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1.
The horizontal vorticity equation used in this study was obtained using the equations of motion in the pressure coordinate system without considering friction, to reveal its relationship with vertical shear. By diagnostically analyzing each term in the horizontal vorticity equation during a squall line process that occurred on 19 June 2010, we found that the non-thermal wind term had a negative contribution to the local change of upward movement in the low-level atmosphere, and that its impact changed gradually from negative to positive with altitude, which could influence upward movement in the mid- and upper-level atmosphere greatly. The contribution of upward vertical transport to vertical movement was the largest in the low-level atmosphere, but had negative contribution to the upper-level atmosphere. These features were most evident in the development stage of the squall line. Based on analysis of convection cells along a squall line, we found that in the process of cell development diabatic heating caused the subsidence of constant potential temperature surface and non- geostrophic motion, which then triggered strong convergence of horizontal acceleration in the mid-level atmosphere and divergence of horizontal acceleration in the upper-level atmosphere. These changes of horizontal wind field could cause a counterclockwise increment of the horizontal vorticity around the warm cell, which then generated an increase of upward movement. This was the main reason why the non-thermal wind term had the largest contribution to the strengthening of upward movement in the mid- and upper-level atmosphere. The vertical transport of large value of horizontal vorticity was the key to trigger convection in this squall line process.  相似文献   
2.
本文利用NCEP分析资料、多普勒雷达观测资料、常规气象观测资料以及数值模拟结果,对2016年7月30日发生在华北、辽宁附近的一次强飑线过程中后向入流的演变及成因进行研究。结果表明,此次飑线发生在中纬度新生冷涡槽前,低层有水汽辐合区和地面辐合线对应,且过程中伴有较强的对流有效位能释放。飑线后部中层(冷涡槽后)一直存在α中尺度西风大值带,此大风速带造成了上下层相反的水平涡度,并形成喇叭形环流结构,该结构不同于经典飑线结构。飑线后部水平方向上水平涡度分布不均匀,并形成水平涡度旋度上正下负的分布,即导致中层强风区上部上升运动、下部下沉运动,该下沉运动引发飑线中的后向入流和低层强风速带形成。在中层,飑线的后部边缘始终有较强的风速大值带伴随飑线的发展,该大值带的形成与对流强弱和非热成风涡度有关,对流过程中低层非热成风涡度为负,中上层非热成风涡度为正,导致飑线后部中层西风加速和低层西风减速,有利于后向入流的发展和飑线的维持,当对流减弱时,非热成风涡度与后向入流均减弱。文中给出了后向入流形成演变的概念模式。  相似文献   
3.
Using the WRF (Weather Research Forecast) model, this work performed analysis and simulation on the rainband change during the landfall of Typhoon Haitang (2005) and found that breaking may occur over land and oceans leads to distinct asymmetric precipitation. The breaking is related to the topographic effect as well as interactions between the typhoon and midlatitude systems at upper levels. During the landfall, divergent flows at the 200-hPa level of the South-Asian high combined with divergent flows at the periphery of the typhoon to form a weak, inverted trough in the northwest part of the storm, with the mid- and low-level divergence fields on the west and northwest side of the typhoon center maintaining steadily. It intensifies the upper-level cyclonic flows, in association with positive vorticity rotating counterclockwise together with air currents that travel stepwise into a vorticity zone in the vicinity of the typhoon core, thereby forming a vorticity transfer belt in 22–25? N that extends to the eastern part of the storm. It is right here that the high-level vorticity band is subsiding so that rainfall is prevented from developing, resulting in the rainbelt breaking, which is the principal cause of asymmetric precipitation occurrence. Migrating into its outer region, the banded vorticity of Haitang at high levels causes further amplification of the cyclonic circulation in the western part and transfer of positive vorticity into the typhoon such that the rainband breaking is more distinct.  相似文献   
4.
利用NCEP/NCAR 1°×1°再分析资料,计算了2009年第8号台风“莫拉克”引发浙江沿海地区强降水过程的湿位涡(MPV)和假相当位温(θse),重点分析了正压项(MPV1)和斜压项(MPV2)的正负值变化特征.结果表明,通过判断大气对流不稳定处,θse陡立面密集区,能量锋较强区域,同时结合上升运动,可以作为判断强...  相似文献   
5.
利用2013—2017年6—8月FY-2E和FY-2G地球静止卫星相当黑体温度(Black Body Temperature,TBB)资料、NCEP/NCAR再分析资料,对我国夏季东北冷涡下东北地区MCS的分布和活动特征进行了统计分析,结果表明:(1) MCS的活动具有明显的月际变化和日变化特征,6月对流活动最活跃。MCS的主要移向是东、东北和东南,平均移动距离3.99个经纬距。(2) MCS成熟时刻的面积、偏心率和生命史均小于江淮地区以及中国中东部,云顶高度低于江淮地区,整个生命史表现出发展快消亡慢的特征,与江淮地区相反。(3)基于MCS的定义得到的Z标准,对2016—2017年的MCS作了统计分析并与J标准统计得到的MCS进行对比,得出,两种定义下的MCS环境场特征基本一致,主要表现为MCS多生成于500 hPa槽前和槽后,对流层高层MCS位于双急流之间靠近北支急流的辐散区,南侧急流高度在200 hPa,北侧的急流高度在250 hPa。低层,位于低空急流左侧,低涡南侧、东南侧,有较强的水汽和动量输送。槽前生成的MCS南侧中层存在垂直反环流向MCS输送干暖空气与位涡,槽后生成的MCS两侧均有大值位涡向其输送,同时北侧冷干空气的输送使锋区及上升运动加强,更有利于MCS的形成。(4)两种标准下的MCS造成的降水明显不同,在统计强降水方面Z标准要优于J标准。由于Z标准空间与时间尺度较小,统计得到的MCS较多;但同时会遗漏部分相对弱的MCS。  相似文献   
6.
“莫拉克”台风(2009)登陆前后强度与结构分析   总被引:1,自引:0,他引:1  
利用NCEP每日4次全球预报场(GFS)分析资料、卫星云图资料以及实况观测台风路径、强度资料对0908号台风"莫拉克"在台湾登陆前后其强度、结构变化特征进行天气动力学诊断分析,从而为台风强度、结构预报提供参考依据。结果表明:(1)低层切向风大值区中心所在半径处的切向风非对称性幅度之切向平均值可作为诊断分析台风强度的一个重要参考指标;(2)"莫拉克"中心高层干位涡大值区具有沿着低层切向风大值区中心内侧的切向风梯度密集带向下延伸的趋势;(3)未考虑摩擦、湍流混合的柱坐标切向风运动方程主要有四项是决定切向风变化的,即切向风径向平流项、切向风垂直输送项、惯性离心力作用项以及地转偏向力作用项;(4)台风低层辐合中心在切向上具有沿着切向风梯度密集区移动、发展的趋势。  相似文献   
7.
2000—2009年5、6月华南暖区暴雨形成系统统计分析   总被引:1,自引:0,他引:1  
利用2000—2009年5月和6月的NCEP 1°×1°再分析资料和气象台站常规资料,对产生华南暖区暴雨的500 hPa及以下的环流特征进行统计分析,并将影响暖区暴雨的环流系统划分为三大类型,即切变线型、低涡型和偏南风风速切变辐合型(简称偏南风型)。切变线型在南海夏季风爆发前以冷式切变为主,季风爆发后以暖式切变为主;低涡型在季风爆发前的发生次数远少于季风爆发后,在低涡中心的东北-东南方向最易产生暖区暴雨;偏南风型总体以西风风速切变辐合为主,而南风风速切变辐合在季风爆发后的比例有所增加。对影响暖区暴雨的高空槽分析发现,高原槽对暖区暴雨影响明显,其次为南支槽。低涡型最易受高空槽影响。对各种类型暖区暴雨的合成分析发现,各类型暖区暴雨500 hPa高空槽的位置特点均不相同,暴雨辐合中心均在850hPa以下的低层,副高脊线距雨区约6~8纬距是产生华南暖区暴雨的重要天气形势。  相似文献   
8.
用中尺度对称不稳定“S”判据对9711号远距离台风暴雨过程进行了诊断分析,结果表明;台风远距离雨区存在明显的对称不稳定降水。低层S〈0的区域作对称不稳定区,与后期台风远距离不有比较好的对应,可以作为远距离台风暴雨落区的一个指标。  相似文献   
9.
利用ECMWF资料作初始场,MM4模式输出的结果和Zwack-Okossi方程作诊断工具,对1981年12月20~21日生成在西北太平洋的一次爆发性气旋进行了数值试验和诊断分析。得到气旋的爆发性发展主要是由正涡度平流和非地转场激发,其中涡度平流对气旋发展贡献最大,温度平流的影响则较小,两者主要是在对流层高层起作用,而非地转场则在对流层低层起主要作用。由水汽造成的非绝热加热对本次爆发性气旋的生成影响不大,积云对流潜热的反馈作用更小。另外次天气尺度系统对爆发性气旋形成贡献较小。  相似文献   
10.
This paper uses the ARW-WRF model to carry out a numerical simulation of a warm-sector heavy rainfall event over southern China on the 22–23 May, 2014. A composite analysis method was used to analyze the evolution process and structural features of the convective cells on a convection line during this rainfall event. This analysis identified three stages: (1) Stage of activation: the equivalent potential temperature surfaces as lower layers start to bulge and form warm cells and weak vertical convective cloud towers which are subject to the impact of low-level warm moist updrafts in the rainfall sector; (2) Stage of development: the warm cells continue to bulge and form warm air columns and the convective cloud towers develop upwards becoming stronger as they rise; (3) Stage of maturity: the warm air columns start to connect with the stable layer in the upper air; the convective cloud tower will bend and tilt westward with each increasing in height, and the convection cell is characterized by a “crescent-shaped echo” above the 700hPa plane. During this stage the internal temperature of the cell is higher than the ambient temperature and the dynamic structural field is manifested as intensive vertical upward movement. The large-value centers of the northerly and westerly winds in the middle layer correspond to the warm moist center in the cells and the relatively cold center south of the warm air column. Further analysis shows that the formation of the “crescent-shaped” convective cell is associated with horizontal vorticity. Horizontal vorticity in the center and west of the warm cell experiences stronger cyclonic and anticyclonic shear transformation over time; this not only causes the original suborbicular cell echo shape to develop into a crescent-like shape, but also makes a convection line consisting of cells that develop to the northwest.  相似文献   
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