Energy radiated by the switching of currents in a system of conductors

G. Mrozynski
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Abstract

The calculation of transient electromagnetic fields is becoming more important future because of the increasing demands on system design under EMC-constraints. The switching of currents in a system of conductors is especially crucial because a transient wave is stimulated in the nonconducting environment which can be responsible for the default of electronic systems. The total energy which is radiated by the transient wave can be calculated by integrating the Poynting vector over an appropriate closed surface and over the time interval between the switching moment and infinity. The calculation of the total energy radiated by a switching process can be simplified by applying the principle of conservation of energy. As a consequence only the energy which is dissipated in the conducting space during the transient current distribution after the moment of switching has to be calculated. The applicability is shown for two examples. In the first one a permeable and conducting hollow sphere is exposed to the transient field of a current of arbitrary time dependence flowing in a loop of arbitrary shape. In the second, a continuous current flowing in a homogeneous two wire loop in parallel with a solid conductor of rectangular cross section is switched off. At the moment of switching a part of the energy of the nonconducting space is transferred by a guided wave. The remaining energy can be calculated from the current sheet which is excited on the conductor's surface at the moment of switching. This part of the energy is dissipated in the material during the following transient current distribution.
由导体系统中电流的转换所辐射的能量
随着对电磁约束下系统设计的要求越来越高,瞬变电磁场的计算变得越来越重要。导体系统中电流的切换尤其重要,因为在不导电的环境中会产生瞬态波,这可能是导致电子系统失效的原因。瞬态波辐射的总能量可以通过对波印亭矢量在一个适当的封闭表面上和在开关时刻和无穷远之间的时间间隔上积分来计算。应用能量守恒原理,可以简化开关过程辐射总能量的计算。因此,只需计算开关瞬间后瞬态电流分布过程中在导通空间中耗散的能量。通过两个示例说明了该方法的适用性。在第一种方法中,将一个具有渗透性和导电性的空心球体暴露在任意时间相关电流的瞬态场中,该电流在任意形状的环路中流动。在第二种方法中,切断与矩形截面固体导体平行的均匀两线环中的连续电流。在开关时刻,非导电空间的一部分能量通过导波传递。剩余能量可以从开关时刻导体表面的激发态电流片计算出来。在以下瞬态电流分布过程中,这部分能量在材料中耗散。
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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