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Distribution of electrical charge in a system of finite conductors

机译:有限导体系统中电荷的分布

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Numerical approximation of the distribution of electrical charge in systems of mutually electrically isolated conductors carrying different electric potential is in practice extremely difficult by means of standard FE schemes. The main obstacles are represented by lack of the boundary conditions and geometrical incommensurability of various elements present within the investigated domain. The paper reformulates the problem onto a system of the first-kind Fredholm integral equations with a weakly singular kernel that is discretized alternatively to the classical Nystrom method. Solvability and unambiguousness of the continuous mathematical model as well as convergence of the numerical scheme is shown. Quasi equilibrium approach for the simulation of moving conductors is also discussed. The methodology is illustrated on a typical example.
机译:在实践中,借助于标准的FE方案,在相互电绝缘的带有不同电势的导体系统中,电荷分布的数值近似非常困难。主要障碍是由于缺乏边界条件和所研究领域内存在的各种元素的几何不可通约性。本文将问题重新构造为具有弱奇异核的第一类Fredholm积分方程组,该方程组可以替代经典的Nystrom方法离散化。显示了连续数学模型的可解性和明确性,以及数值格式的收敛性。还讨论了用于运动导体仿真的拟均衡方法。在一个典型示例中说明了该方法。

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