The Influence of Island Topography on Typhoon Track

The Influence of Island Topography on Typhoon Track

1708 MONTHLY WEATHER REVIEW VOLUME 139 The Influence of Island Topography on Typhoon Track Deflection YI-HSUAN HUANG AND CHUN-CHIEH WU Department of Atmospheric Sciences, National Taiwan University, Taipei, Taiwan YUQING WANG International Pacific Research Center, and Department of Meteorology, University of Hawaii at Manoa, Honolulu, Hawaii (Manuscript received 2 July 2010, in final form 10 January 2011) ABSTRACT High-resolution simulations for Typhoon Krosa (2007) and a set of idealized experiments are conducted using a full-physics model to investigate the eminent deflection of typhoon track prior to its landfall over mountainous island topography. The terrain height of Taiwan plays the most important role in Typhoon Krosa’s looping motion at its landfall, while the surface properties, details in the topographic shape of Taiwan, and the cloud microphysics are shown to be secondary to the track deflection. A simulation with 3-km res- olution and realistic model settings reproduces the observed Krosa’s track, while that with 9-km resolution fails, suggesting that high resolution to better resolve the typhoon–terrain interactions is important for the prediction and simulation of typhoon track deflection prior to landfall. Results from idealized experiments with model configurations mimicking those of Supertyphoon Krosa show that vortices approaching the northern and central topography are significantly deflected to the south before making sharp turns to the north, forming a kinked track pattern prior to and during landfall. This storm movement is consistent with the observed looping cases in Taiwan. Both real-case and idealized simulations show strong channel winds enhanced between the storm and the terrain when deflection occurs. Backward trajectory analyses support the concept of the channeling effect, which has been previously found to be crucial to the looping motion of Typhoon Haitang (2005) as well. However, the inner-core asymmetric ventilation flow does not match the movement of a deflected typhoon perfectly, partly because the steering flow is not well defined and could not completely capture the terrain- induced deflection in the simulation and in nature. 1. Introduction can cause significant changes in typhoon tracks and in- tensity, and the accompanying rainfall patterns. Further- Located in the western North Pacific, Taiwan suffers more, the intricacies of the terrain shape lead to from 3 to 6 typhoons each year. The severe wind gusts highly variable precipitation distributions over Taiwan. and heavy rain associated with a typhoon often lead to Although many previous studies have investigated this major catastrophes, making typhoons one of the most topic, the quantitative results are not consistent. Besides, serious meteorological phenomena. Taiwan is a moun- significant track deflection prior to landfall has been little tainous area with complex terrain features, including addressed in the literature. Apparently, topographic im- plains in the west and rugged mountains running in five pacts on typhoons indigenous to Taiwan make typhoon ranges from the northern to the southern tips of the is- forecasting very challenging. Terrain-induced tropical cy- land. Particularly noteworthy is the Central Mountain clone (TC) evolution, including track, intensity, structure, Range (CMR) with an average elevation of 2000 m and and the associated rainfall, depends primarily on how a TC a peak close to 4000 m. These exceptionally high ranges approaches the topography. Accordingly, the influence of the topography on track deflection, sharp turns in partic- ular, is regarded as a priority for investigation. Corresponding author address: Chun-Chieh Wu, Dept. of At- mospheric Sciences, National Taiwan University, No. 1, Sec. 4, Both observational and numerical studies have Roosevelt Rd., Taipei 106, Taiwan. shown that typhoons are prone to being deflected when E-mail: [email protected] approaching Taiwan. Earlier related studies have been DOI: 10.1175/2011MWR3560.1 Ó 2011 American Meteorological Society Unauthenticated | Downloaded 10/04/21 04:00 AM UTC JUNE 2011 H U A N G E T A L . 1709 reviewed in detail by Wu and Kuo (1999). Observations flow in the inner-core region is generated, and may drift showed that westbound typhoons tend to move cyclon- the vortex northward prior to landfall (region C). Al- ically around the northern side of the CMR (e.g., Brand though Yeh and Elsberry (1993a) stressed the impor- and Blelloch 1974; Wang 1980; Chang 1982). Wang tance of the terrain-induced inner-core imbalance in (1980) indicated that this might be due to the deflection leading to the deflection, the inner-core structure was not of the mean steering flow upstream of the CMR. To resolved well with the coarse model resolution (45 km). further understand the influence of topography on TC More recently, Lin et al. (2005) conducted idealized tracks, numerical simulations have been employed as simulations with much higher resolution, but without well (e.g., Chang 1982; Bender et al. 1987; Wu 2001; Yeh moist physics and the effect of surface friction. They and Elsberry 1993a,b; Lin et al. 1999, 2005). Chang introduced six nondimensional parameters for TC track (1982) found that mountain-induced deflection of deflection inferred from previous studies. These param- steering flow is confined to the lower levels. Idealized eters are Vmax/Nh, U/Nh, Vmax/fR, U/fLx, h/Lx,andR/Ly; experiments conducted by Yeh and Elsberry (1993a,b) namely, the Froude numbers of the vortex and the basic showed that the track deflection could be larger for the flow, the Rossby numbers of the vortex and the basic case of weaker and slower-moving storms, which is flow, the steepness of the topography, and the ratio of consistent with the findings of real-case simulations con- the vortex size to the barrier scale in the y direction, ducted by Bender et al. (1987). A cyclonic track (north- respectively. Here the y direction is normal to the move- westward deflection around the upstream of the terrain) ment of the vortex. Consistent with the earlier observa- induced by Taiwan’s topography was captured in a sim- tional and numerical studies, most of their simulations ulation of Typhoon Gladys by Wu (2001). Using a full- showed that vortices are deflected northward prior to physics model, Yeh and Elsberry (1993a) designed landfall. Greater track variations occur in the simula- a series of idealized experiments with model resolution tions with smaller Froude numbers of the vortex and of 45 km. They found that vortices approaching the the basic flow, ratio of the vortex size to the barrier scale southern portion of the barrier were deflected to the (y direction), Rossby numbers of the vortex and the south in a region approximately between 250 and 400 km basic flow, and with steeper topography. Nevertheless, upstream of the barrier (region B in their Figs. 13 and 22), southward deflection occurs under a specific condition, while those approaching the central and northern por- which is the combination of extremely small values of tion were slightly deflected to the north or not deflected Vmax/Nh, U/Nh, Vmax/fR, U/fLx, and R/Ly, and a very (see their Fig. 12). By subtracting the deflection from the large value of h/Lx. However, this southward track de- influence of the basic flow (deep-layer mean flow in their flection has rarely been found in the earlier observations barrier control experiment), Yeh and Elsberry (1993a) (Brand and Blelloch 1974) or numerical studies (e.g., examined the deflection without contribution from the Chang 1982; Bender et al. 1987; Yeh and Elsberry terrain-modified basic flow. Based on the analyses of the 1993a). The difference between the results of Yeh and asymmetric structure and the ventilation flow, Yeh and Elsberry (1993a) and Lin et al. (2005) implies that high- Elsberry (1993a) speculated that the channeling effect resolution full-physics models may be crucial to the may drift a vortex southward (relative to the steering of study of terrain-induced track deviations. Wu and Kuo the basic flow) to the topography over region B. The (1999) and Wu (2001) also showed the importance of channeling effect occurs when flow passes the narrow typhoon initialization and moist processes for track space between the barrier and the inner-core vortex, prediction. Although a number of idealized numerical where the inertial stability is strong enough to be a vir- studies have been conducted to simulate the track de- tual barrier. When getting closer to the topography flections, few of them were based on a full-physics model (250 km upstream of the terrain, region C in their Figs. with high model resolution. Therefore numerical studies 13 and 22), the storm motion behaved differently; vorti- with full-physics high-resolution models are indispens- ces approaching the southern part of the barrier were able for investigating the dynamics of the terrain-induced initially deflected northward, while those approaching track deflection. the northern end were only slightly influenced. Yeh and In some cases, tracks can be dramatically deflected Elsberry (1993a) found that it was the terrain-induced by topography, causing a looping motion [e.g., Shirley imbalance of the inner-core structure that led to the (1960), Mary (1965), Sarah (1989), Polly (1992), Haitang northward turn. Winds to the west of the storm were (2005), Krosa (2007), and Sinlaku (2008)]. Areas lashed weakened by the topography, in particular for those by severe rainfall and gusts can be shifted greatly because approaching the southern part of the barrier because of sharp turns, bringing about one of the important the cyclonic circulation impinged onto a wider area of typhoon forecasting problems. However, such unusual the topography. Hence, significant southerly asymmetric motion has not been well addressed in the literature. Unauthenticated | Downloaded 10/04/21 04:00 AM UTC 1710 MONTHLY WEATHER REVIEW VOLUME 139 FIG. 1. (a) CWB’s best track of Haitang (2005) and Krosa (2007) with hourly temporal resolution from 0000 UTC 17 Oct to 0600 UTC 19 Oct and from 0000 UTC 5 Oct to 0000 UTC 8 Oct, respectively.

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