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基于闪电先导随机模式对不同连接形态的模拟

廖义慧 吕伟涛 齐奇 张荣 张冬冬 谭涌波 张义军

廖义慧, 吕伟涛, 齐奇, 等. 基于闪电先导随机模式对不同连接形态的模拟. 应用气象学报, 2016, 27(3): 361-369. DOI: 10.11898/1001-7313.20160311..
引用本文: 廖义慧, 吕伟涛, 齐奇, 等. 基于闪电先导随机模式对不同连接形态的模拟. 应用气象学报, 2016, 27(3): 361-369. DOI: 10.11898/1001-7313.20160311.
Liao Yihui, Lü Weitao, Qi Qi, et al. Simulation of various connecting patterns during the lightning connection process based on the stochastic lightning leader model. J Appl Meteor Sci, 2016, 27(3): 361-369. DOI:  10.11898/1001-7313.20160311.
Citation: Liao Yihui, Lü Weitao, Qi Qi, et al. Simulation of various connecting patterns during the lightning connection process based on the stochastic lightning leader model. J Appl Meteor Sci, 2016, 27(3): 361-369. DOI:  10.11898/1001-7313.20160311.

基于闪电先导随机模式对不同连接形态的模拟

DOI: 10.11898/1001-7313.20160311
资助项目: 

中国气象科学研究院基本科研业务费项目 2014R015

国家重点基础研究发展计划 2014CB441405

国家自然科学基金项目 51420105011

国家自然科学基金项目 41475003

详细信息
    通信作者:

    谭涌波, email: ybtan@ustc.edu

Simulation of Various Connecting Patterns During the Lightning Connection Process Based on the Stochastic Lightning Leader Model

  • 摘要: 考虑到下行负极性地闪过程中大多上行正先导发展时不分叉的观测事实,基于已有的闪电先导二维随机模式,改变上行正先导的模拟方案,使其发展时不产生分叉,并对雷击高建筑物过程中下行先导与上行连接先导 (upward connecting leader,UCL) 之间头部-头部连接和头部-侧面连接 (侧击) 的两种形态进行模拟。以高度为440 m的建筑物为例,通过改变下行先导始发点 (高度为1000 m) 与高建筑物的水平距离,模拟高建筑物上雷击过程中先导之间的连接过程,结果表明:当下行先导始发点与高建筑物的水平距离从0增加到700 m时,UCL的长度呈持续增大趋势,UCL受侧击的概率总体上呈先增大后减小的趋势 (在距离为500 m时达到最大值58%),侧击时UCL连接点以上的部分占整个UCL长度的比例总体呈持续增大趋势 (13%~49%)。
  • 图  1  先导发展示意图

    Fig. 1  Schematic diagram for the development of the leader

    图  2  建筑物与下行先导始发点位置的选取

    Fig. 2  The building and the selection of initiation positions for the downward leader

    图  3  不同接地点的不同连接形态

    Fig. 3  Different connection behavior at different grounding points

    图  4  不同位置接地概率随d变化 (a) 与UCL平均长度随d变化 (b)

    Fig. 4  Changes of grounding probability at different locations with d(a) and changes of the average length of UCL with d(b)

    图  5  d不同UCL受侧击的模拟结果

    Fig. 5  Simulation results of the tip-to-lateral connection behavior with different d

    图  6  UCL受侧击概率随d的变化 (a) 及Rd的变化 (b)

    (R为UCL连接点以上的长度与UCL总长度比值的平均值)

    Fig. 6  Changes of probability of tip-to-lateral connection behavior with d(a) and changes of R with d(b)

    (R is the average ratio of the length between connection point to the tip of UCL and the whole length of UCL)

    表  1  不同位置的接地概率

    Table  1  Grounding probability at different locations

    d/m 地面/% 高建筑物侧面/% 高建筑物顶面/%
    0 0 0 100
    100 0 0 100
    200 0 1 99
    300 0 4 96
    400 4 23 74
    500 25 34 41
    600 54 31 15
    700 84 14 2
    下载: 导出CSV

    表  2  各位置起始UCL的长度范围

    Table  2  The length of UCL initiating from different locations

    d/m 地面 建筑物侧面 建筑物顶面
    范围/m 平均值/m 范围/m 平均值/m 范围/m 平均值/m
    0 44~400 189
    100 58~376 187
    200 10~24 16 118~428 198
    300 24~30 16 134~464 211
    400 10~38 18 10~44 18 104~516 245
    500 10~58 19 10~64 21 142~569 276
    600 10~68 18 10~77 20 157~519 296
    700 10~72 18 10~58 16 197~494 317
    下载: 导出CSV

    表  3  高建筑物顶面起始的UCL长度范围

    Table  3  The length of UCL initiating from the top of the tall structure

    d/m 头部连接的UCL 受侧击的UCL
    范围/m 平均值/m 范围/m 平均值/m
    0 44~288 183 74~400 199
    100 58~356 179 118~376 198
    200 128~428 191 118~390 207
    300 134~373 190 134~464 229
    400 104~516 239 132~436 251
    500 148~508 265 142~569 285
    600 157~490 285 187~519 306
    700 197~494 307 188~450 320
    下载: 导出CSV

    表  4  d不同情况下UCL受侧击情况的模拟结果

    Table  4  Simulation results of tip-to-lateral connection as the value of d changes

    d/m Nt Nl P/% R Lu/m Lc/m
    0 400 136 35 0.13 199 27
    100 400 165 41 0.17 198 35
    200 396 175 44 0.18 207 42
    300 384 203 53 0.26 229 66
    400 295 149 51 0.26 251 71
    500 165 95 58 0.34 285 101
    600 59 31 53 0.37 306 110
    700 7 2 29 0.49 320 156
      注:Nt为接地点在建筑物顶面的次数,Nl为UCL受侧击的次数,P为UCL受侧击的概率, R为UCL连接点以上的长度与UCL总长度比值的平均值,Lu为UCL平均长度,Lc为连接点到UCL头部的长度。
    下载: 导出CSV
  • [1] 马明, 吕伟涛, 张义军, 等.1997—2006年我国雷电灾情特征.应用气象学报, 2008, 19(4):393-400. doi:  10.11898/1001-7313.20080402
    [2] 张义军, 周秀骥.雷电研究的回顾和进展.应用气象学报, 2006, 17(6):829-834. doi:  10.11898/1001-7313.20060619
    [3] Dwyer J R, Uman M A.The physics of lightning.Physics Reports, 2014, 534(4):147-241. doi:  10.1016/j.physrep.2013.09.004
    [4] Lu W T, Chen L W, Ma Y, et al.Lightning attachment process involving connecting of the downward negative leader to the lateral surface of the upward connecting leader.Geophys Res Lett, 2013, 40(20):5531-5535. doi:  10.1002/2013GL058060
    [5] Gao Y, Lu W T, Ma Y, et al.Three-dimensional propagation characteristics of the upward connecting leaders in six negative tall-object flashes in Guangzhou.Atmos Res, 2014, 149:193-203. doi:  10.1016/j.atmosres.2014.06.008
    [6] 任晓毓, 张义军, 吕伟涛, 等.雷击建筑物的先导连接过程模拟.应用气象学报, 2010, 21(4):450-457. doi:  10.11898/1001-7313.20100408
    [7] Lu W T, Ma Y, Chen L W, et al.Four Ways of How Downward and Upward Leaders Make Connecting During the Lightning Attachment Process.XV International Conference on Atmospheric Electricity, 2014.
    [8] 谭涌波, 张冬冬, 周博文, 等.地闪近地面形态特征的数值模拟.应用气象学报, 2015, 26(2):211-220. doi:  10.11898/1001-7313.20150209
    [9] 任晓毓, 张义军, 吕伟涛, 等.闪电先导随机模式的建立与应用.应用气象学报, 2011, 22(2):194-202. doi:  10.11898/1001-7313.20110208
    [10] 张义军, 吕伟涛, 郑栋, 等.负地闪先导-回击过程的光学观测和分析.高电压技术, 2008, 34(10):2022-2029. http://www.cnki.com.cn/Article/CJFDTOTAL-GDYJ200810002.htm
    [11] 李丹, 张义军, 吕伟涛.风力发电机叶片姿态与雷击概率关系模拟分析.应用气象学报, 2013, 24(5):585-594. doi:  10.11898/1001-7313.20130508
    [12] Peesapati V, Cotton I.Lightning Protection of Wind Turbines-A Comparison of Real Lightning Strike Data and Finite Element Lightning Attachment Analysis.Sustainable Power Generation and Supply, 2009:1-8. https://www.researchgate.net/publication/224087708_Lightning_protection_of_wind_turbines_-_A_comparison_of_real_lightning_strike_data_and_finite_element_lightning_attachment_analysis
    [13] Riousset J A.Three-dimensional fractal modeling of intracloud lightning discharge in a New Mexico thunderstorm and comparison with lightning mapping observations.J Geophys Res, 2007, 112(15203):1-17. http://www.academia.edu/905177/Three-dimensional_fractal_modeling_of_intracloud_lightning_discharge_in_a_New_Mexico_thunderstorm_and_comparison_with_lightning_mapping_observations
    [14] Wiesmann H J, Zeller H R.A fractal model of dielectric breakdown and prebreakdown in solid dielectrics.Appl Phys, 1986, 60(5):1770-1773. doi:  10.1063/1.337219
    [15] Femia N, Niemeyer L, Tucci V.Fractal characteristics of electrical discharges:Experiments and simulation.Phys D Appl Phys, 1993, 24(6):615-622. https://www.researchgate.net/publication/221963723_Fractal_characteristics_of_electrical_discharges_Experiments_and_simulation
    [16] Popov N A.Spatial structure of the braching streamer channel in a corona discharge.Plasma Physics Reports, 2002, 28(7):615-622. doi:  10.1134/1.1494061
    [17] Perera M D N, Sonnadara D U J.Research Article Fractal nature of simulated lightning channels.Sri Lankan Journal of Physics, 2012, 13(2):9-25.
    [18] 王道洪, 郄秀书, 郭昌明.雷电与人工引雷.上海:上海交通大学出版社, 2000:58-66.
    [19] Vladislav M, Lothar H R.Evaluation of the Lightning Protection System at the WSR-88D Radar Sites.National Oceanic and Atmospheric Administration Final Report, 2001:1-53.
    [20] Wang D, Takagi N, Watanabe T, et al.Observed characteristics of upward leaders that are initiated from a windmill and its lightning protection tower.Geophys Res Lett, 2008, 35, L02803, doi: 10.029/2007GL032136.22.
    [21] Becerra M, Cooray V.On the velocity of positive connecting leaders associated with negative downward lightning leaders.Geophys Res Lett, 2008, 3(5):1-5. http://adsabs.harvard.edu/abs/2008GeoRL..35.2801B
    [22] Mousa A M.Validity of the Collection Volume Method/Field Intensification Method for the Placement of Lightning rods on Buildings.Proc of the 26th International Conference on Lightning Protection, 2002:1-6.
    [23] Lu W T, Chen L W, Zhang Y, et al.Characteristics of unconnected upward leaders initiated from tall structures observed in Guangzhou.J Geophys Res:Atmosphere, 2012, 117(19):1984-2012. https://www.researchgate.net/publication/258662982_Characteristics_of_unconnected_upward_leaders_initiated_from_tall_structures_observed_in_Guangzhou
    [24] 张义军, 吕伟涛, 张阳, 等.广州地区地闪放电过程的观测及其特征分析.高电压技术, 2013, 39(2):383-392. http://www.cnki.com.cn/Article/CJFDTOTAL-GDYJ201302020.htm
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出版历程
  • 收稿日期:  2015-11-02
  • 修回日期:  2016-02-22
  • 刊出日期:  2016-05-31

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