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首页> 外文期刊>Journal of Electrostatics >Determination of lightning currents from far electromagnetic fields: Effect of a strike object
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Determination of lightning currents from far electromagnetic fields: Effect of a strike object

机译:确定远电磁场产生的雷电流:撞击物体的影响

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We discuss in this paper the influence of the presence of an elevated strike object on the peak of the lightning return stroke current determined from remote field measurements. We develop analytical expressions relating the lightning return stroke channel-base current and the far electromagnetic field for different specific cases, namely, (1) ground-initiated return strokes (classical transmission line (TL) model), (2) ground-initiated return strokes including possible reflections at ground level, (3) tall strike objects for which the current's zero-to-peak time is smaller than the travel time along the object, and (4) electrically short strike objects. It is shown that for tall structures, the field enhancement relative to a return stroke initiated at ground level is expressed through a factor equal to k(tall) = [1 + c/v(1 - 2 rho(t))]/(1 - rho(t)), where v and c are the return stroke front speed and the speed of light in vacuum, respectively, and rho(t) is the top reflection coefficient. For very short towers and/or very slow return stroke current wavefronts, when the condition t(f) >= h/c applies, expressions relating the far electromagnetic field and the return stroke current were also derived. For case (2), return strokes initiated at ground level, the field enhancement relative to a return stroke initiated at ground level, case (1), is expressed through a factor equal to k(short) = (1 + (c/v)rho(ch-g))/(1 + rho(ch-g)), Where rho(ch-g) represents the reflection coefficient between the lightning channel and the grounding impedance. (c) 2006 Elsevier B.V. All rights reserved.
机译:我们在本文中讨论高架打击物体的存在对根据远程现场测量确定的雷电回程电流峰值的影响。我们针对不同的特定情况,开发了有关雷击回程通道基电流和远电磁场的解析表达式,即(1)地面引发的回程(经典传输线(TL)模型),(2)地面引发的回程笔触,包括在地平面的可能反射;(3)高触击对象,其电流的零峰时间小于沿对象的传播时间;(4)电击触对象。结果表明,对于高层建筑,相对于地面发起的回程的场增强通过等于k(tall)= [1 + c / v(1-2-rho(t))] /( 1-rho(t)),其中v和c分别是返回行程前速度和真空中的光速,rho(t)是顶部反射系数。对于非常短的塔架和/或非常慢的回程电流波前,当条件t(f)> = h / c适用时,还可以得出与远电磁场和回程电流有关的表达式。对于情况(2),在地面启动的回程,相对于在情况(1)在地面启动的回程的场增强通过等于k(short)=(1 +(c / v)的因数表示rho(ch-g))/(1 + rho(ch-g)),其中rho(ch-g)表示雷电通道和接地阻抗之间的反射系数。 (c)2006 Elsevier B.V.保留所有权利。

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