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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 />

41

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