A028-03
Aerosol direct radiative effects at the ARM SGP and TWP Sites

Monday, 7 December 2020: 20:38
Virtual
Kelly Balmes, University of Washington Seattle Campus, Department of Atmospheric Sciences, Seattle, WA, United States, Qiang Fu, University of Washington, Atmospheric Sciences, Seattle, WA, United States and Xiaolin Wu, Beijing Normal University, Beijing, China
Abstract:
The aerosol direct radiative effect (DRE) was estimated at the Atmospheric Radiation Measurement (ARM) Southern Great Plains (SGP) and Tropical Western Pacific (TWP) sites first under clear-sky conditions. The NASA Langley Fu-Liou radiative transfer model was used with observed inputs including aerosol vertical extinction profile from the Raman lidar; aerosol spectral optical depth, single-scattering albedo and asymmetry factor from Aerosol Robotic Network (AERONET); temperature and water vapor profiles from radiosondes; and surface shortwave spectral albedo from radiometers. A radiative closure experiment was conducted for clear-sky conditions. The mean differences of modeled and observed surface downwelling shortwave total fluxes were 1 W m-2 at SGP and 2 W m-2 at TWP, which are within observational uncertainty. At SGP, the estimated annual mean clear-sky aerosol DRE is -3.00 W m-2 at the top of atmosphere (TOA) and -6.85 W m-2 at the surface. The strongest aerosol DRE of -4.81 (-10.77) W m-2 at the TOA (surface) are in the summer when the AOD is largest. The weakest aerosol DRE of -1.28 (-2.77) W m-2 at the TOA (surface) are in November-January when AODs and single-scattering albedos are lowest. At TWP, the annual mean clear-sky DRE is -2.82 W m-2 at the TOA and -10.34 W m-2 at the surface. The strongest aerosol DRE of -5.95 W m-2 (-22.20 W m-2) at the TOA (surface) are in November (October) due to the biomass burning season’s peak. The weakest aerosol DRE of -0.96 (-4.16) W m-2 at the TOA (surface) are in March (April) when AODs are smallest. We will also quantify the cloudy-sky aerosol DRE for the transparent and opaque cloud situation. For transparent cloudy-skies, cloud detection and retrieved particulate extinction from the Raman lidar will be utilized. For opaque cloudy-skies, cloud detection and retrieved extinction from the Ka-band ARM Zenith Radar will be utilized. The whole-sky aerosol DRE will then be quantified by combining the aerosol DRE for clear- and cloudy-skies.