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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >High accuracy calculation of electric field in composite dielectric system by improved 3-D boundary charge method
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High accuracy calculation of electric field in composite dielectric system by improved 3-D boundary charge method

机译:改进的3D边界电荷法高精度计算复合介质中的电场

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摘要

In this paper, we propose an improved three-dimensional (3-D) boundary charge method for a composite dielectric system where there is a great difference in magnitude of the permittivity between neighboring dielectric materials. The method is based on the idea that the whole region of the composite dielectric system is divided into two regions; one being the region H containing the dielectric material of high permittivity ε_H and the other being the region L containing the dielectric material of low permittivity ε_L. The boundary of division is selected so as to coincide with the interface between ε_H and ε_L. We then arrange surface charge densities on both sides of the interface between ε_H and ε_L as well as on every conductor-to-dielectric interface in respective regions of H and L. The key point of our improved method is that when we calculate the electric field in the region H, for example, we use only the surface charge densities in the same region and do not use those in the region L. When we calculate the electric field in the region L, a similar rule is applied. In order to determine the surface charge density on every interface we utilize boundary conditions for potential and electric field at every interface. This procedure eliminates the loss of numerical accuracy arising from cancellation in addition, and we have succeeded in improving numerical accuracy even when there is a great difference in magnitude of the permittivity between neighboring dielectric materials.
机译:在本文中,我们为复合介电系统提出了一种改进的三维(3-D)边界电荷方法,该方法在相邻介电材料之间的介电常数幅度上存在很大差异。该方法基于将复合电介质系统的整个区域划分为两个区域的想法。一个是包含高介电常数ε_H的介电材料的区域H,另一个是包含低介电常数ε_L的介电材料的区域L。选择划分的边界,使其与ε_H和ε_L之间的界面一致。然后,我们在ε_H和ε_L之间的界面两侧以及H和L的各个区域中的每个导体-电介质界面上排列表面电荷密度。改进方法的关键在于,当我们计算电场时例如,在区域H中,我们仅使用相同区域中的表面电荷密度,而不使用区域L中的表面电荷密度。当我们计算区域L中的电场时,将应用类似的规则。为了确定每个界面上的表面电荷密度,我们利用边界条件来确定每个界面上的电势和电场。该程序消除了由于消除引起的数值精度的损失,并且即使相邻介电材料之间的介电常数的大小差异很大,我们也已经成功地提高了数值精度。

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