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East Asia and Western Pacific METEOROLOGY AND CLIMATE

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20<br />

3. SWDPTiC ^mLYSIS WD DIA^DSTIC STUDIES<br />

The detailed case study of the Mei-Yu frontal system in June 10-<br />

15, 1975 presented by Chen <strong>and</strong> Tsay (35) was probably the first paper<br />

in Taiwan belonging to the category of diagnostic study. The synoptic<br />

conditions <strong>and</strong> the budgets on moisture, kinetic energy <strong>and</strong> vorticity<br />

were studied to reveal the structure <strong>and</strong> dynamics of the Mei-Yu<br />

system. It was found that cumulus convection played an important role<br />

in the maintenance of the intensity of the Mei-Yu front (in terms of<br />

vorticity) in addition to the mid latitude baroclinic processes. The<br />

transport of the heat <strong>and</strong> moist rue by the low level jet was found to<br />

be essential in maintaining the cumulus convection (7,12,27,36). The<br />

mean vertical motion field for this case showed that the vertical<br />

advection <strong>and</strong> twisting terms cannot be neglected in the vorticity<br />

equation over mountain slopes <strong>and</strong> baroclinic zone (8). Results also<br />

showed that the major moisture source for the Mei-Yu area was the Bay<br />

of Bengal. The temperature <strong>and</strong> vertical motion fields showed that a<br />

thermally direct circulation with ascending warm air <strong>and</strong> descending<br />

cold air prevailed over the Mei-Yu area. This secondary circulation<br />

was particularly strong over the baroclinic region especially in the<br />

vicinity of Japan.<br />

Chen (10) observed that there was a continuous cloud b<strong>and</strong><br />

accompanying the Mei-Yu frontal system which extended from the<br />

vicinity of Japan southwestward to Taiwan <strong>and</strong> southern China. Along<br />

the Mei-Yu frontal system, a marked wind shear line at 850 mb <strong>and</strong> 700<br />

mb coincided with the maximum gradient of mixing ratio, relative<br />

humidity <strong>and</strong> equivalent potential temperature. To the south of the<br />

wind shear line, a 700 mb low level jet was located over the area of<br />

maximum mixing ratio <strong>and</strong> high equivalent potential temperature. Over<br />

<strong>and</strong> to the south of the wind shear line, strong cyclonic vorticity,<br />

horizontal convergence <strong>and</strong> upward motion prevailed. The strong<br />

convection in the southern portion of the cloud b<strong>and</strong> occurred over the<br />

area of maximum value of these kinematic parameters. The vorticity <strong>and</strong><br />

kinetic energy budget studies by Chen <strong>and</strong> Tsay (37) showed that an<br />

area of maximum vorticity at 850 mb was located between the Mei-Yu<br />

trough <strong>and</strong> the area of maximum horizontal convergence (or maximum<br />

upward motion). The generation of cyclonic vorticity due to horizontal<br />

convergence was counteracted by negative vorticity advections <strong>and</strong> thus<br />

led to a quasi -stationary state of the Mei-Yu front at surface <strong>and</strong> 850<br />

mb, Kinetic energy budget showed that a major part of the kinetic<br />

energy generated by cross-contour processes tended to dissipate in<br />

situ over the Mei-Yu area while only a very small portion (15%) was<br />

transported to the environment. The mesoscale analysis of this case<br />

(13,36) showed that the mesoscale circulation system with horizontal<br />

dimensions of 200-300 km was characterized by cyclonic vorticity,<br />

horizontal convergence <strong>and</strong> upward motion in the boundary layer. This<br />

mesoscale circulation system tended to organize <strong>and</strong> enhance the<br />

mesoscale convective systems.

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