击穿电压
等离子体
电场
材料科学
电气故障
机械
阳极
气体放电
原子物理学
电刷放电
电压
化学
局部放电
电气工程
电极
光电子学
物理
物理化学
量子力学
电介质
工程类
作者
Chengzhi Guo,Hao Wu,Yanli Peng,Zhijiang Wang,Wei Jiang,Ya Zhang
标识
DOI:10.1088/1361-6463/ac923e
摘要
Abstract Micro-discharge is the process that gas breakdown occurs on a small spatial scale to generate plasma. With the decrease of the discharge scale, the high electric field makes the field emission (FE) play a leading role in the breakdown process of the micro-discharge, which is one of the reasons that the breakdown voltage deviates from the Paschen curve in a small gap. A one-dimensional implicit particle-in-cell Monte Carlo collision model is used to simulate the whole breakdown process of direct current micro-discharge sustained by FE in argon. The results show that the discharge after breakdown is in arc mode, the breakdown process can be divided into three stages: the pre-breakdown stage, the breakdown stage, and the post-breakdown stage. In the pre-breakdown stage, the sheath and plasma are not formed, the external electric field can penetrate the entire gap. In the breakdown stage, gas breakdown occurs. As the sheath is formed, the rate of change of plasma parameters increases rapidly and the discharge gap changes from capacitive to resistive. In the post-breakdown stage, the anode sheath gradually becomes thinner, but the region where the field is reversed still exists. The particle and energy balance gradually reach equilibrium, and the entire discharge evolves to a quasi-steady-state.
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