Talk
Abstract:
Modeling of Atmospheric Aerosols
Francis
S. Binkowski
Atmospheric Sciences Modeling Division (NOAA)
US Environmental Protection Agency
fzb@hpcc.epa.gov
Modeling
aerosol particles in the atmosphere has some major differences
from modeling species such as water vapor or trace gases. For
such species, a mass concentration or mixing ratio is sufficient.
Particles on the other hand have a size distribution with diameters
ranging over several orders of magnitude, from a few nanometers
to many micrometers. To represent this size distribution, atmospheric
modelers have resorted to two major paradigms. The first of
these is a sectional approach in which the size distribution
is subdivided into sections covering a small range of particle
diameters. This approach has been very popular and has an obvious
analogy with particle samplers which measure in size ranges
such as a cascade impactor. The second approach assumes that
there is an appropriate mathematical functional form which represents
the size distribution. Moments of this distribution describe
characteristics of the distribution. The zeroeth moment is the
total number of particles, the second, and third moments are
related to total surface area and volume respectively. Some
modelers calculate even higher moments and related them to radiative
information which may be gathered from remote sensing.
After a brief review of the two paradigms, most of the presentation
will concentrate on the second paradigm as implemented in a
three-dimensional chemical-transport model, the EPA Community
Multiscale Air Quality (CMAQ) modeling system. In this implementation,
particles smaller than 2.5 micrometers in diameter are represented
by the superposition of two log-normal subdistributions and
larger particles are represented by a single log-normal distribution.
In the smaller size range, the total number, total surface area,
and the constituent chemical species masses are the predicted
variables. For the larger particle range only number and species
masses are predicted.
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