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1.
用Micaps,地面自动站加密资料,新一代多普勒天气雷达资料和GFS 0.5°×0.5°再分析资料以及中尺度WRF模式输出资料对2014夏季发生在宁波市地区的一个局地强雷暴天气过程进行了分析总结,得出:宁波新一代多普勒雷达反射率回波出现弱窄带回波时,对应边界层辐合线海风锋,在有利天气形势背景下易诱发强对流的发生发展。此次强雷雨过程是在有利天气背景条件下发生的,强对流发生在局地层结不稳定和较好的水汽条件下;利用中尺度WRF模式输出资料进行分析看到,海风锋的锋生造成的地转强迫促使次级环流加强,在东西风辐合线西侧有垂直上升运动出现;海风锋本身有一辐合抬升区,辐合上升运动的加强为雷暴的发生提供了有利的动力条件,从而触发了该地区不稳定能量的强烈释放,促使了雷暴的新生发展。  相似文献   

2.
渤海湾海风锋与雷暴天气   总被引:10,自引:1,他引:9       下载免费PDF全文
王彦  于莉莉  朱男男  汪靖 《高原气象》2011,30(1):245-251
利用天津新一代天气雷达探测到的2008年6~9月共56次渤海湾海风锋天气过程资料、 255 m高的气象铁塔资料及相应的自动气象站资料, 统计分析了渤海湾海风锋的气候特征, 包括渤海湾海风锋出现的时间、 频率和海风锋触发形成雷暴天气的演变特征。结果表明, 2008年6~9月雷达共观测到渤海湾海风锋56次; 每日海风锋的形成时间有所不同, 最早形成时间是09:30(北京时, 下同), 最晚在16:00; 维持时间也各有长短, 最长维持时间为6.5 h, 最短的仅1 h; 伸展到内陆的一般距离为70~80 km, 最远距离达120 km, 高度一般为1.5 km, 最高为2.0 km。同时, 结合2002-2007年典型的海风锋天气个例分析表明, 单一海风锋由于水平范围小, 垂直厚度最高为2 km, 一般不能形成雷暴天气。但是, 当它与西边很弱的冷锋形成一定角度(30°~90°)碰撞时, 在碰撞的交叉处能够形成雷暴天气; 当海风锋与其它系统呈追赶碰撞时, 一般不能形成雷暴天气; 当海风锋与其它系统平行碰撞时, 有时雷暴加强, 有时雷暴减弱。  相似文献   

3.
海风锋在渤海西岸局地暴雨过程中的作用   总被引:9,自引:4,他引:5  
东高红  何群英  刘一玮  解以扬  戴云伟 《气象》2011,37(9):1100-1107
利用常规观测资料、地面加密自动站资料、多普勒雷达观测资料及中尺度TJ-WRF模式输出资料,对2009年7月6日天津宁河地区出现的暴雨天气过程进行了分析,重点分析了渤海湾海风锋对沿岸局地暴雨的触发机理。结果表明:此次局地暴雨过程是在有利天气背景条件下发生的,暴雨发生地存在局地层结不稳定和较好的水汽条件。海风锋本身有一辐合抬升区,区域内有弱对流存在;当海风锋移到局地存在层结不稳定且水汽充足的区域,其抬升区的辐合上升运动迅速加强,从而触发该地区雷暴的新生发展;海风锋与迎面移来的雷暴相遇,会对雷暴的加速发展起到加强作用。利用中尺度WRF模式输出资料进行分析看到,两条辐合线相交处易激发出强雷暴,雷暴出现在近地层大气暖干区的北端、湿空气的交汇处;海风锋对雷暴的新生发展有明显的触发抬升作用。  相似文献   

4.
一次海风锋触发的强对流天气分析   总被引:5,自引:1,他引:5       下载免费PDF全文
利用自动气象站、多普勒天气雷达等各种观测资料,分析了2009年6月5日江苏出现的罕见大范围强对流天气,同时利用WRFV3模式对这次海风锋的发生、发展过程进行了模拟。结果表明,由于地面加热不均和海陆温湿差异导致的变形场锋生所形成的海风锋,是造成这次强对流天气过程的主要中尺度激发和强化系统。对流云团进入锋区后在切变线的辐合作用下发展,并随平均风向向前传播。海风锋在雷暴高压下沉出流的推动下,移动路径偏离主回波,在移动过程中其后部不仅激发出对流单体,还组织新的MCS发展。海风锋起到了加强和触发强对流天气的作用,对流单体进入海风锋后发展剧烈,垂直速度和低层辐合明显加大。另外,在有利的温湿条件下,雷暴高压的出流能加强海风锋的上升气流。  相似文献   

5.
对2007年8月13日天津多普勒天气雷达(CIN RAD WSR/98D)探测的雷暴天气个例进行分析,结果表明:此次雷暴天气是由渤海湾海风锋与阵风锋碰撞形成的;碰撞后,在海风锋前端、阵风锋前部有新的雷暴单体形成;阵风锋后部的对流回波主体加强,对流回波主体由椭圆状加强为典型的弓状。应用天津36个自动气象站的地面六要素资料和北京850 hPa以上探空资料,组成新的诊断资料,对该个例进行诊断分析,结果表明:雷达探测的海风锋前端具有较强的低层垂直风切变梯度和露点温度梯度大值区,海风锋前沿与0~3 km垂直风切变梯度密集区相对应,且与露点温度梯度变化较快的区域基本吻合;海风锋与阵风锋相互碰撞时,0~3 km垂直风切变在2 h内变化较快,且有明显的增加趋势,CAPE(convective available potential energy,对流有效位能)值在雷暴形成前有较明显增加;随着雷暴天气结束,上述特征随之消失。  相似文献   

6.
利用常规气象观测资料、多普勒气象雷达资料、浙江省自动站加密资料、NCEP/FNL再分析资料,结合高分辨率中尺度数值模式WRF对杭州湾地区2016年7月28日一次海风锋触发雷暴天气的发生、发展演变特征进行数值模拟。结果表明:1)海风锋是此次强雷暴天气过程的主要触发系统。2)中尺度模式WRF较好地模拟出此次雷暴过程的降水和低层风场、温度场分布以及海风锋水平垂直结构。3)海风锋对局地比湿及涡度特征的加强有明显的促进作用,为雷暴的发生发展提供有利的水汽和动力条件。4)分析对流参数演变曲线的突变位置,对雷暴发生的时间有一定的指示和预报意义,杭州湾南侧单纯的海风锋也可以触发雷暴的发生发展。  相似文献   

7.
城市热岛与海风锋叠加作用对一次局地强降水的影响   总被引:1,自引:2,他引:1  
东高红  刘一玮  孙蜜娜  戴云伟 《气象》2013,39(11):1422-1430
利用常规观测资料、天津255 m气象塔资料、多普勒雷达资料和VDRAS反演资料及中尺度TJ WRF模式输出资料,对2010年8月16日天津城区出现的一次局地强降水过程进行分析,重点分析了城市热岛与海风锋叠加作用对此次局地强降水的触发机制。结果表明:此次局地强降水发生在低层槽后弱的反环流条件下,具有明显的γ中尺度对流降水特征;城市热岛效应能造成局地的热力不均匀,这对形成地面中尺度辐合线非常有利。海风锋由岸边向市区移动中与中尺度辐合线相遇,能激发局地不稳定能量的释放,从而产生强对流天气。城市热岛对海风锋的移动有明显阻挡作用;当海风锋移到城市热岛效应明显区域附近时,其后侧气流会出现明显分支绕流和爬升现象,而且两者相遇处的辐合上升运动会迅速加强,这为该地不稳定能量的释放及雷暴的发生发展提供了有利的动力热力条件。中尺度TJ WRF模式可以很好地模拟出这一现象。  相似文献   

8.
利用浙江省常规气象站观测资料、地面自动站加密资料、新一代多普勒天气雷达资料、NCEP GFS分析资料以及WRF中尺度模式,对2013年7月29日发生在宁波市地区的一个局地强雷暴天气过程进行了诊断分析和数值模拟。通过对天气环流和数值模拟结果的分析发现:本次强雷暴过程发生在较稳定的大气背景下,主要影响系统是中尺度辐合线海风锋;多普勒雷达出现弱窄带回波时,对应中尺度辐合线海风锋;海风锋向内陆推进时,对应站点温度降低、湿度增大。WRF模式能较好地模拟出此次雷暴过程以及宁波地区低层海风锋环流,高空回流随时间和空间的演变特征;海风锋的锋生造成的地转强迫促使次级环流加强,在东西风辐合线西侧有垂直上升运动出现;通过与敏感试验的对比可知,海陆热力差异是影响雷暴降水强度、海风锋水平垂直环流的重要因素。  相似文献   

9.
渤海湾海风锋雷达回波特征分析   总被引:7,自引:3,他引:7  
王彦  李胜山  郭立  冯金湖  王庆元  东高红 《气象》2006,32(12):23-28
应用天津新一代天气雷达和相应的自动气象站资料,统计分析雷达监测到的4次渤海湾海风锋的特点,并研究渤海湾海风锋与强对流天气形成、发展和消散过程演变特征。结果表明:渤海湾海风锋在低仰角(O.5°或1.5°)基本反射率产品中表现为平行于渤海湾的窄带弱回波,强度一般仅维持在15~25dBz,长度约为100~300km,宽度随着季节、天气背景场的变化而变化;并且移动速度非常缓慢,基本维持在10~15km·h~(-1)。低仰角(O.5°或1.5°)的基本速度产品上,海风锋几乎呈准静止的零速度窄带回波。当海风锋与弱冷锋相遇时,相遇交叉处能够产生强对流天气;而单一海风锋不能产生强对流天气,仅能改变气温和风向等气象要素特征。  相似文献   

10.
利用地面自动气象站观测数据、多普勒雷达探空数据、FY卫星云图反演数据,对2008年6月5日发生在北部湾海域的一次海风锋触发形成的强对流天气进行了综合分析,归纳出本次北部湾海风锋系统活动的特征。结果表明,本次海风锋为一个中-β尺度对流系统,主要受偏南海风、偏北陆风和出海高压后部东风波动的共同影响而形成,锋面呈现东西两端,其中东段深入内陆约150km。  相似文献   

11.
Using the International Comprehensive Ocean-Atmosphere Data Set(ICOADS) and ERA-Interim data, spatial distributions of air-sea temperature difference(ASTD) in the South China Sea(SCS) for the past 35 years are compared,and variations of spatial and temporal distributions of ASTD in this region are addressed using empirical orthogonal function decomposition and wavelet analysis methods. The results indicate that both ICOADS and ERA-Interim data can reflect actual distribution characteristics of ASTD in the SCS, but values of ASTD from the ERA-Interim data are smaller than those of the ICOADS data in the same region. In addition, the ASTD characteristics from the ERA-Interim data are not obvious inshore. A seesaw-type, north-south distribution of ASTD is dominant in the SCS; i.e., a positive peak in the south is associated with a negative peak in the north in November, and a negative peak in the south is accompanied by a positive peak in the north during April and May. Interannual ASTD variations in summer or autumn are decreasing. There is a seesaw-type distribution of ASTD between Beibu Bay and most of the SCS in summer, and the center of large values is in the Nansha Islands area in autumn. The ASTD in the SCS has a strong quasi-3a oscillation period in all seasons, and a quasi-11 a period in winter and spring. The ASTD is positively correlated with the Nio3.4 index in summer and autumn but negatively correlated in spring and winter.  相似文献   

12.
<正>The Taal Volcano in Luzon is one of the most active and dangerous volcanoes of the Philippines. A recent eruption occurred on 12 January 2020(Fig. 1a), and this volcano is still active with the occurrence of volcanic earthquakes. The eruption has become a deep concern worldwide, not only for its damage on local society, but also for potential hazardous consequences on the Earth’s climate and environment.  相似文献   

13.
The moving-window correlation analysis was applied to investigate the relationship between autumn Indian Ocean Dipole (IOD) events and the synchronous autumn precipitation in Huaxi region, based on the daily precipitation, sea surface temperature (SST) and atmospheric circulation data from 1960 to 2012. The correlation curves of IOD and the early modulation of Huaxi region’s autumn precipitation indicated a mutational site appeared in the 1970s. During 1960 to 1979, when the IOD was in positive phase in autumn, the circulations changed from a “W” shape to an ”M” shape at 500 hPa in Asia middle-high latitude region. Cold flux got into the Sichuan province with Northwest flow, the positive anomaly of the water vapor flux transported from Western Pacific to Huaxi region strengthened, caused precipitation increase in east Huaxi region. During 1980 to 1999, when the IOD in autumn was positive phase, the atmospheric circulation presented a “W” shape at 500 hPa, the positive anomaly of the water vapor flux transported from Bay of Bengal to Huaxi region strengthened, caused precipitation ascend in west Huaxi region. In summary, the Indian Ocean changed from cold phase to warm phase since the 1970s, caused the instability of the inter-annual relationship between the IOD and the autumn rainfall in Huaxi region.  相似文献   

14.
The atmospheric and oceanic conditions before the onset of EP El Ni?o and CP El Ni?o in nearly 30 years are compared and analyzed by using 850 hPa wind, 20℃ isotherm depth, sea surface temperature and the Wheeler and Hendon index. The results are as follows: In the western equatorial Pacific, the occurrence of the anomalously strong westerly winds of the EP El Ni?o is earlier than that of the CP El Ni?o. Its intensity is far stronger than that of the CP El Ni?o. Two months before the El Ni?o, the anomaly westerly winds of the EP El Ni?o have extended to the eastern Pacific region, while the westerly wind anomaly of the CP El Ni?o can only extend to the west of the dateline three months before the El Ni?o and later stay there. Unlike the EP El Ni?o, the CP El Ni?o is always associated with easterly wind anomaly in the eastern equatorial Pacific before its onset. The thermocline depth anomaly of the EP El Ni?o can significantly move eastward and deepen. In addition, we also find that the evolution of thermocline is ahead of the development of the sea surface temperature for the EP El Ni?o. The strong MJO activity of the EP El Ni?o in the western and central Pacific is earlier than that of the CP El Ni?o. Measured by the standard deviation of the zonal wind square, the intensity of MJO activity of the EP El Ni?o is significantly greater than that of the CP El Ni?o before the onset of El Ni?o.  相似文献   

15.
Various features of the atmospheric environment affect the number of migratory insects, besides their initial population. However, little is known about the impact of atmospheric low-frequency oscillation(10 to 90 days) on insect migration. A case study was conducted to ascertain the influence of low-frequency atmospheric oscillation on the immigration of brown planthopper, Nilaparvata lugens(Stl), in Hunan and Jiangxi provinces. The results showed the following:(1) The number of immigrating N. lugens from April to June of 2007 through 2016 mainly exhibited a periodic oscillation of 10 to 20 days.(2) The 10-20 d low-frequency number of immigrating N. lugens was significantly correlated with a low-frequency wind field and a geopotential height field at 850 h Pa.(3) During the peak phase of immigration, southwest or south winds served as a driving force and carried N. lugens populations northward, and when in the back of the trough and the front of the ridge, the downward airflow created a favorable condition for N. lugens to land in the study area. In conclusion, the northward migration of N. lugens was influenced by a low-frequency atmospheric circulation based on the analysis of dynamics. This study was the first research connecting atmospheric low-frequency oscillation to insect migration.  相似文献   

16.
基于最新的GTAP8 (Global Trade Analysis Project)数据库,使用投入产出法,分析了2004年到2007年全球贸易变化下南北集团贸易隐含碳变化及对全球碳排放的影响。结果显示,随着发展中国家进出口规模扩张,全球贸易隐含碳流向的重心逐渐向发展中国家转移。2004年到2007年,发达国家高端设备制造业和服务业出口以及发展中国家资源、能源密集型行业及中低端制造业出口的趋势加强,该过程的生产转移导致全球碳排放增长4.15亿t,占研究时段全球贸易隐含碳增量的63%。未来发展中国家的出口隐含碳比重还将进一步提高。贸易变化带来的南北集团隐含碳流动变化对全球应对气候变化行动的影响日益突出,发达国家对此负有重要责任。  相似文献   

17.
正ERRATUM to: Atmospheric and Oceanic Science Letters, 4(2011), 124-130 On page 126 of the printed edition (Issue 2, Volume 4), Fig. 2 was a wrong figure because the contact author made mistake giving the wrong one. The corrected edition has been updated on our website. The editorial office is sincerely sorry for any  相似文献   

18.
19.
Index to Vol.31     
正AN Junling;see LI Ying et al.;(5),1221—1232AN Junling;see QU Yu et al.;(4),787-800AN Junling;see WANG Feng et al.;(6),1331-1342Ania POLOMSKA-HARLICK;see Jieshun ZHU et al.;(4),743-754Baek-Min KIM;see Seong-Joong KIM et al.;(4),863-878BAI Tao;see LI Gang et al.;(1),66-84BAO Qing;see YANG Jing et al.;(5),1147—1156BEI Naifang;  相似文献   

20.
正Journal of Meteorological Research is an international academic journal in atmospheric sciences edited and published by Acta Meteorologica Sinica Press,sponsored by the Chinese Meteorological Society.It has been acting as a bridge of academic exchange between Chinese and foreign meteorologists and aiming at introduction of the current advancements in atmospheric sciences in China.The journal columns include Articles.Note and Correspondence,and research letters.Contributions from all over the world are welcome.  相似文献   

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