TCAR - Typhoon Committee
TCAR - Typhoon Committee
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 />
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