ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
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overshooting air and the amount <strong>of</strong> environmental air. Assuming the fraction <strong>of</strong><br />
detraining air in the mixture is dr, the potential temperature <strong>of</strong> the mixture is<br />
θ<br />
m<br />
= dr ⋅θ<br />
a<br />
+ ( 1−<br />
dr)<br />
⋅θ<br />
(1)<br />
The potential temperature difference between the mixture and the environment is<br />
( dr ⋅θ<br />
+ ( 1−<br />
dr ⋅θ<br />
) −θ<br />
dθ<br />
= θ<br />
m<br />
−θ<br />
=<br />
a<br />
)<br />
(2)<br />
If we rearrange this equation for dr,<br />
dθ<br />
Q ⋅ dt<br />
dr = =<br />
(3)<br />
θ −θ<br />
θ −θ<br />
a<br />
a<br />
where Q is the cooling rate, which we measured to be about –7 K/day.<br />
For the usual values <strong>of</strong> potential temperatures (θ a = 355 K at LNB and θ = 375 K<br />
at 100 hPa), the fraction <strong>of</strong> detraining air in the mixture that is needed to generate the<br />
-7 K/day cooling is<br />
dr<br />
dt<br />
Q − 7K<br />
/ day<br />
= =<br />
θ<br />
a<br />
−θ<br />
355K<br />
− 375K<br />
= 0.35 (1/day) (4)<br />
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