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一次多弓状中尺度雨带的成因机理及其与水平涡度的关系
引用本文:王丹妮,丁治英,王咏青,窦慧敏,乔娜,王联军. 一次多弓状中尺度雨带的成因机理及其与水平涡度的关系[J]. 热带气象学报, 2020, 36(1): 131-144. DOI: 10.16032/j.issn.1004-4965.2020.013
作者姓名:王丹妮  丁治英  王咏青  窦慧敏  乔娜  王联军
作者单位:1.南京信息工程大学气象灾害教育部重点实验室/气候与环境变化国际合作联合实验室/气象灾害预报预警与评估协同创新中心,江苏南京 210044
基金项目:国家重点基础研究发展计划2015CB453201国家自然科学基金41975054国家自然科学基金41530427国家自然科学基金41790471国家自然科学基金41775040
摘    要:用WRF中尺度数值模式、NCEP/NCAR再分析资料、多普勒雷达观测资料等,对2018年5月5日发生在我国华中地区的一次多弓状雨带降水过程的形成机理及其与水平涡度的关系进行分析发现:雨带发生在切变线南侧的西南气流中,多弓状雨带出现前,大尺度高低层气旋式曲率的水平涡度和对流有效位能为降水提供了有利于上升运动的背景场。弓状雨带最初形成在对流不稳定和低层气流辐合条件下,局地强降水引发的下沉运动使中低层大风出现,大风中心南侧反气旋式的环流与背景场中的西南气流汇合构成了短波槽,尾部雨带出现在短波槽中,弓状头部生成于北侧的气旋式风场切变中,大风中心相较南北两侧更快的移速使雨带中部向前侧凸起。流场上的短波槽发生在700 hPa以下,在西南气流的背景场下,该槽向前后两侧的双向传播是多弓状雨带形成的重要触发因子。中尺度弓状雨带附近低层的水平涡度在强盛期、减弱期和消散期有着明显不同的结构特征;而在高层,雨带发展时和强盛期都为气旋式水平涡度控制,减弱期多为反气旋式水平涡度控制。

关 键 词:多弓状雨带  水平涡度  负浮力  对流有效位能  短波槽
收稿时间:2019-05-30

THE RELATIONSHIP BETWEEN THE FORMATION MECHANISM OF A MULTI-MESOSCALE-BOW-RAINBAND AND HORIZONTAL VORTICITY
WANG Dan-ni,DING Zhi-ying,WANG Yong-qing,DOU Hui-min,QIAO N,WANG Lian-jun. THE RELATIONSHIP BETWEEN THE FORMATION MECHANISM OF A MULTI-MESOSCALE-BOW-RAINBAND AND HORIZONTAL VORTICITY[J]. Journal of Tropical Meteorology, 2020, 36(1): 131-144. DOI: 10.16032/j.issn.1004-4965.2020.013
Authors:WANG Dan-ni  DING Zhi-ying  WANG Yong-qing  DOU Hui-min  QIAO N  WANG Lian-jun
Affiliation:1.Key Laboratory of Meteorological Disaster, Ministry of Education/ Joint International Research Laboratory of Climate and Environment Change/ Collaborative Innovation Center on Forecast and Evaluation of Meteorological Disasters, Nanjing University of Information Science and Technology, Nanjing 210044, China2.Shuangfeng Meteorological Administration, Loudi 417700, China
Abstract:A multi-bow-rainband process in central China on May 5, 2018 was simulated using WRF mesoscale numerical model, NCEP/NCAR reanalysis data and Doppler radar observation data. The relationship between the formation of multi-bow-rainband and horizontal vorticity was studied. It is found that these rainbands occurred in the southwest airflow on the south of the shear line. Before the multi-bow-rainband emerged, the large-scale clockwise-rotating horizontal vorticity in the high and low level and convective effective potential energy provided a favorable background for precipitation. The bow-rainband was originally formed under the condition of convective instability and low-level airflow convergence. The gale in the middle and low level appeared as a result of downward motion caused by local heavy precipitation. The anticyclonic circulation on the south side of low-level gale center merged with southwest airflow in the background field, forming a short-wave trough where the tail of rainband emerged. The head of the bow-rainband generated in the cyclonic circulation on the north side of gale center. The gale center moved faster than the north and south side of the gale, inducing the middle of the rainband convex to move forward. The short-wave trough of airflow field occurred below 700hPa in the background of south-west airflow, and the two-way propagation (forward and backward) of this trough was an important trigger for the formation of multi-bow-rainband. The horizontal vorticity in the low level near the mesoscale-bow-rainband had different structural characteristics during the strong, weak and dissipative periods of the mesoscale-bow-rainband. In the high level, horizontal vorticity was cyclonic in the developing and strong periods of rainbands, whereas it was anticyclonic in the weak period of rainbands.
Keywords:multi-bow-rainband   horizontal vorticity   negative buoyancy   convective effective potential energy   short wave trough
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