On the Divergenceless Property of the Magnetic Induction Field

S. Severini, A. Settimi
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引用次数: 1

Abstract

Maxwell's equations beautifully describe the electromagnetic fields properties. In what follows we will be interested in giving a new perspective to divergence-free Maxwell’s equations regarding the magnetic induction field: . To this end we will consider some physical aspects of a system consisting of massive nonrelativistic charged particles, as sources of an electromagnetic field (e.m.) propagating in free space. In particular the link between conservation of total momentum and divergence-free condition for the magnetic induction field will be deeply investigated. This study presents a new context in which the necessary condition for the divergence-free property of the magnetic induction field in the whole space, known as solenoidality condition, directly comes from the conservation of total momentum for the system, that is, sources and field. This work, in general, leads to results that leave some open questions on the existence, or at least the observability, of magnetic monopoles, theoretically plausible only under suitable symmetry assumptions as we will show.
论磁感应场的无发散性
麦克斯韦方程组很好地描述了电磁场的性质。在接下来的内容中,我们将有兴趣给出关于磁感应场的无散度麦克斯韦方程组的新视角:为此,我们将考虑一个由大量非相对论性带电粒子组成的系统的一些物理方面,作为在自由空间中传播的电磁场(e.m.)的来源。特别是总动量守恒和磁感应场无散度条件之间的联系将被深入研究。本研究提出了一种新的背景,即磁感应场在整个空间内无发散性的必要条件,即螺线性条件,直接来自于系统的总动量守恒,即源和场。总的来说,这项工作的结果留下了一些关于磁单极子的存在性或至少可观测性的开放性问题,理论上只有在合适的对称性假设下才有可能,正如我们将展示的那样。
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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