脉冲在不规则和/或非均匀地球上的传播,理论与实验的比较

A. Amri, J. Fontaine, J. Chandezon
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摘要

在长度分别为49公里和55-4公里的两条不同传播路径上进行了超视距和直接视距地波传播测量。数据是在1983年法国的St-Privat d ' Allier实验期间收集的。这里给出的结果包括测量脉冲和预测脉冲之间的比较。预测是基于论文AMRI等人(1)。测量的脉冲证明了该方法在提供振幅和波形预测方面的有效性。电磁脉冲通过地波在不规则和/或非均匀地球上的传播具有相当大的意义。在工业工厂中引入敏感的固态器件使这些器件更容易受到电磁脉冲的影响,因此可能需要额外的保护。在这种情况下,显然需要更多关于电磁脉冲传播的知识。这些知识可以通过前面出版物(1)中作者开发的方法从理论上获得。在这里,我们将1983年在法国St-Privat d'Allier闪电触发站获得的一些实验结果与理论得到的结果进行比较。脉冲传播理论根据傅里叶变换积分定理(6)(2j),我们知道在地球表面时刻t和距离r0处的瞬态场E(t,r0)与连续时谐解E(jti), ro)有关,假设传播介质的振幅响应是线性的。E(t,r) = je3mt E(jio, ro) M(ju)do)(1)其中M(jto)是源时刻M(t)的拉普拉斯变换+°°M(J 本文章由计算机程序翻译,如有差异,请以英文原文为准。
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Propagation of Pulses Over an Irregular and/or Inhomogeneous Earth, Comparison of the Theory and the Experiment
Beyond and direct line-of-sight ground wave propagation measurements were made over two different propagation paths 49 km and 55-4 km in length. Data were collected during the St-Privat d ’Allier experimen­ tal compaign in 1983 in France. Results presented here include a comparison between measured and predicted pulses. The predictions are based on the paper AMRI et al (l). Measured pulses demonstrated the usefulness of the method developped in;this late paper in providing amplitude and wave-form predictions. INTRODUCTION The propagation of electromagnetic pulses over an irregular and/or inhomogeneous earth by ground wave is of considerable interest. The introduction of sensitive solid state devices into the industrial plants makes these devices more susceptible to the electroma­ gnetic pulses and, there fore may require additional protection. In this context, it has become evident thg£ more knowledge regarding the propagation of the elec­ tromagnetic pulses is required. Such knowledge can be acquired theoretically by the method developped by the authors in the preceding publication (l). Here, we will compare some of our experimental results obtained in 1983 at the lightning triggering station at St-Privat d'Allier (France) with that obtained theoretically. THEORY OF PULSE PROPAGATION We know that the transient field E(t,r0) at a time t and a distance r0 on the surface of the earth is related to the continuo us time-harmonic solution E(jti), ro), assuming a linear amplitude response of the medium of propagation, by the Fourier transform-integral theorem (6) (2j : E(t,r ) = J e3Mt E(jio, ro) M(ju)do) (1) where M(jto) is the Laplace transform of the moment m(t) of the source +°° M(j
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