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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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from the center of cyclone. Tn addition, at r* = 5 <strong>and</strong> 800<br />

hPa, there Is a negative circulation. The reason of its<br />

formation is not clear.<br />

xlOOhPa 5.5<br />

551<br />

1 2 3 + 5 6, 7 r*<br />

Pig, 1 The secondary circulation forced by the diabatic<br />

heating term, with interval of stream function being 0.8*10"<br />

!.) Turbulent flux of heat<br />

Tt is generally accepted that the vertical flux of<br />

heat (the 3-rd. term on the right h<strong>and</strong> side of Eq. (2)) is<br />

much wore important than the horizontal flux (the 2-nd<br />

t.errn)in the development of typhoons,<br />

For the secondary circulation forced by the horizontal<br />

turbulent flux of heat, there is a weak positive<br />

circulation with two centers at about 750 hPa in the lower<br />

<strong>and</strong> middle troposphere (not shown). A negative circulation<br />

is located in the upper troposphere, with two stronger<br />

centers found in the layer of 300-200 "'hPa .<br />

The secondary circulation forced by the vertical<br />

turbulent flux of heat shows a complete pair of positive<br />

<strong>and</strong> negative circulation cells, with the center of the<br />

former found, at 550 hPa <strong>and</strong> the center of the latter at 750<br />

hPa (not shown), Above 300 hPa, one may observe a weak<br />

positive circulation,<br />

forced<br />

greater<br />

of heat<br />

3)<br />

Tt<br />

Tn comparison, the magnitude of secondary circulation<br />

by the vertical turbulent flux of heat is much<br />

than that forced by the horizontal turbulent flux<br />

Cumulus horizontal flux of heat<br />

is generally recognized that the transport of heat<br />

by cumulus convection (the 6-th term on the right h<strong>and</strong> side<br />

of Eq, (2}) is much greater than that by turbulence. Kuo<br />

(1974) suggested that this term may foe estimated according<br />

to K-th.eory, but it is very important to -take K value<br />

appropriately. As a rough approximation f we take this'<br />

coefficient to be three times as great as the eddy<br />

viscosity coefficient. The secondary circulation thus<br />

obtained has a pattern similar to that forced by horizontal<br />

turbulent flux of heat, only with greater magnitudes of<br />

.(not", shown ) , •"." •' ' ... : . • ' . - . ' . .. ;'./•' • ' • . . • .; •.•;' '• • • . v ' • ' • • ' • • "

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