期刊文献+

Evaluation of the Ocean Feedback on Height Characteristics of the Tropical Cyclone Boundary Layer

Evaluation of the Ocean Feedback on Height Characteristics of the Tropical Cyclone Boundary Layer
原文传递
导出
摘要 In this study, the interaction between the tropical cyclone(TC) and the underlying ocean is reproduced by using a coupled atmosphere-ocean model. Based on the simulation results, characteristics of the TC boundary layer depth are investigated in terms of three commonly used definitions, i.e., the height of the mixed layer depth(HVTH), the height of the maximum tangential winds(HTAN), and the inflow layer depth(HRAD). The symmetric height of the boundary layer is shown to be cut down by the ocean response, with the decrease of HVTH slightly smaller than that of HTAN and HRAD. The ocean feedback also leads to evident changes in asymmetric features of the boundary layer depth. The HVTH in the right rear of the TC is significantly diminished due to presence of the cold wake, while the changes of HVTH in other regions are rather small. The decreased surface virtual potential temperature by the cold wake is identified to be dominant in the asymmetric changes in HVTH. The impacts of ocean response on the asymmetric distributions of HTAN are nonetheless not distinct, which is attributed to the highly axisymmetric property of tangential winds. The HRAD possesses remarkable asymmetric features and the inflow layer does not exist in all regions, an indication of the inadequacy of the definition based on symmetric inflow layer depth. Under influences of the cold wake, the peak inflow area rotates counterclockwise distinctly. As a consequence, the HRAD becomes deeper in the east while shallower in the west of the TC. In this study, the interaction between the tropical cyclone(TC) and the underlying ocean is reproduced by using a coupled atmosphere-ocean model. Based on the simulation results, characteristics of the TC boundary layer depth are investigated in terms of three commonly used definitions, i.e., the height of the mixed layer depth(HVTH), the height of the maximum tangential winds(HTAN), and the inflow layer depth(HRAD). The symmetric height of the boundary layer is shown to be cut down by the ocean response, with the decrease of HVTH slightly smaller than that of HTAN and HRAD. The ocean feedback also leads to evident changes in asymmetric features of the boundary layer depth. The HVTH in the right rear of the TC is significantly diminished due to presence of the cold wake, while the changes of HVTH in other regions are rather small. The decreased surface virtual potential temperature by the cold wake is identified to be dominant in the asymmetric changes in HVTH. The impacts of ocean response on the asymmetric distributions of HTAN are nonetheless not distinct, which is attributed to the highly axisymmetric property of tangential winds. The HRAD possesses remarkable asymmetric features and the inflow layer does not exist in all regions, an indication of the inadequacy of the definition based on symmetric inflow layer depth. Under influences of the cold wake, the peak inflow area rotates counterclockwise distinctly. As a consequence, the HRAD becomes deeper in the east while shallower in the west of the TC.
出处 《Acta meteorologica Sinica》 SCIE 2013年第6期910-922,共13页
基金 Supported by the China Meteorological Administration Special Public Welfare Research Fund (GYHY201106004) National Natural Science Foundation of China (41230421,41005029,and 41105065)
关键词 tropical cyclone boundary layer ocean feedback air-sea interaction tropical cyclone boundary layer ocean feedback air-sea interaction
  • 相关文献

参考文献38

  • 1Anthes, R. A., and S. W. Chang, 1978: Response of the hurricane boundary layer to changes of sea surface temperature in a numerical model. J. Atmos. Sci., 35, 1240–1255.
  • 2Bender, M. A., and I. Ginis, 2000: Real-case simulations of hurricane-ocean interaction using a high-resolution coupled model: Effects on hurricane intensity. Mon. Wea. Rev., 128, 917–946.
  • 3Betts, A. K., and M. J. Miller, 1986: A new convective adjustment scheme. Part II: Single column tests using GATE wave, BOMEX, ATEX and arctic airmass data sets. Quart. J. Roy. Meteor. Soc., 112, 693–709.
  • 4Bryan, G. H., and R. Rotunno, 2009: The maximum intensity of tropical cyclones in axisymmetric numerical model simulations. Mon. Wea. Rev., 137, 1770–1789.
  • 5Chen, S., T. J. Campbell, H. Jin, et al., 2010: Effect of two-way air-sea coupling in high and low wind speed regimes. Mon. Wea. Rev., 138, 3579–3602.
  • 6Duan, Y. H., R. S. Wu, R. L. Yu, et al., 2013: Numerical simulation of tropical cyclone intensity change with a coupled air-sea model. Acta Meteor. Sinica, 27, doi: 10.1007/s13351-013-0503-2. (in press).
  • 7Emanuel, K. A., 1986: An air-sea interaction theory for tropical cyclones. Part I: Steady-state maintenance. J. Atmos. Sci., 43, 585–605.
  • 8Emanuel, K. A.,1988: The maximum intensity of hurricanes. J. Atmos. Sci., 45, 1143–1155.
  • 9Emanuel, K. A.,1995: Sensitivity of tropical cyclones to surface exchange coefficients and a revised steady-state model incorporating eye dynamics. J. Atmos. Sci., 52, 3969–3976.
  • 10Hogsett, W., and D.-L. Zhang, 2009: Numerical simulation of Hurricane Bonnie (1998). Part III: Energetics. J. Atmos. Sci., 66, 2678–2696.

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部