Mechanism for initial brows-like meso-scale vortex effects on tropical cyclone track  

作　　者：LUO ZheXian PING Fan 

机构地区：[1]Key Laboratory of Meteorological Disaster of Ministry of Education,Nanjing University of Information Science and Technology,Nanjing 210044,China [2]Laboratory of Cloud-Precipitation Physics and Severe Storms(LACS),Institute of Atmospheric Physics,Chinese Academy of Sciences,Beijing 100029,China [3]Wuxi Research Center of Environment Science and Technology,Wuxi 214031,China

出　　处：《Science China Earth Sciences》2012年第4期611-621,共11页中国科学(地球科学英文版)

基　　金：supported by,National Natural Science Foundation of China (Grant Nos.40775038,40875031,40975036 and 40730948);Wuxi Research Center for Environment Science and Technology

摘　　要：We used a two-dimensional quasi-geostrophic barotropic model simulation to study effects of an initial brows-like meso-scale vortex on tropical cyclone (TC) track. Our results show that the impact of each of the three foundational factors (the environ- mental current, the asymmetric structure and the asymmetric convection system) on TC track varies with time and the im- portance of each of the factors is different for the different TC motion time period. They show two kinds of the effects. One is a direct way. The asymmetric outer wind structure and the positive longitudinal wind speed averaged in radial-band (100-300) km in the period of (0-11) h are caused by the introduction of the initial brows-like meso-scale vortex, which results in TC track to turn to the north from the northwest directly. The other is an indirect influence. First, initial TC axisymmetric circula- tion becomes a non-axisyrnmetric circulation after the addition of the meso-scale vortex. The initial non-axisymmetric circula- tion experiences an axisymmetrizational process in the period of (0-11) h. Second, axisymmetrizationed TC horizontal size is enlarged after t=-12 h. Third, both the TC asymmetric structure and the TC energy dispersion induced-anticyclone are intensi- fied, which quickens the TC motion and results in the track to turn to the north indirectly. The TC motion is characterized by the unusual track under the direct and the indirect effect. The formation of the unusual track should be attributed to the com- mon effects of three factors, including the environmental flow, the TC asymmetric structure and the asymmetric convection system.We used a two-dimensional quasi-geostrophic barotropic model simulation to study effects of an initial brows-like meso-scale vortex on tropical cyclone(TC) track.Our results show that the impact of each of the three foundational factors(the environmental current,the asymmetric structure and the asymmetric convection system) on TC track varies with time and the importance of each of the factors is different for the different TC motion time period.They show two kinds of the effects.One is a direct way.The asymmetric outer wind structure and the positive longitudinal wind speed averaged in radial-band(100-300) km in the period of(0-11) h are caused by the introduction of the initial brows-like meso-scale vortex,which results in TC track to turn to the north from the northwest directly.The other is an indirect influence.First,initial TC axisymmetric circulation becomes a non-axisymmetric circulation after the addition of the meso-scale vortex.The initial non-axisymmetric circulation experiences an axisymmetrizational process in the period of(0-11) h.Second,axisymmetrizationed TC horizontal size is enlarged after t=12 h.Third,both the TC asymmetric structure and the TC energy dispersion induced-anticyclone are intensified,which quickens the TC motion and results in the track to turn to the north indirectly.The TC motion is characterized by the unusual track under the direct and the indirect effect.The formation of the unusual track should be attributed to the common effects of three factors,including the environmental flow,the TC asymmetric structure and the asymmetric convection system.

关 键 词：tropical cyclone unusual track environmental flow asymmetric structure asymmetric convection system 

分 类 号：P444[天文地球—大气科学及气象学] P457.8