WMOD00317

• Contract/Permit #: 14-06-D-6999
• Project Name: CAWRP
• Title: Cascades Atmosphere Water Resources Program - Volume I
• Prepared For: US Department of the Interior Bureau of Reclaimation
• Date: 7/1/1970
• Weather Modification - Doc Type: Report

where K is a constant on a streamline, and the integral has been taken from

Let us consider now the integral on the right hand side of eqn. (3.53).

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, ;)';31 -

BE(l - A)
-a3Vp x Vp = v . V(c T + Lws>i
POllO P

where

dUn eEl
BE = dz
o

Substituting eqns.{3.3) and (3.48) into eqn. (3.1) gives

. v.,

. d: 't' SE
Va!! + (1 - A) !. '. V['- (c T + Lws)]i = 0
Pouo P

or,

Po
- nv .
P -

BE BE
V + v . V -(c T + 1M ) - Av . V[ - (0 T + Lw )] = 0
ups ups
o 0

The Bernoulli equation can be ~itten as

. '. 1\

2
c T +g1; + L + Lw = constant (on a streamline)'
P 2 s

Therefore, eqn. (3.5~) becomes

Po BE 2
- n - U ( r + g~)
P 0

BE
u
o

11; Ad(c T + Lw )] ;I K
P s
o

zero displacement of the parcel to displacement t.

The 1st law of thermodynamics can be Wl'itten as

(3.48)

(3.49)

(3,50)

(3.51)

(3.52)

(3.53)