Abstract
A cloud consists of I "cloudlets', each comprising cloud droplets with radii from zero to rmax, the latter value depending on the drop size distribution (DSD). Evaporation occurs only within the EZ comprised of J ≤ I cloudlets. When the cloudlet at cloud edge evaporates, the EZ progresses one cloudlet into the cloud's interior. This eventually results in evaporation of the cloud in time tE = K(H/h)r2max(1 - Se)-1, where H is the cloud thickness, h the EZ thickness, Se the environmental saturation ratio, and K a constant. Values of tE(1 - Se) versus h are presented for eight observed DSDs. For use in atmospheric general circulation models (GCMs), the cloud evaporation process is represented by dm/dt = -(1 - Se)m/τ, where m is the cloud-water mixing ratio and τ = K(H/h)r2maxn-1. With parameter n chosen sufficiently large, a GCM cloud will evaporate virtually entirely in time tE, for example, 99.3% for n = 5. -from Authors
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CITATION STYLE
Schlesinger, M. E., & Oh, J. H. (1993). A cloud-evaporation parameterization for general circulation models. Monthly Weather Review, 121(4), 1239–1248. https://doi.org/10.1175/1520-0493(1993)121<1239:ACEPFG>2.0.CO;2
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