The Potential Vorticity Budget of Typhoon Nari (2001)

碩士 === 國立中央大學 === 大氣物理研究所 === 99 === Potential Vorticity (PV) is a quantity that combines both dynamic and thermodynamic information, and it is conserved under the adiabatic and frictionless condition. Therefore it is suitable for analyzing tropical cyclones’ (TC) dynamic. In recent years, there hav...

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Main Authors: Po-Hsu Lin, 林柏旭
Other Authors: Ming-Jen Yang
Format: Others
Language:zh-TW
Published: 2011
Online Access:http://ndltd.ncl.edu.tw/handle/44580436669963717907
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spelling ndltd-TW-099NCU050210402015-10-19T04:03:15Z http://ndltd.ncl.edu.tw/handle/44580436669963717907 The Potential Vorticity Budget of Typhoon Nari (2001) 納莉颱風(2001)之位渦收支分析 Po-Hsu Lin 林柏旭 碩士 國立中央大學 大氣物理研究所 99 Potential Vorticity (PV) is a quantity that combines both dynamic and thermodynamic information, and it is conserved under the adiabatic and frictionless condition. Therefore it is suitable for analyzing tropical cyclones’ (TC) dynamic. In recent years, there have been considerable studies between TCs and the PV. However, it appears that only a few studies using the potential vorticity budget to analyze a real TC case. Thus, what kind of dynamical / thermodynamical interaction processes could be obtained from the PV budget analysis, and what phenomena will be caused by the steep topography of Taiwan are worthy of study. A compressible nonhydrostatic PV budget equation, derived base on Pedlosky (1987) and Schubert et al. (2001), is used here to gain insights into the PV budget evolution of a typhoon from its oceanic stage to landfall stage. The budget is conducted using high spatial resolution (2-km horizontal grid size) hourly outputs from Yang et al. (2008), in which the Pennsylvania State University / National Center for Atmospheric Research Fifth Generation Mesoscale Model was used to simulate Typhoon Nari (2001) and reproduced reasonably-well results as verified against observations. Subsequently, a series of terrain-sensitivity tests were performed to examine the effect of Taiwan’s topography on PV budget. When Nari was located on the ocean, its PV distribution exhibited the typical feature in a mature oceanic TC. By the time of landfall, its eyewall was contracted and convection was intensified due to the topography. From the budget perspective, PV was redistributed via horizontal and vertical advections. Latent heating term accounted for major PV generation in lower levels during the oceanic and early landfall stage. And it also acts as a major PV sink term at mid-upper levels. The friction term included both effects of eddy mixing and surface friction; hence, it did not just act as a PV sink term. In the terrain-sensitivity experiments, if the Taiwan topography was removed, the friction term began to reduce PV over the Taiwan area in lower levels, which was opposed to that for the full-terrain run. As a result, the existence of Taiwan topography could enhance vertical eddy mixing. When comparing latent heating term and friction term, it is evident that both the Taiwan topography and surface friction are prone to trigger convection, releasing more latent heat and leading to the increase of PV. And the cut-off of ocean fluxes such as sensible heat and latent heat flux will cause the dissipation of the PV ring. In the no-terrain experiment, after the typhoon moves into the ocean again, a larger new PV ring formed. The asymmetry latent heating effect occurred on the land-sea interface not only contributed to the formation of this new PV ring, but make this new PV ring became polygonal as well. This phenomenon may also be a reason that causes the typhoon move in a trochoidal manner afterward. Ming-Jen Yang 楊明仁 2011 學位論文 ; thesis 68 zh-TW
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description 碩士 === 國立中央大學 === 大氣物理研究所 === 99 === Potential Vorticity (PV) is a quantity that combines both dynamic and thermodynamic information, and it is conserved under the adiabatic and frictionless condition. Therefore it is suitable for analyzing tropical cyclones’ (TC) dynamic. In recent years, there have been considerable studies between TCs and the PV. However, it appears that only a few studies using the potential vorticity budget to analyze a real TC case. Thus, what kind of dynamical / thermodynamical interaction processes could be obtained from the PV budget analysis, and what phenomena will be caused by the steep topography of Taiwan are worthy of study. A compressible nonhydrostatic PV budget equation, derived base on Pedlosky (1987) and Schubert et al. (2001), is used here to gain insights into the PV budget evolution of a typhoon from its oceanic stage to landfall stage. The budget is conducted using high spatial resolution (2-km horizontal grid size) hourly outputs from Yang et al. (2008), in which the Pennsylvania State University / National Center for Atmospheric Research Fifth Generation Mesoscale Model was used to simulate Typhoon Nari (2001) and reproduced reasonably-well results as verified against observations. Subsequently, a series of terrain-sensitivity tests were performed to examine the effect of Taiwan’s topography on PV budget. When Nari was located on the ocean, its PV distribution exhibited the typical feature in a mature oceanic TC. By the time of landfall, its eyewall was contracted and convection was intensified due to the topography. From the budget perspective, PV was redistributed via horizontal and vertical advections. Latent heating term accounted for major PV generation in lower levels during the oceanic and early landfall stage. And it also acts as a major PV sink term at mid-upper levels. The friction term included both effects of eddy mixing and surface friction; hence, it did not just act as a PV sink term. In the terrain-sensitivity experiments, if the Taiwan topography was removed, the friction term began to reduce PV over the Taiwan area in lower levels, which was opposed to that for the full-terrain run. As a result, the existence of Taiwan topography could enhance vertical eddy mixing. When comparing latent heating term and friction term, it is evident that both the Taiwan topography and surface friction are prone to trigger convection, releasing more latent heat and leading to the increase of PV. And the cut-off of ocean fluxes such as sensible heat and latent heat flux will cause the dissipation of the PV ring. In the no-terrain experiment, after the typhoon moves into the ocean again, a larger new PV ring formed. The asymmetry latent heating effect occurred on the land-sea interface not only contributed to the formation of this new PV ring, but make this new PV ring became polygonal as well. This phenomenon may also be a reason that causes the typhoon move in a trochoidal manner afterward.
author2 Ming-Jen Yang
author_facet Ming-Jen Yang
Po-Hsu Lin
林柏旭
author Po-Hsu Lin
林柏旭
spellingShingle Po-Hsu Lin
林柏旭
The Potential Vorticity Budget of Typhoon Nari (2001)
author_sort Po-Hsu Lin
title The Potential Vorticity Budget of Typhoon Nari (2001)
title_short The Potential Vorticity Budget of Typhoon Nari (2001)
title_full The Potential Vorticity Budget of Typhoon Nari (2001)
title_fullStr The Potential Vorticity Budget of Typhoon Nari (2001)
title_full_unstemmed The Potential Vorticity Budget of Typhoon Nari (2001)
title_sort potential vorticity budget of typhoon nari (2001)
publishDate 2011
url http://ndltd.ncl.edu.tw/handle/44580436669963717907
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