HR: 16:55h
AN: A34C-04 [Abstracts]
TI: Retrieval of Aerosol Liquid Water Path and Hygroscopic Growth from the AERONET database
AU: * Schuster, G L
EM: gregory.l.schuster@nasa.gov
AF: NASA Langley Research Center, Mail Stop 420, Hampton, VA 23681, United States
AU: Lin, B
EM: bing.lin@nasa.gov
AF: NASA Langley Research Center, Mail Stop 420, Hampton, VA 23681, United States
AU: Dubovik, O
EM: dubovik@loa630.univ-lille1.fr
AF: Laboratoire d'Optique Atmospherique, 59655 Villeneuve d'Ascq CEDEX, Lille, 59655,
France
AU: Holben, B
EM: bholben@pop900.gsfc.nasa.gov
AF: NASA GSFC, Code 614.4, Greenbelt, MD 20771, United States
AU: Sinyuk, A
EM: Aliaksandr.Sinyuk-1@nasa.gov
AF: NASA GSFC, Code 614.4, Greenbelt, MD 20771, United States
AB:
Aerosol water uptake in the atmosphere alters aerosol size distributions, changes aerosol optical properties, and
consequently impacts the aerosol radiative forcing. The parameterization of water uptake in aerosol transport
models is empirical and unchecked, largely because of the lack of available measurements. We have developed
a retrieval of the aerosol liquid water path (LWP) and hygroscopic growth using the AERONET database, and
apply our results at over 200 AERONET locations.
The real refractive index of prevalent atmospheric aerosols at the 500 nm wavelength ranges from 1.50 for sea
salt to 1.56 for dust. Liquid water, on the other hand, has a real refractive index of 1.33 at 500 nm. We use this
disparity in refractive indices to determine the equivalent water fractions for aerosol mixtures associated with the
AERONET refractive index retrievals. Once the aerosol water fraction is known, we can also determine the
hygroscopic growth factor, aerosol LWP, and the dry aerosol loading in the atmospheric column.
Our aerosol LWP results are highly correlated with the following parameters: fine mode volume concentration,
aerosol optical thickness (440 nm), aerosol water fraction, and coarse mode volume concentration (average
correlation coefficients for all 200 sites ranges from 0.47 for the coarse mode concentration to 0.78 for the fine
mode concentration). The regressions of these parameters have different slopes at each of the AERONET sites,
which suggests a LWP sensitivity to aerosol composition. Aerosol liquid water path is not highly correlated with
the mode radii or the fine mode volume fraction (average correlation coefficients for all sites range from 0.11 for
the coarse mode median radius to 0.27 for the fine mode volume fraction).
We compiled monthy-averaged statistics at over 200 AERONET locations based upon the daily-average
AERONET retrievals; our results are consistent with regional and seasonal expectations. Aerosol water fractions
range from a low value of 0.14 at the Etosha Pan site (Namibia) to a high value of 0.73 at the Anmyon site (South
Korea) in August, which is consistent with the arid and humid climates of those two sites. Likewise, the
hygroscopic growth factor ranges from 1.05 at Etosha Pan to 1.69 at Anmyon for that month. The aerosol water
fraction does not necessarily dominate the aerosol LWP (the effective radius and aerosol loading are also
important), so these two sites do not represent the extreme aerosol LWPs. Rather, Beijing had the highest
average LWP for August, with a value of 120 mg m-2, and Tinga Tingana in Australia had the lowest August
average with a value of 5 mg m-2. We will present the regional and seasonal variability of these retrieved
parameters at several representative AERONET sites. We will also discuss the sensitivity of this retrieval to a
variety of aerosol mixtures.
DE: 0305 Aerosols and particles (0345, 4801, 4906)
DE: 0394 Instruments and techniques
SC: Atmospheric Sciences [A]
MN: 2007 Fall Meeting