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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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123<br />

where N is nondimensional Newtonian cooling coefficient, S<br />

measures mean static stability of the basic state; I <strong>and</strong> B<br />

represent ratios of latent heating to adiabatic cooling due<br />

to vertical motion at P2 <strong>and</strong> p e/ respectively. We have used<br />

c 0 / (c 0 /B) 1/2 , (6c 0 )~ 1/2 , GO, <strong>and</strong> 2Ap(Bc 0 ) 1/2 as horizontal<br />

velocity, length, time, geopotential, <strong>and</strong> vertical p-<br />

velocity scales, respectively, where c 0 is long gravity wave<br />

speed in 2-level model.<br />

The boundary layer friction-induced vertical velocity<br />

OJ e can be expressed in terms of geopotential at p e <strong>and</strong> 0 e<br />

(Wang <strong>and</strong> Chen, 1988):<br />

^2 A S (E 2 + 2 ) ^"^271^EVy a x)<br />

where E=p e gAz/ [ (p s -p e ) /Bc 0 -h- In(h/z 0 ) ] is the Ekman number<br />

determined by turbulent viscosity A z , depth of the surface<br />

layer h, the surface roughness length z 0 <strong>and</strong> density p c .<br />

The upper boundary <strong>and</strong> lateral boundary conditions are<br />

c

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