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1.
利用LS8000闪电定位系统2009—2011年的地闪观测资料对上海及周边地区(120~122.5°E,30~32°N)的地闪活动特征进行了研究。结果表明:分析区域内正地闪的比例约占8.5%,大电流地闪(电流绝对值大于50kA)的比例约为5.6%。地闪活动主要集中在6—9月,峰值出现在8月;日变化上,12:00—19:00闪电活动最为活跃,峰值出现在14:00,凌晨闪电活动最弱。从日变化上来说,正地闪和大电流地闪比例在地闪活动较强时段低于地闪活动较弱时段;在月分布上,在地闪活动最强的夏季,正地闪比例普遍在10%以下,在地闪活动较弱的春、秋、冬季,正地闪比例普遍在10%以上。以北纬31°为界,分析区域北部地闪密度基本在6~12次·km-2·a-1以上,南部基本在2.4~4.8次·km-2·a-1。同时陆地上的地闪密度要显著高于湖泊和海洋上的地闪密度,而海洋上的正地闪比例和大电流地闪比例要显著高于陆地。闪电空间分布的时间变化说明,下午地闪活动主要出现在陆地,而凌晨地闪主要出现在水体附近,其它时段则表现出过渡特征,这与下垫面的加热作用紧密相关。  相似文献   

2.
利用TRMM/LIS 0.1°超高分辨率闪电定位产品, 分析了浙江省及周边地区(117.5~123.0°E, 26~32°N)卫星闪电资料的时空分布特点; 并结合中国区域地面气象要素驱动数据集、亚洲大陆气溶胶光学厚度数据集, 分析了该区域闪电与气象要素的关系。结果表明: 研究区域内闪电平均密度为5.97 f1/(km2·a), 其中陆地闪电平均密度为7.94 f1/(km2·a), 海洋闪电平均密度为2.09 f1/(km2·a), 陆地闪电平均密度为海洋闪电平均密度的3.80倍; 平均闪电密度值逐月变化特征在陆地和海洋区域有很好的一致性, 夏季闪电密度最大, 冬季闪电密度值最小; 陆地闪电密度日变化呈现单峰结构, 海洋闪电密度日变化呈现双峰双谷波形。该区域陆地气温、地面辐射、比湿及降水率均与闪电密度的月变化成正相关, 其中地面降水率和闪电密度月变化相关系数最高, 为0.858 0;气溶胶光学厚度与闪电密度月变化呈现弱的负相关, 相关系数为-0.397 8。   相似文献   

3.
基于ADTD系统的闪电频次分布特征分析   总被引:7,自引:2,他引:5  
闪电频次是反映雷电活动强弱特征的重要参数。在统计分析重庆市ADTD系统地闪监测资料的基础上,重点分析闪电频次的极性、幅值、雷电流波头陡度和时间分布特征,同时利用GIS软件获取地闪点的高程属性,初步分析了其空间分布特征。结果表明:闪电频次随极性、雷电流幅值和陡度不同而差异显著;闪电雷电流幅值和陡度的频次呈现对数正态分布;闪电频次的月际分布特征表现为正闪集中在4—7月,负闪集中在7—8月;日际分布特征表现为闪电频次主要集中在03:00—07:00和15:00—19:00;在高度空间分布上闪电发生频次最高地区为海拔300~500 m的区域,以后呈现随高度上升而呈递减趋势;在纬度分布中,高频区域分布在28.9~30.3 °N,次高频地区为30.7~31.5 °N之间;经度分布特征来看,呈现双峰双谷(两个峰值区分别为105.9~106.9 °E、108.1~109.1 °E);高幅值区域正负闪频次比值高于低幅值区域;闪电频次较高地方集中在重庆市东北部、东南部和西部等地。在此基础上获得了重庆地区的雷电流幅值和陡度频次分布表达式,为雷电防护提供了重要的理论基础。   相似文献   

4.
闪电初始阶段和尺度判别方法及其特征   总被引:5,自引:5,他引:0       下载免费PDF全文
基于LMA三维闪电定位数据,对2004年10月5日发生于美国新墨西哥州的一次超级单体过程的闪电初始及其尺度特征进行研究,提出闪电初始阶段自动判别及其特征参量提取方法,并给出参量分布特征。结果显示:闪电初始阶段上行负先导(下行负先导)的持续时间中值为13.5 ms(7.5 ms),三维位移中值为1.4 km(1.0 km),三维平均位移速度中值为9.2×104 m·s-1(1.2×105 m·s-1),上行负先导速度随时间递减,下行反之,二者与垂直方向夹角的中值分别为40°和54°。表征闪电尺度的闪电凸壳面积和闪电总长度的概率密度呈负幂函数分布,在小值方向分布更为集中。闪电水平延展距离中值为6.1 km,垂直延展距离中值为4.3 km,约83%的闪电其水平延展距离大于垂直延展距离;闪电的持续时间中值为271.0 ms。分析发现,以水平延展为主的闪电起始高度分布峰值位于8.5 km,以垂直延展为主的闪电起始高度分布峰值位于11 km。闪电初始阶段位移方向越接近水平,对应闪电垂直延展越小,说明闪电初始段的传播方向对于闪电垂直延展具有重要影响。  相似文献   

5.
北京及其周边地区夏季地闪活动时空特征分析   总被引:13,自引:9,他引:13       下载免费PDF全文
利用M-LDARS闪电定位系统对北京及其周边地区1995~1997年6~9月的闪电观测数据, 分析闪电活动的时空分布特征。结果表明:闪电活动在时间分布上存在两个峰值时段, 13 :00~21:00和23:00~次日05 :00。通过对总地闪、分时段及峰值时段的地闪密度分析, 发现北京及周边地区闪电活动有几个明显的集中区域, 地闪高密度区主要出现在下垫面为山脉和水体的地方, 闪电活动与下垫面的水汽条件关系密切, 且正、负地闪的空间分布也呈现较大差异, 表明雷暴云的电荷结构存在一定差异。  相似文献   

6.
利用山东电网雷电监测定位系统(SLDN)2005—2007年的地闪定位资料,对胜利油田主体地区闪电活动的时空分布特征及其规律进行研究。结果表明:该地区逐月闪电次数差异较大,闪电的季节变化明显,7月份闪电最多。近3年闪电活动日分布呈现双峰形式,最高峰值时间段在00:00-01:00之间,次高峰值时段出现在17:00—18:00之间。空间分布上,闪电多发生在在广饶县南部地区和黄河入海口地区。正地闪占总地闪的百分比为7%,正闪的平均强度为51.3kA,负闪的平均强度为35.36kA。  相似文献   

7.
利用2019-2020年风云四号气象卫星A星(FY-4A)多通道扫描成像辐射计(AGRI)提供的云顶数据和地基全球闪电定位网(WWLLN)提供的闪电数据,结合MICAPS气象观测站和海洋浮标记录的极大风数据,研究南海区域(5°~30°N,105°~125°E)71次雷暴大风过程的时空分布及其闪电和对流活动特征。结果表明:观测站记录的雷暴大风主要分布在南海北部;雷暴大风主要发生在5-9月,峰值出现在8月,3月发生次数最少;雷暴大风主要发生在07:00-12:00(北京时,下同),10:00频次最高,午后频次减少。雷暴大风闪电密度的极大值分布在广东南部近海区域,且闪电集中发生在距离观测站40~80 km半径范围内;孤立雷暴大风过程首次闪电跃变的发生时刻相对大风峰值时刻超前30 min至2 min。在对流特征方面,在雷暴大风风速峰值时刻,观测站处的云顶亮温为200~220 K,云顶高度为12.5~15 km。孤立雷暴大风云团云顶亮温最低值(即最强对流发生位置)与大风观测站点的距离平均为77.2 km,云顶亮温平均相差2.6 K。  相似文献   

8.
用TRMM/LIS资料分析长江三角洲地区的闪电活动   总被引:10,自引:2,他引:10       下载免费PDF全文
统计分析了1998~2004年长江三角洲(长三角)地区由星载闪电成像传感器(LIS)观测的闪电资料,发现了该地区LIS闪电活动的一些时空分布特征:闪电次数的年差异较大,最多年份是最少年份的3倍;7~8月盛夏季节是闪电高发期,闪电次数和日数分别占全年的70%和60%;闪电高发期间的抬升指数(IL)小于-2℃;7~8月闪电主要集中于午后,3~6月则集中在上半夜;上海地区单日LIS闪电次数超过8次时,多伴有强对流天气和短时强降水;长三角地区的闪电活动区主要分布在上海的东部,部分沿江、沿湖地区和浙江的龙门山等山区;水域闪电少于陆地,大城市城区下风方向闪电活动较多,部分雷暴刚入海时有加强的趋势。分析表明:太阳辐射的季节变化和日变化等是造成闪电时间分布的主要原因;地形的动力作用和下垫面的物理特性及其差异是造成气候意义上中小尺度闪电空间分布差异的主要原因。文章对LIS闪电定位资料进行了探测效率订正,根据LIS注视时间计算了闪电密度,并与地基闪电定位资料和多普勒天气雷达资料进行了对比。LIS闪电活动特征的分析,对雷暴预警和防灾减灾有指导意义。  相似文献   

9.
卫星观测的我国近海海域闪电分布特征   总被引:1,自引:1,他引:0       下载免费PDF全文
利用星载闪电探测仪OTD(optical transient detecter)和LIS(lightning imaging sensor)所获取的1995年6月—2006年4月的卫星闪电资料,结合NOAA Optimum Interpolation SST海温资料,分析我国近海海域的闪电分布时空特征以及闪电活动与该海域海温之间的相关性。结果表明:我国近海闪电密度平均值为3.39 fl·km~(-2)·a~(-1),其中,南海和渤海的闪电活动相对频繁,随着与海岸线间距离以及纬度的增加,该海域闪电密度逐渐下降;在春季和冬季,黑潮主干海域的海温值相对较高,该处闪电活动也明显强于同纬度的东海近海和太平洋海域,表明黑潮海域是强闪电活动区;在季节变化上,我国近海海域闪电活动与同海域海温呈明显正相关,相关系数达0.797,闪电活动与海温变化体现出了一致的变化趋势;而在年际变化上,我国近海海域闪电活动与该海域海温的线性相关不显著,说明我国近海海域海温的年际变化并不是引起该海域闪电活动年际变化的主要原因。  相似文献   

10.
赵生昊  杨磊 《气象科技》2016,44(5):822-827
利用2008—2013年MODIS 3级数据土地覆盖类型产品MCD12Q1及重庆市ADTD闪电定位资料,以重庆市内106°~107°E,29°~30°N范围的矩形区域为研究区域,结合频次、强度、时段、地貌等要素对局地内的地表覆盖种类与地闪分布关系进行了研究,结果表明:研究区内地闪分布在各地表覆盖种类上差异显著,在水域、农田、城镇上的闪电密度都高于平均值;地闪中轻中度闪电、强闪电的分布在同一地表覆盖种类上的差异明显,强闪电更易产生于水域、林地种类上;同一地表覆盖种类上地闪分布与季节的关系不明显;地闪活动在某些地表覆盖种类上的昼夜分布具有明显差异;植被覆盖面上的地闪分布与地貌条件关系密切,同一类覆盖面上的强闪电比例与海拔高度呈正相关关系。  相似文献   

11.
Characteristics of convective initiation (CI) in the Beijing-Tianjin region during the warm season of2008-2013 are examined. A total of 38877 CI cases are identified by a thunderstorm identification, tracking, analysis, and nowcasting algorithm. CI cases are evaluated in the context of associated terrain, weather systems, and land cover properties. The spatial distribution of all CI cases shows that there are dense CI activities around the 200-m elevation, which means that convective storms are more easily triggered over foothills. From 1500-1800 to 0300-0600 BT (Beijing Time), the high-occurrence CI region tends to propagate southeastward (i.e., from mountains to plains, then to ocean). Among the four local weather systems, the Mongolian cold vortex has the highest CI frequency while the after-trough system has the lowest CI frequency. For the land cover relationships with CI, the urban land cover has the highest CI density and the forest-type land cover has the second highest CI density; these two types of land cover are more conducive to CI formation.  相似文献   

12.
中国及周边海域对流云团的水平和垂直尺度   总被引:1,自引:0,他引:1  
利用2007年1月-2010年12月CloudSat-CALIPSO二级云产品2B-CLDCLASS-LIDAR,统计中国及其周边海域对流云的发生频率,根据对流云发生频率的分布特征将中国及周边海域划分为青藏高原(TP)、东部陆地(EC)、南部海域(SO)和西北太平洋(WP)4个子区域,并研究了4个子区域积云团和深对流云团的水平尺度和垂直尺度。统计结果表明,海洋积云团的水平尺度约为2 km,陆地积云团的水平尺度约为1 km,海洋下垫面热力性质均匀,积云团尺度更大;陆地下垫面非均匀性强,积云团分布更为零散。深对流云团的水平尺度为10-50 km,东部陆地最大,约为45 km,西北太平洋最小,约为30 km。陆地深对流云团水平尺度较海洋上大,且多尺度特征显著,应该与深对流云发生的复杂天气背景有关。积云团的垂直尺度范围为0.24-2 km,4个区域无明显差异。垂直尺度海洋深对流云团大于陆地云团,其中在南部海域地区最大,约为15 km,青藏高原最小,约为10 km。与陆地云团相比,海洋深对流云团表现为水平尺度更小、垂直尺度更大的中尺度对流体特征。   相似文献   

13.
This study examined lightning activity and its relationship to precipitation and convective available potential energy(CAPE) in South China during 2001–12, based on data from the Guangdong Lightning Location System, the Tropical Rainfall Measuring Mission satellite, and the ERA-Interim dataset. Two areas of high lightning density are identified: one over the Pearl River Delta, and the other to the north of Leizhou Peninsula. Large peak-current cloud-to-ground(LPCCG) lightning(75 kA) shows weaker land–offshore contrasts than total CG lightning, in which negative cloud-to-ground(NCG) lightning occurs more prominently than positive cloud-to-ground(PCG) lightning on land. While the frequency of total CG lightning shows a main peak in June and a second peak in August, the LPCCG lightning over land shows only a single peak in June.The ratio of positive LPCCG to total lightning is significantly greater during February–April than during other times of the year. Diurnally, CG lightning over land shows only one peak in the afternoon, whereas CG lightning offshore shows morning and afternoon peaks. The rain yield per flash is on the order of 10~7–10~8kg per flash across the analysis region, and its spatial distribution is opposite to that of lightning density. Our data show that lightning activity over land is more sensitive than that over offshore waters to CAPE. The relationships between lightning activity and both precipitation and CAPE are associated with convection activity in the analysis region.  相似文献   

14.
Due to the higher temporal and spatial resolution and the better integrality of long-term satellite infrared(IR) Brightness Temperature(TBB) data,a climatology of deep convection during summer over South China and the adjacent waters is presented in this paper based on the 1-hourly infrared IR TBB data during June-August of 1996-2007(except 2004).The results show that the geographic distribution of deep convection denoted by TBB ≤-52℃ over South China and the adjacent waters are basically consistent with previous statistical results based on surface thunderstorm observations and low-orbit satellite lightning observations.The monthly,ten-day,five-day and diurnal variations of deep convection in this region are focused on in this paper.There are 5 active deep-convection areas in June-August.The monthly variations of the deep convection are closely associated with the large-scale atmospheric circulations.The deep convection over the land areas of South China is more active in June while that over the South China Sea is more active in July and August.The development of deep convection is prominently intermittent and its period is about 3 to 5 five-day periods.However,the deep convection over the coastal areas in South China remains more active during summer and has no apparent intermittence.The ten-day and five-day variations of deep convection show that there are different variations of deep convection over different areas in South China and the adjacent waters.The tendency of deep convection over the land areas of South China is negatively correlated with that over the South China Sea.The diurnal variations of deep convection show that the sea-land breeze,caused by the thermal differences between land and sea,and the mountain-valley breeze,caused by the thermal differences between mountains and plains or basins,cause deep convection to propagate from sea to land in the afternoon and from land to sea after midnight,and the convection over mountains propagates from mountains to plains after midnight.The different diurnal variations of deep convection over different underlying surfaces show that not only there are general mountainous,marine and multi-peak deep convection,but also there is longer-duration deep convection over coastal areas and other deep convection triggered and maintained by larger-scale weather systems in South China during summer.  相似文献   

15.
基于卫星观测资料的全球闪电活动特征研究   总被引:4,自引:0,他引:4  
利用卫星携带的闪电探测系统所获取的11年(1995年5月至2006年4月)闪电资料,对全球闪电活 动特征进行了详细分析。结果表明:全球闪电频数约为46.2 fl s-1(fl为flash简写,表征闪电发生的次数),在30°S~30°N闪电数占全球闪电总数的78.1%,陆地和海洋的闪电密度之比为9.64:1。近海海域面积占海洋面积的近3成,但闪电数占海洋闪电总数的近7成,远海海域闪电的密度很小。陆地和近海海域闪电活动随季节变化呈现出单峰特征,峰值出现在7月。中高纬度大陆东部近海海域闪电频数大于西部,赤道附近区域相反,大陆西部近海海域闪电频数大于东部。闪电活动随海拔高度的变化呈两峰三谷的特征,两峰分别出现在海拔100~2400 m和3300~4600 m,3个低谷分别出现在海拔100 m以下、2400~3300 m和4600 m以上,这是在地理位置和海拔高度的影响下,各种因素综合作用的结果。  相似文献   

16.
The extratropical transitions(ETs)of tropical cyclones(TCs)over China and the ocean east to 150°E are investigated by the use of best-track data and JRA-25 reanalysis spanning 1979-2008.The ET events occurring north of 25°N and in the warm season(from May to October)are extracted from the reanalysis to emphasize the interaction between TC and midlatitude circulation.Statistical analysis shows that 18.5%of the warm-season TCs go through land ETs north of 25°N in the western North Pacific.And 20.5%of the ET events occur over the ocean east of 150°E.Most(62.2%)ET TCs over China gradually die out after ET,but more(70.7%)ocean ET cases have post-ET reintensification.The evolutions in cyclone phase space and the composite fields for land and ocean ETs,as well as the ET cases with and without post-ET reintensification,are further analyzed.It is found that most TCs with ET over China and those without post-ET reintensification evolve along the typical ET phase path as follows:emergence of thermal asymmetry→losing upper-level warm core→losing lower-level cold core→evolving as extratropical cyclone.The TCs undergoing ETs over ocean and those with post-ET reintensification form a high-level cold core before the ET onset.The TCs with land ET have long distance between the landing TC and a high-level trough.That makes the TC maintain more tropical features and isolates the TC flow from the upstream and downstream jets of the midlatitude trough.The structure of circulation leads to weak development of baroclinicity in land ET.On the contrary,shorter distance between ocean TC and high-level trough makes the high-level trough absorb the TC absolutely.Under that baroclinicity-favorable environment,strong cold advection makes the TC lose its high-level warm core before ET onset.The composite fields confirm that the TC with ocean ET has stronger baroclinic features.Generally,the TC at land ET onset is located to the south of the ridge of the subtropical high,which tends to prevent the TCs from interacting with midlatitude circulation.But for the ocean ET,the situation is just the opposite.Similar analyses are also carried out for the TCs with and without post-ET reintensification over both land and ocean east of 150°E.The results further prove that the TC with stronger baroclinic characteristics,especially in the circumstance favorable to its interaction with high-level midlatitude systems,has more opportunity to reintensify as an extratropical cyclone after ET.  相似文献   

17.
冬、夏季热带及副热带穿透性对流气候特征分析   总被引:2,自引:0,他引:2  
刘鹏  王雨  冯沙  李崇银  傅云飞 《大气科学》2012,36(3):579-589
文中利用热带测雨卫星 (TRMM) 搭载的测雨雷达 (PR) 1998~2007年的探测结果, 就热带及副热带地区穿透性对流的频次、条件降水强度及垂直廓线等特征进行了分析。研究结果表明: 深对流和穿透性对流都主要发生在热带辐合带 ( ITCZ)、南太平洋辐合带 (SPCZ)、亚洲季风区、20°N以南的非洲以及美洲等地区, 它们的空间分布具有明显的地域性和季节变化特征, 而且陆地深对流更容易发展成为穿透性对流, 但绝大部分地区的穿透性对流频次不超过0.2%。对穿透性对流条件降水强度的分析表明, 热带及副热带大部分地区的穿透性对流条件降水强度在10 mm/h以上, 且洋面的条件降水强度要比陆地大, 但由于其频次较小导致其对总降水的贡献并不大。尽管深对流和穿透性对流降水廓线的外形比较相似, 但相同的高度, 深对流的降水强度要比穿透性对流偏小, 而且这种差异随海陆和纬度的不同而有所区别。此外, 热带地区 (15°S~15°N) 冬、夏季深对流和穿透性对流降水廓线都只存在较小差异, 并没有显示出明显的季节变化。  相似文献   

18.
王芳  郄秀书  崔雪东 《大气科学》2017,41(6):1167-1176
利用2005~2014年全球闪电定位网(WWLLN)资料和中国气象局提供的热带气旋(Tropical Cyclone,TC)位置和强度资料,分析了近10年西北太平洋地区228个TC中的闪电时空分布特征及其与气旋强度变化的关系。结果表明:TC闪电活动年际变化呈震荡分布,夏半年闪电活动比冬半年强,闪电频数日变化呈单峰分布,峰值出现在12:00(地方时,下同),谷值出现在06:00。闪电密度呈三圈分布结构,内核区和外雨带区闪电密度较高,内雨带区最低;闪电密度空间不对称分布,最高值出现在TC南侧。TC强度改变时,内核区闪电密度随TC不同强度等级的分布与外雨带区不同。TC内核区闪电活动较外雨带区强,内核区和外雨带区的闪电密度最大值分别出现在TC快速增强和强度一般变化时;快速增强过程一般发生在中等强度的TC中,而快速减弱过程一般发生在强度较强的TC中。TC快速增强前后,内核区闪电活动变化比全部TC闪电和外雨带区明显,表明内核闪电活动较全部TC闪电和外雨带区闪电能更好的指示TC的快速增强。  相似文献   

19.
The establishment of the upper-level South Asian high(SAH) over the Indo-China Peninsula(ICP) during late boreal spring and its possible causes are investigated using long-term NCEP–NCAR and ERA-40 reanalysis and satellite-observed OLR data. Results show that, from early March to mid-April, deep convection stays south of ~6?N over the northern Sumatran islands. As the maximum solar radiation moves over the latitudes of the ICP(10?–20?N) in late April, the air over the ICP becomes unstable. It ascends over the ICP and descends over the adjacent waters to the east and west. This triggers deep convection over the ICP that induces large latent heating and strong updrafts and upper-level divergence, leading to the formation of an upper-level anticyclonic circulation and the SAH over the ICP. During early to mid-May, deep convection over the ICP intensifies and extends northwards to the adjacent waters. Strong latent heating from deep convection enhances and maintains the strong updrafts and upper-level divergence, and the SAH is fully established by mid-May. Thus, the seasonal maximum solar heating and the land–sea contrast around the ICP provide the basic conditions for deep convection to occur preferentially over the ICP, which leads to the formation of the SAH over the ICP from late April to mid-May. Simulations using Reg CM4 also indicate that the diabatic heating over the ICP is conducive to the generation and development of upperlevel anticyclonic circulation, which leads to an earlier establishment of the SAH.  相似文献   

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