On the scheme for seeking the solution to a system of Maxwell's equations in a spherically symmetric model of the Earth-ionosphere waveguide

V. Popov
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Abstract

A classical scheme for solving the boundary-value problem for a system of Maxwell's equations in a spherically stratified model of the Earth-ionosphere waveguide has been known since the beginning of the 20th century, and implies the following. The elementary electric or magnetic dipoles are usually assumed as emitters. In each of these cases the Hertz potentials are introduced, which satisfy partial differential equations with separable variables. Solutions to this equations are sought either in the form of a series in terms of eigenfunctions of the angular operator or in the form of a series in terms of eigenfunctions of the radial operator. The transition from one series to the other is accomplished through the Watson transformation. Attempts to generalize this scheme to the case of more sophisticated waveguide and emitter models led the author to the conclusion that the scheme should be modified. To elucidate the essence of the problem, a very simple model is considered. Unlike the classical scheme, we abandoned the idea of introducing any potentials, and formulated boundary-value problems for the components of fields. The objective of this paper is to devise a reasonably rigorous mathematical scheme for seeking the formal expressions for solving a system of Maxwell's equations.
在地球-电离层波导球对称模型中求解麦克斯韦方程组的方案
在地球-电离层波导的球形分层模型中,求解麦克斯韦方程组边值问题的经典方案自20世纪初就已为人所知,它包含以下内容。基本电偶极子或磁偶极子通常被假定为发射体。在每一种情况下引入赫兹势,它满足可分离变量的偏微分方程。该方程的解要么以角算子的本征函数的级数形式求,要么以径向算子的本征函数的级数形式求。从一个系列到另一个系列的转换是通过沃森转换完成的。作者试图将该方案推广到更复杂的波导和发射极模型的情况下,得出结论认为该方案应进行修改。为了阐明问题的实质,我们考虑一个非常简单的模型。与经典方案不同,我们放弃了引入任何势的想法,并为场的分量制定了边值问题。本文的目的是设计一个合理严格的数学方案来寻求求解麦克斯韦方程组的形式表达式。
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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