Optimized Charge Simulation Models of Horizontal Sphere Gaps

Navneet Kishore, G. S. Punekar, H. Shastry
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引用次数: 1

Abstract

The horizontal sphere gap is modeled using six point charges per electrode as a test case. Two intuitively felt optimized charge simulation method (OCSM) models of horizontal sphere gap arrangement are set up by selectively changing degree of freedom to understand its effect on the simulation errors. The optimal location of charges is obtained using genetic algorithm (GA). A large number of numerical experiments are conducted by varying potential assigned to the low potential sphere, height of the spheres above the ground plane and gap separation. Lower potential sphere always shows higher error. For a typical case, the maximum surface potential error with increased freedom in locating charges reduced to 4% from its earlier value of 9.5%. The simulations with symmetrical supply show maximum surface potential error of 1.0% on both the spheres. On the other hand simulating a ground potential electrode near a high voltage electrode involves more errors and hence more effort. The charge simulation method being semi analytical technique, the shape of the geometry and symmetry (if any) plays a major role and setting up accurate OCSM model still requires user experience.
优化的水平球隙电荷模拟模型
水平球面间隙采用每电极六个点电荷作为测试用例进行建模。通过选择性地改变自由度,建立了水平球面间隙排列的两种直观感知优化电荷模拟方法(OCSM)模型,了解其对模拟误差的影响。利用遗传算法得到电荷的最优位置。通过改变低电位球的电势、球距地平面的高度和间隙间距进行了大量的数值实验。电位越低,误差越大。在典型情况下,随着定位电荷自由度的增加,最大表面电位误差从之前的9.5%降低到4%。在对称供电的情况下,两种球的最大表面电位误差均为1.0%。另一方面,模拟靠近高压电极的地电位电极涉及更多的误差,因此需要更多的努力。电荷模拟方法是半解析技术,几何形状和对称(如果有的话)起着主要作用,建立准确的OCSM模型仍然需要用户体验。
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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