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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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562<br />

Our study is to obtain <strong>and</strong> analyze the tropical cyclone's outflow<br />

structure as simulated by the NRL model, <strong>and</strong> to examine whether the<br />

hypothesized interactions between the upper-tropospheric systems <strong>and</strong><br />

the outflow are likely. For this purpose, a realistic steady-state<br />

tropical cyclone structure is obtained by initializing the NRL regional<br />

model with the mean tropical sounding <strong>and</strong> a Rankine vortex. In the<br />

simulated tropical cyclone, it is found that the outflow layer is<br />

dominated, in angular momentum transfer, by one or two jets, depending<br />

on the zonal wind shear. It is also found that there are secondary<br />

circulations around the outflow jet (Fig. 2). The secondary<br />

circulations in the jet entrance region is a thermally direct<br />

circulation, i.e., the rising branch is located on the anticyclonic<br />

shear side of the jet toward the storm center, while the subsiding<br />

branch is located on the cyclonic shear side of the jet away from the<br />

center. In the jet exit region, the direction of the secondary<br />

circulation is reversed <strong>and</strong> thermally indirect.<br />

We found that these circum-jet secondary circulations play<br />

important roles in the interaction of the outflow jet with uppertropospheric<br />

systems. In a numerical experiment we found that when the<br />

jet is accelerating, simulating the confluence of the outflow jet <strong>and</strong><br />

an approaching westerly trough, the secondary circulation is enhanced<br />

<strong>and</strong> initiates deep convections in the area of upward branches near the<br />

jet (Fig. 3). These findings will be reported in Shi et al. (1989).<br />

IV. VERTICAL NORMAL MODE INITIALIZATION.<br />

In order to filter out the spurious oscillations in the first few<br />

hours in the forecast of the regional model, a new initialization<br />

scheme is devised based on the vertical normal modes of the model. The<br />

spurious oscillations are mainly caused by the existence of fast-moving<br />

gravity waves, which arise due to the incapability of observing<br />

atmospheric state on all scales <strong>and</strong> errors in the regional analysis.<br />

The vertical normal mode method is to project the analysis into the<br />

model's vertical eigen space* A steady state solution of the

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