Simulation on breakdowns in the post-arc phase of a vacuum interruption

Zhenxing Wang, Haoran Wang, Yanjun Jiang, Liqiong Sun, Jianhua Wang, Yingsan Geng, Zhiyuan Liu
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Abstract

Breakdowns in the post-arc phase are affected by a combination effect of both plasma and metal vapor. The objective of this paper is to study the breakdown boundary as a function of plasma and metal vapor density. A fully kinetic PIC-MCC model was developed to study breakdowns in the post-arc phase. Relevant collisions were taken into consideration, and an external circuit was added to the model to make the calculations self-consistent. From the results, we obtained the breakdown boundary in the post-arc phase under effect of both metal vapor and residual plasma. The residual plasma does not play a major role in breakdowns if the density was below 1017 m-3. However, if the residual plasma density exceeded 1017 m-3, the critical metal atom density for a breakdown steeply decreased with the increase of the plasma density. Therefore, a sufficiently high plasma density gives rise to a higher probability of breakdowns. For this reason, the threshold of metal vapor density could be overestimated if the residual plasma is not considered in the simulations.
真空中断弧后阶段故障的模拟
电弧后阶段的击穿受到等离子体和金属蒸气的综合作用的影响。本文的目的是研究击穿边界作为等离子体和金属蒸气密度的函数。建立了一个完全动力学的PIC-MCC模型来研究弧后阶段的击穿。考虑了相关的碰撞,并在模型中加入了外部电路,使计算自洽。根据实验结果,得到了金属蒸气和残余等离子体作用下电弧后相击穿边界。当密度低于1017 m-3时,残余等离子体在击穿中不起主要作用。然而,当残余等离子体密度超过1017 m-3时,击穿的临界金属原子密度随等离子体密度的增加而急剧下降。因此,足够高的等离子体密度会导致更高的击穿概率。因此,如果在模拟中不考虑残余等离子体,金属蒸气密度阈值可能会被高估。
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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