
Such a scenario is quite plausible in regions associated with wind-shear near cloud base. The argument is that if cloudy air is mixed downward into unsaturated air with a higher value of hl, and just enough mixing occurs to evaporate all of the liquid water in the cloudy air, the resulting mixture will be negatively buoyant with respect to the surrounding air. The thermal then mixes with the sub-cloud air causing evaporation, and the negatively buoyant parcel accelerates downward, disappearing at the point that all liquid water in the parcel fully evaporates.
Here we explore this hypothesis in more detail. Consider an initially saturated penetrative downdraft in the form of a spherical similarity thermal of radius R, vertical velocity w, total water surplus Q = qvs + ql - qve that descends from cloud base into clear air with vapor content qve.
The entrainment parameter is α: i.e. in the absence of sources or sinks a parameter X
inside the thermal obeys the equation
=
= 3R2αwX
e + SourceψX
At cloudbase R = 0, w = 0, ψX = ψX0
= w
. Show that the equations for the water
surplus and heat in the plume, at distance ζ below cloud base are


where

hankhan

HiCoudl

is not very different from
hle
.

where ε is the eddy dissipation rate and N is the buoyancy frequency in a vertically stratified fluid.