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Generalized Magnetostatic Analysis by Boundary Integral Equation Derived From Scalar Potential

机译:从标量势导出边界积分方程进行广义静磁分析

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The volume integral equation approach replaces the loop currents over the volume elements in magnetic material with the loop currents on the material surface to derive a boundary integral equation (BIE). The surface loop current is equivalent to the double layer charge, which offers an integral form of scalar potential to give the BIE. Once BIE has been solved, the loop current gives the magnetic flux density $B$ by Biot-Savart law. The BIE has many advantages such as giving accurate solutions and evaluating $B$ at edges and corners. But it has some severe drawbacks due to a multi-valued function of the excitation potential caused by the source currents and that is why its application has been restricted mostly to simply connected problem. This paper presents a novel generalized approach, which is applicable for solving generic problems such as multi-material, multiply connected and thin shielding problems.
机译:体积积分方程法将磁性材料中体积元素上的环路电流替换为材料表面上的环路电流,以得出边界积分方程(BIE)。表面环路电流等效于双层电荷,它提供标量电势的积分形式以提供BIE。解决了BIE后,回路电流将根据Biot-Savart法则给出磁通量密度 $ B $ 。 BIE具有许多优势,例如提供准确的解决方案以及在边缘和拐角处评估 $ B $ 。但是由于源电流引起的激发电势的多值函数,它具有一些严重的缺点,这就是为什么它的应用主要局限于简单连接的问题。本文提出了一种新颖的广义方法,适用于解决通用问题,例如多材料,多重连接和薄屏蔽问题。

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