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An axiomatic approach to Maxwell's equations

机译:麦克斯韦方程的公理化方法

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This paper suggests an axiomatic approach to Maxwell's equations. The basis of this approach is a theorem formulated for two sets of functions localized in space and time. If each set satisfies a continuity equation then the theorem provides an integral representation for each function. A corollary of this theorem yields Maxwell's equations with magnetic monopoles. It is pointed out that the causality principle and the conservation of electric and magnetic charges are the most fundamental physical axioms underlying these equations. Another application of the corollary yields Maxwell's equations in material media. The theorem is also formulated in the Minkowski space-time and applied to obtain the covariant form of Maxwell's equations with magnetic monopoles and the covariant form of Maxwell's equations in material media. The approach makes use of the infinite-space Green function of the wave equation and is therefore suitable for an advanced course in electrodynamics.
机译:本文提出了麦克斯韦方程的公理化方法。这种方法的基础是为两个空间和时间局部函数集制定的一个定理。如果每个集合都满足一个连续性方程,则该定理将为每个函数提供一个积分表示。该定理的推论得出了带有磁单极子的麦克斯韦方程。指出因果关系原理和电荷和磁电荷守恒是这些方程式最基本的物理公理。推论的另一个应用是在物质介质中产生麦克斯韦方程。该定理还用Minkowski时空公式表示,并用于获得具有磁性单极子的Maxwell方程的协变形式和材料介质中Maxwell方程的协变形式。该方法利用了波动方程的无限空间格林函数,因此适用于电动力学的高级课程。

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