> retrievals in the oxygen A band, and discusses its implications. The underlying physics are introduced by analysing the top-of-atmosphere reflectance spectrum as a sum of atmospheric path contribution and surface contribution, obtained using a radiative transfer model. Furthermore, error analysis of an <span class="hlt">aerosol</span> layer <span class="hlt">height</span> retrieval algorithm is conducted over dark and bright surfaces to show the dependence on surface reflectance. The analysis shows that the derivative with respect to <span class="hlt">aerosol</span> layer <span class="hlt">height</span> of the atmospheric path contribution to the top-of-atmosphere reflectance is opposite in sign to that of the surface contribution - an increase in surface brightness results in a decrease in information content. In the case of <span class="hlt">aerosol</span> optical thickness, these derivatives are anti-correlated, leading to large retrieval errors in high surface albedo regimes. The consequence of this anti-correlation is demonstrated with measured spectra in the oxygen A band from the GOME-2 instrument on board the Metop-A satellite over the 2010 Russian wildfires incident.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070031188&hterms=Conveyed+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DConveyed%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070031188&hterms=Conveyed+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DConveyed%2Bwaves"><span>Atmospheric Teleconnection over Eurasia Induced by <span class="hlt">Aerosol</span> Radiative Forcing during Boreal Spring</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, Maeng-Ki; Lau, William K. M.; Chin, Mian; Kim, Kyu-Myong; Sud, Y. C.; Walker, Greg K.</p> <p>2006-01-01</p> <p>The direct effects of <span class="hlt">aerosols</span> on global and regional climate during boreal spring are investigated based on numerical simulations with the NASA Global Modeling and Assimilation Office finite-volume general circulation model (fvGCM) with Microphyics of Clouds with the Relaxed Arakawa Schubert Scheme (McRAS), using <span class="hlt">aerosol</span> forcing functions derived from the Goddard Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport model (GOCART). The authors find that anomalous atmospheric heat sources induced by absorbing <span class="hlt">aerosols</span> (dust and black carbon) excite a planetary-<span class="hlt">scale</span> teleconnection pattern in sea level pressure, temperature, and geopotential <span class="hlt">height</span> spanning North Africa through Eurasia to the North Pacific. Surface cooling due to direct effects of <span class="hlt">aerosols</span> is found in the vicinity and downstream of the <span class="hlt">aerosol</span> source regions, that is, South Asia, East Asia, and northern and western Africa. Significant atmospheric heating is found in regions with large loading of dust (over northern Africa and the Middle East) and black carbon (over Southeast Asia). Paradoxically, the most pronounced feature in <span class="hlt">aerosol</span>-induced surface temperature is an east west dipole anomaly with strong cooling over the Caspian Sea and warming over central and northeastern Asia, where <span class="hlt">aerosol</span> concentrations are low. Analyses of circulation anomalies show that the dipole anomaly is a part of an atmospheric teleconnection pattern driven by atmospheric heating anomalies induced by absorbing <span class="hlt">aerosols</span> in the source regions, but the influence was conveyed globally through barotropic energy dispersion and sustained by feedback processes associated with the regional circulations. The surface temperature signature associated with the <span class="hlt">aerosol</span>-induced teleconnection bears striking resemblance to the spatial pattern of observed long-term trend in surface temperature over Eurasia. Additionally, the boreal spring wave train pattern is similar to that reported by Fukutomi et al. associated with the boreal summer</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7081E..0TD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7081E..0TD"><span>WindCam and MSPI: two cloud and <span class="hlt">aerosol</span> instrument concepts derived from Terra/MISR heritage</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diner, David J.; Mischna, Michael; Chipman, Russell A.; Davis, Ab; Cairns, Brian; Davies, Roger; Kahn, Ralph A.; Muller, Jan-Peter; Torres, Omar</p> <p>2008-08-01</p> <p>The Multi-angle Imaging SpectroRadiometer (MISR) has been acquiring global cloud and <span class="hlt">aerosol</span> data from polar orbit since February 2000. MISR acquires moderately high-resolution imagery at nine view angles from nadir to 70.5°, in four visible/near-infrared spectral bands. Stereoscopic parallax, time lapse among the nine views, and the variation of radiance with angle and wavelength enable retrieval of geometric cloud and <span class="hlt">aerosol</span> plume <span class="hlt">heights</span>, <span class="hlt">height</span>-resolved cloud-tracked winds, and <span class="hlt">aerosol</span> optical depth and particle property information. Two instrument concepts based upon MISR heritage are in development. The Cloud Motion Vector Camera, or WindCam, is a simplified version comprised of a lightweight, compact, wide-angle camera to acquire multiangle stereo imagery at a single visible wavelength. A constellation of three WindCam instruments in polar Earth orbit would obtain <span class="hlt">height</span>-resolved cloud-motion winds with daily global coverage, making it a low-cost complement to a spaceborne lidar wind measurement system. The Multiangle SpectroPolarimetric Imager (MSPI) is aimed at <span class="hlt">aerosol</span> and cloud microphysical properties, and is a candidate for the National Research Council Decadal Survey's <span class="hlt">Aerosol</span>-Cloud-Ecosystem (ACE) mission. MSPI combines the capabilities of MISR with those of other <span class="hlt">aerosol</span> sensors, extending the spectral coverage to the ultraviolet and shortwave infrared and incorporating high-accuracy polarimetric imaging. Based on requirements for the nonimaging <span class="hlt">Aerosol</span> Polarimeter Sensor on NASA's Glory mission, a degree of linear polarization uncertainty of 0.5% is specified within a subset of the MSPI bands. We are developing a polarization imaging approach using photoelastic modulators (PEMs) to accomplish this objective.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AMT.....9..793E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AMT.....9..793E"><span>Global cloud top <span class="hlt">height</span> retrieval using SCIAMACHY limb spectra: model studies and first results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eichmann, Kai-Uwe; Lelli, Luca; von Savigny, Christian; Sembhi, Harjinder; Burrows, John P.</p> <p>2016-03-01</p> <p>Cloud top <span class="hlt">heights</span> (CTHs) are retrieved for the period 1 January 2003 to 7 April 2012 using <span class="hlt">height</span>-resolved limb spectra measured with the SCanning Imaging Absorption SpectroMeter for Atmospheric CHartographY (SCIAMACHY) on board ENVISAT (ENVIronmental SATellite). In this study, we present the retrieval code SCODA (SCIAMACHY cloud detection algorithm) based on a colour index method and test the accuracy of the retrieved CTHs in comparison to other methods. Sensitivity studies using the radiative transfer model <span style="" class="text">SCIATRAN show that the method is capable of detecting cloud tops down to about 5 km and very thin cirrus clouds up to the tropopause. Volcanic particles can be detected that occasionally reach the lower stratosphere. Upper tropospheric ice clouds are observable for a nadir cloud optical thickness (COT) ≥ 0.01, which is in the subvisual range. This detection sensitivity decreases towards the lowermost troposphere. The COT detection limit for a water cloud top <span class="hlt">height</span> of 5 km is roughly 0.1. This value is much lower than thresholds reported for passive cloud detection methods in nadir-viewing direction. Low clouds at 2 to 3 km can only be retrieved under very clean atmospheric conditions, as light scattering of <span class="hlt">aerosol</span> particles interferes with the cloud particle scattering. We compare co-located SCIAMACHY limb and nadir cloud parameters that are retrieved with the Semi-Analytical CloUd Retrieval Algorithm (SACURA). Only opaque clouds (τN,c > 5) are detected with the nadir passive retrieval technique in the UV-visible and infrared wavelength ranges. Thus, due to the frequent occurrence of thin clouds and subvisual cirrus clouds in the tropics, larger CTH deviations are detected between both viewing geometries. Zonal mean CTH differences can be as high as 4 km in the tropics. The agreement in global cloud fields is sufficiently good. However, the land-sea contrast, as seen in nadir cloud occurrence frequency distributions, is not</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10466E..3WS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10466E..3WS"><span>Potential sources of Southern Siberia <span class="hlt">aerosols</span> by data of AERONET site in Tomsk, Russia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shukurov, K. A.; Shukurova, L. M.</p> <p>2017-11-01</p> <p>For all days of measurements in 2002-2015 of volume concentration of <span class="hlt">aerosols</span> at the AERONET Tomsk/Tomsk-22 station an array of 10-day backward trajectories of air parcels arriving in Tomsk into seven layers of the troposphere with <span class="hlt">heights</span> in the range of 0.5-5.0 km is calculated using the trajectory model NOAA HYSPLIT_4. For the three fractions of the <span class="hlt">aerosol</span> with particle sizes < 1.0 μm, 1.0-2.5 μm, 2.5-5.0 μm and their sum (< 5.0 μm), the field of capacity of the potential sources of <span class="hlt">aerosols</span> of these fractions for southern Siberia is determined by the CWT (concentration weighted trajectory) method using the backward trajectory array. The analysis is carried out taking into account the processes both the scavenging of the <span class="hlt">aerosols</span> with precipitation and the dry deposition. Trajectories arriving at different <span class="hlt">heights</span> were analyzed taking into account the weight coefficients proportional to the backward light scattering coefficients of an <span class="hlt">aerosols</span> at corresponding <span class="hlt">heights</span> for warm and cold seasons in Western Siberia. The most capable (in unit of volume concentration μm3 /μm2 ) potential sources of these fractions for southern Siberia are located above North Africa, Eastern Siberia, Central Asia and the Dzhungarian desert in the Xinjiang-Uyghur Autonomous Region of China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.U21B..01B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.U21B..01B"><span>Importance of Anthropogenic <span class="hlt">Aerosols</span> for Climate Prediction: a Study on East Asian Sulfate <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bartlett, R. E.; Bollasina, M. A.</p> <p>2017-12-01</p> <p>Climate prediction is vital to ensure that we are able to adapt to our changing climate. Understandably, the main focus for such prediction is greenhouse gas forcing, as this will be the main anthropogenic driver of long-term global climate change; however, other forcings could still be important. Atmospheric <span class="hlt">aerosols</span> represent one such forcing, especially in regions with high present-day <span class="hlt">aerosol</span> loading such as Asia; yet, uncertainty in their future emissions are under-sampled by commonly used climate forcing projections, such as the Representative Concentration Pathways (RCPs). Globally, anthropogenic <span class="hlt">aerosols</span> exert a net cooling, but their effects show large variation at regional <span class="hlt">scales</span>. Studies have shown that <span class="hlt">aerosols</span> impact locally upon temperature, precipitation and hydroclimate, and also upon larger <span class="hlt">scale</span> atmospheric circulation (for example, the Asian monsoon) with implications for climate remote from <span class="hlt">aerosol</span> sources. We investigate how future climate could evolve differently given the same greenhouse gas forcing pathway but differing <span class="hlt">aerosol</span> emissions. Specifically, we use climate modelling experiments (using HadGEM2-ES) of two scenarios based upon RCP2.6 greenhouse gas forcing but with large differences in sulfur dioxide emissions over East Asia. Results show that increased sulfate <span class="hlt">aerosols</span> (associated with increased sulfur dioxide) lead to large regional cooling through <span class="hlt">aerosol</span>-radiation and <span class="hlt">aerosol</span>-cloud interactions. Focussing on dynamical mechanisms, we explore the consequences of this cooling for the Asian summer and winter monsoons. In addition to local temperature and precipitation changes, we find significant changes to large <span class="hlt">scale</span> atmospheric circulation. Wave-like responses to upper-level atmospheric changes propagate across the northern hemisphere with far-reaching effects on surface climate, for example, cooling over Europe. Within the tropics, we find alterations to zonal circulation (notably, shifts in the Pacific Walker cell) and monsoon</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010069577','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010069577"><span>Measurements of <span class="hlt">Aerosol</span> Vertical Profiles and Optical Properties during INDOEX 1999 Using Micro-Pulse Lidars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Welton, Ellsworth J.; Voss, Kenneth J.; Quinn, Patricia K.; Flatau, Piotr J.; Markowicz, Krzysztof; Campbell, James R.; Spinhirne, James D.; Gordon, Howard R.; Johnson, James E.; Starr, David OC. (Technical Monitor)</p> <p>2001-01-01</p> <p>Micro-pulse lidar systems (MPL) were used to measure <span class="hlt">aerosol</span> properties during the Indian Ocean Experiment (INDOEX) 1999 field phase. Measurements were made from two platforms: the NOAA ship RN Ronald H. Brown, and the Kaashidhoo Climate Observatory (KCO) in the Maldives. Sunphotometers were used to provide <span class="hlt">aerosol</span> optical depths (AOD) needed to calibrate the MPL. This study focuses on the <span class="hlt">height</span> distribution and optical properties (at 523 nm) of <span class="hlt">aerosols</span> observed during the campaign. The <span class="hlt">height</span> of the highest <span class="hlt">aerosols</span> (top <span class="hlt">height</span>) was calculated and found to be below 4 km for most of the cruise. The marine boundary layer (MBL) top was calculated and found to be less than 1 km. MPL results were combined with air mass trajectories, radiosonde profiles of temperature and humidity, and <span class="hlt">aerosol</span> concentration and optical measurements. Humidity varied from approximately 80% near the surface to 50% near the top <span class="hlt">height</span> during the entire cruise. The average value and standard deviation of <span class="hlt">aerosol</span> optical parameters were determined for characteristic air mass regimes. Marine <span class="hlt">aerosols</span> in the absence of any continental influence were found to have an AOD of 0.05 +/- 0.03, an extinction-to-backscatter ratio (S-ratio) of 33 +/- 6 sr, and peak extinction values around 0.05/km (near the MBL top). The marine results are shown to be in agreement with previously measured and expected values. Polluted marine areas over the Indian Ocean, influenced by continental <span class="hlt">aerosols</span>, had AOD values in excess of 0.2, S-ratios well above 40 sr, and peak extinction values approximately 0.20/km (near the MBL top). The polluted marine results are shown to be similar to previously published values for continental <span class="hlt">aerosols</span>. Comparisons between MPL derived extinction near the ship (75 m) and extinction calculated at ship-level using scattering measured by a nephelometer and absorption using a PSAP were conducted. The comparisons indicated that the MPL algorithm (using a constant S-ratio throughout the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACP....14.4749M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACP....14.4749M"><span>Impacts of increasing the <span class="hlt">aerosol</span> complexity in the Met Office global numerical weather prediction model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulcahy, J. P.; Walters, D. N.; Bellouin, N.; Milton, S. F.</p> <p>2014-05-01</p> <p>The inclusion of the direct and indirect radiative effects of <span class="hlt">aerosols</span> in high-resolution global numerical weather prediction (NWP) models is being increasingly recognised as important for the improved accuracy of short-range weather forecasts. In this study the impacts of increasing the <span class="hlt">aerosol</span> complexity in the global NWP configuration of the Met Office Unified Model (MetUM) are investigated. A hierarchy of <span class="hlt">aerosol</span> representations are evaluated including three-dimensional monthly mean speciated <span class="hlt">aerosol</span> climatologies, fully prognostic <span class="hlt">aerosols</span> modelled using the CLASSIC <span class="hlt">aerosol</span> scheme and finally, initialised <span class="hlt">aerosols</span> using assimilated <span class="hlt">aerosol</span> fields from the GEMS project. The prognostic <span class="hlt">aerosol</span> schemes are better able to predict the temporal and spatial variation of atmospheric <span class="hlt">aerosol</span> optical depth, which is particularly important in cases of large sporadic <span class="hlt">aerosol</span> events such as large dust storms or forest fires. Including the direct effect of <span class="hlt">aerosols</span> improves model biases in outgoing long-wave radiation over West Africa due to a better representation of dust. However, uncertainties in dust optical properties propagate to its direct effect and the subsequent model response. Inclusion of the indirect <span class="hlt">aerosol</span> effects improves surface radiation biases at the North Slope of Alaska ARM site due to lower cloud amounts in high-latitude clean-air regions. This leads to improved temperature and <span class="hlt">height</span> forecasts in this region. Impacts on the global mean model precipitation and large-<span class="hlt">scale</span> circulation fields were found to be generally small in the short-range forecasts. However, the indirect <span class="hlt">aerosol</span> effect leads to a strengthening of the low-level monsoon flow over the Arabian Sea and Bay of Bengal and an increase in precipitation over Southeast Asia. Regional impacts on the African Easterly Jet (AEJ) are also presented with the large dust loading in the <span class="hlt">aerosol</span> climatology enhancing of the heat low over West Africa and weakening the AEJ. This study highlights the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012GeoRL..39.9809Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012GeoRL..39.9809Z"><span>Increases in <span class="hlt">aerosol</span> concentrations over eastern China due to the decadal-<span class="hlt">scale</span> weakening of the East Asian summer monsoon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Jianlei; Liao, Hong; Li, Jianping</p> <p>2012-05-01</p> <p>China has been experiencing increased concentrations of <span class="hlt">aerosols</span>, commonly attributed to the large increases in emissions associated with the rapid economic development. We show by using a chemical transport model driven by the assimilated meteorological fields that the observed decadal-<span class="hlt">scale</span> weakening of the East Asian summer monsoon also contributed to the increases in <span class="hlt">aerosols</span> in China. We find that the simulated <span class="hlt">aerosol</span> concentrations have strong negative correlations with the strength of the East Asian Summer monsoon. Accounting for sulfate, nitrate, ammonium, black carbon, and organic carbon <span class="hlt">aerosols</span>, the summer surface-layer PM2.5 concentration averaged over eastern China (110°-125°E, 20°-45°N) can be 17.7% higher in the weakest monsoon years than in the strongest monsoon years. The weakening of the East Asian Summer monsoon increases <span class="hlt">aerosol</span> concentrations mainly by the changes in atmospheric circulation (the convergence of air pollutants) in eastern China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.3929S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.3929S"><span>An intercomparison of long-term planetary boundary layer <span class="hlt">heights</span> retrieved from CALIPSO, ground-based lidar, and radiosonde measurements over Hong Kong</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Su, Tianning; Li, Jing; Li, Chengcai; Xiang, Pengzhan; Lau, Alexis Kai-Hon; Guo, Jianping; Yang, Dongwei; Miao, Yucong</p> <p>2017-04-01</p> <p>The planetary boundary layer <span class="hlt">height</span> (PBLH) is a very important parameter in the atmosphere, because it determines the range where the most effective dispersion processes take place, and serves as a constraint on the vertical transport of heat, moisture, and pollutants. As the only space-borne lidar, Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization onboard Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) measures the vertical distribution of <span class="hlt">aerosol</span> signals and thus offers the potential to retrieve large-<span class="hlt">scale</span> PBLH climatology. In this study, we explore different techniques for retrieving PBLH from CALIPSO measurements and validate the results against those obtained from ground-based micropulse lidar (MPL) and radiosonde (RS) data over Hong Kong, where long-term MPL and RS measurements are available. Two methods, namely maximum standard deviation (MSD) and wavelet covariance transform (WCT), are used to retrieve PBLH from CALIPSO. Results show that the RS- and MPL-derived PBLHs share similar interannual variation and seasonality and can complement each other. Both MSD and WCT perform reasonably well compared with MPL/RS products, especially under sufficient <span class="hlt">aerosol</span> loading. Uncertainties increase when <span class="hlt">aerosol</span> loading is low and the CALIPSO signal consequently becomes noisier. Overall, CALIPSO captures the general PBLH seasonal variability over Hong Kong, despite a high bias in spring and a low bias in summer. The spring high bias is likely associated with elevated <span class="hlt">aerosol</span> layers due to transport, while the summer low bias can be attributed to higher noise level associated with weaker <span class="hlt">aerosol</span> signal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.H21A1073H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.H21A1073H"><span><span class="hlt">Aerosol</span> Delivery for Amendment Distribution in Contaminated Vadose Zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hall, R. J.; Murdoch, L.; Riha, B.; Looney, B.</p> <p>2011-12-01</p> <p>Remediation of contaminated vadose zones is often hindered by an inability to effectively distribute amendments. Many amendment-based approaches have been successful in saturated formations, however, have not been widely pursued when treating contaminated unsaturated materials due to amendment distribution limitations. <span class="hlt">Aerosol</span> delivery is a promising new approach for distributing amendments in contaminated vadose zones. Amendments are <span class="hlt">aerosolized</span> and injected through well screens. During injection the <span class="hlt">aerosol</span> particles are transported with the gas and deposited on the surfaces of soil grains. Resulting distributions are radially and vertically broad, which could not be achieved by injecting pure liquid-phase solutions. The objectives of this work were A) to characterize transport and deposition behaviors of <span class="hlt">aerosols</span>; and B) to develop capabilities for predicting results of <span class="hlt">aerosol</span> injection scenarios. <span class="hlt">Aerosol</span> transport and deposition processes were investigated by conducting lab-<span class="hlt">scale</span> injection experiments. These experiments involved injection of <span class="hlt">aerosols</span> through a 2m radius, sand-filled wedge. A particle analyzer was used to measure <span class="hlt">aerosol</span> particle distributions with time, and sand samples were taken for amendment content analysis. Predictive capabilities were obtained by constructing a numerical model capable of simulating <span class="hlt">aerosol</span> transport and deposition in porous media. Results from tests involving vegetable oil <span class="hlt">aerosol</span> injection show that liquid contents appropriate for remedial applications could be readily achieved throughout the sand-filled wedge. Lab-<span class="hlt">scale</span> tests conducted with aqueous <span class="hlt">aerosols</span> show that liquid accumulation only occurs near the point of injection. Tests were also conducted using 200 g/L salt water as the <span class="hlt">aerosolized</span> liquid. Liquid accumulations observed during salt water tests were minimal and similar to aqueous <span class="hlt">aerosol</span> results. However, particles were measured, and salt deposited distal to the point of injection. Differences between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A13F3257A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A13F3257A"><span>Airborne LIDAR Measurements of <span class="hlt">Aerosol</span> and Ozone Above the Alberta Oil Sands Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aggarwal, M.; Whiteway, J. A.; Seabrook, J.; Gray, L. H.</p> <p>2014-12-01</p> <p>Lidar measurements of ozone and <span class="hlt">aerosol</span> were conducted from a Twin Otter aircraft above the oil sands region of northern Alberta. The field campaign was carried out with a total of five flights out of Fort McMurray, Alberta during the period between August 22 and August 26, 2013. Significant amounts of <span class="hlt">aerosol</span> were observed within the boundary layer, up to a <span class="hlt">height</span> of 1.6 km, but the ozone concentration remained at or below background levels. On August 24th the lidar observed a separated layer of <span class="hlt">aerosol</span> above the boundary layer, at a <span class="hlt">height</span> of 1.8 km, in which the ozone mixing ratio increased to 70 ppbv. Backward trajectory calculations revealed that the air containing this separated <span class="hlt">aerosol</span> layer had passed over an area of forest fires. Directly below the layer of forest fire smoke, in the pollution from the oil sands industry, the measured ozone mixing ratio was lower than the background levels (≤35 ppbv).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A23F0399D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A23F0399D"><span>Biology of the Coarse <span class="hlt">Aerosol</span> Mode: Insights Into Urban <span class="hlt">Aerosol</span> Ecology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dueker, E.; O'Mullan, G. D.; Montero, A.</p> <p>2015-12-01</p> <p>Microbial <span class="hlt">aerosols</span> have been understudied, despite implications for climate studies, public health, and biogeochemical cycling. Because viable bacterial <span class="hlt">aerosols</span> are often associated with coarse <span class="hlt">aerosol</span> particles, our limited understanding of the coarse <span class="hlt">aerosol</span> mode further impedes our ability to develop models of viable bacterial <span class="hlt">aerosol</span> production, transport, and fate in the outdoor environment, particularly in crowded urban centers. To address this knowledge gap, we studied <span class="hlt">aerosol</span> particle biology and size distributions in a broad range of urban and rural settings. Our previously published findings suggest a link between microbial viability and local production of coarse <span class="hlt">aerosols</span> from waterways, waste treatment facilities, and terrestrial systems in urban and rural environments. Both in coastal Maine and in New York Harbor, coarse <span class="hlt">aerosols</span> and viable bacterial <span class="hlt">aerosols</span> increased with increasing wind speeds above 4 m s-1, a dynamic that was observed over time <span class="hlt">scales</span> ranging from minutes to hours. At a New York City superfund-designated waterway regularly contaminated with raw sewage, aeration remediation efforts resulted in significant increases of coarse <span class="hlt">aerosols</span> and bacterial <span class="hlt">aerosols</span> above that waterway. Our current research indicates that bacterial communities in <span class="hlt">aerosols</span> at this superfund site have a greater similarity to bacterial communities in the contaminated waterway with wind speeds above 4 m s-1. Size-fractionated sampling of viable microbial <span class="hlt">aerosols</span> along the urban waterfront has also revealed significant shifts in bacterial <span class="hlt">aerosols</span>, and specifically bacteria associated with coarse <span class="hlt">aerosols</span>, when wind direction changes from onshore to offshore. This research highlights the key connections between bacterial <span class="hlt">aerosol</span> viability and the coarse <span class="hlt">aerosol</span> fraction, which is important in assessments of production, transport, and fate of bacterial contamination in the urban environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820010903&hterms=properties+physical+gases&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dproperties%2Bphysical%2Bgases','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820010903&hterms=properties+physical+gases&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dproperties%2Bphysical%2Bgases"><span>Stratospheric <span class="hlt">aerosols</span> and precursor gases</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1982-01-01</p> <p>Measurements were made of the <span class="hlt">aerosol</span> size, <span class="hlt">height</span> and geographical distribution, their composition and optical properties, and their temporal variation with season and following large volcanic eruptions. Sulfur-bearing gases were measured in situ in the stratosphere, and studied of the chemical and physical processes which control gas-to-particle conversion were carried out in the laboratory.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ems..confE.261G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ems..confE.261G"><span>The Tall Wind project - exploring the wind profile and boundary-layer <span class="hlt">height</span> in the atmosphere's first kilometer over flat terrain.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gryning, S. E.; Batchvarova, E.; Pena, A.; Mikkelsen, T.; Brümmer, B.; Emeis, S.; Gulstad, L.; Lee, N.</p> <p>2010-09-01</p> <p>Predicting the wind at typical <span class="hlt">heights</span> of present and future wind turbines is a considerable scientific challenge. Presently applied models are accurate within the surface layer. New measurements and instrument synergies are necessary as basis for developing new wind models and understanding the physical processes that form the wind profile in order to describe the wind profile above it. Analysis of the wind and turbulence profiles from a meteorological mast at <span class="hlt">heights</span> up to 160 meters and wind lidars up to 300 meters at the National test station at Høvsøre, Denmark, shows deviations of the wind profile above 80 meters the from the profile used so far near the surface. It also reveals the importance of the boundary-layer <span class="hlt">height</span> as a physical parameter for the description of the wind profile. In the Tall Wind project, mast and lidar measurements of wind and fluxes will be combined with monitoring of the boundary-layer <span class="hlt">height</span> by use of an <span class="hlt">aerosol</span> lidar. At the main project monitoring sites (Høvsøre in Denmark and Hamburg in Germany) long term monitoring programmes on tall masts (160 and 300 meters) already exists and will be intensified. As part of the project the wind profile will be measured up to 1000 meters by a wind lidar (windcube) and the boundary-layer <span class="hlt">height</span> by an <span class="hlt">aerosol</span> lidar. The new data sets can be used for theoretical developments and evaluation of meso-<span class="hlt">scale</span> meteorological models. The project is an international collaboration between academia (Risoe-DTU, HU and KIT) and industry (Vestas and DONG), funded by the Danish Research Agency, the Strategic Research Council (Sagsnr. 2104-08-0025). In the paper the set-up of the Tall Wind project will be described and some first results and experience will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACPD...1015417G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACPD...1015417G"><span>A critical look at spatial <span class="hlt">scale</span> choices in satellite-based <span class="hlt">aerosol</span> indirect effect studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grandey, B. S.; Stier, P.</p> <p>2010-06-01</p> <p>Analysing satellite datasets over large regions may introduce spurious relationships between <span class="hlt">aerosol</span> and cloud properties due to spatial variations in <span class="hlt">aerosol</span> type, cloud regime and synoptic regime climatologies. Using MODerate resolution Imaging Spectroradiometer data, we calculate relationships between <span class="hlt">aerosol</span> optical depth τa, derived liquid cloud droplet effective number concentration Ne and liquid cloud droplet effective radius re at different spatial <span class="hlt">scales</span>. Generally, positive values of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: .7em; color: #000;"> dlnNe <span style="margin-left: -2.5em; margin-right: .5em; vertical-align: -15%; font-size: .7em; color: #000;"> dlnτa are found for ocean regions, whilst negative values occur for many land regions. The spatial distribution of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: .7em; color: #000;"> dlnre <span style="margin-left: -2.5em; margin-right: .5em; vertical-align: -15%; font-size: .7em; color: #000;"> dlnτa shows approximately the opposite pattern, with generally postive values for land regions and negative values for ocean regions. We find that for region sizes larger than 4°×4°, spurious spatial variations in retrieved cloud and <span class="hlt">aerosol</span> properties can introduce widespread significant errors to calculations of <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: .7em; color: #000;"> dlnNe <span style="margin-left: -2.5em; margin-right: .5em; vertical-align: -15%; font-size: .7em; color: #000;"> dlnτa and <span style="border-bottom: 1px solid #000; vertical-align: 50%; font-size: .7em; color: #000;"> dlnre <span style="margin-left: -2.5em; margin-right: .5em; vertical-align: -15%; font-size: .7em; color: #000;"> dlnτa . For regions on the <span class="hlt">scale</span> of 60°×60°, these methodological errors may lead to an overestimate in global cloud albedo effect radiative forcing of order 80%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150000271','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150000271"><span>Stereoscopic Retrieval of Smoke Plume <span class="hlt">Heights</span> and Motion from Space-Based Multi-Angle Imaging, Using the MISR INteractive eXplorer(MINX)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nelson, David L.; Kahn, Ralph A.</p> <p>2014-01-01</p> <p>Airborne particles desert dust, wildfire smoke, volcanic effluent, urban pollution affect Earth's climate as well as air quality and health. They are found in the atmosphere all over the planet, but vary immensely in amount and properties with season and location. Most <span class="hlt">aerosol</span> particles are injected into the near-surface boundary layer, but some, especially wildfire smoke, desert dust and volcanic ash, can be injected higher into the atmosphere, where they can stay aloft longer, travel farther, produce larger climate effects, and possibly affect human and ecosystem health far downwind. So monitoring <span class="hlt">aerosol</span> injection <span class="hlt">height</span> globally can make important contributions to climate science and air quality studies. The Multi-angle Imaging Spectro-Radiometer (MISR) is a space borne instrument designed to study Earths clouds, <span class="hlt">aerosols</span>, and surface. Since late February 2000 it has been retrieving <span class="hlt">aerosol</span> particle amount and properties, as well as cloud <span class="hlt">height</span> and wind data, globally, about once per week. The MINX visualization and analysis tool complements the operational MISR data products, enabling users to retrieve <span class="hlt">heights</span> and winds locally for detailed studies of smoke plumes, at higher spatial resolution and with greater precision than the operational product and other space-based, passive remote sensing techniques. MINX software is being used to provide plume <span class="hlt">height</span> statistics for climatological studies as well as to investigate the dynamics of individual plumes, and to provide parameterizations for climate modeling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988RvGeo..26...89S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988RvGeo..26...89S"><span>Antarctic <span class="hlt">aerosols</span> - 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>Shaw, Glenn E.</p> <p>1988-02-01</p> <p>Tropospheric <span class="hlt">aerosols</span> with the diameter range of half a micron reside in the atmosphere for tens of days and teleconnect Antarctica with other regions by transport that reaches planetary <span class="hlt">scales</span> of distances; thus, the <span class="hlt">aerosol</span> on the Antarctic ice represents 'memory modules' of events that took place at regions separated from Antarctica by tens of thousands of kilometers. In terms of <span class="hlt">aerosol</span> mass, the <span class="hlt">aerosol</span> species include insoluble crustal products (less than 5 percent), transported sea-salt residues (highly variable but averaging about 10 percent), Ni-rich meteoric material, and anomalously enriched material with an unknown origin. Most (70-90 percent by mass) of the <span class="hlt">aerosol</span> over the Antarctic ice shield, however, is the 'natural acid sulfate <span class="hlt">aerosol</span>', apparently deriving from biological processes taking place in the surrounding oceans.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012Nanos...4.3746S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012Nanos...4.3746S"><span>Simultaneous growth of self-patterned carbon nanotube forests with dual <span class="hlt">height</span> <span class="hlt">scales</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sam, Ebru Devrim; Kucukayan-Dogu, Gokce; Baykal, Beril; Dalkilic, Zeynep; Rana, Kuldeep; Bengu, Erman</p> <p>2012-05-01</p> <p>In this study, we report on a unique, one-step fabrication technique enabling the simultaneous synthesis of vertically aligned multi-walled carbon nanotubes (VA-MWCNTs) with dual <span class="hlt">height</span> <span class="hlt">scales</span> through alcohol catalyzed chemical vapor deposition (ACCVD). Regions of VA-MWCNTs with different <span class="hlt">heights</span> were well separated from each other leading to a self-patterning on the surface. We devised a unique layer-by-layer process for application of catalyst and inhibitor precursors on oxidized Si (100) surfaces before the ACCVD step to achieve a hierarchical arrangement. Patterning could be controlled by adjusting the molarity and application sequence of precursors. Contact angle measurements on these self-patterned surfaces indicated that manipulation of these hierarchical arrays resulted in a wide range of hydrophobic behavior changing from that of a sticky rose petal to a lotus leaf.In this study, we report on a unique, one-step fabrication technique enabling the simultaneous synthesis of vertically aligned multi-walled carbon nanotubes (VA-MWCNTs) with dual <span class="hlt">height</span> <span class="hlt">scales</span> through alcohol catalyzed chemical vapor deposition (ACCVD). Regions of VA-MWCNTs with different <span class="hlt">heights</span> were well separated from each other leading to a self-patterning on the surface. We devised a unique layer-by-layer process for application of catalyst and inhibitor precursors on oxidized Si (100) surfaces before the ACCVD step to achieve a hierarchical arrangement. Patterning could be controlled by adjusting the molarity and application sequence of precursors. Contact angle measurements on these self-patterned surfaces indicated that manipulation of these hierarchical arrays resulted in a wide range of hydrophobic behavior changing from that of a sticky rose petal to a lotus leaf. Electronic supplementary information (ESI) available: Fig. S1; AFM image of the Co-O layer which was first dried at 40 °C and then oxidized at 200 °C. Fig. S2; graph relative to the area of CNT islands for different</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940017171','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940017171"><span>Stratospheric <span class="hlt">Aerosol</span> and Gas Experiment (SAGE 3)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mccormick, M. P.</p> <p>1993-01-01</p> <p>The proposed SAGE III instrument would be the principal source of data for global changes of stratospheric <span class="hlt">aerosols</span>, stratospheric water vapor, and ozone profiles, and a contributing source of data for upper tropospheric water vapor, <span class="hlt">aerosols</span>, and clouds. The ability to obtain such data has been demonstrated by the predecessor instrument, SAGE II, but SAGE III will be substantially more capable, as discussed below. The capabilities for monitoring the profiles of atmospheric constituents have been verified in detail, including ground-based validations, for <span class="hlt">aerosol</span>, ozone, and water vapor. Indeed, because of its self-calibrating characteristics, SAGE II was an essential component of the international ozone trend assessments, and SAGE II is now proving to be invaluable in tracking the <span class="hlt">aerosols</span> from Mt. Pinatubo. Although SAGE profiles generally terminate at the <span class="hlt">height</span> of the first tropospheric cloud layer, it has been found that the measurements extend down to 3 km altitude more than 40 percent of the time at most latitudes. Thus, useful information can also be obtained on upper tropospheric <span class="hlt">aerosols</span>, water vapor, and ozone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308471&keyword=Scheme&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=308471&keyword=Scheme&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>Grid-<span class="hlt">scale</span> Indirect Radiative Forcing of Climate due to <span class="hlt">aerosols</span> over the northern hemisphere simulated by the integrated WRF-CMAQ model: Preliminary results</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>In this study, indirect <span class="hlt">aerosol</span> effects on grid-<span class="hlt">scale</span> clouds were implemented in the integrated WRF3.3-CMAQ5.0 modeling system by including parameterizations for both cloud droplet and ice number concentrations calculated from the CMAQ-predicted <span class="hlt">aerosol</span> particles. The resulting c...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JGR...104.6477Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JGR...104.6477Q"><span>Interactive coupling of regional climate and sulfate <span class="hlt">aerosol</span> models over eastern Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qian, Yun; Giorgi, Filippo</p> <p>1999-03-01</p> <p>The NCAR regional climate model (RegCM) is interactively coupled to a simple radiatively active sulfate <span class="hlt">aerosol</span> model over eastern Asia. Both direct and indirect <span class="hlt">aerosol</span> effects are represented. The coupled model system is tested for two simulation periods, November 1994 and July 1995, with <span class="hlt">aerosol</span> sources representative of present-day anthropogenic sulfur emissions. The model sensitivity to the intensity of the <span class="hlt">aerosol</span> source is also studied. The main conclusions from our work are as follows: (1) The <span class="hlt">aerosol</span> distribution and cycling processes show substantial regional spatial variability, and temporal variability varying on a range of <span class="hlt">scales</span>, from the diurnal <span class="hlt">scale</span> of boundary layer and cumulus cloud evolution to the 3-10 day <span class="hlt">scale</span> of synoptic <span class="hlt">scale</span> events and the interseasonal <span class="hlt">scale</span> of general circulation features; (2) both direct and indirect <span class="hlt">aerosol</span> forcings have regional effects on surface climate; (3) the regional climate response to the <span class="hlt">aerosol</span> forcing is highly nonlinear, especially during the summer, due to the interactions with cloud and precipitation processes; (4) in our simulations the role of the <span class="hlt">aerosol</span> indirect effects is dominant over that of direct effects; (5) <span class="hlt">aerosol</span>-induced feedback processes can affect the <span class="hlt">aerosol</span> burdens at the subregional <span class="hlt">scale</span>. This work constitutes the first step in a long term research project aimed at coupling a hierarchy of chemistry/<span class="hlt">aerosol</span> models to the RegCM over the eastern Asia region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1195588','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1195588"><span>A new WRF-Chem treatment for studying regional-<span class="hlt">scale</span> impacts of cloud processes on <span class="hlt">aerosol</span> and trace gases in parameterized cumuli</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>Berg, L. K.; Shrivastava, M.; Easter, R. C.</p> <p></p> <p>A new treatment of cloud effects on <span class="hlt">aerosol</span> and trace gases within parameterized shallow and deep convection, and <span class="hlt">aerosol</span> effects on cloud droplet number, has been implemented in the Weather Research and Forecasting model coupled with Chemistry (WRF-Chem) version 3.2.1 that can be used to better understand the <span class="hlt">aerosol</span> life cycle over regional to synoptic <span class="hlt">scales</span>. The modifications to the model include treatment of the cloud droplet number mixing ratio; key cloud microphysical and macrophysical parameters (including the updraft fractional area, updraft and downdraft mass fluxes, and entrainment) averaged over the population of shallow clouds, or a single deep convectivemore » cloud; and vertical transport, activation/resuspension, aqueous chemistry, and wet removal of <span class="hlt">aerosol</span> and trace gases in warm clouds. These changes have been implemented in both the WRF-Chem chemistry packages as well as the Kain–Fritsch (KF) cumulus parameterization that has been modified to better represent shallow convective clouds. Testing of the modified WRF-Chem has been completed using observations from the Cumulus Humilis <span class="hlt">Aerosol</span> Processing Study (CHAPS). The simulation results are used to investigate the impact of cloud–<span class="hlt">aerosol</span> interactions on regional-<span class="hlt">scale</span> transport of black carbon (BC), organic <span class="hlt">aerosol</span> (OA), and sulfate <span class="hlt">aerosol</span>. Based on the simulations presented here, changes in the column-integrated BC can be as large as –50% when cloud–<span class="hlt">aerosol</span> interactions are considered (due largely to wet removal), or as large as +40% for sulfate under non-precipitating conditions due to sulfate production in the parameterized clouds. The modifications to WRF-Chem are found to account for changes in the cloud droplet number concentration (CDNC) and changes in the chemical composition of cloud droplet residuals in a way that is consistent with observations collected during CHAPS. Efforts are currently underway to port the changes described here to the latest version of WRF-Chem, and it</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1195588-new-wrf-chem-treatment-studying-regional-scale-impacts-cloud-processes-aerosol-trace-gases-parameterized-cumuli','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1195588-new-wrf-chem-treatment-studying-regional-scale-impacts-cloud-processes-aerosol-trace-gases-parameterized-cumuli"><span>A new WRF-Chem treatment for studying regional-<span class="hlt">scale</span> impacts of cloud processes on <span class="hlt">aerosol</span> and trace gases in parameterized cumuli</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Berg, L. K.; Shrivastava, M.; Easter, R. C.; ...</p> <p>2015-02-24</p> <p>A new treatment of cloud effects on <span class="hlt">aerosol</span> and trace gases within parameterized shallow and deep convection, and <span class="hlt">aerosol</span> effects on cloud droplet number, has been implemented in the Weather Research and Forecasting model coupled with Chemistry (WRF-Chem) version 3.2.1 that can be used to better understand the <span class="hlt">aerosol</span> life cycle over regional to synoptic <span class="hlt">scales</span>. The modifications to the model include treatment of the cloud droplet number mixing ratio; key cloud microphysical and macrophysical parameters (including the updraft fractional area, updraft and downdraft mass fluxes, and entrainment) averaged over the population of shallow clouds, or a single deep convectivemore » cloud; and vertical transport, activation/resuspension, aqueous chemistry, and wet removal of <span class="hlt">aerosol</span> and trace gases in warm clouds. These changes have been implemented in both the WRF-Chem chemistry packages as well as the Kain–Fritsch (KF) cumulus parameterization that has been modified to better represent shallow convective clouds. Testing of the modified WRF-Chem has been completed using observations from the Cumulus Humilis <span class="hlt">Aerosol</span> Processing Study (CHAPS). The simulation results are used to investigate the impact of cloud–<span class="hlt">aerosol</span> interactions on regional-<span class="hlt">scale</span> transport of black carbon (BC), organic <span class="hlt">aerosol</span> (OA), and sulfate <span class="hlt">aerosol</span>. Based on the simulations presented here, changes in the column-integrated BC can be as large as –50% when cloud–<span class="hlt">aerosol</span> interactions are considered (due largely to wet removal), or as large as +40% for sulfate under non-precipitating conditions due to sulfate production in the parameterized clouds. The modifications to WRF-Chem are found to account for changes in the cloud droplet number concentration (CDNC) and changes in the chemical composition of cloud droplet residuals in a way that is consistent with observations collected during CHAPS. Efforts are currently underway to port the changes described here to the latest version of WRF-Chem, and it</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1043372-assessing-regional-scale-predictions-aerosols-marine-stratocumulus-interactions-during-vocals-rex-using-wrf-chem','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1043372-assessing-regional-scale-predictions-aerosols-marine-stratocumulus-interactions-during-vocals-rex-using-wrf-chem"><span>Assessing regional <span class="hlt">scale</span> predictions of <span class="hlt">aerosols</span>, marine stratocumulus, and their interactions during VOCALS-REx using WRF-Chem</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>Yang Q.; Lee Y.; Gustafson Jr., W. I.</p> <p>2011-12-02</p> <p> observations in AERO, compared to the MET simulation. Nevertheless, biases in some of the simulated meteorological quantities (e.g., MBL temperature and humidity) and <span class="hlt">aerosol</span> quantities (e.g., underestimations of accumulation mode <span class="hlt">aerosol</span> number) might affect simulated stratocumulus and energy fluxes over the Southeastern Pacific, and require further investigation. The well-simulated timing and outflow patterns of polluted and clean episodes demonstrate the model's ability to capture daily/synoptic <span class="hlt">scale</span> variations of <span class="hlt">aerosol</span> and cloud properties, and suggest that the model is suitable for studying atmospheric processes associated with pollution outflow over the ocean. The overall performance of the regional model in simulating mesoscale clouds and boundary layer properties is encouraging and suggests that reproducing gradients of <span class="hlt">aerosol</span> and cloud droplet concentrations and coupling cloud-<span class="hlt">aerosol</span>-radiation processes are important when simulating marine stratocumulus over the Southeast Pacific.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.A33B0979H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.A33B0979H"><span>Seasonality of Forcing by Carbonaceous <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Habib, G.; Bond, T.; Rasch, P. J.; Coleman, D.</p> <p>2006-12-01</p> <p><span class="hlt">Aerosols</span> can influence the energy balance of Earth-Atmosphere system with profound effect on regional climate. Atmospheric processes, such as convection, scavenging, wet and dry deposition, govern the lifetime and location of <span class="hlt">aerosol</span>; emissions affect its quantity and location. Both affect climate forcing. Here we investigate the effect of seasonality in emissions and atmospheric processes on radiative forcing by carbonaceous <span class="hlt">aerosols</span>, focusing on <span class="hlt">aerosol</span> from fossil fuel and biofuel. Because <span class="hlt">aerosol</span> lifetime is seasonal, ignoring the seasonality of sources such as residential biofuel may introduce a bias in <span class="hlt">aerosol</span> burden and therefore in predicted climate forcing. We present a global emission inventory of carbonaceous <span class="hlt">aerosols</span> with seasonality, and simulate atmospheric concentrations using the Community Atmosphere Model (CAM). We discuss where and when the seasonality of emissions and atmospheric processes has strong effects on atmospheric burden, lifetime, climate forcing and <span class="hlt">aerosol</span> optical depth (AOD). Previous work has shown that <span class="hlt">aerosol</span> forcing is higher in summer than in winter, and has identified the importance of <span class="hlt">aerosol</span> above cloud in determining black carbon forcing. We show that predicted cloud <span class="hlt">height</span> is a very important factor in determining normalized radiative forcing (forcing per mass), especially in summer. This can affect the average summer radiative forcing by nearly 50%. Removal by cloud droplets is the dominant atmospheric cleansing mechanism for carbonaceous <span class="hlt">aerosols</span>. We demonstrate the modeled seasonality of removal processes and compare the importance of scavenging by warm and cold clouds. Both types of clouds contribute significantly to <span class="hlt">aerosol</span> removal. We estimate uncertainty in direct radiative forcing due to scavenging by tagging the <span class="hlt">aerosol</span> which has experienced cloud interactions. Finally, seasonal variations offer an opportunity to assess modeled processes when a single process dominates variability. We identify regions where <span class="hlt">aerosol</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A11O..05T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A11O..05T"><span>The OMI <span class="hlt">Aerosol</span> Absorption Product: An A-train application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Torres, O.; Jethva, H. T.; Ahn, C.</p> <p>2017-12-01</p> <p>Because of the uniquely large sensitivity of satellite-measured near-UV radiances to absorption by desert dust, carbonaceous and volcanic ash <span class="hlt">aerosols</span>, observations by a variety of UV-capable sensors have been routinely used over the last forty years in both qualitative and quantitative applications for estimating the absorption properties of these <span class="hlt">aerosol</span> types. In this presentation we will discuss a multi-sensor application involving observations from A-train sensors OMI, AIRS and CALIOP for the creation of a 13-year record of <span class="hlt">aerosol</span> optical depth (AOD) and single scattering albedo (SSA). Determination of <span class="hlt">aerosol</span> type, in terms of particle size distribution and refractive index, is an important algorithmic step that requires using external information. AIRS CO measurements are used as carbonaceous <span class="hlt">aerosols</span> tracer to differentiate this <span class="hlt">aerosol</span> type from desert dust. On the other hand, the <span class="hlt">height</span> of the absorbing <span class="hlt">aerosol</span> layer, an important parameter in UV <span class="hlt">aerosol</span> retrievals, is prescribed using a CALIOP-based climatology. The combined use of these observations in the developments of the OMI long-term AOD/SSA record will be discussed along with an evaluation of retrieval results using independent observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMPP13E..07W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMPP13E..07W"><span>A Sulfate <span class="hlt">Aerosol</span> Trigger for the Sturtian Neoproterozoic Snowball Event</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wordsworth, R. D.; Macdonald, F. A.</p> <p>2017-12-01</p> <p>Despite the dominance of the carbon cycle in determining the evolution of Earth's climate in general, certain events defy easy explanation via atmospheric CO2 changes alone. Here we discuss the particular role that transient planetary albedo changes via sulfate <span class="hlt">aerosol</span> formation can play in major climate transitions. Specifically, we propose that SO2 outgassing associated with the eruption of the Franklin Large Igneous Province (LIP) led to the first Neoproterozoic Snowball event, the Sturtian, 716 Ma. We summarize U/Pb zircon and baddeleyite dating indicating the synchronicity of the Franklin eruptions and the onset of the Sturtian, and paleomagnetic data indicating that the Franklin erupted close to the equator. We then discuss in detail the modeling we have performed of eruption rate, the plume <span class="hlt">height</span> achieved during basaltic fissure volcanism, the chemistry and microphysics of sulfate <span class="hlt">aerosol</span> formation, and the dependence of <span class="hlt">aerosol</span> longwave and shortwave radiative effects on atmospheric loading, particle size and surface albedo. We discuss the critical importance of the latitude of eruption, the tropopause <span class="hlt">height</span>, and ocean dynamics in determining the strength and sign of <span class="hlt">aerosol</span> radiative forcing. We finish by comparing the Franklin event with other LIP emplacement events in Earth history and make suggestions for future modeling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AtmEn..43.5526Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AtmEn..43.5526Z"><span>Vertical distributions of <span class="hlt">aerosols</span> under different weather conditions: Analysis of in-situ aircraft measurements in Beijing, China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Qiang; Ma, XinCheng; Tie, Xuexi; Huang, Mengyu; Zhao, Chunsheng</p> <p></p> <p>In this study, <span class="hlt">aerosol</span> vertical distributions of 17 in-situ aircraft measurements during 2005 and 2006 springs are analyzed. The 17 flights are carefully selected to exclude dust events, and the analyses are focused on the vertical distributions of <span class="hlt">aerosol</span> particles associated with anthropogenic activities. The results show that the vertical distributions of <span class="hlt">aerosol</span> particles are strongly affected by weather and meteorological conditions, and 3 different types of <span class="hlt">aerosol</span> vertical distributions corresponding to different weather systems are defined in this study. The measurement with a flat vertical gradient and low surface <span class="hlt">aerosol</span> concentrations is defined as type-1; a gradual decrease of <span class="hlt">aerosols</span> with altitudes and modest surface <span class="hlt">aerosol</span> concentrations is defined as type-2; a sharp vertical gradient (<span class="hlt">aerosols</span> being strongly depressed in the PBL) with high surface <span class="hlt">aerosol</span> concentrations is defined as type-3. The weather conditions corresponding to the 3 different <span class="hlt">aerosol</span> types are high pressure, between two high pressures, and low pressure systems (frontal inversions), respectively. The vertical mixing and horizontal transport for the 3 different vertical distributions are analyzed. Under the type-1 condition, the vertical mixing and horizontal transport were rapid, leading to strong dilution of <span class="hlt">aerosols</span> in both vertical and horizontal directions. As a result, the <span class="hlt">aerosol</span> concentrations in PBL (planetary boundary layer) were very low, and the vertical distribution was flat. Under the type-2 condition, the vertical mixing was strong and there was no strong barrier at the PBL <span class="hlt">height</span>. The horizontal transport (wind flux) was modest. As a result, the <span class="hlt">aerosol</span> concentrations were gradually reduced with altitude, with modest surface <span class="hlt">aerosol</span> concentrations. Under the type-3 condition, there was a cold front near the region. As a result, a frontal inversion associated with weak vertical mixing appeared at the top of the inversion layer, forming a very strong barrier to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ACPD...1534149M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ACPD...1534149M"><span>Potential of polarization lidar to provide profiles of CCN- and INP-relevant <span class="hlt">aerosol</span> parameters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mamouri, R. E.; Ansmann, A.</p> <p>2015-12-01</p> <p>We investigate the potential of polarization lidar to provide vertical profiles of <span class="hlt">aerosol</span> parameters from which cloud condensation nucleus (CCN) and ice nucleating particle (INP) number concentrations can be estimated. We show that <span class="hlt">height</span> profiles of number concentrations of <span class="hlt">aerosol</span> particles with radius > 50 nm (APC50, reservoir of favorable CCN) and with radius > 250 nm (APC250, reservoir of favorable INP), as well as profiles of the <span class="hlt">aerosol</span> particle surface area concentration (ASC, used in INP parameterization) can be retrieved from lidar-derived <span class="hlt">aerosol</span> extinction coefficients (AEC) with relative uncertainties of a factor of around 2 (APC50), and of about 25-50 % (APC250, ASC). Of key importance is the potential of polarization lidar to identify mineral dust particles and to distinguish and separate the <span class="hlt">aerosol</span> properties of basic <span class="hlt">aerosol</span> types such as mineral dust and continental pollution (haze, smoke). We investigate the relationship between AEC and APC50, APC250, and ASC for the main lidar wavelengths of 355, 532 and 1064 nm and main <span class="hlt">aerosol</span> types (dust, pollution, marine). Our study is based on multiyear <span class="hlt">Aerosol</span> Robotic Network (AERONET) photometer observations of <span class="hlt">aerosol</span> optical thickness and column-integrated particle size distribution at Leipzig, Germany, and Limassol, Cyprus, which cover all realistic <span class="hlt">aerosol</span> mixtures of continental pollution, mineral dust, and marine <span class="hlt">aerosol</span>. We further include AERONET data from field campaigns in Morocco, Cabo Verde, and Barbados, which provide pure dust and pure marine <span class="hlt">aerosol</span> scenarios. By means of a simple relationship between APC50 and the CCN-reservoir particles (APCCCN) and published INP parameterization schemes (with APC250 and ASC as input) we finally compute APCCCN and INP concentration profiles. We apply the full methodology to a lidar observation of a heavy dust outbreak crossing Cyprus with dust up to 8 km <span class="hlt">height</span> and to a case during which anthropogenic pollution dominated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990004378','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990004378"><span>Impact of Tropospheric <span class="hlt">Aerosol</span> Absorption on Ozone Retrieval from buv Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Torres, O.; Bhartia, P. K.</p> <p>1998-01-01</p> <p>The impact of tropospheric <span class="hlt">aerosols</span> on the retrieval of column ozone amounts using spaceborne measurements of backscattered ultraviolet radiation is examined. Using radiative transfer calculations, we show that uv-absorbing desert dust may introduce errors as large as 10% in ozone column amount, depending on the <span class="hlt">aerosol</span> layer <span class="hlt">height</span> and optical depth. Smaller errors are produced by carbonaceous <span class="hlt">aerosols</span> that result from biomass burning. Though the error is produced by complex interactions between ozone absorption (both stratospheric and tropospheric), <span class="hlt">aerosol</span> scattering, and <span class="hlt">aerosol</span> absorption, a surprisingly simple correction procedure reduces the error to about 1%, for a variety of <span class="hlt">aerosols</span> and for a wide range of <span class="hlt">aerosol</span> loading. Comparison of the corrected TOMS data with operational data indicates that though the zonal mean total ozone derived from TOMS are not significantly affected by these errors, localized affects in the tropics can be large enough to seriously affect the studies of tropospheric ozone that are currently undergoing using the TOMS data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1034573-evaluating-wrf-chem-multi-scale-model-simulating-aerosol-radiative-properties-over-tropics-case-study-over-india','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1034573-evaluating-wrf-chem-multi-scale-model-simulating-aerosol-radiative-properties-over-tropics-case-study-over-india"><span>Evaluating WRF-Chem multi-<span class="hlt">scale</span> model in simulating <span class="hlt">aerosol</span> radiative properties over the tropics – A case study over India</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>Seethala, C.; Pandithurai, G.; Fast, Jerome D.</p> <p></p> <p>We utilized WRF-Chem multi-<span class="hlt">scale</span> model to simulate the regional distribution of <span class="hlt">aerosols</span>, optical properties and its effect on radiation over India for a winter month. The model is evaluated using measurements obtained from upper-air soundings, AERONET sun photometers, various satellite instruments, and pyranometers operated by the Indian Meteorological Department. The simulated downward shortwave flux was overestimated when the effect of <span class="hlt">aerosols</span> on radiation and clouds was neglected. Downward shortwave radiation from a simulation that included <span class="hlt">aerosol</span>-radiation interaction processes was 5 to 25 Wm{sup -2} closer to the observations, while a simulation that included <span class="hlt">aerosol</span>-cloud interaction processes were another 1 tomore » 20 Wm{sup -2} closer to the observations. For the few observations available, the model usually underestimated particulate concentration. This is likely due to turbulent mixing, transport errors and the lack of secondary organic <span class="hlt">aerosol</span> treatment in the model. The model efficiently captured the broad regional hotspots such as high <span class="hlt">aerosol</span> optical depth over Indo-Gangetic basin as well as the northwestern and southern part of India. The regional distribution of <span class="hlt">aerosol</span> optical depth compares well with AVHRR <span class="hlt">aerosol</span> optical depth and the TOMS <span class="hlt">aerosol</span> index. The magnitude and wavelength-dependence of simulated <span class="hlt">aerosol</span> optical depth was also similar to the AERONET observations across India. Differences in surface shortwave radiation between simulations that included and neglected <span class="hlt">aerosol</span>-radiation interactions were as high as -25 Wm{sup -2}, while differences in surface shortwave radiation between simulations that included and neglect <span class="hlt">aerosol</span>-radiation-cloud interactions were as high as -30 Wm{sup -2}. The spatial variations of these differences were also compared with AVHRR observation. This study suggests that the model is able to qualitatively simulate the impact of <span class="hlt">aerosols</span> on radiation over India; however, additional measurements of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E.916K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E.916K"><span>What We Can Say About the Roles of Natural and Anthropogenic <span class="hlt">Aerosols</span> in Climate Change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kahn, Ralph</p> <p>2016-07-01</p> <p>Although particles from natural sources dominate the globally averaged <span class="hlt">aerosol</span> load, it is widely understood that human activity has added significantly to the atmospheric <span class="hlt">aerosol</span> inventory in many regions. Anthropogenic contributions include pollution particles from industrial activity, transportation, cook-stoves, and other combustion sources, smoke from agricultural fires and those wildfires that result from land-management practices, soil and mineral dust mobilized in regions where overgrazing, severe tilling, or overuse of surface water resources have occurred, and biogenic particles from vegetation planted and maintained by the populance. The history of human influence is complex - in the 18th and 19th centuries agricultural burning tended to dominate the anthropogenic component in most places, whereas more recently, fossil fuel combustion leads the human contribution is many areas. However, identifying and quantifying the anthropogenic <span class="hlt">aerosol</span> component on global <span class="hlt">scales</span> is a challenging endeavor at present. Most estimates of the anthropogenic component come from <span class="hlt">aerosol</span> transport models that are initialized with <span class="hlt">aerosol</span> and precursor-gas source locations, emission strengths, and injection <span class="hlt">heights</span>. The <span class="hlt">aerosol</span> is then advected based on meteorological modeling, possibly modified chemically or physically, and removed by parameterized wet or dry deposition processes. <span class="hlt">Aerosol</span> effects on clouds are also represented in some climate models, but with even greater uncertainty than the direct <span class="hlt">aerosol</span> effects on Earth's radiation balance. Even for present conditions, <span class="hlt">aerosol</span> source inventories are deduced from whatever constraints can be found, along with much creativity and many assumptions. <span class="hlt">Aerosol</span> amount (i.e., <span class="hlt">aerosol</span> optical depth) is routinely measured globally from space, but observational constraints on the anthropogenic component require some knowledge of the <span class="hlt">aerosol</span> type as well, a much more difficult quantity to derive. As large-swath, multi-spectral, single</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JGRD..11124201C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JGRD..11124201C"><span>A one-dimensional sectional <span class="hlt">aerosol</span> model integrated with mesoscale meteorological data to study marine boundary layer <span class="hlt">aerosol</span> dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caffrey, Peter F.; Hoppel, William A.; Shi, Jainn J.</p> <p>2006-12-01</p> <p>The dynamics of <span class="hlt">aerosols</span> in the marine boundary layer are simulated with a one-dimensional, multicomponent, sectional <span class="hlt">aerosol</span> model using vertical profiles of turbulence, relative humidity, temperature, vertical velocity, cloud cover, and precipitation provided by 3-D mesoscale meteorological model output. The Naval Research Laboratory's (NRL) sectional <span class="hlt">aerosol</span> model MARBLES (Fitzgerald et al., 1998a) was adapted to use hourly meteorological input taken from NRL's Coupled Ocean-Atmosphere Prediction System (COAMPS). COAMPS-generated turbulent mixing coefficients and large-<span class="hlt">scale</span> vertical velocities determine vertical exchange within the marine boundary layer and exchange with the free troposphere. Air mass back trajectories were used to define the air column history along which the meteorology was retrieved for use with the <span class="hlt">aerosol</span> model. Details on the integration of these models are described here, as well as a description of improvements made to the <span class="hlt">aerosol</span> model, including transport by large-<span class="hlt">scale</span> vertical motions (such as subsidence and lifting), a revised sea-salt <span class="hlt">aerosol</span> source function, and separate tracking of sulfate mass from each of the five sources (free tropospheric, nucleated, condensed from gas phase oxidation products, cloud-processed, and produced from heterogeneous oxidation of S(IV) on sea-salt <span class="hlt">aerosol</span>). Results from modeling air masses arriving at Oahu, Hawaii, are presented, and the relative contribution of free-tropospheric sulfate particles versus sea-salt <span class="hlt">aerosol</span> from the surface to CCN concentrations is discussed. Limitations and benefits of the method are presented, as are sensitivity analyses of the effect of large-<span class="hlt">scale</span> vertical motions versus turbulent mixing.</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/2013EGUGA..1510267B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1510267B"><span>Intercomparison of <span class="hlt">aerosol</span> optical parameters from WALI and R-MAN510 <span class="hlt">aerosol</span> Raman lidars in the framework of HyMeX campaign</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boytard, Mai-Lan; Royer, Philippe; Chazette, Patrick; Shang, Xiaoxia; Marnas, Fabien; Totems, Julien; Bizard, Anthony; Bennai, Baya; Sauvage, Laurent</p> <p>2013-04-01</p> <p>The HyMeX program (Hydrological cycle in Mediterranean eXperiment) aims at improving our understanding of hydrological cycle in the Mediterranen and at a better quantification and forecast of high-impact weather events in numerical weather prediction models. The first Special Observation Period (SOP1) took place in September/October 2012. During this period two <span class="hlt">aerosol</span> Raman lidars have been deployed at Menorca Island (Spain) : one Water-vapor and <span class="hlt">Aerosol</span> Raman LIdar (WALI) operated by LSCE/CEA (Laboratoire des Sciences du Climat et de l'Environnement/Commissariat à l'Energie Atomique) and one <span class="hlt">aerosol</span> Raman and dual-polarization lidar (R-Man510) developed and commercialized by LEOSPHERE company. Both lidars have been continuously running during the campaign and have provided information on <span class="hlt">aerosol</span> and cloud optical properties under various atmospheric conditions (maritime background <span class="hlt">aerosols</span>, dust events, cirrus clouds...). We will present here the results of intercomparisons between R-Man510, and WALI <span class="hlt">aerosol</span> lidar systems and collocated sunphotometer measurements. Limitations and uncertainties on the retrieval of extinction coefficients, depolarization ratio, <span class="hlt">aerosol</span> optical depths and detection of atmospheric structures (planetary boundary layer <span class="hlt">height</span>, <span class="hlt">aerosol</span>/cloud layers) will be discussed according atmospheric conditions. The results will also be compared with theoretical uncertainty assessed with direct/inverse model of lidar profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.B33B1027W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.B33B1027W"><span>Direct Radiative Impacts of Central American Biomass Burning Smoke <span class="hlt">Aerosols</span>: Analysis from a Coupled <span class="hlt">Aerosol</span>-Radiation-Meteorology Model RAMS-AROMA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, J.; Christopher, S. A.; Nair, U. S.; Reid, J. S.; Prins, E. M.</p> <p>2005-12-01</p> <p>Considerable efforts including various field experiments have been carried out in the last decade for studying the regional climatic impact of smoke <span class="hlt">aerosols</span> produced by biomass burning activities in Africa and South America. In contrast, only few investigations have been conducted for Central American Biomass Burning (CABB) region. Using a coupled <span class="hlt">aerosol</span>-radiation-meteorology model called RAMS-AROMA together with various ground-based observations, we present a comprehensive analysis of the smoke direct radiative impacts on the surface energy budget, boundary layer evolution, and e precipitation process during the CABB events in Spring 2003. Quantitative estimates are also made regarding the transboundary carbon mass to the U.S. in the form of smoke particles. Buult upon the Regional Atmospheric Modeling System (RAMS) mesoscale model, the RAMS AROMA has several features including Assimilation and Radiation Online Modeling of <span class="hlt">Aerosols</span> (AROMA) algorithms. The model simulates smoke transport by using hourly smoke emission inventory from the Fire Locating and Modeling of Burning Emissions (FLAMBE) geostationary satellite database. It explicitly considers the smoke effects on the radiative transfer at each model time step and model grid, thereby coupling the dynamical processes and <span class="hlt">aerosol</span> transport. Comparison with ground-based observation show that the simulation realistically captured the smoke transport timeline and distribution from daily to hourly <span class="hlt">scales</span>. The effects of smoke radiative extinction on the decrease of 2m air temperature (2mT), diurnal temperature range (DTR), and boundary layer <span class="hlt">height</span> over the land surface are also quantified. Warming due to smoke absorption of solar radiation can be found in the lower troposphere over the ocean, but not near the underlying land surface. The increase of boundary layer stability produces a positive feedback where more smoke particles are trapped in the lower boundary layer. These changes in temperature, surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/993659-spatial-temporal-variations-aerosols-around-beijing-summer-local-column-aerosol-optical-properties','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/993659-spatial-temporal-variations-aerosols-around-beijing-summer-local-column-aerosol-optical-properties"><span>Spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing in summer 2006: 2. Local and column <span class="hlt">aerosol</span> optical properties</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>Matsui, Hitoshi; Koike, Makoto; Kondo, Yutaka</p> <p></p> <p>Weather Research and Forecasting (WRF)-chem model calculations were conducted to study <span class="hlt">aerosol</span> optical properties around Beijing, China, during the Campaign of Air Quality Research in Beijing and Surrounding Region 2006 (CAREBeijing-2006) period. In this paper, we interpret <span class="hlt">aerosol</span> optical properties in terms of <span class="hlt">aerosol</span> mass concentrations and their chemical compositions by linking model calculations with measurements. In general, model calculations reproduced observed features of spatial and temporal variations of various surface and column <span class="hlt">aerosol</span> optical parameters in and around Beijing. Spatial and temporal variations of <span class="hlt">aerosol</span> absorption, scattering, and extinction coefficient corresponded well to those of elemental carbon (primary <span class="hlt">aerosol</span>),more » sulfate (secondary <span class="hlt">aerosol</span>), and the total <span class="hlt">aerosol</span> mass concentration, respectively. These results show that spatial and temporal variations of the absorption coefficient are controlled by local emissions (within 100 km around Beijing during the preceding 24 h), while those of the scattering coefficient are controlled by regional-<span class="hlt">scale</span> emissions (within 500 km around Beijing during the preceding 3 days) under synoptic-<span class="hlt">scale</span> meteorological conditions, as discussed in our previous study of <span class="hlt">aerosol</span> mass concentration. Vertical profiles of <span class="hlt">aerosol</span> extinction revealed that the contribution of secondary <span class="hlt">aerosols</span> and their water uptake increased with altitude within the planetary boundary layer, leading to a considerable increase in column <span class="hlt">aerosol</span> optical depth (AOD) around Beijing. These effects are the main factors causing differences in regional and temporal variations between particulate matter (PM) mass concentration at the surface and column AOD over a wide region in the northern part of the Great North China Plain.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA111255','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA111255"><span>Maritime Infrared Propagation: Particle Size Distribution Measurements Using a Helicopter-Borne <span class="hlt">Aerosol</span> Counter.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1981-09-01</p> <p>COUNTER by R. R. Allan S. Craig SUMMARY -Particle size distribution measurements were made on nine successive days in late August 1980 using a PMS FSSP-100...<span class="hlt">aerosol</span> counter flown on a Wessex Mk 5 helicopter. In all, 14 flights were made giving data at two <span class="hlt">heights</span>, 30 and 100 ft above the sea surface...<span class="hlt">aerosol</span> content over deep water. It was a specific recommendation of TTCP-JAG9 that airborne <span class="hlt">aerosol</span> measurements should be made in conjunction with al</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10697E..38S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10697E..38S"><span>Measurement of phase function of <span class="hlt">aerosol</span> at different altitudes by CCD Lidar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Peiyu; Yuan, Ke'e.; Yang, Jie; Hu, Shunxing</p> <p>2018-02-01</p> <p>The <span class="hlt">aerosols</span> near the ground are closely related to human health and climate change, the study on which has important significance. As we all know, the <span class="hlt">aerosol</span> is inhomogeneous at different altitudes, of which the phase function is also different. In order to simplify the retrieval algorithm, it is usually assumed that the <span class="hlt">aerosol</span> is uniform at different altitudes, which will bring measurement error. In this work, an experimental approach is demonstrated to measure the scattering phase function of atmospheric <span class="hlt">aerosol</span> particles at different <span class="hlt">heights</span> by CCD lidar system, which could solve the problem of the traditional CCD lidar system in assumption of phase function. The phase functions obtained by the new experimental approach are used to retrieve the <span class="hlt">aerosol</span> extinction coefficient profiles. By comparison of the <span class="hlt">aerosol</span> extinction coefficient retrieved by Mie-scattering <span class="hlt">aerosol</span> lidar and CCD lidar at night, the reliability of new experimental approach is verified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010060336&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTOM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010060336&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTOM"><span>A Long-term Record of Saharan Dust <span class="hlt">Aerosol</span> Properties from TOMS Observations: Optical Depth and Single Scattering Albedo</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Torres, Omar; Bhartia, P. K.; Herman, J. R.; Einaudi, Franco (Technical Monitor)</p> <p>2000-01-01</p> <p>The interaction between the strong Rayleigh scattering in the near UV spectral region (330-380 nm) and the processes of <span class="hlt">aerosol</span> absorption and scattering, produce a clear spectral signal in the upwelling radiance at the top of the atmosphere. This interaction is the basis of the TOMS (Total Ozone Mapping Spectrometer) <span class="hlt">aerosol</span> retrieval technique that can be used for their characterization and to differentiate non-absorbing sulfates from strongly UV-absorbing <span class="hlt">aerosols</span> such as mineral dust. For absorbing <span class="hlt">aerosols</span>, the characterization is in terms of the optical depth and single scattering albedo with assumptions about the <span class="hlt">aerosol</span> plume <span class="hlt">height</span>. The results for non-absorbing <span class="hlt">aerosols</span> are not dependent on plume <span class="hlt">height</span>. Although iron compounds represent only between 5% to 8% of desert dust <span class="hlt">aerosol</span> mass, hematite (Fe2O3) accounts for most of the near UV absorption. Because of the large ultraviolet absorption characteristic of hematite, the near UV method of <span class="hlt">aerosol</span> sensing is especially suited for the detection and characterization of desert dust <span class="hlt">aerosols</span>. Using the combined record of near UV measurements by the Nimbus7 (1978-1992) and Earth Probe (1996-present) TOMS instruments, a global longterm climatology of near UV optical depth and single scattering albedo has been produced. The multi-year long record of mineral <span class="hlt">aerosol</span> properties over the area of influence of the Saharan desert, will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/4068195','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/4068195"><span>Accuracy of recumbent <span class="hlt">height</span> measurement.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gray, D S; Crider, J B; Kelley, C; Dickinson, L C</p> <p>1985-01-01</p> <p>Since many patients requiring specialized nutritional support are bedridden, measurement of <span class="hlt">height</span> for purposes of nutritional assessment or prescription must often be done with the patient in bed. This study examined the accuracy of measuring body <span class="hlt">height</span> in bed in the supine position. Two measurements were performed on 108 ambulatory inpatients: (1) standing <span class="hlt">height</span> using a standard <span class="hlt">height</span>-weight <span class="hlt">scale</span>, and (2) bed <span class="hlt">height</span> using a flexible tape. Patients were divided into four groups based on which of two researchers performed each of the two measurements. Each patient was also weighed and self-reported <span class="hlt">height</span>, weight, sex, and age were recorded. Bed <span class="hlt">height</span> was significantly longer than standing <span class="hlt">height</span> by 3.68 cm, but the two measurements were equally precise. It was believed, however, that this 2% difference was probably not clinically significant in most circumstances. Bed <span class="hlt">height</span> correlated highly with standing <span class="hlt">height</span> (r = 0.95), and the regression equation was standing <span class="hlt">height</span> = 13.82 +/- 0.09 bed <span class="hlt">height</span>. Patients overestimated their <span class="hlt">heights</span>. <span class="hlt">Heights</span> recorded by nurses were more accurate when patients were measured than when asked about their <span class="hlt">heights</span>, but the patients were more often asked than measured.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACPD...1024135P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACPD...1024135P"><span>Modelled and measured effects of clouds on UV <span class="hlt">Aerosol</span> Indices on a local, regional, and global <span class="hlt">scale</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Penning de Vries, M.; Wagner, T.</p> <p>2010-10-01</p> <p>The UV <span class="hlt">Aerosol</span> Indices (UVAI) form one of very few available tools in satellite remote sensing that provide information on <span class="hlt">aerosol</span> absorption. The UVAI are also quite insensitive to surface type and are determined in the presence of clouds - situations where most <span class="hlt">aerosol</span> retrieval algorithms do not work. The UVAI are most sensitive to elevated layers of absorbing <span class="hlt">aerosols</span>, such as mineral dust and smoke from biomass burning, but they can also be used to study non-absorbing <span class="hlt">aerosols</span>, such as sulphate and secondary organic <span class="hlt">aerosols</span>. Although UVAI are determined for cloud-contaminated pixels, clouds do affect the value of UVAI in several ways. One way to correct for these effects is to remove clouded pixels using a cloud filter. However, this causes a large loss of data, biases the results towards clear skies, and removes all potentially very interesting pixels where <span class="hlt">aerosols</span> and clouds co-exist. We here propose to correct the effects of clouds on UVAI in a more sophisticated way, namely by simulating the contribution of clouds to UVAI, and then subtracting it from the measured data. To this aim, we modelled UVAI from clouds by using measured cloud optical parameters - either with low spatial resolution from SCIAMACHY, or high resolution from MERIS - as input. The modelled UVAI were compared with UVAI measured by SCIAMACHY on different spatial (local, regional and global) and temporal <span class="hlt">scales</span> (single measurement, daily means and seasonal means). The general dependencies of UVAI on cloud parameters were quite well reproduced, but several issues remain unclear: compared to the modelled UVAI, measured UVAI show a bias, in particular for large cloud fractions, and much larger scatter. Also, the viewing angle dependence differs for measured and modelled UVAI. The modelled UVAI from clouds will be used to correct measured UVAI for the effect of clouds, thus allowing a more quantitative analysis of UVAI and enabling investigations of <span class="hlt">aerosol</span>-cloud interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Icar..307..294M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Icar..307..294M"><span>Retrieval of water vapor column abundance and <span class="hlt">aerosol</span> properties from ChemCam passive sky spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McConnochie, Timothy H.; Smith, Michael D.; Wolff, Michael J.; Bender, Steve; Lemmon, Mark; Wiens, Roger C.; Maurice, Sylvestre; Gasnault, Olivier; Lasue, Jeremie; Meslin, Pierre-Yves; Harri, Ari-Matti; Genzer, Maria; Kemppinen, Osku; Martínez, Germán M.; DeFlores, Lauren; Blaney, Diana; Johnson, Jeffrey R.; Bell, James F.</p> <p>2018-06-01</p> <p>We derive water vapor column abundances and <span class="hlt">aerosol</span> properties from Mars Science Laboratory (MSL) ChemCam passive mode observations of scattered sky light. This paper covers the methodology and initial results for water vapor and also provides preliminary results for <span class="hlt">aerosols</span>. The data set presented here includes the results of 113 observations spanning from Mars Year 31 Ls = 291° (March 30, 2013) to Mars Year 33 Ls= 127° (March 24, 2016). Each ChemCam passive sky observation acquires spectra at two different elevation angles. We fit these spectra with a discrete-ordinates multiple scattering radiative transfer model, using the correlated-k approximation for gas absorption bands. The retrieval proceeds by first fitting the continuum of the ratio of the two elevation angles to solve for <span class="hlt">aerosol</span> properties, and then fitting the continuum-removed ratio to solve for gas abundances. The final step of the retrieval makes use of the observed CO2 absorptions and the known CO2 abundance to correct the retrieved water vapor abundance for the effects of the vertical distribution of scattering <span class="hlt">aerosols</span> and to derive an <span class="hlt">aerosol</span> <span class="hlt">scale</span> <span class="hlt">height</span> parameter. Our water vapor results give water vapor column abundance with a precision of ±0.6 precipitable microns and systematic errors no larger than ±0.3 precipitable microns, assuming uniform vertical mixing. The ChemCam-retrieved water abundances show, with only a few exceptions, the same seasonal behavior and the same timing of seasonal minima and maxima as the TES, CRISM, and REMS-H data sets that we compare them to. However ChemCam-retrieved water abundances are generally lower than zonal and regional <span class="hlt">scale</span> from-orbit water vapor data, while at the same time being significantly larger than pre-dawn REMS-H abundances. Pending further analysis of REMS-H volume mixing ratio uncertainties, the differences between ChemCam and REMS-H pre-dawn mixing ratios appear to be much too large to be explained by large <span class="hlt">scale</span> circulations and thus</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ACP....1112715P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ACP....1112715P"><span>Modelled and measured effects of clouds on UV <span class="hlt">Aerosol</span> Indices on a local, regional, and global <span class="hlt">scale</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Penning de Vries, M.; Wagner, T.</p> <p>2011-12-01</p> <p>The UV <span class="hlt">Aerosol</span> Indices (UVAI) form one of very few available tools in satellite remote sensing that provide information on <span class="hlt">aerosol</span> absorption. The UVAI are also quite insensitive to surface type and are determined in the presence of clouds - situations where most <span class="hlt">aerosol</span> retrieval algorithms do not work. The UVAI are most sensitive to elevated layers of absorbing <span class="hlt">aerosols</span>, such as mineral dust and smoke, but they can also be used to study non-absorbing <span class="hlt">aerosols</span>, such as sulphate and secondary organic <span class="hlt">aerosols</span>. Although UVAI are determined for cloud-contaminated pixels, clouds do affect the value of UVAI in several ways: (1) they shield the underlying scene (potentially containing <span class="hlt">aerosols</span>) from view, (2) they enhance the apparent surface albedo of an elevated <span class="hlt">aerosol</span> layer, and (3) clouds unpolluted by <span class="hlt">aerosols</span> also yield non-zero UVAI, here referred to as "cloudUVAI". The main purpose of this paper is to demonstrate that clouds can cause significant UVAI and that this cloudUVAI can be well modelled using simple assumptions on cloud properties. To this aim, we modelled cloudUVAI by using measured cloud optical parameters - either with low spatial resolution from SCIAMACHY, or high resolution from MERIS - as input. The modelled cloudUVAI were compared with UVAI determined from SCIAMACHY reflectances on different spatial (local, regional and global) and temporal <span class="hlt">scales</span> (single measurement, daily means and seasonal means). The general dependencies of UVAI on cloud parameters were quite well reproduced, but several issues remain unclear: compared to the modelled cloudUVAI, measured UVAI show a bias, in particular for large cloud fractions. Also, the spread in measured UVAI is larger than in modelled cloudUVAI. In addition to the original, Lambert Equivalent Reflector (LER)-based UVAI algorithm, we have also investigated the effects of clouds on UVAI determined using the so-called Modified LER (MLER) algorithm (currently applied to TOMS and OMI data). For medium</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1712528S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1712528S"><span>Satellite remote sensing of <span class="hlt">aerosol</span> and cloud properties over Eurasia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sogacheva, Larisa; Kolmonen, Pekka; Saponaro, Giulia; Virtanen, Timo; Rodriguez, Edith; Sundström, Anu-Maija; Atlaskina, Ksenia; de Leeuw, Gerrit</p> <p>2015-04-01</p> <p>Satellite remote sensing provides the spatial distribution of <span class="hlt">aerosol</span> and cloud properties over a wide area. In our studies large data sets are used for statistical studies on <span class="hlt">aerosol</span> and cloud interaction in an area over Fennoscandia, the Baltic Sea and adjacent regions over the European mainland. This area spans several regimes with different influences on <span class="hlt">aerosol</span> cloud interaction such as a the transition from relative clean air over Fennoscandia to more anthropogenically polluted air further south, and the influence maritime air over the Baltic and oceanic air advected from the North Atlantic. Anthropogenic pollution occurs in several parts of the study area, and in particular near densely populated areas and megacities, but also in industrialized areas and areas with dense traffic. The <span class="hlt">aerosol</span> in such areas is quite different from that produced over the boreal forest and has different effects on air quality and climate. Studies have been made on the effects of <span class="hlt">aerosols</span> on air quality and on the radiation balance in China. The aim of the study is to study the effect of these different regimes on <span class="hlt">aerosol</span>-cloud interaction using a large <span class="hlt">aerosol</span> and cloud data set retrieved with the (Advanced) Along Track Scanning Radiometer (A)ATSR Dual View algorithm (ADV) further developed at Finnish Meteorological Institute and <span class="hlt">aerosol</span> and cloud data provided by MODIS. Retrieval algorithms for <span class="hlt">aerosol</span> and clouds have been developed for the (A)ATSR, consisting of a series of instruments of which we use the second and third one: ATSR-2 which flew on the ERS-2 satellite (1995-2003) and AATSR which flew on the ENVISAT satellite (2002-2012) (both from the European Space Agency, ESA). The ADV algorithm provides <span class="hlt">aerosol</span> data on a global <span class="hlt">scale</span> with a default resolution of 10x10km2 (L2) and an aggregate product on 1x1 degree (L3). Optional, a 1x1 km2 retrieval products is available over smaller areas for specific studies. Since for the retrieval of AOD no prior knowledge is needed on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9680E..2TK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9680E..2TK"><span>Spatial variability of <span class="hlt">aerosol</span> and black carbon concentrations in the troposphere of the Russian Arctic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kozlov, Valerii S.; Panchenko, Mikhail V.; Paris, Jean D.; Nédéléc, Philippe; Chernov, Dmitry G.; Shmargunov, Vladimir P.</p> <p>2015-11-01</p> <p>A cycle of flights of the Optik TU-134 Flying Laboratory of IAO SB RAS over regions of Western Siberia and the Russian Arctic (55.0-74.8°N, 61.3-82.9°E) was carried out on October 15-17 of 2014 within the framework of the YAK-AEROSIB Russian—French Project. The mass concentrations of submicron <span class="hlt">aerosol</span> and Black Carbon (BC) in the troposphere up to a <span class="hlt">height</span> of 8.5 km were measured in the flights. The ranges of variability were 0.3-20 μg/m3 for the <span class="hlt">aerosol</span> concentration and 0.02-1 μg/m3 for the BC concentration. In the subpolar latitudes of 71-74.8°N, the lower levels of <span class="hlt">aerosol</span> (0.8-6 μg/m3) and BC (0.02-0.3 μg/m3) were observed. The comparison of the results of airborne sensing in 2008 and 2014 has shown that in the Western Subartic the <span class="hlt">aerosol</span> and BC concentrations in the vertical profiles up to six times exceeded those observed in the Eastern Subarctic (0.3-1 μg/m3 and 10-50 ng/m3). The excess of the mean integral BC concentrations and the <span class="hlt">aerosol</span> optical depth was, on average, 2-2.5 times (0.16 mg/m2; 0.02). In the region of the Kara Sea at <span class="hlt">heights</span> of 0.5-2 and 4-6 km, the excess of the <span class="hlt">aerosol</span> content in the western sector in comparison with the eastern one was, on average, 2 times, while for the black carbon the excess achieved 7 times at <span class="hlt">heights</span> of 1-2 km (0.25- 0.035 μg/m3). The mean integral concentrations of <span class="hlt">aerosol</span> and black carbon ˜ 1.3 times exceeded those in the clearer eastern region of the sea (0.31 mg/m2; 0.049). The obtained estimates indicate the decrease of the <span class="hlt">aerosol</span> and BC concentrations in the subpolar latitudes of the Russian Federation from the west to the east.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JGRD..11522207M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JGRD..11522207M"><span>Spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing in summer 2006: 2. Local and column <span class="hlt">aerosol</span> optical properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsui, H.; Koike, M.; Kondo, Y.; Takegawa, N.; Fast, J. D.; PöSchl, U.; Garland, R. M.; Andreae, M. O.; Wiedensohler, A.; Sugimoto, N.; Zhu, T.</p> <p>2010-11-01</p> <p>Model calculations were conducted using the Weather Research and Forecasting model coupled with chemistry (WRF-chem) for the region around Beijing, China, in the summer of 2006, when the CAREBeijing-2006 intensive campaign was conducted. In this paper, we interpret <span class="hlt">aerosol</span> optical properties in terms of <span class="hlt">aerosol</span> mass concentrations and their chemical compositions by linking model calculations with measurements. The model calculations generally captured the observed variability of various surface and column <span class="hlt">aerosol</span> optical parameters in and around Beijing. At the surface, the spatial and temporal variations of <span class="hlt">aerosol</span> absorption and scattering coefficients corresponded well to those of elemental carbon and sulfate mass concentrations, respectively, and were controlled by local-<span class="hlt">scale</span> (<100 km and <24 hours) and regional-<span class="hlt">scale</span> (<500 km and <3 days) emissions, respectively. The contribution of secondary <span class="hlt">aerosols</span> and their water uptake increased with altitude within the planetary boundary layer. This variation led to a considerable increase in column <span class="hlt">aerosol</span> optical depth and was responsible for the differences in regional and temporal variations between surface and column <span class="hlt">aerosol</span> optical properties around Beijing. These processes are expected to be common in other megacity regions as well. Model calculations, however, underestimated or overestimated the absolute levels of <span class="hlt">aerosol</span> optical properties in and around Beijing by up to 60%. Sensitivity studies showed that these discrepancies were mostly due to the uncertainties in <span class="hlt">aerosol</span> mixing state and <span class="hlt">aerosol</span> density (affecting mass extinction efficiency) in the model calculations. Good agreement with measurements is achieved when these <span class="hlt">aerosol</span> properties are accurately predicted or assumed; however, significant bias can result when these properties are inadequately treated, even if total <span class="hlt">aerosol</span> mass concentrations are reproduced well in the model calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA533019','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA533019"><span>Large-<span class="hlt">Scale</span> <span class="hlt">Aerosol</span> Modeling and Analysis</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-09-30</p> <p>novel method of simultaneous real- time measurements of ice-nucleating particle concentrations and size- resolved chemical composition of individual...is to develop a practical predictive capability for visibility and weather effects of <span class="hlt">aerosol</span> particles for the entire globe for timely use in...prediction follows that used in numerical weather prediction, namely real- time assessment for initialization of first-principles models. The Naval</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1615786M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1615786M"><span>MAESTRO Measurements of Atmospheric <span class="hlt">Aerosol</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McElroy, Tom; Drummond, James; Zou, Jason</p> <p>2014-05-01</p> <p>MAESTRO (Measurements of <span class="hlt">Aerosol</span> Extinction in the Stratosphere and Troposphere Retrieved by Occultation) is now in its 11th year on orbit as part of the Atmospheric Chemistry Experiment on the Canadian Space Agency's SCISAT satellite. MAESTRO data analysis has been dogged by a deficiency in accurate timing between the measurements made by the partner instrument, the ACE-FTS (Atmospheric Chemistry Experiment, Fourier Transform Spectrometer), that provides the atmospheric pressure-temperature profile and observation tangent altitudes used in the MAESTRO data analysis. Attempts have been made to use apparent air column density and oxygen A-band absorption as a mechanism to line up the tangent <span class="hlt">heights</span>, but to no avail. A new product is now being produced, based on matching the modeled ozone slant columns from the ACE-FTS retrievals with the MAESTRO slant column measurements. The approach is very promising and indicates that a valuable product from the MAESTRO wavelength-dependent <span class="hlt">aerosol</span> extinction likely result. The usefulness of the profile matching technique will be demonstrated and some <span class="hlt">aerosol</span> absorption profiles will be presented in comparison with measurements made by the ACE Imager <span class="hlt">aerosol</span> profile results. While the process optimizes the comparison between ACE-FTS ozone profile data and that from MAESTRO, it does not detract from the higher vertical resolution information provided by MAESTRO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRD..123.3175X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRD..123.3175X"><span>Coupled Retrieval of Liquid Water Cloud and Above-Cloud <span class="hlt">Aerosol</span> Properties Using the Airborne Multiangle SpectroPolarimetric Imager (AirMSPI)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Feng; van Harten, Gerard; Diner, David J.; Davis, Anthony B.; Seidel, Felix C.; Rheingans, Brian; Tosca, Mika; Alexandrov, Mikhail D.; Cairns, Brian; Ferrare, Richard A.; Burton, Sharon P.; Fenn, Marta A.; Hostetler, Chris A.; Wood, Robert; Redemann, Jens</p> <p>2018-03-01</p> <p>An optimization algorithm is developed to retrieve liquid water cloud properties including cloud optical depth (COD), droplet size distribution and cloud top <span class="hlt">height</span> (CTH), and above-cloud <span class="hlt">aerosol</span> properties including <span class="hlt">aerosol</span> optical depth (AOD), single-scattering albedo, and microphysical properties from sweep-mode observations by Jet Propulsion Laboratory's Airborne Multiangle SpectroPolarimetric Imager (AirMSPI) instrument. The retrieval is composed of three major steps: (1) initial estimate of the mean droplet size distribution across the entire image of 80-100 km along track by 10-25 km across track from polarimetric cloudbow observations, (2) coupled retrieval of image-<span class="hlt">scale</span> cloud and above-cloud <span class="hlt">aerosol</span> properties by fitting the polarimetric data at all observation angles, and (3) iterative retrieval of 1-D radiative transfer-based COD and droplet size distribution at pixel <span class="hlt">scale</span> (25 m) by establishing relationships between COD and droplet size and fitting the total radiance measurements. Our retrieval is tested using 134 AirMSPI data sets acquired during the National Aeronautics and Space Administration (NASA) field campaign ObseRvations of <span class="hlt">Aerosols</span> above CLouds and their intEractionS. The retrieved above-cloud AOD and CTH are compared to coincident HSRL-2 (HSRL-2, NASA Langley Research Center) data, and COD and droplet size distribution parameters (effective radius reff and effective variance veff) are compared to coincident Research Scanning Polarimeter (RSP) (NASA Goddard Institute for Space Studies) data. Mean absolute differences between AirMSPI and HSRL-2 retrievals of above-cloud AOD at 532 nm and CTH are 0.03 and <0.5 km, respectively. At RSP's footprint <span class="hlt">scale</span> ( 323 m), mean absolute differences between RSP and AirMSPI retrievals of COD, reff, and veff in the cloudbow area are 2.33, 0.69 μm, and 0.020, respectively. Neglect of smoke <span class="hlt">aerosols</span> above cloud leads to an underestimate of image-averaged COD by 15%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050156613&hterms=Asian&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DAsian','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050156613&hterms=Asian&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DAsian"><span>Anomalies of the Asian Monsoon Induced by <span class="hlt">Aerosol</span> Forcings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lau, William K. M.; Kim, M. K.</p> <p>2004-01-01</p> <p>Impacts of <span class="hlt">aerosols</span> on the Asian summer monsoon are studied using the NASA finite volume General Circulation Model (fvGCM), with radiative forcing derived from three-dimensional distributions of five <span class="hlt">aerosol</span> species i.e., black carbon, organic carbon, soil dust, and sea salt from the Goddard Chemistry <span class="hlt">Aerosol</span> Radiation and Transport Model (GOCART). Results show that absorbing <span class="hlt">aerosols</span>, i.e., black carbon and dust, induce large-<span class="hlt">scale</span> upper-level heating anomaly over the Tibetan Plateau in April and May, ushering in & early onset of the Indian summer monsoon. Absorbing <span class="hlt">aerosols</span> also I i enhance lower-level heating and anomalous ascent over northern India, intensifying the Indian monsoon. Overall, the <span class="hlt">aerosol</span>-induced large-<span class="hlt">scale</span> surface' temperature cooling leads to a reduction of monsoon rainfall over the East Asia continent, and adjacent oceanic regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JCHyd.190...15H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JCHyd.190...15H"><span>Evaluation of liquid <span class="hlt">aerosol</span> transport through porous media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hall, R.; Murdoch, L.; Falta, R.; Looney, B.; Riha, B.</p> <p>2016-07-01</p> <p>Application of remediation methods in contaminated vadose zones has been hindered by an inability to effectively distribute liquid- or solid-phase amendments. Injection as <span class="hlt">aerosols</span> in a carrier gas could be a viable method for achieving useful distributions of amendments in unsaturated materials. The objectives of this work were to characterize radial transport of <span class="hlt">aerosols</span> in unsaturated porous media, and to develop capabilities for predicting results of <span class="hlt">aerosol</span> injection scenarios at the field-<span class="hlt">scale</span>. Transport processes were investigated by conducting lab-<span class="hlt">scale</span> injection experiments with radial flow geometry, and predictive capabilities were obtained by developing and validating a numerical model for simulating coupled <span class="hlt">aerosol</span> transport, deposition, and multi-phase flow in porous media. Soybean oil was transported more than 2 m through sand by injecting it as micron-<span class="hlt">scale</span> <span class="hlt">aerosol</span> droplets. Oil saturation in the sand increased with time to a maximum of 0.25, and decreased with radial distance in the experiments. The numerical analysis predicted the distribution of oil saturation with only minor calibration. The results indicated that evolution of oil saturation was controlled by <span class="hlt">aerosol</span> deposition and subsequent flow of the liquid oil, and simulation requires including these two coupled processes. The calibrated model was used to evaluate field applications. The results suggest that amendments can be delivered to the vadose zone as <span class="hlt">aerosols</span>, and that gas injection rate and <span class="hlt">aerosol</span> particle size will be important controls on the process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A43N..06N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A43N..06N"><span>Reconciling the <span class="hlt">aerosol</span>-liquid water path relationship in the ECHAM6-HAM GCM and the <span class="hlt">Aerosol</span>_cci/Cloud_cci (A)ATSR dataset by minimizing the effect of <span class="hlt">aerosol</span> swelling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neubauer, D.; Christensen, M.; Lohmann, U.; Poulsen, C. A.</p> <p>2016-12-01</p> <p>Studies using present day variability to assess statistical relationships between <span class="hlt">aerosol</span> and cloud properties find different strengths of these relationships between satellite data and general circulation model (GCM) data. This discrepancy can be explained by structural uncertainties due to differences in the analysis/observational <span class="hlt">scale</span> and the process <span class="hlt">scale</span> or spurious relationships between <span class="hlt">aerosol</span> and cloud properties. Such spurious relationships are the growth of <span class="hlt">aerosol</span> particles in the humid environment surrounding clouds, misclassification of partly cloudy satellite pixels as cloud free pixels, brightening of <span class="hlt">aerosol</span> particles by sunlight reflected at cloud edges, or effects of clouds on <span class="hlt">aerosol</span> like processing of <span class="hlt">aerosol</span> particles in clouds by nucleation or impact scavenging and subsequent growth by heterogeneous chemistry and release by cloud droplet evaporation or wet scavenging of <span class="hlt">aerosol</span> particles. To minimize the effects of spatial aggregation and spurious relationships we apply a new nearest neighbour approach to high resolution (A)ATSR datasets from the <span class="hlt">Aerosol</span>_cci and Cloud_cci projects of the Climate Change Initiative (CCI) programme of ESA. For the ECHAM6-HAM GCM we quantify the impact of using dry <span class="hlt">aerosol</span> (without <span class="hlt">aerosol</span> water) in the analysis to mimic the effect of the nearest neighbour approach. The <span class="hlt">aerosol</span>-liquid water path relationship in ECHAM6-HAM is systematically stronger than in (A)ATSR data and cannot be explained by an overestimation of autoconversion when using diagnostic precipitation but rather by <span class="hlt">aerosol</span> swelling in regions where humidity is high and clouds are present. When <span class="hlt">aerosol</span> water is removed from the analysis in ECHAM6-HAM the strength of the <span class="hlt">aerosol</span>-liquid water path relationship agrees much better with the ones of (A)ATSR or MODIS. We further find that while the observed relationships of different satellite sensors ((A)ATSR vs. MODIS) are not always consistent for tested environmental conditions the relationships in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JGeod..85....1S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JGeod..85....1S"><span><span class="hlt">Height</span> bias and <span class="hlt">scale</span> effect induced by antenna gravitational deformations in geodetic VLBI data analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarti, Pierguido; Abbondanza, Claudio; Petrov, Leonid; Negusini, Monia</p> <p>2011-01-01</p> <p>The impact of signal path variations (SPVs) caused by antenna gravitational deformations on geodetic very long baseline interferometry (VLBI) results is evaluated for the first time. Elevation-dependent models of SPV for Medicina and Noto (Italy) telescopes were derived from a combination of terrestrial surveying methods to account for gravitational deformations. After applying these models in geodetic VLBI data analysis, estimates of the antenna reference point positions are shifted upward by 8.9 and 6.7 mm, respectively. The impact on other parameters is negligible. To simulate the impact of antenna gravitational deformations on the entire VLBI network, lacking measurements for other telescopes, we rescaled the SPV models of Medicina and Noto for other antennas according to their size. The effects of the simulations are changes in VLBI <span class="hlt">heights</span> in the range [-3, 73] mm and a net <span class="hlt">scale</span> increase of 0.3-0.8 ppb. The <span class="hlt">height</span> bias is larger than random errors of VLBI position estimates, implying the possibility of significant <span class="hlt">scale</span> distortions related to antenna gravitational deformations. This demonstrates the need to precisely measure gravitational deformations of other VLBI telescopes, to derive their precise SPV models and to apply them in routine geodetic data 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_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.osti.gov/biblio/1134522-comparison-mixed-layer-heights-from-airborne-high-spectral-resolution-lidar-ground-based-measurements-wrp-chem-model-during-calnex-cares','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1134522-comparison-mixed-layer-heights-from-airborne-high-spectral-resolution-lidar-ground-based-measurements-wrp-chem-model-during-calnex-cares"><span>Comparison of Mixed Layer <span class="hlt">Heights</span> from Airborne High Spectral Resolution Lidar, Ground-based Measurements, and the WRP-Chem Model during CalNex and CARES</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>Scarino, Amy Jo; Obland, Michael; Fast, Jerome D.</p> <p>2014-06-05</p> <p>The California Research at the Nexus of Air Quality and Climate Change (CalNex) and Carbonaceous <span class="hlt">Aerosol</span> and Radiative Effects Study (CARES) field campaigns during May and June 2010 provided a data set appropriate for studying characteristics of the planetary boundary layer (PBL). The NASA Langley Research Center (LaRC) airborne High Spectral Resolution Lidar (HSRL) was deployed to California onboard the NASA LaRC B-200 aircraft to aid incharacterizing <span class="hlt">aerosol</span> properties during these two field campaigns. Measurements of <span class="hlt">aerosol</span> extinction (532 nm), backscatter (532 and 1064 nm), and depolarization (532 and 1064 nm) profiles during 31 flights, many in coordination with othermore » research aircraft and ground sites, constitute a diverse data set for use in characterizing the spatial and temporal distribution of <span class="hlt">aerosols</span>, as well as the depth and variability of the daytime mixed layer (ML), which is a subset within the PBL. This work illustrates the temporal and spatial variability of the ML in the vicinity of Los Angeles and Sacramento, CA. ML <span class="hlt">heights</span> derived from HSRL measurements are compared to PBL <span class="hlt">heights</span> derived from radiosonde profiles, ML <span class="hlt">heights</span> measured from ceilometers, and simulated PBL <span class="hlt">heights</span> from the Weather Research and Forecasting Chemistry (WRF-Chem) community model. Comparisons between the HSRL ML <span class="hlt">heights</span> and the radiosonde profiles in Sacramento result in a correlation coefficient value (R) of 0.93 (root7 mean-square (RMS) difference of 157 m and bias difference (HSRL radiosonde) of 5 m). HSRL ML <span class="hlt">heights</span> compare well with those from the ceilometer in the LA Basin with an R of 0.89 (RMS difference of 108 m and bias difference (HSRL Ceilometer) of -9.7 m) for distances of up to 30 km between the B-200 flight track and the ceilometer site. Simulated PBL <span class="hlt">heights</span> from WRF-Chem were compared with those obtained from all flights for each campaign, producing an R of 0.58 (RMS difference of 604 m and a bias difference (WRF-Chem HSRL) of -157 m) for Cal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACPD...1313721S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACPD...1313721S"><span>Comparison of mixed layer <span class="hlt">heights</span> from airborne high spectral resolution lidar, ground-based measurements, and the WRF-Chem model during CalNex and CARES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scarino, A. J.; Obland, M. D.; Fast, J. D.; Burton, S. P.; Ferrare, R. A.; Hostetler, C. A.; Berg, L. K.; Lefer, B.; Haman, C.; Hair, J. W.; Rogers, R. R.; Butler, C.; Cook, A. L.; Harper, D. B.</p> <p>2013-05-01</p> <p>The California Research at the Nexus of Air Quality and Climate Change (CalNex) and Carbonaceous <span class="hlt">Aerosol</span> and Radiative Effects Study (CARES) field campaigns during May and June 2010 provided a data set appropriate for studying characteristics of the planetary boundary layer (PBL). The NASA Langley Research Center (LaRC) airborne High Spectral Resolution Lidar (HSRL) was deployed to California onboard the NASA LaRC B-200 aircraft to aid in characterizing <span class="hlt">aerosol</span> properties during these two field campaigns. Measurements of <span class="hlt">aerosol</span> extinction (532 nm), backscatter (532 and 1064 nm), and depolarization (532 and 1064 nm) profiles during 31 flights, many in coordination with other research aircraft and ground sites, constitute a diverse data set for use in characterizing the spatial and temporal distribution of <span class="hlt">aerosols</span>, as well as the depth and variability of the daytime mixed layer (ML), which is a subset within the PBL. This work illustrates the temporal and spatial variability of the ML in the vicinity of Los Angeles and Sacramento, CA. ML <span class="hlt">heights</span> derived from HSRL measurements are compared to PBL <span class="hlt">heights</span> derived from radiosonde profiles, ML <span class="hlt">heights</span> measured from ceilometers, and simulated PBL <span class="hlt">heights</span> from the Weather Research and Forecasting Chemistry (WRF-Chem) community model. Comparisons between the HSRL ML <span class="hlt">heights</span> and the radiosonde profiles in Sacramento result in a correlation coefficient value (R) of 0.93 (root-mean-square (RMS) difference of 157 m and bias difference (HSRL - radiosonde) of 57 m). HSRL ML <span class="hlt">heights</span> compare well with those from the ceilometer in the LA Basin with an R of 0.89 (RMS difference of 108 m and bias difference (HSRL - Ceilometer) of -9.7 m) for distances of up to 30 km between the B-200 flight track and the ceilometer site. Simulated PBL <span class="hlt">heights</span> from WRF-Chem were compared with those obtained from all flights for each campaign, producing an R of 0.58 (RMS difference of 604 m and a bias difference (WRF-Chem - HSRL) of -157 m) for Cal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PNAS..110E4581F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PNAS..110E4581F"><span>Microphysical effects determine macrophysical response for <span class="hlt">aerosol</span> impacts on deep convective clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fan, Jiwen; Leung, L. Ruby; Rosenfeld, Daniel; Chen, Qian; Li, Zhanqing; Zhang, Jinqiang; Yan, Hongru</p> <p>2013-11-01</p> <p>Deep convective clouds (DCCs) play a crucial role in the general circulation, energy, and hydrological cycle of our climate system. <span class="hlt">Aerosol</span> particles can influence DCCs by altering cloud properties, precipitation regimes, and radiation balance. Previous studies reported both invigoration and suppression of DCCs by <span class="hlt">aerosols</span>, but few were concerned with the whole life cycle of DCC. By conducting multiple monthlong cloud-resolving simulations with spectral-bin cloud microphysics that capture the observed macrophysical and microphysical properties of summer convective clouds and precipitation in the tropics and midlatitudes, this study provides a comprehensive view of how <span class="hlt">aerosols</span> affect cloud cover, cloud top <span class="hlt">height</span>, and radiative forcing. We found that although the widely accepted theory of DCC invigoration due to <span class="hlt">aerosol</span>'s thermodynamic effect (additional latent heat release from freezing of greater amount of cloud water) may work during the growing stage, it is microphysical effect influenced by <span class="hlt">aerosols</span> that drives the dramatic increase in cloud cover, cloud top <span class="hlt">height</span>, and cloud thickness at the mature and dissipation stages by inducing larger amounts of smaller but longer-lasting ice particles in the stratiform/anvils of DCCs, even when thermodynamic invigoration of convection is absent. The thermodynamic invigoration effect contributes up to ∼27% of total increase in cloud cover. The overall <span class="hlt">aerosol</span> indirect effect is an atmospheric radiative warming (3-5 Wṡm-2) and a surface cooling (-5 to -8 Wṡm-2). The modeling findings are confirmed by the analyses of ample measurements made at three sites of distinctly different environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24218569','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24218569"><span>Microphysical effects determine macrophysical response for <span class="hlt">aerosol</span> impacts on deep convective clouds.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fan, Jiwen; Leung, L Ruby; Rosenfeld, Daniel; Chen, Qian; Li, Zhanqing; Zhang, Jinqiang; Yan, Hongru</p> <p>2013-11-26</p> <p>Deep convective clouds (DCCs) play a crucial role in the general circulation, energy, and hydrological cycle of our climate system. <span class="hlt">Aerosol</span> particles can influence DCCs by altering cloud properties, precipitation regimes, and radiation balance. Previous studies reported both invigoration and suppression of DCCs by <span class="hlt">aerosols</span>, but few were concerned with the whole life cycle of DCC. By conducting multiple monthlong cloud-resolving simulations with spectral-bin cloud microphysics that capture the observed macrophysical and microphysical properties of summer convective clouds and precipitation in the tropics and midlatitudes, this study provides a comprehensive view of how <span class="hlt">aerosols</span> affect cloud cover, cloud top <span class="hlt">height</span>, and radiative forcing. We found that although the widely accepted theory of DCC invigoration due to <span class="hlt">aerosol</span>'s thermodynamic effect (additional latent heat release from freezing of greater amount of cloud water) may work during the growing stage, it is microphysical effect influenced by <span class="hlt">aerosols</span> that drives the dramatic increase in cloud cover, cloud top <span class="hlt">height</span>, and cloud thickness at the mature and dissipation stages by inducing larger amounts of smaller but longer-lasting ice particles in the stratiform/anvils of DCCs, even when thermodynamic invigoration of convection is absent. The thermodynamic invigoration effect contributes up to ~27% of total increase in cloud cover. The overall <span class="hlt">aerosol</span> indirect effect is an atmospheric radiative warming (3-5 W m(-2)) and a surface cooling (-5 to -8 W m(-2)). The modeling findings are confirmed by the analyses of ample measurements made at three sites of distinctly different environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020064465&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=20020064465&hterms=air+asia&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dair%2Basia"><span>Overview of ACE-Asia Spring 2001 Investigations On <span class="hlt">Aerosol</span>-Radiation Interactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Russell, P. B.; Flatau, P. J.; Valero, F. P. J.; Nakajima, T.; Holben, B.; Pilewskie, P.; Bergin, M.; Schmid, B.; Bergstrom, R. W.; Vogelmann, A.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20020064465'); toggleEditAbsImage('author_20020064465_show'); toggleEditAbsImage('author_20020064465_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20020064465_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20020064465_hide"></p> <p>2002-01-01</p> <p>ACE-Asia's extensive measurements from land, ocean, air and space quantified <span class="hlt">aerosol</span>-radiation interactions. Results from each platform type, plus satellite-suborbital combinations, include: 1. Time series of multiwavelength <span class="hlt">aerosol</span> optical depth (ADD), Angstrom exponent (alpha), single-scattering albedo (SSA), and size distribution from AERONET radiometry at 13 stations. In China and Korea AOD and alpha were strongly anticorrelated (reflecting transient dust events); dust volume-size modes peaked near 8 microns diameter; and SSA(dust) greater than SSA(pollution). 2. Calculations and measurements of photosynthetically active radiation and <span class="hlt">aerosols</span> in China yield 24-h average downward surface radiative forcing per AOD(500 nm) of -27 W/sq m (400-700 nm). 3. The Hawaii-Japan cruise sampled a gradient with AOD(500 nm) extremes of 0.1 and 1.1. Shipboard measurements showed that adding dust to pollution increased SSA(550 nm, 55% RH), typically from -0.91 to approx. 0.97. Downwelling 8-12 micron radiances showed <span class="hlt">aerosol</span> effects, especially in the major April dust event, with longwave forcing estimated at -5 to 15 W/sq m. 4. Extinction profiles from airborne sunphotometry and total-direct-diffuse radiometry show wavelength dependence often varying strongly with <span class="hlt">height</span>, reflecting layering of dust-dominated over pollution-dominated <span class="hlt">aerosols</span>. Comparing sunphotometric extinction profiles to those from in situ measurements (number and composition vs size, or scattering and absorption) shows layer <span class="hlt">heights</span> agree, but extinction sometimes differs. 5. Airborne solar spectral flux radiometry yields absorption spectra for layers. Combining with AOD spectra yields best-fit <span class="hlt">aerosol</span> single scattering albedo spectra. 6. Visible, NIR and total solar fluxes combined with AOD give radiative forcing efficiencies at surface and aloft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.8801W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.8801W"><span>The impact of <span class="hlt">aerosol</span> vertical distribution on <span class="hlt">aerosol</span> optical depth retrieval using CALIPSO and MODIS data: Case study over dust and smoke regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Yerong; de Graaf, Martin; Menenti, Massimo</p> <p>2017-08-01</p> <p>Global quantitative <span class="hlt">aerosol</span> information has been derived from MODerate Resolution Imaging SpectroRadiometer (MODIS) observations for decades since early 2000 and widely used for air quality and climate change research. However, the operational MODIS <span class="hlt">Aerosol</span> Optical Depth (AOD) products Collection 6 (C6) can still be biased, because of uncertainty in assumed <span class="hlt">aerosol</span> optical properties and <span class="hlt">aerosol</span> vertical distribution. This study investigates the impact of <span class="hlt">aerosol</span> vertical distribution on the AOD retrieval. We developed a new algorithm by considering dynamic vertical profiles, which is an adaptation of MODIS C6 Dark Target (C6_DT) algorithm over land. The new algorithm makes use of the <span class="hlt">aerosol</span> vertical profile extracted from Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) measurements to generate an accurate top of the atmosphere (TOA) reflectance for the AOD retrieval, where the profile is assumed to be a single layer and represented as a Gaussian function with the mean <span class="hlt">height</span> as single variable. To test the impact, a comparison was made between MODIS DT and <span class="hlt">Aerosol</span> Robotic Network (AERONET) AOD, over dust and smoke regions. The results show that the <span class="hlt">aerosol</span> vertical distribution has a strong impact on the AOD retrieval. The assumed <span class="hlt">aerosol</span> layers close to the ground can negatively bias the retrievals in C6_DT. Regarding the evaluated smoke and dust layers, the new algorithm can improve the retrieval by reducing the negative biases by 3-5%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A21D0070S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A21D0070S"><span>Regional and transported <span class="hlt">aerosols</span> during DRAGON-Japan experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sano, I.; Holben, B. N.; Mukai, S.; Nakata, M.; Nakaguchi, Y.; Sugimoto, N.; Hatakeyama, S.; Nishizawa, T.; Takamura, T.; Takemura, T.; Yonemitsu, M.; Fujito, T.; Schafer, J.; Eck, T. F.; Sorokin, M.; Kenny, P.; Goto, M.; Hiraki, T.; Iguchi, N.; Kouzai, K.; KUJI, M.; Muramatsu, K.; Okada, Y.; Sadanaga, Y.; Tohno, S.; Toyazaki, Y.; Yamamoto, K.</p> <p>2013-12-01</p> <p><span class="hlt">Aerosol</span> properties over Japan have been monitored by AERONET sun / sky photometers since 2000. These measurements provides us with long term information of local <span class="hlt">aerosols</span>, which are influenced by transported <span class="hlt">aerosols</span>, such as Asian dusts or anthropogenic pollutants due to rapid increasing of energy consumption in Asian countries. A new <span class="hlt">aerosol</span> monitoring experiment, Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON) - Japan is operated in spring of 2012. The main instrument of DRAGON network is AERONET sun/sky radiometers. Some of them are sparsely set along the Japanese coast and some others make a dense network in Osaka, which is the second-largest city in Japan and famous for manufacturing town. Several 2ch NIES-LIDAR systems are also co-located with AERONET instrument to monitor Asian dusts throughout the campaign. The objects of Dragon-Japan are to characterize local <span class="hlt">aerosols</span> as well as transported ones from the continent of China, and to acquire the detailed <span class="hlt">aerosol</span> information for validating satellite data with high resolved spatial <span class="hlt">scale</span>. This work presents the comprehensive results of <span class="hlt">aerosol</span> properties with respect to regional- and/or transported- <span class="hlt">scale</span> during DRAGON-Japan experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870027224&hterms=vertical+height&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dvertical%2Bheight','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870027224&hterms=vertical+height&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dvertical%2Bheight"><span>Vertical normal modes of a mesoscale model using a <span class="hlt">scaled</span> <span class="hlt">height</span> coordinate</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lipton, A. E.; Pielke, R. A.</p> <p>1986-01-01</p> <p>Vertical modes were derived for a version of the Colorado State Regional Atmospheric Mesoscale Modeling System. The impacts of three options for dealing with the upper boundary of the model were studied. The standard model formulation holds pressure constant at a fixed altitude near the model top, and produces a fastest mode with a speed of about 90 m/sec. An alternative formulation, which allows for an external mode, could require recomputation of vertical modes for every surface elevation on the horizontal grid unless the modes are derived in a particular way. These results have bearing on the feasibility of applying vertical mode initialization to models with <span class="hlt">scaled</span> <span class="hlt">height</span> coordinates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AtmEn..40.4751T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AtmEn..40.4751T"><span>Atmospheric <span class="hlt">aerosol</span> composition and source apportionments to <span class="hlt">aerosol</span> in southern Taiwan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsai, Ying I.; Chen, Chien-Lung</p> <p></p> <p>In this study, the chemical characteristics of winter <span class="hlt">aerosol</span> at four sites in southern Taiwan were determined and the Gaussian Trajectory transfer coefficient model (GTx) was then used to identify the major air pollutant sources affecting the study sites. <span class="hlt">Aerosols</span> were found to be acidic at all four sites. The most important constituents of the particulate matter (PM) by mass were SO 42-, organic carbon (OC), NO 3-, elemental carbon (EC) and NH 4+, with SO 42-, NO 3-, and NH 4+ together constituting 86.0-87.9% of the total PM 2.5 soluble inorganic salts and 68.9-78.3% of the total PM 2.5-10 soluble inorganic salts, showing that secondary photochemical solution components such as these were the major contributors to the <span class="hlt">aerosol</span> water-soluble ions. The coastal site, Linyuan (LY), had the highest PM mass percentage of sea salts, higher in the coarse fraction, and higher sea salts during daytime than during nighttime, indicating that the prevailing daytime sea breeze brought with it more sea-salt <span class="hlt">aerosol</span>. Other than sea salts, crustal matter, and EC in PM 2.5 at Jenwu (JW) and in PM 2.5-10 at LY, all <span class="hlt">aerosol</span> components were higher during nighttime, due to relatively low nighttime mixing <span class="hlt">heights</span> limiting vertical and horizontal dispersion. At JW, a site with heavy traffic loadings, the OC/EC ratio in the nighttime fine and coarse fractions of approximately 2.2 was higher than during daytime, indicating that in addition to primary organic <span class="hlt">aerosol</span> (POA), secondary organic <span class="hlt">aerosol</span> (SOA) also contributed to the nighttime PM 2.5. This was also true of the nighttime coarse fraction at LY. The GTx produced correlation coefficients ( r) for simulated and observed daily concentrations of PM 10 at the four sites (receptors) in the range 0.45-0.59 and biases from -6% to -20%. Source apportionment indicated that point sources were the largest PM 10 source at JW, LY and Daliao (DL), while at Meinung (MN), a suburban site with less local PM 10, SO x and NO x emissions, upwind</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDM35010S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDM35010S"><span>From bubble bursting to droplet evaporation in the context of champagne <span class="hlt">aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seon, Thomas; Ghabache, Elisabeth; Antkowiak, Arnaud; Liger-Belair, Gerard</p> <p>2015-11-01</p> <p>As champagne or sparkling wine is poured into a glass, a myriad of ascending bubbles collapse and therefore radiate a multitude of tiny droplets above the free surface into the form of very characteristic and refreshing <span class="hlt">aerosols</span>. Because these <span class="hlt">aerosols</span> have been found to hold the organoleptic ``essence'' of champagne they are believed to play a crucial role in the flavor release in comparison with that from a flat wine for example. Based on the model experiment of a single bubble bursting in idealized champagnes, the velocity, radius and maximum <span class="hlt">height</span> of the first jet drop following bubble collapse have been characterized, with varying bubble size and liquid properties in the context of champagne <span class="hlt">aerosols</span>. Using the experimental results and simple theoretical models for drop and surface evaporation, we show that bubble bursting <span class="hlt">aerosols</span> drastically enhance the transfer of liquid in the atmosphere with respect to a flat liquid surface. Contrary to popular opinion, we exhibit that small bubbles are negative in terms of aroma release, and we underline bubble radii enabling to optimize the droplet <span class="hlt">height</span> and evaporation in the whole range of champagne properties. These results pave the road to the fine tuning of champagne aroma diffusion, a major issue of the sparkling wine industry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.147v0901B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.147v0901B"><span>Perspective: <span class="hlt">Aerosol</span> microphysics: From molecules to the chemical physics of <span class="hlt">aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bzdek, Bryan R.; Reid, Jonathan P.</p> <p>2017-12-01</p> <p><span class="hlt">Aerosols</span> are found in a wide diversity of contexts and applications, including the atmosphere, pharmaceutics, and industry. <span class="hlt">Aerosols</span> are dispersions of particles in a gas, and the coupling of the two phases results in highly dynamic systems where chemical and physical properties like size, composition, phase, and refractive index change rapidly in response to environmental perturbations. <span class="hlt">Aerosol</span> particles span a wide range of sizes from 1 nm to tens of micrometres or from small molecular clusters that may more closely resemble gas phase molecules to large particles that can have similar qualities to bulk materials. However, even large particles with finite volumes exhibit distinct properties from the bulk condensed phase, due in part to their higher surface-to-volume ratio and their ability to easily access supersaturated solute states inaccessible in the bulk. <span class="hlt">Aerosols</span> represent a major challenge for study because of the facile coupling between the particle and gas, the small amounts of sample available for analysis, and the sheer breadth of operative processes. Time <span class="hlt">scales</span> of <span class="hlt">aerosol</span> processes can be as short as nanoseconds or as long as years. Despite their very different impacts and applications, fundamental chemical physics processes serve as a common theme that underpins our understanding of <span class="hlt">aerosols</span>. This perspective article discusses challenges in the study of <span class="hlt">aerosols</span> and highlights recent chemical physics advancements that have enabled improved understanding of these complex systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11993964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11993964"><span><span class="hlt">Aerosol</span> impacts on visible light extinction in the atmosphere of Mexico City.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Eidels-Dubovoi, Silvia</p> <p>2002-03-27</p> <p>Eleven diurnal <span class="hlt">aerosol</span> visible light absorption and scattering patterns were obtained from measurements done with an aethalometer and an integrating nephelometer during 28 February-10 March 1997 at two different sites in the Mexico City basin. Both measurement sites, the Merced site affected by regional and urban-<span class="hlt">scale</span> <span class="hlt">aerosol</span> and the Pedregal site dominated by regional-<span class="hlt">scale</span> <span class="hlt">aerosol</span>, showed a variety of diurnal light absorption and scattering patterns. For the majority of the 11 studied days, the highest absorption peaks appeared in the early morning, 07.00-09.30 h while those of scattering appeared later, 09.30-11.00 h. The earlier absorption peaks could be attributed to the elevated elemental carbon vehicular emissions during the heavy traffic hours whereas the later scattering peaks could be attributed to secondary <span class="hlt">aerosols</span> formed photochemically in the atmosphere. During the period examined, the Pedregal site exhibited on the average a lower <span class="hlt">aerosol</span> scattering and a higher <span class="hlt">aerosol</span> absorption contribution to the total <span class="hlt">aerosol</span> visible light extinction and a better visibility than that of the Merced site. Hence, the impact of <span class="hlt">aerosol</span> absorption on the visibility degradation due to <span class="hlt">aerosols</span> was greater at the less hazy Pedregal site. The overall 11-day <span class="hlt">aerosol</span> visibility average of 20.9 km found at La Merced site, was only 9.4 km lower than that of 30.3 km found at the Pedregal site. This small <span class="hlt">aerosol</span> visibility difference, of the order of the standard deviation, led to the conclusion that besides the regional-<span class="hlt">scale</span> <span class="hlt">aerosol</span> impact, the urban-<span class="hlt">scale</span> <span class="hlt">aerosol</span> impact on <span class="hlt">aerosol</span> visible light extinction is very similar at La Merced and Pedregal sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003892&hterms=layer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlayer','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003892&hterms=layer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlayer"><span>Elevated <span class="hlt">Aerosol</span> Layers and Their Radiative Impact over Kanpur During Monsoon Onset Period</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sarangi, Chandan; Tripathi, S. N.; Mishra, A. K.; Welton, E. J.</p> <p>2016-01-01</p> <p>Accurate information about <span class="hlt">aerosol</span> vertical distribution is needed to reduce uncertainties in <span class="hlt">aerosol</span> radiative forcing and its effect on atmospheric dynamics. The present study deals with synergistic analyses of <span class="hlt">aerosol</span> vertical distribution and <span class="hlt">aerosol</span> optical depth (AOD) with meteorological variables using multisatellite and ground-based remote sensors over Kanpur in central Indo-Gangetic Plain (IGP). Micro-Pulse Lidar Network-derived <span class="hlt">aerosol</span> vertical extinction (sigma) profiles are analyzed to quantify the interannual and daytime variations during monsoon onset period (May-June) for 2009-2011. The mean <span class="hlt">aerosol</span> profile is broadly categorized into two layers viz., a surface layer (SL) extending up to 1.5 km (where sigma decreased exponentially with <span class="hlt">height</span>) and an elevated <span class="hlt">aerosol</span> layer (EAL) extending between 1.5 and 5.5 km. The increase in total columnar <span class="hlt">aerosol</span> loading is associated with relatively higher increase in contribution from EAL loading than that from SL. The mean contributions of EALs are about 60%, 51%, and 50% to total columnar AOD during 2009, 2010, and 2011, respectively. We observe distinct parabolic EALs during early morning and late evening but uniformly mixed EALs during midday. The interannual and daytime variations of EALs are mainly influenced by long-range transport and convective capacity of the local emissions, respectively. Radiative flux analysis shows that clear-sky incoming solar radiation at surface is reduced with increase in AOD, which indicates significant cooling at surface. Collocated analysis of atmospheric temperature and <span class="hlt">aerosol</span> loading reveals that increase in AOD not only resulted in surface dimming but also reduced the temperature (approximately 2-3 C) of lower troposphere (below 3 km altitude). Radiative transfer simulations indicate that the reduction of incoming solar radiation at surface is mainly due to increased absorption by EALs (with increase in total AOD). The observed cooling in lower troposphere in high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GMD....10.2231D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GMD....10.2231D"><span>Implementation of <span class="hlt">aerosol</span>-cloud interactions in the regional atmosphere-<span class="hlt">aerosol</span> model COSMO-MUSCAT(5.0) and evaluation 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>Dipu, Sudhakar; Quaas, Johannes; Wolke, Ralf; Stoll, Jens; Mühlbauer, Andreas; Sourdeval, Odran; Salzmann, Marc; Heinold, Bernd; Tegen, Ina</p> <p>2017-06-01</p> <p>The regional atmospheric model Consortium for Small-<span class="hlt">scale</span> Modeling (COSMO) coupled to the Multi-<span class="hlt">Scale</span> Chemistry <span class="hlt">Aerosol</span> Transport model (MUSCAT) is extended in this work to represent <span class="hlt">aerosol</span>-cloud interactions. Previously, only one-way interactions (scavenging of <span class="hlt">aerosol</span> and in-cloud chemistry) and <span class="hlt">aerosol</span>-radiation interactions were included in this model. The new version allows for a microphysical <span class="hlt">aerosol</span> effect on clouds. For this, we use the optional two-moment cloud microphysical scheme in COSMO and the online-computed <span class="hlt">aerosol</span> information for cloud condensation nuclei concentrations (Cccn), replacing the constant Cccn profile. In the radiation scheme, we have implemented a droplet-size-dependent cloud optical depth, allowing now for <span class="hlt">aerosol</span>-cloud-radiation interactions. To evaluate the models with satellite data, the Cloud Feedback Model Intercomparison Project Observation Simulator Package (COSP) has been implemented. A case study has been carried out to understand the effects of the modifications, where the modified modeling system is applied over the European domain with a horizontal resolution of 0.25° × 0.25°. To reduce the complexity in <span class="hlt">aerosol</span>-cloud interactions, only warm-phase clouds are considered. We found that the online-coupled <span class="hlt">aerosol</span> introduces significant changes for some cloud microphysical properties. The cloud effective radius shows an increase of 9.5 %, and the cloud droplet number concentration is reduced by 21.5 %.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930036960&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dvertical%2Bheight','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930036960&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dvertical%2Bheight"><span>Observations of <span class="hlt">height</span>-dependent pressure-perturbation structure of a strong mesoscale gravity wave</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Starr, David O'C.; Korb, C. L.; Schwemmer, Geary K.; Weng, Chi Y.</p> <p>1992-01-01</p> <p>Airborne observations using a downward-looking, dual-frequency, near-infrared, differential absorption lidar system provide the first measurements of the <span class="hlt">height</span>-dependent pressure-perturbation field associated with a strong mesoscale gravity wave. A pressure-perturbation amplitude of 3.5 mb was measured within the lowest 1.6 km of the atmosphere over a 52-km flight line. Corresponding vertical displacements of 250-500 m were inferred from lidar-observed displacement of <span class="hlt">aerosol</span> layers. Accounting for probable wave orientation, a horizontal wavelength of about 40 km was estimated. Satellite observations reveal wave structure of a comparable <span class="hlt">scale</span> in concurrent cirrus cloud fields over an extended area. Smaller-<span class="hlt">scale</span> waves were also observed. Local meteorological soundings are analyzed to confirm the existence of a suitable wave duct. Potential wave-generation mechanisms are examined and discussed. The large pressure-perturbation wave is attributed to rapid amplification or possible wave breaking of a gravity wave as it propagated offshore and interacted with a very stable marine boundary layer capped by a strong shear layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010087128&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D20%26Ntt%3DRussell','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010087128&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D20%26Ntt%3DRussell"><span>On the Feasibility of Studying Shortwave <span class="hlt">Aerosol</span> Radiative Forcing of Climate Using Dual-Wavelength <span class="hlt">Aerosol</span> Backscatter Lidar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Redemann, Jens; Russell, Philip B.; Winker, David M.; McCormick, M. Patrick; Hipskind, R. Stephen (Technical Monitor)</p> <p>2000-01-01</p> <p>The current low confidence in the estimates of <span class="hlt">aerosol</span>-induced perturbations of Earth's radiation balance is caused by the highly non-uniform compositional, spatial and temporal distributions of tropospheric <span class="hlt">aerosols</span> on a global <span class="hlt">scale</span> owing to their heterogeneous sources and short lifetimes. Nevertheless, recent studies have shown that the inclusion of <span class="hlt">aerosol</span> effects in climate model calculations can improve agreement with observed spatial and temporal temperature distributions. In light of the short lifetimes of <span class="hlt">aerosols</span>, determination of their global distribution with space-borne sensors seems to be a necessary approach. Until recently, satellite measurements of tropospheric <span class="hlt">aerosols</span> have been approximate and did not provide the full set of information required to determine their radiative effects. With the advent of active <span class="hlt">aerosol</span> remote sensing from space (e.g., PICASSO-CENA), the applicability fo lidar-derived <span class="hlt">aerosol</span> 180 deg -backscatter data to radiative flux calculations and hence studies of <span class="hlt">aerosol</span> effects on climate needs to be investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A52D..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A52D..07L"><span><span class="hlt">Aerosol</span> Indirect Effects on Cirrus Clouds in Global <span class="hlt">Aerosol</span>-Climate Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, X.; Zhang, K.; Wang, Y.; Neubauer, D.; Lohmann, U.; Ferrachat, S.; Zhou, C.; Penner, J.; Barahona, D.; Shi, X.</p> <p>2015-12-01</p> <p>Cirrus clouds play an important role in regulating the Earth's radiative budget and water vapor distribution in the upper troposphere. <span class="hlt">Aerosols</span> can act as solution droplets or ice nuclei that promote ice nucleation in cirrus clouds. Anthropogenic emissions from fossil fuel and biomass burning activities have substantially perturbed and enhanced concentrations of <span class="hlt">aerosol</span> particles in the atmosphere. Global <span class="hlt">aerosol</span>-climate models (GCMs) have now been used to quantify the radiative forcing and effects of <span class="hlt">aerosols</span> on cirrus clouds (IPCC AR5). However, the estimate uncertainty is very large due to the different representation of ice cloud formation and evolution processes in GCMs. In addition, large discrepancies have been found between model simulations in terms of the spatial distribution of ice-nucleating <span class="hlt">aerosols</span>, relative humidity, and temperature fluctuations, which contribute to different estimates of the <span class="hlt">aerosol</span> indirect effect through cirrus clouds. In this presentation, four GCMs with the start-of-the art representations of cloud microphysics and <span class="hlt">aerosol</span>-cloud interactions are used to estimate the <span class="hlt">aerosol</span> indirect effects on cirrus clouds and to identify the causes of the discrepancies. The estimated global and annual mean anthropogenic <span class="hlt">aerosol</span> indirect effect through cirrus clouds ranges from 0.1 W m-2 to 0.3 W m-2 in terms of the top-of-the-atmosphere (TOA) net radiation flux, and 0.5-0.6 W m-2 for the TOA longwave flux. Despite the good agreement on global mean, large discrepancies are found at the regional <span class="hlt">scale</span>. The physics behind the <span class="hlt">aerosol</span> indirect effect is dramatically different. Our analysis suggests that burden of ice-nucleating <span class="hlt">aerosols</span> in the upper troposphere, ice nucleation frequency, and relative role of ice formation processes (i.e., homogeneous versus heterogeneous nucleation) play key roles in determining the characteristics of the simulated <span class="hlt">aerosol</span> indirect effects. In addition to the indirect effect estimate, we also use field campaign</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AMT....11.3031K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AMT....11.3031K"><span>Characteristics of <span class="hlt">aerosol</span> vertical profiles in Tsukuba, Japan, and their impacts on the evolution of the atmospheric boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kudo, Rei; Aoyagi, Toshinori; Nishizawa, Tomoaki</p> <p>2018-05-01</p> <p>.6 K) and the direct heating of <span class="hlt">aerosols</span> in the FA (0.0 to 0.4 K) strengthened the capping inversion around the top of the ABL. Consequently, the ABL <span class="hlt">height</span> was decreased by 133 to 208 m in simulations with <span class="hlt">aerosols</span> compared to simulations without <span class="hlt">aerosols</span>. (2) We also conducted simulations in which all <span class="hlt">aerosols</span> were compressed into the ABL but in which the columnar properties were the same and compared with the simulation results for uncompressed <span class="hlt">aerosol</span> profiles. The results showed that the reductions in net downward radiation and in sensible and latent heat fluxes were the same in both types of simulations. However, the capping inversion in the simulations with compression was weakened owing to <span class="hlt">aerosol</span> direct heating in the ABL and the lack of direct heating in the FA. This resulted in an increase in the ABL <span class="hlt">height</span>, compared with that in the simulations without compression. (3) The dependencies of the 2 m temperature and ABL <span class="hlt">height</span> on the optical thickness and Ångström exponent in the FA were investigated using the results of the numerical sensitivity tests. The 2 m temperature and ABL <span class="hlt">height</span> was decreased with an increase in the optical thickness, and their reduction rates increase with a decrease in the Ångström exponent because the optical thickness in the near-infrared wavelength region was large when the Ångström exponent was small. However, there was a case in which the Ångström exponent was large but the decrease in the ABL <span class="hlt">height</span> was the largest of all the simulation results. In this case, the strong capping inversion due to the large extinction coefficient around the top of the ABL was an import factor. These results suggest that the vertical profiles of the <span class="hlt">aerosol</span> physical and optical properties, and the resulting direct heating has important effects on the ABL evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H21E1509B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H21E1509B"><span>Understanding <span class="hlt">aerosol</span>-cloud interactions in the development of orographic cumulus congestus during IPHEx</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barros, A. P.; Duan, Y.</p> <p>2017-12-01</p> <p>A new cloud parcel model (CPM) including activation, condensation, collision-coalescence, and lateral entrainment processes is presented here to investigate <span class="hlt">aerosol</span>-cloud interactions (ACI) in cumulus development prior to rainfall onset. The CPM was employed along with ground based radar and surface <span class="hlt">aerosol</span> measurements to predict the vertical structure of cloud formation at early stages and evaluated against airborne observations of cloud microphysics and thermodynamic conditions during the Integrated Precipitation and Hydrology Experiment (IPHEx) over the Southern Appalachian Mountains. Further, the CPM was applied to explore the space of ACI physical parameters controlling cumulus congestus growth not available from measurements, and to examine how variations in <span class="hlt">aerosol</span> properties and microphysical processes influence the evolution and thermodynamic state of clouds over complex terrain via sensitivity analysis. Modeling results indicate that simulated spectra with a low value of condensation coefficient (0.01) are in good agreement with IPHEx aircraft observations around the same altitude. This is in contrast with high values reported in previous studies assuming adiabatic conditions. Entrainment is shown to govern the vertical development of clouds and the change of droplet numbers with <span class="hlt">height</span>, and the sensitivity analysis suggests that there is a trade-off between entrainment strength and condensation process. Simulated CDNC also exhibits high sensitivity to variations in initial <span class="hlt">aerosol</span> concentration at cloud base, but weak sensitivity to <span class="hlt">aerosol</span> hygroscopicity. Exploratory multiple-parcel simulations capture realistic time-<span class="hlt">scales</span> of vertical development of cumulus congestus (deeper clouds and faster droplet growth). These findings provide new insights into determinant factors of mid-day cumulus congestus formation that can explain a large fraction of warm season rainfall in mountainous regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160012701','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160012701"><span><span class="hlt">Aerosol</span> Complexity and Implications for Predictability and Short-Term Forecasting</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Colarco, Peter</p> <p>2016-01-01</p> <p>There are clear NWP and climate impacts from including <span class="hlt">aerosol</span> radiative and cloud interactions. Changes in dynamics and cloud fields affect <span class="hlt">aerosol</span> lifecycle, plume <span class="hlt">height</span>, long-range transport, overall forcing of the climate system, etc. Inclusion of <span class="hlt">aerosols</span> in NWP systems has benefit to surface field biases (e.g., T2m, U10m). Including <span class="hlt">aerosol</span> affects has impact on analysis increments and can have statistically significant impacts on, e.g., tropical cyclogenesis. Above points are made especially with respect to <span class="hlt">aerosol</span> radiative interactions, but <span class="hlt">aerosol</span>-cloud interaction is a bigger signal on the global system. Many of these impacts are realized even in models with relatively simple (bulk) <span class="hlt">aerosol</span> schemes (approx.10 -20 tracers). Simple schemes though imply simple representation of <span class="hlt">aerosol</span> absorption and importantly for <span class="hlt">aerosol</span>-cloud interaction particle-size distribution. Even so, more complex schemes exhibit a lot of diversity between different models, with issues such as size selection both for emitted particles and for modes. Prospects for complex sectional schemes to tune modal (and even bulk) schemes toward better selection of size representation. I think this is a ripe topic for more research -Systematic documentation of benefits of no vs. climatological vs. interactive (direct and then direct+indirect) <span class="hlt">aerosols</span>. Document <span class="hlt">aerosol</span> impact on analysis increments, inclusion in NWP data assimilation operator -Further refinement of baseline assumptions in model design (e.g., absorption, particle size distribution). Did not get into model resolution and interplay of other physical processes with <span class="hlt">aerosols</span> (e.g., moist physics, obviously important), chemistry</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/26421659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26421659"><span>Estimation of surface-level PM concentration from satellite observation taking into account the <span class="hlt">aerosol</span> vertical profiles and hygroscopicity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Kwanchul; Lee, Kwon H; Kim, Ji I; Noh, Youngmin; Shin, Dong H; Shin, Sung K; Lee, Dasom; Kim, Jhoon; Kim, Young J; Song, Chul H</p> <p>2016-01-01</p> <p>Surface-level PM10 distribution was estimated from the satellite <span class="hlt">aerosol</span> optical depth (AOD) products, taking the account of vertical profiles and hygroscopicity of <span class="hlt">aerosols</span> over Jeju, Korea during March 2008 and October 2009. In this study, MODIS AOD data from the Terra and Aqua satellites were corrected with <span class="hlt">aerosol</span> extinction profiles and relative humidity data. PBLH (Planetary Boundary Layer <span class="hlt">Height</span>) was determined from MPLNET lidar-derived <span class="hlt">aerosol</span> extinction coefficient profiles. Through statistical analysis, better agreement in correlation (R = 0.82) between the hourly PM10 concentration and hourly average Sunphotometer AOD was the obtained when vertical fraction method (VFM) considering Haze Layer <span class="hlt">Height</span> (HLH) and hygroscopic growth factor f(RH) was used. The validity of the derived relationship between satellite AOD and surface PM10 concentration clearly demonstrates that satellite AOD data can be utilized for remote sensing of spatial distribution of regional PM10 concentration. Copyright © 2015 The Authors. Published by Elsevier Ltd.. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....16.9201W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....16.9201W"><span>The importance of plume rise on the concentrations and atmospheric impacts of biomass burning <span class="hlt">aerosol</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Walter, Carolin; Freitas, Saulo R.; Kottmeier, Christoph; Kraut, Isabel; Rieger, Daniel; Vogel, Heike; Vogel, Bernhard</p> <p>2016-07-01</p> <p>We quantified the effects of the plume rise of biomass burning <span class="hlt">aerosol</span> and gases for the forest fires that occurred in Saskatchewan, Canada, in July 2010. For this purpose, simulations with different assumptions regarding the plume rise and the vertical distribution of the emissions were conducted. Based on comparisons with observations, applying a one-dimensional plume rise model to predict the injection layer in combination with a parametrization of the vertical distribution of the emissions outperforms approaches in which the plume <span class="hlt">heights</span> are initially predefined. Approximately 30 % of the fires exceed the <span class="hlt">height</span> of 2 km with a maximum <span class="hlt">height</span> of 8.6 km. Using this plume rise model, comparisons with satellite images in the visible spectral range show a very good agreement between the simulated and observed spatial distributions of the biomass burning plume. The simulated <span class="hlt">aerosol</span> optical depth (AOD) with data of an AERONET station is in good agreement with respect to the absolute values and the timing of the maximum. Comparison of the vertical distribution of the biomass burning <span class="hlt">aerosol</span> with CALIPSO (Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation) retrievals also showed the best agreement when the plume rise model was applied. We found that downwelling surface short-wave radiation below the forest fire plume is reduced by up to 50 % and that the 2 m temperature is decreased by up to 6 K. In addition, we simulated a strong change in atmospheric stability within the biomass burning plume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4138729','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4138729"><span>Variations of <span class="hlt">Scale</span> <span class="hlt">Height</span> at F-Region Peak Based on Ionosonde Measurements during Solar Maximum over the Crest of Equatorial Ionization Anomaly Region</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chuo, Yu-Jung</p> <p>2014-01-01</p> <p><span class="hlt">Scale</span> <span class="hlt">height</span> is an important parameter in characterizing the shape of the ionosphere and its physical processes. In this study, we attempt to examine and discuss the variation of <span class="hlt">scale</span> <span class="hlt">height</span>, H m, around the F-layer peak <span class="hlt">height</span> during high solar activity at the northern crest of the equatorial ionization anomaly (EIA) region. H m exhibits day-to-day variation and seasonal variation, with a greater average daily variation during daytime in summer. Furthermore, the diurnal variation of H m exhibits an abnormal peak at presunrise during all the seasons, particularly in winter. This increase is also observed in the F2-layer peak <span class="hlt">height</span> for the same duration with an upward movement associated with thermospheric wind toward the equator; this upward movement increases the N2/O ratio and H m, but it causes a decrease in the F2-layer maximum critical frequency during the presunrise period. PMID:25162048</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1246477-anthropogenic-aerosols-distribution-past-large-scale-precipitation-change','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1246477-anthropogenic-aerosols-distribution-past-large-scale-precipitation-change"><span>Anthropogenic <span class="hlt">aerosols</span> and the distribution of past large-<span class="hlt">scale</span> precipitation change</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wang, Chien</p> <p>2015-12-28</p> <p>In this paper, the climate response of precipitation to the effects of anthropogenic <span class="hlt">aerosols</span> is a critical while not yet fully understood aspect in climate science. Results of selected models that participated the Coupled Model Intercomparison Project Phase 5 and the data from the Twentieth Century Reanalysis Project suggest that, throughout the tropics and also in the extratropical Northern Hemisphere, <span class="hlt">aerosols</span> have largely dominated the distribution of precipitation changes in reference to the preindustrial era in the second half of the last century. <span class="hlt">Aerosol</span>-induced cooling has offset some of the warming caused by the greenhouse gases from the tropics tomore » the Arctic and thus formed the gradients of surface temperature anomaly that enable the revealed precipitation change patterns to occur. Improved representation of <span class="hlt">aerosol</span>-cloud interaction has been demonstrated as the key factor for models to reproduce consistent distributions of past precipitation change with the reanalysis data.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000052545&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D90%26Ntt%3DRussell','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000052545&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D90%26Ntt%3DRussell"><span>North Atlantic <span class="hlt">Aerosol</span> Radiative Impacts Based on Satellite Measurements and <span class="hlt">Aerosol</span> Intensive Properties from TARFOX and ACE-2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Russell, P. B.; Bergstrom, Robert W.; Schmid, B.; Livingston, J. M.</p> <p>2000-01-01</p> <p>We estimate the impact of North Atlantic <span class="hlt">aerosols</span> on the net short-wave flux at the tropopause by combining satellite-derived <span class="hlt">aerosol</span> optical depth (AOD) maps with model <span class="hlt">aerosol</span> properties determined via closure analyses in TARFOX and ACE 2. We exclude African dust, primarily by restricting latitudes to 25-60 N. The analyses use in situ <span class="hlt">aerosol</span> composition measurements and air- and ship-borne sun-photometer measurements of AOD spectra. The <span class="hlt">aerosol</span> model yields computed flux sensitivities (dFlux/dAOD) that agree with measurements by airborne flux radiometers in TARFOX. Its midvisible single-scattering albedo is 0.9. which is in the range obtained from in situ measurements of scattering and absorption in both TARFOX and ACE 2. Combining satellite-derived AOD maps with the <span class="hlt">aerosol</span> model yields maps of 24-hour average net radiative flux changes. For simultaneous AVHRR, radiance measurements exceeded the sunphotometer AODs by about 0.04. However. shipboard sunphotometer and AVHRR AODs agreed Within 0.02 for data acquired during satellite overflights on two other days. We discuss attempts to demonstrate column closure within the MBL by comparing shipboard sunphotometer AODs and values calculated from simultaneous shipboard in-situ <span class="hlt">aerosol</span> size distribution measurements. These comparisons were mostly unsuccessful, but they illustrate the difficulties inherent in this type of closure analysis. Specifically, AODs derived from near-surface in-situ size distribution measurements are extremely sensitive to the assumed hygroscopic growth model that itself requires an assumption of particle composition as a function of <span class="hlt">height</span> and size, to the radiosonde-measured relative humidity, and to the vertical profile of particle number. We investigate further the effects of hygroscopic particle growth within the MBL by using shipboard lidar <span class="hlt">aerosol</span> backscatter profiles together with the sunphotometer AOD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070022884','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070022884"><span>Midweek Increase in U.S. Summer Rain and Storm <span class="hlt">Heights</span>, Suggests Air Pollution Invigorates Rainstorms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bell, Thomas L.; Rosenfeld, Daniel; Kim, Kyu-Myong; Yoo, Jung-Moon; Hahnenberger, Maura</p> <p>2007-01-01</p> <p>Tropical Rainfall Measuring Mission (TRMM) satellite data show a significant midweek increase in summertime rainfall over the southeast U.S., due to afternoon intensification. TRMM radar data show a significant midweek increase in rain area and in the <span class="hlt">heights</span> reached by afternoon storms. Weekly variations in model-reanalysis wind patterns over the region and in rain-gauge data are consistent with the satellite data. A midweek decrease of rainfall over the nearby Atlantic is also seen. EPA measurements of particulate concentrations show a midweek peak over much of the U.S. These observations are consistent with the theory that anthropogenic air pollution suppresses cloud-drop coalescence and early rainout during the growth of thunderstorms over land, allowing more water to be carried above the 0 C isotherm, where freezing yields additional latent heat, invigorating the storms--most dramatically evidenced by the shift in the midweek distribution of afternoon-storm <span class="hlt">heights</span>--and producing large ice hydrometeors. The enhanced convection induces regional convergence, uplifting and an overall increase of rainfall. Compensating downward air motion suppresses convection over the adjacent ocean areas. Pre-TRMM-era data suggest that the weekly cycle only became strong enough to be detectable beginning in the 1980's. Rain-gauge data also suggest that a weekly cycle may have been detectable in the 1940's, but with peak rainfall on Sunday or Monday, possibly explained by the difference in composition of <span class="hlt">aerosol</span> pollution at that time. This "weekend effect" may thus offer climate researchers an opportunity to study the regional climate-<span class="hlt">scale</span> impact of <span class="hlt">aerosols</span> on storm development and monsoon-like circulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AtmRe.120..334M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AtmRe.120..334M"><span>Typical tropospheric <span class="hlt">aerosol</span> backscatter profiles for Southern Ireland: The Cork Raman lidar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McAuliffe, Michael A. P.; Ruth, Albert A.</p> <p>2013-02-01</p> <p>A Raman lidar instrument (UCLID) was established at the University College Cork as part of the European lidar network EARLINET. Raman backscatter coefficients, extinction coefficients and lidar ratios were measured within the period 28/08/2010 and 24/04/2011. Typical atmospheric scenarios over Southern Ireland in terms of the <span class="hlt">aerosol</span> load in the planetary boundary layer are outlined. The lidar ratios found are typical for marine atmospheric condition (lidar ratio ca. 20-25 sr). The <span class="hlt">height</span> of the planetary boundary layer is below 1000 m and therefore low in comparison to <span class="hlt">heights</span> found at other lidar sites in Europe. On the 21st of April a large <span class="hlt">aerosol</span> load was detected, which was assigned to a Saharan dust event based on HYSPLIT trajectories and DREAM forecasts along with the lidar ratio (70 sr) for the period concerned. The dust was found at two <span class="hlt">heights</span>, pure dust at 2.5 km and dust mixing with pollution from 0.7 to 1.8 km with a lidar ratio of 40-50 sr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1409788-retrieval-water-vapor-column-abundance-aerosol-properties-from-chemcam-passive-sky-spectroscopy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1409788-retrieval-water-vapor-column-abundance-aerosol-properties-from-chemcam-passive-sky-spectroscopy"><span>Retrieval of water vapor column abundance and <span class="hlt">aerosol</span> properties from ChemCam passive sky spectroscopy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>McConnochie, Timothy H.; Smith, Michael D.; Wolff, Michael J.; ...</p> <p>2017-11-03</p> <p>In this work, we derive water vapor column abundances and <span class="hlt">aerosol</span> properties from Mars Science Laboratory (MSL) ChemCam passive mode observations of scattered sky light. This paper covers the methodology and initial results for water vapor and also provides preliminary results for <span class="hlt">aerosols</span>. The data set presented here includes the results of 113 observations spanning from Mars Year 31 L s = 291° (March 30, 2013) to Mars Year 33 L s= 127° (March 24, 2016). Each ChemCam passive sky observation acquires spectra at two different elevation angles. We fit these spectra with a discrete-ordinates multiple scattering radiative transfer model,more » using the correlated-k approximation for gas absorption bands. The retrieval proceeds by first fitting the continuum of the ratio of the two elevation angles to solve for <span class="hlt">aerosol</span> properties, and then fitting the continuum-removed ratio to solve for gas abundances. The final step of the retrieval makes use of the observed CO 2 absorptions and the known CO 2 abundance to correct the retrieved water vapor abundance for the effects of the vertical distribution of scattering <span class="hlt">aerosols</span> and to derive an <span class="hlt">aerosol</span> <span class="hlt">scale</span> <span class="hlt">height</span> parameter. Our water vapor results give water vapor column abundance with a precision of ±0.6 precipitable microns and systematic errors no larger than ±0.3 precipitable microns, assuming uniform vertical mixing. The ChemCam-retrieved water abundances show, with only a few exceptions, the same seasonal behavior and the same timing of seasonal minima and maxima as the TES, CRISM, and REMS-H data sets that we compare them to. However ChemCam-retrieved water abundances are generally lower than zonal and regional <span class="hlt">scale</span> from-orbit water vapor data, while at the same time being significantly larger than pre-dawn REMS-H abundances. Pending further analysis of REMS-H volume mixing ratio uncertainties, the differences between ChemCam and REMS-H pre-dawn mixing ratios appear to be much too large to be explained by large</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1409788-retrieval-water-vapor-column-abundance-aerosol-properties-from-chemcam-passive-sky-spectroscopy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1409788-retrieval-water-vapor-column-abundance-aerosol-properties-from-chemcam-passive-sky-spectroscopy"><span>Retrieval of water vapor column abundance and <span class="hlt">aerosol</span> properties from ChemCam passive sky spectroscopy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>McConnochie, Timothy H.; Smith, Michael D.; Wolff, Michael J.</p> <p></p> <p>In this work, we derive water vapor column abundances and <span class="hlt">aerosol</span> properties from Mars Science Laboratory (MSL) ChemCam passive mode observations of scattered sky light. This paper covers the methodology and initial results for water vapor and also provides preliminary results for <span class="hlt">aerosols</span>. The data set presented here includes the results of 113 observations spanning from Mars Year 31 L s = 291° (March 30, 2013) to Mars Year 33 L s= 127° (March 24, 2016). Each ChemCam passive sky observation acquires spectra at two different elevation angles. We fit these spectra with a discrete-ordinates multiple scattering radiative transfer model,more » using the correlated-k approximation for gas absorption bands. The retrieval proceeds by first fitting the continuum of the ratio of the two elevation angles to solve for <span class="hlt">aerosol</span> properties, and then fitting the continuum-removed ratio to solve for gas abundances. The final step of the retrieval makes use of the observed CO 2 absorptions and the known CO 2 abundance to correct the retrieved water vapor abundance for the effects of the vertical distribution of scattering <span class="hlt">aerosols</span> and to derive an <span class="hlt">aerosol</span> <span class="hlt">scale</span> <span class="hlt">height</span> parameter. Our water vapor results give water vapor column abundance with a precision of ±0.6 precipitable microns and systematic errors no larger than ±0.3 precipitable microns, assuming uniform vertical mixing. The ChemCam-retrieved water abundances show, with only a few exceptions, the same seasonal behavior and the same timing of seasonal minima and maxima as the TES, CRISM, and REMS-H data sets that we compare them to. However ChemCam-retrieved water abundances are generally lower than zonal and regional <span class="hlt">scale</span> from-orbit water vapor data, while at the same time being significantly larger than pre-dawn REMS-H abundances. Pending further analysis of REMS-H volume mixing ratio uncertainties, the differences between ChemCam and REMS-H pre-dawn mixing ratios appear to be much too large to be explained by large</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080014273','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080014273"><span>Inter-Comparison of ILAS-II Version 1.4 <span class="hlt">Aerosol</span> Extinction Coefficient at 780 nm with SAGE II, SAGE III, and POAM III <span class="hlt">Aerosol</span> Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Saitoh, Naoko; Hayashida, S.; Sugita, T.; Nakajima, H.; Yokota, T.; Hayashi, M.; Shiraishi, K.; Kanzawa, H.; Ejiri, M. K.; Irie, H.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20080014273'); toggleEditAbsImage('author_20080014273_show'); toggleEditAbsImage('author_20080014273_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20080014273_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20080014273_hide"></p> <p>2006-01-01</p> <p>The Improved Limb Atmospheric Spectrometer (ILAS) II on board the Advanced Earth Observing Satellite (ADEOS) II observed stratospheric <span class="hlt">aerosol</span> in visible/near-infrared/infrared spectra over high latitudes in the Northern and Southern Hemispheres. Observations were taken intermittently from January to March, and continuously from April through October, 2003. We assessed the data quality of ILAS-II version 1.4 <span class="hlt">aerosol</span> extinction coefficients at 780 nm from comparisons with the Stratospheric <span class="hlt">Aerosol</span> and Gas Experiment (SAGE) II, SAGE III, and the Polar Ozone and <span class="hlt">Aerosol</span> Measurement (POAM) III <span class="hlt">aerosol</span> data. At <span class="hlt">heights</span> below 20 km in the Northern Hemisphere, <span class="hlt">aerosol</span> extinction coefficients from ILAS-II agreed with those from SAGE II and SAGE III within 10%, and with those from POAM III within 15%. From 20 to 26 km, ILAS-II <span class="hlt">aerosol</span> extinction coefficients were smaller than extinction coefficients from the other sensors; differences between ILAS-II and SAGE II ranged from 10% at 20 km to 34% at 26 km. ILAS-II <span class="hlt">aerosol</span> extinction coefficients from 20 to 25 km in February over the Southern Hemisphere had a negative bias (12-66%) relative to SAGE II <span class="hlt">aerosol</span> data. The bias increased with increasing altitude. Comparisons between ILAS-II and POAM III <span class="hlt">aerosol</span> extinction coefficients from January to May in the Southern Hemisphere (defined as the non-Polar Stratospheric Cloud (PSC) season ) yielded qualitatively similar results. From June to October (defined as the PSC season ), <span class="hlt">aerosol</span> extinction coefficients from ILAS-II were smaller than those from POAM III above 17 km, as in the case of the non-PSC season; however, ILAS-II and POAM III <span class="hlt">aerosol</span> data were within 15% of each other from 12 to 17 km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1812194G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1812194G"><span>Diurnal cycling of urban <span class="hlt">aerosols</span> under different weather regimes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gregorič, Asta; Drinovec, Luka; Močnik, Griša; Remškar, Maja; Vaupotič, Janja; Stanič, Samo</p> <p>2016-04-01</p> <p>A one month measurement campaign was performed in summer 2014 in Ljubljana, the capital of Slovenia (population 280,000), aiming to study temporal and spatial distribution of urban <span class="hlt">aerosols</span> and the mixing state of primary and secondary <span class="hlt">aerosols</span>. Two background locations were chosen for this purpose, the first one in the city center (urban background - KIS) and the second one in the suburban background (Brezovica). Simultaneous measurements of black carbon (BC) and particle number size distribution of submicron <span class="hlt">aerosols</span> (PM1) were conducted at both locations. In the summer season emission from traffic related sources is expected to be the main local contribution to BC concentration. Concentrations of <span class="hlt">aerosol</span> species and gaseous pollutants within the planetary boundary layer are controlled by the balance between emission sources of primary <span class="hlt">aerosols</span> and gases, production of secondary <span class="hlt">aerosols</span>, chemical reactions of precursor gases under solar radiation and the rate of dilution by mixing within the planetary boundary layer (PBL) as well as with tropospheric air. Only local emission sources contribute to BC concentration during the stable PBL with low mixing layer <span class="hlt">height</span>, whereas during the time of fully mixed PBL, regionally transported BC and other <span class="hlt">aerosols</span> can contribute to the surface measurements. The study describes the diurnal behaviour of the submicron <span class="hlt">aerosol</span> at the urban and suburban background location under different weather regimes. Particles in three size modes - nucleation (< 25 nm, NUM), Aitken (25 - 90 nm, AIM) and accumulation mode (90 - 800 nm, ACM), as well as BC mass concentration were evaluated separately for sunny, cloudy and rainy days, taking into account modelled values of PBL <span class="hlt">height</span>. Higher particle number and black carbon concentrations were observed at the urban background (KIS) than at the suburban background location (Brezovica). Significant diurnal pattern of total particle concentration and black carbon concentration was observed at both</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.A41E..07K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.A41E..07K"><span>Natural and Anthropogenic <span class="hlt">Aerosols</span> in the World's Megacities and Climate Impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kafatos, M.; Singh, R.; El-Askary, H.; Qu, J.</p> <p>2005-12-01</p> <p> <span class="hlt">aerosols</span>. The highest boundary layer <span class="hlt">heights</span> are associated with regions where the sensible heat flux is greatest, and latent heat flux is smallest due to lack of vegetation. Boundary layer <span class="hlt">heights</span> in the deserts may be systematically higher than the slightly wetter regions at the edges of deserts. Latent heat flux model runs and MODIS observations of dust storms affecting the Nile Delta and Cairo indicate strong influence on the local weather and climate forcings. In the Indo-Gangetic, during the pre-monsoon period, dust storms form. We have examined SDS transport using RS data acquired from NASA's MODIS MISR instruments and from sun photometer measurements. The <span class="hlt">aerosol</span> optical depth and size of the dust particles are found to be significantly higher during such dust storm events. Moreover, our results clearly show that power plants in this region are the key point source of air pollutants. The detailed analysis of <span class="hlt">aerosol</span> parameters show the existence of absorbing and non-absorbing <span class="hlt">aerosols</span> emitted from these plants. The combined effects of urban <span class="hlt">aerosols</span> with dust <span class="hlt">aerosols</span> in India and Cairo not only affect megacities, they also have long-term climate impacts. We will also discuss how the assimilation of RS data into mesoscale models can improve these models and predictability of hazards and effects on megacities, such as SDS events, and forest fires, all sources of <span class="hlt">aerosols</span>. Therefore RS data can improve the prediction of climate forcings by <span class="hlt">aerosols</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.A41A0052N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.A41A0052N"><span>Characterization of Cooking-Related <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Niedziela, R. F.; Blanc, L. E.</p> <p>2010-12-01</p> <p>The temperatures at which food is cooked are usually high enough to drive oils and other organic compounds out of materials which are being prepared for consumption. As these compounds move away from the hot cooking surface and into the atmosphere, they can participate in chemical reactions or condense to form particles. Given the high concentration of cooking in urban areas, cooking-related <span class="hlt">aerosols</span> likely contribute to the overall amount of particulate matter on a local <span class="hlt">scale</span>. Reported here are results for the mid-infrared optical characterization of <span class="hlt">aerosols</span> formed during the cooking of several meat and vegetable samples in an inert atmosphere. The samples were heated in a novel <span class="hlt">aerosol</span> generator that is designed to collect particles formed immediately above the cooking surface and inject them into a laminar <span class="hlt">aerosol</span> flow cell. Preliminary results for the chemical processing of cooking-related <span class="hlt">aerosols</span> in synthetic air will also be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120015714','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120015714"><span>Satellite Perspective of <span class="hlt">Aerosol</span> Intercontinental Transport: From Qualitative Tracking to Quantitative Characterization</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, Hongbin; Remer, Lorraine A.; Kahn, Ralph A.; Chin, Mian; Zhang, Yan</p> <p>2012-01-01</p> <p>Evidence of <span class="hlt">aerosol</span> intercontinental transport (ICT) is both widespread and compelling. Model simulations suggest that ICT could significantly affect regional air quality and climate, but the broad inter-model spread of results underscores a need of constraining model simulations with measurements. Satellites have inherent advantages over in situ measurements to characterize <span class="hlt">aerosol</span> ICT, because of their spatial and temporal coverage. Significant progress in satellite remote sensing of <span class="hlt">aerosol</span> properties during the Earth Observing System (EOS) era offers opportunity to increase quantitative characterization and estimates of <span class="hlt">aerosol</span> ICT, beyond the capability of pre-EOS era satellites that could only qualitatively track <span class="hlt">aerosol</span> plumes. EOS satellites also observe emission strengths and injection <span class="hlt">heights</span> of some <span class="hlt">aerosols</span>, <span class="hlt">aerosol</span> precursors, and <span class="hlt">aerosol</span>-related gases, which can help characterize <span class="hlt">aerosol</span> ICT. After an overview of these advances, we review how the current generation of satellite measurements have been used to (1) characterize the evolution of <span class="hlt">aerosol</span> plumes (e.g., both horizontal and vertical transport, and properties) on an episodic basis, (2) understand the seasonal and inter-annual variations of <span class="hlt">aerosol</span> ICT and their control factors, (3) estimate the export and import fluxes of <span class="hlt">aerosols</span>, and (4) evaluate and constrain model simulations. Substantial effort is needed to further explore an integrated approach using measurements from on-orbit satellites (e.g., A-Train synergy) for observational characterization and model constraint of <span class="hlt">aerosol</span> intercontinental transport and to develop advanced sensors for future missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3845117','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3845117"><span>Microphysical effects determine macrophysical response for <span class="hlt">aerosol</span> impacts on deep convective clouds</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fan, Jiwen; Leung, L. Ruby; Rosenfeld, Daniel; Chen, Qian; Li, Zhanqing; Zhang, Jinqiang; Yan, Hongru</p> <p>2013-01-01</p> <p>Deep convective clouds (DCCs) play a crucial role in the general circulation, energy, and hydrological cycle of our climate system. <span class="hlt">Aerosol</span> particles can influence DCCs by altering cloud properties, precipitation regimes, and radiation balance. Previous studies reported both invigoration and suppression of DCCs by <span class="hlt">aerosols</span>, but few were concerned with the whole life cycle of DCC. By conducting multiple monthlong cloud-resolving simulations with spectral-bin cloud microphysics that capture the observed macrophysical and microphysical properties of summer convective clouds and precipitation in the tropics and midlatitudes, this study provides a comprehensive view of how <span class="hlt">aerosols</span> affect cloud cover, cloud top <span class="hlt">height</span>, and radiative forcing. We found that although the widely accepted theory of DCC invigoration due to aerosol’s thermodynamic effect (additional latent heat release from freezing of greater amount of cloud water) may work during the growing stage, it is microphysical effect influenced by <span class="hlt">aerosols</span> that drives the dramatic increase in cloud cover, cloud top <span class="hlt">height</span>, and cloud thickness at the mature and dissipation stages by inducing larger amounts of smaller but longer-lasting ice particles in the stratiform/anvils of DCCs, even when thermodynamic invigoration of convection is absent. The thermodynamic invigoration effect contributes up to ∼27% of total increase in cloud cover. The overall <span class="hlt">aerosol</span> indirect effect is an atmospheric radiative warming (3–5 W⋅m−2) and a surface cooling (−5 to −8 W⋅m−2). The modeling findings are confirmed by the analyses of ample measurements made at three sites of distinctly different environments. PMID:24218569</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080024015','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080024015"><span><span class="hlt">Aerosol</span> Profile Measurements from the NASA Langley Research Center Airborne High Spectral Resolution Lidar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Obland, Michael D.; Hostetler, Chris A.; Ferrare, Richard A.; Hair, John W.; Roers, Raymond R.; Burton, Sharon P.; Cook, Anthony L.; Harper, David B.</p> <p>2008-01-01</p> <p>Since achieving first light in December of 2005, the NASA Langley Research Center (LaRC) Airborne High Spectral Resolution Lidar (HSRL) has been involved in seven field campaigns, accumulating over 450 hours of science data across more than 120 flights. Data from the instrument have been used in a variety of studies including validation and comparison with the Cloud- <span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) satellite mission, <span class="hlt">aerosol</span> property retrievals combining passive and active instrument measurements, <span class="hlt">aerosol</span> type identification, <span class="hlt">aerosol</span>-cloud interactions, and cloud top and planetary boundary layer (PBL) <span class="hlt">height</span> determinations. Measurements and lessons learned from the HSRL are leading towards next-generation HSRL instrument designs that will enable even further studies of <span class="hlt">aerosol</span> intensive and extensive parameters and the effects of <span class="hlt">aerosols</span> on the climate system. This paper will highlight several of the areas in which the NASA Airborne HSRL is making contributions to climate science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1019187-downscaling-aerosols-impact-neglected-subgrid-processes-direct-aerosol-radiative-forcing-representative-global-climate-model-grid-spacing','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1019187-downscaling-aerosols-impact-neglected-subgrid-processes-direct-aerosol-radiative-forcing-representative-global-climate-model-grid-spacing"><span>Downscaling <span class="hlt">Aerosols</span> and the Impact of Neglected Subgrid Processes on Direct <span class="hlt">Aerosol</span> Radiative Forcing for a Representative Global Climate Model Grid Spacing</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, William I.; Qian, Yun; Fast, Jerome D.</p> <p>2011-07-13</p> <p>Recent improvements to many global climate models include detailed, prognostic <span class="hlt">aerosol</span> calculations intended to better reproduce the observed climate. However, the trace gas and <span class="hlt">aerosol</span> fields are treated at the grid-cell <span class="hlt">scale</span> with no attempt to account for sub-grid impacts on the <span class="hlt">aerosol</span> fields. This paper begins to quantify the error introduced by the neglected sub-grid variability for the shortwave <span class="hlt">aerosol</span> radiative forcing for a representative climate model grid spacing of 75 km. An analysis of the value added in downscaling <span class="hlt">aerosol</span> fields is also presented to give context to the WRF-Chem simulations used for the sub-grid analysis. We foundmore » that 1) the impact of neglected sub-grid variability on the <span class="hlt">aerosol</span> radiative forcing is strongest in regions of complex topography and complicated flow patterns, and 2) <span class="hlt">scale</span>-induced differences in emissions contribute strongly to the impact of neglected sub-grid processes on the <span class="hlt">aerosol</span> radiative forcing. The two of these effects together, when simulated at 75 km vs. 3 km in WRF-Chem, result in an average daytime mean bias of over 30% error in top-of-atmosphere shortwave <span class="hlt">aerosol</span> radiative forcing for a large percentage of central Mexico during the MILAGRO field campaign.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860020281','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860020281"><span>Chemical analysis of <span class="hlt">aerosol</span> in the Venusian cloud layer by reaction gas chromatography on board the Vega landers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gelman, B. G.; Drozdov, Y. V.; Melnikov, V. V.; Rotin, V. A.; Khokhlov, V. N.; Bondarev, V. B.; Dolnikov, G. G.; Dyachkov, A. V.; Nenarokov, D. F.; Mukhin, L. M.</p> <p>1986-01-01</p> <p>The experiment on sulfuric acid <span class="hlt">aerosol</span> determination in the Venusian cloud layer on board the Vega landers is described. An average content of sulfuric acid of approximately 1 mg/cu m was found for the samples taken from the atmosphere at <span class="hlt">heights</span> from 63 to 48 km and analyzed with the SIGMA-3 chromatograph. Sulfur dioxide (SO2) was revealed in the gaseous sample at the <span class="hlt">height</span> of 48 km. From the experimental results and blank run measurements, a suggestion is made that the Venusian cloud layer <span class="hlt">aerosol</span> consists of more complicated particles than the sulfuric acid water solution does.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130013402','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130013402"><span>Satellite Remote Sensing: <span class="hlt">Aerosol</span> Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kahn, Ralph A.</p> <p>2013-01-01</p> <p><span class="hlt">Aerosols</span> are solid or liquid particles suspended in the air, and those observed by satellite remote sensing are typically between about 0.05 and 10 microns in size. (Note that in traditional <span class="hlt">aerosol</span> science, the term "<span class="hlt">aerosol</span>" refers to both the particles and the medium in which they reside, whereas for remote sensing, the term commonly refers to the particles only. In this article, we adopt the remote-sensing definition.) They originate from a great diversity of sources, such as wildfires, volcanoes, soils and desert sands, breaking waves, natural biological activity, agricultural burning, cement production, and fossil fuel combustion. They typically remain in the atmosphere from several days to a week or more, and some travel great distances before returning to Earth's surface via gravitational settling or washout by precipitation. Many <span class="hlt">aerosol</span> sources exhibit strong seasonal variability, and most experience inter-annual fluctuations. As such, the frequent, global coverage that space-based <span class="hlt">aerosol</span> remote-sensing instruments can provide is making increasingly important contributions to regional and larger-<span class="hlt">scale</span> <span class="hlt">aerosol</span> studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A21D3057C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A21D3057C"><span>Estimation of global anthropogenic dust <span class="hlt">aerosol</span> using CALIOP satellite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, B.; Huang, J.; Liu, J.</p> <p>2014-12-01</p> <p>Anthropogenic dust <span class="hlt">aerosols</span> are those produced by human activity, which mainly come from cropland, pasture, and urban in this paper. Because understanding of the emissions of anthropogenic dust is still very limited, a new technique for separating anthropogenic dust from natural dustusing CALIPSO dust and planetary boundary layer <span class="hlt">height</span> retrievalsalong with a land use dataset is introduced. Using this technique, the global distribution of dust is analyzed and the relative contribution of anthropogenic and natural dust sources to regional and global emissions are estimated. Local anthropogenic dust <span class="hlt">aerosol</span> due to human activity, such as agriculture, industrial activity, transportation, and overgrazing, accounts for about 22.3% of the global continentaldust load. Of these anthropogenic dust <span class="hlt">aerosols</span>, more than 52.5% come from semi-arid and semi-wet regions. On the whole, anthropogenic dust emissions from East China and India are higher than other regions.</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('https://www.ncbi.nlm.nih.gov/pubmed/20119418','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20119418"><span>Degree and Direction of Polarization of Multiple Scattered Light. 2: Earth's Atmosphere with <span class="hlt">Aerosols</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Plass, G N; Kattawar, G W</p> <p>1972-12-01</p> <p>The degree of polarization as well as the direction of the polarization are calculated by a Monte Carlo method for the reflected and transmitted photons from the earth's atmosphere. The solar photons are followed through multiple collisions with the <span class="hlt">aerosols</span> and the Rayleigh scattering centers in the atmosphere. The <span class="hlt">aerosol</span> number density as well as the ratio of <span class="hlt">aerosol</span> to Rayleigh scattering vary with <span class="hlt">height</span>. The <span class="hlt">aerosol</span> index of refraction is assumed to be 1.55. The proportion of <span class="hlt">aerosol</span> to Rayleigh scattering is appropriately chosen at each wavelength (lambda = 0.4 micro and 0.7 micro); ozone absorption is included where appropriate. Three different <span class="hlt">aerosol</span> number densities are used to study the effects of <span class="hlt">aerosol</span> variations. Results are given for a solar zenith angle of 81.37 degrees and various surface albedos. The radiance and polarization of the reflected and transmitted photons is particularly sensitive to the amount of <span class="hlt">aerosols</span> in the atmosphere at certain angles of observation. The direction of pola ization shows little dependence on the surface albedo.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ACPD...1225389K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ACPD...1225389K"><span><span class="hlt">Aerosol</span> pollution potential from major population centers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kunkel, D.; Tost, H.; Lawrence, M. G.</p> <p>2012-09-01</p> <p>Major population centers (MPCs) or mega-cities represent the largest of growing urban agglomerations with major societal and environmental implications. In terms of air quality they are seen as localized but strong emission sources of <span class="hlt">aerosols</span> and trace gases which in turn affect air pollution levels in the city or in downwind regions. In the state-of-the-art atmospheric chemistry general circulation model EMAC, generic <span class="hlt">aerosol</span> and gas phase tracers with equal emission source strengths at 46 MPC locations are used to study the balance between local pollution build up and pollution export, either vertically into the upper troposphere or horizontally, but remaining in the lower atmosphere. The insoluble gas phase tracers with fixed lifetimes are transported with the atmospheric circulation, while the <span class="hlt">aerosol</span> tracers also undergo gravitational sedimentation as well as dry and wet deposition processes. The strength of low-level tracer export depends on the location of the emission source and prevailing meteorology, in particular on atmospheric stability and the <span class="hlt">height</span> of the boundary layer and the mixing out of this layer. In contrast, vertical transport of tracer mass depends on the tracer's solubility: the more soluble a tracer is the less mass reaches altitudes above five kilometers. Hence, the mass of insoluble gas phase tracer above five kilometers can be up to ten times higher than the hydrophilic <span class="hlt">aerosol</span> mass from the same source. In the case of <span class="hlt">aerosol</span> tracers, pollution build up around the source is determined by meteorological factors which have only indirect effects on tracer lifetime, like surface wind, boundary layer <span class="hlt">height</span>, and turbulent mixing as well as those which affect the lifetime of the tracers such as precipitation. The longer a tracer stays in the atmosphere, the lower is the relative importance of the location of the source to the atmospheric mass and thus the lower is the relative local pollution build up. We further use <span class="hlt">aerosol</span> deposition</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ACP....13.4203K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ACP....13.4203K"><span><span class="hlt">Aerosol</span> pollution potential from major population centers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kunkel, D.; Tost, H.; Lawrence, M. G.</p> <p>2013-04-01</p> <p>Major population centers (MPCs), or megacities, represent the largest of growing urban agglomerations with major societal and environmental implications. In terms of air quality, they are seen as localized but strong emission sources of <span class="hlt">aerosols</span> and trace gases which in turn affect air pollution levels in the city or in downwind regions. In the state-of-the-art atmospheric chemistry general circulation model EMAC, generic <span class="hlt">aerosol</span> and gas-phase tracers with equal emission source strengths at 46 MPC locations are used to study the balance between local pollution build-up and pollution export, either vertically into the upper troposphere or horizontally in the lower troposphere. The insoluble gas-phase tracers with fixed lifetimes are transported with the atmospheric circulation, while the <span class="hlt">aerosol</span> tracers also undergo gravitational sedimentation as well as dry and wet deposition processes. The strength of low-level tracer export depends on the location of the emission source and prevailing meteorology, in particular on atmospheric stability and the <span class="hlt">height</span> of the boundary layer and the mixing out of this layer. In contrast, vertical transport of tracer mass depends on the tracer's solubility: the more soluble a tracer is, the less mass reaches altitudes above five kilometers. Hence, the mass of insoluble gas-phase tracer above five kilometers can be up to ten times higher than the hydrophilic <span class="hlt">aerosol</span> mass from the same source. In the case of <span class="hlt">aerosol</span> tracers, pollution build-up around the source is determined by meteorological factors which have only indirect effects on tracer lifetime, like surface wind, boundary layer <span class="hlt">height</span>, and turbulent mixing, as well as those which affect the lifetime of the tracers such as precipitation. The longer a tracer stays in the atmosphere, the lower is the relative importance of the location of the source to the atmospheric mass, and thus the lower is the relative local pollution build-up. We further use <span class="hlt">aerosol</span> deposition fields to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.4513K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.4513K"><span>Probing into the aging dynamics of biomass burning <span class="hlt">aerosol</span> by using satellite measurements of <span class="hlt">aerosol</span> optical depth and carbon monoxide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Konovalov, Igor B.; Beekmann, Matthias; Berezin, Evgeny V.; Formenti, Paola; Andreae, Meinrat O.</p> <p>2017-04-01</p> <p>Carbonaceous <span class="hlt">aerosol</span> released into the atmosphere from open biomass burning (BB) is known to undergo considerable chemical and physical transformations (aging). However, there is substantial controversy about the nature and observable effects of these transformations. A shortage of consistent observational evidence on BB <span class="hlt">aerosol</span> aging processes under different environmental conditions and at various temporal <span class="hlt">scales</span> hinders development of their adequate representations in chemistry transport models (CTMs). In this study, we obtain insights into the BB <span class="hlt">aerosol</span> dynamics by using available satellite measurements of <span class="hlt">aerosol</span> optical depth (AOD) and carbon monoxide (CO). The basic concept of our method is to consider AOD as a function of the BB <span class="hlt">aerosol</span> <q>photochemical age</q> (that is, the time period characterizing the exposure of BB <span class="hlt">aerosol</span> emissions to atmospheric oxidation reactions) predicted by means of model tracers. We evaluate the AOD enhancement ratio (ER) defined as the ratio of optical depth of actual BB <span class="hlt">aerosol</span> with respect to that of a modeled <span class="hlt">aerosol</span> tracer that is assumed to originate from the same fires as the real BB <span class="hlt">aerosol</span> but that is not affected by any aging processes. To limit possible effects of model transport errors, the AOD measurements are normalized to CO column amounts that are also retrieved from satellite measurements. The method is applied to the analysis of the meso- and synoptic-<span class="hlt">scale</span> evolution of <span class="hlt">aerosol</span> in smoke plumes from major wildfires that occurred in Siberia in summer 2012. AOD and CO retrievals from MODIS and IASI measurements, respectively, are used in combination with simulations performed with the CHIMERE CTM. The analysis indicates that aging processes strongly affected the evolution of BB <span class="hlt">aerosol</span> in the situation considered, especially in dense plumes (with spatial average PM2. 5 concentration exceeding 100 µg m-3). For such plumes, the ER is found to increase almost 2-fold on the <span class="hlt">scale</span> of ˜ 10 h of daytime <span class="hlt">aerosol</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120012513','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120012513"><span><span class="hlt">Aerosol</span> Remote Sensing from AERONET, the Ground-Based Satellite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holben, Brent N.</p> <p>2012-01-01</p> <p>Atmospheric particles including mineral dust, biomass burning smoke, pollution from carbonaceous <span class="hlt">aerosols</span> and sulfates, sea salt, impact air quality and climate. The <span class="hlt">Aerosol</span> Robotic Network (AERONET) program, established in the early 1990s, is a federation of ground-based remote sensing <span class="hlt">aerosol</span> networks of Sun/sky radiometers distributed around the world, which provides a long-term, continuous and readily accessible public domain database of <span class="hlt">aerosol</span> optical (e.g., <span class="hlt">aerosol</span> optical depth) and microphysical (e.g., <span class="hlt">aerosol</span> volume size distribution) properties for <span class="hlt">aerosol</span> characterization, validation of satellite retrievals, and synergism with Earth science databases. Climatological <span class="hlt">aerosol</span> properties will be presented at key worldwide locations exhibiting discrete dominant <span class="hlt">aerosol</span> types. Further, AERONET's temporary mesoscale network campaign (e.g., UAE2, TIGERZ, DRAGON-USA.) results that attempt to quantify spatial and temporal variability of <span class="hlt">aerosol</span> properties, establish validation of ground-based <span class="hlt">aerosol</span> retrievals using aircraft profile measurements, and measure <span class="hlt">aerosol</span> properties on compatible spatial <span class="hlt">scales</span> with satellite retrievals and <span class="hlt">aerosol</span> transport models allowing for more robust validation will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130014342','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130014342"><span>Modeling of 2008 Kasatochi Volcanic Sulfate Direct Radiative Forcing: Assimilation of OMI SO2 Plume <span class="hlt">Height</span> Data and Comparison with MODIS and CALIOP Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wang, J.; Park, S.; Zeng, J.; Ge, C.; Yang, K.; Carn, S.; Krotkov, N.; Omar, A. H.</p> <p>2013-01-01</p> <p>Volcanic SO2 column amount and injection <span class="hlt">height</span> retrieved from the Ozone Monitoring Instrument (OMI) with the Extended Iterative Spectral Fitting (EISF) technique are used to initialize a global chemistry transport model (GEOS-Chem) to simulate the atmospheric transport and lifecycle of volcanic SO2 and sulfate <span class="hlt">aerosol</span> from the 2008 Kasatochi eruption, and to subsequently estimate the direct shortwave, top-of-the-atmosphere radiative forcing of the volcanic sulfate <span class="hlt">aerosol</span>. Analysis shows that the integrated use of OMI SO2 plume <span class="hlt">height</span> in GEOS-Chem yields: (a) good agreement of the temporal evolution of 3-D volcanic sulfate distributions between model simulations and satellite observations from the Moderate Resolution Imaging Spectroradiometer (MODIS) and Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarisation (CALIOP), and (b) an e-folding time for volcanic SO2 that is consistent with OMI measurements, reflecting SO2 oxidation in the upper troposphere and stratosphere is reliably represented in the model. However, a consistent (approx. 25 %) low bias is found in the GEOS-Chem simulated SO2 burden, and is likely due to a high (approx.20 %) bias of cloud liquid water amount (as compared to the MODIS cloud product) and the resultant stronger SO2 oxidation in the GEOS meteorological data during the first week after eruption when part of SO2 underwent aqueous-phase oxidation in clouds. Radiative transfer calculations show that the forcing by Kasatochi volcanic sulfate <span class="hlt">aerosol</span> becomes negligible 6 months after the eruption, but its global average over the first month is -1.3W/sq m, with the majority of the forcing-influenced region located north of 20degN, and with daily peak values up to -2W/sq m on days 16-17. Sensitivity experiments show that every 2 km decrease of SO2 injection <span class="hlt">height</span> in the GEOS-Chem simulations will result in a approx.25% decrease in volcanic sulfate forcing; similar sensitivity but opposite sign also holds for a 0.03 m increase of geometric radius of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A41K..01F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A41K..01F"><span>Evaluating <span class="hlt">Aerosol</span> Process Modules within the Framework of the <span class="hlt">Aerosol</span> Modeling Testbed</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fast, J. D.; Velu, V.; Gustafson, W. I.; Chapman, E.; Easter, R. C.; Shrivastava, M.; Singh, B.</p> <p>2012-12-01</p> <p>Factors that influence predictions of <span class="hlt">aerosol</span> direct and indirect forcing, such as <span class="hlt">aerosol</span> mass, composition, size distribution, hygroscopicity, and optical properties, still contain large uncertainties in both regional and global models. New <span class="hlt">aerosol</span> treatments are usually implemented into a 3-D atmospheric model and evaluated using a limited number of measurements from a specific case study. Under this modeling paradigm, the performance and computational efficiency of several treatments for a specific <span class="hlt">aerosol</span> process cannot be adequately quantified because many other processes among various modeling studies (e.g. grid configuration, meteorology, emission rates) are different as well. The scientific community needs to know the advantages and disadvantages of specific <span class="hlt">aerosol</span> treatments when the meteorology, chemistry, and other <span class="hlt">aerosol</span> processes are identical in order to reduce the uncertainties associated with <span class="hlt">aerosols</span> predictions. To address these issues, an <span class="hlt">Aerosol</span> Modeling Testbed (AMT) has been developed that systematically and objectively evaluates new <span class="hlt">aerosol</span> treatments for use in regional and global models. The AMT consists of the modular Weather Research and Forecasting (WRF) model, a series testbed cases for which extensive in situ and remote sensing measurements of meteorological, trace gas, and <span class="hlt">aerosol</span> properties are available, and a suite of tools to evaluate the performance of meteorological, chemical, <span class="hlt">aerosol</span> process modules. WRF contains various parameterizations of meteorological, chemical, and <span class="hlt">aerosol</span> processes and includes interactive <span class="hlt">aerosol</span>-cloud-radiation treatments similar to those employed by climate models. In addition, the physics suite from the Community Atmosphere Model version 5 (CAM5) have also been ported to WRF so that they can be tested at various spatial <span class="hlt">scales</span> and compared directly with field campaign data and other parameterizations commonly used by the mesoscale modeling community. Data from several campaigns, including the 2006</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACPD...1025759C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACPD...1025759C"><span>Estimating the atmospheric boundary layer <span class="hlt">height</span> over sloped, forested terrain from surface spectral analysis during BEARPEX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, W.; Faloona, I. C.; McKay, M.; Goldstein, A. H.; Baker, B.</p> <p>2010-11-01</p> <p>In this study the atmospheric boundary layer (ABL) <span class="hlt">height</span> (zi) over complex, forested terrain is estimated based on the power spectra and the integral length <span class="hlt">scale</span> of horizontal winds obtained from a three-axis sonic anemometer during the BEARPEX (Biosphere Effects on <span class="hlt">Aerosol</span> and Photochemistry) Experiment. The zi values estimated with this technique showed very good agreement with observations obtained from balloon tether sonde (2007) and rawinsonde (2009) measurements under unstable conditions (z/L < 0) at the coniferous forest in the California Sierra Nevada. The behavior of the nocturnal boundary layer <span class="hlt">height</span> (h) and power spectra of lateral winds and temperature under stable conditions (z/L > 0) is also presented. The nocturnal boundary layer <span class="hlt">height</span> is found to be fairly well predicted by a recent interpolation formula proposed by Zilitinkevich et al. (2007), although it was observed to only vary from 60-80 m during the experiment. Finally, significant directional wind shear was observed during both day and night with winds backing from the prevailing west-southwesterlies in the ABL (anabatic cross-valley circulation) to consistent southerlies in a layer ~1 km thick just above the ABL before veering to the prevailing westerlies further aloft. We show that this is consistent with the forcing of a thermal wind driven by the regional temperature gradient directed due east in the lower troposphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.17610005A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.17610005A"><span><span class="hlt">Aerosol</span> profiling during the large <span class="hlt">scale</span> field campaign CINDI-2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Apituley, Arnoud; Roozendael, Michel Van; Richter, Andreas; Wagner, Thomas; Friess, Udo; Hendrick, Francois; Kreher, Karin; Tirpitz, Jan-Lukas</p> <p>2018-04-01</p> <p>For the validation of space borne observations of NO2 and other trace gases from hyperspectral imagers, ground based instruments based on the MAXDOAS technique are an excellent choice, since they rely on similar retrieval techniques as the observations from orbit. To ensure proper traceability of the MAXDOAS observations, a thorough validation and intercomparison is mandatory. Advanced MAXDOAS observation and retrieval techniques enable inferring vertical structure of trace gases and <span class="hlt">aerosols</span>. These techniques and their results need validation by e.g. lidar techniques. For the proper understanding of the results from passive remote sensing techniques, independent observations are needed that include parameters needed to understand the light paths, i.e. in-situ <span class="hlt">aerosol</span> observations of optical and microphysical properties, and essential are in particular the vertical profiles of <span class="hlt">aerosol</span> optical properties by (Raman) lidar. The approach used in the CINDI-2 campaign held in Cabauw in 2016 is presented in this paper and the results will be discussed in the presentation at the conference.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRD..121.9814F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRD..121.9814F"><span>Model representations of <span class="hlt">aerosol</span> layers transported from North America over the Atlantic Ocean during the Two-Column <span class="hlt">Aerosol</span> Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fast, Jerome D.; Berg, Larry K.; Zhang, Kai; Easter, Richard C.; Ferrare, Richard A.; Hair, Johnathan W.; Hostetler, Chris A.; Liu, Ying; Ortega, Ivan; Sedlacek, Arthur; Shilling, John E.; Shrivastava, Manish; Springston, Stephen R.; Tomlinson, Jason M.; Volkamer, Rainer; Wilson, Jacqueline; Zaveri, Rahul A.; Zelenyuk, Alla</p> <p>2016-08-01</p> <p>The ability of the Weather Research and Forecasting model with chemistry (WRF-Chem) version 3.7 and the Community Atmosphere Model version 5.3 (CAM5) in simulating profiles of <span class="hlt">aerosol</span> properties is quantified using extensive in situ and remote sensing measurements from the Two-Column <span class="hlt">Aerosol</span> Project (TCAP) conducted during July of 2012. TCAP was supported by the U.S. Department of Energy's Atmospheric Radiation Measurement program and was designed to obtain observations within two atmospheric columns; one fixed over Cape Cod, Massachusetts, and the other several hundred kilometers over the ocean. The performance is quantified using most of the available aircraft and surface measurements during July, and 2 days are examined in more detail to identify the processes responsible for the observed <span class="hlt">aerosol</span> layers. The higher-resolution WRF-Chem model produced more <span class="hlt">aerosol</span> mass in the free troposphere than the coarser-resolution CAM5 model so that the fraction of <span class="hlt">aerosol</span> optical thickness above the residual layer from WRF-Chem was more consistent with lidar measurements. We found that the free troposphere layers are likely due to mean vertical motions associated with synoptic-<span class="hlt">scale</span> convergence that lifts <span class="hlt">aerosols</span> from the boundary layer. The vertical displacement and the time period associated with upward transport in the troposphere depend on the strength of the synoptic system and whether relatively high boundary layer <span class="hlt">aerosol</span> concentrations are present where convergence occurs. While a parameterization of subgrid <span class="hlt">scale</span> convective clouds applied in WRF-Chem modulated the concentrations of <span class="hlt">aerosols</span> aloft, it did not significantly change the overall altitude and depth of the layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21167877-artist-international-project-investigating-aerosol-retention-ruptured-steam-generator','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21167877-artist-international-project-investigating-aerosol-retention-ruptured-steam-generator"><span>ARTIST: An International Project Investigating <span class="hlt">Aerosol</span> Retention in a Ruptured Steam Generator</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>Guentay, S.; Dehbi, A.; Suckow, D.</p> <p>2002-07-01</p> <p>Steam generator tube ruptures (SGTR) with a concurrent stuck open safety relief valve are counted among the risk dominant accident sequences because of the potential for radioactive products to bypass the containment. Owing to the absence of relevant empirical data and the complexity of the geometry and controlling processes, the <span class="hlt">aerosol</span> removal in the steam generator (SG) tubes and in the secondary side is not well understood. Therefore, little or no credit is usually taken for <span class="hlt">aerosol</span> retention due to natural processes in the various components of a SG. To help reduce the uncertainties associated with fission product release followingmore » an SGTR sequence, the Paul Scherrer Institut has initiated an international experimental project to be performed in the ARTIST (<span class="hlt">AeRosol</span> Trapping In a Steam generaTor) facility in the time period from 2002 to 2007. The ARTIST test section is a <span class="hlt">scaled</span> model of a real SG, and is comprised of a 264-tube bundle with a maximum <span class="hlt">height</span> of 3.8 m, as well as one full-size droplet separator and one full-size steam dryer. The ARTIST facility is capable of producing soluble and insoluble <span class="hlt">aerosols</span> and entrain them at sonic gas flow rates (up to 0.25 kg/s, thus matching comparable values predicted by the codes. In addition, <span class="hlt">aerosols</span> can be generated at prototypical concentrations (up to 5 g/m{sup 3}) and sizes (0.2-5 mm AMMD). State of the art instrumentation is used (Low-pressure impactors, photometers, on-line particle sizer, online droplet sizer, etc.). The ARTIST project will simulate the flow and retention of <span class="hlt">aerosol</span>-borne fission products in the SG, and provide a unique database to support safety assessments and analytical models. The project is foreseen in seven phases: 1) <span class="hlt">Aerosol</span> retention in the tube under dry secondary side conditions, 2) <span class="hlt">Aerosol</span> retention in the near field close to break under dry conditions, 3) <span class="hlt">Aerosol</span> retention in the bundle far field under dry conditions, 4) <span class="hlt">Aerosol</span> retention in the separator and dryer under</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27553773','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27553773"><span>A predictive nondestructive model for the covariation of tree <span class="hlt">height</span>, diameter, and stem volume <span class="hlt">scaling</span> relationships.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Zhongrui; Zhong, Quanlin; Niklas, Karl J; Cai, Liang; Yang, Yusheng; Cheng, Dongliang</p> <p>2016-08-24</p> <p>Metabolic <span class="hlt">scaling</span> theory (MST) posits that the <span class="hlt">scaling</span> exponents among plant <span class="hlt">height</span> H, diameter D, and biomass M will covary across phyletically diverse species. However, the relationships between <span class="hlt">scaling</span> exponents and normalization constants remain unclear. Therefore, we developed a predictive model for the covariation of H, D, and stem volume V <span class="hlt">scaling</span> relationships and used data from Chinese fir (Cunninghamia lanceolata) in Jiangxi province, China to test it. As predicted by the model and supported by the data, normalization constants are positively correlated with their associated <span class="hlt">scaling</span> exponents for D vs. V and H vs. V, whereas normalization constants are negatively correlated with the <span class="hlt">scaling</span> exponents of H vs. D. The prediction model also yielded reliable estimations of V (mean absolute percentage error = 10.5 ± 0.32 SE across 12 model calibrated sites). These results (1) support a totally new covariation <span class="hlt">scaling</span> model, (2) indicate that differences in stem volume <span class="hlt">scaling</span> relationships at the intra-specific level are driven by anatomical or ecophysiological responses to site quality and/or management practices, and (3) provide an accurate non-destructive method for predicting Chinese fir stem volume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CosRe..56...85U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CosRe..56...85U"><span>Investigations of the Background Stratospheric <span class="hlt">Aerosol</span> Using Multicolor Wide-Angle Measurements of the Twilight Glow Background</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ugolnikov, O. S.; Maslov, I. A.</p> <p>2018-03-01</p> <p>The first results of multiwave measurements of twilight background and the all-sky camera with a color (RGB) CCD matrix conducted in the spring and summer of 2016 in Central Russia (55.2° N, 37.5° E) have been discussed. The observations reveal the effect of <span class="hlt">aerosol</span> scattering at <span class="hlt">heights</span> of up to 35 km, which is substantially enhanced in the long-wave part of the spectrum (R band with an effective wavelength of 624 nm). An analysis of the behavior of the sky color during light period of twilight with allowance for the absorption by ozone in the Chappuis bands make it possible to restore the angular dependences of the intensity of the <span class="hlt">aerosol</span> scattering of the light. This is used to determine the parameters of the lognormal distribution of <span class="hlt">aerosol</span> particles over their sizes with a mean radius of 0.08 μm and a width of 1.5-1.6 for the stratospheric <span class="hlt">height</span> interval.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMIN32A..02Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMIN32A..02Y"><span>Near Real Time Vertical Profiles of Clouds and <span class="hlt">Aerosols</span> from the Cloud-<span class="hlt">Aerosol</span> Transport System (CATS) on the International Space Station</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yorks, J. E.; McGill, M. J.; Nowottnick, E. P.</p> <p>2015-12-01</p> <p>Plumes from hazardous events, such as ash from volcanic eruptions and smoke from wildfires, can have a profound impact on the climate system, human health and the economy. Global <span class="hlt">aerosol</span> transport models are very useful for tracking hazardous plumes and predicting the transport of these plumes. However <span class="hlt">aerosol</span> vertical distributions and optical properties are a major weakness of global <span class="hlt">aerosol</span> transport models, yet a key component of tracking and forecasting smoke and ash. The Cloud-<span class="hlt">Aerosol</span> Transport System (CATS) is an elastic backscatter lidar designed to provide vertical profiles of clouds and <span class="hlt">aerosols</span> while also demonstrating new in-space technologies for future Earth Science missions. CATS has been operating on the Japanese Experiment Module - Exposed Facility (JEM-EF) of the International Space Station (ISS) since early February 2015. The ISS orbit provides more comprehensive coverage of the tropics and mid-latitudes than sun-synchronous orbiting sensors, with nearly a three-day repeat cycle. The ISS orbit also provides CATS with excellent coverage over the primary <span class="hlt">aerosol</span> transport tracks, mid-latitude storm tracks, and tropical convection. Data from CATS is used to derive properties of clouds and <span class="hlt">aerosols</span> including: layer <span class="hlt">height</span>, layer thickness, backscatter, optical depth, extinction, and depolarization-based discrimination of particle type. The measurements of atmospheric clouds and <span class="hlt">aerosols</span> provided by the CATS payload have demonstrated several science benefits. CATS provides near-real-time observations of cloud and <span class="hlt">aerosol</span> vertical distributions that can be used as inputs to global models. The infrastructure of the ISS allows CATS data to be captured, transmitted, and received at the CATS ground station within several minutes of data collection. The CATS backscatter and vertical feature mask are part of a customized near real time (NRT) product that the CATS processing team produces within 6 hours of collection. The continuous near real time CATS data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26SS....5...19Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26SS....5...19Z"><span>Negative <span class="hlt">Aerosol</span>-Cloud re Relationship From Aircraft Observations Over Hebei, China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Chuanfeng; Qiu, Yanmei; Dong, Xiaobo; Wang, Zhien; Peng, Yiran; Li, Baodong; Wu, Zhihui; Wang, Yang</p> <p>2018-01-01</p> <p>Using six flights observations in September 2015 over Hebei, China, this study shows a robust negative <span class="hlt">aerosol</span>-cloud droplet effective radius (<fi>r</fi><fi>e</fi>) relationship for liquid clouds, which is different from previous studies that found positive <span class="hlt">aerosol</span>-cloud <fi>r</fi><fi>e</fi> relationship over East China using satellite observations. A total of 27 cloud samples was analyzed with the classification of clean and polluted conditions using lower and upper 1/3 <span class="hlt">aerosol</span> concentration at 200 m below the cloud bases. By normalizing the profiles of cloud droplet <fi>r</fi><fi>e</fi>, we found significant smaller values under polluted than under clean condition at most <span class="hlt">heights</span>. Moreover, the averaged profiles of cloud liquid water content (LWC) show larger values under polluted than clean conditions, indicating even stronger negative <span class="hlt">aerosol</span>-cloud <fi>r</fi><fi>e</fi> relationship if LWC is kept constant. The droplet size distributions further demonstrate that more droplets concentrate within smaller size ranges under polluted conditions. Quantitatively, the <span class="hlt">aerosol</span>-cloud interaction is found around 0.10-0.19 for the study region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000052537&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D70%26Ntt%3DRussell','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000052537&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D70%26Ntt%3DRussell"><span>Measurements and Modeling of <span class="hlt">Aerosol</span> Absorption and Single Scattering Albedo at Ambient Relative Hum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Redemann, J.; Russell, P. B.; Hamill, P.</p> <p>2000-01-01</p> <p>Uncertainties in the <span class="hlt">aerosol</span> single scattering albedo have been identified to be an important source of errors in current large-<span class="hlt">scale</span> model estimates of the direct <span class="hlt">aerosol</span> radiative forcing of climate. A number of investigators have obtained estimates of the single scattering albedo from a variety of remote sensing and in situ measurements during <span class="hlt">aerosol</span> field experiments. During the Tropospheric <span class="hlt">Aerosol</span> Radiative Forcing Observational Experiment (TARFOX, 1996) for example, estimates of the <span class="hlt">aerosol</span> single scattering albedo were obtained (1) as a best-fit parameter in comparing radiative flux changes measured by airborne pyranometer to those computed from independently measured <span class="hlt">aerosol</span> properties; (2) from estimates of the <span class="hlt">aerosol</span> complex index of refraction derived using a combination of airborne sunphotometer, lidar backscatter and in situ size distribution measurements; and (3) from airborne measurements of <span class="hlt">aerosol</span> scattering and absorption using nephelometers and absorption photometers. In this paper, we briefly compare the results of the latter two methods for two TARFOX case studies, since those techniques provide <span class="hlt">height</span>-resolved information about the <span class="hlt">aerosol</span> single scattering albedo. Estimates of the <span class="hlt">aerosol</span> single scattering albedo from nephelometer and absorption photometer measurements require knowledge of the scattering and absorption humidification (i.e., the increase in these properties in response to an increase in ambient relative humidity), since both measurements are usually carried out at a relative humidity different from the ambient atmosphere. In principle, the scattering humidification factor can be measured, but there is currently no technique widely available to measure the absorption of an <span class="hlt">aerosol</span> sample as a function of relative humidity. Frequently, for lack of better knowledge, the absorption humidification is assumed to be unity (meaning that there is no change in <span class="hlt">aerosol</span> absorption due to an increase in ambient relative humidity). This</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1253673-indirect-semi-direct-aerosol-campaign-impact-arctic-aerosols-clouds','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1253673-indirect-semi-direct-aerosol-campaign-impact-arctic-aerosols-clouds"><span>Indirect and semi-direct <span class="hlt">aerosol</span> campaign: The impact of Arctic <span class="hlt">aerosols</span> on clouds</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>McFarquhar, Greg M.; Ghan, Steven; Verlinde, Johannes; ...</p> <p>2011-02-01</p> <p>A comprehensive dataset of microphysical and radiative properties of <span class="hlt">aerosols</span> and clouds in the boundary layer in the vicinity of Barrow, Alaska, was collected in April 2008 during the Indirect and Semi-Direct <span class="hlt">Aerosol</span> Campaign (ISDAC). ISDAC's primary aim was to examine the effects of <span class="hlt">aerosols</span>, including those generated by Asian wildfires, on clouds that contain both liquid and ice. ISDAC utilized the Atmospheric Radiation Measurement Pro- gram's permanent observational facilities at Barrow and specially deployed instruments measuring <span class="hlt">aerosol</span>, ice fog, precipitation, and radiation. The National Research Council of Canada Convair-580 flew 27 sorties and collected data using an unprecedented 41more » stateof- the-art cloud and <span class="hlt">aerosol</span> instruments for more than 100 h on 12 different days. <span class="hlt">Aerosol</span> compositions, including fresh and processed sea salt, biomassburning particles, organics, and sulfates mixed with organics, varied between flights. Observations in a dense arctic haze on 19 April and above, within, and below the single-layer stratocumulus on 8 and 26 April are enabling a process-oriented understanding of how <span class="hlt">aerosols</span> affect arctic clouds. Inhomogeneities in reflectivity, a close coupling of upward and downward Doppler motion, and a nearly constant ice profile in the single-layer stratocumulus suggests that vertical mixing is responsible for its longevity observed during ISDAC. Data acquired in cirrus on flights between Barrow and Fairbanks, Alaska, are improving the understanding of the performance of cloud probes in ice. Furthermore, ISDAC data will improve the representation of cloud and <span class="hlt">aerosol</span> processes in models covering a variety of spatial and temporal <span class="hlt">scales</span>, and determine the extent to which surface measurements can provide retrievals of <span class="hlt">aerosols</span>, clouds, precipitation, and radiative heating.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28630907','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28630907"><span>Wind-invariant saltation <span class="hlt">heights</span> imply linear <span class="hlt">scaling</span> of aeolian saltation flux with shear stress.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martin, Raleigh L; Kok, Jasper F</p> <p>2017-06-01</p> <p>Wind-driven sand transport generates atmospheric dust, forms dunes, and sculpts landscapes. However, it remains unclear how the flux of particles in aeolian saltation-the wind-driven transport of sand in hopping trajectories-<span class="hlt">scales</span> with wind speed, largely because models do not agree on how particle speeds and trajectories change with wind shear velocity. We present comprehensive measurements, from three new field sites and three published studies, showing that characteristic saltation layer <span class="hlt">heights</span> remain approximately constant with shear velocity, in agreement with recent wind tunnel studies. These results support the assumption of constant particle speeds in recent models predicting linear <span class="hlt">scaling</span> of saltation flux with shear stress. In contrast, our results refute widely used older models that assume that particle speed increases with shear velocity, thereby predicting nonlinear 3/2 stress-flux <span class="hlt">scaling</span>. This conclusion is further supported by direct field measurements of saltation flux versus shear stress. Our results thus argue for adoption of linear saltation flux laws and constant saltation trajectories for modeling saltation-driven aeolian processes on Earth, Mars, and other planetary surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5462498','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5462498"><span>Wind-invariant saltation <span class="hlt">heights</span> imply linear <span class="hlt">scaling</span> of aeolian saltation flux with shear stress</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Martin, Raleigh L.; Kok, Jasper F.</p> <p>2017-01-01</p> <p>Wind-driven sand transport generates atmospheric dust, forms dunes, and sculpts landscapes. However, it remains unclear how the flux of particles in aeolian saltation—the wind-driven transport of sand in hopping trajectories—<span class="hlt">scales</span> with wind speed, largely because models do not agree on how particle speeds and trajectories change with wind shear velocity. We present comprehensive measurements, from three new field sites and three published studies, showing that characteristic saltation layer <span class="hlt">heights</span> remain approximately constant with shear velocity, in agreement with recent wind tunnel studies. These results support the assumption of constant particle speeds in recent models predicting linear <span class="hlt">scaling</span> of saltation flux with shear stress. In contrast, our results refute widely used older models that assume that particle speed increases with shear velocity, thereby predicting nonlinear 3/2 stress-flux <span class="hlt">scaling</span>. This conclusion is further supported by direct field measurements of saltation flux versus shear stress. Our results thus argue for adoption of linear saltation flux laws and constant saltation trajectories for modeling saltation-driven aeolian processes on Earth, Mars, and other planetary surfaces. PMID:28630907</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmEn.158..236C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmEn.158..236C"><span>Time-resolved analysis of primary volatile emissions and secondary <span class="hlt">aerosol</span> formation potential from a small-<span class="hlt">scale</span> pellet boiler</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Czech, Hendryk; Pieber, Simone M.; Tiitta, Petri; Sippula, Olli; Kortelainen, Miika; Lamberg, Heikki; Grigonyte, Julija; Streibel, Thorsten; Prévôt, André S. H.; Jokiniemi, Jorma; Zimmermann, Ralf</p> <p>2017-06-01</p> <p>Small-<span class="hlt">scale</span> pellet boilers and stoves became popular as a wood combustion appliance for domestic heating in Europe, North America and Asia due to economic and environmental aspects. Therefore, an increasing contribution of pellet boilers to air pollution is expected despite their general high combustion efficiency. As emissions of primary organic <span class="hlt">aerosol</span> (POA) and permanent gases of pellet boilers are well investigated, the scope of this study was to investigate the volatile organic emissions and the formation potential of secondary <span class="hlt">aerosols</span> for this type of appliance. Fresh and aged emissions were analysed by a soot-particle <span class="hlt">aerosol</span> time-of-flight mass spectrometry (SP-AMS) and the molecular composition of the volatile precursors with single-photon ionisation time-of-flight mass spectrometry (SPI-TOFMS) at different pellet boiler operation conditions. Organic emissions in the gas phase were dominated by unsaturated hydrocarbons while wood-specific VOCs, e.g. phenolic species or substituted furans, were only detected during the starting phase. Furthermore, organic emissions in the gas phase were found to correlate with fuel grade and combustion technology in terms of secondary air supply. Secondary organic <span class="hlt">aerosols</span> of optimised pellet boiler conditions (OPT, state-of-the-art combustion appliance) and reduced secondary air supply (RSA, used as a proxy for pellet boilers of older type) were studied by simulating atmospheric ageing in a Potential <span class="hlt">Aerosol</span> Mass (PAM) flow reactor. Different increases in OA mass (55% for OPT, 102% for RSA), associated with higher average carbon oxidation state and O:C, could be observed in a PAM chamber experiment. Finally, it was found that derived SOA yields and emission factors were distinctly lower than reported for log wood stoves.</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/2006AGUFM.A32A..06M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.A32A..06M"><span>Long-term <span class="hlt">Aerosol</span> Lidar Measurements At CNR-IMAA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mona, L.; Amodeo, A.; D'Amico, G.; Pandolfi, M.; Pappalardo, G.</p> <p>2006-12-01</p> <p>Actual estimations of the <span class="hlt">aerosol</span> effect on the radiation budget are affected by a large uncertainties mainly due to the high inhomogeneity and variability of atmospheric <span class="hlt">aerosol</span>, in terms of concentration, shape, size distribution, refractive index and vertical distribution. Long-term measurements of vertical profiles of <span class="hlt">aerosol</span> optical properties are needed to reduce these uncertainties. At CNR-IMAA (40° 36'N, 15° 44' E, 760 m above sea level), a lidar system for <span class="hlt">aerosol</span> study is operative since May 2000 in the framework of EARLINET (European <span class="hlt">Aerosol</span> Research Lidar Network). Until August 2005, it provided independent measurements of <span class="hlt">aerosol</span> extinction and backscatter at 355 nm and <span class="hlt">aerosol</span> backscatter profiles at 532 nm. After an upgrade of the system, it provides independent measurements of <span class="hlt">aerosol</span> extinction and backscatter profiles at 355 and 532 nm, and of <span class="hlt">aerosol</span> backscatter profiles at 1064 nm and depolarization ratio at 532 nm. For these measurements, lidar ratio at 355 and 532 nm and Angstrom exponent profiles at 355/532 nm are also obtained. Starting on May 2000, systematic measurements are performed three times per week according to the EARLINET schedule and further measurements are performed in order to investigate particular events, like dust intrusions, volcanic eruptions and forest fires. A climatological study has been carried out in terms of the seasonal behavior of the PBL <span class="hlt">height</span> and of the <span class="hlt">aerosol</span> optical properties calculated inside the PBL itself. In the free troposphere, an high occurrences of Saharan dust intrusions (about 1 day of Saharan dust intrusion every 10 days) has been observed at CNR-IMAA because of the short distance from the Sahara region. During 6 years of observations, very peculiar cases of volcanic <span class="hlt">aerosol</span> emitted by Etna volcano and <span class="hlt">aerosol</span> released by large forest fires burning occurred in Alaska and Canada have been observed in the free troposphere at our site. Particular attention is devoted to lidar ratio both for the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1346557','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1346557"><span>Campaign datasets for Two-Column <span class="hlt">Aerosol</span> Project (TCAP)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Berg,Larry; Mei,Fan; Cairns,Brian; Chand,Duli; Comstock,Jennifer; Cziczo,Daniel; Hostetler,Chris; Hubbe,John; Long,Chuck; Michalsky,Joseph; Pekour,Mikhail; Russell,Phil; Scott,Herman; Sedlacek,Arthur; Shilling,John; Springston,Stephen; Tomlinson,Jason; Watson,Thomas; Zelenyuk-Imre,Alla</p> <p>2013-12-30</p> <p>This campaign was designed to provide a detailed set of observations with which to 1) perform radiative and cloud condensation nuclei (CCN) closure studies, 2) evaluate a new retrieval algorithm for <span class="hlt">aerosol</span> optical depth (AOD) in the presence of clouds using passive remote sensing 3) extend a previously developed technique to investigate <span class="hlt">aerosol</span> indirect effects, and 4) evaluate the performance of a detailed regional-<span class="hlt">scale</span> model and a more parameterized global-<span class="hlt">scale</span> model in simulating particle activation and AOD associated with the aging of anthropogenic <span class="hlt">aerosols</span>. To meet these science objectives, the ARM Mobile Facility (AMF) and the Mobile <span class="hlt">Aerosol</span> Observing System (MAOS) was deployed on Cape Cod, Massachusetts for a 12-month period starting in the summer of 2012 in order to quantify <span class="hlt">aerosol</span> properties, radiation and cloud characteristics at a location subject to both clear- and cloudy- conditions, and clean- and polluted-conditions. These observations were supplemented by two aircraft intensive observation periods (IOPS), one in the summer and a second in the winter. Each IOP required two aircraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000013616&hterms=four+seasons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfour%2Bseasons','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000013616&hterms=four+seasons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dfour%2Bseasons"><span>Global <span class="hlt">Aerosol</span> Radiative Forcing Derived from Sea WiFS-Inferred <span class="hlt">Aerosol</span> Optical Properties</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chou, Ming-Dah; Chan, Pui-King; Wang, Menghua</p> <p>1999-01-01</p> <p><span class="hlt">Aerosol</span> optical properties inferred from the Sea-viewing Wide Field-of-view Sensor (SeaWiFS) radiance measurements are used to compute the <span class="hlt">aerosol</span> shortwave radiative forcing using a radiative transfer model. The <span class="hlt">aerosol</span> optical thickness at the wavelength of 865-nm is taken from the SeaWIFS archive. It is found that the nominal optical thickness over oceans ranges from 0.1 to 0.2. Using a maritime <span class="hlt">aerosol</span> model and the radiances measured at the various SeaWiFS channels, the Angstrom exponent is determined to be 0.2174, the single-scattering albedo to be 0.995, and the asymmetry factor to be 0.786. The radiative transfer model has eight bands in the visible and ultraviolet spectral regions and three bands in the near infrared. It includes the absorption due to <span class="hlt">aerosols</span>, water vapor, carbon dioxide, and oxygen, and the scattering due to <span class="hlt">aerosols</span> and gases (Rayleigh scattering). The radiative forcing is computed over global oceans for four months (January, April, July, and October, 1998) to represent four seasons. It is found that the <span class="hlt">aerosol</span> radiative forcing is large and changes significantly with seasons near the continents with large-<span class="hlt">scale</span> forest fires and desert dust. Averaged over oceans and the four months, the <span class="hlt">aerosol</span> radiative forcing is approximately 7 W/sq m at the top of the atmosphere. This large radiative forcing is expected to have a significant cooling effect on the Earth's climate as implied from simulations of a number of general circulation models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150021891&hterms=remote+sensing&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dremote%2Bsensing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150021891&hterms=remote+sensing&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dremote%2Bsensing"><span>Remote Sensing of <span class="hlt">Aerosol</span> in the Terrestrial Atmosphere from Space: New Missions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Milinevsky, G.; Yatskiv, Ya.; Degtyaryov, O.; Syniavskyi, I.; Ivanov, Yu.; Bovchaliuk, A.; Mishchenko, M.; Danylevsky, V.; Sosonkin, M.; Bovchaliuk, V.</p> <p>2015-01-01</p> <p>The distribution and properties of atmospheric <span class="hlt">aerosols</span> on a global <span class="hlt">scale</span> are not well known in terms of determination of their effects on climate. This mostly is due to extreme variability of <span class="hlt">aerosol</span> concentrations, properties, sources, and types. <span class="hlt">Aerosol</span> climate impact is comparable to the effect of greenhouse gases, but its influence is more difficult to measure, especially with respect to <span class="hlt">aerosol</span> microphysical properties and the evaluation of anthropogenic <span class="hlt">aerosol</span> effect. There are many satellite missions studying <span class="hlt">aerosol</span> distribution in the terrestrial atmosphere, such as MISR/Terra, OMI/Aura, AVHHR, MODIS/Terra and Aqua, CALIOP/CALIPSO. To improve the quality of data and climate models, and to reduce <span class="hlt">aerosol</span> climate forcing uncertainties, several new missions are planned. The gap in orbital instruments for studying <span class="hlt">aerosol</span> microphysics has arisen after the Glory mission failed during launch in 2011. In this review paper, we describe several planned <span class="hlt">aerosol</span> space missions, including the Ukrainian project <span class="hlt">Aerosol</span>-UA that obtains data using a multi-channel scanning polarimeter and wide-angle polarimetric camera. The project is designed for remote sensing of the <span class="hlt">aerosol</span> microphysics and cloud properties on a global <span class="hlt">scale</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4601626','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4601626"><span>Surfactant Driven Post-Deposition Spreading of <span class="hlt">Aerosols</span> on Complex Aqueous Subphases. 2: Low Deposition Flux Representative of <span class="hlt">Aerosol</span> Delivery to Small Airways</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sharma, Ramankur; Khanal, Amsul; Corcoran, Timothy E.; Przybycien, Todd M.; Tilton, Robert D.</p> <p>2015-01-01</p> <p>Abstract Background: Cystic fibrosis (CF) is associated with the accumulation of dehydrated mucus in the pulmonary airways. This alters ventilation and <span class="hlt">aerosol</span> deposition patterns in ways that limit drug delivery to peripheral lung regions. We investigated the use of surfactant-based, self-dispersing <span class="hlt">aerosol</span> carriers that produce surface tension gradients to drive two-dimensional transport of <span class="hlt">aerosolized</span> medications via Marangoni flows after deposition on the airway surface liquid (ASL). We considered the post-deposition spreading of individual <span class="hlt">aerosol</span> droplets and two-dimensional expansion of a field of <span class="hlt">aerosol</span> droplets, when deposited at low fluxes that are representative of <span class="hlt">aerosol</span> deposition in the small airways. Methods: We used physically entangled aqueous solutions of poly(acrylamide) or porcine gastric mucin as simple ASL mimics that adequately capture the full miscibility but slow penetration of entangled macromolecular chains of the ASL into the deposited drop. Surfactant formulations were prepared with aqueous solutions of nonionic tyloxapol or FS-3100 fluorosurfactant. Fluorescein dye served as a model “drug” tracer and to visualize the extent of post-deposition spreading. Results: The surfactants not only enhanced post-deposition spreading of individual <span class="hlt">aerosol</span> droplets due to localized Marangoni stresses, as previously observed with macroscopic drops, but they also produced large-<span class="hlt">scale</span> Marangoni stresses that caused the deposited <span class="hlt">aerosol</span> fields to expand into initially unexposed regions of the subphase. We show that the latter is the main mechanism for spreading drug over large distances when <span class="hlt">aerosol</span> is deposited at low fluxes representative of the small airways. The large <span class="hlt">scale</span> convective expansion of the <span class="hlt">aerosol</span> field drives the tracer (drug mimic) over areas that would cover an entire airway generation or more, in peripheral airways, where sub-monolayer droplet deposition is expected during <span class="hlt">aerosol</span> inhalation. Conclusions: The results suggest</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AtmEn.159...26C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AtmEn.159...26C"><span>Estimation of surface-level PM2.5 concentration using <span class="hlt">aerosol</span> optical thickness through <span class="hlt">aerosol</span> type analysis 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, Qi-Xiang; Yuan, Yuan; Huang, Xing; Jiang, Yan-Qiu; Tan, He-Ping</p> <p>2017-06-01</p> <p>Surface-level particulate matter is closely related to column <span class="hlt">aerosol</span> optical thickness (AOT). Previous researches have successfully used column AOT and different meteorological parameters to estimate surface-level PM concentration. In this study, the performance of a selected linear model that estimates surface-level PM2.5 concentration was evaluated following the <span class="hlt">aerosol</span> type analysis method (ATAM) for the first time. We utilized 443 daily average data for Xuzhou, Jiangsu province, collected using <span class="hlt">Aerosol</span> Robotic Network (AERONET) during the period October 2013 to April 2016. Several parameters including atmospheric boundary layer <span class="hlt">height</span> (BLH), relative humidity (RH), and effective radius of the <span class="hlt">aerosol</span> size distribution (Ref) were used to assess the relationship between the column AOT and PM2.5 concentration. By including the BLH, ambient RH, and effective radius, the correlation (R2) increased from 0.084 to 0.250 at Xuzhou, and with the use of ATAM, the correlation increased further to 0.335. To compare the results, 450 daily average data for Beijing, pertaining to the same period, were utilized. The study found that model correlations improved by varying degrees in different seasons and at different sites following ATAM. The average urban industry (UI) <span class="hlt">aerosol</span> ratios at Xuzhou and Beijing were 0.792 and 0.451, respectively, demonstrating poorer air conditions at Xuzhou. PM2.5 estimation at Xuzhou showed lower correlation (R2 = 0.335) compared to Beijing (R2 = 0.407), and the increase of R2 at Xuzhou and Beijing site following use of ATAM were 33.8% and 12.4%, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A53F2314H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A53F2314H"><span>An increase in <span class="hlt">aerosol</span> burden due to the land-sea warming contrast</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hassan, T.; Allen, R.; Randles, C. A.</p> <p>2017-12-01</p> <p>Climate models simulate an increase in most <span class="hlt">aerosol</span> species in response to warming, particularly over the tropics and Northern Hemisphere midlatitudes. This increase in <span class="hlt">aerosol</span> burden is related to a decrease in wet removal, primarily due to reduced large-<span class="hlt">scale</span> precipitation. Here, we show that the increase in <span class="hlt">aerosol</span> burden, and the decrease in large-<span class="hlt">scale</span> precipitation, is related to a robust climate change phenomenon—the land/sea warming contrast. Idealized simulations with two state of the art climate models, the National Center for Atmospheric Research Community Atmosphere Model version 5 (NCAR CAM5) and the Geophysical Fluid Dynamics Laboratory Atmospheric Model 3 (GFDL AM3), show that muting the land-sea warming contrast negates the increase in <span class="hlt">aerosol</span> burden under warming. This is related to smaller decreases in near-surface relative humidity over land, and in turn, smaller decreases in large-<span class="hlt">scale</span> precipitation over land—especially in the NH midlatitudes. Furthermore, additional idealized simulations with an enhanced land/sea warming contrast lead to the opposite result—larger decreases in relative humidity over land, larger decreases in large-<span class="hlt">scale</span> precipitation, and larger increases in <span class="hlt">aerosol</span> burden. Our results, which relate the increase in <span class="hlt">aerosol</span> burden to the robust climate projection of enhanced land warming, adds confidence that a warmer world will be associated with a larger <span class="hlt">aerosol</span> burden.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AtmRe..74..581Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AtmRe..74..581Z"><span>Ceilometer observations of <span class="hlt">aerosol</span> layer structure above the Petit Lubéron during ESCOMPTE's IOP 2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zéphoris, Marcel; Holin, Hubert; Lavie, Franck; Cenac, Nadine; Cluzeau, Michel; Delas, Olivier; Eideliman, Françoise; Gagneux, Jacqueline; Gander, Alain; Thibord, Corinne</p> <p>2005-03-01</p> <p>A modified ceilometer has been used during the second Intensive Observation Period (IOP) of the "Expérience sur Site pour COntraindre les Modèles de Pollution atmosphériques et de Transport d'Émission" (ESCOMPTE) to perform continuous remote observations of <span class="hlt">aerosol</span> accumulations in the first 3 km of the atmosphere. These observations encompassed an episode of intense particulate and photochemical pollution. The submicronic particles density, measured at an altitude of 600 m, went from a very low point of a few tens of particles per cubic centimeter (at the end of a Mistral episode in the free atmosphere) to a high point of more than 4500 particles per cubic centimeter (when pollutants were trapped by thermal inversions). The main result is that this instrument enables a fine documentation of the mixing layer <span class="hlt">height</span> and of <span class="hlt">aerosol</span> particles stratifications and circulation. Airborne <span class="hlt">aerosol</span> measurements have been made above the mountainous region of Mérindol in order to validate in situ the remote sensing measurements. Ozone measurements near the summit of the mountains as well as in the valley were performed in order to correlate <span class="hlt">aerosol</span> accumulation and ozone concentration. As a notable example, the two-layer <span class="hlt">aerosol</span> stratification seen in the first 2 days of IOP 2b in that part of the ESCOMPTE domain confirms the results of another team which used backtrajectories. The low-altitude pollution for this timeframe had a local origin (the Fos industrial area), whereas above 500 m, the air masses had undergone regional-<span class="hlt">scale</span> transport (from north-eastern Spain). The second major result is the highlighting of a pattern, in sea breeze conditions and in this part of the ESCOMPTE experiment zone, of nocturnal <span class="hlt">aerosol</span> accumulation at an altitude of between 500 and 2000 m, followed by high ozone concentration the next day.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.7368G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.7368G"><span>Absolute calibration of the Jenoptik CHM15k-x ceilometer and its applicability for quantitative <span class="hlt">aerosol</span> monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Geiß, Alexander; Wiegner, Matthias</p> <p>2014-05-01</p> <p>The knowledge of the spatiotemporal distribution of atmospheric <span class="hlt">aerosols</span> and its optical characterization is essential for the understanding of the radiation budget, air quality, and climate. For this purpose, lidar is an excellent system as it is an active remote sensing technique. As multi-wavelength research lidars with depolarization channels are quite complex and cost-expensive, increasing attention is paid to so-called ceilometers. They are simple one-wavelength backscatter lidars with low pulse energy for eye-safe operation. As maintenance costs are low and continuous and unattended measurements can be performed, they are suitable for long-term <span class="hlt">aerosol</span> monitoring in a network. However, the signal-to-noise ratio is low, and the signals are not calibrated. The only optical property that can be derived from a ceilometer is the particle backscatter coefficient, but even this quantity requires a calibration of the signals. With four years of measurements from a Jenoptik ceilometer CHM15k-x, we developed two methods for an absolute calibration on this system. This advantage of our approach is that only a few days with favorable meteorological conditions are required where Rayleigh-calibration and comparison with our research lidar is possible to estimate the lidar constant. This method enables us to derive the particle backscatter coefficient at 1064 nm, and we retrieved for the first time profiles in near real-time within an accuracy of 10 %. If an appropriate lidar ratio is assumed the <span class="hlt">aerosol</span> optical depth of e.g. the mixing layer can be determined with an accuracy depending on the accuracy of the lidar ratio estimate. Even for 'simple' applications, e.g. assessment of the mixing layer <span class="hlt">height</span>, cloud detection, detection of elevated <span class="hlt">aerosol</span> layers, the particle backscatter coefficient has significant advantages over the measured (uncalibrated) attenuated backscatter. The possibility of continuous operation under nearly any meteorological condition with temporal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120009892','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009892"><span>Comparative Study of <span class="hlt">Aerosol</span> and Cloud Detected by CALIPSO and OMI</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chen, Zhong; Torres, Omar; McCormick, M. Patrick; Smith, William; Ahn, Changwoo</p> <p>2012-01-01</p> <p>The Ozone Monitoring Instrument (OMI) on the Aura Satellite detects the presence of desert dust and smoke particles (also known as <span class="hlt">aerosols</span>) in terms of a parameter known as the UV <span class="hlt">Aerosol</span> Index (UV AI). The Cloud-<span class="hlt">Aerosol</span> Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) mission measures the vertical distribution of <span class="hlt">aerosols</span> and clouds. <span class="hlt">Aerosols</span> and clouds play important roles in the atmosphere and climate system. Accurately detecting their presence, altitude, and properties using satellite radiance measurements is a very important task. This paper presents a comparative analysis of the CALIPSO Version 2 Vertical Feature Mask (VFM) product with the (OMI) UV <span class="hlt">Aerosol</span> Index (UV AI) and reflectivity datasets for a full year of 2007. The comparison is done at regional and global <span class="hlt">scales</span>. Based on CALIPSO arid OMI observations, the vertical and horizontal extent of clouds and <span class="hlt">aerosols</span> are determined and the effects of <span class="hlt">aerosol</span> type selection, load, cloud fraction on <span class="hlt">aerosol</span> identification are discussed. It was found that the spatial-temporal correlation found between CALIPSO and OMI observations, is strongly dependent on <span class="hlt">aerosol</span> types and cloud contamination. CALIPSO is more sensitivity to cloud and often misidentifies desert dust <span class="hlt">aerosols</span> as cloud, while some small <span class="hlt">scale</span> <span class="hlt">aerosol</span> layers as well as some pollution <span class="hlt">aerosols</span> are unidentified by OMI UV AI. Large differences in <span class="hlt">aerosol</span> distribution patterns between CALIPSO and OMI are observed, especially for the smoke and pollution <span class="hlt">aerosol</span> dominated areas. In addition, the results found a significant correlation between CALIPSO lidar 1064 nm backscatter and the OMI UV AI over the study regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1340781-model-representations-aerosol-layers-transported-from-north-america-over-atlantic-ocean-during-two-column-aerosol-project','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1340781-model-representations-aerosol-layers-transported-from-north-america-over-atlantic-ocean-during-two-column-aerosol-project"><span>Model representations of <span class="hlt">aerosol</span> layers transported from North America over the Atlantic Ocean during the Two-Column <span class="hlt">Aerosol</span> Project</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>Fast, Jerome D.; Berg, Larry K.; Zhang, Kai</p> <p>2016-08-22</p> <p>The ability of the Weather Research and Forecasting model with chemistry (WRF-Chem) version 3.7 and the Community Atmosphere Model version 5.3 (CAM5) in simulating profiles of <span class="hlt">aerosol</span> properties is quantified using extensive in situ and remote sensing measurements from the Two Column <span class="hlt">Aerosol</span> Project (TCAP) conducted during July of 2012. TCAP was supported by the U.S. Department of Energy’s Atmospheric Radiation Measurement program and was designed to obtain observations within two atmospheric columns; one fixed over Cape Cod, Massachusetts and the other several hundred kilometers over the ocean. The performance is quantified using most of the available aircraft and surfacemore » measurements during July, and two days are examined in more detail to identify the processes responsible for the observed <span class="hlt">aerosol</span> layers. The higher resolution WRF-Chem model produced more <span class="hlt">aerosol</span> mass in the free troposphere than the coarser resolution CAM5 model so that the fraction of <span class="hlt">aerosol</span> optical thickness above the residual layer from WRF-Chem was more consistent with lidar measurements. We found that the free troposphere layers are likely due to mean vertical motions associated with synoptic-<span class="hlt">scale</span> convergence that lifts <span class="hlt">aerosols</span> from the boundary layer. The vertical displacement and the time period associated with upward transport in the troposphere depend on the strength of the synoptic system and whether relatively high boundary layer <span class="hlt">aerosol</span> concentrations are present where convergence occurs. While a parameterization of subgrid <span class="hlt">scale</span> convective clouds applied in WRF-Chem modulated the concentrations of <span class="hlt">aerosols</span> aloft, it did not significantly change the overall altitude and depth of the layers.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1331075-model-representations-aerosol-layers-transported-from-north-america-over-atlantic-ocean-during-two-column-aerosol-project','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1331075-model-representations-aerosol-layers-transported-from-north-america-over-atlantic-ocean-during-two-column-aerosol-project"><span>Model representations of <span class="hlt">aerosol</span> layers transported from North America over the Atlantic Ocean during the Two-Column <span class="hlt">Aerosol</span> Project</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fast, Jerome D.; Berg, Larry K.; Zhang, Kai; ...</p> <p>2016-08-22</p> <p>The ability of the Weather Research and Forecasting model with chemistry (WRF-Chem) version 3.7 and the Community Atmosphere Model version 5.3 (CAM5) in simulating profiles of <span class="hlt">aerosol</span> properties is quantified using extensive in situ and remote sensing measurements from the Two-Column <span class="hlt">Aerosol</span> Project (TCAP) conducted during July of 2012. TCAP was supported by the U.S. Department of Energy's Atmospheric Radiation Measurement program and was designed to obtain observations within two atmospheric columns; one fixed over Cape Cod, Massachusetts, and the other several hundred kilometers over the ocean. The performance is quantified using most of the available aircraft and surface measurementsmore » during July, and 2 days are examined in more detail to identify the processes responsible for the observed <span class="hlt">aerosol</span> layers. The higher-resolution WRF-Chem model produced more <span class="hlt">aerosol</span> mass in the free troposphere than the coarser-resolution CAM5 model so that the fraction of <span class="hlt">aerosol</span> optical thickness above the residual layer from WRF-Chem was more consistent with lidar measurements. We found that the free troposphere layers are likely due to mean vertical motions associated with synoptic-<span class="hlt">scale</span> convergence that lifts <span class="hlt">aerosols</span> from the boundary layer. The vertical displacement and the time period associated with upward transport in the troposphere depend on the strength of the synoptic system and whether relatively high boundary layer <span class="hlt">aerosol</span> concentrations are present where convergence occurs. In conclusion, while a parameterization of subgrid <span class="hlt">scale</span> convective clouds applied in WRF-Chem modulated the concentrations of <span class="hlt">aerosols</span> aloft, it did not significantly change the overall altitude and depth of the layers.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC21H1180L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC21H1180L"><span>Background <span class="hlt">aerosol</span> over the Himalayas and Tibetan Plateau: observed characteristics of <span class="hlt">aerosol</span> mass loading</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, B.; Cong, Z.; Wang, Y.; Xin, J.; Wan, X.; Pan, Y.; Liu, Z.; Wang, Y.; Zhang, G.; Kang, S.</p> <p>2016-12-01</p> <p>To investigate the atmospheric <span class="hlt">aerosols</span> of the Himalayas and Tibetan Plateau (HTP), an observation network was established within the region's various ecosystems, including at Ngari, Qomolangma (QOMS), Nam Co, and SouthEastern Tibetan (SET) stations. In this paper we illustrate <span class="hlt">aerosol</span> mass loadings by integrating in situ measurements with satellite and ground-based remote sensing datasets for the 2011-2013 period, on both local and large <span class="hlt">scales</span>. Mass concentrations of these surface atmospheric <span class="hlt">aerosols</span> were relatively low and varied with land cover, showing a general tendency of Ngari and QOMS (barren sites) > Nam Co (grassland site) > SET (forest site). Bimodal mass distributions of size-segregated particles were found at all sites, with a relatively small peak in accumulation mode and a more notable peak in coarse mode. Diurnal variations in fine <span class="hlt">aerosol</span> masses generally displayed a bi-peak pattern at the QOMS, Nam Co and SET stations and a single-peak pattern at the Ngari station, controlled by the effects of local geomorphology, mountain-valley breeze circulation and <span class="hlt">aerosol</span> emissions. Combining surface <span class="hlt">aerosols</span> data and atmospheric-column <span class="hlt">aerosol</span> optical properties, the TSP mass and <span class="hlt">aerosol</span> optical depth (AOD) of the Multi-angle Imaging Spectroradiometer (MISR) generally decreased as land cover changed from barren to forest, in inverse relation to the PM2.5 ratios. The seasonality of <span class="hlt">aerosol</span> mass parameters was land-cover dependent. Over forest and grassland areas, TSP mass, PM2.5 mass, MISR-AOD and fine-mode AOD were higher in spring and summer, followed by relatively lower values in autumn and winter. At the barren site (the QOMS station), there were inconsistent seasonal variations between surface TSP mass (PM2.5 mass) and atmospheric column AOD (fine-mode AOD). Our findings implicate that, HTP <span class="hlt">aerosol</span> masses (especially their reginal characteristics and fine particle emissions) need to be treated sensitively in relation to assessments of their climatic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22356638-milky-way-red-dwarfs-borg-survey-galactic-scale-height-distribution-dwarf-stars-wfc3-imaging','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22356638-milky-way-red-dwarfs-borg-survey-galactic-scale-height-distribution-dwarf-stars-wfc3-imaging"><span>Milky Way red dwarfs in the BoRG survey; galactic <span class="hlt">scale-height</span> and the distribution of dwarf stars in WFC3 imaging</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>Holwerda, B. W.; Bouwens, R.; Trenti, M.</p> <p>2014-06-10</p> <p>We present a tally of Milky Way late-type dwarf stars in 68 Wide Field Camera 3 (WFC3) pure-parallel fields (227 arcmin{sup 2}) from the Brightest of Reionizing Galaxies survey for high-redshift galaxies. Using spectroscopically identified M-dwarfs in two public surveys, the Cosmic Assembly Near-IR Deep Extragalactic Legacy Survey and the Early Release Science mosaics, we identify a morphological selection criterion using the half-light radius (r {sub 50}), a near-infrared J – H, G – J color region where M-dwarfs are found, and a V – J relation with M-dwarf subtype. We apply this morphological selection of stellar objects, color-color selectionmore » of M-dwarfs, and optical-near-infrared color subtyping to compile a catalog of 274 M-dwarfs belonging to the disk of the Milky Way with a limiting magnitude of m {sub F125W} < 24(AB). Based on the M-dwarf statistics, we conclude that (1) the previously identified north-south discrepancy in M-dwarf numbers persists in our sample; there are more M-dwarfs in the northern fields on average than in southern ones, (2) the Milky Way's single disk <span class="hlt">scale-height</span> for M-dwarfs is 0.3-4 kpc, depending on subtype, (3) the <span class="hlt">scale-height</span> depends on M-dwarf subtype with early types (M0-4) high <span class="hlt">scale-height</span> (z {sub 0} = 3-4 kpc) and later types M5 and above in the thin disk (z {sub 0} = 0.3-0.5 kpc), (4) a second component is visible in the vertical distribution, with a different, much higher <span class="hlt">scale-height</span> in the southern fields compared to the northern ones. We report the M-dwarf component of the Sagittarius stream in one of our fields with 11 confirmed M-dwarfs, seven of which are at the stream's distance. In addition to the M-dwarf catalog, we report the discovery of 1 T-dwarfs and 30 L-dwarfs from their near-infrared colors. The dwarf <span class="hlt">scale-height</span> and the relative low incidence in our fields of L- and T-dwarfs in these fields makes it unlikely that these stars will be interlopers in great numbers in color-selected samples of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26423470','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26423470"><span>Water availability predicts forest canopy <span class="hlt">height</span> at the global <span class="hlt">scale</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Klein, Tamir; Randin, Christophe; Körner, Christian</p> <p>2015-12-01</p> <p>The tendency of trees to grow taller with increasing water availability is common knowledge. Yet a robust, universal relationship between the spatial distribution of water availability and forest canopy <span class="hlt">height</span> (H) is lacking. Here, we created a global water availability map by calculating an annual budget as the difference between precipitation (P) and potential evapotranspiration (PET) at a 1-km spatial resolution, and in turn correlated it with a global H map of the same resolution. Across forested areas over the globe, Hmean increased with P-PET, roughly: Hmean (m) = 19.3 + 0.077*(P-PET). Maximum forest canopy <span class="hlt">height</span> also increased gradually from ~ 5 to ~ 50 m, saturating at ~ 45 m for P-PET > 500 mm. Forests were far from their maximum <span class="hlt">height</span> potential in cold, boreal regions and in disturbed areas. The strong association between forest <span class="hlt">height</span> and P-PET provides a useful tool when studying future forest dynamics under climate change, and in quantifying anthropogenic forest disturbance. © 2015 John Wiley & Sons Ltd/CNRS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120009523','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009523"><span>Impact of <span class="hlt">Aerosols</span> on Convective Clouds and Precipitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tao, Wei-Kuo; Chen, Jen-Ping; Li, Zhanqing; Wang, Chien; Zhang, Chidong</p> <p>2011-01-01</p> <p><span class="hlt">Aerosols</span> are a critical factor in the atmospheric hydrological cycle and radiation budget. As a major reason for clouds to form and a significant attenuator of solar radiation, <span class="hlt">aerosols</span> affect climate in several ways. Current research suggests that <span class="hlt">aerosol</span> effects on clouds could further extend to precipitation, both through the formation of cloud particles and by exerting persistent radiative forcing on the climate system that disturbs dynamics. However, the various mechanisms behind these effects, in particular the ones connected to precipitation, are not yet well understood. The atmospheric and climate communities have long been working to gain a better grasp of these critical effects and hence to reduce the significant uncertainties in climate prediction resulting from such a lack of adequate knowledge. The central theme of this paper is to review past efforts and summarize our current understanding of the effect of <span class="hlt">aerosols</span> on precipitation processes from theoretical analysis of microphysics, observational evidence, and a range of numerical model simulations. In addition, the discrepancy between results simulated by models, as well as that between simulations and observations will be presented. Specifically, this paper will address the following topics: (1) fundamental theories of <span class="hlt">aerosol</span> effects on microphysics and precipitation processes, (2) observational evidence of the effect of <span class="hlt">aerosols</span> on precipitation processes, (3) signatures of the <span class="hlt">aerosol</span> impact on precipitation from large-<span class="hlt">scale</span> analyses, (4) results from cloud-resolving model simulations, and (5) results from large-<span class="hlt">scale</span> numerical model simulations. Finally, several future research directions on <span class="hlt">aerosol</span> - precipitation interactions are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120003515','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120003515"><span>The <span class="hlt">Aerosol</span>-Monsoon Climate System of Asia</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lau, William K. M.; Kyu-Myong, Kim</p> <p>2012-01-01</p> <p>In Asian monsoon countries such as China and India, human health and safety problems caused by air-pollution are worsening due to the increased loading of atmospheric pollutants stemming from rising energy demand associated with the rapid pace of industrialization and modernization. Meanwhile, uneven distribution of monsoon rain associated with flash flood or prolonged drought, has caused major loss of human lives, and damages in crop and properties with devastating societal impacts on Asian countries. Historically, air-pollution and monsoon research are treated as separate problems. However a growing number of recent studies have suggested that the two problems may be intrinsically intertwined and need to be studied jointly. Because of complexity of the dynamics of the monsoon systems, <span class="hlt">aerosol</span> impacts on monsoons and vice versa must be studied and understood in the context of <span class="hlt">aerosol</span> forcing in relationship to changes in fundamental driving forces of the monsoon climate system (e.g. sea surface temperature, land-sea contrast etc.) on time <span class="hlt">scales</span> from intraseasonal variability (weeks) to climate change ( multi-decades). Indeed, because of the large contributions of <span class="hlt">aerosols</span> to the global and regional energy balance of the atmosphere and earth surface, and possible effects of the microphysics of clouds and precipitation, a better understanding of the response to climate change in Asian monsoon regions requires that <span class="hlt">aerosols</span> be considered as an integral component of a fully coupled <span class="hlt">aerosol</span>-monsoon system on all time <span class="hlt">scales</span>. In this paper, using observations and results from climate modeling, we will discuss the coherent variability of the coupled <span class="hlt">aerosol</span>-monsoon climate system in South Asia and East Asia, including <span class="hlt">aerosol</span> distribution and types, with respect to rainfall, moisture, winds, land-sea thermal contrast, heat sources and sink distributions in the atmosphere in seasonal, interannual to climate change time <span class="hlt">scales</span>. We will show examples of how elevated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080033606&hterms=indices+diversity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dindices%2Bdiversity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080033606&hterms=indices+diversity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dindices%2Bdiversity"><span><span class="hlt">Aerosol</span> Absorption and Radiative Forcing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stier, Philip; Seinfeld, J. H.; Kinne, Stefan; Boucher, Olivier</p> <p>2007-01-01</p> <p>We present a comprehensive examination of <span class="hlt">aerosol</span> absorption with a focus on evaluating the sensitivity of the global distribution of <span class="hlt">aerosol</span> absorption to key uncertainties in the process representation. For this purpose we extended the comprehensive <span class="hlt">aerosol</span>-climate model ECHAM5-HAM by effective medium approximations for the calculation of <span class="hlt">aerosol</span> effective refractive indices, updated black carbon refractive indices, new cloud radiative properties considering the effect of <span class="hlt">aerosol</span> inclusions, as well as by modules for the calculation of long-wave <span class="hlt">aerosol</span> radiative properties and instantaneous <span class="hlt">aerosol</span> forcing. The evaluation of the simulated <span class="hlt">aerosol</span> absorption optical depth with the AERONET sun-photometer network shows a good agreement in the large <span class="hlt">scale</span> global patterns. On a regional basis it becomes evident that the update of the BC refractive indices to Bond and Bergstrom (2006) significantly improves the previous underestimation of the <span class="hlt">aerosol</span> absorption optical depth. In the global annual-mean, absorption acts to reduce the shortwave anthropogenic <span class="hlt">aerosol</span> top-of-atmosphere (TOA) radiative forcing clear-sky from -0.79 to -0.53 W m(sup -2) (33%) and all-sky from -0.47 to -0.13W m(sup -2 (72%). Our results confirm that basic assumptions about the BC refractive index play a key role for <span class="hlt">aerosol</span> absorption and radiative forcing. The effect of the usage of more accurate effective medium approximations is comparably small. We demonstrate that the diversity in the AeroCom land-surface albedo fields contributes to the uncertainty in the simulated anthropogenic <span class="hlt">aerosol</span> radiative forcings: the usage of an upper versus lower bound of the AeroCom land albedos introduces a global annual-mean TOA forcing range of 0.19W m(sup -2) (36%) clear-sky and of 0.12W m(sup -2) (92%) all-sky. The consideration of black carbon inclusions on cloud radiative properties results in a small global annual-mean all-sky absorption of 0.05W m(sup -2) and a positive TOA forcing perturbation of 0</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/6611914','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/6611914"><span>Pretest <span class="hlt">aerosol</span> code comparisons for LWR <span class="hlt">aerosol</span> containment tests LA1 and LA2</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>Wright, A.L.; Wilson, J.H.; Arwood, P.C.</p> <p></p> <p>The Light-Water-Reactor (LWR) <span class="hlt">Aerosol</span> Containment Experiments (LACE) are being performed in Richland, Washington, at the Hanford Engineering Development Laboratory (HEDL) under the leadership of an international project board and the Electric Power Research Institute. These tests have two objectives: (1) to investigate, at large <span class="hlt">scale</span>, the inherent <span class="hlt">aerosol</span> retention behavior in LWR containments under simulated severe accident conditions, and (2) to provide an experimental data base for validating <span class="hlt">aerosol</span> behavior and thermal-hydraulic computer codes. <span class="hlt">Aerosol</span> computer-code comparison activities are being coordinated at the Oak Ridge National Laboratory. For each of the six LACE tests, ''pretest'' calculations (for code-to-code comparisons) andmore » ''posttest'' calculations (for code-to-test data comparisons) are being performed. The overall goals of the comparison effort are (1) to provide code users with experience in applying their codes to LWR accident-sequence conditions and (2) to evaluate and improve the code models.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AMTD....8.3471C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AMTD....8.3471C"><span>Peak fitting and integration uncertainties for the Aerodyne <span class="hlt">Aerosol</span> Mass Spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Corbin, J. C.; Othman, A.; Haskins, J. D.; Allan, J. D.; Sierau, B.; Worsnop, D. R.; Lohmann, U.; Mensah, A. A.</p> <p>2015-04-01</p> <p>The errors inherent in the fitting and integration of the pseudo-Gaussian ion peaks in Aerodyne High-Resolution <span class="hlt">Aerosol</span> Mass Spectrometers (HR-AMS's) have not been previously addressed as a source of imprecision for these instruments. This manuscript evaluates the significance of these uncertainties and proposes a method for their estimation in routine data analysis. Peak-fitting uncertainties, the most complex source of integration uncertainties, are found to be dominated by errors in m/z calibration. These calibration errors comprise significant amounts of both imprecision and bias, and vary in magnitude from ion to ion. The magnitude of these m/z calibration errors is estimated for an exemplary data set, and used to construct a Monte Carlo model which reproduced well the observed trends in fits to the real data. The empirically-constrained model is used to show that the imprecision in the fitted <span class="hlt">height</span> of isolated peaks <span class="hlt">scales</span> linearly with the peak <span class="hlt">height</span> (i.e., as n1), thus contributing a constant-relative-imprecision term to the overall uncertainty. This constant relative imprecision term dominates the Poisson counting imprecision term (which <span class="hlt">scales</span> as n0.5) at high signals. The previous HR-AMS uncertainty model therefore underestimates the overall fitting imprecision. The constant relative imprecision in fitted peak <span class="hlt">height</span> for isolated peaks in the exemplary data set was estimated as ~4% and the overall peak-integration imprecision was approximately 5%. We illustrate the importance of this constant relative imprecision term by performing Positive Matrix Factorization (PMF) on a~synthetic HR-AMS data set with and without its inclusion. Finally, the ability of an empirically-constrained Monte Carlo approach to estimate the fitting imprecision for an arbitrary number of known overlapping peaks is demonstrated. Software is available upon request to estimate these error terms in new data sets.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1610523G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1610523G"><span>Assessment of microphysical and chemical factors of <span class="hlt">aerosols</span> over seas of the Russian Artic Eastern Section</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Golobokova, Liudmila; Polkin, Victor</p> <p>2014-05-01</p> <p>The newly observed kickoff of the Northern Route development drew serious attention to state of the Arctic Resource environment. Occurring climatic and environmental changes are more sensitively seen in polar areas in particular. Air environment control allows for making prognostic assessments which are required for planning hazardous environmental impacts preventive actions. In August - September 2013, RV «Professor Khlustin» Northern Sea Route expeditionary voyage took place. En-route <span class="hlt">aerosol</span> sampling was done over the surface of the Beringov, Chukotka and Eastern-Siberia seas (till the town of Pevek). The purpose of sampling was to assess spatio-temporal variability of optic, microphysical and chemical characteristics of <span class="hlt">aerosol</span> particles of the surface layer within different areas adjacent to the Northern Sea Route. <span class="hlt">Aerosol</span> test made use of automated mobile unit consisting of photoelectric particles counter AZ-10, aetalometr MDA-02, aspirator on NBM-1.2 pump chassis, and the impactor. This set of equipment allows for doing measurements of number concentration, dispersed composition of <span class="hlt">aerosols</span> within sizes d=0.3-10 mkm, mass concentration of submicron sized <span class="hlt">aerosol</span>, and filter-conveyed <span class="hlt">aerosols</span> sampling. Filter-conveyed <span class="hlt">aerosols</span> sampling was done using method accepted by EMEP and EANET monitoring networks. The impactor channel was upgraded to separate particles bigger than 1 mkm in size, and the fine grain fraction settled down on it. Reverse 5-day and 10-day trajectories of air mass transfer executed at <span class="hlt">heights</span> of 10, 1500 and 3500 m were analyzed. The <span class="hlt">heights</span> were selected by considerations that 3000 m is the <span class="hlt">height</span> which characterizes air mass trend in the lower troposphere. 1500 m is the upper border of the atmospheric boundary layer, and the sampling was done in the Earth's surface layer at less than 10 m. Minimum values of the bespoken microphysical characteristics are better characteristic of higher latitudes where there are no man induced sources of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A52A..05R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A52A..05R"><span>Use of the NASA GEOS-5 SEAC4RS Meteorological and <span class="hlt">Aerosol</span> Reanalysis for assessing simulated <span class="hlt">aerosol</span> optical properties as a function of smoke age</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Randles, C. A.; da Silva, A. M., Jr.; Colarco, P. R.; Darmenov, A.; Buchard, V.; Govindaraju, R.; Chen, G.; Hair, J. W.; Russell, P. B.; Shinozuka, Y.; Wagner, N.; Lack, D.</p> <p>2014-12-01</p> <p>The NASA Goddard Earth Observing System version 5 (GEOS-5) Earth system model, which includes an online <span class="hlt">aerosol</span> module, provided chemical and weather forecasts during the SEAC4RS field campaign. For post-mission analysis, we have produced a high resolution (25 km) meteorological and <span class="hlt">aerosol</span> reanalysis for the entire campaign period. In addition to the full meteorological observing system used for routine NWP, we assimilate 550 nm <span class="hlt">aerosol</span> optical depth (AOD) derived from MODIS (both Aqua and Terra satellites), ground-based AERONET sun photometers, and the MISR instrument (over bright surfaces only). Daily biomass burning emissions of CO, CO2, SO2, and <span class="hlt">aerosols</span> are derived from MODIS fire radiative power retrievals. We have also introduced novel smoke "age" tracers, which provide, for a given time, a snapshot histogram of the age of simulated smoke <span class="hlt">aerosol</span>. Because GEOS-5 assimilates remotely sensed AOD data, it generally reproduces observed (column) AOD compared to, for example, the airborne 4-STAR instrument. Constraining AOD, however, does not imply a good representation of either the vertical profile or the <span class="hlt">aerosol</span> microphysical properties (e.g., composition, absorption). We do find a reasonable vertical structure for <span class="hlt">aerosols</span> is attained in the model, provided actual smoke injection <span class="hlt">heights</span> are not much above the planetary boundary layer, as verified with observations from DIAL/HRSL aboard the DC8. The translation of the simulated <span class="hlt">aerosol</span> microphysical properties to total column AOD, needed in the <span class="hlt">aerosol</span> assimilation step, is based on prescribed mass extinction efficiencies that depend on wavelength, composition, and relative humidity. Here we also evaluate the performance of the simulated <span class="hlt">aerosol</span> speciation by examining in situ retrievals of <span class="hlt">aerosol</span> absorption/single scattering albedo and scattering growth factor (f(RH)) from the LARGE and AOP suite of instruments. Putting these comparisons in the context of smoke age as diagnosed by the model helps us to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.U21D..01S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.U21D..01S"><span>High Altitude Emissions of Black Carbon <span class="hlt">Aerosols</span>: Potential Climate Implications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Satheesh, S. K.</p> <p>2017-12-01</p> <p>Synthesizing a series of ground-based and airborne measurements of <span class="hlt">aerosols</span> over the Indian region during summer and pre-monsoon seasons have revealed the persistence of elevated absorbing <span class="hlt">aerosol</span> layers over most of the Indian region; more than 50% of which located above clouds. Subsequent, in situ measurements of black carbon (BC) using high-altitude balloons, showed surprising layers with high concentrations in the middle and upper troposphere even at an altitude of 8 to 10 kms. Simultaneous measurements of the vertical thermal structure have shown localized warming due to BC absorption leading to large reduction in lapse rate and sharp temperature inversion, which in turn increases the atmospheric stability. This <span class="hlt">aerosol</span>-induced stable layer is conducive for maintaining the black carbon layer longer at that level, leading thereby to further solar absorption and subsequently triggering dry convection. These observations support the `solar escalator' concept through which absorption-warming-convection cycles lead to self-lifting of BC to upper troposphere or even to lower stratosphere under favorable conditions in a matter of a few days. Employing an on-line regional chemistry transport model (WRF-Chem), incorporating aircraft emissions, it is shown that emissions from high-flying aircrafts as the most likely source of these elevated black carbon layers. These in-situ injected particles, produce significant warming of the thin air in those <span class="hlt">heights</span> and lift these layers to even upper tropospheric/lower stratospheric <span class="hlt">heights</span>, aided by the strong monsoonal convection occurring over the region, which are known to overshoot the tropical tropopause leading to injection of tropospheric air mass (along with its constituent <span class="hlt">aerosols</span>) into the stratosphere, especially during monsoon season when the tropical tropopause layer is known to be thinnest. These simulations are further supported by the CALIPSO space-borne LIDAR derived extinction coefficient profiles. Based on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800042216&hterms=Formation+soils&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DFormation%2Bsoils','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800042216&hterms=Formation+soils&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DFormation%2Bsoils"><span>Formation and deposition of volcanic sulfate <span class="hlt">aerosols</span> on Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Settle, M.</p> <p>1979-01-01</p> <p>The paper considers the formation and deposition of volcanic sulfate <span class="hlt">aerosols</span> on Mars. The rate limiting step in sulfate <span class="hlt">aerosol</span> formation on Mars is the gas phase oxidation of SO2 by chemical reactions with O, OH, and HO2; submicron <span class="hlt">aerosol</span> particles would circuit Mars and then be removed from the atmosphere by gravitational forces, globally dispersed, and deposited over a range of equatorial and mid-latitudes. Volcanic sulfate <span class="hlt">aerosols</span> on Mars consist of liquid droplets and slurries containing sulfuric acid; <span class="hlt">aerosol</span> deposition on a global or hemispheric <span class="hlt">scale</span> could account for the similar concentrations of sulfur within surficial soils at the two Viking lander sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730004894','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730004894"><span>Mixing-<span class="hlt">height</span> measurement by lidar, particle counter, and rawinsonde in the Williamette Valley, Oregon</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mccormick, M. P.; Melfi, S. H.; Olsson, L. E.; Tuft, W. L.; Elliott, W. P.; Egami, R.</p> <p>1972-01-01</p> <p>The feasibility of using laser radar (lidar) to measure the spatial distribution of <span class="hlt">aerosols</span> and water vapor in the earth's mixing or boundary layer is shown. From these data the important parameter of actual mixing <span class="hlt">height</span> was determined, that is, the maximum <span class="hlt">height</span> to which particulate pollutants actually mix. Data are shown for simultaneous lidar, rawinsonde, and aircraft-mounted condensation nuclei counter and temperature measurements. The synoptic meteorology is also presented. The Williamette Valley, Oregon, was chosen for the measurements because of its unique combination of meteorology, terrain, and pollutant source, along with an ongoing Oregon State University study of the natural ventilation of this valley.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1916259W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916259W"><span>Comparison of mineral dust and droplet residuals measured with two single particle <span class="hlt">aerosol</span> mass spectrometers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wonaschütz, Anna; Ludwig, Wolfgang; Zawadowicz, Maria; Hiranuma, Naruki; Hitzenberger, Regina; Cziczo, Daniel; DeMott, Paul; Möhler, Ottmar</p> <p>2017-04-01</p> <p>Single Particle mass spectrometers are used to gain information on the chemical composition of individual <span class="hlt">aerosol</span> particles, <span class="hlt">aerosol</span> mixing state, and other valuable <span class="hlt">aerosol</span> characteristics. During the Mass Spectrometry Intercomparison at the Fifth Ice Nucleation (FIN-01) Workshop, the new LAAPTOF single particle <span class="hlt">aerosol</span> mass spectrometer (AeroMegt GmbH) was conducting simultaneous measurements together with the PALMS (Particle Analysis by Laser Mass Spectrometry) instrument. The <span class="hlt">aerosol</span> particles were sampled from the AIDA chamber during ice cloud expansion experiments. Samples of mineral dust and ice droplet residuals were measured simultaneously. In this work, three expansion experiments are chosen for a comparison between the two mass spectrometers. A fuzzy clustering routine is used to group the spectra. Cluster centers describing the ensemble of particles are compared. First results show that while differences in the peak <span class="hlt">heights</span> are likely due to the use of an amplifier in PALMS, cluster centers are comparable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.A11F0142L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.A11F0142L"><span>Evolution of <span class="hlt">aerosol</span> downwind of a major highway</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liggio, J.; Staebler, R. M.; Brook, J.; Li, S.; Vlasenko, A. L.; Sjostedt, S. J.; Gordon, M.; Makar, P.; Mihele, C.; Evans, G. J.; Jeong, C.; Wentzell, J. J.; Lu, G.; Lee, P.</p> <p>2010-12-01</p> <p>Primary <span class="hlt">aerosol</span> from traffic emissions can have a considerable impact local and regional <span class="hlt">scale</span> air quality. In order to assess the effect of these emissions and of future emissions scenarios, air quality models are required which utilize emissions representative of real world conditions. Often, the emissions processing systems which provide emissions input for the air quality models rely on laboratory testing of individual vehicles under non-ambient conditions. However, on the sub-grid <span class="hlt">scale</span> particle evolution may lead to changes in the primary emitted size distribution and gas-particle partitioning that are not properly considered when the emissions are ‘instantly mixed’ within the grid volume. The affect of this modeling convention on model results is not well understood. In particular, changes in organic gas/particle partitioning may result in particle evaporation or condensation onto pre-existing <span class="hlt">aerosol</span>. The result is a change in the particle distribution and/or an increase in the organic mass available for subsequent gas-phase oxidation. These effects may be missing from air-quality models, and a careful analysis of field data is necessary to quantify their impact. A study of the sub-grid evolution of <span class="hlt">aerosols</span> (FEVER; Fast Evolution of Vehicle Emissions from Roadways) was conducted in the Toronto area in the summer of 2010. The study included mobile measurements of particle size distributions with a Fast mobility particle sizer (FMPS), <span class="hlt">aerosol</span> composition with an Aerodyne <span class="hlt">aerosol</span> mass spectrometer (AMS), black carbon (SP2, PA, LII), VOCs (PTR-MS) and other trace gases. The mobile laboratory was used to measure the concentration gradient of the emissions at perpendicular distances from the highway as well as the physical and chemical evolution of the <span class="hlt">aerosol</span>. Stationary sites at perpendicular distances and upwind from the highway also monitored the particle size distribution. In addition, sonic anemometers mounted on the mobile lab provided measurements of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27222566','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27222566"><span>Improving our fundamental understanding of the role of <span class="hlt">aerosol</span>-cloud interactions in the climate system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Seinfeld, John H; Bretherton, Christopher; Carslaw, Kenneth S; Coe, Hugh; DeMott, Paul J; Dunlea, Edward J; Feingold, Graham; Ghan, Steven; Guenther, Alex B; Kahn, Ralph; Kraucunas, Ian; Kreidenweis, Sonia M; Molina, Mario J; Nenes, Athanasios; Penner, Joyce E; Prather, Kimberly A; Ramanathan, V; Ramaswamy, Venkatachalam; Rasch, Philip J; Ravishankara, A R; Rosenfeld, Daniel; Stephens, Graeme; Wood, Robert</p> <p>2016-05-24</p> <p>The effect of an increase in atmospheric <span class="hlt">aerosol</span> concentrations on the distribution and radiative properties of Earth's clouds is the most uncertain component of the overall global radiative forcing from preindustrial time. General circulation models (GCMs) are the tool for predicting future climate, but the treatment of <span class="hlt">aerosols</span>, clouds, and <span class="hlt">aerosol</span>-cloud radiative effects carries large uncertainties that directly affect GCM predictions, such as climate sensitivity. Predictions are hampered by the large range of <span class="hlt">scales</span> of interaction between various components that need to be captured. Observation systems (remote sensing, in situ) are increasingly being used to constrain predictions, but significant challenges exist, to some extent because of the large range of <span class="hlt">scales</span> and the fact that the various measuring systems tend to address different <span class="hlt">scales</span>. Fine-<span class="hlt">scale</span> models represent clouds, <span class="hlt">aerosols</span>, and <span class="hlt">aerosol</span>-cloud interactions with high fidelity but do not include interactions with the larger <span class="hlt">scale</span> and are therefore limited from a climatic point of view. We suggest strategies for improving estimates of <span class="hlt">aerosol</span>-cloud relationships in climate models, for new remote sensing and in situ measurements, and for quantifying and reducing model uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170001439&hterms=1091&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3D%2526%25231091','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170001439&hterms=1091&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3D%2526%25231091"><span>Improving Our Fundamental Understanding of the Role of <span class="hlt">Aerosol</span> Cloud Interactions in the Climate System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Seinfeld, John H.; Bretherton, Christopher; Carslaw, Kenneth S.; Coe, Hugh; DeMott, Paul J.; Dunlea, Edward J.; Feingold, Graham; Ghan, Steven; Guenther, Alex B.; Kahn, Ralph; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170001439'); toggleEditAbsImage('author_20170001439_show'); toggleEditAbsImage('author_20170001439_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170001439_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170001439_hide"></p> <p>2016-01-01</p> <p>The effect of an increase in atmospheric <span class="hlt">aerosol</span> concentrations on the distribution and radiative properties of Earth's clouds is the most uncertain component of the overall global radiative forcing from preindustrial time. General circulation models (GCMs) are the tool for predicting future climate, but the treatment of <span class="hlt">aerosols</span>, clouds, and <span class="hlt">aerosol</span>-cloud radiative effects carries large uncertainties that directly affect GCM predictions, such as climate sensitivity. Predictions are hampered by the large range of <span class="hlt">scales</span> of interaction between various components that need to be captured. Observation systems (remote sensing, in situ) are increasingly being used to constrain predictions, but significant challenges exist, to some extent because of the large range of <span class="hlt">scales</span> and the fact that the various measuring systems tend to address different <span class="hlt">scales</span>. Fine-<span class="hlt">scale</span> models represent clouds, <span class="hlt">aerosols</span>, and <span class="hlt">aerosol</span>-cloud interactions with high fidelity but do not include interactions with the larger <span class="hlt">scale</span> and are therefore limited from a climatic point of view. We suggest strategies for improving estimates of <span class="hlt">aerosol</span>-cloud relationships in climate models, for new remote sensing and in situ measurements, and for quantifying and reducing model uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1327134-improving-our-fundamental-understanding-role-aerosol-cloud-interactions-climate-system','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1327134-improving-our-fundamental-understanding-role-aerosol-cloud-interactions-climate-system"><span>Improving our fundamental understanding of the role of <span class="hlt">aerosol</span>-cloud interactions in the climate system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Seinfeld, John H.; Bretherton, Christopher; Carslaw, Kenneth S.; ...</p> <p>2016-05-24</p> <p>The effect of an increase in atmospheric <span class="hlt">aerosol</span> concentrations on the distribution and radiative properties of Earth’s clouds is the most uncertain component of the overall global radiative forcing from pre-industrial time. General Circulation Models (GCMs) are the tool for predicting future climate, but the treatment of <span class="hlt">aerosols</span>, clouds, and <span class="hlt">aerosol</span>-cloud radiative effects carries large uncertainties that directly affect GCM predictions, such as climate sensitivity. Predictions are hampered by the large range of <span class="hlt">scales</span> of interaction between various components that need to be captured. Observation systems (remote sensing, in situ) are increasingly being used to constrain predictions but significant challengesmore » exist, to some extent because of the large range of <span class="hlt">scales</span> and the fact that the various measuring systems tend to address different <span class="hlt">scales</span>. Fine-<span class="hlt">scale</span> models represent clouds, <span class="hlt">aerosols</span>, and <span class="hlt">aerosol</span>-cloud interactions with high fidelity but do not include interactions with the larger <span class="hlt">scale</span> and are therefore limited from a climatic point of view. Lastly, we suggest strategies for improving estimates of <span class="hlt">aerosol</span>-cloud relationships in climate models, for new remote sensing and in situ measurements, and for quantifying and reducing model uncertainty.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000096236&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DTOM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000096236&hterms=TOM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DTOM"><span>Preliminary Results from an Assimilation of TOMS <span class="hlt">Aerosol</span> Observations Into the GOCART Model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>daSilva, Arlindo; Weaver, Clark J.; Ginoux, Paul; Torres, Omar; Einaudi, Franco (Technical Monitor)</p> <p>2000-01-01</p> <p>At NASA Goddard we are developing a global <span class="hlt">aerosol</span> data assimilation system that combines advances in remote sensing and modeling of atmospheric <span class="hlt">aerosols</span>. The goal is to provide high resolution, 3-D <span class="hlt">aerosol</span> distributions to the research community. Our first step is to develop a simple assimilation system for Saharan mineral <span class="hlt">aerosol</span>. The Goddard Chemistry and <span class="hlt">Aerosol</span> Radiation model (GOCART) provides accurate 3-D mineral <span class="hlt">aerosol</span> size distributions that compare well with TOMS satellite observations. Surface, mobilization, wet and dry deposition, convective and long-range transport are all driven by assimilated fields from the Goddard Earth Observing System Data Assimilation System, GEOS-DAS. Our version of GOCART transports sizes from.08-10 microns and only simulates Saharan dust. TOMS radiance observations in the ultra violet provide information on the mineral and carbonaceous <span class="hlt">aerosol</span> fields. We use two main observables in this study: the TOMS <span class="hlt">aerosol</span> index (AI) which is directly related to the ratio of the 340 and 380 radiances and the 380 radiance. These are sensitive to the <span class="hlt">aerosol</span> optical thickness, the single scattering albedo and the <span class="hlt">height</span> of the <span class="hlt">aerosol</span> layer. The Goddard <span class="hlt">Aerosol</span> Assimilation System (GAAS) uses the Data Assimilation Office's Physical-space Statistical Analysis System (PSAS) to combine TOMS observations and GOCART model first guess fields. At this initial phase we only assimilate observations into the the GOCART model over regions of Africa and the Atlantic where mineral <span class="hlt">aerosols</span> dominant and carbonaceous <span class="hlt">aerosols</span> are minimal, Our preliminary results during summer show that the assimilation with TOMS data modifies both the <span class="hlt">aerosol</span> mass loading and the single scattering albedo. Assimilated <span class="hlt">aerosol</span> fields will be compared with assimilated <span class="hlt">aerosol</span> fields from GOCART and AERONET observations over Cape Verde.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1338293','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1338293"><span>Improvement of Representation of the Cloud-<span class="hlt">Aerosol</span> Interaction in Large-<span class="hlt">Scale</span> Models</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Khain, Alexander; Phillips, Vaughan; Pinsky, Mark</p> <p></p> <p>The main achievements reached under the DOE award DE-SC0006788 are described. It is shown that the plan of the Project is completed. Unique results concerning cloud-<span class="hlt">aerosol</span> interaction are obtained. It is shown that <span class="hlt">aerosols</span> affect intensity of hurricanes. The effects of small <span class="hlt">aerosols</span> on formation of ice in anvils of deep convective clouds are discovered, for the first time the mechanisms of drizzle formation are found and described quantitatively. Mechanisms of formation of warm rain are clarified and the dominating role of adiabatic processes and turbulence are stressed. Important results concerning the effects of sea spray on intensity of cloudsmore » and tropical cyclones are obtained. A novel methods of calculation of hail formation has been developed and implemented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1012285-indirect-semi-direct-aerosol-campaign-impact-arctic-aerosols-clouds','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1012285-indirect-semi-direct-aerosol-campaign-impact-arctic-aerosols-clouds"><span>Indirect and Semi-Direct <span class="hlt">Aerosol</span> Campaign: The Impact of Arctic <span class="hlt">Aerosols</span> on Clouds</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>McFarquhar, Greg; Ghan, Steven J.; Verlinde, J.</p> <p>2011-02-01</p> <p>A comprehensive dataset of microphysical and radiative properties of <span class="hlt">aerosols</span> and clouds in the arctic boundary layer in the vicinity of Barrow, Alaska was collected in April 2008 during the Indirect and Semi-Direct <span class="hlt">Aerosol</span> Campaign (ISDAC) sponsored by the Department of Energy Atmospheric Radiation Measurement (ARM) and Atmospheric Science Programs. The primary aim of ISDAC was to examine indirect effects of <span class="hlt">aerosols</span> on clouds that contain both liquid and ice water. The experiment utilized the ARM permanent observational facilities at the North Slope of Alaska (NSA) in Barrow. These include a cloud radar, a polarized micropulse lidar, and an atmosphericmore » emitted radiance interferometer as well as instruments specially deployed for ISDAC measuring <span class="hlt">aerosol</span>, ice fog, precipitation and spectral shortwave radiation. The National Research Council of Canada Convair-580 flew 27 sorties during ISDAC, collecting data using an unprecedented 42 cloud and <span class="hlt">aerosol</span> instruments for more than 100 hours on 12 different days. Data were obtained above, below and within single-layer stratus on 8 April and 26 April 2008. These data enable a process-oriented understanding of how <span class="hlt">aerosols</span> affect the microphysical and radiative properties of arctic clouds influenced by different surface conditions. Observations acquired on a heavily polluted day, 19 April 2008, are enhancing this understanding. Data acquired in cirrus on transit flights between Fairbanks and Barrow are improving our understanding of the performance of cloud probes in ice. Ultimately the ISDAC data will be used to improve the representation of cloud and <span class="hlt">aerosol</span> processes in models covering a variety of spatial and temporal <span class="hlt">scales</span>, and to determine the extent to which long-term surface-based measurements can provide retrievals of <span class="hlt">aerosols</span>, clouds, precipitation and radiative heating in the Arctic.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ACP....11.6837C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ACP....11.6837C"><span>Estimating the atmospheric boundary layer <span class="hlt">height</span> over sloped, forested terrain from surface spectral analysis during BEARPEX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, W.; Faloona, I. C.; McKay, M.; Goldstein, A. H.; Baker, B.</p> <p>2011-07-01</p> <p>The atmospheric boundary layer (ABL) <span class="hlt">height</span> (zi) over complex, forested terrain is estimated based on the power spectra and the integral length <span class="hlt">scale</span> of cross-stream winds obtained from a three-axis sonic anemometer during the two summers of the BEARPEX (Biosphere Effects on <span class="hlt">Aerosol</span> and Photochemistry) Experiment. The zi values estimated with this technique show very good agreement with observations obtained from balloon tether sondes (2007) and rawinsondes (2009) under unstable conditions (z/L < 0) at the coniferous forest in the California Sierra Nevada. On the other hand, the low frequency behavior of the streamwise upslope winds did not exhibit significant variations and was therefore not useful in predicting boundary layer <span class="hlt">height</span>. The behavior of the nocturnal boundary layer <span class="hlt">height</span> (h) with respect to the power spectra of the v-wind component and temperature under stable conditions (z/L > 0) is also presented. The nocturnal boundary layer <span class="hlt">height</span> is found to be fairly well predicted by a recent interpolation formula proposed by Zilitinkevich et al. (2007), although it was observed to only vary from 60-80 m during the 2009 experiment in which it was measured. Finally, significant directional wind shear was observed during both day and night soundings. The winds were found to be consistently backing from the prevailing west-southwesterlies within the ABL (the anabatic cross-valley circulation) to southerlies in a layer ~1-2 km thick just above the ABL before veering to the prevailing westerlies further aloft. This shear pattern is shown to be consistent with the forcing of a thermal wind driven by the regional temperature gradient directed east-southeast in the lower troposphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A13F2162L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A13F2162L"><span>The physico-chemical evolution of atmospheric <span class="hlt">aerosols</span> and the gas-particle partitioning of inorganic <span class="hlt">aerosol</span> during KORUS-AQ</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, T.; Park, T.; Lee, J. B.; Lim, Y. J.; Ahn, J.; Park, J. S.; Soo, C. J.; Desyaterik, Y.; Collett, J. L., Jr.</p> <p>2017-12-01</p> <p><span class="hlt">Aerosols</span> influence climate change directly by scattering and absorption and indirectly by acting as cloud condensation nuclei and some of the effects of <span class="hlt">aerosols</span> are reduction in visibility, deterioration of human health, and deposition of pollutants to ecosystems. Urban area is large source of <span class="hlt">aerosols</span> and <span class="hlt">aerosol</span> precursors. <span class="hlt">Aerosol</span> sources are both local and from long-range transport. Long-range transport processed <span class="hlt">aerosol</span> are often dominant sources of <span class="hlt">aerosol</span> pollution in Korea. To improve our knowledge of <span class="hlt">aerosol</span> chemistry, Korea and U.S-Air Quality (KORUS-AQ) of Aircraft-based <span class="hlt">aerosol</span> measurement took place in and around Seoul, Korea during May and June 2016. KORUS-AQ campaigns were conducted to study the chemical characterization and processes of pollutants in the Seoul Metropolitan area to regional <span class="hlt">scales</span> of Korean peninsula. Aerodyne High Resolution Time of Flight <span class="hlt">Aerosol</span> Mass Spectrometer (HR-ToF-AMS) was deployed on aircraft platforms on-board DC-8 (NASA) aircraft. We characterized <span class="hlt">aerosol</span> chemical properties and mass concentrations of sulfate, nitrate, ammonium and organics in polluted air plumes and investigate the spatial and vertical distribution of the species. The results of studies show that organics is predominant in <span class="hlt">Aerosol</span> and a significant fraction of the organics is oxygenated organic <span class="hlt">aerosol</span> (OOA) at the high altitude. Both Nitrate and sulfate can partition between the gas and particle phases. The ratios for HNO3/(N(V) (=gaseous HNO3 + particulate Nitrate) and SO2/(SO2+Sulfate) were found to exhibit quite different distributions between the particles and gas phase for the locations during KORUS-AQ campaign, representing potential for formation of additional particulate nitrate and sulfate. The results of those studies can provide highly resolved temporal and spatial air pollutant, which are valuable for air quality model input parameters for <span class="hlt">aerosol</span> behaviour.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040171157&hterms=coverage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dcoverage','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040171157&hterms=coverage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dcoverage"><span>Cloud Coverage and <span class="hlt">Height</span> Distribution from the GLAS Polar Orbiting Lidar: Comparison to Passive Cloud Retrievals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Spinhime, J. D.; Palm, S. P.; Hlavka, D. L.; Hart, W. D.; Mahesh, A.</p> <p>2004-01-01</p> <p>The Geoscience Laser Altimeter System (GLAS) began full on orbit operations in September 2003. A main application of the two-wavelength GLAS lidar is highly accurate detection and profiling of global cloud cover. Initial analysis indicates that cloud and <span class="hlt">aerosol</span> layers are consistently detected on a global basis to cross-sections down to 10(exp -6) per meter. Images of the lidar data dramatically and accurately show the vertical structure of cloud and <span class="hlt">aerosol</span> to the limit of signal attenuation. The GLAS lidar has made the most accurate measurement of global cloud coverage and <span class="hlt">height</span> to date. In addition to the calibrated lidar signal, GLAS data products include multi level boundaries and optical depth of all transmissive layers. Processing includes a multi-variable separation of cloud and <span class="hlt">aerosol</span> layers. An initial application of the data results is to compare monthly cloud means from several months of GLAS observations in 2003 to existing cloud climatologies from other satellite measurement. In some cases direct comparison to passive cloud retrievals is possible. A limitation of the lidar measurements is nadir only sampling. However monthly means exhibit reasonably good global statistics and coverage results, at other than polar regions, compare well with other measurements but show significant differences in <span class="hlt">height</span> distribution. For polar regions where passive cloud retrievals are problematic and where orbit track density is greatest, the GLAS results are particularly an advance in cloud cover information. Direct comparison to MODIS retrievals show a better than 90% agreement in cloud detection for daytime, but less than 60% at night. <span class="hlt">Height</span> retrievals are in much less agreement. GLAS is a part of the NASA EOS project and data products are thus openly available to the science community (see http://glo.gsfc.nasa.gov).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914777N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914777N"><span>Micrometeorological flux measurements of <span class="hlt">aerosol</span> and gases above Beijing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nemitz, Eiko; Langford, Ben; Mullinger, Neil; Cowan, Nicholas; Coyle, Mhairi; Acton, William Joe; Lee, James; Fu, Pingqing</p> <p>2017-04-01</p> <p>Air pollution is estimated to cause 1.6 million premature deaths in China every year and in the winter 2016/17 Beijing had to issue health alerts and put in place ad hoc limitations on industrial and vehicular activity. Much of this pollution is attributed to emissions from industrial processes and in particular coal combustion. By contrast, the diffuse pollutant sources within the city are less well understood. This includes, e.g., emissions from the Beijing traffic fleet, the sewage system, food preparation, solid fuel combustion in the streets and small industrial processes. Within the framework of a major UK-Chinese collaboration to study air pollution and its impact on human health in Beijing, we therefore measured fluxes of a large range of pollutants from a <span class="hlt">height</span> of 102 m on the 325 m meteorological tower at the Institute of Atmospheric Physics. Several instruments were mounted at 102 m: fluxes of CO2 and H2O were measured with an infrared gas analyser (LiCOR 7500) and fluxes of ozone with a combination of a relative fast-response ozone analyser (ROFI) and a 2B absolute O3 instrument. Total particle number fluxes were measured with a condensation particle counter (TSI CPC 3785), and size-segregated fluxes over the size range 0.06 to 20 μm with a combination of an optical Ultrafine High Sensitivity <span class="hlt">Aerosol</span> Spectrometer (UHSAS) and an Aerodynamic Particle Sizer Spectrometer (TSI APS3321). Ammonia (NH3) fluxes were measured for the first time above the urban environment using an Aerodyne compact quantum cascade laser (QCL). In addition, composition resolved <span class="hlt">aerosol</span> fluxes were measured with an Aerodyne <span class="hlt">Aerosol</span> Mass Spectrometer (HR-ToF-AMS), operated in a measurement container at the bottom of the tower, which subsampled from a 120 m long copper tube (15 mm OD). The analysis so far suggests that, due to often low wind speeds, fluxes were at times de-coupled from the surface. Fluxes normalised by CO2, a tracer for the amount of fossil fuel consumed, should be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1210822L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1210822L"><span>The effect of <span class="hlt">aerosols</span> on northern hemisphere wintertime stationary waves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewinschal, Anna; Ekman, Annica M. L.</p> <p>2010-05-01</p> <p><span class="hlt">Aerosol</span> particles have a considerable impact on the energy budget of the atmosphere because of their ability to scatter and absorb incoming solar radiation. Since the beginning of the industrialisation a large increase has been seen mainly in the concentrations of sulphate and black carbon as a result of combustion of fossil fuel and biomass burning. <span class="hlt">Aerosol</span> particles have a relatively short residence time in the atmosphere why the <span class="hlt">aerosol</span> concentration shows a large variation spatially as well as in time where high concentrations are found close to emission sources. This leads to a highly varying radiative forcing pattern which modifies temperature gradients which in turn can alter the pressure distribution and lead to changes in the circulation in the atmosphere. In this study, the effect on the wintertime planetary <span class="hlt">scale</span> waves on the northern hemisphere is specifically considered together with the regional climate impact due to changes in the stationary waves. To investigate the effect of <span class="hlt">aerosols</span> on the circulation a global general circulation model based on the ECMWF operational forecast model is used (EC-Earth). The <span class="hlt">aerosol</span> description in EC-Earth consists of prescribed monthly mean mass concentration fields of five different types of <span class="hlt">aerosols</span>: sulphate, black carbon, organic carbon, dust and sea salt. Only the direct radiative effect is considered and the different <span class="hlt">aerosol</span> types are treated as external mixtures. Changes in the stationary wave pattern are determined by comparing model simulations using present-day and pre-industrial concentrations of <span class="hlt">aerosol</span> particles. Since the planetary <span class="hlt">scale</span> waves largely influence the storm tracks and are an important part of the meridional heat transport, changes in the wave pattern may have substantial impact on the climate globally and locally. By looking at changes in the model simulations globally it can be found that the <span class="hlt">aerosol</span> radiative forcing has the potential to change the stationary wave pattern. Furthermore</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ACPD...1018661R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ACPD...1018661R"><span>Development and evaluation of the <span class="hlt">aerosol</span> dynamic and gas phase chemistry model ADCHEM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roldin, P.; Swietlicki, E.; Schurgers, G.; Arneth, A.; Lehtinen, K. E. J.; Boy, M.; Kulmala, M.</p> <p>2010-08-01</p> <p>The aim of this work was to develop a model ideally suited for detailed studies on <span class="hlt">aerosol</span> dynamics, gas and particle phase chemistry within urban plumes, from local <span class="hlt">scale</span> (1×1 km2) to regional or global <span class="hlt">scale</span>. This article describes and evaluates the trajectory model for <span class="hlt">Aerosol</span> Dynamics, gas and particle phase CHEMistry and radiative transfer (ADCHEM), which has been developed and used at Lund University since 2007. The model treats both vertical and horizontal dispersion perpendicular to an air mass trajectory (2-space dimensions), which is not treated in Lagrangian box-models (0-space dimensions). The Lagrangian approach enables a more detailed representation of the <span class="hlt">aerosol</span> dynamics, gas and particle phase chemistry and a finer spatial and temporal resolution compared to that of available regional 3D-CTMs. These features make it among others ideally suited for urban plume studies. The <span class="hlt">aerosol</span> dynamics model includes Brownian coagulation, dry deposition, wet deposition, in-cloud processing, condensation, evaporation, primary particle emissions and homogeneous nucleation. The gas phase chemistry model calculates the gas phase concentrations of 63 different species, using 119 different chemical reactions. Daily isoprene and monoterpene emissions from European forests were simulated separately with the vegetation model LPJ-GUESS, and included as input to ADCHEM. ADCHEM was used to simulate the ageing of the urban plumes from the city of Malmö in Southern Sweden (280 000 inhabitants). Several sensitivity tests were performed concerning the number of size bins, size structure method, coupled or uncoupled condensation, the volatility basis set (VBS) or traditional 2-product model for secondary organic <span class="hlt">aerosol</span> formation, different <span class="hlt">aerosol</span> dynamic processes and vertical and horizontal mixing. The simulations show that the full-stationary size structure gives accurate results with little numerical diffusion when more than 50 size bins are used between 1.5 and 2500 nm</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000120582&hterms=coastal+zone&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dcoastal%2Bzone','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000120582&hterms=coastal+zone&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dcoastal%2Bzone"><span>Global Distribution of <span class="hlt">Aerosols</span> Over the Open Ocean as Derived from the Coastal Zone Color Scanner</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stegmann, P. M.; Tindale, N. W.</p> <p>1999-01-01</p> <p>Climatological maps of monthly mean <span class="hlt">aerosol</span> radiance levels derived from the coastal zone color scanner (CZCS) were constructed for the world's ocean basins. This is the first study to use the 7.5.-year CZCS data set to examine the distribution and seasonality of <span class="hlt">aerosols</span> over the open ocean on a global <span class="hlt">scale</span>. Examination of our satellite images found the most prominent large-<span class="hlt">scale</span> patch of elevated <span class="hlt">aerosol</span> radiances in each month off the coast of northwest Africa. The well-known, large-<span class="hlt">scale</span> plumes of elevated <span class="hlt">aerosol</span> levels in the Arabian Sea, the northwest Pacific, and off the east coast of North America were also successfully captured. Radiance data were extracted from 13 major open-ocean zones, ranging from the subpolar to equatorial regions. Results from these extractions revealed the <span class="hlt">aerosol</span> load in both subpolar and subtropical zones to be higher in the Northern Hemisphere than in the Southern Hemisphere. <span class="hlt">Aerosol</span> radiances in the subtropics of both hemispheres were about 2 times higher in summer than in winter. In subpolar regions, <span class="hlt">aerosol</span> radiances in late spring/early summer were almost 3 times that observed in winter. In general, the <span class="hlt">aerosol</span> signal was higher during the warmer months and lower during the cooler months, irrespective of location. A comparison between our mean monthly <span class="hlt">aerosol</span> radiance maps with mean monthly chlorophyll maps (also from CZCS) showed similar seasonality between <span class="hlt">aerosol</span> and chlorophyll levels in the subpolar zones of both hemispheres, i.e., high levels in summer, low levels in winter. In the subtropics of both hemispheres, however, chlorophyll levels were higher in winter months which coincided with a depressed <span class="hlt">aerosol</span> signal. Our results indicate that the near-IR channel on ocean color sensors can be used to successfully capture well-known, large-<span class="hlt">scale</span> <span class="hlt">aerosol</span> plumes on a global <span class="hlt">scale</span> and that future ocean color sensors may provide a platform for long-term synoptic studies of combined <span class="hlt">aerosol</span>-phytoplankton productivity</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('http://hdl.handle.net/2060/20140010371','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140010371"><span>Global Analysis of <span class="hlt">Aerosol</span> Properties Above Clouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Waquet, F.; Peers, F.; Ducos, F.; Goloub, P.; Platnick, S. E.; Riedi, J.; Tanre, D.; Thieuleux, F.</p> <p>2013-01-01</p> <p>The seasonal and spatial varability of <span class="hlt">Aerosol</span> Above Cloud (AAC) properties are derived from passive satellite data for the year 2008. A significant amount of <span class="hlt">aerosols</span> are transported above liquid water clouds on the global <span class="hlt">scale</span>. For particles in the fine mode (i.e., radius smaller than 0.3 m), including both clear sky and AAC retrievals increases the global mean <span class="hlt">aerosol</span> optical thickness by 25(+/- 6%). The two main regions with man-made AAC are the tropical Southeast Atlantic, for biomass burning <span class="hlt">aerosols</span>, and the North Pacific, mainly for pollutants. Man-made AAC are also detected over the Arctic during the spring. Mineral dust particles are detected above clouds within the so-called dust belt region (5-40 N). AAC may cause a warming effect and bias the retrieval of the cloud properties. This study will then help to better quantify the impacts of <span class="hlt">aerosols</span> on clouds and climate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7840E..22B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7840E..22B"><span>Quantitative retrieval of <span class="hlt">aerosol</span> optical thickness from FY-2 VISSR data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bai, Linyan; Xue, Yong; Cao, Chunxiang; Feng, Jianzhong; Zhang, Hao; Guang, Jie; Wang, Ying; Li, Yingjie; Mei, Linlu; Ai, Jianwen</p> <p>2010-11-01</p> <p>Atmospheric <span class="hlt">aerosol</span>, as particulate matter suspended in the air, exists in a variety of forms such as dust, fume and mist. It deeply affects climate and land surface environment in both regional and global <span class="hlt">scales</span>, and furthermore, lead to be hugely much influence on human health. For the sake of effectively monitoring it, many atmospheric <span class="hlt">aerosol</span> observation networks are set up and provide associated informational services in the wide world, as well-known <span class="hlt">Aerosol</span> robotic network (AERONET), Canadian Sunphotometer Network (AeroCan) and so forth. Given large-<span class="hlt">scale</span> atmospheric <span class="hlt">aerosol</span> monitoring, that satellite remote sensing data are used to inverse <span class="hlt">aerosol</span> optical depth is one of available and effective approaches. Nowadays, special types of instruments aboard running satellites are applied to obtain related remote sensing data of retrieving atmospheric <span class="hlt">aerosol</span>. However, atmospheric <span class="hlt">aerosol</span> real-timely or near real-timely monitoring hasn't been accomplished. Nevertheless, retrievals, using Fengyun-2 VISSR data, are carried out and the above problem resolved to certain extent, especially over China. In this paper, the authors have developed a new retrieving model/mode to retrieve <span class="hlt">aerosol</span> optical depth, using Fengyun-2 satellite data that were obtained by the VISSR aboard FY-2C and FY-2D. A series of the <span class="hlt">aerosol</span> optical depth distribution maps with high time resolution were able to obtained, is helpful for understanding the forming mechanism, transport, influence and controlling approach of atmospheric <span class="hlt">aerosol</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AtmEn..41.1936C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AtmEn..41.1936C"><span>The continuous field measurements of soluble <span class="hlt">aerosol</span> compositions at the Taipei <span class="hlt">Aerosol</span> Supersite, Taiwan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chang, Shih-Yu; Lee, Chung-Te; Chou, Charles C.-K.; Liu, Shaw-Chen; Wen, Tian-Xue</p> <p></p> <p>The characteristics of ambient <span class="hlt">aerosols</span>, affected by solar radiation, relative humidity, wind speed, wind direction, and gas-<span class="hlt">aerosol</span> interaction, changed rapidly at different spatial and temporal <span class="hlt">scales</span>. In Taipei Basin, dense traffic emissions and sufficient solar radiation for typical summer days favored the formation of secondary <span class="hlt">aerosols</span>. In winter, the air quality in Taipei Basin was usually affected by the Asian continental outflows due to the long-range transport of pollutants carried by the winter monsoon. The conventional filter-based method needs a long time for collecting <span class="hlt">aerosols</span> and analyzing compositions, which cannot provide high time-resolution data to investigate <span class="hlt">aerosol</span> sources, atmospheric transformation processes, and health effects. In this work, the in situ ion chromatograph (IC) system was developed to provide 15-min time-resolution data of nine soluble inorganic species (Cl -, NO 2-, NO 3-, SO 42-, Na +, NH 4+, K +, Mg 2+ and Ca 2+). Over 89% of all particles larger than approximately 0.056 μm were collected by the in situ IC system. The in situ IC system is estimated to have a limit of detection lower than 0.3 μg m -3 for the various ambient ionic components. Depending on the hourly measurements, the pollutant events with high <span class="hlt">aerosol</span> concentrations in Taipei Basin were associated with the local traffic emission in rush hour, the accumulation of pollutants in the stagnant atmosphere, the emission of industrial pollutants from the nearby factories, the photochemical secondary <span class="hlt">aerosol</span> formation, and the long-range transport of pollutants from Asian outflows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.A32A..04M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.A32A..04M"><span>Diurnal Cycles of <span class="hlt">Aerosol</span> Optical Properties at Pico Tres Padres, Mexico City: Evidences for Changes in Particle Morphology and Secondary <span class="hlt">Aerosol</span> Formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mazzoleni, C.; Dubey, M.; Chakrabarty, R.; Moosmuller, H.; Onasch, T.; Zavala, M.; Herndon, S.; Kolb, C.</p> <p>2007-12-01</p> <p><span class="hlt">Aerosol</span> optical properties affect planetary radiative balance and depend on chemical composition, size distribution, and morphology. During the MILAGRO field campaign, we measured <span class="hlt">aerosol</span> absorption and scattering in Mexico City using the Los Alamos <span class="hlt">aerosol</span> photoacoustic (LAPA) instrument operating at 781 nm. The LAPA was mounted on-board the Aerodyne Research Inc. mobile laboratory, which hosted a variety of gaseous and <span class="hlt">aerosol</span> instruments. During the campaign, the laboratory was moved to different sites, capturing spatial and temporal variability. Additionally, we collected ambient <span class="hlt">aerosols</span> on Nuclepore filters for scanning electron microscopy (SEM) analysis. SEM images of selected filters were taken to study particle morphology. Between March 7th and 19th air was sampled at the top of Pico Tres Padres, a mountain on the north side of Mexico City. <span class="hlt">Aerosol</span> absorption and scattering followed diurnal patterns related to boundary layer <span class="hlt">height</span> and solar insulation. We report an analysis of <span class="hlt">aerosol</span> absorption, scattering, and morphology for three days (9th, 11th and 12th of March 2006). The single scattering albedo (SSA, ratio of scattering to total extinction) showed a drop in the tens-of-minutes-to-hour time frame after the boundary layer grew above the sampling site. Later in the day the SSA rose steadily reaching a maximum in the afternoon. The SEM images showed a variety of <span class="hlt">aerosol</span> shapes including fractal-like aggregates, spherical particles, and other shapes. The absorption correlated with the CO2 signal and qualitatively with the fraction of fractal-like particles to the total particle count. In the afternoon the SSA qualitatively correlated with a relative increase in spherical particles and total particle count. These observed changes in optical properties and morphology can be explained by the dominant contribution of freshly emitted particles in the morning and by secondary particle formation in the afternoon. SSA hourly averaged values ranged from ~0.63 in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28453166','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28453166"><span>An analysis of the relationship between bodily injury severity and fall <span class="hlt">height</span> in victims of fatal falls from <span class="hlt">height</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Teresiński, Grzegorz; Milaszkiewicz, Anna; Cywka, Tomasz</p> <p>2016-01-01</p> <p>Aim of the study: One of the basic issues discussed in forensic literature regarding falls from a <span class="hlt">height</span> is determination of fall <span class="hlt">heights</span> and differentiation between suicidal and accidental falls. The aim of the study was to verify the usefulness of the available methods for the purposes of forensic expertises. Material and methods: The study encompassed fatalities of falls from a <span class="hlt">height</span> whose autopsies were performed in the Department of Forensic Medicine in Lublin. Results: Similarly to other authors, the severity of injuries was assessed using the <i>Abbreviated Injury <span class="hlt">Scale</span> </i>(AIS) and injury severity score (ISS). The study findings demonstrated a statistically significant correlation between the fall <span class="hlt">height</span> and the severity of injuries according to ISS and a statistically significant difference in fall <span class="hlt">heights</span> between the groups of accidents and suicides.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120014997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120014997"><span>Impact of <span class="hlt">Aerosols</span> on Convective Clouds and Precipitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tao, Wei-Kuo; Chen, Jen-Ping; Li, Zhanqing; Wang, Chien; Zhang, Chidong; Li, Xiaowen</p> <p>2012-01-01</p> <p><span class="hlt">Aerosols</span> are a critical.factor in the atmospheric hydrological cycle and radiation budget. As a major agent for clouds to form and a significant attenuator of solar radiation, <span class="hlt">aerosols</span> affect climate in several ways. Current research suggests that <span class="hlt">aerosols</span> have a major impact on the dynamics, microphysics, and electrification properties of continental mixed-phase convective clouds. In addition, high <span class="hlt">aerosol</span> concentrations in urban environments could affect precipitation variability by providing a significant source of cloud condensation nuclei (CCN). Such pollution . effects on precipitation potentially have enormous climatic consequences both in terms of feedbacks involving the land surface via rainfall as well as the surface energy budget and changes in latent heat input to the atmosphere. Basically, <span class="hlt">aerosol</span> concentrations can influence cloud droplet size distributions, the warm-rain process, the cold-rain process, cloud-top <span class="hlt">heights</span>, the depth of the mixed-phase region, and the occurrence of lightning. Recently, many cloud resolution models (CRMs) have been used to examine the role of <span class="hlt">aerosols</span> on mixed-phase convective clouds. These modeling studies have many differences in terms of model configuration (two- or three-dimensional), domain size, grid spacing (150-3000 m), microphysics (two-moment bulk, simple or sophisticated spectral-bin), turbulence (1st or 1.5 order turbulent kinetic energy (TKE)), radiation, lateral boundary conditions (i.e., closed, radiative open or cyclic), cases (isolated convection, tropical or midlatitude squall lines) and model integration time (e.g., 2.5 to 48 hours). Among these modeling studies, the most striking difference is that cumulative precipitation can either increase or decrease in response to higher concentrations of CCN. In this presentation, we review past efforts and summarize our current understanding of the effect of <span class="hlt">aerosols</span> on convective precipitation processes. Specifically, this paper addresses the following topics</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214330N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214330N"><span>Synchronised <span class="hlt">Aerosol</span> Mass Spectrometer Measurements across Europe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nemitz, Eiko</p> <p>2010-05-01</p> <p>Up to twelve Aerodyne <span class="hlt">Aerosol</span> Mass Spectrometers (AMSs) were operated simultaneously at rural and background stations (EMEP and EUSAAR sites) across Europe. Measurements took place during three intensive periods, in collaboration between the European EUCAARI IP and the EMEP monitoring activities under the UNECE Convention for Long-Range Transboundary Air Pollution (CLRTAP) during three contrasting months (May 2008, Sep/Oct 2008, Feb/Mar 2009). These measurements were conducted, analysed and quality controlled carefully using a unified protocol, providing the largest spatial database of <span class="hlt">aerosol</span> chemical composition measured with a unified online technique to date, and a unique snapshots of the European non-refractory submicron <span class="hlt">aerosol</span> climatology. As campaign averages over all active monitoring sites, organics represent 28 to 43%, sulphate 18 to 25%, ammonium 13 to 15% and nitrate 15 to 36% of the resolved <span class="hlt">aerosol</span> mass, with the highest relative nitrate contribution during the Feb/Mar campaign. The measurements demonstrate that in NW Europe (e.g. Ireland, UK, The Netherlands, Germany, Switzerland) the regional submicron <span class="hlt">aerosol</span> tends to be neutralised and here nitrates make a major contribution to the <span class="hlt">aerosol</span> mass. By contrast, periods with low nitrate and acidic <span class="hlt">aerosol</span> were observed at sites in S and E Europe (e.g. Greece, Finland), presumably due to a combination of larger SO2 point sources in Easter Europe, smaller local NH3 sources and, in the case of Greece, higher temperatures. While at the more marine and remote sites (Ireland, Scotland, Finland) nitrate concentrations were dominated by episodic transport phenomena, at continental sites (Switzerland, Germany, Hungary) nitrate followed a clear diurnal cycle, reflecting the thermodynamic behaviour of ammonium nitrate. The datasets clearly shows spatially co-ordinated, large-<span class="hlt">scale</span> pollution episodes of organics, sulphate and nitrate, the latter being most pronounced during the Feb/Mar campaign. At selected</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4815K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4815K"><span>Impact of <span class="hlt">aerosols</span>, dust, water vapor and clouds on fair weather PG and implications for the Carnegie curve</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kourtidis, Konstantinos; Georgoulias, Aristeidis</p> <p>2017-04-01</p> <p>We studied the impact of anthropogenic <span class="hlt">aerosols</span>, fine mode natural <span class="hlt">aerosols</span>, Saharan dust, atmospheric water vapor, cloud fraction, cloud optical depth and cloud top <span class="hlt">height</span> on the magnitude of fair weather PG at the rural station of Xanthi. Fair weather PG was measured in situ while the other parameters were obtained from the MODIS instrument onboard the Terra and Aqua satellites. All of the above parameteres were found to impact fair weather PG magnitude. Regarding <span class="hlt">aerosols</span>, the impact was larger for Saharan dust and fine mode natural <span class="hlt">aerosols</span> whereas regarding clouds the impact was larger for cloud fraction while less than that of <span class="hlt">aerosols</span>. Water vapour and ice precipitable water were also found to influence fair weather PG. Since <span class="hlt">aerosols</span> and water are ubiquitous in the atmosphere and exhibit large spatial and temporal variability, we postulate that our understanding of the Carnegie curve might need revision.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.3097M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.3097M"><span>Classification of summertime synoptic patterns in Beijing and their associations with boundary layer structure affecting <span class="hlt">aerosol</span> pollution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miao, Yucong; Guo, Jianping; Liu, Shuhua; Liu, Huan; Li, Zhanqing; Zhang, Wanchun; Zhai, Panmao</p> <p>2017-02-01</p> <p>Meteorological conditions within the planetary boundary layer (PBL) are closely governed by large-<span class="hlt">scale</span> synoptic patterns and play important roles in air quality by directly and indirectly affecting the emission, transport, formation, and deposition of air pollutants. Partly due to the lack of long-term fine-resolution observations of the PBL, the relationships between synoptic patterns, PBL structure, and <span class="hlt">aerosol</span> pollution in Beijing have not been well understood. This study applied the obliquely rotated principal component analysis in T-mode to classify the summertime synoptic conditions over Beijing using the National Centers for Environmental Prediction reanalysis from 2011 to 2014, and investigated their relationships with PBL structure and <span class="hlt">aerosol</span> pollution by combining numerical simulations, measurements of surface meteorological variables, fine-resolution soundings, the concentration of particles with diameters less than or equal to 2.5 µm, total cloud cover (CLD), and reanalysis data. Among the seven identified synoptic patterns, three types accounted for 67 % of the total number of cases studied and were associated with heavy <span class="hlt">aerosol</span> pollution events. These particular synoptic patterns were characterized by high-pressure systems located to the east or southeast of Beijing at the 925 hPa level, which blocked the air flow seaward, and southerly PBL winds that brought in polluted air from the southern industrial zone. The horizontal transport of pollutants induced by the synoptic forcings may be the most important factor affecting the air quality of Beijing in summer. In the vertical dimension, these three synoptic patterns featured a relatively low boundary layer <span class="hlt">height</span> (BLH) in the afternoon, accompanied by high CLD and southerly cold advection from the seas within the PBL. The high CLD reduced the solar radiation reaching the surface, and suppressed the thermal turbulence, leading to lower BLH. Besides, the numerical sensitive experiments show that cold</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080040177','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080040177"><span>A Satellite-based Assessment of Trans-Pacific Transport of Pollution <span class="hlt">Aerosol</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, Hongbin; Remer, Lorraine; Chin, Mian; Bian, Huisheng; Kleidman, Richard; Diehl. Thomas</p> <p>2007-01-01</p> <p>It has been well documented that pollution <span class="hlt">aerosol</span> and dust from East Asia can transport across the North Pacific basin, reaching North America and beyond. Such intercontinental transport extends the impact of <span class="hlt">aerosols</span> for climate change, air quality, atmospheric chemistry, and ocean biology from local and regional <span class="hlt">scales</span> to hemispheric and global <span class="hlt">scales</span>. Long term, measurement-based studies are necessary to adequately assess the implications of these wider impacts. A satellite-based assessment can augment intensive field campaigns by expanding temporal and spatial <span class="hlt">scales</span> and also serve as constraints for model simulations. Satellite imagers have been providing a wealth of evidence for the intercontinental transport of <span class="hlt">aerosols</span> for more than two decades. Quantitative assessments, however, became feasible only recently as a result of the much improved measurement accuracy and enhanced new capabilities of satellite sensors. In this study, we generated a 4-year (2002 to 2005) climatology of optical depth for pollution <span class="hlt">aerosol</span> (defined as a mixture of <span class="hlt">aerosols</span> from urbanlindustrial pollution and biomass burning in this study) over the North Pacific from MODerate resolution Imaging Spectro-radiometer (MODIS) observations of fine- and coarse-mode <span class="hlt">aerosol</span> optical depths. The pollution <span class="hlt">aerosol</span> mass loading and fluxes were then calculated using measurements of the dependence of <span class="hlt">aerosol</span> mass extinction efficiency on relative humidity and of <span class="hlt">aerosol</span> vertical distributions from field campaigns and available satellite observations in the region. We estimated that about 18 Tg/year pollution <span class="hlt">aerosol</span> is exported from East Asia to the northwestern Pacific Ocean, of which about 25% reaches the west coast of North America. The pollution fluxes are largest in spring and smallest in summer. For the period we have examined the strongest export and import of pollution particulates occurred in 2003, due largely to record intense Eurasia wildfires in spring and summer. The overall</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.A13B0258P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.A13B0258P"><span>Re-reading the IPCC Report: <span class="hlt">Aerosols</span>, Droughts and ENSO Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Potts, K. A.</p> <p>2008-12-01</p> <p>The Technical Summary of Working Group One in the IPCC Fourth Assessment Report states that "changes in <span class="hlt">aerosols</span> may have affected precipitation and other aspects of the hydrologic cycle more strongly than other anthropogenic forcing agents" and that "Simulations also suggest that absorbing <span class="hlt">aerosols</span>, particularly black carbon, can reduce the solar radiation reaching the surface and can warm the atmosphere at regional <span class="hlt">scales</span>, affecting the vertical temperature profile and the large-<span class="hlt">scale</span> atmospheric circulation". Taking these two statements at face value I first identify eight seasonal, anthropogenic, regional <span class="hlt">scale</span>, <span class="hlt">aerosol</span> plumes which now occur each year and then report the correlation of the <span class="hlt">aerosol</span> optical depth (AOD) of some of these plumes with climate anomalies in the higher latitudes and with ENSO events. The eight identified <span class="hlt">aerosol</span> plumes vary significantly in extent and AOD inter annually. They have also increased in geographic extent and AOD over recent decades as the population in the tropics, the origin of the majority of these plumes, has increased dramatically requiring increased levels of agriculture and commercial activity. I show that: the AOD of the South East Asian Plume, occurring from late July to November, correlates with four characteristics of drought in south eastern Australia; the <span class="hlt">aerosol</span> index of the Middle East Plume correlates negatively with rainfall in Darfur; and the volume of tephra ejected by volcanoes in south east Asia correlates: negatively with rainfall and water inflows into the Murray River in south eastern Australia; and positively with ENSO events over the period 1890/91 to 2006. I conclude that <span class="hlt">aerosol</span> plumes over south eastern Asia are the cause of drought in south eastern Australia and ENSO events and confirm the statements made in the IPCC Report with respect to these <span class="hlt">aerosol</span> plumes. I propose a new component of surface <span class="hlt">aerosol</span> radiative forcing, Regional Dimming, which interferes with the seasonal movement of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51E2121Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51E2121Z"><span><span class="hlt">Aerosol</span> Microphysical Effects on Cloud Fraction over the Nighttime Arctic Ocean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zamora, L. M.; Kahn, R. A.; Stohl, A.; Eckhardt, S.</p> <p>2017-12-01</p> <p>Cloud fraction is a key component affecting the surface energy balance in the Arctic. <span class="hlt">Aerosol</span> microphysical processes can affect cloud fraction, for example through cloud lifetime effects. However, the importance of <span class="hlt">aerosol</span> impacts on cloud fraction is not well constrained on a regional <span class="hlt">scale</span> at high latitudes. Here we discuss a new method for identifying and comparing clean and <span class="hlt">aerosol</span>-influenced cloud characteristics using a combination of multi-year remote sensing data (CALIPSO, CloudSat) and the FLEXPART <span class="hlt">aerosol</span> model. We use this method to investigate a variety of <span class="hlt">aerosol</span> microphysical impacts on nighttime Arctic Ocean clouds on regional and local <span class="hlt">scales</span>. We observe differences in factors that can impact cloud lifetime, including cloud thickness and phase, within a subset of clean vs. polluted clouds. We will also discuss cumulative cloud fraction differences in clean and non-clean environments, as well as their likely impact on longwave cloud radiative effects at the Arctic Ocean surface during polar night.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1714640Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714640Z"><span>The Regional Environmental Impacts of Atmospheric <span class="hlt">Aerosols</span> over Egypt</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zakey, Ashraf; Ibrahim, Alaa</p> <p>2015-04-01</p> <p>Identifying the origin (natural versus anthropogenic) and the dynamics of <span class="hlt">aerosols</span> over Egypt at varying temporal and spatial <span class="hlt">scales</span> provide valuable knowledge on the regional climate impacts of <span class="hlt">aerosols</span> and their ultimate connections to the Earth's regional climate system at the MENA region. At regional <span class="hlt">scale</span>, Egypt is exposed to air pollution with levels exceeding typical air-quality standards. This is particularly true for the Nile Delta region, being at the crossroads of different <span class="hlt">aerosol</span> species originating from local urban-industrial and biomass-burning activities, regional dust sources, and European pollution from the north. The Environmental Climate Model (EnvClimA) is used to investigate both of the biogenic and anthropogenic <span class="hlt">aerosols</span> over Egypt. The dominant natural <span class="hlt">aerosols</span> over Egypt are due to the sand and dust storms, which frequently occur during the transitional seasons (spring and autumn). In winter, the maximum frequency reaches 2 to 3 per day in the north, which decreases gradually southward with a frequency of 0.5-1 per day. Monitoring one of the most basic <span class="hlt">aerosol</span> parameters, the <span class="hlt">aerosol</span> optical depth (AOD), is a main experimental and modeling task in <span class="hlt">aerosol</span> studies. We used the <span class="hlt">aerosol</span> optical depth to quantify the amount and variability of <span class="hlt">aerosol</span> loading in the atmospheric column over a certain areas. The <span class="hlt">aerosols</span> optical depth from the model is higher in spring season due to the impacts of dust activity over Egypt as results of the westerly wind, which carries more dust particles from the Libyan Desert. The model result shows that the mass load of fine <span class="hlt">aerosols</span> has a longer life-time than the coarse <span class="hlt">aerosols</span>. In autumn season, the modelled <span class="hlt">aerosol</span> optical depth tends to increase due to the biomass burning in the delta of Egypt. Natural <span class="hlt">aerosol</span> from the model tends to scatter the solar radiation while most of the anthropogenic <span class="hlt">aerosols</span> tend to absorb the longwave solar radiation. The overall results indicate that the AOD is lowest in winter</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991PhDT.......141B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991PhDT.......141B"><span>Atmospheric Residence Times of Continental <span class="hlt">Aerosols</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Balkanski, Yves Jacques</p> <p></p> <p>The global atmospheric distributions of ^{222}Rn and ^{210 }Pb are simulated with a three-dimensional model of atmospheric transport based on the meteorology of the NASA GISS^1>=neral circulation model. The short-lived radioactive gas ^ {222}Rn (half-life = 3.8d) is emitted almost exclusively from land, at a relatively uniform rate; hence it is an excellent tracer of continental influences. Lead -210 is produced by decay of ^{222} Rn and immediately condenses to preexisting <span class="hlt">aerosol</span> surfaces. It provides an excellent measure of <span class="hlt">aerosol</span> residence times in the atmosphere because its source is accurately defined by the ^{222} Rn distribution. Results from the three-dimensional model are compared to measurements of ^ {222}Rn and ^{210 }Pb atmospheric concentrations to evaluate model's long-range transport over oceanic regions and to study the deposition mechanisms of atmospheric <span class="hlt">aerosols</span>. Model results for ^{222} Rn are used to examine the long-range transport of continental air over two selected oceanic regions, the subantartic Indian Ocean and the North Pacific. It is shown that fast transport of air from southern Africa causes substantial continental pollution at southern mid-latitudes, a region usually regarded as pristine. Air over the North Pacific is heavily impacted by continental influences year round, but the altitude at which the transport occurs varies seasonally. Observations of <span class="hlt">aerosols</span> at island sites, which are commonly used as diagnostics of continental influences, may be misleading because they do not account for influences at high altitude and because <span class="hlt">aerosols</span> are efficiently scavenged by deposition during transport. The study of ^{210}Pb focuses on defining the residence times of submicron <span class="hlt">aerosols</span> in the troposphere. Scavenging in wet convective updrafts is found to provide the dominant sink on a global <span class="hlt">scale</span>. The globally averaged residence time for ^{210 }Pb-containing <span class="hlt">aerosols</span> in the troposphere is 7 days. The average increase in residence time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110007955&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dvertical%2Bheight','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110007955&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dvertical%2Bheight"><span>The Vertical Distribution of Thin Features Over the Arctic Analysed from CALIPSO Observations. Part 2; <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Devasthale, Abhya; Tjernstrom, Michael; Omar, Ali H.</p> <p>2010-01-01</p> <p>Influx of <span class="hlt">aerosols</span> from the mid-latitudes has a wide range of impacts on the Arctic atmosphere. In this study, the capability of the CALIPSO-CALIOP instrument to provide accurate observations of <span class="hlt">aerosol</span> layers is exploited to characterize their vertical distribution, probability density functions (PDFs) of <span class="hlt">aerosol</span> layer thickness, base and top <span class="hlt">heights</span>, and optical depths over the Arctic for the 4-yr period from June 2006 to May 2010. It is shown that the bulk of <span class="hlt">aerosols</span>, from about 65% in winter to 45% in summer, are confined below the lowermost kilometer of the troposphere. In the middle troposphere (3-5 km), spring and autumn seasons show slightly higher <span class="hlt">aerosol</span> amounts compared to other two seasons. The relative vertical distribution of <span class="hlt">aerosols</span> shows that clean continental <span class="hlt">aerosol</span> is the largest contributor in all seasons except in summer, when layers of polluted continental <span class="hlt">aerosols</span> are almost as large. In winter and spring, polluted continental <span class="hlt">aerosols</span> are the second largest contributor to the total number of observed <span class="hlt">aerosol</span> layers, whereas clean marine <span class="hlt">aerosol</span> is the second largest contributor in summer and autumn. The PDFs of the geometrical thickness of the observed <span class="hlt">aerosol</span> layers peak about 400-700 m. Polluted continental and smoke <span class="hlt">aerosols</span>, which are associated with the intrusions from mid-latitudes, have much broader distributions of optical and geometrical thicknesses, suggesting that they appear more often optically thicker and higher up in the troposphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A44E..02F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A44E..02F"><span>Narrowing the Gap in Quantification of <span class="hlt">Aerosol</span>-Cloud Radiative Effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feingold, G.; McComiskey, A. C.; Yamaguchi, T.; Kazil, J.; Johnson, J. S.; Carslaw, K. S.</p> <p>2016-12-01</p> <p>Despite large advances in our understanding of <span class="hlt">aerosol</span> and cloud processes over the past years, uncertainty in the <span class="hlt">aerosol</span>-cloud radiative effect/forcing is still of major concern. In this talk we will advocate a methodology for quantifying the <span class="hlt">aerosol</span>-cloud radiative effect that considers the primacy of fundamental cloud properties such as cloud amount and albedo alongside the need for process level understanding of <span class="hlt">aerosol</span>-cloud interactions. We will present a framework for quantifying the <span class="hlt">aerosol</span>-cloud radiative effect, regime-by-regime, through process-based modelling and observations at the large eddy <span class="hlt">scale</span>. We will argue that understanding the co-variability between meteorological and <span class="hlt">aerosol</span> drivers of the radiative properties of the cloud system may be as important an endeavour as attempting to untangle these drivers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A54F..03M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A54F..03M"><span>Investigating the influence of volcanic sulfate <span class="hlt">aerosol</span> on cloud properties Along A-Train tracks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mace, G. G.</p> <p>2017-12-01</p> <p>Marine boundary layer (MBL) clouds are central actors in the climate system given their extensive coverage on the Earth's surface, their 1-way influence on the radiative balance (cooling), and their intimate coupling between air motions, anthropogenic and natural <span class="hlt">aerosol</span> sources, and processes within the upper ocean mixed layer. Knowledge of how MBL shallow cumulus clouds respond to changes in <span class="hlt">aerosol</span> is central to understanding how MBL clouds modulate the climate system. A frequent approach to investigating how sulfate <span class="hlt">aerosol</span> influences MBL clouds has been to examine sulfate plumes extending downstream of active island volcanoes. This approach is challenging due to modification of the air motions in the plumes downstream of islands and due to the tendency of most researchers to examine only level-2 retrievals ignoring the actual data collected by sensors such as MODIS. Past studies have concluded that sulfate <span class="hlt">aerosols</span> have large effects consistent with the 1st <span class="hlt">aerosol</span> indirect effect (AIE). We reason that if such effects are as large as suggested in level-2 retrievals then evidence should also be present in the raw MODIS reflectance data as well as other data sources. In this paper we will build on our recently published work where we tested that hypothesis from data collected near Mount Kilauea during a 3-year period. Separating data into <span class="hlt">aerosol</span> optical depth (A) quartiles, we found little support for a large 1st AIE response. We did find an unambiguous increase in sub 1km-<span class="hlt">scale</span> cloud fraction with A. This increase in sub 1 km cloud fraction was entirely consistent with increased reflectance with increasing A that is used, via the level 2 retrievals, to argue for a large AIE response of MBL clouds. While the 1-km pixels became unambiguously brighter, that brightening was due to increased sub 1 km cloud fraction and not necessarily due to changes in pixel-level cloud microphysics. We also found that MBL cloud top <span class="hlt">heights</span> increase as do surface wind speeds as</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1229987-wave-like-signatures-aerosol-optical-depth-associated-radiative-impacts-over-central-himalayan-region','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1229987-wave-like-signatures-aerosol-optical-depth-associated-radiative-impacts-over-central-himalayan-region"><span>Wave like signatures in <span class="hlt">aerosol</span> optical depth and associated radiative impacts over the central Himalayan region</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>Shukla, K. K.; Phanikumar, D. V.; Kumar, K.  Niranjan</p> <p>2015-10-01</p> <p>In this study, we present a case study on 16 October 2011 to show the first observational evidence of the influence of short period gravity waves in <span class="hlt">aerosol</span> transport during daytime over the central Himalayan region. The Doppler lidar data has been utilized to address the daytime boundary layer evolution and related <span class="hlt">aerosol</span> dynamics over the site. Mixing layer <span class="hlt">height</span> is estimated by wavelet covariance transform method and found to be ~ 0.7 km, AGL. <span class="hlt">Aerosol</span> optical depth observations during daytime revealed an asymmetry showing clear enhancement during afternoon hours as compared to forenoon. Interestingly, Fourier and wavelet analysis ofmore » vertical velocity and attenuated backscatter showed similar 50-90 min short period gravity wave signatures during afternoon hours. Moreover, our observations showed that gravity waves are dominant within the boundary layer implying that the daytime boundary layer dynamics is playing a vital role in transporting the <span class="hlt">aerosols</span> from surface to the top of the boundary layer. Similar modulations are also evident in surface parameters like temperature, relative humidity and wind speed indicating these waves are associated with the dynamical aspects over Himalayan region. Finally, time evolution of range-23 <span class="hlt">height</span> indicator snapshots during daytime showed strong upward velocities especially during afternoon hours implying that convective processes through short period gravity waves plays a significant role in transporting <span class="hlt">aerosols</span> from the nearby valley region to boundary layer top over the site. These observations also establish the importance of wave induced daytime convective boundary layer dynamics in the lower Himalayan region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A41G0135B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A41G0135B"><span>Separating Dust Mixtures and Other External <span class="hlt">Aerosol</span> Mixtures Using Airborne High Spectral Resolution Lidar Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burton, S. P.; Ferrare, R. A.; Vaughan, M.; Hostetler, C. A.; Rogers, R. R.; Hair, J. W.; Cook, A. L.; Harper, D. B.</p> <p>2013-12-01</p> <p>Knowledge of <span class="hlt">aerosol</span> type is important for source attribution and for determining the magnitude and assessing the consequences of <span class="hlt">aerosol</span> radiative forcing. The NASA Langley Research Center airborne High Spectral Resolution Lidar (HSRL-1) has acquired considerable datasets of both <span class="hlt">aerosol</span> extensive parameters (e.g. <span class="hlt">aerosol</span> optical depth) and intensive parameters (e.g. <span class="hlt">aerosol</span> depolarization ratio, lidar ratio) that can be used to infer <span class="hlt">aerosol</span> type. An <span class="hlt">aerosol</span> classification methodology has been used extensively to classify HSRL-1 <span class="hlt">aerosol</span> measurements of different <span class="hlt">aerosol</span> types including dust, smoke, urban pollution, and marine <span class="hlt">aerosol</span>. However, atmospheric <span class="hlt">aerosol</span> is frequently not a single pure type, but instead occurs as a mixture of types, and this mixing affects the optical and radiative properties of the <span class="hlt">aerosol</span>. Here we present a comprehensive and unified set of rules for characterizing external mixtures using several key <span class="hlt">aerosol</span> intensive parameters: extinction-to-backscatter ratio (i.e. lidar ratio), backscatter color ratio, and depolarization ratio. Our mixing rules apply not just to the scalar values of <span class="hlt">aerosol</span> intensive parameters, but to multi-dimensional normal distributions with variance in each measurement dimension. We illustrate the applicability of the mixing rules using examples of HSRL-1 data where mixing occurred between different <span class="hlt">aerosol</span> types, including advected Saharan dust mixed with the marine boundary layer in the Caribbean Sea and locally generated dust mixed with urban pollution in the Mexico City surroundings. For each of these cases we infer a time-<span class="hlt">height</span> cross section of mixing ratio along the flight track and we partition <span class="hlt">aerosol</span> extinction into portions attributed to the two pure types. Since multiple <span class="hlt">aerosol</span> intensive parameters are measured and included in these calculations, the techniques can also be used for cases without significant depolarization (unlike similar work by earlier researchers), and so a third example of a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A33J3325A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A33J3325A"><span>Assessment of 10-Year Global Record of <span class="hlt">Aerosol</span> Products from the OMI Near-UV Algorithm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahn, C.; Torres, O.; Jethva, H. T.</p> <p>2014-12-01</p> <p>Global observations of <span class="hlt">aerosol</span> properties from space are critical for understanding climate change and air quality applications. The Ozone Monitoring Instrument (OMI) onboard the EOS-Aura satellite provides information on <span class="hlt">aerosol</span> optical properties by making use of the large sensitivity to <span class="hlt">aerosol</span> absorption and dark surface albedo in the UV spectral region. These unique features enable us to retrieve both <span class="hlt">aerosol</span> extinction optical depth (AOD) and single scattering albedo (SSA) successfully from radiance measurements at 354 and 388 nm by the OMI near UV <span class="hlt">aerosol</span> algorithm (OMAERUV). Recent improvements to algorithms in conjunction with the Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization (CALIOP) and Atmospheric Infrared Sounder (AIRS) carbon monoxide data also reduce uncertainties due to <span class="hlt">aerosol</span> layer <span class="hlt">heights</span> and types significantly in retrieved products. We present validation results of OMI AOD against space and time collocated <span class="hlt">Aerosol</span> Robotic Network (AERONET) measured AOD values over multiple stations representing major <span class="hlt">aerosol</span> episodes and regimes. We also compare the OMI SSA against the inversion made by AERONET as well as an independent network of ground-based radiometer called SKYNET in Japan, China, South-East Asia, India, and Europe. The outcome of the evaluation analysis indicates that in spite of the "row anomaly" problem, affecting the sensor since mid-2007, the long-term <span class="hlt">aerosol</span> record shows remarkable sensor stability. The OMAERUV 10-year global <span class="hlt">aerosol</span> record is publicly available at the NASA data service center web site (http://disc.sci.gsfc.nasa.gov/Aura/data-holdings/OMI/omaeruv_v003.shtml).</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/2015GMD.....8..549A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GMD.....8..549A"><span>Characterising Brazilian biomass burning emissions using WRF-Chem with MOSAIC sectional <span class="hlt">aerosol</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Archer-Nicholls, S.; Lowe, D.; Darbyshire, E.; Morgan, W. T.; Bela, M. M.; Pereira, G.; Trembath, J.; Kaiser, J. W.; Longo, K. M.; Freitas, S. R.; Coe, H.; McFiggans, G.</p> <p>2015-03-01</p> <p>The South American Biomass Burning Analysis (SAMBBA) field campaign took detailed in situ flight measurements of <span class="hlt">aerosol</span> during the 2012 dry season to characterise biomass burning <span class="hlt">aerosol</span> and improve understanding of its impacts on weather and climate. Developments have been made to the Weather Research and Forecast model with chemistry (WRF-Chem) model to improve the representation of biomass burning <span class="hlt">aerosol</span> in the region, by coupling a sectional <span class="hlt">aerosol</span> scheme to the plume-rise parameterisation. Brazilian Biomass Burning Emissions Model (3BEM) fire emissions are used, prepared using PREP-CHEM-SRC, and mapped to CBM-Z and MOSAIC species. Model results have been evaluated against remote sensing products, AERONET sites, and four case studies of flight measurements from the SAMBBA campaign. WRF-Chem predicted layers of elevated <span class="hlt">aerosol</span> loadings (5-20 μg sm-3) of particulate organic matter at high altitude (6-8 km) over tropical forest regions, while flight measurements showed a sharp decrease above 2-4 km altitude. This difference was attributed to the plume-rise parameterisation overestimating injection <span class="hlt">height</span>. The 3BEM emissions product was modified using estimates of active fire size and burned area for the 2012 fire season, which reduced the fire size. The enhancement factor for fire emissions was increased from 1.3 to 5 to retain reasonable <span class="hlt">aerosol</span> optical depths (AODs). The smaller fire size lowered the injection <span class="hlt">height</span> of the emissions, but WRF-Chem still showed elevated <span class="hlt">aerosol</span> loadings between 4-5 km altitude. Over eastern cerrado (savannah-like) regions, both modelled and measured <span class="hlt">aerosol</span> loadings decreased above approximately 4 km altitude. Compared with MODIS satellite data and AERONET sites, WRF-Chem represented AOD magnitude well (between 0.3-1.5) over western tropical forest fire regions in the first half of the campaign, but tended to over-predict them in the second half, when precipitation was more significant. Over eastern cerrado regions, WRF</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GMDD....7.6061A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GMDD....7.6061A"><span>Characterising Brazilian biomass burning emissions using WRF-Chem with MOSAIC sectional <span class="hlt">aerosol</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Archer-Nicholls, S.; Lowe, D.; Darbyshire, E.; Morgan, W. T.; Bela, M. M.; Pereira, G.; Trembath, J.; Kaiser, J. W.; Longo, K. M.; Freitas, S. R.; Coe, H.; McFiggans, G.</p> <p>2014-09-01</p> <p>The South American Biomass Burning Analysis (SAMBBA) field campaign took detailed in-situ flight measurements of <span class="hlt">aerosol</span> during the 2012 dry season to characterise biomass burning <span class="hlt">aerosol</span> and improve understanding of its impacts on weather and climate. Developments have been made to the Weather research and Forecast model with chemistry (WRF-Chem) model to improve the representation of biomass burning <span class="hlt">aerosol</span> in the region by coupling a sectional <span class="hlt">aerosol</span> scheme to the plume rise parameterisation. Brazilian Biomass Burning Emissions Model (3BEM) fire emissions are used, prepared using PREP-CHEM-SRC, and mapped to CBM-Z and MOSAIC species. Model results have been evaluated against remote sensing products, AERONET sites, and four case studies of flight measurements from the SAMBBA campaign. WRF-Chem predicted layers of elevated <span class="hlt">aerosol</span> loadings (5-20 μg sm-3) of particulate organic matter at high altitude (6-8 km) over tropical forest regions, while flight measurements showed a sharp decrease above 2-4 km altitude. This difference was attributed to the plume-rise parameterisation overestimating injection <span class="hlt">height</span>. The 3BEM emissions product was modified using estimates of active fire size and burned area for the 2012 fire season, which reduced the fire size. The enhancement factor for fire emissions was increased from 1.3 to 5 to retain reasonable <span class="hlt">aerosol</span> optical depths (AOD). The smaller fire size lowered the injection <span class="hlt">height</span> of the emissions, but WRF-Chem still showed elevated <span class="hlt">aerosol</span> loadings between 4-5 km altitude. Over eastern Cerrado (savannah-like) regions, both modelled and measured <span class="hlt">aerosol</span> loadings decreased above approximately 4 km altitude. Compared with MODIS satellite data and AERONET sites, WRF-Chem represented AOD magnitude well (between 0.3-1.5) over western tropical forest fire regions in the first half of the campaign, but tended to over-predict them in the second half, when precipitation was more significant. Over eastern Cerrado regions, WRF</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24601011','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24601011"><span>Aqueous <span class="hlt">aerosol</span> SOA formation: impact on <span class="hlt">aerosol</span> physical properties.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Woo, Joseph L; Kim, Derek D; Schwier, Allison N; Li, Ruizhi; McNeill, V Faye</p> <p>2013-01-01</p> <p>Organic chemistry in <span class="hlt">aerosol</span> water has recently been recognized as a potentially important source of secondary organic <span class="hlt">aerosol</span> (SOA) material. This SOA material may be surface-active, therefore potentially affecting <span class="hlt">aerosol</span> heterogeneous activity, ice nucleation, and CCN activity. Aqueous <span class="hlt">aerosol</span> chemistry has also been shown to be a potential source of light-absorbing products ("brown carbon"). We present results on the formation of secondary organic <span class="hlt">aerosol</span> material in <span class="hlt">aerosol</span> water and the associated changes in <span class="hlt">aerosol</span> physical properties from GAMMA (Gas-<span class="hlt">Aerosol</span> Model for Mechanism Analysis), a photochemical box model with coupled gas and detailed aqueous <span class="hlt">aerosol</span> chemistry. The detailed <span class="hlt">aerosol</span> composition output from GAMMA was coupled with two recently developed modules for predicting a) <span class="hlt">aerosol</span> surface tension and b) the UV-Vis absorption spectrum of the <span class="hlt">aerosol</span>, based on our previous laboratory observations. The simulation results suggest that the formation of oligomers and organic acids in bulk <span class="hlt">aerosol</span> water is unlikely to perturb <span class="hlt">aerosol</span> surface tension significantly. Isoprene-derived organosulfates are formed in high concentrations in acidic <span class="hlt">aerosols</span> under low-NO(x) conditions, but more experimental data are needed before the potential impact of these species on <span class="hlt">aerosol</span> surface tension may be evaluated. Adsorption of surfactants from the gas phase may further suppress <span class="hlt">aerosol</span> surface tension. Light absorption by aqueous <span class="hlt">aerosol</span> SOA material is driven by dark glyoxal chemistry and is highest under high-NO(x) conditions, at high relative humidity, in the early morning hours. The wavelength dependence of the predicted absorption spectra is comparable to field observations and the predicted mass absorption efficiencies suggest that aqueous <span class="hlt">aerosol</span> chemistry can be a significant source of <span class="hlt">aerosol</span> brown carbon under urban conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016RvGeo..54..866L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RvGeo..54..866L"><span><span class="hlt">Aerosol</span> and monsoon climate interactions over Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Zhanqing; Lau, W. K.-M.; Ramanathan, V.; Wu, G.; Ding, Y.; Manoj, M. G.; Liu, J.; Qian, Y.; Li, J.; Zhou, T.; Fan, J.; Rosenfeld, D.; Ming, Y.; Wang, Y.; Huang, J.; Wang, B.; Xu, X.; Lee, S.-S.; Cribb, M.; Zhang, F.; Yang, X.; Zhao, C.; Takemura, T.; Wang, K.; Xia, X.; Yin, Y.; Zhang, H.; Guo, J.; Zhai, P. M.; Sugimoto, N.; Babu, S. S.; Brasseur, G. P.</p> <p>2016-12-01</p> <p>The increasing severity of droughts/floods and worsening air quality from increasing <span class="hlt">aerosols</span> in Asia monsoon regions are the two gravest threats facing over 60% of the world population living in Asian monsoon regions. These dual threats have fueled a large body of research in the last decade on the roles of <span class="hlt">aerosols</span> in impacting Asian monsoon weather and climate. This paper provides a comprehensive review of studies on Asian <span class="hlt">aerosols</span>, monsoons, and their interactions. The Asian monsoon region is a primary source of emissions of diverse species of <span class="hlt">aerosols</span> from both anthropogenic and natural origins. The distributions of <span class="hlt">aerosol</span> loading are strongly influenced by distinct weather and climatic regimes, which are, in turn, modulated by <span class="hlt">aerosol</span> effects. On a continental <span class="hlt">scale</span>, <span class="hlt">aerosols</span> reduce surface insolation and weaken the land-ocean thermal contrast, thus inhibiting the development of monsoons. Locally, <span class="hlt">aerosol</span> radiative effects alter the thermodynamic stability and convective potential of the lower atmosphere leading to reduced temperatures, increased atmospheric stability, and weakened wind and atmospheric circulations. The atmospheric thermodynamic state, which determines the formation of clouds, convection, and precipitation, may also be altered by <span class="hlt">aerosols</span> serving as cloud condensation nuclei or ice nuclei. Absorbing <span class="hlt">aerosols</span> such as black carbon and desert dust in Asian monsoon regions may also induce dynamical feedback processes, leading to a strengthening of the early monsoon and affecting the subsequent evolution of the monsoon. Many mechanisms have been put forth regarding how <span class="hlt">aerosols</span> modulate the amplitude, frequency, intensity, and phase of different monsoon climate variables. A wide range of theoretical, observational, and modeling findings on the Asian monsoon, <span class="hlt">aerosols</span>, and their interactions are synthesized. A new paradigm is proposed on investigating <span class="hlt">aerosol</span>-monsoon interactions, in which natural <span class="hlt">aerosols</span> such as desert dust, black carbon from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E1492K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E1492K"><span><span class="hlt">Aerosol</span> algorithm evaluation within <span class="hlt">aerosol</span>-CCI</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kinne, Stefan; Schulz, Michael; Griesfeller, Jan</p> <p></p> <p>Properties of <span class="hlt">aerosol</span> retrievals from space are difficult. Even data from dedicated satellite sensors face contaminations which limit the accuracy of <span class="hlt">aerosol</span> retrieval products. Issues are the identification of complete cloud-free scenes, the need to assume <span class="hlt">aerosol</span> compositional features in an underdetermined solution space and the requirement to characterize the background at high accuracy. Usually the development of <span class="hlt">aerosol</span> is a slow process, requiring continuous feedback from evaluations. To demonstrate maturity, these evaluations need to cover different regions and seasons and many different <span class="hlt">aerosol</span> properties, because <span class="hlt">aerosol</span> composition is quite diverse and highly variable in space and time, as atmospheric <span class="hlt">aerosol</span> lifetimes are only a few days. Three years ago the ESA Climate Change Initiative started to support <span class="hlt">aerosol</span> retrieval efforts in order to develop <span class="hlt">aerosol</span> retrieval products for the climate community from underutilized ESA satellite sensors. The initial focus was on retrievals of AOD (a measure for the atmospheric column amount) and of Angstrom (a proxy for <span class="hlt">aerosol</span> size) from the ATSR and MERIS sensors on ENVISAT. The goal was to offer retrieval products that are comparable or better in accuracy than commonly used NASA products of MODIS or MISR. Fortunately, accurate reference data of ground based sun-/sky-photometry networks exist. Thus, retrieval assessments could and were conducted independently by different evaluation groups. Here, results of these evaluations for the year 2008 are summarized. The capability of these newly developed retrievals is analyzed and quantified in scores. These scores allowed a ranking of competing efforts and also allow skill comparisons of these new retrievals against existing and commonly used retrievals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5313P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5313P"><span>Lessons learned and way forward from 6 years of <span class="hlt">Aerosol</span>_cci</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popp, Thomas; de Leeuw, Gerrit; Pinnock, Simon</p> <p>2017-04-01</p> <p>Within the ESA Climate Change Initiative (CCI) <span class="hlt">Aerosol</span>_cci (2010 - 2017) conducts intensive work to improve and qualify algorithms for the retrieval of <span class="hlt">aerosol</span> information from European sensors. Meanwhile, several validated (multi-) decadal time series of different <span class="hlt">aerosol</span> parameters from complementary sensors are available: <span class="hlt">Aerosol</span> Optical Depth (AOD), stratospheric extinction profiles, a qualitative Absorbing <span class="hlt">Aerosol</span> Index (AAI), fine mode AOD, mineral dust AOD; absorption information and <span class="hlt">aerosol</span> layer <span class="hlt">height</span> are in an evaluation phase and the multi-pixel GRASP algorithm for the POLDER instrument is used for selected regions. Validation (vs. AERONET, MAN) and inter-comparison to other satellite datasets (MODIS, MISR, SeaWIFS) proved the high quality of the available datasets comparable to other satellite retrievals and revealed needs for algorithm improvement (for example for higher AOD values) which were taken into account in an iterative evolution cycle. The datasets contain pixel level uncertainty estimates which were also validated and improved in the reprocessing. The use of an ensemble method was tested, where several algorithms are applied to the same sensor. The presentation will summarize and discuss the lessons learned from the 6 years of intensive collaboration and highlight major achievements (significantly improved AOD quality, fine mode AOD, dust AOD, pixel level uncertainties, ensemble approach); also limitations and remaining deficits shall be discussed. An outlook will discuss the way forward for the continuous algorithm improvement and re-processing together with opportunities for time series extension with successor instruments of the Sentinel family and the complementarity of the different satellite <span class="hlt">aerosol</span> products.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020060509','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020060509"><span>Airborne Lidar Measurements of <span class="hlt">Aerosol</span> Optical Properties During SAFARI-2000</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McGill, M. J.; Hlavka, D. L.; Hart, W. D.; Welton, E. J.; Campbell, J. R.; Starr, David OC. (Technical Monitor)</p> <p>2002-01-01</p> <p>The Cloud Physics Lidar (CPL) operated onboard the NASA ER-2 high altitude aircraft during the SAFARI-2000 field campaign. The CPL provided high spatial resolution measurements of <span class="hlt">aerosol</span> optical properties at both 1064 nm and 532 nm. We present here results of planetary boundary layer (PBL) <span class="hlt">aerosol</span> optical depth analysis and profiles of <span class="hlt">aerosol</span> extinction. Variation of optical depth and extinction are examined as a function of regional location. The wide-<span class="hlt">scale</span> <span class="hlt">aerosol</span> mapping obtained by the CPL is a unique data set that will aid in future studies of <span class="hlt">aerosol</span> transport. Comparisons between the airborne CPL and ground-based MicroPulse Lidar Network (MPL-Net) sites are shown to have good agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214260P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214260P"><span>Impact of <span class="hlt">Aerosol</span> Processing on Orographic Clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pousse-Nottelmann, Sara; Zubler, Elias M.; Lohmann, Ulrike</p> <p>2010-05-01</p> <p>. [6]. Our investigation regarding the influence of <span class="hlt">aerosol</span> processing will focus on the regional <span class="hlt">scale</span> using a cloud-system resolving model with a much higher resolution. Emphasis will be placed on orographic mixed-phase precipitation. Different two-dimensional simulations of idealized orographic clouds will be conducted to estimate the effect of <span class="hlt">aerosol</span> processing on orographic cloud formation and precipitation. Here, cloud lifetime, location and extent as well as the cloud type will be of particular interest. In a supplementary study, the new parameterization will be compared to observations of total and interstitial <span class="hlt">aerosol</span> concentrations and size distribution at the remote high alpine research station Jungfraujoch in Switzerland. In addition, our simulations will be compared to recent simulations of <span class="hlt">aerosol</span> processing in warm, mixed-phase and cold clouds, which have been carried out at the location of Jungfraujoch station [5]. References: [1] Pruppacher & Jaenicke (1995), The processing of water vapor and <span class="hlt">aerosols</span> by atmospheric clouds, a global estimate, Atmos. Res., 38, 283295. [2] Seifert & Beheng (2006), A two-moment microphysics parameterization for mixed-phase clouds. Part 1: Model description, Meteorol. Atmos. Phys., 92, 4566. [3] Vignati et al. (2004), An efficient size-resolved <span class="hlt">aerosol</span> microphysics module for large-<span class="hlt">scale</span> transport models, J. Geophys. Res., 109, D22202 [4] Muhlbauer & Lohmann (2008), Sensitivity studies of the role of <span class="hlt">aerosols</span> in warm-phase orographic precipitation in different flow regimes, J. Atmos. Sci., 65, 25222542. [5] Hoose et al. (2008), <span class="hlt">Aerosol</span> processing in mixed-phase clouds in ECHAM5HAM: Model description and comparison to observations, J. Geophys. Res., 113, D071210. [6] Hoose et al. (2008), Global simulations of <span class="hlt">aerosol</span> processing in clouds, Atmos. Chem. Phys., 8, 69396963.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AMT....10.1893D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AMT....10.1893D"><span>Pathfinder: applying graph theory to consistent tracking of daytime mixed layer <span class="hlt">height</span> with backscatter lidar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Bruine, Marco; Apituley, Arnoud; Donovan, David Patrick; Klein Baltink, Hendrik; Jorrit de Haij, Marijn</p> <p>2017-05-01</p> <p>The <span class="hlt">height</span> of the atmospheric boundary layer or mixing layer is an important parameter for understanding the dynamics of the atmosphere and the dispersion of trace gases and air pollution. The <span class="hlt">height</span> of the mixing layer (MLH) can be retrieved, among other methods, from lidar or ceilometer backscatter data. These instruments use the vertical backscatter lidar signal to infer MLHL, which is feasible because the main sources of <span class="hlt">aerosols</span> are situated at the surface and vertical gradients are expected to go from the <span class="hlt">aerosol</span> loaded mixing layer close to the ground to the cleaner free atmosphere above. Various lidar/ceilometer algorithms are currently applied, but accounting for MLH temporal development is not always well taken care of. As a result, MLHL retrievals may jump between different atmospheric layers, rather than reliably track true MLH development over time. This hampers the usefulness of MLHL time series, e.g. for process studies, model validation/verification and climatology. Here, we introduce a new method <q>pathfinder</q>, which applies graph theory to simultaneously evaluate time frames that are consistent with <span class="hlt">scales</span> of MLH dynamics, leading to coherent tracking of MLH. Starting from a grid of gradients in the backscatter profiles, MLH development is followed using Dijkstra's shortest path algorithm (Dijkstra, 1959). Locations of strong gradients are connected under the condition that subsequent points on the path are limited to a restricted vertical range. The search is further guided by rules based on the presence of clouds and residual layers. After being applied to backscatter lidar data from Cabauw, excellent agreement is found with wind profiler retrievals for a 12-day period in 2008 (R2 = 0.90) and visual judgment of lidar data during a full year in 2010 (R2 = 0.96). These values compare favourably to other MLHL methods applied to the same lidar data set and corroborate more consistent MLH tracking by pathfinder.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....13384B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....13384B"><span>The Global Atmosphere Watch <span class="hlt">Aerosol</span> Programme</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baltensperger, U.</p> <p>2003-04-01</p> <p>The Global Atmosphere Watch (GAW) programme is a WMO sponsored activity and currently supported by about 80 WMO member countries. It is the goal of GAW to develop and maintain long-term measurements of atmospheric constituents in order to detect trends, develop <span class="hlt">aerosol</span> predictive capabilities and understand proc- esses. With respect to <span class="hlt">aerosols</span>, the objective of GAW is to support a global network determining the spatio-temporal distribution of <span class="hlt">aerosol</span> properties related to climate forcing and air quality up to multi-decadal time <span class="hlt">scales</span>. The GAW network consists of 22 Global stations and some 300 Regional stations. The Scientific Advisory Group (SAG) for <span class="hlt">Aerosols</span> will soon publish their recommendations for <span class="hlt">aerosol</span> measurements. Each site should have an acceptable <span class="hlt">aerosol</span> sampling inlet. Regional stations measure <span class="hlt">aerosol</span> optical depth, as well as the <span class="hlt">aerosol</span> light scattering and absorption coefficient. If possible these should be complemented by routine mass concentration and composition measurements in two <span class="hlt">aerosol</span> size fractions. At Global stations, a larger number of measurements are desirable. These include the Regional parameters list above as well as the light scattering, hemispheric backscat- tering, and absorption coefficients at various wavelengths, <span class="hlt">aerosol</span> number concen- tration, cloud condensation nuclei (CCN) concentration at 0.5% supersaturation, and diffuse, global and direct solar radiation. Additional parameters such as the <span class="hlt">aerosol</span> size distribution, detailed size fractionated chemical composition, dependence of <span class="hlt">aerosol</span> properties on relative humidity, CCN concentration at various supersatura- tions, and the vertical distribution of <span class="hlt">aerosol</span> properties should be measured intermit- tently at Global stations. Examples from the Jungfraujoch (Swiss Alps, 3580 m asl) will be given, where many of the parameters listed above are measured. Data are delivered to and made available by the World Data Centre for <span class="hlt">Aerosols</span> (WDCA, located in Ispra, Italy http</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A51I0183Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A51I0183Z"><span><span class="hlt">Aerosol</span> Indirect effect on Stratocumulus Organization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, X.; Heus, T.; Kollias, P.</p> <p>2015-12-01</p> <p>Large-eddy simulations are used to investigate the role of <span class="hlt">aerosol</span> loading on organized Stratocumulus. We prescribed the cloud droplet number concentration (Nc) and considered it as the proxy for different <span class="hlt">aerosol</span> loading. While the presence of drizzle amplifies the mesoscale variability as is in Savic-Jovcic and Stevens (JAS, 2008), two noticeable findings are discussed here: First, the <span class="hlt">scale</span> of marine boundary layer circulation appears to be independent of <span class="hlt">aerosol</span> loading, suggesting a major role of the turbulence. The precise role of the turbulence in stratocumulus organization is studied by modifying the large <span class="hlt">scale</span> fluctuations from the LES domain. Second, while it is commonly thought that the whole circulation needs to be represented for robust cloud development, we find that stratocumulus dynamics, including variables like w'w' and w'w'w', are remarkably robust even if large <span class="hlt">scales</span> are ignored by simply reducing the domain sizes. The only variable that is sensitive to the change of the <span class="hlt">scale</span> is the amount of cloudiness. Despite their smaller cloud thickness and inhomogeneous macroscopic structure for low Nc, individual drizzling clouds have sizes that are commensurate with circulation <span class="hlt">scale</span>. We observe an Nc threshold below which stratocumulus is thin enough so that a little decrease of Nc would lead to great change of cloud fraction. The simulated cloud albedo is more sensitive to in-cloud liquid water content than to the amount of cloudiness since the former decreases at least three times faster than the latter due to drizzle. The main impact of drizzle evaporation is observed to keep the sub-cloud layer moist and as a result to extend the lifetime of stratocumulus by a couple of hours.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26813611','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26813611"><span>Sexual Orientation, Objective <span class="hlt">Height</span>, and Self-Reported <span class="hlt">Height</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Skorska, Malvina N; Bogaert, Anthony F</p> <p>2017-01-01</p> <p>Studies that have used mostly self-reported <span class="hlt">height</span> have found that androphilic men and women are shorter than gynephilic men and women, respectively. This study examined whether an objective <span class="hlt">height</span> difference exists or whether a psychosocial account (e.g., distortion of self-reports) may explain these putative <span class="hlt">height</span> differences. A total of 863 participants, recruited at a Canadian university, the surrounding region, and through lesbian, gay, bisexual, and transgender (LGBT) events across Canada, self-reported their <span class="hlt">height</span> and had their <span class="hlt">height</span> measured. Androphilic men were shorter, on average, than gynephilic men. There was no objective <span class="hlt">height</span> difference between gynephilic, ambiphilic, and androphilic women. Self-reported <span class="hlt">height</span>, statistically controlling for objective <span class="hlt">height</span>, was not related to sexual orientation. These findings are the first to show an objective <span class="hlt">height</span> difference between androphilic and gynephilic men. Also, the findings suggest that previous studies using self-reported <span class="hlt">height</span> found part of a true objective <span class="hlt">height</span> difference between androphilic and gynephilic men. These findings have implications for existing biological theories of men's sexual orientation development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....14709V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....14709V"><span>Secondary <span class="hlt">Aerosol</span> Formation over the ESCOMPTE Area: Results from airborne <span class="hlt">Aerosol</span> and Trace Gas Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Dingenen, R.; Martins-Dos Santos, S.; Putaud, J. P.; Allet, C.; Bretton, E.; Perros, P.</p> <p>2003-04-01</p> <p>From June 10th to July 14th 2001, the ESCOMPTE campaign took place in the Marseille-Berre area in Southern France. The goal of the campaign was to produce a high quality 3-D data base from emissions, transport and air composition measurements during urban photochemical pollution episodes at the meso-<span class="hlt">scale</span>. The CAATER AEROPLUM project was embedded within this international field campaign. AEROPLUM aimed at mapping size distributions of <span class="hlt">aerosols</span> and photo-oxidants in the mixed layer over the ESCOMPTE domain, using the ARAT Fokker 27 as measurement platform. Aircraft sub-micrometer <span class="hlt">aerosol</span> measurements are validated during overpasses against ground-based measurements, carried out with similar instrumentation. We will present and discuss data during periods of seabreeze, transporting coastal industrial and urban pollution land-inwards. This leads to intense photochemical activity, evidenced by elevated O_3 concentrations and <span class="hlt">aerosol</span> levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1433115-boundary-layer-height-buoyancy-determine-horizontal-scale-convective-self-aggregation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1433115-boundary-layer-height-buoyancy-determine-horizontal-scale-convective-self-aggregation"><span>Boundary Layer <span class="hlt">Height</span> and Buoyancy Determine the Horizontal <span class="hlt">Scale</span> of Convective Self-Aggregation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Yang, Da</p> <p>2018-01-24</p> <p>Organized rainstorms and their associated overturning circulations can self-emerge over an ocean surface with uniform temperature in cloud-resolving simulations. This phenomenon is referred to as convective self-aggregation. Convective self-aggregation is argued to be an important building block for tropical weather systems and may help regulate tropical atmospheric humidity and thereby tropical climate stability. Here the author presents a boundary layer theory for the horizontal <span class="hlt">scale</span> λ of 2D (x, z) convective self-aggregation by considering both the momentum and energy constraints for steady circulations. This theory suggests that λ <span class="hlt">scales</span> with the product of the boundary layer <span class="hlt">height</span> h and themore » square root of the amplitude of density variation between aggregated moist and dry regions in the boundary layer, and that this density variation mainly arises from the moisture variation due to the virtual effect of water vapor. Furthermore, this theory predicts the following: 1) the order of magnitude of λ is ~2000 km, 2) the aspect ratio of the boundary layer λ/h increases with surface warming, and 3) λ decreases when the virtual effect of water vapor is disabled. These predictions are confirmed using a sui te of cloud-resolving simulations spanning a wide range of climates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1433115-boundary-layer-height-buoyancy-determine-horizontal-scale-convective-self-aggregation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1433115-boundary-layer-height-buoyancy-determine-horizontal-scale-convective-self-aggregation"><span>Boundary Layer <span class="hlt">Height</span> and Buoyancy Determine the Horizontal <span class="hlt">Scale</span> of Convective Self-Aggregation</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>Yang, Da</p> <p></p> <p>Organized rainstorms and their associated overturning circulations can self-emerge over an ocean surface with uniform temperature in cloud-resolving simulations. This phenomenon is referred to as convective self-aggregation. Convective self-aggregation is argued to be an important building block for tropical weather systems and may help regulate tropical atmospheric humidity and thereby tropical climate stability. Here the author presents a boundary layer theory for the horizontal <span class="hlt">scale</span> λ of 2D (x, z) convective self-aggregation by considering both the momentum and energy constraints for steady circulations. This theory suggests that λ <span class="hlt">scales</span> with the product of the boundary layer <span class="hlt">height</span> h and themore » square root of the amplitude of density variation between aggregated moist and dry regions in the boundary layer, and that this density variation mainly arises from the moisture variation due to the virtual effect of water vapor. Furthermore, this theory predicts the following: 1) the order of magnitude of λ is ~2000 km, 2) the aspect ratio of the boundary layer λ/h increases with surface warming, and 3) λ decreases when the virtual effect of water vapor is disabled. These predictions are confirmed using a sui te of cloud-resolving simulations spanning a wide range of climates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110004374','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110004374"><span>Comparison of Summer and Winter California Central Valley <span class="hlt">Aerosol</span> Distributions from Lidar and MODIS Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lewis, Jasper R., Jr.; DeYoung, Russell J.; Chu, D. Allen</p> <p>2010-01-01</p> <p><span class="hlt">Aerosol</span> distributions from two aircraft lidar campaigns conducted in the California Central Valley are compared in order to identify seasonal variations. Aircraft lidar flights were conducted in June 2003 and February 2008. While the PM2.5 concentration is highest in the winter, the <span class="hlt">aerosol</span> optical depth measured from MODIS is highest in the summer. A seasonal comparison shows that PM2.5 in the winter can exceed summer PM2.5 by 55%, while summer AOD exceeds winter AOD by 43%. Higher temperatures wildfires in the summer produce elevated <span class="hlt">aerosol</span> layers that are detected by satellite measurements, but not surface particulate matter monitors. Measurements of the boundary layer <span class="hlt">height</span> from lidar instruments are necessary to incorporate satellite measurements with air quality measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990064611&hterms=How+get+human+cloud&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DHow%2Bget%2Bhuman%2Bcloud%253F','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990064611&hterms=How+get+human+cloud&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DHow%2Bget%2Bhuman%2Bcloud%253F"><span>Radiative Importance of <span class="hlt">Aerosol</span>-Cloud Interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsay, Si-Chee</p> <p>1999-01-01</p> <p><span class="hlt">Aerosol</span> particles are input into the troposphere by biomass burning, among other sources. These <span class="hlt">aerosol</span> palls cover large expanses of the earth's surface. <span class="hlt">Aerosols</span> may directly scatter solar radiation back to space, thus increasing the earth's albedo and act to cool the earth's surface and atmosphere. <span class="hlt">Aerosols</span> also contribute to the earth's energy balance indirectly. Hygroscopic <span class="hlt">aerosol</span> act as cloud condensation nuclei (CCN) and thus affects cloud properties. In 1977, Twomey theorized that additional available CCN would create smaller but more numerous cloud droplets in a cloud with a given amount of liquid water. This in turn would increase the cloud albedo which would scatter additional radiation back to space and create a similar cooling pattern as the direct <span class="hlt">aerosol</span> effect. Estimates of the magnitude of the <span class="hlt">aerosol</span> indirect effect on a global <span class="hlt">scale</span> range from 0.0 to -4.8 W/sq m. Thus the indirect effect can be of comparable magnitude and opposite in sign to the estimates of global greenhouse gas forcing <span class="hlt">Aerosol</span>-cloud interaction is not a one-way process. Just as <span class="hlt">aerosols</span> have an influence on clouds through the cloud microphysics, clouds have an influence on <span class="hlt">aerosols</span>. Cloud droplets are solutions of liquid water and CCN, now dissolved. When the cloud droplet evaporates it leaves behind an <span class="hlt">aerosol</span> particle. This new particle does not have to have the same properties as the original CCN. In fact, studies show that <span class="hlt">aerosol</span> particles that result from cloud processing are larger in size than the original CCN. Optical properties of <span class="hlt">aerosol</span> particles are dependent on the size of the particles. Larger particles have a smaller backscattering fraction, and thus less incoming solar radiation will be backscattered to space if the <span class="hlt">aerosol</span> particles are larger. Therefore, we see that <span class="hlt">aerosols</span> and clouds modify each other to influence the radiative balance of the earth. Understanding and quantifying the spatial and seasonal patterns of the <span class="hlt">aerosol</span> indirect forcing may have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AMT....11.3177H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AMT....11.3177H"><span>Neural network cloud top pressure and <span class="hlt">height</span> for MODIS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Håkansson, Nina; Adok, Claudia; Thoss, Anke; Scheirer, Ronald; Hörnquist, Sara</p> <p>2018-06-01</p> <p>Cloud top <span class="hlt">height</span> retrieval from imager instruments is important for nowcasting and for satellite climate data records. A neural network approach for cloud top <span class="hlt">height</span> retrieval from the imager instrument MODIS (Moderate Resolution Imaging Spectroradiometer) is presented. The neural networks are trained using cloud top layer pressure data from the CALIOP (Cloud-<span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization) dataset. Results are compared with two operational reference algorithms for cloud top <span class="hlt">height</span>: the MODIS Collection 6 Level 2 <span class="hlt">height</span> product and the cloud top temperature and <span class="hlt">height</span> algorithm in the 2014 version of the NWC SAF (EUMETSAT (European Organization for the Exploitation of Meteorological Satellites) Satellite Application Facility on Support to Nowcasting and Very Short Range Forecasting) PPS (Polar Platform System). All three techniques are evaluated using both CALIOP and CPR (Cloud Profiling Radar for CloudSat (CLOUD SATellite)) <span class="hlt">height</span>. Instruments like AVHRR (Advanced Very High Resolution Radiometer) and VIIRS (Visible Infrared Imaging Radiometer Suite) contain fewer channels useful for cloud top <span class="hlt">height</span> retrievals than MODIS, therefore several different neural networks are investigated to test how infrared channel selection influences retrieval performance. Also a network with only channels available for the AVHRR1 instrument is trained and evaluated. To examine the contribution of different variables, networks with fewer variables are trained. It is shown that variables containing imager information for neighboring pixels are very important. The error distributions of the involved cloud top <span class="hlt">height</span> algorithms are found to be non-Gaussian. Different descriptive statistic measures are presented and it is exemplified that bias and SD (standard deviation) can be misleading for non-Gaussian distributions. The median and mode are found to better describe the tendency of the error distributions and IQR (interquartile range) and MAE (mean absolute error) are found</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720051528&hterms=radiance+rayleigh&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dradiance%2Brayleigh','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720051528&hterms=radiance+rayleigh&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dradiance%2Brayleigh"><span>Effect of <span class="hlt">aerosol</span> variation on radiance in the earth's atmosphere-ocean system.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Plass, G. N.; Kattawar, G. W.</p> <p>1972-01-01</p> <p>Calculation of the radiance at the top and bottom of the atmosphere with a realistic model of both the atmosphere and ocean. It is found that the upward flux at the top of the atmosphere, as well as the angular distribution of the radiation, changes appreciably as the <span class="hlt">aerosol</span> amount increases from normal to ten times normal. At the same time, the upward and downward radiance just above the ocean surface undergoes important changes. The radiance does not change appreciably with variations in the <span class="hlt">aerosol</span> distribution with <span class="hlt">height</span> so long as the total <span class="hlt">aerosol</span> amount remains constant. Similarly, changes in the ozone amount cause only small changes in the radiance at the wavelengths considered (0.7, 0.9, and 1.67 micron). Very little radiation returns to the atmosphere from the ocean at 0.9 and 1.67 micron because of the high absorption of water at these wavelengths.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A14A..08X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A14A..08X"><span>Coupled retrieval of water cloud and above-cloud <span class="hlt">aerosol</span> properties using the Airborne Multiangle SpectroPolarimetric Imager (AirMSPI)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, F.; van Harten, G.; Diner, D. J.; Rheingans, B. E.; Tosca, M.; Seidel, F. C.; Bull, M. A.; Tkatcheva, I. N.; McDuffie, J. L.; Garay, M. J.; Davis, A. B.; Jovanovic, V. M.; Brian, C.; Alexandrov, M. D.; Hostetler, C. A.; Ferrare, R. A.; Burton, S. P.</p> <p>2017-12-01</p> <p>The Airborne Multiangle SpectroPolarimetric Imager (AirMSPI) has been flying aboard the NASA ER-2 high altitude aircraft since October 2010. AirMSPI acquires radiance and polarization data in bands centered at 355, 380, 445, 470*, 555, 660*, 865*, and 935 nm (*denotes polarimetric bands). In sweep mode, georectified images cover an area of 80-100 km (along track) by 10-25 km (across track) between ±66° off nadir, with a map-projected spatial resolution of 25 meters. An efficient and flexible retrieval algorithm has been developed using AirMSPI polarimetric bands for simultaneous retrieval of cloud and above-cloud <span class="hlt">aerosol</span> microphysical properties. We design a three-step retrieval approach, namely 1) estimating effective droplet size distribution using polarimetric cloudbow observations and using it as initial guess for Step 2; 2) combining water cloud and <span class="hlt">aerosol</span> above cloud retrieval by fitting polarimetric signals at all scattering angles (e.g. from 80° to 180°); and 3) constructing a lookup table of radiance for a set of cloud optical depth grids using <span class="hlt">aerosol</span> and cloud information retrieved from Step 2 and then estimating pixel-<span class="hlt">scale</span> cloud optical depth based on 1D radiative transfer (RT) theory by fitting the AirMSPI radiance. Retrieval uncertainty is formulated by accounting for instrumental errors and constraints imposed on spectral variations of <span class="hlt">aerosol</span> and cloud droplet optical properties. As the forward RT model, a hybrid approach is developed to combine the computational strengths of Markov-chain and adding-doubling methods to model polarized RT in a coupled <span class="hlt">aerosol</span>, Rayleigh and cloud system. Our retrieval approach is tested using 134 AirMSPI datasets acquired during NASA ORACLES field campaign in 09/2016, with low to high <span class="hlt">aerosol</span> loadings. For validation, the retrieved <span class="hlt">aerosol</span> optical depths and cloud-top <span class="hlt">heights</span> are compared to coincident High Spectral Resolution Lidar-2 (HSRL-2) data, and the droplet size parameters including effective radius and</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/2018AtmEn.185...15K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AtmEn.185...15K"><span>Smoke <span class="hlt">aerosol</span> chemistry and aging of Siberian biomass burning emissions in a large <span class="hlt">aerosol</span> chamber</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kalogridis, A.-C.; Popovicheva, O. B.; Engling, G.; Diapouli, E.; Kawamura, K.; Tachibana, E.; Ono, K.; Kozlov, V. S.; Eleftheriadis, K.</p> <p>2018-07-01</p> <p>Vegetation open fires constitute a significant source of particulate pollutants on a global <span class="hlt">scale</span> and play an important role in both atmospheric chemistry and climate change. To better understand the emission and aging characteristics of smoke <span class="hlt">aerosols</span>, we performed small-<span class="hlt">scale</span> fire experiments using the Large <span class="hlt">Aerosol</span> Chamber (LAC, 1800 m3) with a focus on biomass burning from Siberian boreal coniferous forests. A series of burn experiments were conducted with typical Siberian biomass (pine and debris), simulating separately different combustion conditions, namely, flaming, smoldering and mixed phase. Following smoke emission and dispersion in the combustion chamber, we investigated aging of <span class="hlt">aerosols</span> under dark conditions. Here, we present experimental data on emission factors of total, elemental and organic carbon, as well as individual organic compounds, such as anhydrosugars, phenolic and dicarboxylic acids. We found that total carbon accounts for up to 80% of the fine mode (PM2.5) smoke <span class="hlt">aerosol</span>. Higher PM2.5 emission factors were observed in the smoldering compared to flaming phase and in pine compared to debris smoldering phase. For low-temperature combustion, organic carbon (OC) contributed to more than 90% of total carbon, whereas elemental carbon (EC) dominated the <span class="hlt">aerosol</span> composition in flaming burns with a 60-70% contribution to the total carbon mass. For all smoldering burns, levoglucosan (LG), a cellulose decomposition product, was the most abundant organic species (average LG/OC = 0.26 for pine smoldering), followed by its isomer mannosan or dehydroabietic acid (DA), an important constituent of conifer resin (DA/OC = 0.033). A levoglucosan-to-mannosan ratio of about 3 was observed, which is consistent with ratios reported for coniferous biomass and more generally softwood. The rates of <span class="hlt">aerosol</span> removal for OC and individual organic compounds were investigated during aging in the chamber in terms of mass concentration loss rates over time under dark</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ACP....15.9217P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ACP....15.9217P"><span>Microphysical processing of <span class="hlt">aerosol</span> particles in orographic clouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pousse-Nottelmann, S.; Zubler, E. M.; Lohmann, U.</p> <p>2015-08-01</p> <p>An explicit and detailed treatment of cloud-borne particles allowing for the consideration of <span class="hlt">aerosol</span> cycling in clouds has been implemented into COSMO-Model, the regional weather forecast and climate model of the Consortium for Small-<span class="hlt">scale</span> Modeling (COSMO). The effects of <span class="hlt">aerosol</span> scavenging, cloud microphysical processing and regeneration upon cloud evaporation on the <span class="hlt">aerosol</span> population and on subsequent cloud formation are investigated. For this, two-dimensional idealized simulations of moist flow over two bell-shaped mountains were carried out varying the treatment of <span class="hlt">aerosol</span> scavenging and regeneration processes for a warm-phase and a mixed-phase orographic cloud. The results allowed us to identify different <span class="hlt">aerosol</span> cycling mechanisms. In the simulated non-precipitating warm-phase cloud, <span class="hlt">aerosol</span> mass is incorporated into cloud droplets by activation scavenging and released back to the atmosphere upon cloud droplet evaporation. In the mixed-phase cloud, a first cycle comprises cloud droplet activation and evaporation via the Wegener-Bergeron-Findeisen (WBF) process. A second cycle includes below-cloud scavenging by precipitating snow particles and snow sublimation and is connected to the first cycle via the riming process which transfers <span class="hlt">aerosol</span> mass from cloud droplets to snowflakes. In the simulated mixed-phase cloud, only a negligible part of the total <span class="hlt">aerosol</span> mass is incorporated into ice crystals. Sedimenting snowflakes reaching the surface remove <span class="hlt">aerosol</span> mass from the atmosphere. The results show that <span class="hlt">aerosol</span> processing and regeneration lead to a vertical redistribution of <span class="hlt">aerosol</span> mass and number. Thereby, the processes impact the total <span class="hlt">aerosol</span> number and mass and additionally alter the shape of the <span class="hlt">aerosol</span> size distributions by enhancing the internally mixed/soluble Aitken and accumulation mode and generating coarse-mode particles. Concerning subsequent cloud formation at the second mountain, accounting for <span class="hlt">aerosol</span> processing and regeneration increases</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51G2152Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51G2152Y"><span>Effect of <span class="hlt">aerosol</span> feedback in the Korea Peninsula using WRF-CMAQ two-way coupled model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yoo, J.; Jeon, W.; Lee, H.; Lee, S.</p> <p>2017-12-01</p> <p><span class="hlt">Aerosols</span> influence the climate system by scattering and absorption of the solar radiation by altering the cloud radiative properties. For the reason, consideration of <span class="hlt">aerosol</span> feedback is important numerical weather prediction and air quality models. The purpose of this study was to investigate the effect of <span class="hlt">aerosol</span> feedback on PM10 simulation in Korean Peninsula using the Weather Research and Forecasting (WRF) and the community multiscale air quality (CMAQ) two-way coupled model. Simulations were conducted with the <span class="hlt">aerosol</span> feedback (FB) and without (NFB). The results of the simulated solar radiation in the west part of Korea decreased due to the <span class="hlt">aerosol</span> feedback effect. The feedback effect was significant in the west part of Korea Peninsula, showing high Particulate Matter (PM) estimates due to dense emissions and its long-range transport from China. The decrease of solar radiation lead to planetary boundary layer (PBL) <span class="hlt">height</span> reduction, thereby dispersion of air pollutants such as PM is suppressed, and resulted in higher PM concentrations. These results indicate that <span class="hlt">aerosol</span> feedback effects can play an important role in the simulation of meteorology and air quality over Korea Peninsula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SPIE.2949..143J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SPIE.2949..143J"><span>Optimizing <span class="hlt">height</span> presentation for aircraft cockpit displays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jordan, Chris S.; Croft, D.; Selcon, Stephen J.; Markin, H.; Jackson, M.</p> <p>1997-02-01</p> <p>This paper describes an experiment conducted to investigate the type of display symbology that most effectively conveys <span class="hlt">height</span> information to users of head-down plan-view radar displays. The experiment also investigated the use of multiple information sources (redundancy) in the design of such displays. Subjects were presented with eight different <span class="hlt">height</span> display formats. These formats were constructed from a control, and/or one, two, or three sources of redundant information. The three formats were letter coding, analogue <span class="hlt">scaling</span>, and toggling (spatially switching the position of the <span class="hlt">height</span> information from above to below the aircraft symbol). Subjects were required to indicate altitude awareness via a four-key, forced-choice keyboard response. Error scores and response times were taken as performance measures. There were three main findings. First, there was a significant performance advantage when the altitude information was presented above and below the symbol to aid the representation of <span class="hlt">height</span> information. Second, the analogue <span class="hlt">scale</span>, a line whose length indicated altitude, proved significantly detrimental to performance. Finally, no relationship was found between the number of redundant information sources employed and performance. The implications for future aircraft and displays are discussed in relation to current aircraft tactical displays and in the context of perceptual psychological theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1376182-multivariate-quadrature-representing-cloud-condensation-nuclei-activity-aerosol-populations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1376182-multivariate-quadrature-representing-cloud-condensation-nuclei-activity-aerosol-populations"><span>Multivariate quadrature for representing cloud condensation nuclei activity of <span class="hlt">aerosol</span> populations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fierce, Laura; McGraw, Robert L.</p> <p>2017-07-26</p> <p>Here, sparse representations of atmospheric <span class="hlt">aerosols</span> are needed for efficient regional- and global-<span class="hlt">scale</span> chemical transport models. Here we introduce a new framework for representing <span class="hlt">aerosol</span> distributions, based on the quadrature method of moments. Given a set of moment constraints, we show how linear programming, combined with an entropy-inspired cost function, can be used to construct optimized quadrature representations of <span class="hlt">aerosol</span> distributions. The sparse representations derived from this approach accurately reproduce cloud condensation nuclei (CCN) activity for realistically complex distributions simulated by a particleresolved model. Additionally, the linear programming techniques described in this study can be used to bound key aerosolmore » properties, such as the number concentration of CCN. Unlike the commonly used sparse representations, such as modal and sectional schemes, the maximum-entropy approach described here is not constrained to pre-determined size bins or assumed distribution shapes. This study is a first step toward a particle-based <span class="hlt">aerosol</span> scheme that will track multivariate <span class="hlt">aerosol</span> distributions with sufficient computational efficiency for large-<span class="hlt">scale</span> simulations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1376182-multivariate-quadrature-representing-cloud-condensation-nuclei-activity-aerosol-populations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1376182-multivariate-quadrature-representing-cloud-condensation-nuclei-activity-aerosol-populations"><span>Multivariate quadrature for representing cloud condensation nuclei activity of <span class="hlt">aerosol</span> populations</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>Fierce, Laura; McGraw, Robert L.</p> <p></p> <p>Here, sparse representations of atmospheric <span class="hlt">aerosols</span> are needed for efficient regional- and global-<span class="hlt">scale</span> chemical transport models. Here we introduce a new framework for representing <span class="hlt">aerosol</span> distributions, based on the quadrature method of moments. Given a set of moment constraints, we show how linear programming, combined with an entropy-inspired cost function, can be used to construct optimized quadrature representations of <span class="hlt">aerosol</span> distributions. The sparse representations derived from this approach accurately reproduce cloud condensation nuclei (CCN) activity for realistically complex distributions simulated by a particleresolved model. Additionally, the linear programming techniques described in this study can be used to bound key aerosolmore » properties, such as the number concentration of CCN. Unlike the commonly used sparse representations, such as modal and sectional schemes, the maximum-entropy approach described here is not constrained to pre-determined size bins or assumed distribution shapes. This study is a first step toward a particle-based <span class="hlt">aerosol</span> scheme that will track multivariate <span class="hlt">aerosol</span> distributions with sufficient computational efficiency for large-<span class="hlt">scale</span> simulations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050139743&hterms=Influence+clouds+climate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DInfluence%2Bclouds%2Bclimate','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050139743&hterms=Influence+clouds+climate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DInfluence%2Bclouds%2Bclimate"><span>Scanning Backscatter Lidar Observations for Characterizing 4-D Cloud and <span class="hlt">Aerosol</span> Fields to Improve Radiative Transfer Parameterizations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schwemmer, Geary K.; Miller, David O.</p> <p>2005-01-01</p> <p>Clouds have a powerful influence on atmospheric radiative transfer and hence are crucial to understanding and interpreting the exchange of radiation between the Earth's surface, the atmosphere, and space. Because clouds are highly variable in space, time and physical makeup, it is important to be able to observe them in three dimensions (3-D) with sufficient resolution that the data can be used to generate and validate parameterizations of cloud fields at the resolution <span class="hlt">scale</span> of global climate models (GCMs). Simulation of photon transport in three dimensionally inhomogeneous cloud fields show that spatial inhomogeneities tend to decrease cloud reflection and absorption and increase direct and diffuse transmission, Therefore it is an important task to characterize cloud spatial structures in three dimensions on the <span class="hlt">scale</span> of GCM grid elements. In order to validate cloud parameterizations that represent the ensemble, or mean and variance of cloud properties within a GCM grid element, measurements of the parameters must be obtained on a much finer <span class="hlt">scale</span> so that the statistics on those measurements are truly representative. High spatial sampling resolution is required, on the order of 1 km or less. Since the radiation fields respond almost instantaneously to changes in the cloud field, and clouds changes occur on <span class="hlt">scales</span> of seconds and less when viewed on <span class="hlt">scales</span> of approximately 100m, the temporal resolution of cloud properties should be measured and characterized on second time <span class="hlt">scales</span>. GCM time steps are typically on the order of an hour, but in order to obtain sufficient statistical representations of cloud properties in the parameterizations that are used as model inputs, averaged values of cloud properties should be calculated on time <span class="hlt">scales</span> on the order of 10-100 s. The Holographic Airborne Rotating Lidar Instrument Experiment (HARLIE) provides exceptional temporal (100 ms) and spatial (30 m) resolution measurements of <span class="hlt">aerosol</span> and cloud backscatter in three</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4254R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4254R"><span>Evaluating <span class="hlt">aerosol</span> impacts on Numerical Weather Prediction in two extreme dust and biomass-burning events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Remy, Samuel; Benedetti, Angela; Jones, Luke; Razinger, Miha; Haiden, Thomas</p> <p>2014-05-01</p> <p>The WMO-sponsored Working Group on Numerical Experimentation (WGNE) set up a project aimed at understanding the importance of <span class="hlt">aerosols</span> for numerical weather prediction (NWP). Three cases are being investigated by several NWP centres with <span class="hlt">aerosol</span> capabilities: a severe dust case that affected Southern Europe in April 2012, a biomass burning case in South America in September 2012, and an extreme pollution event in Beijing (China) which took place in January 2013. At ECMWF these cases are being studied using the MACC-II system with radiatively interactive <span class="hlt">aerosols</span>. Some preliminary results related to the dust and the fire event will be presented here. A preliminary verification of the impact of the <span class="hlt">aerosol</span>-radiation direct interaction on surface meteorological parameters such as 2m Temperature and surface winds over the region of interest will be presented. <span class="hlt">Aerosol</span> optical depth (AOD) verification using AERONET data will also be discussed. For the biomass burning case, the impact of using injection <span class="hlt">heights</span> estimated by a Plume Rise Model (PRM) for the biomass burning emissions will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.9076A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.9076A"><span><span class="hlt">Height</span> biases and <span class="hlt">scale</span> variations in VLBI networks due to antenna gravitational deformations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abbondanza, Claudio; Sarti, Pierguido; Petrov, Leonid; Negusini, Monia</p> <p>2010-05-01</p> <p>The impact of signal path variations (SPVs) caused by antenna gravity deformations on geodetic VLBI results is evaluated for the first time. Elevation-dependent models of SPV for Medicina and Noto (Italy) telescopes were derived from a combination of terrestrial surveying methods to account for gravitational deformations. After applying these models, estimates of the antenna reference point (ARP) positions are shifted upward by 8.9 mm and 6.7 mm, respectively. The impact on other parameters is negligible. To infer the impact of antenna gravity deformations on the entire VLBI network, lacking measurements for other telescopes, we rescaled the SPV models of Medicina and Noto for other antennas according to their size. The effects are changes in VLBI <span class="hlt">heights</span> in the range [-3,73] mm and a significant net <span class="hlt">scale</span> increase of 0.3 - 0.8 ppb. This demonstrates the need to include SPV models in routine VLBI data analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GeoRL..41.5678G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GeoRL..41.5678G"><span>Rainfall-<span class="hlt">aerosol</span> relationships explained by wet scavenging and humidity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grandey, Benjamin S.; Gururaj, Anisha; Stier, Philip; Wagner, Till M.</p> <p>2014-08-01</p> <p>Relationships between precipitation rate and <span class="hlt">aerosol</span> optical depth, the extinction of light by <span class="hlt">aerosol</span> in an atmospheric column, have been observed in satellite-retrieved data. What are the reasons for these precipitation-<span class="hlt">aerosol</span> relationships? We investigate relationships between convective precipitation rate (Rconv) and <span class="hlt">aerosol</span> optical depth (τtot) using the ECHAM5-HAM <span class="hlt">aerosol</span>-climate model. We show that negative Rconv-τtot relationships arise due to wet scavenging of <span class="hlt">aerosol</span>. The apparent lack of negative Rconv-τtot relationships in satellite-retrieved data is likely because the satellite data do not sample wet scavenging events. When convective wet scavenging is excluded in the model, we find positive Rconv-τtot relationships in regions where convective precipitation is the dominant form of model precipitation. The spatial distribution of these relationships is in good agreement with satellite-based results. We further demonstrate that a substantial component of these positive relationships arises due to covariation with large-<span class="hlt">scale</span> relative humidity. Although the interpretation of precipitation-<span class="hlt">aerosol</span> relationships remains a challenging question, we suggest that progress can be made through a synergy between observations and models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....1614795S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....1614795S"><span>Regional and local variations in atmospheric <span class="hlt">aerosols</span> using ground-based sun photometry during Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON) in 2012</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sano, Itaru; Mukai, Sonoyo; Nakata, Makiko; Holben, Brent N.</p> <p>2016-11-01</p> <p><span class="hlt">Aerosol</span> mass concentrations are affected by local emissions as well as long-range transboundary (LRT) <span class="hlt">aerosols</span>. This work investigates regional and local variations of <span class="hlt">aerosols</span> based on Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON). We constructed DRAGON-Japan and DRAGON-Osaka in spring of 2012. The former network covers almost all of Japan in order to obtain <span class="hlt">aerosol</span> information in regional <span class="hlt">scale</span> over Japanese islands. It was determined from the DRAGON-Japan campaign that the values of <span class="hlt">aerosol</span> optical thickness (AOT) decrease from west to east during an <span class="hlt">aerosol</span> episode. In fact, the highest AOT was recorded at Fukue Island at the western end of the network, and the value was much higher than that of urban areas. The latter network (DRAGON-Osaka) was set as a dense instrument network in the megalopolis of Osaka, with a population of 12 million, to better understand local <span class="hlt">aerosol</span> dynamics in urban areas. AOT was further measured with a mobile sun photometer attached to a car. This transect information showed that <span class="hlt">aerosol</span> concentrations rapidly changed in time and space together when most of the Osaka area was covered with moderate LRT <span class="hlt">aerosols</span>. The combined use of the dense instrument network (DRAGON-Osaka) and high-frequency measurements provides the motion of <span class="hlt">aerosol</span> advection, which coincides with the wind vector around the layer between 700 and 850 hPa as provided by the reanalysis data of the National Centers for Environmental Prediction (NCEP).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003282&hterms=sun&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsun','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003282&hterms=sun&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsun"><span>Regional and Local Variations in Atmospheric <span class="hlt">Aerosols</span> Using Ground-Based Sun Photometry During Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON) in 2012</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sano, Itaru; Mukai, Sonoyo; Nakata, Makiko; Holben, Brent N.</p> <p>2016-01-01</p> <p><span class="hlt">Aerosol</span> mass concentrations are affected by local emissions as well as long-range transboundary (LRT) <span class="hlt">aerosols</span>. This work investigates regional and local variations of <span class="hlt">aerosols</span> based on Distributed Regional <span class="hlt">Aerosol</span> Gridded Observation Networks (DRAGON).We constructed DRAGON-Japan and DRAGON-Osaka in spring of 2012. The former network covers almost all of Japan in order to obtain <span class="hlt">aerosol</span> information in regional <span class="hlt">scale</span> over Japanese islands. It was determined from the DRAGON-Japan campaign that the values of <span class="hlt">aerosol</span> optical thickness (AOT) decrease from west to east during an <span class="hlt">aerosol</span> episode. In fact, the highest AOT was recorded at Fukue Island at the western end of the network, and the value was much higher than that of urban areas. The latter network (DRAGON-Osaka) was set as a dense instrument network in the megalopolis of Osaka, with a population of 12 million, to better understand local <span class="hlt">aerosol</span> dynamics in urban areas. AOT was further measured with a mobile sun photometer attached to a car. This transect information showed that <span class="hlt">aerosol</span> concentrations rapidly changed in time and space together when most of the Osaka area was covered with moderate LRT <span class="hlt">aerosols</span>. The combined use of the dense instrument network (DRAGON-Osaka) and high-frequency measurements provides the motion of <span class="hlt">aerosol</span> advection, which coincides with the wind vector around the layer between 700 and 850 hPa as provided by the reanalysis data of the National Centers for Environmental Prediction (NCEP).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A21C0073L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A21C0073L"><span>Evaluation of Air Pollution Applications of AERONET and MODIS <span class="hlt">Aerosol</span> Column Optical Depth by Comparison with In Situ Measurements of <span class="hlt">Aerosol</span> Light Scattering and Absorption for Reno, NV, USA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loria Salazar, S.; Arnott, W. P.; Moosmuller, H.; Colucci, D.</p> <p>2012-12-01</p> <p>Reno, Nevada, USA is subject to typical urban <span class="hlt">aerosol</span>, wind-blown dust, and occasional biomass burning smoke from anthropogenic and natural fires. Reno has complex air flow at levels relevant for <span class="hlt">aerosol</span> transport. At times recirculating mountain and urban flow arrives from the Sierra Nevada, San Francisco, CA and Sacramento, CA. The urban plumes are further modified by biogenic forest emissions and secondary <span class="hlt">aerosol</span> formation during transport over the Sierra Nevada Mountains to Reno. This complicates the use of MODIS <span class="hlt">aerosol</span> optical depth (AOD) for air quality measurements in Reno. Our laboratory at the University of Nevada Reno has collocated multispectral photoacoustic instruments and reciprocal nephelometers to measure light absorption and light scattering coefficients as well as an AERONET operated CIMEL CE-318 ground-based sunphotometer. Preliminary measurements from August 2011 indicate substantially larger Cimel AOD than could be accounted for by use of the in situ <span class="hlt">aerosol</span> extinction measurements combined with mixing <span class="hlt">height</span> estimate. This poster presents new results comparing AERONET AOD and single scattering albedo and MODIS AOD with in situ measurements for summer and fall 2012, along with extensive back trajectory analysis, to evaluate conditions when satellite measurement may be useful for air pollution applications in Reno.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRD..11719301G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRD..11719301G"><span>Primary and secondary organic <span class="hlt">aerosols</span> in Fresno, California during wintertime: Results from high resolution <span class="hlt">aerosol</span> mass spectrometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ge, Xinlei; Setyan, Ari; Sun, Yele; Zhang, Qi</p> <p>2012-10-01</p> <p>Organic <span class="hlt">aerosols</span> (OA) were studied in Fresno, California, in winter 2010 with an Aerodyne High Resolution Time-of-Flight <span class="hlt">Aerosol</span> Mass Spectrometer (HR-ToF-AMS). OA dominated the submicron <span class="hlt">aerosol</span> mass (average = 67%) with an average concentration of 7.9μg m-3 and a nominal formula of C1H1.59N0.014O0.27S0.00008, which corresponds to an average organic mass-to-carbon ratio of 1.50. Three primary OA (POA) factors and one oxygenated OA factor (OOA) representative of secondary OA (SOA) were identified via Positive Matrix Factorization of the high-resolution mass spectra. The three POA factors, which include a traffic-related hydrocarbon-like OA (HOA), a cooking OA (COA), and a biomass burning OA (BBOA) released from residential heating, accounted for an average 57% of the OA mass and up to 80% between 6 - 9 P.M., during which enhanced emissions from evening rush hour traffic, dinner cooking, and residential wood burning were exacerbated by low mixed layer <span class="hlt">height</span>. The mass-based size distributions of the OA factors were estimated based on multilinear analysis of the size-resolved mass spectra of organics. Both HOA and BBOA peaked at ˜140 nm in vacuum aerodynamic diameter (Dva) while OOA peaked at an accumulation mode of ˜460 nm. COA exhibited a unique size distribution with two size modes centering at ˜200 nm and 450 nm respectively. This study highlights the leading roles played by anthropogenic POA emissions, primarily from traffic, cooking and residential heating, in <span class="hlt">aerosol</span> pollution in Fresno in wintertime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.A21A0082M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.A21A0082M"><span>Spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing in summer 2006: Model evaluation and source apportionment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsui, H.; Koike, M.; Kondo, Y.; Takegawa, N.; Kita, K.; Miyazaki, Y.; Hu, M.; Chang, S.; Blake, D. R.; Fast, J. D.; Zaveri, R. A.; Streets, D. G.; Zhang, Q.; Zhu, T.</p> <p>2009-12-01</p> <p>Regional <span class="hlt">aerosol</span> model calculations were made using the WRF-CMAQ and WRF-chem models to study spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing, China, in the summer of 2006, when the CAREBEIJING-2006 intensive campaign was conducted. Model calculations captured temporal variations of primary (such as elemental carbon, EC) and secondary (such as sulfate) <span class="hlt">aerosols</span> observed in and around Beijing. The spatial distributions of <span class="hlt">aerosol</span> optical depth observed by the MODIS satellite sensors were also reproduced over northeast China. Model calculations showed distinct differences in spatial distributions between primary and secondary <span class="hlt">aerosols</span> in association with synoptic-<span class="hlt">scale</span> meteorology. Secondary <span class="hlt">aerosols</span> increased in air around Beijing on a <span class="hlt">scale</span> of about 1000 x 1000 km2 under an anticyclonic pressure system. This airmass was transported northward from the high anthropogenic emission area extending south of Beijing with continuous photochemical production. Subsequent cold front passage brought clean air from the north, and polluted air around Beijing was swept to the south of Beijing. This cycle was repeated about once a week and was found to be responsible for observed enhancements/reductions of <span class="hlt">aerosols</span> at the intensive measurement sites. In contrast to secondary <span class="hlt">aerosols</span>, the spatial distributions of primary <span class="hlt">aerosols</span> (EC) reflected those of emissions, resulting in only slight variability despite the changes in synoptic-<span class="hlt">scale</span> meteorology. In accordance with these results, source apportionment simulations revealed that primary <span class="hlt">aerosols</span> around Beijing were controlled by emissions within 100 km around Beijing within the preceding 24 hours, while emissions as far as 500 km and within the preceding 3 days were found to affect secondary <span class="hlt">aerosols</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.5427D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.5427D"><span>Reflections on current and future applications of multiangle imaging to <span class="hlt">aerosol</span> and cloud remote sensing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diner, David</p> <p>2010-05-01</p> <p>The Multi-angle Imaging SpectroRadiometer (MISR) instrument has been collecting global Earth data from NASA's Terra satellite since February 2000. With its 9 along-track view angles, 4 spectral bands, intrinsic spatial resolution of 275 m, and stable radiometric and geometric calibration, no instrument that combines MISR's attributes has previously flown in space, nor is there is a similar capability currently available on any other satellite platform. Multiangle imaging offers several tools for remote sensing of <span class="hlt">aerosol</span> and cloud properties, including bidirectional reflectance and scattering measurements, stereoscopic pattern matching, time lapse sequencing, and potentially, optical tomography. Current data products from MISR employ several of these techniques. Observations of the intensity of scattered light as a function of view angle and wavelength provide accurate measures of <span class="hlt">aerosol</span> optical depths (AOD) over land, including bright desert and urban source regions. Partitioning of AOD according to retrieved particle classification and incorporation of <span class="hlt">height</span> information improves the relationship between AOD and surface PM2.5 (fine particulate matter, a regulated air pollutant), constituting an important step toward a satellite-based particulate pollution monitoring system. Stereoscopic cloud-top <span class="hlt">heights</span> provide a unique metric for detecting interannual variability of clouds and exceptionally high quality and sensitivity for detection and <span class="hlt">height</span> retrieval for low-level clouds. Using the several-minute time interval between camera views, MISR has enabled a pole-to-pole, <span class="hlt">height</span>-resolved atmospheric wind measurement system. Stereo imagery also makes possible global measurement of the injection <span class="hlt">heights</span> and advection speeds of smoke plumes, volcanic plumes, and dust clouds, for which a large database is now available. To build upon what has been learned during the first decade of MISR observations, we are evaluating algorithm updates that not only refine retrieval</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12492171','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12492171"><span>Indian <span class="hlt">aerosols</span>: present status.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mitra, A P; Sharma, C</p> <p>2002-12-01</p> <p>This article presents the status of <span class="hlt">aerosols</span> in India based on the research activities undertaken during last few decades in this region. Programs, like International Geophysical Year (IGY), Monsoon Experiment (MONEX), Indian Middle Atmospheric Program (IMAP) and recently conducted Indian Ocean Experiment (INDOEX), have thrown new lights on the role of <span class="hlt">aerosols</span> in global change. INDOEX has proved that the effects of <span class="hlt">aerosols</span> are no longer confined to the local levels but extend at regional as well as global <span class="hlt">scales</span> due to occurrence of long range transportation of <span class="hlt">aerosols</span> from source regions along with wind trajectories. The loading of <span class="hlt">aerosols</span> in the atmosphere is on rising due to energy intensive activities for developmental processes and other anthropogenic activities. One of the significant observation of INDOEX is the presence of high concentrations of carbonaceous <span class="hlt">aerosols</span> in the near persistent winter time haze layer over tropical Indian Ocean which have probably been emitted from the burning of fossil-fuels and biofuels in the source region. These have significant bearing on the radiative forcing in the region and, therefore, have potential to alter monsoon and hydrological cycles. In general, the SPM concentrations have been found to be on higher sides in ambient atmosphere in many Indian cities but the NOx concentrations have been found to be on lower side. Even in the haze layer over Indian Ocean and surrounding areas, the NOx concentrations have been reported to be low which is not conducive of O3 formation in the haze/smog layer. The acid rain problem does not seem to exist at the moment in India because of the presence of neutralizing soil dust in the atmosphere. But the high particulate concentrations in most of the cities' atmosphere in India are of concern as it can cause deteriorated health conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890046838&hterms=australian+copyright&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Daustralian%2Bcopyright','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890046838&hterms=australian+copyright&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Daustralian%2Bcopyright"><span>Australian <span class="hlt">aerosol</span> backscatter survey</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gras, John L.; Jones, William D.</p> <p>1989-01-01</p> <p>This paper describes measurements of the atmospheric backscatter coefficient in and around Australia during May and June 1986. One set of backscatter measurements was made with a CO2 lidar operating at 10.6 microns; the other set was obtained from calculations using measured <span class="hlt">aerosol</span> parameters. Despite the two quite different data collection techniques, there is quite good agreement between the two methods. Backscatter values range from near 1 x 10 to the -8th/m per sr near the surface to 4 - 5 x 10 to the -11th/m per sr in the free troposphere at 5-7-km altitude. The values in the free troposphere are somewhat lower than those typically measured at the same <span class="hlt">height</span> in the Northern Hemisphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940009198','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940009198"><span>Determining the solar-flare photospheric <span class="hlt">scale</span> <span class="hlt">height</span> from SMM gamma-ray measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lingenfelter, Richard E.</p> <p>1991-01-01</p> <p>A connected series of Monte Carlo programs was developed to make systematic calculations of the energy, temporal and angular dependences of the gamma-ray line and neutron emission resulting from such accelerated ion interactions. Comparing the results of these calculations with the Solar Maximum Mission/Gamma Ray Spectrometer (SMM/GRS) measurements of gamma-ray line and neutron fluxes, the total number and energy spectrum of the flare-accelerated ions trapped on magnetic loops at the Sun were determined and the angular distribution, pitch angle scattering, and mirroring of the ions on loop fields were constrained. Comparing the calculations with measurements of the time dependence of the neutron capture line emission, a determination of the He-3/H ratio in the photosphere was also made. The diagnostic capabilities of the SMM/GRS measurements were extended by developing a new technique to directly determine the effective photospheric <span class="hlt">scale</span> <span class="hlt">height</span> in solar flares from the neutron capture gamma-ray line measurements, and critically test current atmospheric models in the flare region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014280','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014280"><span><span class="hlt">Aerosol</span>-Induced Changes of Convective Cloud Anvils Produce Strong Climate Warming</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Koren, I.; Remer, L. A.; Altaratz, O.; Martins, J. V.; Davidi, A.</p> <p>2010-01-01</p> <p>The effect of <span class="hlt">aerosol</span> on clouds poses one of the largest uncertainties in estimating the anthropogenic contribution to climate change. Small human-induced perturbations to cloud characteristics via <span class="hlt">aerosol</span> pathways can create a change in the top-of-atmosphere radiative forcing of hundreds of Wm(exp-2) . Here we focus on links between <span class="hlt">aerosol</span> and deep convective clouds of the Atlantic and Pacific Intertropical Convergence Zones, noting that the <span class="hlt">aerosol</span> environment in each region is entirely different. The tops of these vertically developed clouds consisting of mostly ice can reach high levels of the atmosphere, overshooting the lower stratosphere and reaching altitudes greater than 16 km. We show a link between <span class="hlt">aerosol</span>, clouds and the free atmosphere wind profile that can change the magnitude and sign of the overall climate radiative forcing. We find that increased <span class="hlt">aerosol</span> loading is associated with taller cloud towers and anvils. The taller clouds reach levels of enhanced wind speeds that act to spread and thin the anvi1 clouds, increasing areal coverage and decreasing cloud optical depth. The radiative effect of this transition is to create a positive radiative forcing (warming) at top-of-atmosphere. Furthermore we introduce the cloud optical depth (r), cloud <span class="hlt">height</span> (Z) forcing space and show that underestimation of radiative forcing is likely to occur in cases of non homogenous clouds. Specifically, the mean radiative forcing of towers and anvils in the same scene can be several times greater than simply calculating the forcing from the mean cloud optical depth in the scene. Limitations of the method are discussed, alternative sources of <span class="hlt">aerosol</span> loading are tested and meteorological variance is restricted, but the trend of taller clouds; increased and thinner anvils associated with increased <span class="hlt">aerosol</span> loading remains robust through all the different tests and perturbations.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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://ntrs.nasa.gov/search.jsp?R=20070015993&hterms=inventory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinventory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070015993&hterms=inventory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinventory"><span>Compilation of a Global Emission Inventory from 1980 to 2000 for Global Model Simulations of the Long-term Trend of Tropospheric <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Diehl, T. L.; Mian, Chin; Bond, T. C.; Carn, S. A.; Duncan, B. N.; Krotkov, N. A.; Streets, D. G.</p> <p>2007-01-01</p> <p>The approach to create a comprehensive emission inventory for the time period 1980 to 2000 is described in this paper. We have recently compiled an emission database, which we will use for a 21 year simulation of tropospheric <span class="hlt">aerosols</span> with the GOCART model. Particular attention was paid to the time-dependent SO2, black carbon and organic carbon <span class="hlt">aerosol</span> emissions. For the emission of SO2 from sporadically erupting volcanoes, we assembled emission data from the Global Volcanism Program of the Smithsonian Institution, using the VEI to derive the volcanic cloud <span class="hlt">height</span> and the SO2 amount, and amended this dataset by the SO2 emission data from the TOMS instrument when available. 3-dimensional aircraft emission data was obtained for a number of years from the AEAP project, converted from burned fuel to SO2 and interpolated to each year, taking the sparsity of the flight patterns into account. Other anthopogenic SO2 emissions are based on gridded emissions from the EDGAR 2000 database (excluding sources from aircraft, biomass burning and international ship traffic), which were <span class="hlt">scaled</span> to individual years with country/regional based emission inventories. Gridded SO2 emissions from international ship traffic for 2000 and the <span class="hlt">scaling</span> factors for other years are from [Eyring et al., 2005]. We used gridded anthropogenic black and organic carbon emissions for 1996 [Bond et al., 2005], again excluding aircraft, biomass burning and ship sources. These emissions were <span class="hlt">scaled</span> with regional based emission inventories from 1980 to 2000 to derive gridded emissions for each year. The biomass burning emissions are based on a climatology, which is <span class="hlt">scaled</span> with regional <span class="hlt">scaling</span> factors derived from the TOMS <span class="hlt">aerosol</span> index and the AVHRR/ATSR fire counts to each year [Duncan et al., 2003]. Details on the integration of the information from the various sources will be provided and the distribution patterns and total emissions in the final product will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060012307&hterms=inventory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dinventory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060012307&hterms=inventory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dinventory"><span>Compilation of a Global Emission Inventory from 1980 to 2000 for Global Model Simulations of the Long-term Trend of Tropospheric <span class="hlt">Aerosols</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Diehl, Thomas L.; Chin, Mian; Bond, Tami C.; Carn, SImon A.; Duncan, Bryan N.; Krotkov, Nickolay A.; Streets, David G.</p> <p>2006-01-01</p> <p>The approach to create a comprehensive emission inventory for the time period 1980 to 2000 is described in this paper. We have recently compiled an emission database, which we will use for a 21 year simulation of tropospheric <span class="hlt">aerosols</span> with the GOCART model. Particular attention was paid to the time-dependent SO2, black carbon and organic carbon <span class="hlt">aerosol</span> emissions. For the emission of SO2 from sporadically erupting volcanoes, we assembled emission data from the Global Volcanism Program of the Smithsonian Institution, using the VEI to derive the volcanic cloud <span class="hlt">height</span> and the SO2 amount, and amended this dataset by the SO2 emission data from the TOMS instrument when available. 3-dimensional aircraft emission data was obtained for a number of years from the AEAP project, converted from burned fuel to SO2 and interpolated to each year, taking the sparsity of the flight patterns into account. Other anthropogenic SO2 emissions are based on gridded emissions from the EDGAR 2000 database (excluding sources from aircraft, biomass burning and international ship traffic), which were <span class="hlt">scaled</span> to individual years with country/regional based emission inventories. Gridded SO2 emissions from international ship traffic for 2000 and the <span class="hlt">scaling</span> factors for other years are from [Eyring et al., 2005]. We used gridded anthropogenic black and organic carbon emissions for 1996 [Bond et al., 2005], again excluding aircraft, biomass burning and ship sources. These emissions were <span class="hlt">scaled</span> with regional based emission inventories from 1980 to 2000 to derive gridded emissions for each year. The biomass burning emissions are based on a climatology, which is <span class="hlt">scaled</span> with regional <span class="hlt">scaling</span> factors derived from the TOMS <span class="hlt">aerosol</span> index and the AVHRR/ASTR fire counts to each year [Duncan et al., 2003]. Details on the integration of the information from the various sources will be provided and the distribution patterns and total emissions in the final product will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.6558G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.6558G"><span>The effect of cloud screening on MAX-DOAS <span class="hlt">aerosol</span> retrievals.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gielen, Clio; Van Roozendael, Michel; Hendrik, Francois; Fayt, Caroline; Hermans, Christian; Pinardi, Gaia; De Backer, Hugo; De Bock, Veerle; Laffineur, Quentin; Vlemmix, Tim</p> <p>2014-05-01</p> <p>In recent years, ground-based multi-axis differential absorption spectroscopy (MAX-DOAS) has shown to be ideally suited for the retrieval of tropospheric trace gases and deriving information on the <span class="hlt">aerosol</span> properties. These measurements are invaluable to our understanding of the physics and chemistry of the atmospheric system, and the impact on the Earth's climate. Unfortunately, MAX-DOAS measurements are often performed under strong non-clear-sky conditions, causing strong data quality degradation and uncertainties on the retrievals. Here we present the result of our cloud-screening method, using the colour index (CI), on <span class="hlt">aerosol</span> retrievals from MAX-DOAS measurements (AOD and vertical profiles). We focus on two large data sets, from the Brussels and Beijing area. Using the CI we define 3 different sky conditions: bad (=full thick cloud cover/extreme <span class="hlt">aerosols</span>), mediocre (=thin clouds/<span class="hlt">aerosols</span>) and good (=clear sky). We also flag the presence of broken/scattered clouds. We further compare our cloud-screening method with results from cloud-cover fractions derived from thermic infrared measurements. In general, our method shows good results to qualify the sky and cloud conditions of MAX-DOAS measurements, without the need for other external cloud-detection systems. Removing data under bad-sky and broken-cloud conditions results in a strongly improved agreement, in both correlation and slope, between the MAX-DOAS <span class="hlt">aerosol</span> retrievals and data from other instruments (e.g. AERONET, Brewer). With the improved AOD retrievals, the seasonal and diurnal variations of the <span class="hlt">aerosol</span> content and vertical distribution at both sites can be investigated in further detail. By combining with additional information derived by other instruments (Brewer, lidar, ...) operated at the stations, we will further study the observed <span class="hlt">aerosol</span> characteristics, and their influence on and by meteorological conditions such as clouds and/or the boundary layer <span class="hlt">height</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ERL....10a5003B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ERL....10a5003B"><span>Observations and projections of visibility and <span class="hlt">aerosol</span> optical thickness (1956-2100) in the Netherlands: impacts of time-varying <span class="hlt">aerosol</span> composition and hygroscopicity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boers, R.; van Weele, M.; van Meijgaard, E.; Savenije, M.; Siebesma, A. P.; Bosveld, F.; Stammes, P.</p> <p>2015-01-01</p> <p>Time series of visibility and <span class="hlt">aerosol</span> optical thickness for the Netherlands have been constructed for 1956-2100 based on observations and <span class="hlt">aerosol</span> mass scenarios. <span class="hlt">Aerosol</span> optical thickness from 1956 to 2013 has been reconstructed by converting time series of visibility to visible extinction which in turn are converted to <span class="hlt">aerosol</span> optical thickness using an appropriate <span class="hlt">scaling</span> depth. The reconstruction compares closely with remote sensing observations of <span class="hlt">aerosol</span> optical thickness between 1960 and 2013. It appears that <span class="hlt">aerosol</span> optical thickness was relatively constant over the Netherlands in the years 1955-1985. After 1985, visibility has improved, while at the same time <span class="hlt">aerosol</span> optical thickness has decreased. Based on <span class="hlt">aerosol</span> emission scenarios for the Netherlands three <span class="hlt">aerosol</span> types have been identified: (1) a constant background consisting of sea salt and mineral dust, (2) a hydrophilic anthropogenic inorganic mixture, and (3) a partly hydrophobic mixture of black carbon (BC) and organic <span class="hlt">aerosols</span> (OAs). A reduction in overall <span class="hlt">aerosol</span> concentration turns out to be the most influential factor in the reduction in <span class="hlt">aerosol</span> optical thickness. But during 1956-1985, an upward trend in hydrophilic <span class="hlt">aerosols</span> and associated upward trend in optical extinction has partly compensated the overall reduction in optical extinction due to the reduction in less hydrophilic BC and OAs. A constant optical thickness ensues. This feature highlights the influence of <span class="hlt">aerosol</span> hygroscopicity on time-varying signatures of atmospheric optical properties. Within the hydrophilic inorganic <span class="hlt">aerosol</span> mixture there is a gradual shift from sulfur-based (1956-1985) to a nitrogen-based water <span class="hlt">aerosol</span> chemistry (1990 onwards) but always modulated by the continual input of sodium from sea salt. From 2013 to 2100, visibility is expected to continue its increase, while at the same time optical thickness is foreseen to continue to decrease. The contribution of the hydrophilic mixture to the <span class="hlt">aerosol</span> optical</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.1132G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.1132G"><span>Radiative effects of absorbing <span class="hlt">aerosols</span> over northeastern India: Observations and model simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gogoi, Mukunda M.; Babu, S. Suresh; Moorthy, K. Krishna; Bhuyan, Pradip Kumar; Pathak, Binita; Subba, Tamanna; Chutia, Lakhima; Kundu, Shyam Sundar; Bharali, Chandrakala; Borgohain, Arup; Guha, Anirban; De, Barin Kumar; Singh, Brajamani; Chin, Mian</p> <p>2017-01-01</p> <p>Multiyear measurements of spectral properties of <span class="hlt">aerosol</span> absorption are examined over four geographically distinct locations of northeastern India. Results indicated significant spatiotemporal variation in <span class="hlt">aerosol</span> absorption coefficients (σabs) with highest values in winter and lowest in monsoon. The western parts of the region, close to the outflow of Indo-Gangetic Plains, showed higher values of σabs and black carbon (BC) concentration—mostly associated with fossil fuel combustion. But, the eastern parts showed higher contributions from biomass-burning <span class="hlt">aerosols</span>, as much as 20-25% to the total <span class="hlt">aerosol</span> absorption, conspicuously during premonsoon season. This is attributed to a large number of burning activities over the Southeast Asian region, as depicted from Moderate Resolution Imaging Spectroradiometer fire count maps, whose spatial extent and magnitude peaks during March/April. The nearly consistent high values of <span class="hlt">aerosol</span> index (AI) and layer <span class="hlt">height</span> from Ozone Monitoring Instrument indicate the presence of absorbing <span class="hlt">aerosols</span> in the upper atmosphere. The observed seasonality has been captured fairly well by Goddard Chemistry <span class="hlt">Aerosol</span> Radiation and Transport (GOCART) as well as Weather Research and Forecasting-Chemistry (WRF-Chem) model simulations. The ratio of column-integrated optical depths due to particulate organic matter and BC from GOCART showed good coincidence with satellite-based observations, indicating the increased vertical dispersion of absorbing <span class="hlt">aerosols</span>, probably by the additional local convection due to higher fire radiative power caused by the intense biomass-burning activities. In the WRF-Chem though underperformed by different magnitude in winter, the values are closer or overestimated near the burnt areas. Atmospheric forcing due to BC was highest ( 30 Wm-2) over the western part associated with the fossil fuel combustion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23207404','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23207404"><span>Optimal <span class="hlt">scaling</span> of weight and waist circumference to <span class="hlt">height</span> for maximal association with DXA-measured total body fat mass by sex, age and race/ethnicity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heo, M; Kabat, G C; Gallagher, D; Heymsfield, S B; Rohan, T E</p> <p>2013-08-01</p> <p>Body mass index (BMI; weight (Wt)/<span class="hlt">height</span> (Ht) (in kg m(-2)) and waist circumference (WC) are widely used as proxy anthropometric measures for total adiposity. Little is known about what <span class="hlt">scaling</span> power of 'x' in both Wt(kg)/Ht(m)(x) and WC(m)/Ht(m)(x) is maximally associated with measured total body fat mass (TBFM). Establishing values for x would provide the information needed to create optimum anthropometric surrogate measures of adiposity. To estimate the value of 'x' that renders Wt/Ht(x) and WC/Ht(x) maximally associated with DXA-measured TBFM. Participants of the NHANES 1999-2004 surveys, stratified by sex (men, women), race/ethnicity (non-Hispanic whites, non-Hispanic blacks, Mexican-Americans), and age(18-29, 30-49, 50-84 years). We apply a grid search by increasing x from 0.0-3.0 by increments of 0.1 to the simple regression models, TBFM=b0+b1*(Wt/Ht(x)) and TBFM=b0+b1*(WC/Ht(x)) to obtain an estimate of x that results in the greatest R(2), taking into account complex survey design features and multiply imputed data. R(2)'s for BMI are 0.86 for men (N=6544) and 0.92 for women (N=6362). The optimal powers x for weight are 1.0 (R(2)=0.90) for men and 0.8 (R(2)=0.96) for women. The optimal power x for WC is 0, that is, no <span class="hlt">scaling</span> of WC to <span class="hlt">height</span>, for men (R(2)=0.90) or women (R(2)=0.82). The optimal powers for weight across nine combinations of race/ethnicity and age groups for each sex vary slightly (x=0.8-1.3) whereas the optimal <span class="hlt">scaling</span> powers for WC are all 0 for both sexes except for non-Hispanic black men aged 18-29y (x=0.1). Although the weight-for-<span class="hlt">height</span> indices with optimal powers are not independent of <span class="hlt">height</span>, they yield more accurate TBFM estimates than BMI. In reference to TBFM, Wt/Ht and Wt/Ht(0.8) are the optimal weight-for-<span class="hlt">height</span> indices for men and women, respectively, whereas WC alone, without Ht adjustment, is the optimal WC-for-<span class="hlt">height</span> index for both sexes. Thus, BMI, an index independent of <span class="hlt">height</span>, may be less useful when predicting TBFM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17..721B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17..721B"><span>Decadal-<span class="hlt">scale</span> relationship between measurements of <span class="hlt">aerosols</span>, land-use change, and fire over Southeast Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blake Cohen, Jason; Lecoeur, Eve; Loong Ng, Daniel Hui</p> <p>2017-01-01</p> <p>A simultaneous analysis of 13 years of remotely sensed data of land cover, fires, precipitation, and <span class="hlt">aerosols</span> from the MODIS, TRMM, and MISR satellites and the AERONET network over Southeast Asia is performed, leading to a set of robust relationships between land-use change and fire being found on inter-annual and intra-annual <span class="hlt">scales</span> over Southeast Asia, reflecting the heavy amounts of anthropogenic influence over land-use change and fires in this region of the world. First, we find that fires occur annually, but with a considerable amount of variance in their onset, duration, and intensity from year to year, and from two separate regions within Southeast Asia. Second, we show that a simple regression model of the land-cover, fire, and precipitation data can be used to recreate a robust representation of the timing and magnitude of measured <span class="hlt">aerosol</span> optical depth (AOD) from multiple measurements sources of this region using either 8-day (better for onset and duration) or monthly (better for magnitude) measurements, but not daily measurements. We find that the reconstructed AOD matches the timing and intensity from AERONET measurements to within 70 to 90 % and the timing and intensity of MISR measurements to within 50 to 95 %. This is a unique finding in this part of the world since cloud-covered regions are large, yet the model is still robustly capable, including over regions where no fires are observed and hence no emissions would be expected to contribute to AOD. Third, we determine that while Southeast Asia is a source region of such intense smoke emissions, portions of it are also impacted by smoke transported from other regions. There are regions in northern Southeast Asia which have two annual AOD peaks, one during the local fire season and the other, smaller peak corresponding to a combination of some local smoke sources as well as transport of <span class="hlt">aerosols</span> from fires in southern Southeast Asia and possibly even from anthropogenic sources in South Asia. Overall</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.A33B0896G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.A33B0896G"><span>Evaluation of data from the Vaisala CT25K for Estimation of PM10 Concentration and Mixing <span class="hlt">Heights</span> in an Urban Environment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gunter, R. L.; Hosker, R. P.</p> <p>2005-12-01</p> <p>During the month of August, the Urban Dispersion Project was conducted in New York City. NOAA's Atmospheric and Turbulence Division (ATDD), Oak Ridge, TN operated a Vaisala CT25K Ceilometer for a two-week timeframe during the project. Typically, ceilometer measurements are used for cloud <span class="hlt">height</span> determination. It has been found that during dry conditions, there is a good correlation between the ceilometer near- range backscatter and in situ PM10 concentration readings. In addition, it also has been determined that the ceilometer is a suitable instrument for determining the convective mixing <span class="hlt">height</span> (MH). <span class="hlt">Aerosol</span> concentrations are calculated and mixing <span class="hlt">heights</span> are estimated using data from the ceilometer during dry conditions in Manhattan. Mixing <span class="hlt">heights</span> are compared to radiosonde data taken during the project.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.5435H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.5435H"><span>Development and first application of an <span class="hlt">Aerosol</span> Collection Module (ACM) for quasi online compound specific <span class="hlt">aerosol</span> measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hohaus, Thorsten; Kiendler-Scharr, Astrid; Trimborn, Dagmar; Jayne, John; Wahner, Andreas; Worsnop, Doug</p> <p>2010-05-01</p> <p>Atmospheric <span class="hlt">aerosols</span> influence climate and human health on regional and global <span class="hlt">scales</span> (IPCC, 2007). In many environments organics are a major fraction of the <span class="hlt">aerosol</span> influencing its properties. Due to the huge variety of organic compounds present in atmospheric <span class="hlt">aerosol</span> current measurement techniques are far from providing a full speciation of organic <span class="hlt">aerosol</span> (Hallquist et al., 2009). The development of new techniques for compound specific measurements with high time resolution is a timely issue in organic <span class="hlt">aerosol</span> research. Here we present first laboratory characterisations of an <span class="hlt">aerosol</span> collection module (ACM) which was developed to allow for the sampling and transfer of atmospheric PM1 <span class="hlt">aerosol</span>. The system consists of an aerodynamic lens system focussing particles on a beam. This beam is directed to a 3.4 mm in diameter surface which is cooled to -30 °C with liquid nitrogen. After collection the <span class="hlt">aerosol</span> sample can be evaporated from the surface by heating it to up to 270 °C. The sample is transferred through a 60cm long line with a carrier gas. In order to test the ACM for linearity and sensitivity we combined it with a GC-MS system. The tests were performed with octadecane <span class="hlt">aerosol</span>. The octadecane mass as measured with the ACM-GC-MS was compared versus the mass as calculated from SMPS derived total volume. The data correlate well (R2 0.99, slope of linear fit 1.1) indicating 100 % collection efficiency. From 150 °C to 270 °C no effect of desorption temperature on transfer efficiency could be observed. The ACM-GC-MS system was proven to be linear over the mass range 2-100 ng and has a detection limit of ~ 2 ng. First experiments applying the ACM-GC-MS system were conducted at the Jülich <span class="hlt">Aerosol</span> Chamber. Secondary organic <span class="hlt">aerosol</span> (SOA) was formed from ozonolysis of 600 ppbv of b-pinene. The major oxidation product nopinone was detected in the <span class="hlt">aerosol</span> and could be shown to decrease from 2 % of the total <span class="hlt">aerosol</span> to 0.5 % of the <span class="hlt">aerosol</span> over the 48 hours of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.........5O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.........5O"><span>Development of 2-D-MAX-DOAS and retrievals of trace gases and <span class="hlt">aerosols</span> optical properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ortega, Ivan</p> <p></p> <p>Air pollution is a major problem worldwide that adversely a_ects human health, impacts ecosystems and climate. In the atmosphere, there are hundreds of important compounds participating in complex atmospheric reactions linked to air quality and climate. <span class="hlt">Aerosols</span> are relevant because they modify the radiation balance, a_ect clouds, and thus Earth albedo. The amount of <span class="hlt">aerosol</span> is often characterized by the vertical integral through the entire <span class="hlt">height</span> of the atmosphere of the logarithm fraction of incident light that is extinguished called <span class="hlt">Aerosol</span> Optical Depth (AOD). The AOD at 550 nm (AOD550) over land is 0.19 (multi annual global mean), and that over oceans is 0.13. About 43 % of the Earth surface shows AOD550 smaller than 0.1. There is a need for measurement techniques that are optimized to measure <span class="hlt">aerosol</span> optical properties under low AOD conditions, sample spatial <span class="hlt">scales</span> that resemble satellite ground-pixels and atmospheric models, and help integrate remote sensing and in-situ observations to obtain optical closure on the effects of <span class="hlt">aerosols</span> and trace gases in our changing environment. In this work, I present the recent development of the University of Colorado two dimensional (2-D) Multi-AXis Differential Optical Absorption Spectroscopy (2-D-MAX-DOAS) instrument to measure the azimuth and altitude distribution of trace gases and <span class="hlt">aerosol</span> optical properties simultaneously with a single instrument. The instrument measures solar scattered light from any direction in the sky, including direct sun light in the hyperspectral domain. In Chapter 2, I describe the capabilities of 2-D measurements in the context of retrievals of azimuth distributions of nitrogen dioxide (NO2), formaldehyde (HCHO), and glyoxal (CHOCHO), which are precursors for tropospheric O3 and <span class="hlt">aerosols</span>. The measurements were carried out during the Multi-Axis DOAS Comparison campaign for <span class="hlt">Aerosols</span> and Trace gases (MAD-CAT) campaign in Mainz, Germany and show the ability to bridge spatial <span class="hlt">scales</span> to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1343564','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1343564"><span>Cloud, <span class="hlt">Aerosol</span>, and Complex Terrain Interactions (CACTI) Preliminary Science Plan</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>Varble, Adam; Nesbitt, Steve; Salio, Paola</p> <p></p> <p>General circulation models and downscaled regional models exhibit persistent biases in deep convective initiation location and timing, cloud top <span class="hlt">height</span>, stratiform area and precipitation fraction, and anvil coverage. Despite important impacts on the distribution of atmospheric heating, moistening, and momentum, nearly all climate models fail to represent convective organization, while system evolution is not represented at all. Improving representation of convective systems in models requires characterization of their predictability as a function of environmental conditions, and this characterization depends on observing many cases of convective initiation, non-initiation, organization, and non-organization. The Cloud, <span class="hlt">Aerosol</span>, and Complex Terrain Interactions (CACTI) experiment inmore » the Sierras de Córdoba mountain range of north-central Argentina is designed to improve understanding of cloud life cycle and organization in relation to environmental conditions so that cumulus, microphysics, and <span class="hlt">aerosol</span> parameterizations in multi-<span class="hlt">scale</span> models can be improved. The Sierras de Córdoba range has a high frequency of orographic boundary-layer clouds, many reaching congestus depths, many initiating into deep convection, and some organizing into mesoscale systems uniquely observable from a single fixed site. Some systems even grow upscale to become among the deepest, largest, and longest-lived in the world. These systems likely contribute to an observed regional trend of increasing extreme rainfall, and poor prediction of them likely contributes to a warm, dry bias in climate models downstream of the Sierras de Córdoba range in a key agricultural region. Many environmental factors influence the convective lifecycle in this region including orographic, low-level jet, and frontal circulations, surface fluxes, synoptic vertical motions influenced by the Andes, cloud detrainment, and <span class="hlt">aerosol</span> properties. Local and long-range transport of smoke resulting from biomass</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24300792','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24300792"><span>Fear of <span class="hlt">heights</span> and visual <span class="hlt">height</span> intolerance.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brandt, Thomas; Huppert, Doreen</p> <p>2014-02-01</p> <p>The aim of this review is, first, to cover the different aspects of visual <span class="hlt">height</span> intolerance such as historical descriptions, definition of terms, phenomenology of the condition, neurophysiological control of gaze, stance and locomotion, and therapy, and, second, to identify warranted epidemiological and experimental studies. Vivid descriptions of fear of <span class="hlt">heights</span> can be found in ancient texts from the Greek, Roman, and Chinese classics. The life-time prevalence of visual <span class="hlt">height</span> intolerance is as high as 28% in the general population, and about 50% of those who are susceptible report an impact on quality of life. When exposed to <span class="hlt">heights</span>, visual exploration by eye and head movements is restricted, and the velocity of locomotion is reduced. Therapy for fear of <span class="hlt">heights</span> is dominated by the behavioral techniques applied during real or virtual reality exposure. Their efficacy might be facilitated by the administration of D-cycloserine or glucocorticoids. Visual <span class="hlt">height</span> intolerance has a considerable impact on daily life and interpersonal interactions. It is much more frequent than fear of <span class="hlt">heights</span>, which is defined as an environmental subtype of a specific phobia. There is certainly a continuum stretching from acrophobia to a less-pronounced visual <span class="hlt">height</span> intolerance, to which the categorical distinction of a specific phobia does not apply.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870007984','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870007984"><span>SAGE <span class="hlt">aerosol</span> measurements. Volume 3: January 1, 1981 to November 18, 1981</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mccormick, M. Patrick</p> <p>1987-01-01</p> <p>The Stratospheric <span class="hlt">Aerosol</span> and Gas Experiment (SAGE) satellite system, launched February 18, 1979, obtained profiles of <span class="hlt">aerosol</span> extinction at 1.00 micron and 0.45 micron ozone concentration, and nitrogen dioxide concentration. Data taken during sunset events are presented in the form of zonal and seasonal averages of <span class="hlt">aerosol</span> extinction of 1.00 micron and 0.45 micron, ratios of <span class="hlt">aerosol</span> extinction to molecular extinction at 1.00 micron and ratios of <span class="hlt">aerosol</span> extinction at 0.45 micron to <span class="hlt">aerosol</span> extinction at 1.00 micron. Averages for 1981 are shown in tables, and in profile and contour plots (as a function of altitude and latitude). In addition, temperature data provided by NOAA for the time and location of each SAGE measurement are averaged and shown in a similar format. The stratospheric <span class="hlt">aerosol</span> distribution for 1981 shows effects of volcanically injected material from eruptions of Ulawun, Alaid, and Pagan. Peak values of <span class="hlt">aerosol</span> extinction at 0.45 micron and 1.00 micron were 2 to 4 times higher than typical peak values observed during near background conditions. Stratospheric <span class="hlt">aerosol</span> optical depth values at 1.00 microns increased by a factor of about 2 from near background levels in regions of volcanic activity. During the year, these values ranged from between 0.001 and 0.006. The largest were near the location of a recent eruption. The distribution of the ratio of <span class="hlt">aerosol</span> to molecular extinction at 1.00 microns also showed that maximum values are found in the vicinity of an eruption. These maximums varied in altitude, but remained below a <span class="hlt">height</span> of about 25 km. No attempt has been made to give detailed explanations or interpretations of these data. The intent is to provide, in a ready-to-use visual format, representative zonal and seasonal averages of <span class="hlt">aerosol</span> extinction data for the third calendar year of the SAGE data set to facilitate atmospheric and climatic studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1393424','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1393424"><span>Electrospray ionizer for mass spectrometry of <span class="hlt">aerosol</span> particles</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>He, Siqin; Hogan, Chris; Li, Lin; Liu, Benjamin Y. H.; Naqwi, Amir; Romay, Francisco</p> <p>2017-09-19</p> <p>A device and method are disclosed to apply ESI-based mass spectroscopy to submicrometer and nanometer <span class="hlt">scale</span> <span class="hlt">aerosol</span> particles. Unipolar ionization is utilized to charge the particles in order to collect them electrostatically on the tip of a tungsten rod. Subsequently, the species composing the collected particles are dissolved by making a liquid flow over the tungsten rod. This liquid with dissolved <span class="hlt">aerosol</span> contents is formed into highly charged droplets, which release unfragmented ions for mass spectroscopy, such as time-of-flight mass spectroscopy. The device is configured to operate in a switching mode, wherein <span class="hlt">aerosol</span> deposition occurs while solvent delivery is turned off and vice versa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACPD...1410311Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACPD...1410311Z"><span>Technical Note: On the use of nudging for <span class="hlt">aerosol</span>-climate model intercomparison studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, K.; Wan, H.; Liu, X.; Ghan, S. J.; Kooperman, G. J.; Ma, P.-L.; Rasch, P. J.</p> <p>2014-04-01</p> <p>Nudging is an assimilation technique widely used in the development and evaluation of climate models. Constraining the simulated wind and temperature fields using global weather reanalysis facilitates more straightforward comparison between simulation and observation, and reduces uncertainties associated with natural variabilities of the large-<span class="hlt">scale</span> circulation. On the other hand, the forcing introduced by nudging can be strong enough to change the basic characteristics of the model climate. In the paper we show that for the Community Atmosphere Model version 5, due to the systematic temperature bias in the standard model and the sensitivity of simulated ice formation to anthropogenic <span class="hlt">aerosol</span> concentration, nudging towards reanalysis results in substantial reductions in the ice cloud amount and the impact of anthropogenic <span class="hlt">aerosols</span> on longwave cloud forcing. In order to reduce discrepancies between the nudged and unconstrained simulations and meanwhile take the advantages of nudging, two alternative experimentation methods are evaluated. The first one constrains only the horizontal winds. The second method nudges both winds and temperature, but replaces the long-term climatology of the reanalysis by that of the model. Results show that both methods lead to substantially improved agreement with the free-running model in terms of the top-of-atmosphere radiation budget and cloud ice amount. The wind-only nudging is more convenient to apply, and provides higher correlations of the wind fields, geopotential <span class="hlt">height</span> and specific humidity between simulation and reanalysis. This suggests nudging the horizontal winds but not temperature is a good strategy for the investigation of <span class="hlt">aerosol</span> indirect effects through ice clouds, since it provides well-constrained meteorology without strongly perturbing the model's mean climate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....1712097S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....1712097S"><span>Classifying <span class="hlt">aerosol</span> type using in situ surface spectral <span class="hlt">aerosol</span> optical properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmeisser, Lauren; Andrews, Elisabeth; Ogren, John A.; Sheridan, Patrick; Jefferson, Anne; Sharma, Sangeeta; Kim, Jeong Eun; Sherman, James P.; Sorribas, Mar; Kalapov, Ivo; Arsov, Todor; Angelov, Christo; Mayol-Bracero, Olga L.; Labuschagne, Casper; Kim, Sang-Woo; Hoffer, András; Lin, Neng-Huei; Chia, Hao-Ping; Bergin, Michael; Sun, Junying; Liu, Peng; Wu, Hao</p> <p>2017-10-01</p> <p>Knowledge of <span class="hlt">aerosol</span> size and composition is important for determining radiative forcing effects of <span class="hlt">aerosols</span>, identifying <span class="hlt">aerosol</span> sources and improving <span class="hlt">aerosol</span> satellite retrieval algorithms. The ability to extrapolate <span class="hlt">aerosol</span> size and composition, or type, from intensive <span class="hlt">aerosol</span> optical properties can help expand the current knowledge of spatiotemporal variability in <span class="hlt">aerosol</span> type globally, particularly where chemical composition measurements do not exist concurrently with optical property measurements. This study uses medians of the scattering Ångström exponent (SAE), absorption Ångström exponent (AAE) and single scattering albedo (SSA) from 24 stations within the NOAA/ESRL Federated <span class="hlt">Aerosol</span> Monitoring Network to infer <span class="hlt">aerosol</span> type using previously published <span class="hlt">aerosol</span> classification schemes.Three methods are implemented to obtain a best estimate of dominant <span class="hlt">aerosol</span> type at each station using <span class="hlt">aerosol</span> optical properties. The first method plots station medians into an AAE vs. SAE plot space, so that a unique combination of intensive properties corresponds with an <span class="hlt">aerosol</span> type. The second typing method expands on the first by introducing a multivariate cluster analysis, which aims to group stations with similar optical characteristics and thus similar dominant <span class="hlt">aerosol</span> type. The third and final classification method pairs 3-day backward air mass trajectories with median <span class="hlt">aerosol</span> optical properties to explore the relationship between trajectory origin (proxy for likely <span class="hlt">aerosol</span> type) and <span class="hlt">aerosol</span> intensive parameters, while allowing for multiple dominant <span class="hlt">aerosol</span> types at each station.The three <span class="hlt">aerosol</span> classification methods have some common, and thus robust, results. In general, estimating dominant <span class="hlt">aerosol</span> type using optical properties is best suited for site locations with a stable and homogenous <span class="hlt">aerosol</span> population, particularly continental polluted (carbonaceous <span class="hlt">aerosol</span>), marine polluted (carbonaceous <span class="hlt">aerosol</span> mixed with sea salt) and continental dust/biomass sites</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.2511M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.2511M"><span>XBAER-derived <span class="hlt">aerosol</span> optical thickness from OLCI/Sentinel-3 observation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mei, Linlu; Rozanov, Vladimir; Vountas, Marco; Burrows, John P.; Richter, Andreas</p> <p>2018-02-01</p> <p>A cloud identification algorithm used for cloud masking, which is based on the spatial variability of reflectances at the top of the atmosphere in visible wavelengths, has been developed for the retrieval of <span class="hlt">aerosol</span> properties by MODIS. It is shown that the spatial pattern of cloud reflectance, as observed from space, is very different from that of <span class="hlt">aerosols</span>. Clouds show a high spatial variability in the <span class="hlt">scale</span> of a hundred metres to a few kilometres, whereas <span class="hlt">aerosols</span> in general are homogeneous. The concept of spatial variability of reflectances at the top of the atmosphere is mainly applicable over the ocean, where the surface background is sufficiently homogeneous for the separation between <span class="hlt">aerosols</span> and clouds. <span class="hlt">Aerosol</span> retrievals require a sufficiently accurate cloud identification to be able to mask these ground scenes. However, a conservative mask will exclude strong <span class="hlt">aerosol</span> episodes and a less conservative mask could introduce cloud contamination that biases the retrieved <span class="hlt">aerosol</span> optical properties (e.g. <span class="hlt">aerosol</span> optical depth and effective radii). A detailed study on the effect of cloud contamination on <span class="hlt">aerosol</span> retrievals has been performed and parameters are established determining the threshold value for the MODIS <span class="hlt">aerosol</span> cloud mask (3×3-STD) over the ocean. The 3×3-STD algorithm discussed in this paper is the operational cloud mask used for MODIS <span class="hlt">aerosol</span> retrievals over the ocean.A prolonged pollution haze event occurred in the northeast part of China during the period 16-21 December 2016. To assess the impact of such events, the amounts and distribution of <span class="hlt">aerosol</span> particles, formed in such events, need to be quantified. The newly launched Ocean Land Colour Instrument (OLCI) onboard Sentinel-3 is the successor of the MEdium Resolution Imaging Spectrometer (MERIS). It provides measurements of the radiance and reflectance at the top of the atmosphere, which can be used to retrieve the <span class="hlt">aerosol</span> optical thickness (AOT) from synoptic to global <span class="hlt">scales</span>. In this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GPC...124...30E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GPC...124...30E"><span>Impact of tropospheric sulphate <span class="hlt">aerosols</span> on the terrestrial carbon cycle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eliseev, Alexey V.</p> <p>2015-01-01</p> <p>Tropospheric sulphate <span class="hlt">aerosols</span> (TSAs) may oxidise the photosynthesising tissues if they are taken up by plants. A parameterisation of this impact of tropospheric sulphate <span class="hlt">aerosols</span> (TSAs) on the terrestrial gross primary production is suggested. This parameterisation is implemented into the global Earth system model developed at the A.M. Obukhov Institute of the Atmospheric Physics, Russian Academy of Sciences (IAP RAS CM). With this coupled model, the simulations are performed which are forced by common anthropogenic and natural climate forcings based on historical reconstructions followed by the RCP 8.5 scenario. The model response to sulphate <span class="hlt">aerosol</span> loading is subdivided into the climatic (related to the influence of TSA on the radiative transport in the atmosphere) and ecological (related to the toxic influence of sulphate <span class="hlt">aerosol</span> on terrestrial plants) impacts. We found that the former basically dominates over the latter on a global <span class="hlt">scale</span> and modifies the responses of the global vegetation and soil carbon stocks to external forcings by 10%. At a regional <span class="hlt">scale</span>, however, ecological impact may be as much important as the climatic one.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915883L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915883L"><span>Regional <span class="hlt">aerosol</span> emissions and temperature response: Local and remote climate impacts of regional <span class="hlt">aerosol</span> forcing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewinschal, Anna; Ekman, Annica; Hansson, Hans-Christen</p> <p>2017-04-01</p> <p>Emissions of anthropogenic <span class="hlt">aerosols</span> vary substantially over the globe and the short atmospheric residence time of <span class="hlt">aerosols</span> leads to a highly uneven radiative forcing distribution, both spatially and temporally. Regional <span class="hlt">aerosol</span> radiative forcing can, nevertheless, exert a large influence on the temperature field away from the forcing region through changes in heat transport or the atmospheric or ocean circulation. Moreover, the global temperature response distribution to <span class="hlt">aerosol</span> forcing may vary depending on the geographical location of the forcing. In other words, the climate sensitivity in one region can vary depending on the location of the forcing. The surface temperature distribution response to changes in sulphate <span class="hlt">aerosol</span> forcing caused by sulphur dioxide (SO2) emission perturbations in four different regions is investigated using the Norwegian Earth System Model (NorESM). The four regions, Europe, North America, East and South Asia, are all regions with historically high <span class="hlt">aerosol</span> emissions and are relevant from both an air-quality and climate policy perspective. All emission perturbations are defined relative to the year 2000 emissions provided for the Coupled Model Intercomparison Project phase 5. The global mean temperature change per unit SO2 emission change is similar for all four regions for similar magnitudes of emissions changes. However, the global temperature change per unit SO2 emission in simulations where regional SO2 emission were removed is substantially higher than that obtained in simulations where regional SO2 emissions were increased. Thus, the climate sensitivity to regional SO2 emissions perturbations depends on the magnitude of the emission perturbation in NorESM. On regional <span class="hlt">scale</span>, on the other hand, the emission perturbations in different geographical locations lead to different regional temperature responses, both locally and in remote regions. The results from the model simulations are used to construct regional temperature potential</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6019129-height-extrapolation-wind-data','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6019129-height-extrapolation-wind-data"><span><span class="hlt">Height</span> extrapolation of wind data</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>Mikhail, A.S.</p> <p>1982-11-01</p> <p>Hourly average data for a period of 1 year from three tall meteorological towers - the Erie tower in Colorado, the Goodnoe Hills tower in Washington and the WKY-TV tower in Oklahoma - were used to analyze the wind shear exponent variabiilty with various parameters such as thermal stability, anemometer level wind speed, projection <span class="hlt">height</span> and surface roughness. Different proposed models for prediction of <span class="hlt">height</span> variability of short-term average wind speeds were discussed. Other models that predict the <span class="hlt">height</span> dependence of Weilbull distribution parameters were tested. The observed power law exponent for all three towers showed strong dependence on themore » anemometer level wind speed and stability (nighttime and daytime). It also exhibited a high degree of dependence on extrapolation <span class="hlt">height</span> with respect to anemometer <span class="hlt">height</span>. These dependences became less severe as the anemometer level wind speeds were increased due to the turbulent mixing of the atmospheric boundary layer. The three models used for Weibull distribution parameter extrapolation were he velocity-dependent power law model (Justus), the velocity, surface roughness, and <span class="hlt">height</span>-dependent model (Mikhail) and the velocity and surface roughness-dependent model (NASA). The models projected the <span class="hlt">scale</span> parameter C fairly accurately for the Goodnoe Hills and WKY-TV towers and were less accurate for the Erie tower. However, all models overestimated the C value. The maximum error for the Mikhail model was less than 2% for Goodnoe Hills, 6% for WKY-TV and 28% for Erie. The error associated with the prediction of the shape factor (K) was similar for the NASA, Mikhail and Justus models. It ranged from 20 to 25%. The effect of the misestimation of hub-<span class="hlt">height</span> distribution parameters (C and K) on average power output is briefly discussed.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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/2012ESASP.703E..23K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ESASP.703E..23K"><span>Sea-Salt <span class="hlt">Aerosol</span> Forecasts Compared with Wave and Sea-Salt Measurements in the Open 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>Kishcha, P.; Starobinets, B.; Bozzano, R.; Pensieri, S.; Canepa, E.; Nickovie, S.; di Sarra, A.; Udisti, R.; Becagli, S.; Alpert, P.</p> <p>2012-03-01</p> <p>Sea-salt <span class="hlt">aerosol</span> (SSA) could influence the Earth's climate acting as cloud condensation nuclei. However, there were no regular measurements of SSA in the open sea. At Tel-Aviv University, the DREAM-Salt prediction system has been producing daily forecasts of 3-D distribution of sea-salt <span class="hlt">aerosol</span> concentrations over the Mediterranean Sea (http://wind.tau.ac.il/saltina/ salt.html). In order to evaluate the model performance in the open sea, daily modeled concentrations were compared directly with SSA measurements taken at the tiny island of Lampedusa, in the Central Mediterranean. In order to further test the robustness of the model, the model performance over the open sea was indirectly verified by comparing modeled SSA concentrations with wave <span class="hlt">height</span> measurements collected by the ODAS Italia 1 buoy and the Llobregat buoy. Model-vs.-measurement comparisons show that the model is capable of producing realistic SSA concentrations and their day-today variations over the open sea, in accordance with observed wave <span class="hlt">height</span> and wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1410831B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1410831B"><span>Seasonal <span class="hlt">aerosol</span> characteristics in the Amazon rain forest</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baars, H.; Althausen, D.; Ansmann, A.; Engelmann, R.; Heese, B.; Müller, D.; Pauliquevis, T.; Souza, R.; Artaxo, P.</p> <p>2012-04-01</p> <p>For the first time in Amazonia, continuous measurements of the vertical <span class="hlt">aerosol</span> structure were carried out in the framework of EUCAARI (European Integrated Project on <span class="hlt">Aerosol</span>, Cloud, Climate, Air Quality Interactions) and AMAZE-08 (Amazonian <span class="hlt">Aerosol</span> Characterization Experiment). The observations were performed 60 km north of Manaus, Brazil (at 2° 35.5' S and 60° 2.3' W) in the central northern part of the Amazon rain forest from January to November 2008 with the automated multi-wavelength-Raman-polarization-lidar PollyXT. With this instrument, vertical profiles of the particle backscatter coefficient at 355, 532, and 1064 nm, of the particle extinction coefficient at 355 and 532 nm, and of the particle linear depolarization ratio at 355 nm can be determined. During the 10-months observational period, measurements were performed on 211 days resulting in more than 2500 hours of tropospheric <span class="hlt">aerosol</span> and cloud profile observations. The analysis of the long-term data set revealed strong differences in the <span class="hlt">aerosol</span> characteristics between the wet and the dry season. In the wet season, very clean atmospheric conditions occurred in ca. 50% of all observation cases. During these clean conditions, the <span class="hlt">aerosol</span> optical depth (AOD) at 532 nm was less than 0.05 and the <span class="hlt">aerosol</span> was trapped in the lowermost 2 km of the troposphere. However, also intrusions of Saharan dust and African biomass-burning <span class="hlt">aerosol</span> (BBA) - characterized by a significantly increased AOD and particle depolarization ratio - were observed in about one third (32%) of all lidar observations. These African <span class="hlt">aerosol</span> plumes extended usually from the surface up to about 3.5 km agl. During the dry season, BBA from fires on the South American continent was the dominant <span class="hlt">aerosol</span> species. The mean AOD of the dry season was found to be a factor of 3 higher than the mean AOD of the wet season (0.26 compared to 0.08 at 532 nm). This is due to the high BBA concentration in the atmosphere. Maximum AOD values were less than 0</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.7049A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.7049A"><span>Laboratory studies of <span class="hlt">aerosol</span> electrification and experimental evidence for electrical breakdown at different <span class="hlt">scales</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alois, Stefano; Merrison, Jonathan; Iversen, Jens Jacob; Sesterhenn, Joern</p> <p>2017-04-01</p> <p>Contact electrification between different particles size/material can lead to electric field generation high enough to produce electrical breakdown. Experimental studies of solid <span class="hlt">aerosol</span> contact electrification (Alois et al., 2016) has shown various electrical breakdown phenomena; these range from field emission at the contact site (nm-<span class="hlt">scale</span>) limiting particle surface charge concentration, to visible electrical discharges (cm-<span class="hlt">scale</span>) observed both with the use of an electrometer and high-speed camera. In these experiments micron-size particles are injected into a low-pressure chamber, where they are deviated by an applied electric field. A laser Doppler velocimeter allows the simultaneous determination of particle size and charge of single grains. Results have shown an almost constant surface charge concentration, which is likely to be due to charge limitation by field emission at the contact site between particle and injector. In a second measurement technique, the electrically isolated injector tube (i.e. a Faraday cage) is connected to an oscilloscope and synchronised to a high speed camera filming the injection. Here the electrification of a large cloud of particles can be quantified and discharging effects studied. This study advances our understanding on the physical processes leading to electrification and electrical breakdown mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912358W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912358W"><span>Optical and microphysical properties of <span class="hlt">aerosol</span> vertical distribution over Vipava valley retrieved by ground-based elastic lidar and in-situ measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Longlong; Gregorič, Asta; Stanič, Samo; Mole, Maruška; Bergant, Klemen; Močnik, Griša; Drinovec, Luka; Vaupotič, Janja; Miler, Miloš; Gosar, Mateja</p> <p>2017-04-01</p> <p>Atmospheric <span class="hlt">aerosols</span> influence Earth's radiation budget, visibility and air quality, as well as the cloud formation processes and precipitation. The structure of the vertical <span class="hlt">aerosol</span> distribution, in particular that of black carbon, significantly influences the <span class="hlt">aerosol</span> direct radiative effect, followed by feedbacks on cloud and planetary boundary layer dynamics. The knowledge on <span class="hlt">aerosol</span> vertical distribution and properties therefore provides an important insight into many atmospheric processes. In order to retrieve the vertical distribution of <span class="hlt">aerosol</span> properties in the Vipava valley (Slovenia) and the influence of planetary boundary layer <span class="hlt">height</span> on the local air quality, in-situ and LIDAR measurements were performed. In-situ methods consisted of <span class="hlt">aerosol</span> size distribution and number concentration and black carbon concentration measurements which were performed during a one-month extensive measurement campaign in spring 2016. <span class="hlt">Aerosol</span> size distribution (10 nm to 30 µm) was measured at the valley floor using scanning mobility particle sizer (SMPS, Grimm <span class="hlt">Aerosol</span> Technique, Germany) and optical particle counter (OPC, Grimm <span class="hlt">Aerosol</span> Technique, Germany). Black carbon concentrations were measured by Aethalometer AE33 (<span class="hlt">Aerosol</span> d.o.o., Slovenia) at the valley floor (125 m a.s.l.) and at the top of the adjacent mountain ridge (951 m a.s.l.), the later representing regional background conditions. The in-situ measurements were combined with LIDAR remote sensing, where the vertical profiles of <span class="hlt">aerosol</span> backscattering coefficients were retrieved using the Klett method. In addition, <span class="hlt">aerosol</span> samples were analyzed by SEM-EDX to obtain <span class="hlt">aerosol</span> morphology and chemical composition. Two different cases with expected dominant presence of specific <span class="hlt">aerosol</span> types were investigated in more detail. They show significantly different <span class="hlt">aerosol</span> properties and distributions within the valley, which has an important implication for the direct radiative effect. In the first case, during a Saharan dust</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFM.A72E..10T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFM.A72E..10T"><span>Distribution and radiative forcing of Asian dust and anthropogenic <span class="hlt">aerosols</span> from East Asia simulated by SPRINTARS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takemura, T.; Nakajima, T.; Uno, I.</p> <p>2002-12-01</p> <p>A three-dimensional <span class="hlt">aerosol</span> transport-radiation model, SPRINTARS (Spectral Radiation-Transport Model for <span class="hlt">Aerosol</span> Species), has been developed based on an atmospheric general circulation model of the Center for Climate System Research, University of Tokyo/National Institute for Environmental Studies, Japan to research the effects of <span class="hlt">aerosols</span> on the climate system and atmospheric environment. SPRINTARS successfully simulates the long-range transport of the large-<span class="hlt">scale</span> Asian dust storms from East Asia to North America by crossing the North Pacific Ocean in springtime 2001 and 2002. It is found from the calculated dust optical thickness that 10 to 20% of Asian dust around Japan reached North America. The simulation also reveals the importance of anthropogenic <span class="hlt">aerosols</span>, which are carbonaceous and sulfate <span class="hlt">aerosols</span> emitted from the industrialized areas in the East Asian continent, to air turbidity during the large-<span class="hlt">scale</span> Asian dust storms. The simulated results are compared with a volume of observation data regarding the <span class="hlt">aerosol</span> characteristics over East Asia in the spring of 2001 acquired by the intensive observation campaigns of ACE-Asia (Asian Pacific Regional <span class="hlt">Aerosol</span> Characterization Experiment) and APEX (Asian Atmospheric Particulate Environmental Change Studies). The comparisons are carried out not only for <span class="hlt">aerosol</span> concentrations but also for <span class="hlt">aerosol</span> optical properties, such as optical thickness, Angstrom exponent which is a size index calculated by the log-slope exponent of the optical thickness between two wavelengths, and single scattering albedo. The consistence of Angstrom exponent between the simulation and observations means the reasonable simulation of the ratio of anthropogenic <span class="hlt">aerosols</span> to Asian dust, which supports the suggestion by the simulation on the importance of anthropogenic <span class="hlt">aerosols</span> to air turbidity during the large-<span class="hlt">scale</span> Asian dust storms. SPRINTARS simultaneously calculates the <span class="hlt">aerosol</span> direct and indirect radiative forcings. The direct radiative</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ACP....14.8631Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ACP....14.8631Z"><span>Technical Note: On the use of nudging for <span class="hlt">aerosol</span>-climate model intercomparison studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, K.; Wan, H.; Liu, X.; Ghan, S. J.; Kooperman, G. J.; Ma, P.-L.; Rasch, P. J.; Neubauer, D.; Lohmann, U.</p> <p>2014-08-01</p> <p>Nudging as an assimilation technique has seen increased use in recent years in the development and evaluation of climate models. Constraining the simulated wind and temperature fields using global weather reanalysis facilitates more straightforward comparison between simulation and observation, and reduces uncertainties associated with natural variabilities of the large-<span class="hlt">scale</span> circulation. On the other hand, the forcing introduced by nudging can be strong enough to change the basic characteristics of the model climate. In the paper we show that for the Community Atmosphere Model version 5 (CAM5), due to the systematic temperature bias in the standard model and the sensitivity of simulated ice formation to anthropogenic <span class="hlt">aerosol</span> concentration, nudging towards reanalysis results in substantial reductions in the ice cloud amount and the impact of anthropogenic <span class="hlt">aerosols</span> on long-wave cloud forcing. In order to reduce discrepancies between the nudged and unconstrained simulations, and meanwhile take the advantages of nudging, two alternative experimentation methods are evaluated. The first one constrains only the horizontal winds. The second method nudges both winds and temperature, but replaces the long-term climatology of the reanalysis by that of the model. Results show that both methods lead to substantially improved agreement with the free-running model in terms of the top-of-atmosphere radiation budget and cloud ice amount. The wind-only nudging is more convenient to apply, and provides higher correlations of the wind fields, geopotential <span class="hlt">height</span> and specific humidity between simulation and reanalysis. Results from both CAM5 and a second <span class="hlt">aerosol</span>-climate model ECHAM6-HAM2 also indicate that compared to the wind-and-temperature nudging, constraining only winds leads to better agreement with the free-running model in terms of the estimated shortwave cloud forcing and the simulated convective activities. This suggests nudging the horizontal winds but not temperature is a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.1001L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.1001L"><span>Fast Adjustments of the Asian Summer Monsoon to Anthropogenic <span class="hlt">Aerosols</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, Xiaoqiong; Ting, Mingfang; Lee, Dong Eun</p> <p>2018-01-01</p> <p>Anthropogenic <span class="hlt">aerosols</span> are a major factor contributing to human-induced climate change, particularly over the densely populated Asian monsoon region. Understanding the physical processes controlling the <span class="hlt">aerosol</span>-induced changes in monsoon rainfall is essential for reducing the uncertainties in the future projections of the hydrological cycle. Here we use multiple coupled and atmospheric general circulation models to explore the physical mechanisms for the <span class="hlt">aerosol</span>-driven monsoon changes on different time <span class="hlt">scales</span>. We show that anthropogenic <span class="hlt">aerosols</span> induce an overall reduction in monsoon rainfall and circulation, which can be largely explained by the fast adjustments over land north of 20∘N. This fast response occurs before changes in sea surface temperature (SST), largely driven by <span class="hlt">aerosol</span>-cloud interactions. However, <span class="hlt">aerosol</span>-induced SST feedbacks (slow response) cause substantial changes in the monsoon meridional circulation over the oceanic regions. Both the land-ocean asymmetry and meridional temperature gradient are key factors in determining the overall monsoon circulation response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28667308','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28667308"><span>Enhanced PM2.5 pollution in China due to <span class="hlt">aerosol</span>-cloud interactions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhao, Bin; Liou, Kuo-Nan; Gu, Yu; Li, Qinbin; Jiang, Jonathan H; Su, Hui; He, Cenlin; Tseng, Hsien-Liang R; Wang, Shuxiao; Liu, Run; Qi, Ling; Lee, Wei-Liang; Hao, Jiming</p> <p>2017-06-30</p> <p><span class="hlt">Aerosol</span>-cloud interactions (<span class="hlt">aerosol</span> indirect effects) play an important role in regional meteorological variations, which could further induce feedback on regional air quality. While the impact of <span class="hlt">aerosol</span>-cloud interactions on meteorology and climate has been extensively studied, their feedback on air quality remains unclear. Using a fully coupled meteorology-chemistry model, we find that increased <span class="hlt">aerosol</span> loading due to anthropogenic activities in China substantially increases column cloud droplet number concentration and liquid water path (LWP), which further leads to a reduction in the downward shortwave radiation at surface, surface air temperature and planetary boundary layer (PBL) <span class="hlt">height</span>. The shallower PBL and accelerated cloud chemistry due to larger LWP in turn enhance the concentrations of particulate matter with diameter less than 2.5 μm (PM 2.5 ) by up to 33.2 μg m -3 (25.1%) and 11.0 μg m -3 (12.5%) in January and July, respectively. Such a positive feedback amplifies the changes in PM 2.5 concentrations, indicating an additional air quality benefit under effective pollution control policies but a penalty for a region with a deterioration in PM 2.5 pollution. Additionally, we show that the cloud processing of <span class="hlt">aerosols</span>, including wet scavenging and cloud chemistry, could also have substantial effects on PM 2.5 concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1040324-vertical-distribution-aerosols-vicinity-mexico-city-during-milagro-campaign','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1040324-vertical-distribution-aerosols-vicinity-mexico-city-during-milagro-campaign"><span>Vertical distribution of <span class="hlt">aerosols</span> in the vicinity of Mexico City during MILAGRO-2006 Campaign</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>Lewandowski, P.A.; Kleinman, L.; Eichinger, W. E.</p> <p></p> <p>On 7 March 2006, a mobile, ground-based, vertical pointing, elastic lidar system made a North-South transect through the Mexico City basin. Column averaged, <span class="hlt">aerosol</span> size distribution (ASD) measurements were made on the ground concurrently with the lidar measurements. The ASD ground measurements allowed calculation of the column averaged mass extinction efficiency (MEE) for the lidar system (1064 nm). The value of column averaged MEE was combined with spatially resolved lidar extinction coefficients to produce total <span class="hlt">aerosol</span> mass concentration estimates with the resolution of the lidar (1.5 m vertical spatial and 1 s temporal). Airborne ASD measurements from DOE G-1 aircraftmore » made later in the day on 7 March 2006, allowed the evaluation of the assumptions of constant ASD with <span class="hlt">height</span> and time used for estimating the column averaged MEE. The results showed that the <span class="hlt">aerosol</span> loading within the basin is about twice what is observed outside of the basin. The total <span class="hlt">aerosol</span> base concentrations observed in the basin are of the order of 200 {mu}g/m{sup 3} and the base levels outside are of the order of 100 {mu}g/m{sup 3}. The local heavy traffic events can introduce <span class="hlt">aerosol</span> levels near the ground as high as 900 {mu}g/m{sup 3}. The article presents the methodology for estimating <span class="hlt">aerosol</span> mass concentration from mobile, ground-based lidar measurements in combination with <span class="hlt">aerosol</span> size distribution measurements. An uncertainty analysis of the methodology is also presented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813677F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813677F"><span>Response of different regional online coupled models to <span class="hlt">aerosol</span>-radiation interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Forkel, Renate; Balzarini, Alessandra; Brunner, Dominik; Baró, Rocio; Curci, Gabriele; Hirtl, Marcus; Honzak, Luka; Jiménez-Guerrero, Pedro; Jorba, Oriol; Pérez, Juan L.; Pirovano, Guido; San José, Roberto; Schröder, Wolfram; Tuccella, Paolo; Werhahn, Johannes; Wolke, Ralf; Žabkar, Rahela</p> <p>2016-04-01</p> <p> the inclusion of <span class="hlt">aerosol</span> radiative effects improves simulated temperatures in this area. In summary, the direct <span class="hlt">aerosol</span> effect leads to lower temperatures and PBL <span class="hlt">heights</span> for all seasons whereas the impact of the <span class="hlt">aerosol</span> indirect effect on temperature and pollutant concentrations over Northern Europe was found to depend strongly on the season. It cannot be generalized whether the inclusion of <span class="hlt">aerosol</span> radiative effects and <span class="hlt">aerosol</span> cloud interactions based on simulated <span class="hlt">aerosol</span> concentrations does improve the simulation results. Furthermore, assumptions how <span class="hlt">aerosol</span> optical properties are calculated, i.e. on the <span class="hlt">aerosol</span>'s mixing state have a strong effect on simulated <span class="hlt">aerosol</span> optical depth and the <span class="hlt">aerosol</span> effect on incoming solar radiation and temperature. The inter-model variation of the response of different online coupled models suggests that further work comparing the methodologies and parameterizations used to represent the direct and indirect <span class="hlt">aerosol</span> effect in these models is still necessary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRD..123.1179Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRD..123.1179Z"><span>Enhancement of PM2.5 Concentrations by <span class="hlt">Aerosol</span>-Meteorology Interactions 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>Zhang, Xin; Zhang, Qiang; Hong, Chaopeng; Zheng, Yixuan; Geng, Guannan; Tong, Dan; Zhang, Yuxuan; Zhang, Xiaoye</p> <p>2018-01-01</p> <p><span class="hlt">Aerosol</span>-meteorology interactions can change surface <span class="hlt">aerosol</span> concentrations via different mechanisms such as altering radiation budget or cloud microphysics. However, few studies investigated the impacts of different mechanisms on temporal and spatial distribution of PM2.5 concentrations over China. Here we used the fully coupled Weather Research and Forecasting model with online chemistry (WRF-Chem) to quantify the enhancement of PM2.5 concentrations by <span class="hlt">aerosol</span>-meteorology feedback in China in 2014 for different seasons and separate the relative impacts of <span class="hlt">aerosol</span> radiation interactions (ARIs) and <span class="hlt">aerosol</span>-cloud interactions (ACIs). We found that ARIs and ACIs could increase population-weighted annual mean PM2.5 concentration over China by 4.0 μg/m3 and 1.6 μg/m3, respectively. We found that ARIs play a dominant role in <span class="hlt">aerosol</span>-meteorology interactions in winter, while the enhancement of PM2.5 concentration by ARIs and ACIs is comparable in other three seasons. ARIs reduced the wintertime monthly mean wind speed and planetary boundary layer (PBL) <span class="hlt">height</span> by up to 0.1 m/s and 160 m, respectively, but increased the relative humidity by up to 4%, leading to accumulation of pollutants within PBL. Also, ARIs reduced dry deposition velocity of <span class="hlt">aerosols</span> by up to 20%, resulting in an increase in PM2.5 lifetime and concentrations. ARIs can increase wintertime monthly mean surface PM2.5 concentration by a maximum of 30 μg/m3 in Sichuan Basin. ACIs can also increase PM2.5 concentration with more significant impacts in wet seasons via reduced wet scavenging and enhanced in-cloud chemistry. Dominant processes in PM2.5 enhancement are also clarified in different seasons. Results show that physical process is more important than chemical processes in winter in ARIs, while chemical process of secondary inorganic <span class="hlt">aerosols</span> production may be crucial in wet seasons via ACIs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.5289A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.5289A"><span><span class="hlt">Aerosol</span> and Cloud Microphysical Properties in the Asir region of Saudi Arabia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Axisa, Duncan; Kucera, Paul; Burger, Roelof; Li, Runjun; Collins, Don; Freney, Evelyn; Posada, Rafael; Buseck, Peter</p> <p>2010-05-01</p> <p>In recent advertent and inadvertent weather modification studies, a considerable effort has been made to understand the impact of varying <span class="hlt">aerosol</span> properties and concentration on cloud properties. Significant uncertainties exist with <span class="hlt">aerosol</span>-cloud interactions for which complex microphysical processes link the <span class="hlt">aerosol</span> and cloud properties. Under almost all environmental conditions, increased <span class="hlt">aerosol</span> concentrations within polluted air masses will enhance cloud droplet concentration relative to that in unperturbed regions. The interaction between dust particles and clouds are significant, yet the conditions in which dust particles become cloud condensation nuclei (CCN) are uncertain. In order to quantify this <span class="hlt">aerosol</span> effect on clouds and precipitation, a field campaign was launched in the Asir region of Saudi Arabia as part of a Precipitation Enhancement Feasibility Study. Ground measurements of <span class="hlt">aerosol</span> size distributions, hygroscopic growth factor, CCN concentrations as well as aircraft measurements of cloud hydrometeor size distributions were done in the Asir region of Saudi Arabia in August 2009. Research aircraft operations focused primarily on conducting measurements in clouds that are targeted for cloud top-seeding, on their microphysical characterization, especially the preconditions necessary for precipitation; understanding the evolution of droplet coalescence, supercooled liquid water, cloud ice and precipitation hydrometeors is necessary if advances are to be made in the study of cloud modification by cloud seeding. Non-precipitating mixed-phase clouds less than 3km in diameter that developed on top of the stable inversion were characterized by flying at the convective cloud top just above the inversion. <span class="hlt">Aerosol</span> measurements were also done during the climb to cloud base <span class="hlt">height</span>. The presentation will include a summary of the analysis and results with a focus on the unique features of the Asir region in producing convective clouds, characterization of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998LNES...72..247A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998LNES...72..247A"><span>Long term atmospheric <span class="hlt">aerosol</span> characterization in the Amazon Basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Artaxo, Paulo; Gerab, Fábio; Yamasoe, Marcia A.</p> <p></p> <p>This chapter presents a characterization of atmospheric <span class="hlt">aerosols</span> collected in different places in the Amazon Basin. Both the biogenic <span class="hlt">aerosol</span> emission from the forest and the particulate material which is emitted to the atmosphere due to the large <span class="hlt">scale</span> man-made burns during the dry season were studied. The samples were collected during a three year period at three different locations in the Amazon (Cuiabá, Alta Floresta and Serra do Navio), using stacked filter units. <span class="hlt">Aerosol</span> samples were also collected directly over fires of cerrado vegetation and tropical primary forest burns The samples were analyzed using several techniques for a number of elements. Gravimetric analyses were used to determine the total atmospheric <span class="hlt">aerosol</span> concentration. Multivariate statistical analysis was used in order to identify and characterize the sources of the atmospheric <span class="hlt">aerosol</span> present in the sampled regions. Cerrado burning emissions were enriched compared to forest ones, specially for Cl, K and Zn. High atmospheric <span class="hlt">aerosol</span> concentrations were observed in large amazonian areas due to emissions from man-made burns in the period from June to September. The emissions from burns dominate the fine fraction of the atmospheric <span class="hlt">aerosol</span> with characteristic high contents of black carbon, S and K. <span class="hlt">Aerosols</span> emitted in biomass burning process are correlated to the increase in the <span class="hlt">aerosol</span> optical thickness of the atmosphere during the Amazonian dry season. The Serra do Navio <span class="hlt">aerosol</span> is characterized by biogenic emissions with strong marine influence. The presence of trace elements characteristic of soil particulate associated with this marine contribution indicates the existence of <span class="hlt">aerosol</span> transport from Africa to South America. Similar composition characteristics were observed in the biogenic emission <span class="hlt">aerosols</span> from Serra do Navio and Alta Floresta.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008058','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008058"><span><span class="hlt">Aerosol</span> Observability and Predictability: From Research to Operations for Chemical Weather Forecasting. Lagrangian Displacement Ensembles for <span class="hlt">Aerosol</span> Data Assimilation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>da Silva, Arlindo</p> <p>2010-01-01</p> <p>A challenge common to many constituent data assimilation applications is the fact that one observes a much smaller fraction of the phase space that one wishes to estimate. For example, remotely sensed estimates of the column average concentrations are available, while one is faced with the problem of estimating 3D concentrations for initializing a prognostic model. This problem is exacerbated in the case of <span class="hlt">aerosols</span> because the observable <span class="hlt">Aerosol</span> Optical Depth (AOD) is not only a column integrated quantity, but it also sums over a large number of species (dust, sea-salt, carbonaceous and sulfate <span class="hlt">aerosols</span>. An <span class="hlt">aerosol</span> transport model when driven by high-resolution, state-of-the-art analysis of meteorological fields and realistic emissions can produce skillful forecasts even when no <span class="hlt">aerosol</span> data is assimilated. The main task of <span class="hlt">aerosol</span> data assimilation is to address the bias arising from inaccurate emissions, and Lagrangian misplacement of plumes induced by errors in the driving meteorological fields. As long as one decouples the meteorological and <span class="hlt">aerosol</span> assimilation as we do here, the classic baroclinic growth of error is no longer the main order of business. We will describe an <span class="hlt">aerosol</span> data assimilation scheme in which the analysis update step is conducted in observation space, using an adaptive maximum-likelihood scheme for estimating background errors in AOD space. This scheme includes e explicit sequential bias estimation as in Dee and da Silva. Unlikely existing <span class="hlt">aerosol</span> data assimilation schemes we do not obtain analysis increments of the 3D concentrations by <span class="hlt">scaling</span> the background profiles. Instead we explore the Lagrangian characteristics of the problem for generating local displacement ensembles. These high-resolution state-dependent ensembles are then used to parameterize the background errors and generate 3D <span class="hlt">aerosol</span> increments. The algorithm has computational complexity running at a resolution of 1/4 degree, globally. We will present the result of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5977R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5977R"><span>Surface <span class="hlt">aerosol</span> and rehabilitation properties of ground-level atmosphere in the mountains of the North Caucasus</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reps, Valentina; Efimenko, Natalia; Povolotskaya, Nina; Abramtsova, Anna; Ischenko, Dmitriy; Senik, Irina; Slepikh, Victor</p> <p>2017-04-01</p> <p>The rehabilitative properties (RP) of ground-level atmosphere (GA) of Russian resorts are considered as natural healing resources and received state legal protection [1]. Due to global urbanization the chemical composition and particle size distribution of the surface <span class="hlt">aerosol</span> are changing rapidly. However, the influence of surface <span class="hlt">aerosol</span> on the RP of GA has been insufficiently studied. At the resort region of the North Caucasus complex monitoring (<span class="hlt">aerosol</span>, trace gases NOx, CO, O3, CH4; periodically - heavy metals) is performed at two high levels (860 masl - a park zone of a large mountain resort, 2070 masl - alpine grassland, the net station). The results of the measurements are used in programs of bioclimatic, landscape and medical monitoring to specify the influence of <span class="hlt">aerosol</span> on rehabilitation properties of the environment and human adaptative reserves. The <span class="hlt">aerosol</span> particles of size range 500-1000 nm are used as a marker of the pathogenic effect of <span class="hlt">aerosol</span> [2]. In the conditions of regional urbanization and complicated mountain atmospheric circulation the influence of <span class="hlt">aerosol</span> on RP of GA and the variability of heart rhythm with the volunteers at different <span class="hlt">heights</span> were investigated. At the <span class="hlt">height</span> of 860 masl (urbanized resort) there have been noticed <span class="hlt">aerosol</span> variations in the range of 0,04-0,35 particles/cm3 (slightly <span class="hlt">aerosol</span> polluted), in mountain conditions - background pollution <span class="hlt">aerosol</span> level. The difference of bioclimatic conditions at the specified high-rise levels has been referred to the category of contrasts. The natural aero ionization ∑(N+)+(N-) varied from 960 ion/cm3 to 1460 ion/cm3 in the resort park (860 m); from 1295 ion/cm3 to 4850 ion/cm3 on the Alpine meadow (2070 m); from 1128 ion/cm3 to 3420 ion/cm3 - on the tested site near the edge of the pinewood (1720 m). In the group of volunteers the trip from low-hill terrain zone (860 m) to the lower zone of highlands (2070 m) caused the activation of neuro and humoral regulation, vegetative and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120011727','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120011727"><span>Impact of <span class="hlt">Aerosols</span> on Convective Clouds and Precipitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tao, Wei-Kuo; Chen, Jen-Ping; Li, Zhanqing; Wang, Chien; Zhang, Chidong</p> <p>2012-01-01</p> <p><span class="hlt">Aerosols</span> are a critical factor in the atmospheric hydrological cycle and radiation budget. As a major agent for clouds to form and a significant attenuator of solar radiation, <span class="hlt">aerosols</span> affect climate in several ways. Current research suggests that <span class="hlt">aerosol</span> effects on clouds could further extend to precipitation, both through the formation of cloud particles and by exerting persistent radiative forcing on the climate system that disturbs dynamics. However, the various mechanisms behind these effects, in particular the ones connected to precipitation, are not yet well understood. The atmospheric and climate communities have long been working to gain a better grasp of these critical effects and hence to reduce the significant uncertainties in climate prediction resulting from such a lack of adequate knowledge. Here we review past efforts and summarize our current understanding of the effect of <span class="hlt">aerosols</span> on convective precipitation processes from theoretical analysis of microphysics, observational evidence, and a range of numerical model simulations. In addition, the discrepancy between results simulated by models, as well as that between simulations and observations, are presented. Specifically, this paper addresses the following topics: (1) fundamental theories of <span class="hlt">aerosol</span> effects on microphysics and precipitation processes, (2) observational evidence of the effect of <span class="hlt">aerosols</span> on precipitation processes, (3) signatures of the <span class="hlt">aerosol</span> impact on precipitation from largescale analyses, (4) results from cloud-resolving model simulations, and (5) results from large-<span class="hlt">scale</span> numerical model simulations. Finally, several future research directions for gaining a better understanding of <span class="hlt">aerosol</span>--cloud-precipitation interactions are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120009164','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009164"><span>An Overview of the GEOS-5 <span class="hlt">Aerosol</span> Reanalysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>da Silva, Arlindo; Colarco, Peter Richard; Damenov, Anton Spasov; Buchard-Marchant, Virginie; Randles, Cynthia A.; Gupta, Pawan</p> <p>2011-01-01</p> <p>GEOS-5 is the latest version of the NASA Global Modeling and Assimilation Office (GMAO) earth system model. GEOS-5 contains components for atmospheric circulation and composition (including data assimilation), ocean circulation and biogeochemistry, and land surface processes. In addition to traditional meteorological parameters, GEOS-5 includes modules representing the atmospheric composition, most notably <span class="hlt">aerosols</span> and tropospheric/stratospheric chemical constituents, taking explicit account of the impact of these constituents on the radiative processes of the atmosphere. MERRA is a NASA meteorological reanalysis for the satellite era (1979-present) using GEOS-5. This project focuses on historical analyses of the hydrological cycle on a broad range of weather and climate time <span class="hlt">scales</span>. As a first step towards an integrated Earth System Analysis (IESA), the GMAO is extending MERRA with reanalyses for other components of the earth system: land, ocean, bio-geochemistry and atmospheric constituents. In this talk we will present results from the MERRA-driven <span class="hlt">aerosol</span> reanalysis covering the Aqua period (2003-present). The assimilation of <span class="hlt">Aerosol</span> Optical Depth (AOD) in GEOS-5 involves very careful cloud screening and homogenization of the observing system by means of a Neural Net scheme that translates MODIS radiances into AERONET calibrated AOD. These measurements are further quality controlled using an adaptive buddy check scheme, and assimilated using the Local Displacement Ensemble (LDE) methodology. For this reanalysis, GEOS-5 runs at a nominal 50km horizontal resolution with 72 vertical layers (top at approx. 8Skm). GEOS-5 is driven by daily biomass burning emissions derived from MODIS fire radiative power retrievals. We will present a summary of our efforts to validate such dataset. The GEOS-5 assimilated <span class="hlt">aerosol</span> fields are first validated by comparison to independent in-situ measurements (AERONET and PM2.5 surface concentrations). In order to asses <span class="hlt">aerosol</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JGRD..114.0G13M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JGRD..114.0G13M"><span>Spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing in summer 2006: Model evaluation and source apportionment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsui, H.; Koike, M.; Kondo, Y.; Takegawa, N.; Kita, K.; Miyazaki, Y.; Hu, M.; Chang, S.-Y.; Blake, D. R.; Fast, J. D.; Zaveri, R. A.; Streets, D. G.; Zhang, Q.; Zhu, T.</p> <p>2009-01-01</p> <p>Regional <span class="hlt">aerosol</span> model calculations were made using the Weather Research and Forecasting (WRF)-Community Multiscale Air Quality (CMAQ) and WRF-chem models to study spatial and temporal variations of <span class="hlt">aerosols</span> around Beijing, China, in the summer of 2006, when the Campaigns of Air Quality Research in Beijing and Surrounding Region 2006 (CAREBeijing) intensive campaign was conducted. Model calculations captured temporal variations of primary (such as elemental carbon (EC)) and secondary (such as sulfate) <span class="hlt">aerosols</span> observed in and around Beijing. The spatial distributions of <span class="hlt">aerosol</span> optical depth observed by the MODIS satellite sensors were also reproduced over northeast China. Model calculations showed distinct differences in spatial distributions between primary and secondary <span class="hlt">aerosols</span> in association with synoptic-<span class="hlt">scale</span> meteorology. Secondary <span class="hlt">aerosols</span> increased in air around Beijing on a <span class="hlt">scale</span> of about 1000 × 1000 km2 under an anticyclonic pressure system. This air mass was transported northward from the high anthropogenic emission area extending south of Beijing with continuous photochemical production. Subsequent cold front passage brought clean air from the north, and polluted air around Beijing was swept to the south of Beijing. This cycle was repeated about once a week and was found to be responsible for observed enhancements/reductions of <span class="hlt">aerosols</span> at the intensive measurement sites. In contrast to secondary <span class="hlt">aerosols</span>, the spatial distributions of primary <span class="hlt">aerosols</span> (EC) reflected those of emissions, resulting in only slight variability despite the changes in synoptic-<span class="hlt">scale</span> meteorology. In accordance with these results, source apportionment simulations revealed that primary <span class="hlt">aerosols</span> around Beijing were controlled by emissions within 100 km around Beijing within the preceding 24 h, while emissions as far as 500 km and within the preceding 3 days were found to affect secondary <span class="hlt">aerosols</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A53E3269A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A53E3269A"><span>Spatial Variability of CCN Sized <span class="hlt">Aerosol</span> Particles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asmi, A.; Väänänen, R.</p> <p>2014-12-01</p> <p>The computational limitations restrict the grid size used in GCM models, and for many cloud types they are too large when compared to the <span class="hlt">scale</span> of the cloud formation processes. Several parameterizations for e.g. convective cloud formation exist, but information on spatial subgrid variation of the cloud condensation nuclei (CCNs) sized <span class="hlt">aerosol</span> concentration is not known. We quantify this variation as a function of the spatial <span class="hlt">scale</span> by using datasets from airborne <span class="hlt">aerosol</span> measurement campaigns around the world including EUCAARI LONGREX, ATAR, INCA, INDOEX, CLAIRE, PEGASOS and several regional airborne campaigns in Finland. The typical shapes of the distributions are analyzed. When possible, we use information obtained by CCN counters. In some other cases, we use particle size distribution measured by for example SMPS to get approximated CCN concentration. Other instruments used include optical particle counters or condensational particle counters. When using the GCM models, the CCN concentration used for each the grid-box is often considered to be either flat, or as an arithmetic mean of the concentration inside the grid-box. However, the aircraft data shows that the concentration values are often lognormal distributed. This, combined with the subgrid variations in the land use and atmospheric properties, might cause that the <span class="hlt">aerosol</span>-cloud interactions calculated by using mean values to vary significantly from the true effects both temporary and spatially. This, in turn, can cause non-linear bias into the GCMs. We calculate the CCN <span class="hlt">aerosol</span> concentration distribution as a function of different spatial <span class="hlt">scales</span>. The measurements allow us to study the variation of these distributions within from hundreds of meters up to hundreds of kilometers. This is used to quantify the potential error when mean values are used in GCMs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=312470&keyword=cmaq&acttype=product&timstype=journal&timssubtypeid=+&deid=&epanumber=&ntisid=&archivestatus=both&ombcat=any&datebegincreated=&dateendcreated=&datebeginpublishedpresented=&dateendpublishedpresented=&datebeginupdated=&dateendupdated=&datebegincompleted=&dateendcompleted=&view=citation%20&personid=&role=any&journalid=&publisherid=&sortby=fy&count=25&cfid=77182256&cftoken=94527145','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=312470&keyword=cmaq&acttype=product&timstype=journal&timssubtypeid=+&deid=&epanumber=&ntisid=&archivestatus=both&ombcat=any&datebegincreated=&dateendcreated=&datebeginpublishedpresented=&dateendpublishedpresented=&datebeginupdated=&dateendupdated=&datebegincompleted=&dateendcompleted=&view=citation%20&personid=&role=any&journalid=&publisherid=&sortby=fy&count=25&cfid=77182256&cftoken=94527145"><span>Air pollution and climate response to <span class="hlt">aerosol</span> direct radiative ...</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>Decadal hemispheric Weather Research and Forecast-Community Multiscale Air Quality simulations from 1990 to 2010 were conducted to examine the meteorology and air quality responses to the <span class="hlt">aerosol</span> direct radiative effects. The model's performance for the simulation of hourly surface temperature, relative humidity, wind speed, and direction was evaluated through comparison with observations from NOAA's National Climatic Data Center Integrated Surface Data. The inclusion of <span class="hlt">aerosol</span> direct radiative effects improves the model's ability to reproduce the trend in daytime temperature range which over the past two decades was increasing in eastern China but decreasing in eastern U.S. and Europe. Trends and spatial and diurnal variations of the surface-level gaseous and particle concentrations to the <span class="hlt">aerosol</span> direct effect were analyzed. The inclusion of <span class="hlt">aerosol</span> direct radiative effects was found to increase the surface-level concentrations of SO2, NO2, O3, SO42−, NO3−, and particulate matter 2.5 in eastern China, eastern U.S., and Europe by 1.5–2.1%, 1–1.5%, 0.1–0.3%, 1.6–2.3%, 3.5–10.0%, and 2.2–3.2%, respectively, on average over the entire 21 year period. However, greater impacts are noted during polluted days with increases of 7.6–10.6%, 6.2–6.7%, 2.0–3.0%, 7.8–9.5%, 11.1–18.6%, and 7.2–10.1%, respectively. Due to the <span class="hlt">aerosol</span> direct radiative effects, stabilizing of the atmosphere associated with reduced planetary boundary layer <span class="hlt">height</span> a</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('https://ntrs.nasa.gov/search.jsp?R=20020083154&hterms=Net+Present+Value&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DNet%2BPresent%2BValue','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020083154&hterms=Net+Present+Value&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DNet%2BPresent%2BValue"><span>MPL-Net Measurements of <span class="hlt">Aerosol</span> and Cloud Vertical Distributions at Co-Located AERONET Sites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Welton, Ellsworth J.; Campbell, James R.; Berkoff, Timothy A.; Spinhirne, James D.; Tsay, Si-Chee; Holben, Brent; Starr, David OC. (Technical Monitor)</p> <p>2002-01-01</p> <p>In the early 1990s, the first small, eye-safe, and autonomous lidar system was developed, the Micropulse Lidar (MPL). The MPL acquires signal profiles of backscattered laser light from <span class="hlt">aerosols</span> and clouds. The signals are analyzed to yield multiple layer <span class="hlt">heights</span>, optical depths of each layer, average extinction-to-backscatter ratios for each layer, and profiles of extinction in each layer. In 2000, several MPL sites were organized into a coordinated network, called MPL-Net, by the Cloud and <span class="hlt">Aerosol</span> Lidar Group at NASA Goddard Space Flight Center (GSFC) using funding provided by the NASA Earth Observing System. tn addition to the funding provided by NASA EOS, the NASA CERES Ground Validation Group supplied four MPL systems to the project, and the NASA TOMS group contributed their MPL for work at GSFC. The Atmospheric Radiation Measurement Program (ARM) also agreed to make their data available to the MPL-Net project for processing. In addition to the initial NASA and ARM operated sites, several other independent research groups have also expressed interest in joining the network using their own instruments. Finally, a limited amount of EOS funding was set aside to participate in various field experiments each year. The NASA Sensor Intercomparison and Merger for Biological and Interdisciplinary Oceanic Studies (SIMBIOS) project also provides funds to deploy their MPL during ocean research cruises. All together, the MPL-Net project has participated in four major field experiments since 2000. Most MPL-Net sites and field experiment locations are also co-located with sunphotometers in the NASA <span class="hlt">Aerosol</span> Robotic Network. (AERONET). Therefore, at these locations data is collected on both <span class="hlt">aerosol</span> and cloud vertical structure as well as column optical depth and sky radiance. Real-time data products are now available from most MPL-Net sites. Our real-time products are generated at times of AERONET <span class="hlt">aerosol</span> optical depth (AOD) measurements. The AERONET AOD is used as input to our</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=sex+AND+videos&pg=2&id=EJ1169192','ERIC'); return false;" href="https://eric.ed.gov/?q=sex+AND+videos&pg=2&id=EJ1169192"><span><span class="hlt">Scaling</span> Constraints in Junior Tennis: The Influence of Net <span class="hlt">Height</span> on Skilled Players' Match-Play Performance</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>Limpens, Vera; Buszard, Tim; Shoemaker, Emma; Savelsbergh, Geert J. P.; Reid, Machar</p> <p>2018-01-01</p> <p>Purpose: The net <span class="hlt">height</span> in tennis (0.91 m) is approximately 50% of a professional tennis player's <span class="hlt">height</span>. Children are also expected to play with this net <span class="hlt">height</span>, even though it is approximately 70% of the average 10-year-old's <span class="hlt">height</span>. This study examined the immediate effect of lowering net <span class="hlt">height</span> on the performance characteristics of skilled…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080031633&hterms=smart+city&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsmart%2Bcity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080031633&hterms=smart+city&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsmart%2Bcity"><span>Ground-based Network and Supersite Measurements for Studying <span class="hlt">Aerosol</span> Properties and <span class="hlt">Aerosol</span>-Cloud Interactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsay, Si-Chee; Holben, Brent N.</p> <p>2008-01-01</p> <p> capability of AERONET SMART-COMMIT in current Asian Monsoon Year-2008 campaigns that are designed and being executed to study the compelling variability in temporal <span class="hlt">scale</span> of both anthropogenic and natural <span class="hlt">aerosols</span> (e.g., airborne dust, smoke, mega-city pollutant). Feedback mechanisms between <span class="hlt">aerosol</span> radiative effects and monsoon dynamics have been recently proposed, however there is a lack of consensus on whether <span class="hlt">aerosol</span> forcing would be more likely to enhance or reduce the strength of the monsoon circulation. We envision robust approaches which well-collocated ground-based measurements and space-borne observations will greatly advance our understanding of absorbing <span class="hlt">aerosols</span> (e.g., "Global Dimming" vs. "Elevated Heat-Pump" effects) on <span class="hlt">aerosol</span> cloud water cycle interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B53H0611M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B53H0611M"><span>Deriving Temporal <span class="hlt">Height</span> Information for Maize Breeding</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malambo, L.; Popescu, S. C.; Murray, S.; Sheridan, R.; Richardson, G.; Putman, E.</p> <p>2016-12-01</p> <p>Phenotypic data such as <span class="hlt">height</span> provide useful information to crop breeders to better understand their field experiments and associated field variability. However, the measurement of crop <span class="hlt">height</span> in many breeding programs is done manually which demands significant effort and time and does not <span class="hlt">scale</span> well when large field experiments are involved. Through structure from motion (SfM) techniques, small unmanned aerial vehicles (sUAV) or drones offer tremendous potential for generating crop <span class="hlt">height</span> data and other morphological data such as canopy area and biomass in cost-effective and efficient way. We present results of an on-going UAV application project aimed at generating temporal <span class="hlt">height</span> metrics for maize breeding at the Texas A&M AgriLife Research farm in Burleson County, Texas. We outline the activities involved from the drone aerial surveys, image processing and generation of crop <span class="hlt">height</span> metrics. The experimental period ran from April (planting) through August (harvest) 2016 and involved 36 maize hybrids replicated over 288 plots ( 1.7 Ha). During the time, crop <span class="hlt">heights</span> were manually measured per plot at weekly intervals. Corresponding aerial flights were carried out using a DJI Phantom 3 Professional UAV at each interval and images captured processed into point clouds and image mosaics using Pix4D (Pix4D SA; Lausanne, Switzerland) software. LiDAR data was also captured at two intervals (05/06 and 07/29) to provide another source of <span class="hlt">height</span> information. To obtain <span class="hlt">height</span> data per plot from SfM point clouds and LiDAR data, percentile <span class="hlt">height</span> metrics were then generated using FUSION software. Results of the comparison between SfM and field measurement <span class="hlt">height</span> show high correlation (R2 > 0.7), showing that use of sUAV can replace laborious manual <span class="hlt">height</span> measurement and enhance plant breeding programs. Similar results were also obtained from the comparison of SfM and LiDAR <span class="hlt">heights</span>. Outputs of this project are helping plant breeders at Texas A&M automate routine <span class="hlt">height</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150006839','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150006839"><span>High Resolution <span class="hlt">Aerosol</span> Data from MODIS Satellite for Urban Air Quality Studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chudnovsky, A.; Lyapustin, A.; Wang, Y.; Tang, C.; Schwartz, J.; Koutrakis, P.</p> <p>2013-01-01</p> <p>The Moderate Resolution Imaging Spectroradiometer (MODIS) provides daily global coverage, but the 10 km resolution of its <span class="hlt">aerosol</span> optical depth (AOD) product is not suitable for studying spatial variability of <span class="hlt">aerosols</span> in urban areas. Recently, a new Multi-Angle Implementation of Atmospheric Correction (MAIAC) algorithm was developed for MODIS which provides AOD at 1 km resolution. Using MAIAC data, the relationship between MAIAC AOD and PM(sub 2.5) as measured by the 27 EPA ground monitoring stations was investigated. These results were also compared to conventional MODIS 10 km AOD retrievals (MOD04) for the same days and locations. The coefficients of determination for MOD04 and for MAIAC are R(exp 2) =0.45 and 0.50 respectively, suggested that AOD is a reasonably good proxy for PM(sub 2.5) ground concentrations. Finally, we studied the relationship between PM(sub 2.5) and AOD at the intra-urban <span class="hlt">scale</span> (10 km) in Boston. The fine resolution results indicated spatial variability in particle concentration at a sub-10 kilometer <span class="hlt">scale</span>. A local analysis for the Boston area showed that the AOD-PM(sub 2.5) relationship does not depend on relative humidity and air temperatures below approximately 7 C. The correlation improves for temperatures above 7 - 16 C. We found no dependence on the boundary layer <span class="hlt">height</span> except when the former was in the range 250-500 m. Finally, we apply a mixed effects model approach to MAIAC <span class="hlt">aerosol</span> optical depth (AOD) retrievals from MODIS to predict PM(sub 2.5) concentrations within the greater Boston area. With this approach we can control for the inherent day-to-day variability in the AOD-PM(sub 2.5) relationship, which depends on time-varying parameters such as particle optical properties, vertical and diurnal concentration profiles and ground surface reflectance. Our results show that the model-predicted PM(sub 2.5) mass concentrations are highly correlated with the actual observations (out-of-sample R(exp 2) of 0.86). Therefore, adjustment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002PhDT........76A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002PhDT........76A"><span>Whitecaps, sea-salt <span class="hlt">aerosols</span>, and climate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anguelova, Magdalena Dimitrova</p> <p></p> <p>Oceanic whitecaps are the major source of sea-salt <span class="hlt">aerosols</span>. Because these <span class="hlt">aerosols</span> are dominant in remote marine air, they control the radiative properties of the clean background atmosphere by scattering sunlight, changing cloud properties and lifetime, and providing media for chemical reactions. Including sea-salt effects in climate models improves predictions, but simulating their generation is first necessary. To make the sea-salt generation function currently used in climate models more relevant for <span class="hlt">aerosol</span> investigations, this study proposes two modifications. First, the conventional relation between whitecap coverage, W, and the 10-meter wind speed, U10, used in typical generation functions is expanded to include additional factors that affect whitecaps and sea-salt <span class="hlt">aerosol</span> formation. Second, the sea-salt generation function is extended to smaller sizes; sea-salt <span class="hlt">aerosol</span> with initial radii from 0.4 to 20 mum can now be modeled. To achieve these goals, this thesis develops a new method for estimating whitecap coverage on a global <span class="hlt">scale</span> using satellite measurements of the brightness temperature of the ocean surface. Whitecap coverage evaluated with this method incorporates the effects of atmospheric stability, sea-surface temperature, salinity, wind fetch, wind duration, and the amount of surface-active material. Assimilating satellite-derived values for whitecap coverage in the sea-salt generation function incorporates the effects of all environmental factors on sea-salt production and predicts realistic sea-salt <span class="hlt">aerosol</span> loadings into the atmosphere. An extensive database of whitecap coverage and sea-salt <span class="hlt">aerosol</span> fluxes has been compiled with the new method and is used to investigate their spatial and temporal characteristics. The composite effect of all environmental factors suggests a more uniform latitudinal distribution of whitecaps and sea-salt <span class="hlt">aerosols</span> than that predicted from wind speed alone. The effect of sea-surface temperature, TS, is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A33H3302G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A33H3302G"><span>The Global Ozone and <span class="hlt">Aerosol</span> Profiles and <span class="hlt">Aerosol</span> Hygroscopic Effect and Absorption Optical Depth (GOA2HEAD) Network Initiative</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, R. S.; Elkins, J. W.; Frost, G. J.; McComiskey, A. C.; Murphy, D. M.; Ogren, J. A.; Petropavlovskikh, I. V.; Rosenlof, K. H.</p> <p>2014-12-01</p> <p>Inverse modeling using measurements of ozone (O3) and <span class="hlt">aerosol</span> is a powerful tool for deriving pollutant emissions. Because they have relatively long lifetimes, O3 and <span class="hlt">aerosol</span> are transported over large distances. Frequent and globally spaced vertical profiles rather than ground-based measurements alone are therefore highly desired. Three requirements necessary for a successful global monitoring program are: Low equipment cost, low operation cost, and reliable measurements of known uncertainty. Conventional profiling using aircraft provides excellent data, but is cost prohibitive on a large <span class="hlt">scale</span>. Here we describe a new platform and instruments meeting all three global monitoring requirements. The platform consists of a small balloon and an auto-homing glider. The glider is released from the balloon at about 5 km altitude, returning the light instrument package to the launch location, and allowing for consistent recovery of the payload. Atmospheric profiling can be performed either during ascent or descent (or both) depending on measurement requirements. We will present the specifications for two instrument packages currently under development. The first measures O3, RH, p, T, dry <span class="hlt">aerosol</span> particle number and size distribution, and <span class="hlt">aerosol</span> optical depth. The second measures dry <span class="hlt">aerosol</span> particle number and size distribution, and <span class="hlt">aerosol</span> absorption coefficient. Other potential instrument packages and the desired spatial/temporal resolution for the GOA2HEAD monitoring initiative will also be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1657m0001T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1657m0001T"><span>Investigation of <span class="hlt">aerosol</span> distribution patterns and its optical properties at different time <span class="hlt">scale</span> by using LIDAR system and AERONET</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tan, Fuyi; Khor, Wei Ying; Hee, Wan Shen; Choon, Yeap Eng; San, Lim Hwee; Abdullah, Khiruddin</p> <p>2015-04-01</p> <p>Atmospheric <span class="hlt">aerosol</span> is a major health-impairment issue in Malaysia especially during southeast monsoon period (June-September) due to the active open burning activities. However, hazy days were an issue in Penang, Malaysia during March, 2014. Haze intruded Penang during March and lasted for a month except for the few days after rain. Rain water had washed out the <span class="hlt">aerosols</span> from the atmosphere. Therefore, this study intends to analyse the <span class="hlt">aerosol</span> profile and the optical properties of <span class="hlt">aerosol</span> during this haze event and after rain. Meanwhile, several days after the haze event (during April, 2014) were also analyzed for comparison purposes. Additionally, the dominant <span class="hlt">aerosol</span> type (i.e., dust, biomass burning, industrial and urban, marine, and mixed <span class="hlt">aerosol</span>) during the study period was identified according to the scattering plots of the <span class="hlt">aerosol</span> optical depth (AOD) against the Angstrom exponent.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A13A0162L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A13A0162L"><span>Secondary Organic <span class="hlt">Aerosol</span> Formation in the Captive <span class="hlt">Aerosol</span> Growth and Evolution (CAGE) Chambers during the Southern Oxidant and <span class="hlt">Aerosol</span> Study (SOAS) in Centreville, AL</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Leong, Y.; Karakurt Cevik, B.; Hernandez, C.; Griffin, R. J.; Taylor, N.; Matus, J.; Collins, D. R.</p> <p>2013-12-01</p> <p>Secondary organic <span class="hlt">aerosol</span> (SOA) represents a large portion of sub-micron particulate matter on a global <span class="hlt">scale</span>. The composition of SOA and its formation processes are heavily influenced by anthropogenic and biogenic activity. Volatile organic compounds (VOCs) that are emitted naturally from forests or from human activity serve as precursors to SOA formation. Biogenic SOA (BSOA) is formed from biogenic VOCs and is prevalent in forested regions like the Southeastern United States. The formation and enhancement of BSOA under anthropogenic influences such as nitrogen oxides (NOx), sulfur dioxide (SO2), and oxygen radicals are still not well understood. The lack of information on anthropogenic BSOA enhancement and the reversibility of SOA formation could explain the underprediction of SOA in current models. To address some of these gaps in knowledge, this study was conducted as part of the Southern Oxidant and <span class="hlt">Aerosol</span> Study (SOAS) in Centreville, AL during the summer of 2013. SOA growth experiments were conducted in two Captive <span class="hlt">Aerosol</span> Growth and Evolution (CAGE) outdoor chambers located at the SEARCH site. Ambient trace gas concentrations were maintained in these chambers using semi-permeable gas-exchange membranes, while studying the growth of injected monodisperse seed <span class="hlt">aerosol</span>. The control chamber was operated under ambient conditions; the relative humidity and oxidant and NOx levels were perturbed in the second chamber. This design allows experiments to capture the natural BSOA formation processes in the southeastern atmosphere and to study the influence of anthropogenic activity on <span class="hlt">aerosol</span> chemistry. Chamber experiments were periodically monitored with physical and chemical instrumentation including a scanning mobility particle sizer (SMPS), a cloud condensation nuclei counter (CCNC), a humidified tandem differential mobility analyzer (H-TDMA), and an Aerodyne high-resolution time-of-flight <span class="hlt">aerosol</span> mass spectrometer (HR-ToF-AMS). The CAGE experiments focused on SOA</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17..449L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17..449L"><span>Background <span class="hlt">aerosol</span> over the Himalayas and Tibetan Plateau: observed characteristics of <span class="hlt">aerosol</span> mass loading</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Bin; Cong, Zhiyuan; Wang, Yuesi; Xin, Jinyuan; Wan, Xin; Pan, Yuepeng; Liu, Zirui; Wang, Yonghong; Zhang, Guoshuai; Wang, Zhongyan; Wang, Yongjie; Kang, Shichang</p> <p>2017-01-01</p> <p>To investigate the atmospheric <span class="hlt">aerosols</span> of the Himalayas and Tibetan Plateau (HTP), an observation network was established within the region's various ecosystems, including at the Ngari, Qomolangma (QOMS), Nam Co, and Southeastern Tibetan (SET) stations. In this paper we illustrate <span class="hlt">aerosol</span> mass loadings by integrating in situ measurements with satellite and ground-based remote sensing datasets for the 2011-2013 period, on both local and large <span class="hlt">scales</span>. Mass concentrations of these surface atmospheric <span class="hlt">aerosols</span> were relatively low and varied with land cover, showing a general tendency of Ngari and QOMS (barren sites) > Nam Co (grassland site) > SET (forest site). Daily averages of online PM2.5 (particulates with aerodynamic diameters below 2.5 µm) at these sites were sequentially 18.2 ± 8.9, 14.5 ± 7.4, 11.9 ± 4.9 and 11.7 ± 4.7 µg m-3. Correspondingly, the ratios of PM2.5 to total suspended particles (TSP) were 27.4 ± 6.65, 22.3 ± 10.9, 37.3 ± 11.1 and 54.4 ± 6.72 %. Bimodal mass distributions of size-segregated particles were found at all sites, with a relatively small peak in accumulation mode and a more notable peak in coarse mode. Diurnal variations in fine-<span class="hlt">aerosol</span> masses generally displayed a bi-peak pattern at the QOMS, Nam Co and SET stations and a single-peak pattern at the Ngari station, controlled by the effects of local geomorphology, mountain-valley breeze circulation and <span class="hlt">aerosol</span> emissions. Dust <span class="hlt">aerosol</span> content in PM2.1 samples gave fractions of 26 % at the Ngari station and 29 % at the QOMS station, or ˜ 2-3 times that of reported results at human-influenced sites. Furthermore, observed evidence confirmed the existence of the aerodynamic conditions necessary for the uplift of fine particles from a barren land surface. Combining surface <span class="hlt">aerosol</span> data and atmospheric-column <span class="hlt">aerosol</span> optical properties, the TSP mass and <span class="hlt">aerosol</span> optical depth (AOD) of the Multi-angle Imaging Spectroradiometer (MISR) generally decreased as land cover changed from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.A23A0275W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.A23A0275W"><span>Evaluation of 3-D Air Quality System Remotely-Sensed <span class="hlt">Aerosol</span> Optical Depth for the Baltimore/Washington Metropolitan Air Shed</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weber, S. A.; Engel-Cox, J. A.; Hoff, R. M.; Prados, A.; Zhang, H.</p> <p>2008-12-01</p> <p>Integrating satellite- and ground-based <span class="hlt">aerosol</span> optical depth (AOD) observations with surface total fine particulate (PM2.5) and sulfate concentrations allows for a more comprehensive understanding of local- and urban-<span class="hlt">scale</span> air quality. This study evaluates the utility of integrated databases being developed for NOAA and EPA through the 3D-AQS project by examining the relationship between remotely-sensed AOD and PM2.5 concentrations for each platform for the summer of 2004 and the entire year of 2005. We compare results for the Baltimore, MD/Washington, DC metropolitan air shed, incorporating AOD products from the Terra and GOES-12 satellites, AERONET sunphotometer, and ground-based lidar, and PM2.5 concentrations from five surface monitoring sites. The satellite-derived products include AOD from the Moderate Resolution Imaging Spectroradiometer (MODIS) and Multi-angle Imaging Spectroradiometer (MISR), as well as the GOES <span class="hlt">Aerosol</span>/Smoke Product (GASP). The vertical profile of lidar backscatter is used to retrieve the planetary boundary layer (PBL) <span class="hlt">height</span> in an attempt to capture only that fraction of the AOD arising from near surface <span class="hlt">aerosols</span>. Adjusting the AOD data using platform- and season-specific ratios, calculated using the parameters of the regression equations, for two case studies resulted in a more accurate representation of surface PM2.5 concentrations when compared to a constant ratio that is currently being used in the NOAA IDEA product. This work demonstrates that quantitative relationships between remotely-sensed and in-situ <span class="hlt">aerosol</span> observations in an integrated database can be computed and applied to improve the use of remotely-sensed observations for estimating surface concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A23C2369R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A23C2369R"><span>CATS Cloud and <span class="hlt">Aerosol</span> Level 2 Heritage Edition Data Products.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rodier, S. D.; Vaughan, M.; Yorks, J. E.; Palm, S. P.; Selmer, P. A.; Hlavka, D. L.; McGill, M. J.; Trepte, C. R.</p> <p>2017-12-01</p> <p>The Cloud-<span class="hlt">Aerosol</span> Transport System (CATS) instrument was developed at NASA's Goddard Space Flight Center (GSFC) and deployed to the International Space Station (ISS) in January 2015. The CATS elastic backscatter lidars have been operating continuously in one of two science modes since February 2015. One of the primary science objectives of CATS is to continue the CALIPSO <span class="hlt">aerosol</span> and cloud profile data record to provide continuity of lidar climate observations during the transition from CALIPSO to EarthCARE. To accomplish this, the CATS project at NASA's Goddard Space Flight Center (GSFC) and the CALIPSO project at NASA's Langley Research Center (LaRC) closely collaborated to develop and deliver a full suite of CALIPSO-like level 2 data products using the latest version of the CALIPSO level 2 Version 4 algorithms for the CATS data acquired while operating in science mode 1 (Multi-beam backscatter detection at 1064 and 532 nm, with depolarization measurement at both wavelengths). In this work, we present the current status of the CATS Heritage (i.e. CALIPSO-like) level 2 data products derived from the recent released CATS Level 1B V2-08 data. Extensive comparisons are performed between the three data sets (CALIPSO V4.10 Level 2, CATS Level 2 Operational V2-00 and CATS Heritage V1.00) for cloud and <span class="hlt">aerosol</span> measurements (e.g., cloud-top <span class="hlt">height</span> cloud-phase, cloud-layer occurrence frequency and cloud-<span class="hlt">aerosol</span> discrimination) along the ISS path. In addition, global comparisons (between 52°S and 52°N) of <span class="hlt">aerosol</span> extinction profiles derived from the CATS Level 2 Operational products and CALIOP V4 Level 2 products are presented. Comparisons of <span class="hlt">aerosol</span> optical depths retrieved from active sensors (CATS and CALIOP) and passive sensors (MODIS) will provide context for the extinction profile comparisons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110007811&hterms=april+pierce&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dapril%2Bpierce','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110007811&hterms=april+pierce&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dapril%2Bpierce"><span>Detecting Thin Cirrus in Multiangle Imaging Spectroradiometer <span class="hlt">Aerosol</span> Retrievals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pierce, Jeffrey R.; Kahn, Ralph A.; Davis, Matt R.; Comstock, Jennifer M.</p> <p>2010-01-01</p> <p>Thin cirrus clouds (optical depth (OD) < 03) are often undetected by standard cloud masking in satellite <span class="hlt">aerosol</span> retrieval algorithms. However, the Mu]tiangle Imaging Spectroradiometer (MISR) <span class="hlt">aerosol</span> retrieval has the potential to discriminate between the scattering phase functions of cirrus and <span class="hlt">aerosols</span>, thus separating these components. Theoretical tests show that MISR is sensitive to cirrus OD within Max{0.05 1 20%l, similar to MISR's sensitivity to <span class="hlt">aerosol</span> OD, and MISR can distinguish between small and large crystals, even at low latitudes, where the range of scattering angles observed by MISR is smallest. Including just two cirrus components in the <span class="hlt">aerosol</span> retrieval algorithm would capture typical MISR sensitivity to the natural range of cinus properties; in situations where cirrus is present but the retrieval comparison space lacks these components, the retrieval tends to underestimate OD. Generally, MISR can also distinguish between cirrus and common <span class="hlt">aerosol</span> types when the proper cirrus and <span class="hlt">aerosol</span> optical models are included in the retrieval comparison space and total column OD is >-0.2. However, in some cases, especially at low latitudes, cirrus can be mistaken for some combinations of dust and large nonabsorbing spherical <span class="hlt">aerosols</span>, raising a caution about retrievals in dusty marine regions when cirrus is present. Comparisons of MISR with lidar and <span class="hlt">Aerosol</span> Robotic Network show good agreement in a majority of the cases, but situations where cirrus clouds have optical depths >0.15 and are horizontally inhomogeneous on spatial <span class="hlt">scales</span> shorter than 50 km pose difficulties for cirrus retrieval using the MISR standard <span class="hlt">aerosol</span> algorithm..</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.7709B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.7709B"><span>How much of the global <span class="hlt">aerosol</span> optical depth is found in the boundary layer and free troposphere?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bourgeois, Quentin; Ekman, Annica M. L.; Renard, Jean-Baptiste; Krejci, Radovan; Devasthale, Abhay; Bender, Frida A.-M.; Riipinen, Ilona; Berthet, Gwenaël; Tackett, Jason L.</p> <p>2018-06-01</p> <p>The global <span class="hlt">aerosol</span> extinction from the CALIOP space lidar was used to compute <span class="hlt">aerosol</span> optical depth (AOD) over a 9-year period (2007-2015) and partitioned between the boundary layer (BL) and the free troposphere (FT) using BL <span class="hlt">heights</span> obtained from the ERA-Interim archive. The results show that the vertical distribution of AOD does not follow the diurnal cycle of the BL but remains similar between day and night highlighting the presence of a residual layer during night. The BL and FT contribute 69 and 31 %, respectively, to the global tropospheric AOD during daytime in line with observations obtained in Aire sur l'Adour (France) using the Light Optical <span class="hlt">Aerosol</span> Counter (LOAC) instrument. The FT AOD contribution is larger in the tropics than at mid-latitudes which indicates that convective transport largely controls the vertical profile of <span class="hlt">aerosols</span>. Over oceans, the FT AOD contribution is mainly governed by long-range transport of <span class="hlt">aerosols</span> from emission sources located within neighboring continents. According to the CALIOP <span class="hlt">aerosol</span> classification, dust and smoke particles are the main <span class="hlt">aerosol</span> types transported into the FT. Overall, the study shows that the fraction of AOD in the FT - and thus potentially located above low-level clouds - is substantial and deserves more attention when evaluating the radiative effect of <span class="hlt">aerosols</span> in climate models. More generally, the results have implications for processes determining the overall budgets, sources, sinks and transport of <span class="hlt">aerosol</span> particles and their description in atmospheric models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000024928&hterms=remote+sensing+satellites&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dremote%2Bsensing%2Bsatellites','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000024928&hterms=remote+sensing+satellites&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dremote%2Bsensing%2Bsatellites"><span>Satellite Remote Sensing of <span class="hlt">Aerosol</span> Forcing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Remer, Lorraine; Kaufman, Yoram; Ramaprasad, Jaya; Procopio, Aline; Levin, Zev</p> <p>1999-01-01</p> <p>The role of <span class="hlt">aerosol</span> forcing remains one of the largest uncertainties in estimating man's impact on the global climate system. One school of thought suggests that remote sensing by satellite sensors will provide the data necessary to narrow these uncertainties. While satellite measurements of direct <span class="hlt">aerosol</span> forcing appear to be straightforward, satellite measurements of <span class="hlt">aerosol</span> indirect forcing will be more complicated. Pioneering studies identified indirect <span class="hlt">aerosol</span> forcing using AVHRR data in the biomass burning regions of Brazil. We have expanded this analysis with AVHRR to include an additional year of data and assimilated water vapor fields. The results show similar latitudinal dependence as reported by Kaufman and Fraser, but by using water vapor observations we conclude that latitude is not a proxy for water vapor and the strength of the indirect effect is not correlated to water vapor amounts. In addition to the AVHRR study we have identified indirect <span class="hlt">aerosol</span> forcing in Brazil at much smaller spatial <span class="hlt">scales</span> using the MODIS Airborne Simulator. The strength of the indirect effect appears to be related to cloud type and cloud dynamics. There is a suggestion that some of the cloud dynamics may be influenced by smoke destabilization of the atmospheric column. Finally, this study attempts to quantify remote sensing limitations due to the accuracy limits of the retrieval algorithms. We use a combination of numerical <span class="hlt">aerosol</span> transport models, ground-based AERONET data and ISCCP cloud climatology to determine how much of the forcing occurs in regions too clean to determine from satellite retrievals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984NIMPB...3..296B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984NIMPB...3..296B"><span>Large <span class="hlt">scale</span> intercomparison of <span class="hlt">aerosol</span> trace element analysis by different analytical methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bombelka, E.; Richter, F.-W.; Ries, H.; Wätjen, U.</p> <p>1984-04-01</p> <p>The general agreement of PIXE analysis with other methods (INAA, XRF, AAS, OES-ICP, and PhAA) is very good based on the analysis of filter pieces taken from 250 <span class="hlt">aerosol</span> samples. It is better than 5% for Pb and Zn, better than 10% for V, Cr, and Mn, indicating that the accuracy of PIXE analysis can be within 10%. For elements such as Cd and Sb, difficult to analyze by PIXE because of their low mass content in the sample, the agreement is given mainly by the reproducibility of the method (20% to 30%). Similar agreement is found for sulfur, after taking account of the depth distribution of the <span class="hlt">aerosol</span> in the filter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4114406','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4114406"><span>A Multi-Year <span class="hlt">Aerosol</span> Characterization for the Greater Tehran Area Using Satellite, Surface, and Modeling 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>Crosbie, Ewan; Sorooshian, Armin; Monfared, Negar Abolhassani; Shingler, Taylor; Esmaili, Omid</p> <p>2014-01-01</p> <p>This study reports a multi-year (2000–2009) <span class="hlt">aerosol</span> characterization for metropolitan Tehran and surrounding areas using multiple datasets (Moderate Resolution Imaging Spectroradiometer (MODIS), Multi-angle Imaging Spectroradiometer (MISR), Total Ozone Mapping Spectrometer (TOMS), Goddard Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport (GOCART), and surface and upper air data from local stations). Monthly trends in <span class="hlt">aerosol</span> characteristics are examined in the context of the local meteorology, regional and local emission sources, and air mass back-trajectory data. Dust strongly affects the region during the late spring and summer months (May–August) when <span class="hlt">aerosol</span> optical depth (AOD) is at its peak and precipitation accumulation is at a minimum. In addition, the peak AOD that occurs in July is further enhanced by a substantial number of seasonal wildfires in upwind regions. Conversely, AOD is at a minimum during winter; however, reduced mixing <span class="hlt">heights</span> and a stagnant lower atmosphere trap local <span class="hlt">aerosol</span> emissions near the surface and lead to significant reductions in visibility within Tehran. The unique meteorology and topographic setting makes wintertime visibility and surface <span class="hlt">aerosol</span> concentrations particularly sensitive to local anthropogenic sources and is evident in the noteworthy improvement in visibility observed on weekends. Scavenging of <span class="hlt">aerosol</span> due to precipitation is evident during the winter when aconsistent increase in surface visibility and concurrent decrease in AOD is observed in the days after rain compared with the days immediately before rain. PMID:25083295</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....1714871N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....1714871N"><span>Changing transport processes in the stratosphere by radiative heating of sulfate <span class="hlt">aerosols</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Niemeier, Ulrike; Schmidt, Hauke</p> <p>2017-12-01</p> <p>The injection of sulfur dioxide (SO2) into the stratosphere to form an artificial stratospheric <span class="hlt">aerosol</span> layer is discussed as an option for solar radiation management. Sulfate <span class="hlt">aerosol</span> scatters solar radiation and absorbs infrared radiation, which warms the stratospheric sulfur layer. Simulations with the general circulation model ECHAM5-HAM, including <span class="hlt">aerosol</span> microphysics, show consequences of this warming, including changes of the quasi-biennial oscillation (QBO) in the tropics. The QBO slows down after an injection of 4 Tg(S) yr-1 and completely shuts down after an injection of 8 Tg(S) yr-1. Transport of species in the tropics and sub-tropics depends on the phase of the QBO. Consequently, the heated <span class="hlt">aerosol</span> layer not only impacts the oscillation of the QBO but also the meridional transport of the sulfate <span class="hlt">aerosols</span>. The stronger the injection, the stronger the heating and the simulated impact on the QBO and equatorial wind systems. With increasing injection rate the velocity of the equatorial jet streams increases, and the less sulfate is transported out of the tropics. This reduces the global distribution of sulfate and decreases the radiative forcing efficiency of the <span class="hlt">aerosol</span> layer by 10 to 14 % compared to simulations with low vertical resolution and without generated QBO. Increasing the <span class="hlt">height</span> of the injection increases the radiative forcing only for injection rates below 10 Tg(S) yr-1 (8-18 %), a much smaller value than the 50 % calculated previously. Stronger injection rates at higher levels even result in smaller forcing than the injections at lower levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790011306','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790011306"><span>The investigation of advanced remote sensing techniques for the measurement of <span class="hlt">aerosol</span> characteristics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Deepak, A.; Becher, J.</p> <p>1979-01-01</p> <p>Advanced remote sensing techniques and inversion methods for the measurement of characteristics of <span class="hlt">aerosol</span> and gaseous species in the atmosphere were investigated. Of particular interest were the physical and chemical properties of <span class="hlt">aerosols</span>, such as their size distribution, number concentration, and complex refractive index, and the vertical distribution of these properties on a local as well as global <span class="hlt">scale</span>. Remote sensing techniques for monitoring of tropospheric <span class="hlt">aerosols</span> were developed as well as satellite monitoring of upper tropospheric and stratospheric <span class="hlt">aerosols</span>. Computer programs were developed for solving multiple scattering and radiative transfer problems, as well as inversion/retrieval problems. A necessary aspect of these efforts was to develop models of <span class="hlt">aerosol</span> properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.A13A0179K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.A13A0179K"><span>Measurements of Semi-volatile <span class="hlt">Aerosol</span> and Its Effect on <span class="hlt">Aerosol</span> Optical Properties During Southern Oxidant and <span class="hlt">Aerosol</span> Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khlystov, A.; Grieshop, A. P.; Saha, P.; Subramanian, R.</p> <p>2013-12-01</p> <p>Semi-volatile compounds, including particle-bound water, comprise a large part of <span class="hlt">aerosol</span> mass and have a significant influence on <span class="hlt">aerosol</span> lifecycle and its optical properties. Understanding the properties of semi-volatile compounds, especially those pertaining to gas/<span class="hlt">aerosol</span> partitioning, is of critical importance for our ability to predict concentrations and properties of ambient <span class="hlt">aerosol</span>. A set of state-of-the-art instruments was deployed at the SEARCH site near Centerville, AL during the Southern Oxidant and <span class="hlt">Aerosol</span> Study (SOAS) campaign in summer 2013 to measure the effect of temperature and relative humidity on <span class="hlt">aerosol</span> size distribution, composition and optical properties. Light scattering and absorption by temperature- and humidity-conditioned <span class="hlt">aerosols</span> was measured using three photo-acoustic extinctiometers (PAX) at three wavelengths (405 nm, 532 nm, and 870 nm). In parallel to these measurements, a long residence time temperature-stepping thermodenuder and a variable residence time constant temperature thermodenuder in combination with three SMPS systems and an <span class="hlt">Aerosol</span> Chemical Speciation Monitor (ACSM) were used to assess <span class="hlt">aerosol</span> volatility and kinetics of <span class="hlt">aerosol</span> evaporation. It was found that both temperature and relative humidity have a strong effect on <span class="hlt">aerosol</span> optical properties. The variable residence time thermodenuder data suggest that <span class="hlt">aerosol</span> equilibrated fairly quickly, within 2 s, in contrast to other ambient observations. Preliminary analysis show that approximately 50% and 90% of total <span class="hlt">aerosol</span> mass evaporated at temperatures of 100 C and 180C, respectively. Evaporation varied substantially with ambient <span class="hlt">aerosol</span> loading and composition and meteorology. During course of this study, T50 (temperatures at which 50% <span class="hlt">aerosol</span> mass evaporates) varied from 60 C to more than 120 C.</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/2015AGUFM.A33G0249H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A33G0249H"><span>Global Climate Models Intercomparison of Anthropogenic <span class="hlt">Aerosols</span> Effects on Regional Climate over North Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, J.; Zhang, R.; Wang, Y.; Ming, Y.; Lin, Y.; Pan, B.</p> <p>2015-12-01</p> <p><span class="hlt">Aerosols</span> can alter atmospheric radiation and cloud physics, which further exert impacts on weather and global climate. With the development and industrialization of the developing Asian countries, anthropogenic <span class="hlt">aerosols</span> have received considerable attentions and remain to be the largest uncertainty in the climate projection. Here we assess the performance of two stat-of-art global climate models (National Center for Atmospheric Research-Community Atmosphere Model 5 (CAM5) and Geophysical Fluid Dynamics Laboratory Atmosphere Model 3 (AM3)) in simulating the impacts of anthropogenic <span class="hlt">aerosols</span> on North Pacific storm track region. By contrasting two <span class="hlt">aerosol</span> scenarios, i.e. present day (PD) and pre-industrial (PI), both models show <span class="hlt">aerosol</span> optical depth (AOD) enhanced by about 22%, with CAM5 AOD 40% lower in magnitude due to the long range transport of anthropogenic <span class="hlt">aerosols</span>. <span class="hlt">Aerosol</span> effects on the ice water path (IWP), stratiform precipitation, convergence and convection strengths in the two models are distinctive in patterns and magnitudes. AM3 shows qualitatively good agreement with long-term satellite observations, while CAM5 overestimates convection and liquid water path resulting in an underestimation of large-<span class="hlt">scale</span> precipitation and IWP. Due to coarse resolution and parameterization in convection schemes, both models' performance on convection needs to be improved. <span class="hlt">Aerosols</span> performance on large-<span class="hlt">scale</span> circulation and radiative budget are also examined in this study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.A11D0121V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.A11D0121V"><span>Toward Investigating Optically Trapped Organic <span class="hlt">Aerosols</span> with CARS Microspectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Voss, L. F.</p> <p>2009-12-01</p> <p>The Intergovernmental Panel on Climate Change notes the huge uncertainty in the effect that atmospheric <span class="hlt">aerosols</span> play in determining overall global temperature, specifically in their ability to nucleate clouds. To better understand <span class="hlt">aerosol</span> chemistry, the novel coupling of gradient force optical trapping with broad bandwidth coherent anti-Stokes Raman scattering (CARS) spectroscopy is being developed to study single particles suspended in air. Building on successful designs employed separately for the techniques, this hybrid technology will be used to explain how the oxidation of organic compounds changes the chemical and physical properties of <span class="hlt">aerosols</span>. By trapping the particles, an individual <span class="hlt">aerosol</span> can be studied for up to several days. Using a broad bandwidth pulse for one of the incident beams will result in a Raman vibrational spectrum from every laser pulse. Combined with signal enhancement due to resonance and coherence of nonlinear CARS spectroscopy, this technique will allow for acquisition of data on the millisecond time <span class="hlt">scale</span>, facilitating the study of dynamic processes. This will provide insights on how <span class="hlt">aerosols</span> react with and absorb species from the gas phase. These experiments will increase understanding of <span class="hlt">aerosol</span> oxidation and growth mechanisms and the effects that <span class="hlt">aerosols</span> have on our atmosphere and climate. Progress in efforts developing this novel technique to study model systems is presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26257345','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26257345"><span>Vertical distribution of <span class="hlt">aerosol</span> optical properties based on aircraft measurements over the Loess Plateau 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>Li, Junxia; Liu, Xingang; Yuan, Liang; Yin, Yan; Li, Zhanqing; Li, Peiren; Ren, Gang; Jin, Lijun; Li, Runjun; Dong, Zipeng; Li, Yiyu; Yang, Junmei</p> <p>2015-08-01</p> <p>Vertical distributions of <span class="hlt">aerosol</span> optical properties based on aircraft measurements over the Loess Plateau were measured for the first time during a summertime aircraft campaign, 2013 in Shanxi, China. Data from four flights were analyzed. The vertical distributions of <span class="hlt">aerosol</span> optical properties including <span class="hlt">aerosol</span> scattering coefficients (σsc), absorption coefficients (σab), Angström exponent (α), single scattering albedo (ω), backscattering ratio (βsc), <span class="hlt">aerosol</span> mass scattering proficiency (Qsc) and <span class="hlt">aerosol</span> surface scattering proficiency (Qsc(')) were obtained. The mean statistical values of σsc were 77.45 Mm(-1) (at 450 nm), 50.72 Mm(-1) (at 550n m), and 32.02 Mm(-1) (at 700 nm). The mean value of σab was 7.62 Mm(-1) (at 550 nm). The mean values of α, βsc and ω were 1.93, 0.15, and 0.91, respectively. <span class="hlt">Aerosol</span> concentration decreased with altitude. Most effective diameters (ED) of <span class="hlt">aerosols</span> were less than 0.8 μm. The vertical profiles of σsc,, α, βsc, Qsc and Qsc(') showed that the <span class="hlt">aerosol</span> scattering properties at lower levels contributed the most to the total <span class="hlt">aerosol</span> radiative forcing. Both α and βsc had relatively large values, suggesting that most <span class="hlt">aerosols</span> in the observational region were small particles. The mean values of σsc, α, βsc, Qsc, Qsc('), σab and ω at different <span class="hlt">height</span> ranges showed that most of the parameters decreased with altitude. The forty-eight hour backward trajectories of air masses during the observation days indicated that the majority of <span class="hlt">aerosols</span> in the lower level contributed the most to the total <span class="hlt">aerosol</span> loading, and most of these particles originated from local or regional pollution emissions. Copyright © 2015. Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1424984-growth-kinetics-size-distribution-dynamics-viscous-secondary-organic-aerosol','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1424984-growth-kinetics-size-distribution-dynamics-viscous-secondary-organic-aerosol"><span>Growth Kinetics and Size Distribution Dynamics of Viscous Secondary Organic <span class="hlt">Aerosol</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zaveri, Rahul A.; Shilling, John E.; Zelenyuk, Alla; ...</p> <p>2017-12-15</p> <p>Low bulk diffusivity inside viscous semisolid atmospheric secondary organic <span class="hlt">aerosol</span> (SOA) can prolong equilibration time <span class="hlt">scale</span>, but its broader impacts on <span class="hlt">aerosol</span> growth and size distribution dynamics are poorly understood. In this article, we present quantitative insights into the effects of bulk diffusivity on the growth and evaporation kinetics of SOA formed under dry conditions from photooxidation of isoprene in the presence of a bimodal <span class="hlt">aerosol</span> consisting of Aitken (ammonium sulfate) and accumulation (isoprene or α-pinene SOA) mode particles. <span class="hlt">Aerosol</span> composition measurements and evaporation kinetics indicate that isoprene SOA is composed of several semivolatile organic compounds (SVOCs), with some reversiblymore » reacting to form oligomers. Model analysis shows that liquid-like bulk diffusivities can be used to fit the observed evaporation kinetics of accumulation mode particles but fail to explain the growth kinetics of bimodal <span class="hlt">aerosol</span> by significantly under-predicting the evolution of the Aitken mode. In contrast, the semisolid scenario successfully reproduces both evaporation and growth kinetics, with the interpretation that hindered partitioning of SVOCs into large viscous particles effectively promotes the growth of smaller particles that have shorter diffusion time <span class="hlt">scales</span>. This effect has important implications for the growth of atmospheric ultrafine particles to climatically active sizes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1424984-growth-kinetics-size-distribution-dynamics-viscous-secondary-organic-aerosol','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1424984-growth-kinetics-size-distribution-dynamics-viscous-secondary-organic-aerosol"><span>Growth Kinetics and Size Distribution Dynamics of Viscous Secondary Organic <span class="hlt">Aerosol</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>Zaveri, Rahul A.; Shilling, John E.; Zelenyuk, Alla</p> <p></p> <p>Low bulk diffusivity inside viscous semisolid atmospheric secondary organic <span class="hlt">aerosol</span> (SOA) can prolong equilibration time <span class="hlt">scale</span>, but its broader impacts on <span class="hlt">aerosol</span> growth and size distribution dynamics are poorly understood. In this article, we present quantitative insights into the effects of bulk diffusivity on the growth and evaporation kinetics of SOA formed under dry conditions from photooxidation of isoprene in the presence of a bimodal <span class="hlt">aerosol</span> consisting of Aitken (ammonium sulfate) and accumulation (isoprene or α-pinene SOA) mode particles. <span class="hlt">Aerosol</span> composition measurements and evaporation kinetics indicate that isoprene SOA is composed of several semivolatile organic compounds (SVOCs), with some reversiblymore » reacting to form oligomers. Model analysis shows that liquid-like bulk diffusivities can be used to fit the observed evaporation kinetics of accumulation mode particles but fail to explain the growth kinetics of bimodal <span class="hlt">aerosol</span> by significantly under-predicting the evolution of the Aitken mode. In contrast, the semisolid scenario successfully reproduces both evaporation and growth kinetics, with the interpretation that hindered partitioning of SVOCs into large viscous particles effectively promotes the growth of smaller particles that have shorter diffusion time <span class="hlt">scales</span>. This effect has important implications for the growth of atmospheric ultrafine particles to climatically active sizes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ACP....1614657J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ACP....1614657J"><span>Evaluation of biomass burning <span class="hlt">aerosols</span> in the HadGEM3 climate model with observations from the SAMBBA 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>Johnson, Ben T.; Haywood, James M.; Langridge, Justin M.; Darbyshire, Eoghan; Morgan, William T.; Szpek, Kate; Brooke, Jennifer K.; Marenco, Franco; Coe, Hugh; Artaxo, Paulo; Longo, Karla M.; Mulcahy, Jane P.; Mann, Graham W.; Dalvi, Mohit; Bellouin, Nicolas</p> <p>2016-11-01</p> <p>We present observations of biomass burning <span class="hlt">aerosol</span> from the South American Biomass Burning Analysis (SAMBBA) and other measurement campaigns, and use these to evaluate the representation of biomass burning <span class="hlt">aerosol</span> properties and processes in a state-of-the-art climate model. The evaluation includes detailed comparisons with aircraft and ground data, along with remote sensing observations from MODIS and AERONET. We demonstrate several improvements to <span class="hlt">aerosol</span> properties following the implementation of the Global Model for <span class="hlt">Aerosol</span> Processes (GLOMAP-mode) modal <span class="hlt">aerosol</span> scheme in the HadGEM3 climate model. This predicts the particle size distribution, composition, and optical properties, giving increased accuracy in the representation of <span class="hlt">aerosol</span> properties and physical-chemical processes over the Coupled Large-<span class="hlt">scale</span> <span class="hlt">Aerosol</span> Scheme for Simulations in Climate Models (CLASSIC) bulk <span class="hlt">aerosol</span> scheme previously used in HadGEM2. Although both models give similar regional distributions of carbonaceous <span class="hlt">aerosol</span> mass and <span class="hlt">aerosol</span> optical depth (AOD), GLOMAP-mode is better able to capture the observed size distribution, single scattering albedo, and Ångström exponent across different tropical biomass burning source regions. Both <span class="hlt">aerosol</span> schemes overestimate the uptake of water compared to recent observations, CLASSIC more so than GLOMAP-mode, leading to a likely overestimation of <span class="hlt">aerosol</span> scattering, AOD, and single scattering albedo at high relative humidity. Observed <span class="hlt">aerosol</span> vertical distributions were well captured when biomass burning <span class="hlt">aerosol</span> emissions were injected uniformly from the surface to 3 km. Finally, good agreement between observed and modelled AOD was gained only after <span class="hlt">scaling</span> up GFED3 emissions by a factor of 1.6 for CLASSIC and 2.0 for GLOMAP-mode. We attribute this difference in <span class="hlt">scaling</span> factor mainly to different assumptions for the water uptake and growth of <span class="hlt">aerosol</span> mass during ageing via oxidation and condensation of organics. We also note that similar agreement</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AMT....10.4235D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AMT....10.4235D"><span>Combined neural network/Phillips-Tikhonov approach to <span class="hlt">aerosol</span> retrievals over land from the NASA Research Scanning Polarimeter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Di Noia, Antonio; Hasekamp, Otto P.; Wu, Lianghai; van Diedenhoven, Bastiaan; Cairns, Brian; Yorks, John E.</p> <p>2017-11-01</p> <p>In this paper, an algorithm for the retrieval of <span class="hlt">aerosol</span> and land surface properties from airborne spectropolarimetric measurements - combining neural networks and an iterative scheme based on Phillips-Tikhonov regularization - is described. The algorithm - which is an extension of a scheme previously designed for ground-based retrievals - is applied to measurements from the Research Scanning Polarimeter (RSP) on board the NASA ER-2 aircraft. A neural network, trained on a large data set of synthetic measurements, is applied to perform <span class="hlt">aerosol</span> retrievals from real RSP data, and the neural network retrievals are subsequently used as a first guess for the Phillips-Tikhonov retrieval. The resulting algorithm appears capable of accurately retrieving <span class="hlt">aerosol</span> optical thickness, fine-mode effective radius and <span class="hlt">aerosol</span> layer <span class="hlt">height</span> from RSP data. Among the advantages of using a neural network as initial guess for an iterative algorithm are a decrease in processing time and an increase in the number of converging retrievals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.5648H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.5648H"><span>Long term measurements of the estimated hygroscopic enhancement of <span class="hlt">aerosol</span> optical properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hervo, Maxime; Sellegri, Karine; Pichon, Jean Marc; Roger, Jean Claude; Laj, Paolo</p> <p>2015-04-01</p> <p>Water vapour has a major impact on <span class="hlt">aerosol</span> optical properties, thus on the Radiative Forcing for <span class="hlt">aerosol</span>-radiation interaction (RFari). However there is few studies measuring this impact over a large period. Optical properties of <span class="hlt">aerosols</span> were measured at the GAW Puy de Dôme station (1465m) over a seven year period (2006-2012). The impact of hygroscopicity on <span class="hlt">aerosol</span> optical properties was calculated over a two year period (2010-2011). The analysis of the spatial and temporal variability of the dry optical properties showed that while no long term trend was found, a clear seasonal and diurnal variation was observed on the extensive parameters (scattering, absorption). Scattering and absorption coefficients were highest during the warm season and daytime, in concordance with the seasonality and diurnal variation of the planetary boundary layer <span class="hlt">height</span> reaching the site. Intensive parameters (single scattering albedo, asymmetry factor, refractive index) did not show such a strong diurnal variability, but still indicated different values depending on the season. Both extensive and intensive optical parameters were sensitive to the air mass origin. A strong impact of hygroscopicity on <span class="hlt">aerosol</span> optical properties was calculated, mainly on <span class="hlt">aerosol</span> scattering, with a dependence on the <span class="hlt">aerosol</span> type and the season. At 90% humidity, the scattering factor enhancement (fsca) was more than 4.4 for oceanic <span class="hlt">aerosol</span> that have mixed with a pollution plume. Consequently, the <span class="hlt">aerosol</span> radiative forcing was estimated to be 2.8 times higher at RH= 90% and 1.75 times higher at ambient RH when hygroscopic growth of the <span class="hlt">aerosol</span> was considered. The hygroscopicity enhancement factor of the scattering coefficient was parameterized as a function of humidity and air mass type. To our knowledge, these results are one of the first presenting the impact of water vapour on the <span class="hlt">aerosol</span> optical properties for a long period, and the first for a site at the border between the planetary boundary layer</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1712924M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1712924M"><span>LOCAL AIR: Local <span class="hlt">Aerosol</span> monitoring combining in-situ and Remote Sensing observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mona, Lucia; Caggiano, Rosa; Donvito, Angelo; Giannini, Vincenzo; Papagiannopoulos, Nikolaos; Sarli, Valentina; Trippetta, Serena</p> <p>2015-04-01</p> <p>The atmospheric <span class="hlt">aerosols</span> have effects on climate, environment and health. Although the importance of the study of <span class="hlt">aerosols</span> is well recognized, the current knowledge of the characteristics and their distribution is still insufficient, and there are large uncertainties in the current understanding of the role of <span class="hlt">aerosols</span> on climate and the environment, both on a regional and local level. Overcoming these uncertainties requires a search strategy that integrates data from multiple platforms (eg, terrestrial, satellite, ships and planes) and the different acquisition techniques (for example, in situ measurements, remote sensing, modeling numerical and data assimilation) (Yu et al., 2006). To this end, in recent years, there have been many efforts such as the creation of networks dedicated to systematic observation of <span class="hlt">aerosols</span> (eg, European Monitoring and Evaluation Programme-EMEP, European <span class="hlt">Aerosol</span> Research Lidar NETwork-EARLINET, MicroPulse Lidar Network- MPLNET, and <span class="hlt">Aerosol</span> Robotic NETwork-AERONET), the development and implementation of new satellite sensors and improvement of numerical models. The recent availability of numerous data to the ground, columnar and profiles of <span class="hlt">aerosols</span> allows to investigate these aspects. An integrated approach between these different techniques could be able to provide additional information, providing greater insight into the properties of <span class="hlt">aerosols</span> and their distribution and overcoming the limits of each single technique. In fact, the ground measurements allow direct determination of the physico-chemical properties of <span class="hlt">aerosols</span>, but cannot be considered representative for large spatial and temporal <span class="hlt">scales</span> and do not provide any information about the vertical profile of <span class="hlt">aerosols</span>. On the other hand, the remote sensing techniques from the ground and satellite provide information on the vertical distribution of atmospheric <span class="hlt">aerosols</span> both in the Planetary Boundary Layer (PBL), mainly characterized by the presence of <span class="hlt">aerosols</span> originating from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ISPAr.XL4..105J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ISPAr.XL4..105J"><span>Development of large Area Covering <span class="hlt">Height</span> Model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jacobsen, K.</p> <p>2014-04-01</p> <p><span class="hlt">Height</span> information is a basic part of topographic mapping. Only in special areas frequent update of <span class="hlt">height</span> models is required, usually the update cycle is quite lower as for horizontal map information. Some <span class="hlt">height</span> models are available free of charge in the internet; for commercial <span class="hlt">height</span> models a fee has to be paid. Mostly digital surface models (DSM) with the <span class="hlt">height</span> of the visible surface are given and not the bare ground <span class="hlt">height</span>, as required for standard mapping. Nevertheless by filtering of DSM, digital terrain models (DTM) with the <span class="hlt">height</span> of the bare ground can be generated with the exception of dense forest areas where no <span class="hlt">height</span> of the bare ground is available. These <span class="hlt">height</span> models may be better as the DTM of some survey administrations. In addition several DTM from national survey administrations are classified, so as alternative the commercial or free of charge available information from internet can be used. The widely used SRTM DSM is available also as ACE-2 GDEM corrected by altimeter data for systematic <span class="hlt">height</span> errors caused by vegetation and orientation errors. But the ACE-2 GDEM did not respect neighbourhood information. With the worldwide covering TanDEM-X <span class="hlt">height</span> model, distributed starting 2014 by Airbus Defence and Space (former ASTRIUM) as WorldDEM, higher level of details and accuracy is reached as with other large area covering <span class="hlt">height</span> models. At first the raw-version of WorldDEM will be available, followed by an edited version and finally as WorldDEM-DTM a <span class="hlt">height</span> model of the bare ground. With 12 m spacing and a relative standard deviation of 1.2 m within an area of 1° x 1° an accuracy and resolution level is reached, satisfying also for larger map <span class="hlt">scales</span>. For limited areas with the HDEM also a <span class="hlt">height</span> model with 6 m spacing and a relative vertical accuracy of 0.5 m can be generated on demand. By bathymetric LiDAR and stereo images also the <span class="hlt">height</span> of the sea floor can be determined if the water has satisfying transparency. Another method of getting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33G2470N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33G2470N"><span>Investigating the Use of a Simplified <span class="hlt">Aerosol</span> Parameterization in Space-Based XCO2 Retrievals from OCO-2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nelson, R. R.; O'Dell, C.</p> <p>2017-12-01</p> <p>The primary goal of OCO-2 is to use hyperspectral measurements of reflected near-infrared sunlight to retrieve the column-averaged dry-air mole fraction of carbon dioxide (XCO2) with high accuracy. This is only possible for measurements of scenes nearly free of optically thick clouds and <span class="hlt">aerosols</span>. As some cloud or <span class="hlt">aerosol</span> contamination will always be present, the OCO-2 retrieval algorithm includes clouds and <span class="hlt">aerosols</span> as retrieved properties in its state vector. Information content analyses demonstrate that there are only 2-6 pieces of information about <span class="hlt">aerosols</span> in the OCO-2 radiances. However, the upcoming OCO-2 algorithm (B8) attempts to retrieve 9 <span class="hlt">aerosol</span> parameters; this over-fitting can hinder convergence and produce multiple solutions. In this work, we develop a simplified cloud and <span class="hlt">aerosol</span> parameterization that intelligently reduces the number of retrieved parameters to 5 by only retrieving information about two <span class="hlt">aerosol</span> layers: a lower tropospheric layer and an upper tropospheric / stratospheric layer. We retrieve the optical depth of each layer and the <span class="hlt">height</span> of the lower tropospheric layer. Each of these layers contains a mixture of fine and coarse mode <span class="hlt">aerosol</span>. In comparisons between OCO-2 XCO2 estimates and validation sources including TCCON, this scheme performs about as well as the more complicated OCO-2 retrieval algorithm, but has the potential benefits of more interpretable <span class="hlt">aerosol</span> results, faster convergence, less nonlinearity, and greater throughput. We also investigate the dependence of our results on the optical properties of the fine and coarse mode <span class="hlt">aerosol</span> types, such as their effective radii and the environmental relative humidity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040012777&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dvertical%2Bheight','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040012777&hterms=vertical+height&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dvertical%2Bheight"><span>Observations of Dust Using the NASA Geoscience Laser Altimeter System (GLAS): New New Measurements of <span class="hlt">Aerosol</span> Vertical Distribution From Space</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Welton, Ellsworth; Spinhirne, James D.; Palm, Steven P.; Hlavka, Dennis; Hart, William</p> <p>2003-01-01</p> <p>On January 12, 2003 NASA launched the first satellite-based lidar, the Geoscience Laser -Altimeter System (GLAS), onboard the ICESat spacecraft. The GLAS atmospheric measurements introduce a fundamentally new and important tool for understanding the atmosphere and climate. In the past, <span class="hlt">aerosols</span> have only been studied from space using images gathered by passive sensors. Analysis of this passive data has lead to an improved understanding of <span class="hlt">aerosol</span> properties, spatial distribution, and their effect on the earth's climate. However, these images do not show the <span class="hlt">aerosol</span>'s vertical distribution. As a result, a key piece of information has been missing. The measurements now obtained by GLAS will provide information on the vertical distribution of <span class="hlt">aerosols</span> and clouds, and improve our ability to study their transport processes and <span class="hlt">aerosol</span>-cloud interactions. Here we show an overview of GLAS, provide an update of its current status, and present initial observations of dust profiles. In particular, a strategy of characterizing the <span class="hlt">height</span> profile of dust plumes over source regions will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.17605022M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.17605022M"><span><span class="hlt">Aerosol</span> optical properties variability during biomass burning events observed by the eole-aias depolarization lidars over Athens, Greece (2007-2016)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mylonaki, Maria; Papayannis, Alexandros; Mamouri, Rodanthi; Argyrouli, Athina; Kokkalis, Panagiotis; Tsaknakis, Georgios; Soupiona, Ourania</p> <p>2018-04-01</p> <p>The EOLE multi-wavelength <span class="hlt">aerosol</span> Ramandepolarization lidar, and the AIAS depolarization lidar, in synergy with a sun photometer (CIMEL), were used, in the period 2007-2016, to provide the vertical profiles of the <span class="hlt">aerosol</span> optical properties over Athens, Greece. More than 30 biomass burning events (fresh and aged smoke particles) were observed, with smoke layers between 1.5 up to 4-5 km <span class="hlt">height</span>, while their duration ranged from 1-3 days. Lidar ratio (LR) values ranged from 40-105 sr (at 355 nm) and from 40-100 sr (at 532 nm), while the linear particle depolarization ratio (LPDR) at both 355 and 532 nm, remained <7%. The extinction-related Ångström exponent (AEa) at 355 nm/532 nm) ranged from 0.3 to 2.1. Additionally, a case of a near-range transport of biomass burning <span class="hlt">aerosols</span> arriving over Athens up to 4 km <span class="hlt">height</span>, between 27 and 28 June 2016, was studied. For this case, we found LRs of the order of 70±5 sr (355 nm) and 65±15 sr (532 nm) and AEa(355 nm/532 nm) around 1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3331822','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3331822"><span>Cough <span class="hlt">aerosol</span> in healthy participants: fundamental knowledge to optimize droplet-spread infectious respiratory disease management</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>2012-01-01</p> <p>Background The Influenza A H1N1 virus can be transmitted via direct, indirect, and airborne route to non-infected subjects when an infected patient coughs, which expels a number of different sized droplets to the surrounding environment as an <span class="hlt">aerosol</span>. The objective of the current study was to characterize the human cough <span class="hlt">aerosol</span> pattern with the aim of developing a standard human cough bioaerosol model for Influenza Pandemic control. Method 45 healthy non-smokers participated in the open bench study by giving their best effort cough. A laser diffraction system was used to obtain accurate, time-dependent, quantitative measurements of the size and number of droplets expelled by the cough <span class="hlt">aerosol</span>. Results Voluntary coughs generated droplets ranging from 0.1 - 900 microns in size. Droplets of less than one-micron size represent 97% of the total number of measured droplets contained in the cough <span class="hlt">aerosol</span>. Age, sex, weight, <span class="hlt">height</span> and corporal mass have no statistically significant effect on the <span class="hlt">aerosol</span> composition in terms of size and number of droplets. Conclusions We have developed a standard human cough <span class="hlt">aerosol</span> model. We have quantitatively characterized the pattern, size, and number of droplets present in the most important mode of person-to-person transmission of IRD: the cough bioaerosol. Small size droplets (< 1 μm) predominated the total number of droplets expelled when coughing. The cough <span class="hlt">aerosol</span> is the single source of direct, indirect and/or airborne transmission of respiratory infections like the Influenza A H1N1 virus. Study design Open bench, Observational, Cough, <span class="hlt">Aerosol</span> study PMID:22436202</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22436202','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22436202"><span>Cough <span class="hlt">aerosol</span> in healthy participants: fundamental knowledge to optimize droplet-spread infectious respiratory disease management.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zayas, Gustavo; Chiang, Ming C; Wong, Eric; MacDonald, Fred; Lange, Carlos F; Senthilselvan, Ambikaipakan; King, Malcolm</p> <p>2012-03-21</p> <p>The Influenza A H1N1 virus can be transmitted via direct, indirect, and airborne route to non-infected subjects when an infected patient coughs, which expels a number of different sized droplets to the surrounding environment as an <span class="hlt">aerosol</span>. The objective of the current study was to characterize the human cough <span class="hlt">aerosol</span> pattern with the aim of developing a standard human cough bioaerosol model for Influenza Pandemic control. 45 healthy non-smokers participated in the open bench study by giving their best effort cough. A laser diffraction system was used to obtain accurate, time-dependent, quantitative measurements of the size and number of droplets expelled by the cough <span class="hlt">aerosol</span>. Voluntary coughs generated droplets ranging from 0.1 - 900 microns in size. Droplets of less than one-micron size represent 97% of the total number of measured droplets contained in the cough <span class="hlt">aerosol</span>. Age, sex, weight, <span class="hlt">height</span> and corporal mass have no statistically significant effect on the <span class="hlt">aerosol</span> composition in terms of size and number of droplets. We have developed a standard human cough <span class="hlt">aerosol</span> model. We have quantitatively characterized the pattern, size, and number of droplets present in the most important mode of person-to-person transmission of IRD: the cough bioaerosol. Small size droplets (< 1 μm) predominated the total number of droplets expelled when coughing. The cough <span class="hlt">aerosol</span> is the single source of direct, indirect and/or airborne transmission of respiratory infections like the Influenza A H1N1 virus. Open bench, Observational, Cough, <span class="hlt">Aerosol</span> study. © 2012 Zayas et al; licensee BioMed Central Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33E2403B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33E2403B"><span>Impacts of East Asian Sulfate <span class="hlt">Aerosols</span> on Local and Remote Climate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bartlett, R. E.; Bollasina, M. A.</p> <p>2017-12-01</p> <p>Anthropogenic <span class="hlt">aerosols</span> exert significant climate forcing, which increases with emissions following trends of growing population and industry. Globally, <span class="hlt">aerosols</span> cause a net cooling, counteracting greenhouse gas warming; however, regional impacts vary since emissions are spatially and temporally heterogeneous. While European and North American emissions have decreased in recent decades, Asian, particularly East Asian, emissions continued to rise into the 21st century. In addition to links between Asian anthropogenic <span class="hlt">aerosols</span> and significant local climate impacts - for example, changes to the Asian monsoon system - studies have also shown influences on remote climate. Sulfate <span class="hlt">aerosols</span> are particularly important for East Asia, remaining at constant levels higher than column burdens of other <span class="hlt">aerosol</span> species. If a concerted effort - as laid out by government policies aiming to improve air quality - is made, the effects of anthropogenic <span class="hlt">aerosols</span> (due to their short atmospheric lifetime) could be quickly reversed. Thus, it is vital to understand the climate impact <span class="hlt">aerosols</span> have had up to now to aid in determining what will happen in the future. We use transient climate modelling experiments with the Community Earth System Model to investigate the impacts of East Asian sulfate <span class="hlt">aerosols</span> in the present day compared to 1950 (i.e. before rapid industrialisation in this region), focusing on dynamical mechanisms leading to the occurrence of such impacts, and how their influence can spread to remote regions. We find, in addition to significant monsoon impacts, noticeable shifts in large-<span class="hlt">scale</span> circulation features such as the ITCZ and the Pacific Walker cell. Through diabatic heating responses, changes to upper-level atmospheric dynamics are evident, leading to downstream effects on surface climate - for example, surface cooling over Europe. Understanding of these impacts is vital when considering how the good intentions of air quality improvement might inadvertently have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5714M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5714M"><span>Regional variation of carbonaceous <span class="hlt">aerosols</span> from space and simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukai, Sonoyo; Sano, Itaru; Nakata, Makiko; Kokhanovsky, Alexander</p> <p>2017-04-01</p> <p>Satellite remote sensing provides us with a systematic monitoring in a global <span class="hlt">scale</span>. As such, <span class="hlt">aerosol</span> observation via satellites is known to be useful and effective. However, before attempting to retrieve <span class="hlt">aerosol</span> properties from satellite data, the efficient algorithms for <span class="hlt">aerosol</span> retrieval need to be considered. The characteristics and distributions of atmospheric <span class="hlt">aerosols</span> are known to be complicated, owing to both natural factors and human activities. It is known that the biomass burning <span class="hlt">aerosols</span> generated by the large-<span class="hlt">scale</span> forest fires and burn agriculture have influenced the severity of air pollution. Nevertheless the biomass burning episodes increase due to global warming and climate change and vice versa. It is worth noting that the near ultra violet (NUV) measurements are helpful for the detection of carbonaceous particles, which are the main component of <span class="hlt">aerosols</span> from biomass burning. In this work, improved retrieval algorithms for biomass burning <span class="hlt">aerosols</span> are shown by using the measurements observed by GLI and POLDER-2 on Japanese short term mission ADEOS-2 in 2003. The GLI sensor has 380nm channel. For detection of biomass burning episodes, the <span class="hlt">aerosol</span> optical thickness of carbonaceous <span class="hlt">aerosols</span> simulated with the numerical model simulations (SPRINTARS) is available as well as fire products from satellite imagery. Moreover the algorithm using shorter wavelength data is available for detection of absorbing <span class="hlt">aerosols</span>. An algorithm based on the combined use of near-UV and violet data has been introduced in our previous work with ADEOS (Advanced Earth Observing Satellite) -2 /GLI measurements [1]. It is well known that biomass burning plume is a seasonal phenomenon peculiar to a particular region. Hence, the mass concentrations of <span class="hlt">aerosols</span> are frequently governed with spatial and/or temporal variations of biomass burning plumes. Accordingly the satellite data sets for our present study are adopted from the view points of investigation of regional and seasonal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1052947-impact-natural-anthropogenic-aerosols-stratocumulus-precipitation-southeast-pacific-regional-modelling-study-using-wrf-chem','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1052947-impact-natural-anthropogenic-aerosols-stratocumulus-precipitation-southeast-pacific-regional-modelling-study-using-wrf-chem"><span>Impact of natural and anthropogenic <span class="hlt">aerosols</span> on stratocumulus and precipitation in the Southeast Pacific: a regional modelling study using WRF-Chem</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>Yang, Q.; Gustafson, W. I.; Fast, J. D.</p> <p>2012-09-28</p> <p>Cloud-system resolving simulations with the chemistry version of the Weather Research and Forecasting (WRF-Chem) model are used to quantify the relative impacts of regional anthropogenic and oceanic emissions on changes in <span class="hlt">aerosol</span> properties, cloud macro- and microphysics, and cloud radiative forcing over the Southeast Pacific (SEP) during the VAMOS Ocean-Cloud-Atmosphere-Land Study Regional Experiment (VOCALS-REx) (15 October–16 November 2008). Two distinct regions are identified. The near-coast polluted region is characterized by low surface precipitation rates, the strong suppression of non-sea-salt particle activation due to sea-salt particles, a predominant albedo effect in <span class="hlt">aerosol</span> indirect effects, and limited impact of <span class="hlt">aerosols</span> associated withmore » anthropogenic emissions on clouds. Opposite sensitivities to natural marine and anthropogenic <span class="hlt">aerosol</span> perturbations are seen in cloud properties (e.g., cloud optical depth and cloud-top and cloud-base <span class="hlt">heights</span>), precipitation, and the top-of-atmosphere and surface shortwave fluxes over this region. The relatively clean remote region is characterized by large contributions of <span class="hlt">aerosols</span> from non-regional sources (lateral boundaries) and much stronger drizzle at the surface. Under a scenario of five-fold increase in regional anthropogenic emissions, this relatively clean region shows large cloud responses, for example, a 13% increase in cloud-top <span class="hlt">height</span> and a 9% increase in albedo in response to a moderate increase (25% of the reference case) in cloud condensation nuclei (CCN) concentration. The reduction of precipitation due to this increase in anthropogenic <span class="hlt">aerosols</span> more than doubles the <span class="hlt">aerosol</span> lifetime in the clean marine boundary layer. Therefore, the <span class="hlt">aerosol</span> impacts on precipitation are amplified by the positive feedback of precipitation on <span class="hlt">aerosol</span>, which ultimately alters the cloud micro- and macro-physical properties, leading to strong <span class="hlt">aerosol</span>-cloud-precipitation interactions. The high sensitivity is also</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A33C3201K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A33C3201K"><span>The Effect of <span class="hlt">Aerosol</span> Hygroscopicity and Volatility on <span class="hlt">Aerosol</span> Optical Properties During Southern Oxidant and <span class="hlt">Aerosol</span> Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khlystov, A.; Grieshop, A. P.; Saha, P.; Subramanian, R.</p> <p>2014-12-01</p> <p>Secondary organic <span class="hlt">aerosol</span> (SOA) from biogenic sources can influence optical properties of ambient <span class="hlt">aerosol</span> by altering its hygroscopicity and contributing to light absorption directly via formation of brown carbon and indirectly by enhancing light absorption by black carbon ("lensing effect"). The magnitude of these effects remains highly uncertain. A set of state-of-the-art instruments was deployed at the SEARCH site near Centerville, AL during the Southern Oxidant and <span class="hlt">Aerosol</span> Study (SOAS) campaign in summer 2013 to measure the effect of relative humidity and temperature on <span class="hlt">aerosol</span> size distribution, composition and optical properties. Light scattering and absorption by temperature- and humidity-conditioned <span class="hlt">aerosols</span> was measured using three photo-acoustic extinctiometers (PAX) at three wavelengths (405 nm, 532 nm, and 870 nm). The sample-conditioning system provided measurements at ambient RH, 10%RH ("dry"), 85%RH ("wet"), and 200 C ("TD"). In parallel to these measurements, a long residence time temperature-stepping thermodenuder (TD) and a variable residence time constant temperature TD in combination with three SMPS systems and an <span class="hlt">Aerosol</span> Chemical Speciation Monitor (ACSM) were used to assess <span class="hlt">aerosol</span> volatility and kinetics of <span class="hlt">aerosol</span> evaporation. We will present results of the on-going analysis of the collected data set. We will show that both temperature and relative humidity have a strong effect on <span class="hlt">aerosol</span> optical properties. SOA appears to increase <span class="hlt">aerosol</span> light absorption by about 10%. TD measurements suggest that <span class="hlt">aerosol</span> equilibrated fairly quickly, within 2 s. Evaporation varied substantially with ambient <span class="hlt">aerosol</span> loading and composition and meteorology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1240299-characteristics-aerosol-indirect-effect-based-dynamic-regimes-global-climate-models','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1240299-characteristics-aerosol-indirect-effect-based-dynamic-regimes-global-climate-models"><span>On the characteristics of <span class="hlt">aerosol</span> indirect effect based on dynamic regimes in global climate models</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhang, Shipeng; Wang, Minghuai; Ghan, Steven J.; ...</p> <p>2016-03-04</p> <p>Aerosol–cloud interactions continue to constitute a major source of uncertainty for the estimate of climate radiative forcing. The variation of <span class="hlt">aerosol</span> indirect effects (AIE) in climate models is investigated across different dynamical regimes, determined by monthly mean 500 hPa vertical pressure velocity ( ω 500), lower-tropospheric stability (LTS) and large-<span class="hlt">scale</span> surface precipitation rate derived from several global climate models (GCMs), with a focus on liquid water path (LWP) response to cloud condensation nuclei (CCN) concentrations. The LWP sensitivity to <span class="hlt">aerosol</span> perturbation within dynamic regimes is found to exhibit a large spread among these GCMs. It is in regimes of strongmore » large-<span class="hlt">scale</span> ascent ( ω 500  <  −25 hPa day −1) and low clouds (stratocumulus and trade wind cumulus) where the models differ most. Shortwave <span class="hlt">aerosol</span> indirect forcing is also found to differ significantly among different regimes. Shortwave <span class="hlt">aerosol</span> indirect forcing in ascending regimes is close to that in subsidence regimes, which indicates that regimes with strong large-<span class="hlt">scale</span> ascent are as important as stratocumulus regimes in studying AIE. It is further shown that shortwave <span class="hlt">aerosol</span> indirect forcing over regions with high monthly large-<span class="hlt">scale</span> surface precipitation rate (> 0.1 mm day −1) contributes the most to the total <span class="hlt">aerosol</span> indirect forcing (from 64 to nearly 100 %). Results show that the uncertainty in AIE is even larger within specific dynamical regimes compared to the uncertainty in its global mean values, pointing to the need to reduce the uncertainty in AIE in different dynamical regimes.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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://hdl.handle.net/2060/20120008717','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120008717"><span>Using Satellite <span class="hlt">Aerosol</span> Retrievals to Monitor Surface Particulate Air Quality</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levy, Robert C.; Remer, Lorraine A.; Kahn, Ralph A.; Chu, D. Allen; Mattoo, Shana; Holben, Brent N.; Schafer, Joel S.</p> <p>2011-01-01</p> <p>The MODIS and MISR <span class="hlt">aerosol</span> products were designed nearly two decades ago for the purpose of climate applications. Since launch of Terra in 1999, these two sensors have provided global, quantitative information about column-integrated <span class="hlt">aerosol</span> properties, including <span class="hlt">aerosol</span> optical depth (AOD) and relative <span class="hlt">aerosol</span> type parameters (such as Angstrom exponent). Although primarily designed for climate, the air quality (AQ) community quickly recognized that passive satellite products could be used for particulate air quality monitoring and forecasting. However, AOD and particulate matter (PM) concentrations have different units, and represent <span class="hlt">aerosol</span> conditions in different layers of the atmosphere. Also, due to low visible contrast over brighter surface conditions, satellite-derived <span class="hlt">aerosol</span> retrievals tend to have larger uncertainty in urban or populated regions. Nonetheless, the AQ community has made significant progress in relating column-integrated AOD at ambient relative humidity (RH) to surface PM concentrations at dried RH. Knowledge of <span class="hlt">aerosol</span> optical and microphysical properties, ambient meteorological conditions, and especially vertical profile, are critical for physically relating AOD and PM. To make urban-<span class="hlt">scale</span> maps of PM, we also must account for spatial variability. Since surface PM may vary on a finer spatial <span class="hlt">scale</span> than the resolution of standard MODIS (10 km) and MISR (17km) products, we test higher-resolution versions of MODIS (3km) and MISR (1km research mode) retrievals. The recent (July 2011) DISCOVER-AQ campaign in the mid-Atlantic offers a comprehensive network of sun photometers (DRAGON) and other data that we use for validating the higher resolution satellite data. In the future, we expect that the wealth of aircraft and ground-based measurements, collected during DISCOVER-AQ, will help us quantitatively link remote sensed and ground-based measurements in the urban region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017664','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017664"><span>Sources, Sinks, and Transatlantic Transport of North African Dust <span class="hlt">Aerosol</span>: A Multimodel Analysis and Comparison With Remote Sensing Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, Dongchul; Chin, Mian; Yu, Hongbin; Diehl, Thomas; Tan, Qian; Kahn, Ralph A.; Tsigaridis, Kostas; Bauer, Susanne E.; Takemura, Toshihiko; Pozzoli, Luca; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140017664'); toggleEditAbsImage('author_20140017664_show'); toggleEditAbsImage('author_20140017664_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140017664_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140017664_hide"></p> <p>2014-01-01</p> <p>This study evaluates model-simulated dust <span class="hlt">aerosols</span> over North Africa and the North Atlantic from five global models that participated in the <span class="hlt">Aerosol</span> Comparison between Observations and Models phase II model experiments. The model results are compared with satellite <span class="hlt">aerosol</span> optical depth (AOD) data from Moderate Resolution Imaging Spectroradiometer (MODIS), Multiangle Imaging Spectroradiometer (MISR), and Sea-viewing Wide Field-of-view Sensor, dust optical depth (DOD) derived from MODIS and MISR, AOD and coarse-mode AOD (as a proxy of DOD) from ground-based <span class="hlt">Aerosol</span> Robotic Network Sun photometer measurements, and dust vertical distributions/centroid <span class="hlt">height</span> from Cloud <span class="hlt">Aerosol</span> Lidar with Orthogonal Polarization and Atmospheric Infrared Sounder satellite AOD retrievals. We examine the following quantities of AOD and DOD: (1) the magnitudes over land and over ocean in our study domain, (2) the longitudinal gradient from the dust source region over North Africa to the western North Atlantic, (3) seasonal variations at different locations, and (4) the dust vertical profile shape and the AOD centroid <span class="hlt">height</span> (altitude above or below which half of the AOD is located). The different satellite data show consistent features in most of these aspects; however, the models display large diversity in all of them, with significant differences among the models and between models and observations. By examining dust emission, removal, and mass extinction efficiency in the five models, we also find remarkable differences among the models that all contribute to the discrepancies of model-simulated dust amount and distribution. This study highlights the challenges in simulating the dust physical and optical processes, even in the best known dust environment, and stresses the need for observable quantities to constrain the model processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1440889-field-evidences-positive-effects-aerosols-tree-growth','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1440889-field-evidences-positive-effects-aerosols-tree-growth"><span>Field evidences for the positive effects of <span class="hlt">aerosols</span> on tree growth</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>Wang, Xin; Wu, Jin; Chen, Min</p> <p></p> <p>Theoretical and eddy-covariance studies demonstrate that <span class="hlt">aerosol</span>-loading stimulates canopy photosynthesis, but field evidence for the <span class="hlt">aerosol</span> effect on tree growth is limited. For this study, we measured in-situ daily stem growth rates of aspen trees under a wide range of <span class="hlt">aerosol</span>-loading in China. The results showed that daily stem growth rates were positively correlated with <span class="hlt">aerosol</span>-loading, even at exceptionally high <span class="hlt">aerosol</span> levels. Using structural equation modelling analysis, we showed that variations in stem growth rates can be largely attributed to two environmental variables co-varying with <span class="hlt">aerosol</span> loading: diffuse fraction of radiation and vapor pressure deficit (VPD). Furthermore, we found thatmore » these two factors influence stem growth by influencing photosynthesis from different parts of canopy. By using field observations and a mechanistic photosynthesis model, we demonstrate that photosynthetic rates of both sun and shade leaves increased under high <span class="hlt">aerosol</span>-loading conditions but for different reasons. For sun leaves, the photosynthetic increase was primarily attributed to the concurrent lower VPD; for shade leaves, the positive <span class="hlt">aerosol</span> effect was tightly connected with increased diffuse light. Overall, our study provides the first field-evidence of increased tree growth under high <span class="hlt">aerosol</span> loading. We highlight the importance of understanding biophysical mechanisms of <span class="hlt">aerosol</span>-meteorology interactions, and incorporating the different pathways of <span class="hlt">aerosol</span> effects into earth system models to improve the prediction of large-<span class="hlt">scale</span> <span class="hlt">aerosol</span> impacts, and the associated vegetation-mediated climate feedbacks.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1440889-field-evidences-positive-effects-aerosols-tree-growth','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1440889-field-evidences-positive-effects-aerosols-tree-growth"><span>Field evidences for the positive effects of <span class="hlt">aerosols</span> on tree growth</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wang, Xin; Wu, Jin; Chen, Min; ...</p> <p>2018-06-01</p> <p>Theoretical and eddy-covariance studies demonstrate that <span class="hlt">aerosol</span>-loading stimulates canopy photosynthesis, but field evidence for the <span class="hlt">aerosol</span> effect on tree growth is limited. For this study, we measured in-situ daily stem growth rates of aspen trees under a wide range of <span class="hlt">aerosol</span>-loading in China. The results showed that daily stem growth rates were positively correlated with <span class="hlt">aerosol</span>-loading, even at exceptionally high <span class="hlt">aerosol</span> levels. Using structural equation modelling analysis, we showed that variations in stem growth rates can be largely attributed to two environmental variables co-varying with <span class="hlt">aerosol</span> loading: diffuse fraction of radiation and vapor pressure deficit (VPD). Furthermore, we found thatmore » these two factors influence stem growth by influencing photosynthesis from different parts of canopy. By using field observations and a mechanistic photosynthesis model, we demonstrate that photosynthetic rates of both sun and shade leaves increased under high <span class="hlt">aerosol</span>-loading conditions but for different reasons. For sun leaves, the photosynthetic increase was primarily attributed to the concurrent lower VPD; for shade leaves, the positive <span class="hlt">aerosol</span> effect was tightly connected with increased diffuse light. Overall, our study provides the first field-evidence of increased tree growth under high <span class="hlt">aerosol</span> loading. We highlight the importance of understanding biophysical mechanisms of <span class="hlt">aerosol</span>-meteorology interactions, and incorporating the different pathways of <span class="hlt">aerosol</span> effects into earth system models to improve the prediction of large-<span class="hlt">scale</span> <span class="hlt">aerosol</span> impacts, and the associated vegetation-mediated climate feedbacks.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15504519','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15504519"><span>Street canyon <span class="hlt">aerosol</span> pollutant transport measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Longley, I D; Gallagher, M W; Dorsey, J R; Flynn, M; Bower, K N; Allan, J D</p> <p>2004-12-01</p> <p>Current understanding of dispersion in street canyons is largely derived from relatively simple dispersion models. Such models are increasingly used in planning and regulation capacities but are based upon a limited understanding of the transport of substances within a real canyon. In recent years, some efforts have been made to numerically model localised flow in idealised canyons (e.g., J. Appl. Meteorol. 38 (1999) 1576-89) and stepped canyons (Assimakopoulos V. Numerical modelling of dispersion of atmospheric pollution in and above urban canopies. PhD thesis, Imperial College, London, 2001) but field studies in real canyons are rare. To further such an understanding, a measurement campaign has been conducted in an asymmetric street canyon with busy one-way traffic in central Manchester in northern England. The eddy correlation method was used to determine fluxes of size-segregated accumulation mode <span class="hlt">aerosol</span>. Measurements of <span class="hlt">aerosol</span> at a static location were made concurrently with measurements on a platform lift giving vertical profiles. Size-segregated measurements of ultrafine and coarse particle concentrations were also made simultaneously at various <span class="hlt">heights</span>. In addition, a small mobile system was used to make measurements of turbulence at various pavement locations within the canyon. From this data, various features of turbulent transport and dispersion in the canyon will be presented. The concentration and the ventilation fluxes of vehicle-related <span class="hlt">aerosol</span> pollutants from the canyon will be related to controlling factors. The results will also be compared with citywide ventilation data from a separate measurement campaign conducted above the urban canopy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26831092','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26831092"><span>New approaches to quantifying <span class="hlt">aerosol</span> influence on the cloud radiative effect.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Feingold, Graham; McComiskey, Allison; Yamaguchi, Takanobu; Johnson, Jill S; Carslaw, Kenneth S; Schmidt, K Sebastian</p> <p>2016-05-24</p> <p>The topic of cloud radiative forcing associated with the atmospheric <span class="hlt">aerosol</span> has been the focus of intense scrutiny for decades. The enormity of the problem is reflected in the need to understand aspects such as <span class="hlt">aerosol</span> composition, optical properties, cloud condensation, and ice nucleation potential, along with the global distribution of these properties, controlled by emissions, transport, transformation, and sinks. Equally daunting is that clouds themselves are complex, turbulent, microphysical entities and, by their very nature, ephemeral and hard to predict. Atmospheric general circulation models represent <span class="hlt">aerosol</span>-cloud interactions at ever-increasing levels of detail, but these models lack the resolution to represent clouds and <span class="hlt">aerosol</span>-cloud interactions adequately. There is a dearth of observational constraints on <span class="hlt">aerosol</span>-cloud interactions. We develop a conceptual approach to systematically constrain the <span class="hlt">aerosol</span>-cloud radiative effect in shallow clouds through a combination of routine process modeling and satellite and surface-based shortwave radiation measurements. We heed the call to merge Darwinian and Newtonian strategies by balancing microphysical detail with <span class="hlt">scaling</span> and emergent properties of the <span class="hlt">aerosol</span>-cloud radiation system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1097441','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1097441"><span>Final Report: Process Models of the Equilibrium Size & State of Organic/Inorganic <span class="hlt">Aerosols</span> for the Development of Large <span class="hlt">Scale</span> Atmospheric Models & the Analysis of Field Data</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>Wexler, Anthony Stein; Clegg, Simon Leslie</p> <p>2013-10-26</p> <p>Our work addressed the following elements of the Call for Proposals: (i) “to improve the theoretical representation of <span class="hlt">aerosol</span> processes studied in ASP laboratory or field studies”, (ii) “to enhance the incorporation of <span class="hlt">aerosol</span> process information into modules suitable for large-<span class="hlt">scale</span> or global atmospheric models”, and (iii) “provide systematic experimental validation of process model predictions ... using data from targeted laboratory and field experiments”. Achievements to the end of 2012 are described in four previous reports, and include: new models of densities and surface tensions of pure (single solute) and mixed aqueous solutions of typical <span class="hlt">aerosol</span> composition under all atmosphericmore » conditions (0 to 100% RH and T > 150 K); inclusion of these models into the widely used Extended <span class="hlt">Aerosol</span> Inorganics model (E-AIM, http://www.aim.env.uea.ac.uk/aim/aim.php); the addition of vapor pressure calculators for organic compounds to the E-AIM website; the ability of include user-defined organic compounds and/or lumped surrogates in gas/<span class="hlt">aerosol</span> partitioning calculations; the development of new equations to represent the properties of soluble <span class="hlt">aerosols</span> over the entire concentration range (using methods based upon adsorption isotherms, and derived using statistical mechanics), including systems at close to zero RH. These results are described in publications 1-6 at the end of this report, and on the “News” page of the E-AIM website (http://www.aim.env.uea.ac.uk/aim/info/news.html). During 2012 and 2013 we have collaborated in a combined observation and lab-based study of the water uptake of the organic component of atmospheric <span class="hlt">aerosols</span> (PI Gannet Hallar, of the Desert Research Institute). The <span class="hlt">aerosol</span> samples were analyzed using several complementary techniques (GC/MS, FT-ICR MS, and ion chromatography) to produce a very complete organic “speciation” including both polar and non-polar compounds. Hygroscopic growth factors of the samples were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008073','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008073"><span>Influence of <span class="hlt">Aerosol</span> Heating on the Stratospheric Transport of the Mt. Pinatubo Eruption</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Aquila, Valentina; Oman, Luke D.; Stolarski, Richard S.</p> <p>2011-01-01</p> <p>On June 15th, 1991 the eruption of Mt. Pinatubo (15.1 deg. N, 120.3 Deg. E) in the Philippines injected about 20 Tg of sulfur dioxide in the stratosphere, which was transformed into sulfuric acid <span class="hlt">aerosol</span>. The large perturbation of the background <span class="hlt">aerosol</span> caused an increase in temperature in the lower stratosphere of 2-3 K. Even though stratospheric winds climatological]y tend to hinder the air mixing between the two hemispheres, observations have shown that a large part of the SO2 emitted by Mt. Pinatubo have been transported from the Northern to the Southern Hemisphere. We simulate the eruption of Mt. Pinatubo with the Goddard Earth Observing System (GEOS) version 5 global climate model, coupled to the <span class="hlt">aerosol</span> module GOCART and the stratospheric chemistry module StratChem, to investigate the influence of the eruption of Mt. Pinatubo on the stratospheric transport pattern. We perform two ensembles of simulations: the first ensemble consists of runs without coupling between <span class="hlt">aerosol</span> and radiation. In these simulations the plume of <span class="hlt">aerosols</span> is treated as a passive tracer and the atmosphere is unperturbed. In the second ensemble of simulations <span class="hlt">aerosols</span> and radiation are coupled. We show that the set of runs with interactive <span class="hlt">aerosol</span> produces a larger cross-equatorial transport of the Pinatubo cloud. In our simulations the local heating perturbation caused by the sudden injection of volcanic <span class="hlt">aerosol</span> changes the pattern of the stratospheric winds causing more intrusion of air from the Northern into the Southern Hemisphere. Furthermore, we perform simulations changing the injection <span class="hlt">height</span> of the cloud, and study the transport of the plume resulting from the different scenarios. Comparisons of model results with SAGE II and AVHRR satellite observations will be shown.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18608473','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18608473"><span>Modelling foot <span class="hlt">height</span> and foot shape-related dimensions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xiong, Shuping; Goonetilleke, Ravindra S; Witana, Channa P; Lee Au, Emily Yim</p> <p>2008-08-01</p> <p>The application of foot anthropometry to design good-fitting footwear has been difficult due to the lack of generalised models. This study seeks to model foot dimensions so that the characteristic shapes of feet, especially in the midfoot region, can be understood. Fifty Hong Kong Chinese adults (26 males and 24 females) participated in this study. Their foot lengths, foot widths, ball girths and foot <span class="hlt">heights</span> were measured and then evaluated using mathematical models. The results showed that there were no significant allometry (p > 0.05) effects of foot length on ball girth and foot width. Foot <span class="hlt">height</span> showed no direct relationship with foot length. However, a normalisation with respect to foot length and foot <span class="hlt">height</span> resulted in a significant relationship for both males and females with R(2) greater than 0.97. Due to the lack of a direct relationship between foot <span class="hlt">height</span> and foot length, the current practice of grading shoes with a constant increase in <span class="hlt">height</span> or proportionate <span class="hlt">scaling</span> in response to foot length is less than ideal. The results when validated with other populations can be a significant way forward in the design of footwear that has an improved fit in the <span class="hlt">height</span> dimension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=336006&keyword=air&subject=air%20research&showcriteria=2&fed_org_id=111&datebeginpublishedpresented=04/05/2012&dateendpublishedpresented=04/05/2017&sortby=pubdateyear','PESTICIDES'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?direntryid=336006&keyword=air&subject=air%20research&showcriteria=2&fed_org_id=111&datebeginpublishedpresented=04/05/2012&dateendpublishedpresented=04/05/2017&sortby=pubdateyear"><span>Does temperature nudging overwhelm <span class="hlt">aerosol</span> radiative ...</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>For over two decades, data assimilation (popularly known as nudging) methods have been used for improving regional weather and climate simulations by reducing model biases in meteorological parameters and processes. Similar practice is also popular in many regional integrated meteorology-air quality models that include <span class="hlt">aerosol</span> direct and indirect effects. However in such multi-modeling systems, temperature changes due to nudging can compete with temperature changes induced by radiatively active & hygroscopic short-lived tracers leading to interesting dilemmas: From weather and climate prediction’s (retrospective or future) point of view when nudging is continuously applied, is there any real added benefit of using such complex and computationally expensive regional integrated modeling systems? What are the relative sizes of these two competing forces? To address these intriguing questions, we convert temperature changes due to nudging into radiative fluxes (referred to as the pseudo radiative forcing, PRF) at the surface and troposphere, and compare the net PRF with the reported <span class="hlt">aerosol</span> radiative forcing. Results indicate that the PRF at surface dominates PRF at top of the atmosphere (i.e., the net). Also, the net PRF is about 2-4 times larger than estimated <span class="hlt">aerosol</span> radiative forcing at regional <span class="hlt">scales</span> while it is significantly larger at local <span class="hlt">scales</span>. These results also show large surface forcing errors at many polluted urban sites. Thus, operational c</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A53C0293L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A53C0293L"><span>Constructing An Event Based <span class="hlt">Aerosol</span> Product Under High <span class="hlt">Aerosol</span> Loading Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levy, R. C.; Shi, Y.; Mattoo, S.; Remer, L. A.; Zhang, J.</p> <p>2016-12-01</p> <p>High <span class="hlt">aerosol</span> loading events, such as the Indonesia's forest fire in Fall 2015 or the persistent wintertime haze near Beijing, gain tremendous interests due to their large impact on regional visibility and air quality. Understanding the optical properties of these events and further being able to simulate and predict these events are beneficial. However, it is a great challenge to consistently identify and then retrieve <span class="hlt">aerosol</span> optical depth (AOD) from passive sensors during heavy <span class="hlt">aerosol</span> events. Some reasons include:1). large differences between optical properties of high-loading <span class="hlt">aerosols</span> and those under normal conditions, 2) spectral signals of optically thick <span class="hlt">aerosols</span> can be mistaken with surface depending on <span class="hlt">aerosol</span> types, and 3) Extremely optically thick <span class="hlt">aerosol</span> plumes can also be misidentified as clouds due to its high optical thickness. Thus, even under clear-sky conditions, the global distribution of extreme <span class="hlt">aerosol</span> events is not well captured in datasets such as the MODIS Dark-Target (DT) <span class="hlt">aerosol</span> product. In this study, with the synthetic use of OMI <span class="hlt">Aerosol</span> Index, MODIS cloud product, and operational DT product, the heavy smoke events over the seven sea region are identified and retrieved over the dry season. An event based <span class="hlt">aerosol</span> product that would compensate the standard "global" <span class="hlt">aerosol</span> retrieval will be created and evaluated. The impact of missing high AOD retrievals on the regional <span class="hlt">aerosol</span> climatology will be studied using this newly developed research product.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/439','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/439"><span>Comparisons of modeled <span class="hlt">height</span> predictions to ocular <span class="hlt">height</span> estimates</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>W.A. Bechtold; S.J. Zarnoch; W.G. Burkman</p> <p>1998-01-01</p> <p>Equations used by USDA Forest Service Forest Inventory and Analysis projects to predict individual tree <span class="hlt">heights</span> on the basis of species and d.b.h. were improved by the addition of mean overstory <span class="hlt">height</span>. However, ocular estimates of total <span class="hlt">height</span> by field crews were more accurate than the statistically improved models, especially for hardwood species. <span class="hlt">Height</span> predictions...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A52H..07Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A52H..07Z"><span>Direct Observations of Isoprene Secondary Organic <span class="hlt">Aerosol</span> Formation in Ambient Cloud Droplets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zelenyuk, A.; Bell, D.; Thornton, J. A.; Fast, J. D.; Shrivastava, M. B.; Berg, L. K.; Imre, D. G.; Mei, F.; Shilling, J.; Suski, K. J.; Liu, J.; Tomlinson, J. M.; Wang, J.</p> <p>2017-12-01</p> <p>Multiphase chemistry of isoprene photooxidation products has been shown to be one of the major sources of secondary organic <span class="hlt">aerosol</span> (SOA) in the atmosphere. A number of recent studies indicate that aqueous <span class="hlt">aerosol</span> phase provides a medium for reactive uptake of isoprene photooxidation products, and in particular, isomeric isoprene epoxydiols (IEPOX), with reaction rates and yields being dependent on <span class="hlt">aerosol</span> acidity, water content, sulfate concentration, and organic coatings. However, very few studies focused on chemistry occurring within actual cloud droplets. We will present data acquired during recent Holistic Interactions of Shallow Clouds, <span class="hlt">Aerosols</span>, and Land Ecosystems (HI-<span class="hlt">SCALE</span>) Campaign, which provide direct evidence for IEPOX-SOA formation in cloud droplets. Single particle mass spectrometer, miniSPLAT, and a high-resolution, time-of-flight <span class="hlt">aerosol</span> mass spectrometer were used to characterize the composition of <span class="hlt">aerosol</span> particles and cloud droplet residuals, while a high-resolution, time-of-flight chemical ionization mass spectrometer (HR-ToF-CIMS) was used to characterize gas-phase compounds. We find that the composition of cloud droplet residuals was markedly different than that of <span class="hlt">aerosol</span> particles sampled outside the cloud. Cloud droplet residuals were comprised of individual particles with high relative fractions of sulfate and nitrate and significant fraction of particles with mass spectra that are nearly identical to those of laboratory-generated IEPOX-SOA particles. The observed cloud-induced formation of IEPOX-SOA was accompanied by simultaneous decrease in measured concentrations of IEPOX and other gas-phase isoprene photooxidation products. Ultimately, the combined cloud, <span class="hlt">aerosol</span>, and gas-phase measurements conducted during HI-<span class="hlt">SCALE</span> will be used to develop and evaluate model treatments of aqueous-phase isoprene SOA formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21546060','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21546060"><span>Vertical profiles of <span class="hlt">aerosol</span> absorption coefficient from micro-Aethalometer data and Mie calculation over Milan.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ferrero, L; Mocnik, G; Ferrini, B S; Perrone, M G; Sangiorgi, G; Bolzacchini, E</p> <p>2011-06-15</p> <p>Vertical profiles of <span class="hlt">aerosol</span> number-size distribution and black carbon (BC) concentration were measured between ground-level and 500m AGL over Milan. A tethered balloon was fitted with an instrumentation package consisting of the newly-developed micro-Aethalometer (microAeth® Model AE51, Magee Scientific, USA), an optical particle counter, and a portable meteorological station. At the same time, PM(2.5) samples were collected both at ground-level and at a high altitude sampling site, enabling particle chemical composition to be determined. Vertical profiles and PM(2.5) data were collected both within and above the mixing layer. Absorption coefficient (b(abs)) profiles were calculated from the Aethalometer data: in order to do so, an optical enhancement factor (C), accounting for multiple light-scattering within the filter of the new microAeth® Model AE51, was determined for the first time. The value of this parameter C (2.05±0.03 at λ=880nm) was calculated by comparing the Aethalometer attenuation coefficient and <span class="hlt">aerosol</span> optical properties determined from OPC data along vertical profiles. Mie calculations were applied to the OPC number-size distribution data, and the <span class="hlt">aerosol</span> refractive index was calculated using the effective medium approximation applied to <span class="hlt">aerosol</span> chemical composition. The results compare well with AERONET data. The BC and b(abs) profiles showed a sharp decrease at the mixing <span class="hlt">height</span> (MH), and fairly constant values of b(abs) and BC were found above the MH, representing 17±2% of those values measured within the mixing layer. The BC fraction of <span class="hlt">aerosol</span> volume was found to be lower above the MH: 48±8% of the corresponding ground-level values. A statistical mean profile was calculated, both for BC and b(abs), to better describe their behaviour; the model enabled us to compute their average behaviour as a function of <span class="hlt">height</span>, thus laying the foundations for valid parametrizations of vertical profile data which can be useful in both remote sensing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26SS....4..485S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26SS....4..485S"><span>Intercomparison between CMIP5 model and MODIS satellite-retrieved data of <span class="hlt">aerosol</span> optical depth, cloud fraction, and cloud-<span class="hlt">aerosol</span> interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sockol, Alyssa; Small Griswold, Jennifer D.</p> <p>2017-08-01</p> <p><span class="hlt">Aerosols</span> are a critical component of the Earth's atmosphere and can affect the climate of the Earth through their interactions with solar radiation and clouds. Cloud fraction (CF) and <span class="hlt">aerosol</span> optical depth (AOD) at 550 nm from the Moderate Resolution Imaging Spectroradiometer (MODIS) are used with analogous cloud and <span class="hlt">aerosol</span> properties from Historical Phase 5 of the Coupled Model Intercomparison Project (CMIP5) model runs that explicitly include anthropogenic <span class="hlt">aerosols</span> and parameterized cloud-<span class="hlt">aerosol</span> interactions. The models underestimate AOD by approximately 15% and underestimate CF by approximately 10% overall on a global <span class="hlt">scale</span>. A regional analysis is then used to evaluate model performance in two regions with known biomass burning activity and absorbing <span class="hlt">aerosol</span> (South America (SAM) and South Africa (SAF)). In SAM, the models overestimate AOD by 4.8% and underestimate CF by 14%. In SAF, the models underestimate AOD by 35% and overestimate CF by 13.4%. Average annual cycles show that the monthly timing of AOD peaks closely match satellite data in both SAM and SAF for all except the Community Atmosphere Model 5 and Geophysical Fluid Dynamics Laboratory (GFDL) models. Monthly timing of CF peaks closely match for all models (except GFDL) for SAM and SAF. Sorting monthly averaged 2° × 2.5° model or MODIS CF as a function of AOD does not result in the previously observed "boomerang"-shaped CF versus AOD relationship characteristic of regions with absorbing <span class="hlt">aerosols</span> from biomass burning. Cloud-<span class="hlt">aerosol</span> interactions, as observed using daily (or higher) temporal resolution data, are not reproducible at the spatial or temporal resolution provided by the CMIP5 models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.A53O0381A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.A53O0381A"><span>Organic <span class="hlt">Aerosols</span> from SÃO Paulo and its Relationship with <span class="hlt">Aerosol</span> Absorption and Scattering Properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Artaxo, P.; Brito, J. F.; Rizzo, L. V.</p> <p>2012-12-01</p> <p>The megacity of São Paulo with its 19 million people and 7 million cars is a challenge from the point of view of air pollution. High levels of organic <span class="hlt">aerosols</span>, PM10, black carbon and ozone and the peculiar situation of the large <span class="hlt">scale</span> use of ethanol fuel makes it a special case. Little is known about the impact of ethanol on air quality and human health and the increase of ethanol as vehicle fuel is rising worldwide An experiment was designed to physico-chemical properties of <span class="hlt">aerosols</span> in São Paulo, as well as their optical properties. <span class="hlt">Aerosol</span> size distribution in the size range of 1nm to 10 micrometers is being measured with a Helsinki University SMPS (Scanning Mobility Particle Sizer), an NAIS (Neutral ion Spectrometer) and a GRIMM OPC (Optical Particle Counter). Optical properties are being measured with a TSI Nephelometer and a Thermo MAAP (Multi Angle Absorption Photometer). A CIMEL sunphotometer from the AERONET network measure the <span class="hlt">aerosol</span> optical depth. Furthermore, a Proton-Transfer-Reaction Mass Spectrometer (PTR-MS) and an <span class="hlt">Aerosol</span> Chemical Speciation Monitor (ACSM) are used to real-time VOC analysis and <span class="hlt">aerosol</span> composition, respectively. The ACSM was operated for 3 months continuosly during teh wintertime of 2012. The measured total particle concentration typically varies between 10,000 and 30,000 cm-3 being the lowest late in the night and highest around noon and frequently exceeding 50,000 cm-3. Clear diurnal patterns in <span class="hlt">aerosol</span> optical properties were observed. Scattering and absorption coefficients typically range between 20 and 100 Mm-1 at 450 nm, and between 10 to 40 Mm-1 at 637 nm, respectively, both of them peaking at 7:00 local time, the morning rush hour. The corresponding single scattering albedo varies between 0.50 and 0.85, indicating a significant contribution of primary absorbing particles to the <span class="hlt">aerosol</span> population. During the first month a total of seven new particle formation events were observed with growth rates ranging from 9 to 25</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT........52E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT........52E"><span><span class="hlt">Aerosol</span> characterizaton in El Paso-Juarez airshed using optical methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Esparza, Angel Eduardo</p> <p>2011-12-01</p> <p> retrieve the size distribution of them. This method permits the assessment of <span class="hlt">aerosols</span> in the ambient in-situ, without physically extracting them from their current state, as the filter technique does. The second objective was an analysis and comparison of the <span class="hlt">aerosol</span> optical thickness (AOT) data between ground-based instruments and satellite data. In this project, the groundbased instruments are the Multi Filter Rotating Shadowband Radiometers (MFRSR) installed at UTEP and the nearest sun photometer facility, a NASA's <span class="hlt">Aerosol</span> Robotic Network (AERONET), located at White Sands, New Mexico. The satellite data is provided by the NASA's Multi-angle Imaging Spectro-radiometer (MISR) instrument located in the Terra satellite. Finally, the third objective was to estimate ground particulate matter concentration of particles no greater than 2.5 mum in diameter (PM2.5) by using the MISR's satellite data. This objective was achieved by implementing an empirical mathematical model that includes measured data. In addition, this model addressed the geographic characteristics of the region as well as several factors such as season, relative humidity (RH) and the <span class="hlt">height</span> of the planetary boundary layer (PBL).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A33E2406M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A33E2406M"><span>Role of absorbing <span class="hlt">aerosols</span> on hot extremes in India in a GCM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mondal, A.; Sah, N.; Venkataraman, C.; Patil, N.</p> <p>2017-12-01</p> <p>Temperature extremes and heat waves in North-Central India during the summer months of March through June are known for causing significant impact in terms of human health, productivity and mortality. While greenhouse gas-induced global warming is generally believed to intensify the magnitude and frequency of such extremes, <span class="hlt">aerosols</span> are usually associated with an overall cooling, by virtue of their dominant radiation scattering nature, in most world regions. Recently, large-<span class="hlt">scale</span> atmospheric conditions leading to heat wave and extreme temperature conditions have been analysed for the North-Central Indian region. However, the role of absorbing <span class="hlt">aerosols</span>, including black carbon and dust, is still not well understood, in mediating hot extremes in the region. In this study, we use 30-year simulations from a chemistry-coupled atmosphere-only General Circulation Model (GCM), ECHAM6-HAM2, forced with evolving <span class="hlt">aerosol</span> emissions in an interactive <span class="hlt">aerosol</span> module, along with observed sea surface temperatures, to examine large-<span class="hlt">scale</span> and mesoscale conditions during hot extremes in India. The model is first validated with observed gridded temperature and reanalysis data, and is found to represent observed variations in temperature in the North-Central region and concurrent large-<span class="hlt">scale</span> atmospheric conditions during high temperature extremes realistically. During these extreme events, changes in near surface properties include a reduction in single scattering albedo and enhancement in short-wave solar heating rate, compared to climatological conditions. This is accompanied by positive anomalies of black carbon and dust <span class="hlt">aerosol</span> optical depths. We conclude that the large-<span class="hlt">scale</span> atmospheric conditions such as the presence of anticyclones and clear skies, conducive to heat waves and high temperature extremes, are exacerbated by absorbing <span class="hlt">aerosols</span> in North-Central India. Future air quality regulations are expected to reduce sulfate particles and their masking of GHG warming. It is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRD..121.9862W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRD..121.9862W"><span><span class="hlt">Aerosol</span> lidar observations of atmospheric mixing in Los Angeles: Climatology and implications for greenhouse gas observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ware, John; Kort, Eric A.; DeCola, Phil; Duren, Riley</p> <p>2016-08-01</p> <p>Atmospheric observations of greenhouse gases provide essential information on sources and sinks of these key atmospheric constituents. To quantify fluxes from atmospheric observations, representation of transport—especially vertical mixing—is a necessity and often a source of error. We report on remotely sensed profiles of vertical <span class="hlt">aerosol</span> distribution taken over a 2 year period in Pasadena, California. Using an automated analysis system, we estimate daytime mixing layer depth, achieving high confidence in the afternoon maximum on 51% of days with profiles from a Sigma Space Mini Micropulse LiDAR (MiniMPL) and on 36% of days with a Vaisala CL51 ceilometer. We note that considering ceilometer data on a logarithmic <span class="hlt">scale</span>, a standard method, introduces, an offset in mixing <span class="hlt">height</span> retrievals. The mean afternoon maximum mixing <span class="hlt">height</span> is 770 m Above Ground Level in summer and 670 m in winter, with significant day-to-day variance (within season σ = 220m≈30%). Taking advantage of the MiniMPL's portability, we demonstrate the feasibility of measuring the detailed horizontal structure of the mixing layer by automobile. We compare our observations to planetary boundary layer (PBL) <span class="hlt">heights</span> from sonde launches, North American regional reanalysis (NARR), and a custom Weather Research and Forecasting (WRF) model developed for greenhouse gas (GHG) monitoring in Los Angeles. NARR and WRF PBL <span class="hlt">heights</span> at Pasadena are both systematically higher than measured, NARR by 2.5 times; these biases will cause proportional errors in GHG flux estimates using modeled transport. We discuss how sustained lidar observations can be used to reduce flux inversion error by selecting suitable analysis periods, calibrating models, or characterizing bias for correction in post processing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27867786','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27867786"><span><span class="hlt">Aerosol</span> lidar observations of atmospheric mixing in Los Angeles: Climatology and implications for greenhouse gas observations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ware, John; Kort, Eric A; DeCola, Phil; Duren, Riley</p> <p>2016-08-27</p> <p>Atmospheric observations of greenhouse gases provide essential information on sources and sinks of these key atmospheric constituents. To quantify fluxes from atmospheric observations, representation of transport-especially vertical mixing-is a necessity and often a source of error. We report on remotely sensed profiles of vertical <span class="hlt">aerosol</span> distribution taken over a 2 year period in Pasadena, California. Using an automated analysis system, we estimate daytime mixing layer depth, achieving high confidence in the afternoon maximum on 51% of days with profiles from a Sigma Space Mini Micropulse LiDAR (MiniMPL) and on 36% of days with a Vaisala CL51 ceilometer. We note that considering ceilometer data on a logarithmic <span class="hlt">scale</span>, a standard method, introduces, an offset in mixing <span class="hlt">height</span> retrievals. The mean afternoon maximum mixing <span class="hlt">height</span> is 770 m Above Ground Level in summer and 670 m in winter, with significant day-to-day variance (within season σ = 220m≈30%). Taking advantage of the MiniMPL's portability, we demonstrate the feasibility of measuring the detailed horizontal structure of the mixing layer by automobile. We compare our observations to planetary boundary layer (PBL) <span class="hlt">heights</span> from sonde launches, North American regional reanalysis (NARR), and a custom Weather Research and Forecasting (WRF) model developed for greenhouse gas (GHG) monitoring in Los Angeles. NARR and WRF PBL <span class="hlt">heights</span> at Pasadena are both systematically higher than measured, NARR by 2.5 times; these biases will cause proportional errors in GHG flux estimates using modeled transport. We discuss how sustained lidar observations can be used to reduce flux inversion error by selecting suitable analysis periods, calibrating models, or characterizing bias for correction in post processing.</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/2016tac..confE..34R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016tac..confE..34R"><span>Titan's <span class="hlt">aerosol</span> optical properties with VIMS observations at the limb</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rannou, Pascal; Seignovert, Benoit; Le Mouelic, Stephane; Sotin, Christophe</p> <p>2016-06-01</p> <p>The study of Titan properties with remote sensing relies on a good knowledge of the atmosphere properties. The in-situ observations made by Huygens combined with recent advances in the definition of methane properties enable to model and interpret observations with a very good accuracy. Thanks to these progresses, we can analyze in this work the observations made at the limb of Titan in order to retrieve information on the haze properties as its vertical profiles but also the spectral behaviour between 0.88 and 5.2 µm. To study the haze layer and more generally the source of opacities in the stratosphere, we use some observation made at the limb of Titan by the VIMS instrument onboard Cassini. We used a model in spherical geometry and in single scattering, and we accounted for the multiple scattering with a parallel plane model that evaluate the multiple scattering source function at the plane of the limb. Our scope is to retrieve informations about the vertical distribution of the haze, its spectral properties, but also to obtain details about the shape of the methane windows to desantangle the role of the methane and of the <span class="hlt">aerosols</span>. We started our study at the latitude of 55°N, with a image taken in 2006 with a relatively high spatial resolution (for VIMS). Our preliminary results shows the spectral properties of the <span class="hlt">aerosols</span> are the same whatever the altitude. This is a consequence of the large <span class="hlt">scale</span> mixing. From limb profile between 0.9 and 5.2 µm, we can probe the haze layer from about 500 km (at 0.9 µm) to the ground (at 5.2 µm). We find that the vertical profile of the haze layer shows three distinct <span class="hlt">scale</span> <span class="hlt">heights</span> with transitions around 250 km and 350 km. We also clearly a transition around 70-90 km that may be due to the top of a condensation layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28643032','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28643032"><span>Fall from <span class="hlt">heights</span>: does <span class="hlt">height</span> really matter?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alizo, G; Sciarretta, J D; Gibson, S; Muertos, K; Romano, A; Davis, J; Pepe, A</p> <p>2018-06-01</p> <p>Fall from <span class="hlt">heights</span> is high energy injuries and constitutes a fraction of all fall-related trauma evaluations while bearing an increase in morbidity and mortality. We hypothesize that despite advancements in trauma care, the overall survivability has not improved in this subset of trauma patients. All adult trauma patients treated after sustaining a fall from <span class="hlt">heights</span> during a 40-month period were retrospectively reviewed. Admission demographics, clinical data, fall <span class="hlt">height</span> (ft), injury patterns, ISS, GCS, length of stay, and mortality were reviewed. 116 patients sustained a fall from <span class="hlt">heights</span>, 90.4% accidental. A mean age of 37± 14.7 years, 86% male, and a fall <span class="hlt">height</span> of 19 ± 10 ft were encountered. Admission GCS was 13 ± 2 with ISS 10 ± 11. Overall LOS was 6.6 ± 14.9 days and an ICU LOS of 2.8 ± 8.9 days. Falls ≥ 25 ft.(16%) had lower GCS 10.4 ± 5.8, increased ISS 22.6 ± 13.8, a fall <span class="hlt">height</span> 37.9 ± 13.1 ft and associated increased mortality (p < 0.001). Mortality was 5.2%, a mean distance fallen of 39 ± 22 ft. and an ISS of 31.5 ±16.5. Brain injury was the leading cause of death, 50% with open skull fractures. Level of <span class="hlt">height</span> fallen is a good predictor of overall outcome and survival. Despite advances in trauma care, death rates remain unchanged. Safety awareness and injury prevention programs are needed to reduce the risk of high-level falls.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT........84L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT........84L"><span>A simple parameterization of <span class="hlt">aerosol</span> emissions in RAMS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Letcher, Theodore</p> <p></p> <p> model. Furthermore, SA formation is greatly reduced during the winter months due to the lack of naturally produced organic VOC's. Because of these reasons, it was felt that neglecting SOA within the model was the best course of action. The actual parameterization uses a prescribed source map to add <span class="hlt">aerosol</span> to the model at two vertical levels that surround an arbitrary <span class="hlt">height</span> decided by the user. To best represent the real-world, the WRF Chemistry model was run using the National Emissions Inventory (NEI2005) to represent anthropogenic emissions and the Model Emissions of Gases and <span class="hlt">Aerosols</span> from Nature (MEGAN) to represent natural contributions to <span class="hlt">aerosol</span>. WRF Chemistry was run for one hour, after which the <span class="hlt">aerosol</span> output along with the hygroscopicity parameter (κ) were saved into a data file that had the capacity to be interpolated to an arbitrary grid used in RAMS. The comparison of this parameterization to observations collected at Mesa Verde National Park (MVNP) during the Inhibition of Snowfall from Pollution <span class="hlt">Aerosol</span> (ISPA-III) field campaign yielded promising results. The model was able to simulate the variability in near surface <span class="hlt">aerosol</span> concentration with reasonable accuracy, though with a general low bias. Furthermore, this model compared much better to the observations than did the WRF Chemistry model using a fraction of the computational expense. This emissions scheme was able to show reasonable solutions regarding the <span class="hlt">aerosol</span> concentrations and can therefore be used to provide an estimate of the seasonal impact of increased CCN on water resources in Western Colorado with relatively low computational expense.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912128H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912128H"><span>Broadband Measurement of <span class="hlt">Aerosol</span> Extinction in the Visible Range</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Quanfu; Bluvshtein, Nir; Segev, Lior; Flores, Michel; Rudich, Yinon; Washenfelder, Rebecca; Brown, Steven</p> <p>2017-04-01</p> <p>Atmospheric <span class="hlt">aerosols</span> influence the Earth's radiative budget directly by scattering and absorbing incoming solar radiation. <span class="hlt">Aerosol</span> direct forcing remains one of the largest uncertainties in quantifying the role that <span class="hlt">aerosols</span> play in the Earth's radiative budget. The optical properties of <span class="hlt">aerosols</span> vary as a function of wavelength, but few measurements reported the wavelength dependence of <span class="hlt">aerosol</span> extinction cross section and complex refractive indices, particularly in the blue and visible spectral range. There is also currently a large gap in our knowledge of how the optical properties evolve as a function of atmospheric aging in the visible spectrum. In this study, we constructed a new and novel laboratory instrument to measure <span class="hlt">aerosol</span> extinction as a function of wavelength, using cavity enhanced spectroscopy with a white light source. This broadband cavity enhanced spectroscopy (BBCES) covers the 395-700 nm spectral region using a broadband light source and a grating spectrometer with charge-coupled device detector (CCD). We evaluated this BBCES by measuring extinction cross section for <span class="hlt">aerosols</span> that are pure scattering, slightly absorbing and strongly absorbing atomized from standard materials. We also retrieved the refractive indices from the measured extinction cross sections. Secondary organic <span class="hlt">aerosols</span> from biogenic and anthropogenic precursors were "aged" to differential time <span class="hlt">scales</span> (1 to 10 days) in an Oxidation Flow Reactor (OFR) under the combined influence of OH, O3 and UV light. The new BBCES was used to online measure the extinction cross sections of the SOA. This talk will provide a comprehensive understanding of <span class="hlt">aerosol</span> optical properties alerting during aging process in the 395 - 700 nm spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030032926','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030032926"><span>A Global <span class="hlt">Aerosol</span> Model Forecast for the ACE-Asia Field Experiment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chin, Mian; Ginoux, Paul; Lucchesi, Robert; Huebert, Barry; Weber, Rodney; Anderson, Tad; Masonis, Sarah; Blomquist, Byron; Bandy, Alan; Thornton, Donald</p> <p>2003-01-01</p> <p>We present the results of <span class="hlt">aerosol</span> forecast during the <span class="hlt">Aerosol</span> Characterization Experiment (ACE-Asia) field experiment in spring 2001, using the Georgia Tech/Goddard Global Ozone Chemistry <span class="hlt">Aerosol</span> Radiation and Transport (GOCART) model and the meteorological forecast fields from the Goddard Earth Observing System Data Assimilation System (GEOS DAS). The <span class="hlt">aerosol</span> model forecast provides direct information on <span class="hlt">aerosol</span> optical thickness and concentrations, enabling effective flight planning, while feedbacks from measurements constantly evaluate the model, making successful model improvements. We verify the model forecast skill by comparing model predicted total <span class="hlt">aerosol</span> extinction, dust, sulfate, and SO2 concentrations with those quantities measured by the C-130 aircraft during the ACE-Asia intensive operation period. The GEOS DAS meteorological forecast system shows excellent skills in predicting winds, relative humidity, and temperature for the ACE-Asia experiment area as well as for each individual flight, with skill scores usually above 0.7. The model is also skillful in forecast of pollution <span class="hlt">aerosols</span>, with most scores above 0.5. The model correctly predicted the dust outbreak events and their trans-Pacific transport, but it constantly missed the high dust concentrations observed in the boundary layer. We attribute this missing dust source to the desertification regions in the Inner Mongolia Province in China, which have developed in recent years but were not included in the model during forecasting. After incorporating the desertification sources, the model is able to reproduce the observed high dust concentrations at low altitudes over the Yellow Sea. Two key elements for a successful <span class="hlt">aerosol</span> model forecast are correct source locations that determine where the emissions take place, and realistic forecast winds and convection that determine where the <span class="hlt">aerosols</span> are transported. We demonstrate that our global model can not only account for the large-<span class="hlt">scale</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810756L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810756L"><span>Combined observational and modeling efforts of <span class="hlt">aerosol</span>-cloud-precipitation interactions over Southeast Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loftus, Adrian; Tsay, Si-Chee; Nguyen, Xuan Anh</p> <p>2016-04-01</p> <p>Low-level stratocumulus (Sc) clouds cover more of the Earth's surface than any other cloud type rendering them critical for Earth's energy balance, primarily via reflection of solar radiation, as well as their role in the global hydrological cycle. Stratocumuli are particularly sensitive to changes in <span class="hlt">aerosol</span> loading on both microphysical and macrophysical <span class="hlt">scales</span>, yet the complex feedbacks involved in <span class="hlt">aerosol</span>-cloud-precipitation interactions remain poorly understood. Moreover, research on these clouds has largely been confined to marine environments, with far fewer studies over land where major sources of anthropogenic <span class="hlt">aerosols</span> exist. The <span class="hlt">aerosol</span> burden over Southeast Asia (SEA) in boreal spring, attributed to biomass burning (BB), exhibits highly consistent spatiotemporal distribution patterns, with major variability due to changes in <span class="hlt">aerosol</span> loading mediated by processes ranging from large-<span class="hlt">scale</span> climate factors to diurnal meteorological events. Downwind from source regions, the transported BB <span class="hlt">aerosols</span> often overlap with low-level Sc cloud decks associated with the development of the region's pre-monsoon system, providing a unique, natural laboratory for further exploring their complex micro- and macro-<span class="hlt">scale</span> relationships. Compared to other locations worldwide, studies of springtime biomass-burning <span class="hlt">aerosols</span> and the predominately Sc cloud systems over SEA and their ensuing interactions are underrepresented in scientific literature. Measurements of <span class="hlt">aerosol</span> and cloud properties, whether ground-based or from satellites, generally lack information on microphysical processes; thus cloud-resolving models are often employed to simulate the underlying physical processes in <span class="hlt">aerosol</span>-cloud-precipitation interactions. The Goddard Cumulus Ensemble (GCE) cloud model has recently been enhanced with a triple-moment (3M) bulk microphysics scheme as well as the Regional Atmospheric Modeling System (RAMS) version 6 <span class="hlt">aerosol</span> module. Because the <span class="hlt">aerosol</span> burden not only affects cloud</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ACP....17.3133S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ACP....17.3133S"><span>Estimates of the <span class="hlt">aerosol</span> indirect effect over the Baltic Sea region derived from 12 years of MODIS observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saponaro, Giulia; Kolmonen, Pekka; Sogacheva, Larisa; Rodriguez, Edith; Virtanen, Timo; de Leeuw, Gerrit</p> <p>2017-02-01</p> <p>Retrieved from the Moderate Resolution Imaging Spectroradiometer (MODIS) on-board the Aqua satellite, 12 years (2003-2014) of <span class="hlt">aerosol</span> and cloud properties were used to statistically quantify <span class="hlt">aerosol</span>-cloud interaction (ACI) over the Baltic Sea region, including the relatively clean Fennoscandia and the more polluted central-eastern Europe. These areas allowed us to study the effects of different <span class="hlt">aerosol</span> types and concentrations on macro- and microphysical properties of clouds: cloud effective radius (CER), cloud fraction (CF), cloud optical thickness (COT), cloud liquid water path (LWP) and cloud-top <span class="hlt">height</span> (CTH). <span class="hlt">Aerosol</span> properties used are <span class="hlt">aerosol</span> optical depth (AOD), Ångström exponent (AE) and <span class="hlt">aerosol</span> index (AI). The study was limited to low-level water clouds in the summer. The vertical distributions of the relationships between cloud properties and <span class="hlt">aerosols</span> show an effect of <span class="hlt">aerosols</span> on low-level water clouds. CF, COT, LWP and CTH tend to increase with <span class="hlt">aerosol</span> loading, indicating changes in the cloud structure, while the effective radius of cloud droplets decreases. The ACI is larger at relatively low cloud-top levels, between 900 and 700 hPa. Most of the studied cloud variables were unaffected by the lower-tropospheric stability (LTS), except for the cloud fraction. The spatial distribution of <span class="hlt">aerosol</span> and cloud parameters and ACI, here defined as the change in CER as a function of <span class="hlt">aerosol</span> concentration for a fixed LWP, shows positive and statistically significant ACI over the Baltic Sea and Fennoscandia, with the former having the largest values. Small negative ACI values are observed in central-eastern Europe, suggesting that large <span class="hlt">aerosol</span> concentrations saturate the ACI.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070010449&hterms=TRANSPORT+AIR&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DTRANSPORT%2BAIR','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070010449&hterms=TRANSPORT+AIR&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DTRANSPORT%2BAIR"><span>Intercontinental Transport of <span class="hlt">Aerosols</span>: Implication for Regional Air Quality</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; Ginoux, Paul</p> <p>2006-01-01</p> <p><span class="hlt">Aerosol</span> particles, also known as PM2.5 (particle diameter less than 2.5 microns) and PM10 (particle diameter less than 10 microns), is one of the key atmospheric components that determine ambient air quality. Current US air quality standards for PM10 (particles with diameter < 10 microns) and PM2.5 (particles with diameter 2.5 microns) are 50 pg/cu m and 15 pg/cu m, respectively. While local and regional emission sources are the main cause of air pollution problems, <span class="hlt">aerosols</span> can be transported on a hemispheric or global <span class="hlt">scale</span>. In this study, we use the Goddard Chemistry <span class="hlt">Aerosol</span> Radiation and Transport (GOCART) model to quantify contributions of long-range transport vs. local/regional pollution sources and from natural vs. anthropogenic sources to PM concentrations different regions. In particular, we estimate the hemispheric impact of anthropogenic sulfate <span class="hlt">aerosols</span> and dust from major source areas on other regions in the world. The GOCART model results are compared with satellite remote sensing and ground-based network measurements of <span class="hlt">aerosol</span> optical depth and concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1913909P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1913909P"><span>Imaging <span class="hlt">aerosol</span> viscosity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pope, Francis; Athanasiadis, Thanos; Botchway, Stan; Davdison, Nicholas; Fitzgerald, Clare; Gallimore, Peter; Hosny, Neveen; Kalberer, Markus; Kuimova, Marina; Vysniauskas, Aurimas; Ward, Andy</p> <p>2017-04-01</p> <p>Organic <span class="hlt">aerosol</span> particles play major roles in atmospheric chemistry, climate, and public health. <span class="hlt">Aerosol</span> particle viscosity is important since it can determine the ability of chemical species such as oxidants, organics or water to diffuse into the particle bulk. Recent measurements indicate that OA may be present in highly viscous states; however, diffusion rates of small molecules such as water appear not to be limited by these high viscosities. We have developed a technique for measuring viscosity that allows for the imaging of <span class="hlt">aerosol</span> viscosity in micron sized <span class="hlt">aerosols</span> through use of fluorescence lifetime imaging of viscosity sensitive dyes which are also known as 'molecular rotors'. These rotors can be introduced into laboratory generated <span class="hlt">aerosol</span> by adding minute quantities of the rotor to <span class="hlt">aerosol</span> precursor prior to <span class="hlt">aerosolization</span>. Real world <span class="hlt">aerosols</span> can also be studied by doping them in situ with the rotors. The doping is achieved through generation of ultrafine <span class="hlt">aerosol</span> particles that contain the rotors; the ultrafine <span class="hlt">aerosol</span> particles deliver the rotors to the <span class="hlt">aerosol</span> of interest via impaction and coagulation. This work has been conducted both on <span class="hlt">aerosols</span> deposited on microscope coverslips and on particles that are levitated in their true <span class="hlt">aerosol</span> phase through the use of a bespoke optical trap developed at the Central Laser Facility. The technique allows for the direct observation of kinetic barriers caused by high viscosity and low diffusivity in <span class="hlt">aerosol</span> particles. The technique is non-destructive thereby allowing for multiple experiments to be carried out on the same sample. It can dynamically quantify and track viscosity changes during atmospherically relevant processes such oxidation and hygroscopic growth (1). This presentation will focus on the oxidation of <span class="hlt">aerosol</span> particles composed of unsaturated and saturated organic species. It will discuss how the type of oxidant, oxidation rate and the composition of the oxidized products affect the time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110015299','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110015299"><span>Identifying <span class="hlt">Aerosol</span> Type/Mixture from <span class="hlt">Aerosol</span> Absorption Properties Using AERONET</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Giles, D. M.; Holben, B. N.; Eck, T. F.; Sinyuk, A.; Dickerson, R. R.; Thompson, A. M.; Slutsker, I.; Li, Z.; Tripathi, S. N.; Singh, R. P.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20110015299'); toggleEditAbsImage('author_20110015299_show'); toggleEditAbsImage('author_20110015299_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20110015299_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20110015299_hide"></p> <p>2010-01-01</p> <p><span class="hlt">Aerosols</span> are generated in the atmosphere through anthropogenic and natural mechanisms. These sources have signatures in the <span class="hlt">aerosol</span> optical and microphysical properties that can be used to identify the <span class="hlt">aerosol</span> type/mixture. Spectral <span class="hlt">aerosol</span> absorption information (absorption Angstrom exponent; AAE) used in conjunction with the particle size parameterization (extinction Angstrom exponent; EAE) can only identify the dominant absorbing <span class="hlt">aerosol</span> type in the sample volume (e.g., black carbon vs. iron oxides in dust). This AAE/EAE relationship can be expanded to also identify non-absorbing <span class="hlt">aerosol</span> types/mixtures by applying an absorption weighting. This new relationship provides improved <span class="hlt">aerosol</span> type distinction when the magnitude of absorption is not equal (e.g, black carbon vs. sulfates). The <span class="hlt">Aerosol</span> Robotic Network (AERONET) data provide spectral <span class="hlt">aerosol</span> optical depth and single scattering albedo - key parameters used to determine EAE and AAE. The proposed <span class="hlt">aerosol</span> type/mixture relationship is demonstrated using the long-term data archive acquired at AERONET sites within various source regions. The preliminary analysis has found that dust, sulfate, organic carbon, and black carbon <span class="hlt">aerosol</span> types/mixtures can be determined from this AAE/EAE relationship when applying the absorption weighting for each available wavelength (Le., 440, 675, 870nm). Large, non-spherical dust particles absorb in the shorter wavelengths and the application of 440nm wavelength absorption weighting produced the best particle type definition. Sulfate particles scatter light efficiently and organic carbon particles are small near the source and aggregate over time to form larger less absorbing particles. Both sulfates and organic carbon showed generally better definition using the 870nm wavelength absorption weighting. Black carbon generation results from varying combustion rates from a number of sources including industrial processes and biomass burning. Cases with primarily black carbon showed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AMT....11.2085M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AMT....11.2085M"><span><span class="hlt">Aerosol</span> particle size distribution in the stratosphere retrieved from SCIAMACHY limb measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malinina, Elizaveta; Rozanov, Alexei; Rozanov, Vladimir; Liebing, Patricia; Bovensmann, Heinrich; Burrows, John P.</p> <p>2018-04-01</p> <p> distribution parameters showed clear increases in the mode radius after the tropical volcanic eruptions, whereas no distinct behaviour of the absolute distribution width could be identified. A tape recorder, which describes the time lag as the perturbation propagates to higher altitudes, was identified for both parameters after the volcanic eruptions. A quasi-biannual oscillation (QBO) pattern at upper altitudes (28-32 km) is prominent in the anomalies of the analysed parameters. A comparison of the <span class="hlt">aerosol</span> effective radii derived from SCIAMACHY and SAGE II data was performed. The average difference is found to be around 30 % at the lower altitudes, decreasing with increasing <span class="hlt">height</span> to almost zero around 30 km. The data sample available for the comparison is, however, relatively small.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AMTD....3.3643F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AMTD....3.3643F"><span><span class="hlt">Aerosol</span> profiling using the ceilometer network of the German Meteorological Service</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flentje, H.; Heese, B.; Reichardt, J.; Thomas, W.</p> <p>2010-08-01</p> <p>The German Meteorological Service (DWD) operates about 52 lidar ceilometers within its synoptic observations network, covering Germany. These affordable low-power lidar systems provide spatially and temporally high resolved <span class="hlt">aerosol</span> backscatter profiles which can operationally provide quasi 3-D distributions of particle backscatter intensity. Intentionally designed for cloud <span class="hlt">height</span> detection, recent significant improvements allow following the development of the boundary layer and to detect denser particle plumes in the free tropospere like volcanic ash, Saharan dust or fire smoke. Thus the network builds a powerful <span class="hlt">aerosol</span> plume alerting and tracking system. If auxiliary <span class="hlt">aerosol</span> information is available, the particle backscatter coefficient, the extinction coefficient and even particle mass concentrations may be estimated, with however large uncertainties. Therefore, large synergistic benefit is achieved if the ceilometers are linked to existing lidar networks like EARLINET or integrated into WMO's envisioined Global <span class="hlt">Aerosol</span> Lidar Observation Network GALION. To this end, we demonstrate the potential and limitations of ceilometer networks by means of three representative <span class="hlt">aerosol</span> episodes over Europe, namely Sahara dust, Mediterranean fire smoke and, more detailed, the Icelandic Eyjafjoll volcano eruption from mid April 2010 onwards. The DWD (Jenoptik CHM15k) lidar ceilometer network tracked the Eyjafjoll ash layers over Germany and roughly estimated peak extinction coefficients and mass concentrations on 17 April of 4-6(± 2) 10-4 m-1 and 500-750(± 300) μg/m-3, respectively, based on co-located <span class="hlt">aerosol</span> optical depth, nephelometer (scattering coefficient) and particle mass concentration measurements. Though large, the uncertainties are small enough to let the network suit for example as aviation advisory tool, indicating whether the legal flight ban threshold of presently 2 mg/m3 is imminent to be exceeded.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.7961R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.7961R"><span>On the representation of <span class="hlt">aerosol</span> activation and its influence on model-derived estimates of the <span class="hlt">aerosol</span> indirect effect</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rothenberg, Daniel; Avramov, Alexander; Wang, Chien</p> <p>2018-06-01</p> <p>Interactions between <span class="hlt">aerosol</span> particles and clouds contribute a great deal of uncertainty to the scientific community's understanding of anthropogenic climate forcing. <span class="hlt">Aerosol</span> particles serve as the nucleation sites for cloud droplets, establishing a direct linkage between anthropogenic particulate emissions and clouds in the climate system. To resolve this linkage, the community has developed parameterizations of <span class="hlt">aerosol</span> activation which can be used in global climate models to interactively predict cloud droplet number concentrations (CDNCs). However, different activation schemes can exhibit different sensitivities to <span class="hlt">aerosol</span> perturbations in different meteorological or pollution regimes. To assess the impact these different sensitivities have on climate forcing, we have coupled three different core activation schemes and variants with the CESM-MARC (two-Moment, Multi-Modal, Mixing-state-resolving <span class="hlt">Aerosol</span> model for Research of Climate (MARC) coupled with the National Center for Atmospheric Research's (NCAR) Community Earth System Model (CESM; version 1.2)). Although the model produces a reasonable present-day CDNC climatology when compared with observations regardless of the scheme used, ΔCDNCs between the present and preindustrial era regionally increase by over 100 % in zonal mean when using the most sensitive parameterization. These differences in activation sensitivity may lead to a different evolution of the model meteorology, and ultimately to a spread of over 0.8 W m-2 in global average shortwave indirect effect (AIE) diagnosed from the model, a range which is as large as the inter-model spread from the AeroCom intercomparison. Model-derived AIE strongly <span class="hlt">scales</span> with the simulated preindustrial CDNC burden, and those models with the greatest preindustrial CDNC tend to have the smallest AIE, regardless of their ΔCDNC. This suggests that present-day evaluations of <span class="hlt">aerosol</span>-climate models may not provide useful constraints on the magnitude of the AIE, which</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AIPC.1734o0004E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AIPC.1734o0004E"><span><span class="hlt">Aerosols</span> attenuating the solar radiation collected by solar tower plants: The horizontal pathway at surface level</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Elias, Thierry; Ramon, Didier; Dubus, Laurent; Bourdil, Charles; Cuevas-Agulló, Emilio; Zaidouni, Taoufik; Formenti, Paola</p> <p>2016-05-01</p> <p><span class="hlt">Aerosols</span> attenuate the solar radiation collected by solar tower plants (STP), along two pathways: 1) the atmospheric column pathway, between the top of the atmosphere and the heliostats, resulting in Direct Normal Irradiance (DNI) changes; 2) the grazing pathway close to surface level, between the heliostats and the optical receiver. The attenuation along the surface-level grazing pathway has been less studied than the <span class="hlt">aerosol</span> impact on changes of DNI, while it becomes significant in STP of 100 MW or more. Indeed <span class="hlt">aerosols</span> mostly lay within the surface atmospheric layer, called the boundary layer, and the attenuation increases with the distance covered by the solar radiation in the boundary layer. In STP of 100 MW or more, the distance between the heliostats and the optical receiver becomes large enough to produce a significant attenuation by <span class="hlt">aerosols</span>. We used measured <span class="hlt">aerosol</span> optical thickness and computed boundary layer <span class="hlt">height</span> to estimate the attenuation of the solar radiation at surface level at Ouarzazate (Morocco). High variabilities in <span class="hlt">aerosol</span> amount and in vertical layering generated a significant magnitude in the annual cycle and significant inter-annual changes. Indeed the annual mean of the attenuation caused by <span class="hlt">aerosols</span> over a 1-km heliostat-receiver distance was 3.7% in 2013, and 5.4% in 2014 because of a longest desert dust season. The monthly minimum attenuation of less than 3% was observed in winter and the maximum of more than 7% was observed in summer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23500831','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23500831"><span>Utilisation of Rep-PCR to track microbes in <span class="hlt">aerosols</span> collected adjacent to their source, a saline lake in Victoria, Australia.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Munday, Chris I; O'Loingsigh, Tadhg; Tapper, Nigel J; De Deckker, Patrick; Allison, Gwen E</p> <p>2013-04-15</p> <p>Dust storms are a major source of <span class="hlt">aerosolized</span> bacteria, especially in the drought conditions experienced in Australia in the decade to 2009. The major aims of this project were to identify the culturable bacteria in environmental samples and to genetically fingerprint all isolates using repetitive element PCR (Rep-PCR) to investigate the possibility of tracking isolates from their source into the atmosphere. Four field trips were conducted to a dry lake in western Victoria, Australia to sample <span class="hlt">aerosols</span> and sediments. <span class="hlt">Aerosols</span> were collected at <span class="hlt">heights</span> up to 150 m using vacuum pumps with filters attached to a tethered helium balloon, while corresponding sediments were collected in sterile polypropylene tubes. Isolates were cultivated on Tryptic Soy Agar, R2 Agar and Marine Agar, and grown in dark conditions at ambient temperature. By sequencing the 16S rRNA gene of 270 isolates, fifteen different bacterial families were identified, with both the <span class="hlt">aerosols</span> and sediments dominated by the Bacillaceae family. Four sets of Rep-PCR primers were tested, with the ERIC and (GTG)5 primers proving to be the most suitable for fingerprinting the cultured taxa. Rep-PCR revealed very high strain diversity in the samples collected, however some strains were still able to be tracked from sediments up to 150 m in <span class="hlt">height</span>. This shows the potential of Rep-PCR, however very large reference databases would be required for the technique to be more useful. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003270&hterms=inversion&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dinversion','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003270&hterms=inversion&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dinversion"><span>Lidar-Radiometer Inversion Code (LIRIC) for the Retrieval of Vertical <span class="hlt">Aerosol</span> Properties from Combined Lidar Radiometer Data: Development and Distribution in EARLINET</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chaikovsky, A.; Dubovik, O.; Holben, Brent N.; Bril, A.; Goloub, P.; Tanre, D.; Pappalardo, G.; Wandinger, U.; Chaikovskaya, L.; Denisov, S.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003270'); toggleEditAbsImage('author_20170003270_show'); toggleEditAbsImage('author_20170003270_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003270_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003270_hide"></p> <p>2015-01-01</p> <p>This paper presents a detailed description of LIRIC (LIdar-Radiometer Inversion Code)algorithm for simultaneous processing of coincident lidar and radiometric (sun photometric) observations for the retrieval of the <span class="hlt">aerosol</span> concentration vertical profiles. As the lidar radiometric input data we use measurements from European <span class="hlt">Aerosol</span> Re-search Lidar Network (EARLINET) lidars and collocated sun-photometers of <span class="hlt">Aerosol</span> Robotic Network (AERONET). The LIRIC data processing provides sequential inversion of the combined lidar and radiometric data by the estimations of column-integrated <span class="hlt">aerosol</span> parameters from radiometric measurements followed by the retrieval of <span class="hlt">height</span>-dependent concentrations of fine and coarse <span class="hlt">aerosols</span> from lidar signals using integrated column characteristics of <span class="hlt">aerosol</span> layer as a priori constraints. The use of polarized lidar observations allows us to discriminate between spherical and non-spherical particles of the coarse <span class="hlt">aerosol</span> mode. The LIRIC software package was implemented and tested at a number of EARLINET stations. Inter-comparison of the LIRIC-based <span class="hlt">aerosol</span> retrievals was performed for the observations by seven EARLNET lidars in Leipzig, Germany on 25 May 2009. We found close agreement between the <span class="hlt">aerosol</span> parameters derived from different lidars that supports high robustness of the LIRIC algorithm. The sensitivity of the retrieval results to the possible reduction of the available observation data is also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16572788','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16572788"><span>Modeling ozone and <span class="hlt">aerosol</span> formation and transport in the pacific northwest with the community Multi-<span class="hlt">Scale</span> Air Quality (CMAQ) modeling system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>O'Neill, Susan M; Lamb, Brian K; Chen, Jack; Claiborn, Candis; Finn, Dennis; Otterson, Sally; Figueroa, Cristiana; Bowman, Clint; Boyer, Mike; Wilson, Rob; Arnold, Jeff; Aalbers, Steven; Stocum, Jeffrey; Swab, Christopher; Stoll, Matt; Dubois, Mike; Anderson, Mary</p> <p>2006-02-15</p> <p>The Community Multi-<span class="hlt">Scale</span> Air Quality (CMAQ) modeling system was used to investigate ozone and <span class="hlt">aerosol</span> concentrations in the Pacific Northwest (PNW) during hot summertime conditions during July 1-15, 1996. Two emission inventories (El) were developed: emissions for the first El were based upon the National Emission Trend 1996 (NET96) database and the BEIS2 biogenic emission model, and emissions for the second El were developed through a "bottom up" approach that included biogenic emissions obtained from the GLOBEIS model. The two simulations showed that elevated PM2.5 concentrations occurred near and downwind of the Interstate-5 corridor along the foothills of the Cascade Mountains and in forested areas of central Idaho. The relative contributions of organic and inorganic <span class="hlt">aerosols</span> varied by region, but generally organic <span class="hlt">aerosols</span> constituted the largest fraction of PM2.5. In wilderness areas near the 1-5 corridor, organic carbon from anthropogenic sources contributed approximately 50% of the total organic carbon with the remainder from biogenic precursors, while in wilderness areas in Idaho, biogenic organic carbon accounted for 80% of the total organic <span class="hlt">aerosol</span>. Regional analysis of the secondary organic <span class="hlt">aerosol</span> formation in the Columbia River Gorge, Central Idaho, and the Olympics/Puget Sound showed that the production rate of secondary organic carbon depends on local terpene concentrations and the local oxidizing capacity of the atmosphere, which was strongly influenced by anthropogenic emissions. Comparison with observations from 12 IMPROVE sites and 21 ozone monitoring sites showed that results from the two El simulations generally bracketed the average observed PM parameters and that errors calculated for the model results were within acceptable bounds. Analysis across all statistical parameters indicated that the NW-AIRQUEST El solution performed better at predicting PM2.5, PM1, and beta(ext) even though organic carbon PM was over-predicted, and the NET96 El</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.5300S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.5300S"><span>Variation in <span class="hlt">aerosol</span> nucleation and growth in coal-fired power plant plumes due to background <span class="hlt">aerosol</span>, meteorology and emissions: sensitivity analysis and parameterization.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stevens, R. G.; Lonsdale, C. L.; Brock, C. A.; Reed, M. K.; Crawford, J. H.; Holloway, J. S.; Ryerson, T. B.; Huey, L. G.; Nowak, J. B.; Pierce, J. R.</p> <p>2012-04-01</p> <p>New-particle formation in the plumes of coal-fired power plants and other anthropogenic sulphur sources may be an important source of particles in the atmosphere. It remains unclear, however, how best to reproduce this formation in global and regional <span class="hlt">aerosol</span> models with grid-box lengths that are 10s of kilometres and larger. The predictive power of these models is thus limited by the resultant uncertainties in <span class="hlt">aerosol</span> size distributions. In this presentation, we focus on sub-grid sulphate <span class="hlt">aerosol</span> processes within coal-fired power plant plumes: the sub-grid oxidation of SO2 with condensation of H2SO4 onto newly-formed and pre-existing particles. Based on the results of the System for Atmospheric Modelling (SAM), a Large-Eddy Simulation/Cloud-Resolving Model (LES/CRM) with online TwO Moment <span class="hlt">Aerosol</span> Sectional (TOMAS) microphysics, we develop a computationally efficient, but physically based, parameterization that predicts the characteristics of <span class="hlt">aerosol</span> formed within coal-fired power plant plumes based on parameters commonly available in global and regional-<span class="hlt">scale</span> models. Given large-<span class="hlt">scale</span> mean meteorological parameters, emissions from the power plant, mean background condensation sink, and the desired distance from the source, the parameterization will predict the fraction of the emitted SO2 that is oxidized to H2SO4, the fraction of that H2SO4 that forms new particles instead of condensing onto preexisting particles, the median diameter of the newly-formed particles, and the number of newly-formed particles per kilogram SO2 emitted. We perform a sensitivity analysis of these characteristics of the <span class="hlt">aerosol</span> size distribution to the meteorological parameters, the condensation sink, and the emissions. In general, new-particle formation and growth is greatly reduced during polluted conditions due to the large preexisting <span class="hlt">aerosol</span> surface area for H2SO4 condensation and particle coagulation. The new-particle formation and growth rates are also a strong function of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/919902','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/919902"><span><span class="hlt">Aerosol</span> mobility size spectrometer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wang, Jian; Kulkarni, Pramod</p> <p>2007-11-20</p> <p>A device for measuring <span class="hlt">aerosol</span> size distribution within a sample containing <span class="hlt">aerosol</span> particles. The device generally includes a spectrometer housing defining an interior chamber and a camera for recording <span class="hlt">aerosol</span> size streams exiting the chamber. The housing includes an inlet for introducing a flow medium into the chamber in a flow direction, an <span class="hlt">aerosol</span> injection port adjacent the inlet for introducing a charged <span class="hlt">aerosol</span> sample into the chamber, a separation section for applying an electric field to the <span class="hlt">aerosol</span> sample across the flow direction and an outlet opposite the inlet. In the separation section, the <span class="hlt">aerosol</span> sample becomes entrained in the flow medium and the <span class="hlt">aerosol</span> particles within the <span class="hlt">aerosol</span> sample are separated by size into a plurality of <span class="hlt">aerosol</span> flow streams under the influence of the electric field. The camera is disposed adjacent the housing outlet for optically detecting a relative position of at least one <span class="hlt">aerosol</span> flow stream exiting the outlet and for optically detecting the number of <span class="hlt">aerosol</span> particles within the at least one <span class="hlt">aerosol</span> flow stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2488A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2488A"><span>Physico-chemical properties of <span class="hlt">aerosols</span> in Sao Paulo, Brazil and mechanisms of secondary organic <span class="hlt">aerosol</span> formation.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Artaxo, Paulo; Ferreira de Brito, Joel; Varanda Rizzo, Luciana; Luiza Godoy, Maria; Godoy, Jose Marcus</p> <p>2013-04-01</p> <p>Megacities emissions are increasingly becoming a global issue, where emissions from the transportation sector play an increasingly important role. Sao Paulo is a megacity with a population of about 18 million people, 7 million cars and large-<span class="hlt">scale</span> industrial emissions. As a result of the vehicular and industrial emissions, the air quality in Sao Paulo is bellow WMO standards for <span class="hlt">aerosol</span> particles and ozone. Many uncertainties are found on gas- and particulate matter vehicular emission factors and their following atmospheric processes, e.g. secondary organic <span class="hlt">aerosol</span> formation. Due to the uniqueness of the vehicular fuel in Brazil, largely based on ethanol use, such characterization currently holds further uncertainties. To improve the understanding of the role of this unique emission characteristics, we are running a source apportionment study in Sao Paulo focused on the mechanisms of organic <span class="hlt">aerosol</span> formation. One of the goals of this study is a quantitative <span class="hlt">aerosol</span> source apportionment focused on vehicular emissions, including ethanol and gasohol (both fuels used by light-duty vehicles). This study comprises four sampling sites with continuous measurements for one year, where trace elements and organic <span class="hlt">aerosol</span> are being measured for PM2.5 and PM10 along with real-time NOx, O3, PM10 and CO measurements. <span class="hlt">Aerosol</span> optical properties and size distribution are being measured on a rotation basis between sampling stations. Furthermore, a Proton-Transfer-Reaction Mass Spectrometer (PTR-MS) and an <span class="hlt">Aerosol</span> Chemical Speciation Monitor (ACSM) are used to measure in real time VOCs and <span class="hlt">aerosol</span> composition, respectively. Trace elements were measured using XRF and OC/EC analysis was determined with a Sunset OC/EC instrument. A TSI Nephelometer with 3 wavelengths measure light scattering and a MAAP measure black carbon. Results show <span class="hlt">aerosol</span> number concentrations ranging between 10,000 and 35,000 cm-3, mostly concentrated in the nucleation and Aitken modes, with a peak in size at 80</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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