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1.
北京地区闪电活动与气溶胶浓度的关系研究   总被引:1,自引:0,他引:1       下载免费PDF全文
基于2015—2017年北京闪电定位网(BLNET)总闪资料与35个自动空气质量监测站PM2.5数据,分析了北京地区(39.5°N—41.0°N,115.0°E—117.5°E)夏季(6—8月)闪电活动与PM2.5的时空分布特征,同时针对117次雷暴天气,探讨了气溶胶浓度变化对闪电活动的可能影响.结果表明:PM2.5浓度及总闪密度均呈现自西北向东南升高的空间分布特征.闪电峰值在污染背景下出现的时间(19∶00LT)晚于清洁背景下(15∶00LT)约4h,且总闪百分比(~20%)可达清洁背景下(~9%)的两倍.对雷暴前1~4h的PM2.5浓度与时间窗(12∶00—22∶00LT)内总闪数目的中位数进行相关分析,发现PM2.5浓度低于130μg·m-3时,PM2.5与总闪数存在明显正相关,此时气溶胶可能通过影响云微物理过程进而影响雷暴的对流发展,增强闪电活动;PM2.5大于150μg·m-3时,总闪数随PM2.5浓度的增加呈减少趋势,可能的原因是高气溶胶浓度下地面太阳辐射显著下降,对流活动受到抑制,导致闪电活动减少.当PM2.5浓度在130~150μg·m-3时,两者关系不明显.  相似文献   

2.
卫星观测的中国及周边地区闪电密度的气候分布   总被引:22,自引:1,他引:22  
雷暴和闪电活动的气候分布是一个地区气候的基本特征之一, 迄今对中国及周边地区闪电密度分布的实际情况尚缺乏详尽的了解. 基于星载 OTD (1995.4~2000.3)和 LIS (1997.12~2003.3)共8 a观测的闪电资料分析, 给出了这一地区0.5°×0.5°网格点的闪电密度分布, 仔细分析发现: (ⅰ) 喜马拉雅山系南北两侧平均闪电密度的比值达到10倍, 而中国陆地东部和西部平均闪电密度的比值为3.5倍, 闪电密度平均值随海陆距离和纬度呈现规律性的变化, 与年平均降水量的相应变化趋势一致, 说明青藏高原和由西向东的三级阶梯状的大尺度地形以及纬度是形成这个地区雷电活动气候分布总体特征的基本因素. (ⅱ) 中国陆地闪电密度分布的区域性差异是显著的, 在不同的地理环境下闪电密度高值带(中心)与中尺度地形有不同的对应关系: 中国东部湿润地区高闪电密度带经常出现在南北或东北-西南走向、海拔500~1500 m的中尺度山脉和丘陵地区附近, 两者水平尺度和走向大体一致, 而闪电低密度带则经常出现在山间盆(谷)地和平原地区; 中国西部寒旱地区闪电相对密度高值区主要分布在祁连山南麓青海湖地区、天山向西的伊犁河谷以及唐古拉山与念青唐古拉山两山之间的盆地; 滨海100 km以内的海陆过渡带上, 在一系列有山体和丘陵地形隆起及大城市等地区出现闪电密度高值中心. (ⅲ) 中国近海的平均闪电密度是全球海洋相应值的5倍; 而在黑潮主干海域有闪电高密度带, 密度值比邻近海域高2~5倍, 这是黑潮主干海域的高温、高盐特征显著影响该海域强对流发展的一个新的事实. 另外, 还给出了安徽省的云闪/云地闪比Z值约为3.0.  相似文献   

3.
基于近8年卫星观测的全球闪电资料, 对中国东南部和中南半岛各季节闪电密度距平场进行EOF分析发现, 在这一El Ni駉事件期间, 与NINO3区海表温度正距平升高的同时, 1997年春季该地区的闪电活动就出现了显著的正异常, 并一直持续到次年春季结束, 各季度的正异常区闪电密度距平百分率依次是89%, 30%, 45%, 498%和55%, 其中冬季变化幅度最大; 正异常区在冬、春季位于中国南部及其沿海地区, 而在夏、秋季位于中南半岛南部及泰国湾. 与正常年份相比, 各季闪电密度正距平中心位置显著偏西, 特别是冬、春季同时偏北. 另外, 中国南部地区的闪电密度和对流性降水量及高CAPE日数三项距平百分比的年际变化分析表明, 正异常区和黑潮主干区这三项的距平百分比之间两两相关; 在三项中, 闪电密度的相对变化率最大, 闪电活动对El Ni駉事件的响应最灵敏. 但是, 黑潮主干海域、青藏高原和西北、华北-东北等地区的闪电活动对El Ni駉事件的响应情况更为复杂和多样化.  相似文献   

4.
1997/1998 El Niño期间中国南部闪电活动的异常特征   总被引:1,自引:0,他引:1  
基于近8年卫星观测的全球闪电资料, 对中国东南部和中南半岛各季节闪电密度距平场进行EOF分析发现, 在这一El Niño事件期间, 与NINO3区海表温度正距平升高的同时, 1997年春季该地区的闪电活动就出现了显著的正异常, 并一直持续到次年春季结束, 各季度的正异常区闪电密度距平百分率依次是89%, 30%, 45%, 498%和55%, 其中冬季变化幅度最大; 正异常区在冬、春季位于中国南部及其沿海地区, 而在夏、秋季位于中南半岛南部及泰国湾. 与正常年份相比, 各季闪电密度正距平中心位置显著偏西, 特别是冬、春季同时偏北. 另外, 中国南部地区的闪电密度和对流性降水量及高CAPE日数三项距平百分比的年际变化分析表明, 正异常区和黑潮主干区这三项的距平百分比之间两两相关; 在三项中, 闪电密度的相对变化率最大, 闪电活动对El Niño事件的响应最灵敏. 但是, 黑潮主干海域、青藏高原和西北、华北-东北等地区的闪电活动对El Niño事件的响应情况更为复杂和多样化.  相似文献   

5.
基于近8年卫星观测的全球闪电资料,对中国东南部和中南半岛各季节闪电密度距平场进行EOF分析发现,在这一El Nino事件期间,与NINO3区海表温度正距平升高的同时,1997年春季该地区的闪电活动就出现了显著的正异常,并一直持续到次年春季结束,各季度的正异常区闪电密度距平百分率依次是89%,30%,45%,498%和55%,其中冬季变化幅度最大;正异常区在冬、春季位于中国南部及其沿海地区,而在夏、秋季位于中南半岛南部及泰国湾.与正常年份相比,各季闪电密度正距平中心位置显著偏西,特别是冬、春季同时偏北.另外,中国南部地区的闪电密度和对流性降水量及高CAPE日数三项距平百分比的年际变化分析表明,正异常区和黑潮主干区这三项的距平百分比之间两两相关;在三项中,闪电密度的相对变化率最大,闪电活动对ElNino事件的响应最灵敏.但是,黑潮主干海域、青藏高原和西北、华北-东北等地区的闪电活动对El Nino事件的响应情况更为复杂和多样化.  相似文献   

6.
利用16年(1998-2013)的热带降水测量任务卫星(TRMM)降水雷达和闪电成像仪等多传感器观测资料,分析了亚洲季风区内雷暴和强雷暴的空间分布、季节变化及日变化等气候特征.文中取闪电数大于1的雷达降水特征为雷暴,并将闪电频数在前10%的雷暴定义为强雷暴.结果表明:雷暴活动主要集中在陆地及近海区域,陆地与海洋上的雷暴密度之比约为4.4:1,强雷暴密度之比约为7.4:1.0-10°N纬度带内雷暴数占总雷暴的比例最大(占总数的31.7%),而强雷暴则在20°N-30°N区间最为活跃(34.5%).雷暴与闪电密度的空间分布在低纬度区域(0-30°N)较为一致,但在中纬度地区(30°N-36°N)呈现出不同的分布特征,即从西部的青藏高原向东部的江淮流域,雷暴密度逐渐减少但闪电密度逐渐增加;而强雷暴与闪电密度的空间分布基本一致.受亚洲夏季风活动影响,低纬度地区强雷暴更容易发生在春季,强中心位于喜马拉雅山南麓东端,次中心位于中南半岛,而中纬度地区在夏季最为活跃,强中心和次中心则分别位于喜马拉雅山南麓西端和中国江淮流域.陆地上雷暴主要集中在午后至傍晚,少数区域受局地环流和气象条件的影响夜雷暴活动频繁,而海洋上雷暴更易发生在午夜至清晨.  相似文献   

7.
区域闪电活动对地面相对湿度的响应   总被引:17,自引:0,他引:17       下载免费PDF全文
全球闪电活动表现出明显的地域差异,温度和湿度是造成这种差异的基本气象因素.本文利用美国全球水资源和气候中心提供的1995~2002年全球闪电资料和NCEP气象再分析资料,研究了区域闪电密度对地面相对湿度(RH)的响应.发现在平均相对湿度RH<72%的经度带里闪电密度与RH呈正相关.而在RH>73%的经度带里,闪电密度与RH呈负相关;在RH>74%的赤道地区闪电活动与RH呈负相关, 而在RH<72%的中高纬地区闪电密度与RH呈正相关.得到结论:当地面相对湿度过大时,相对湿度的增加不利于闪电活动的发生;而当相对湿度较小时,相对湿度的增加有利于闪电活动的发生.地面相对湿度的临界值域约为72%~74%.此结论在不同经、纬度的几个典型区域均得到了验证,并探讨了过大的相对湿度抑制闪电活动发生的可能原因.  相似文献   

8.
本文利用CHAMP卫星加速度仪测量数据,计算和分析2003年11月20~21日大磁暴期间大气质量密度扰动的全球分布特征;研究暴时变化与极区大尺度对流引起的全球焦耳加热总功率及环电流指数SYM H之间的关系.结果表明,磁暴期间400 km高度上热层大气质量密度大幅度上升, NRLMSISE 00模式预测值与此相比有很大差别;暴时大气密度的增大存在昼/夜半球不对称性:白天强于夜晚,且白天随纬度的分布呈现出比较复杂的图像,在赤道附近和南半球中低纬区(10°N ~50°S)大气密度增大较强,并呈双峰分布,两个峰分别位于0°和45°S,另外在极区也出现大气密度扰动的局部极大,而在夜晚,大气密度变化南北半球比较对称,在赤道低纬区大气密度增大较强;互相关分析表明,中低纬区大气密度变化滞后于全球焦耳加热总功率3~7 h,滞后于环电流指数(SYM H)0~3 h,与二者存在很强的相关,表明极区焦耳加热和赤道环电流过程对暴时热层大气密度扰动有重要影响.  相似文献   

9.
用北半球陆地上48个地面电离层垂测站资料,以及国际参考电离层IRI 90模式,考察1985年1月6~7日F2层电子密度最大值日变化的纬度剖面和经度效应. 结果表明,在亚洲地区的20°N~30°N内,F2层赤道异常“喷泉效应”产生的NmF2“北驼峰”最高,其最大值出现在中午,或稍迟时间. 30°N ~50°N区域内,NmF2的白天峰值幅度逐渐下降,峰值时间移至午前约10:00 LT. 更高纬度(50°N~62°N )台站上,中午前后NmF2出现双峰,傍晚有谷值,夜间又再次抬升. 欧、美地区的低纬台站很少,但借助IRI 90模式分析可发现,在270°E经圈上,“喷泉效应”造成的“北驼峰”幅度最小,而且随纬度增大时,NmF2白天幅度下降也不明显,即纬度剖面的经度效应非常显著. 对中国、日本地区台站资料的小范围经度差异分析表明,在驼峰区的90°E~140°E内,各站NmF2无明显差别;但在中纬地区30°N~50°N内,中国西部上空NmF2白天变化幅度较大,且较为陡直,而中国东部和日本台站上空则相对平缓.  相似文献   

10.
晋东北(北纬38°30′~41°00′,东经113°00′~115°20′)地区包括怀来—西安裂谷系的北端,历史强震和现代地震都较频繁,还有第四纪火山分布.这些地质现象的深部构造背景是什么?浅层构造与深部构造有什么关系?前人论及不多.此次工作研究思路和方法是在详细收集区内地层厚度和密度的基础上,建立地质—密度模型,用重力三维正演方法,逐层消除浅部地质体对布格异常的干扰(“剥皮”),从而获得一套不同深度的剩余重力异常和代表下地壳底部介质密度差异的剩余深部重力异常.然后选取通过本区的D.S.S.剖面上一个莫霍深度值,反演全区地壳厚度.共处理数据37.5万个.  相似文献   

11.
The Tibetan Plateau, the Roof of the World, is the highest plateau with a mean elevation of 4000 m. It is characterized by high levels of solar radiation, low air temperature and low air pressure compared to other regions around the world. The alpine grassland, a typical ecosystem in the Tibetan Plateau, is distributed across regions over the elevation of 4500 m. Few studies for carbon flux in alpine grassland on the Tibetan Plateau were conducted due to rigorous natural conditions. A study of soil respiration under alpine grassland ecosystem on the Tibetan Plateau from October 1999 to October 2001 was conducted at Pangkog County, Tibetan Plateau (31.23°N, 90.01°E, elevation 4800 m). The measurements were taken using a static closed chamber technique, usually every two weeks during the summer and at other times at monthly intervals. The obvious diurnal variation of CO2 emissions from soil with higher emission during daytime and lower emission during nighttime was discovered. Diurnal CO2 flux fluctuated from minimum at 05:00 to maximum at 14:00 in local time. Seasonal CO2 fluxes increased in summer and decreased in winter, representing a great variation of seasonal soil respiration. The mean soil CO2 fluxes in the alpine grassland ecosystem were 21.39 mgCO2 · m-2 · h-1, with an average annual amount of soil respiration of 187.46 gCO2 · m-2 · a-1. Net ecosystem productivity is also estimated, which indicated that the alpine grassland ecosystem is a carbon sink.  相似文献   

12.
We here report our recent research results on the climatic features of Tibetan thermodynamic functions and their impacts on the regional climates of the Northern Hemisphere. The results show that the thermodynamic processes over the Tibetan Plateau not only strongly influence the Asian monsoon and precipitation, but also modulate the atmospheric circulation and climate over North America and Europe through stimulating the large-scale teleconnections such as the Asian-Pacific oscillation and affect the atmospheric circulation over the southern Indian Ocean. The Tibetan climate may be affected by sea surface temperatures over the tropical Pacific. On the other hand, the Tibetan climate also affects the atmosphere-ocean interactions in the tropics and mid-latitudes of the Pacific by the atmospheric circulation over the North Pacific. In spring and summer, the thermodynamic anomalies on the plateau affect the subtropical high pressure, the Hadley circulation, and the intertropical convergence zone over the Pacific, and then modulate the development of the El Niño/Southern Oscillation (ENSO). It is necessary to study the forecasting methods for the development of ENSO from the Tibetan climate anomaly. This result also embodies the essence of interactions among land, atmosphere, and ocean over the Northern Hemisphere. Since the previous studies focused on impacts of the plateau on climates in the Asian monsoon regions, it is essential to pay more attention to studying the roles of the plateau in the Northern Hemispheric and even global climates.  相似文献   

13.
Lightning activity and precipitation structure of hailstorms   总被引:1,自引:0,他引:1  
By using the cloud-to-ground (CG) lightning location data from the lightning detection network of He- nan Province, surface Doppler radar data and standard orbit data of PR, TMI and LIS on TRMM satellite, the spatial and temporal characteristics of CG lightning flashes in 10 severe hailstorms are analyzed. The results show that the percentage of CG lightning in these hailstorms is high with an average value of 45.5%. There is a distinct increase in CG flash rate during the rapid development stage of hailstorms. The hailstone falling corresponds to an active positive flash period, and the increase of CG flash rate is generally accompanied with a decrease of –CG flash rate. The flash rate declines rapidly during the dissipating stage of hailstorms. The precipitation structure and lightning activity in two typical hail- storms are studied in detail. It is found that strong convective cells with reflectivity greater than 30dBZ mainly are situated in the front region of hailstorms, whereas the trailing stratiform region is in the rear part of the hailstorms. The maximum heights of echo top are higher than 14 km. Convective rain con- tributes much more rainfall to the total than stratiform rain, and the convective rain takes about 85% and 97% of the total in the two cases, respectively. Total lightning in the hailstorms is very active with the flash rate up to 183 fl/min and 55 fl/min, respectively. The results also indicate that most lightning flashes occurred in the echo region greater than 30 dBZ and its immediate periphery. The probability of lightning occurrence is 20 times higher in the convective region than in the stratiform region. The result suggests that the lightning information is helpful to the identification of convective rain region. The linear relationship between flash rate and ice water content is disclosed primarily.  相似文献   

14.
According to the boundary layer observations of three stations (Garze, Damxung and Qamdu) and relevant earth satellite, radiosonde and surface observations during the intensive observational period (IOP) of the second Tibetan (Qinghai-Xizang) Plateau Experiment of atmospheric science (TIPEX), the land-air physical process and dynamic model on the Tibetan Plateau were comprehensively analyzed in this study. The dynamic characteristics of boundary layer and the rules of turbulent motion on the plateau were illustrated. The characteristics of distributions of wind speed and direction with mutiple-layer structure and deep convective mixed layer on the plateau, the strong buoyancy effect in turbulent motion on the plateau on which the air density is obviously smaller than on the plain, and the Ekman spiral and its dynamic pump effect of the plateau deep boundary layer have been found. The local static distribution of water vapor and the horizontal advection of water vapor in the plateau boundary layer were studied. The abnomal thermodynamic structure on the plateau surface and boundary layer, including the plateau strong radiation phenomenon and strong heating source characteristics of the middle plateau, was also analyzed. The authors synthesized the above dynamic and thermodynamic structures of both surface and boundary layers on the plateau and posed the comprehensive physical model of the turbulence and convective mixture mechanism on the plateau boundary layer. The characteristics of formation, development and movement for convective cloud cluster over the plateau influencing floods in the Yangtze River area of China were studied. The conceptual model of dynamic and thermodynamic structures of turbulent motion and convective plume related to the frequent occurrence of "pop-corn-like" cloud system is given as well.  相似文献   

15.
Manabu  Abe  Tetsuzo  Yasunari  Akio  Kitoh 《Island Arc》2005,14(4):378-388
Abstract   The relationship between the altitude of the Tibetan Plateau and climate change in central Asia was investigated through a numeric experiment using the Meteorological Research Institute (MRI) coupled atmosphere–ocean general circulation model I (MRI-CGCM1). The results suggest that summer precipitation in central Asia decreased significantly as the Tibetan Plateau rose in height. Spring precipitation, however, increased during initial growth stages when the plateau height was up to 40% of its present-day height, and then decreased with further plateau growth. During the Tibetan Plateau uplift, the difference between precipitation and evaporation was minimal during spring. When the plateau attained a height exceeding 60% of its present height, relatively low precipitation but high evaporation in spring led to a lower amount of ground moisture. In the case of the high plateau, sensible heat flux during summer and fall largely exceeded latent heat flux. Change was particularly significant for cases when the plateau reached 40–60% of its present-day height. The duration of the predominant sensible heat flux became longer with the uplift of the Tibetan Plateau. The period in which latent heat exceeded sensible heat seems to have been restricted to winter and early spring. The numeric experiments suggest that a significant drying of central Asia corresponded to the period in which the Tibetan Plateau exceeded approximately half its present-day height.  相似文献   

16.
青藏高原东南缘构造旋转的古地磁学证据   总被引:6,自引:2,他引:4       下载免费PDF全文
本文在总结青藏高原东南缘近年来地质研究进展的基础上,从古地磁学的角度讨论其新生代以来的构造运动特征.结果表明:相对稳定的欧亚大陆,新生代以来山泰地块发生了约20°~80°顺时针旋转,局部地区旋转量甚至高达135°,且中部地区的旋转量明显高于南北地区;印支地块经历了~30°的顺时针旋转;川滇地块的顺时针旋转量沿102°E...  相似文献   

17.
本文在对比了TRMM多卫星降水分析TMPA(TRMM Multi-satellite Precipitation Analysis)资料和中国643个气象站观测降水量时空分布的基础上,采用2002~2006年夏季TMPA每小时降水量资料,用合成分析和谐波分析的方法研究了青藏高原及其周边地区夏季降水量和降水频率的日变化特征.分析结果表明,平均降水量和降水频率日变化谐波分析的标准振幅显示出青藏高原地区夏季降水具有显著的日变化特征,高原中部地区对流活动日变化最强,其次是高原西南方向的印度半岛地区.谐波分析的位相表明降水量和降水频率最大值出现的时间具有选择性,高原中部降水量最大值多集中在傍晚前后,高原以东的四川盆地通常在夜晚,尤其是在后半夜达到最大值,而长江上游和中下游地区对流活动则分别在上午和下午最为活跃.青藏高原以东地区降水量日变化的位相明显不同于其他陆地地区,也不同于高原中部,具有自西向东传播的信号,四川盆地的夜雨现象可能是高原地区对流活动日变化自西向东传播的结果.  相似文献   

18.
It is difficult to acquire deep seismic reflection profiles on land using the standard oil-industry acquisition parameters. This is especially true over much of Tibetan plateau not only because of severe topography and rapid variation of both velocity and thickness of near-surface layer, but also strong attenuation of seismic wave through the thickest crust of the Earth. Large explosive sources had been successfully detonated in US, but its application in Tibetan plateau rarely has an example of good quality. Presented herein is the data of a 200-kg single shot we recorded in west Qinling, northeastern Tibetan plateau. The shot gather data with phenomenal signal-to-noise ratios illustrate the energy of the PmP phase. Although the observations are only limited to the northeastern Tibetan plateau and thus cannot comprise an exhaustive study, they nevertheless suggest that large explosions may be a useful exploration tool in Tibetan Plateau where standard seismic sources and profiling methods fail to produce adequate data of low crust.  相似文献   

19.
The profile crossing the west Kunlun region cov-ers the area between the Tarim Basin and the Kara-korum Fault, which is the highest (~5000 m a.s.l.) andthe most narrow part (400—500 km from north tosouth) of the Tibetan Plateau, thus attracting great at-tention of the geological community because of itsunique tectonic features. The Geological Bureau of Xinjiang Uygur Auton-omous Region and Chinese Academy of Sciences(CAS) carried out mineral exploration and geologicalmapping in th…  相似文献   

20.
曹建玲  王辉  张晶 《地震》2013,33(4):55-63
青藏高原存在柔性下地壳流动被越来越多的学者接受, 但是关于下地壳流动方式及速度存在争议。 地表运动有GPS等直接测量, 上地幔运动有S波分裂间接反映, 下地壳运动目前没有直接观测手段, 使得开展数值分析非常重要。 本文利用三维球壳黏弹性有限元模型研究了青藏高原下地壳柔性流动方式和流动速度。 本文通过对地表GPS观测资料的拟合与不同数值模型的对比分析, 认为青藏高原柔性下地壳东向流动遇到四川盆地的抵阻, 下地壳物质可能仅在高原东南方向存在物质外溢通道, 而在高原东北方向不存在类似的物质通道; 下地壳的流动速度比地表运动速率每年快几毫米至十几毫米, 对应的黏滞系数为1018~1019 Pa·s。  相似文献   

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