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An Interpretation of Maxwell Equation by Using the Formalism of Gravitational Waves

机译:用引力波的形式主义解释麦克斯韦方程

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Maxwell equations are known to be fully compatible with the special theory of relativity, but have no representation in terms of space-time perturbations, in opposition with gravitationnal waves which are described as the propagation of small perturbations in the metric of space-time. We propose in this paper to interprete Maxwell equations and electromagnetic waves by using the formalism now well established to describe gravitationnal waves. After deriving a momentum-energy tensor T~(ij) for electromagnetic source, we can apply Einstein's equations in their linearised form. We obtain a wave propagation equation on the metric coefficients which is usually used to explain the propagation of gravitationnal waves. Since this propagation equation is identical as the electromagnetic one, we examine how electromagnetic waves can be interpreted as the propagation of small petrurbations in the space-time metric. We show that in such an interpretation, the electromagnetic potential plays an equivalent role as the gravitationnal potential, and then, can be represented by the metric coefficients. We give the explicite relation between electomagnetic potentials and the metric coefficients which are obtained in this approach and the whole electromagnetic energy associated to a point charge.
机译:众所周知,麦克斯韦方程与狭义相对论完全兼容,但与时空摄动无关,与重力波相反,引力波被描述为时空度量中的小摄动的传播。我们建议在本文中使用已经建立的描述引力波的形式主义来解释麦克斯韦方程和电磁波。在推导电磁源的动量-能量张量T〜(ij)之后,我们可以将爱因斯坦方程以其线性化形式应用。我们获得了基于度量系数的波传播方程,该方程通常用于解释重力波的传播。由于此传播方程与电磁方程相同,因此我们研究如何将电磁波解释为时空度量中小石化的传播。我们证明,在这种解释中,电磁势起着引力势的作用,然后可以用度量系数来表示。我们给出了在这种方法中获得的电磁势与度量系数以及与点电荷相关的整个电磁能之间的明确关系。

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