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TCAR - Typhoon Committee

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<strong>TCAR</strong><br />

CHAPTER 5 - RESEARCH FELLOWSHIP TECHNICAL REPORT<br />

initialization scheme is used to predict TS track<br />

and landfall when a TS occurs in the South China<br />

Sea. Bogus vortex including both symmetric and<br />

asymmetric components is constructed based on<br />

the assumption that the storm motion is equal to<br />

the vector sum of the large scale environmental<br />

flow plus the vortex asymmetry (Smith and Ulrich,<br />

1990; Smith, 1991; Smith and Weber, 1993; Weber<br />

and Smith, 1995; Davidson and Weber, 2000).<br />

Numerical experiments have been conducted<br />

to select appropriate parameters in vortex<br />

initialization scheme for correctly presenting<br />

environmental flow, and the assumed vortex<br />

structure in the South China Sea. Experiments<br />

indicated that a scale of approximately 4 times the<br />

radius of outermost closed isobar is appropriate<br />

to preserve key components of the environmental<br />

flow. Also, systematic northwest bias in forecasted<br />

TC tracks caused by asymmetric component<br />

of bogus vortex is corrected. Above mentioned<br />

modifications brought significant improvement in<br />

accuracy of TC (TC) track forecasts near Vietnam<br />

coastline (Nguyen T. M. Phuong, 2003, 2004,<br />

2005, 2006).<br />

In CMA the limited area operational TS prediction<br />

system had been used since 1996. In this system<br />

the vortex initialization is similar to that developed<br />

by Iwasaki et la (1987), i.e the bogus vortex is an<br />

axi-symmetric, constructed by empirical methods<br />

(Ma et la, 2007).<br />

Since 2002 the second generation TS prediction<br />

system, named GMTTP had been used<br />

operationally. This is global spectral model version<br />

T213L31 that is more advanced in both dynamics<br />

and physics contents in comparison with the<br />

limited area operational TS prediction system<br />

(LTCM). Also, the vortex bogus scheme had been<br />

improved by including asymmetric component in<br />

the initial TC vortex. In new vortex initialization<br />

scheme the bogus vortex consists of axisymmetric<br />

component and asymmetric component. The first<br />

is constructed as above mentioned ( similar to<br />

Iwasaki et la 1987). The second is generated<br />

from the analysis field around the TC that is<br />

similar to the method described in Kurihara et la<br />

(1993, 1995). The implementation of this bogus<br />

scheme is as followings : (i) the axisymmetric<br />

vortex is removed from T213L31 analysis field,<br />

(ii) the axisymmetric vortex component is<br />

generated, (iii) the asymmetric vortex component<br />

is constructed, (iv) the axisymmetric and the<br />

asymmetric components are added to form<br />

asymmetric TC bogus vortex and (v) the bogus<br />

vortex is inserted back to analysis field. The<br />

flowchart of the second generation TS prediction<br />

system is given in Fig.1. This asymmetric vortex<br />

bogus scheme significantly improved accuracy<br />

of CMA’s model TS track forecasts, especially in<br />

the short ranges upto 72h. However, there exist<br />

two kinds of systematic errors in the second<br />

generation TS track prediction system : the first<br />

is the westward deflection when a TS moved to<br />

NE and the second is the N deflection when a TS<br />

moved to W or NW due to many different factors<br />

(Ma et la 2007).<br />

Schematic depiction of the TC<br />

prediction system at NMC/China<br />

Fig . 1 . Flowchart of of the CMA’s second<br />

generation TS prediction system (GTCMA) (Qu.<br />

et la, 2009)<br />

In 2006 in the CMA’s third generation TS track<br />

prediction system a new TS initialization scheme<br />

is build. This new scheme includes 3 procedures<br />

(1) When TC occurs at first time, inserting an<br />

appropriate vortex in the first guess fields, it is<br />

called vortex formation.The appropriate vortex<br />

2009<br />

281

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