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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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496<br />

Burgers(l948) had put forward a simple turbulence<br />

model [3 J . Chao(l962) extended Burgers model to include<br />

temperature advection. The basic equations of the<br />

Burger s-Chao model are as follows:<br />

-a<br />

„,<br />

where U(t) <strong>and</strong> T(t) are horizontal velocity <strong>and</strong><br />

temperature averaged for height respectively, w(z,t) <strong>and</strong><br />

0(z,t) are perturb ational vertical velocity <strong>and</strong><br />

temperature respectively, P <strong>and</strong> Q are pressure gradient<br />

force <strong>and</strong> heat source respectively, both of which are<br />

necessary for the maintenance of initial mean motion UQ<br />

<strong>and</strong> mean temperature T Q . The terms involving 3><br />

represent viscous dissipation. Eqs. (1)~(4) represent<br />

the nonlinear dynamical system. The first terms on the<br />

right h<strong>and</strong> of Eqs* (2) <strong>and</strong> (4) represent the mean field<br />

acting on the perturbation fields. The third terms on<br />

the right h<strong>and</strong> of Eqs. (1) <strong>and</strong> (3) represent the<br />

perturbation field acting on the mean fields. £0 denotes<br />

buoyancy force. 1iT^ <strong>and</strong> ^tfl^c<br />

are advection terms.<br />

^-.JL ^ ig ^g^ temperature, taken as a constant), j^<br />

is the adiabatic lapse rate <strong>and</strong> H is the vertical<br />

thickness.<br />

The advection terms are omitted in Chao's model. The<br />

temperature advection term ^M is included in our<br />

model. Let

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