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首页> 外文期刊>Journal of Geophysical Research, D. Atmospheres: JGR >Lightning electromagnetic environment in the presence of a tall grounded strike object
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Lightning electromagnetic environment in the presence of a tall grounded strike object

机译:存在高接地触击物体的雷电电磁环境

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摘要

We have analyzed and compared distance dependences of electric and magnetic fields due to a lightning strike to a tall object and due to the same lightning strike to flat ground. In both cases, lightning was represented by a transmission line energized by a lumped voltage source connected at the channel attachment point. The resultant total charge transfer to ground was the same regardless of the presence of strike object. The electric field for the strike-object case is reduced relative to the flat-ground case at closer distances from the object. If we assume, in an idealized case, that the return stroke wave front speed is equal to the speed of light, v = c, the current reflection coefficient at the bottom of the strike object ρ_(bot) = 1 (grounding impedance Z_(gr) = 0), and that at the top of the object for upward-propagating waves ρ_(top) = 0 (characteristic impedance of the object is equal to that of the channel Z_(ob) = Z ch ), the ratio of the vertical electric fields on ground for the strike-object and flat-ground cases (electric field attenuation factor) will be d/√(d 2 + h 2), where h is the height of the strike object and d is the horizontal distance from the object. The corresponding ratio for the azimuthal magnetic field is equal to unity. We show that the ratio for either electric or magnetic field increases with decreasing ρ bot (ρ bot < 1), decreasing ρ top (ρ_(top) < 0 except for the case of ρ_(bot) = 0), and decreasing v (v < c), and at larger distances can become greater than unity. We additionally show that the ratio of the far fields for the strike-object and flat-ground cases is given by (1 - ρ_(top)) (c/v + 1)/(1 + ρ gr ), where ρ gr is the current reflection coefficient at the lightning channel base when the channel terminates directly on ground. For realistic values of ρ_(top) = -0.5, ρ_(gr) = 1, and v = 0.5c, this ratio (far field enhancement factor) is equal to 2.3.
机译:我们已经分析并比较了由于雷击高个物体和雷击同一平坦地面而引起的电场和磁场的距离依赖性。在这两种情况下,雷电都由传输线表示,该传输线由连接在通道连接点的集总电压源供电。无论是否存在打击对象,最终转移到地面的总电荷都是相同的。在距物体较近的距离处,相对于平坦的壳体,打击目标壳体的电场减小。如果我们在理想情况下假设回程波的波前速度等于光速v = c,则打击对象底部的电流反射系数ρ_(bot)= 1(接地阻抗Z_( gr)= 0),并且对于向上传播的波ρ_(top)= 0(物体的特性阻抗等于通道Z_(ob)= Z ch的阻抗)在物体顶部的比率为打击对象和平坦地面情况下地面上的垂直电场(电场衰减系数)将为d /√(d 2 + h 2),其中h是打击对象的高度,d是水平距离从对象。方位磁场的相应比率等于1。我们表明,电场或磁场的比率随ρbot(ρbot <1)的减小,ρtop(ρ_(top)<0除外,ρ_(bot)= 0的情况)和v( v

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