三维磁场解的边界元法

M. Ingber, G. Kiuttu, J. Ingber, B. Smith
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引用次数: 2

摘要

边界元法(BEM)是一种有效的静磁分析方法。磁矢量势的直接边界元公式在过去的20年里得到了发展。磁通密度有一个不太为人所知的直接边界积分方程。初检时,磁通密度的辅助边界积分方程似乎是齐次的,但在适当的边界条件下,可以证明该方程是适定的和非齐次的。本文推导了磁感应强度的BIE,并说明了如何利用安培定律的积分形式给出的辅助约束来确定良导体上的表面场。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Boundary element method for solution of 3-D magnetic fields
The boundary element method (BEM) has been established as an effective means for magnetostatic analysis. Direct BEM formulations for the magnetic vector potential have been developed over the past 20 years. There is a less well known direct boundary integral equation (BIE) for the magnetic flux density. On first inspection, the ancillary boundary integral equation for the magnetic flux density appears to be homogeneous, but it can be shown that the equation is well-posed and non-homogeneous using appropriate boundary conditions. In this paper we derive the BIE for the magnetic induction and show how it can be used to determine the surface fields on good conductors using an auxiliary constraint given by the integral form of Ampere's Law.
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