1.西安科技大学电气与控制工程学院,陕西西安 710054
2.西安科技大学理学院,陕西西安 710054
[ "王党树 男,1976年生,陕西武功人.副教授,从事电力电子技术研究.E-mail:wangdangshu@126.com" ]
收稿:2020-08-01,
修回:2021-07-19,
纸质出版:2021-12-25
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王党树,栾哲哲,古东明等.基于火花试验装置的真空放电微观特性模拟研究[J].电子学报,2021,49(12):2449-2457.
WANG Dang-shu,LUAN Zhe-zhe,GU Dong-ming,et al.Simulation Research on the Microscopic Characteristics of Vacuum Discharge Based on Spark Test Device[J].ACTA ELECTRONICA SINICA,2021,49(12):2449-2457.
王党树,栾哲哲,古东明等.基于火花试验装置的真空放电微观特性模拟研究[J].电子学报,2021,49(12):2449-2457. DOI: 10.12263/DZXB.20200820.
WANG Dang-shu,LUAN Zhe-zhe,GU Dong-ming,et al.Simulation Research on the Microscopic Characteristics of Vacuum Discharge Based on Spark Test Device[J].ACTA ELECTRONICA SINICA,2021,49(12):2449-2457. DOI: 10.12263/DZXB.20200820.
为了研究火花试验装置中电极在真空中放电的微观特性,本文建立了在真空环境下,以钨为阳极材料、镉为阴极材料的二维平行板放电模型.采用PIC/MCC(Particle-In-Cell
/
Monte Carlo Collision)方法对该模型进行仿真,研究了不同电子发射机制下平行板电极放电的发展过程以及空间场强、阴极表面温度和场增强因子对空间电子变化的影响,得到在场致发射、热发射以及热-场致发射作用下放电过程中的电子浓度和阳极吸收电流的变化以及电子密度和电势的空间分布等.研究发现,场致发射是微间隙阴极电子发射的主导发射机制,当阴极表面温度在焦耳热的作用下达到镉金属的沸点1040K时将产生镉蒸汽,电流密度和电子浓度逐渐增大,此时热发射将开始作用于微间隙放电;当温度大于镉金属气化温度后,场强的影响将大于温度的影响;当场增强因子很小时,热发射几乎不起作用,随着场增强因子不断增大,热发射的作用逐渐增强,导致空间电子浓度明显增加,真空环境下微间隙放电是由热-场共同作用的.
In order to study the micro-characteristics of the electrode discharge in the spark test device in vacuum
this paper established a two-dimensional parallel plate discharge model in a vacuum environment with tungsten as the anode material and cadmium as the cathode material. We simulate the model with the PIC/MCC(Particle-In-Cell/Monte Carlo Collision) method
studies the development process of parallel plate electrode discharge under different electron emission mechanisms and the influence of space field strength
cathode surface temperature and field enhancement factor on the changes of space electrons
and obtains the field emission
thermal emission and thermal-field emission changes in the electron concentration and anode absorption current during the discharge process
as well as the spatial distribution of the electron density and electric potential
etc. The research has found that field emission is the dominant emission mechanism of micro-gap cathode electron emission. When the cathode surface temperature reaches 1040K
the boiling point of cadmium metal under the action of Joule heat
cadmium vapor will be generated
and the current density and electron concentration will gradually increase. At this time
the thermal emission will start to act on the micro-gap discharge. When the temperature is greater than the vaporization temperature of cadmium metal
the influence of the field strength will be greater than that of the temperature. When the field enhancement factor is very small
the thermal emission is almost ineffective. As the field enhancement factor continues to increase
the effect of thermal emission gradually increases
leading to a significant increase in the spatial electron concentration. The micro-gap discharge in a vacuum environment is caused by the combined effect of heat and field.
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