计算机机房雷电感应防护工程方案   总被引：1，自引：1，他引：0  

林伟华  梁美婵  张强 《气象研究与应用》2012,33(1):93-95

阐述了计算机机房综合防雷工程设计与实施的防护措施,为一般企业的计算机机房提供了雷电防护解决方案。  相似文献   

地震台站雷电防护技术探讨     

李庆武  李明威  张娜  孙澎涛  任峻峰  关华  孙贵成  于艳红 《地震地磁观测与研究》2012,33(3):285-290

地震台站的仪器多采用集成电路、集成块等高精密电子元件,承受外部环境能力相对较弱,容易遭受雷电的侵害。在分析雷电如何危害地震台站仪器设备基础上,针对地震台站工作实际,探讨应用雷电防护技术,减轻雷电对地震观测技术系统仪器设备的损害,及对地震台站雷电防护的参考意义。  相似文献   

山西数字测震台站雷击原因分析及防护措施研究     

高伟亮  高跃雄  吕睿  郑树平  李云 《山西地震》2014,(1):36-41

在详细分析雷电灾害特征的基础上,阐述了防雷工作的主要技术手段。分析山西数字测震台站2012年-2013年雷击灾害的成因,针对测震台站的构成特点,研究了台站综合防雷系统的设计方法,提出相应的防护技术措施。  相似文献   

Observation and study on the whole process of cloud-to-ground lightning using narrowband radio interferometer     

GuangShu Zhang  YuXiang Zhao  XiuShu Qie  Tong Zhang  YanHui Wang  ChengPin Chen 《中国科学D辑(英文版)》2008,51(5):694-708

A narrowband radio interferometer has been developed and used to locate the entire sources of VHF radiations from a negative cloud-to-ground (CG) lightning discharge which contains 19 strokes. This system uses five antennas to form an array consisting of short- and long-baselines along two or- thogonal directions. The system error which comes from frequency conversion is reduced by phase detection through direct high frequency amplifying. An interactive graphic analysis procedure is used to remove the fringe ambiguities which exist inherently in interferometry and to determine the direction of lightning radiation sources in two dimensions (azimuth and elevation) as a function of time at a time resolution of microsecond orders. With the developed system, the whole progression process in time and space of a lightning flash can be reconstructed. In this paper, combining the synchronous data of electric filed change and VHF radiation, the whole processes of an example negative CG flash have been studied in detail. It is found that the preliminary breakdown event of the CG flash started from negative charge region and exhibited firstly a downward pregression and then an upward propagation. There were very intense and continuous radiations during stepped leaders which became much stronger when the first return stroke began. In contrast, there were less and only discrete radiations during dart leaders. Stepped leader and dart leader may transform to each other depending on the state of the ionization of the path. The progression speed of initial stepped leaders was about 105 ms?1, while that was about 4.1×106 and 6.0×106 ms?1 for dart leaders and dart-stepped leaders, respectively. M events produced hook-shaped field changes accompanied by active burst of radiations at their begin- nings. Followed these active radiation processes, M events appeared to contact finally into conducting main discharge channels. The mean progression speed of M events was about 7×107 ms?1, greater than that of the dart leaders and dart-step leaders. K events and attempted leaders were essentially the same as dart leaders except that they could not reach the ground and initiate return strokes.  相似文献   

Wavelet analysis of lightning return stroke     

F.J. Miranda   《Journal of Atmospheric and Solar》2008,70(11-12):1401-1407

In this investigation, time series consisting of electric field waveforms of 15 positive return strokes and 10 negative return strokes were analyzed. The data came from a summer thunderstorm in March in a range of about 200 km around São José dos Campos, São Paulo. The electric field recording system consisted of a flat plate antenna with a decay time constant of 260 μs and a sample rate of 800,000 samples per second. The bandwidth observed was up to 100 kHz and the recording system was synchronized with GPS time and located at São José dos Campos. Wavelet analysis of the electric field waveforms was done in order to investigate the behavior of the return stroke spectrum in time. The return stroke was suggested to be divided into two portions: initial stage and overshoot (for far return stroke) and initial stage and ramp (for close return stroke). The return stroke power spectrum was observed to be distributed in a frequency range with the peak value also distributed in a fraction of this range. Power peaks for ramps are stronger than power peaks for initial stage and overshoot. Finally, it was observed how powerful the wavelet is in the analysis of lightning.  相似文献   

沈阳雷电监测定位系统建设研究   总被引：9，自引：3，他引：6       下载免费PDF全文

王建华  张涛  杨雨春  张菁  崔劲松 《气象与环境学报》2006,22(6):65-68

介绍了沈阳雷电监测定位系统由4个雷电探测站、1个数据处理中心站、若干显示终端和通信网络组成。通过系统可实时获得雷击的时间、位置、强度、极性、雷电流等雷电参数。针对系统建设实践中遇到的有关技术问题,给出了解决方案;指出了系统安装过程中需要注意的问题,如网络布局、监测网络信息传输与各种终端接入方式等,并就雷电监测定位系统的工作原理、系统功能及应用情况进行了阐述。  相似文献   

太阳能热水器雷电防护技术分析     

李虹 《气象与环境科学》2013,36(4):88-92

太阳能热水器的雷电防护隐患很大,每年都有不少雷击案例发生。通过调查发现,大多数热水器无雷电防护装置;多安装在屋顶,易招致雷击;安装人员多为非专业人员,缺乏必备的雷电防护知识。对太阳能热水器造成危害的不仅有直击雷,还有感应雷。因此,太阳能热水器的雷电防护,既要采取防直击雷防护措施,也要采取防雷电感应措施。  相似文献   

基于干涉仪原理的甚高频雷电单站预警   总被引：1，自引：0，他引：1  

周康辉  董万胜  刘恒毅  蔡力  杨磊  马祥 《气象科技》2013,41(3):563-568

针对目前闪电单站探测与预警装置的局限性,设计了一套基于闪电宽带干涉仪原理的甚高频单站雷电预警装置.该装置通过测量雷电(包括云闪与地闪)起始时刻的辐射信号到达竖直天线阵列的相位差,计算得到该信号的仰角,根据仰角估算雷电的距离,进而根据雷电的距离和活动特征进行雷电报警.单站测距误差分析结果表明,单站系统对半径50 km范围内闪电测距误差在25％以内,半径100 km范围内的闪电测距误差在30％以内.雷电单站预警装置对一次雷暴过程进行了观测,观测结果表明,该装置能有效探测半径100 km范围内的闪电活动状况,探测到的闪电频次分布、闪电距离与多站闪电定位结果保持较好一致性,证明其能有效探测周围闪电活动状况,起到提前预警雷暴的作用.  相似文献   

云南省雷灾特征分析及灾情评估     

殷娴  尹丽云  许迎杰  刘平英 《气象科技》2013,41(1):184-190

根据云南省2007 2008年的雷电灾害资料以及地闪资料,分析了云南省16个地级市的雷电灾害分布特征,讨论了雷灾分布与地闪分布的关系,并从雷灾记录中提取了6个灾度指标,通过AHP法(层次分析法)建立灾情评估层次模型和灾度评估方程,计算了云南省522次雷灾的灾度值,用SAS中聚类分析过程将灾度值分为4级,并统计分析了各级雷灾在各地区的分布情况,得出云南雷电灾害中小型雷灾分布较广、出现几率较大,而大型和特大型雷灾发生几率较低、主要集中在昆明和德宏地区.该文结论为区域防雷减灾规划提供了科学依据.  相似文献   

北美地区一次冬季中尺度对流系统上空红色精灵现象的空间观测及其母体雷暴分析     

钟丽华  杨静  陆高鹏  王庸平  何其佳  郄秀书 《大气科学》2020,44(5):997-1012

红色精灵是发生在雷暴云上空的一种大尺度瞬态放电发光现象,它们通常出现在地面上空40～90 km之间,是由地闪回击和随后可能存在的连续电流产生的。目前,由于综合同步观测资料较少,与夏季红色精灵相比,全世界对冬季红色精灵的研究屈指可数。2008年12月27～28日,受高空槽及低层暖湿气流的影响,北美阿肯色州地区爆发了一次冬季雷暴天气过程,搭载于FORMOSAT-2卫星上的ISUAL（Imager of Sprites and Upper Atmospheric Lightning）探测器有幸在这次雷暴上空记录到了两例红色精灵事件。本文利用ISUAL获取的红色精灵观测资料、多普勒天气雷达资料、美国国家闪电定位资料、超低频磁场数据、美国国家环境中心/气候预测中心提供的云顶亮温和探空数据等综合观测数据,对产生红色精灵的这次冬季雷暴特征和相关闪电活动规律进行了详细研究。结果表明,在两例红色精灵中,ISUAL均未观测到伴随的“光晕（halo）”现象,第一例为“圆柱状”红色精灵,第二例红色精灵由于发光较暗,无法判断其具体形态。产生红色精灵的母体雷暴是一次中尺度对流系统,该系统于27日15:00（协调世界时,下同）左右出现在阿肯色州北部附近,并自西向东移动。23:59系统发展到最强,最大雷达反射率因子（55～60 dBZ）的面积达到339 km2,之后开始减弱。03:03雷暴强度有所增加,随后云体便逐渐扩散,雷暴开始减弱,并在11:00完全消散。两例红色精灵发生分别在04:46:05和04:47:14,此时雷暴处于消散阶段,正负地闪频数均处于一个较低水平且正地闪比例显著增加,并且多位于云顶亮温?40°C～?50°C的层状云区上空。红色精灵的出现伴随着30～35 dBZ回波面积的增加。在红色精灵发生期间,雷达反射率大于40 dBZ的面积减少,10～40 dBZ的面积增加,表明红色精灵的产生与雷暴对流的减弱和层状云区的发展有关,这与已有的夏季红色精灵的研究结果类似。红色精灵的母体闪电为正地闪单回击,位于中尺度对流系统雷达反射率为25～35 dBZ的层状云降水区,对应的雷达回波顶高分别为2.5 km和5 km,峰值电流分别为+183 kA和+45 kA。根据超低频磁场数据估算两个母体闪电的脉冲电荷矩变化（iCMC）分别为+394 C km和+117 C km。超低频磁天线记录到了第一例红色精灵内部的电流信号,表明这例红色精灵放电很强。  相似文献