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用于三维全电磁粒子模拟的电荷守恒共形发射技术北大核心CSCD
引用本文:王玥,陈再高,王建国. 用于三维全电磁粒子模拟的电荷守恒共形发射技术北大核心CSCD[J]. 强激光与粒子束, 2016, 28(3): 033020-102. DOI: 10.11884/HPLPB201628.033020
作者姓名:王玥  陈再高  王建国
作者单位:1.西北核技术研究所, 西安 71 0024;
基金项目:国家高技术发展计划项目
摘    要:给出了满足电荷守恒的共形发射技术。首先阴极表面由三角网格共形描述,发射带电粒子时,根据电荷和电流线性分配方式和离散高斯定律,带电粒子的初始位置设置在与三角面元处于同一个网格元胞内,离三角面元最近且处于金属内部的网格点上。带电粒子的初始运动由两部分组成:一是由三角面上的法向场推进所产生的运动;二是使发射粒子在阴极面上分布呈随机性而设定的随机运动。运动产生的电流按照电荷守恒定律分配到离散网格中,并且由于粒子的初始位置设置在整网格点上,带电粒子的共形发射不会产生非物理的静电累加。最后通过同轴二极管模型来验证共形发射模型的正确性。

关 键 词:电荷守恒  共形发射  全电磁粒子模拟  时域有限差分  Delaunay三角网格剖分
收稿时间:2015-09-14

Charge conserving emission technique for three-dimensional conformal particle-in-cell simulations
Affiliation:1.Northwest Institute of Nuclear Technology,Xi’an 710024,China;2.School of Electronic and Information Engineering,Xi’an Jiaotong University,Xi’an 710049,China
Abstract:The charge conserving emission technique is presented in this paper. Based on the relationship between the charge and current distributions and Gauss law preservation, the emitting surface is triangulated, and the charged particle is initially located at the nearest conductor node to the conformal emission triangle. The motion trajectory of the charged particle is decided by two components: the normal component and the transversal component. The normal component is the displacement under the normal electric field of the emission triangle within one step; the transversal component is a random displacement parallel to the emission triangle, whose step size is constrained by the shape of the emission triangle. Currents generated by the movement of charged particles are distributed to the discrete grid according to the charge conserving law. As the charged particle starts from the conductor node, the conformal emission is free of nonphysical electrostatic accumulation. Finally a cylindrical diode is simulated to validate the technique.
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