Electromagnetic fields and waves in vacuum

J. Pierrus
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引用次数: 14

Abstract

In previous chapters four experimental laws of electromagnetism were encountered: Gauss’s law in electrostatics, Gauss’s law in magnetism, Faraday’s law and Ampere’s law. Now, in this chapter, these laws are generalized where appropriate to include the time-dependent charge and current densities ρ‎( r, t) and J ( r, t) respectively. The result is a set of four coupled differential equations—known as Maxwell’s equations— which provide the foundation upon which the theory of classical electrodynamics is based. One of the most important aspects which emerges from Maxwell’s theory is the prediction of electromagnetic waves, and an entire spectrum of electromagnetic radiation. Some of the properties of these waves travelling in unbounded vacuum are considered, as well as their polarization states, energy and momentum conservation in the electromagnetic field and also applications to wave guides and transmission lines.
真空中的电磁场和波
在前面的章节中,我们遇到了电磁学的四个实验定律:静电学中的高斯定律、磁学中的高斯定律、法拉第定律和安培定律。现在,在本章中,这些定律在适当的地方进行了推广,分别包括随时间变化的电荷和电流密度ρ′(r, t)和J (r, t)。结果是一组四个耦合的微分方程——被称为麦克斯韦方程——它为经典电动力学理论提供了基础。麦克斯韦理论中最重要的方面之一是对电磁波和整个电磁辐射谱的预测。考虑了这些波在无界真空中传播的一些性质,以及它们在电磁场中的极化态、能量和动量守恒以及在波导和传输线中的应用。
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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