Analysis of application range of simplified models for field to thermo-field to thermionic emission processes from the cathode

Li Sun, Zhuo Dai, Ming Xu, Wei Wang, Zeng-Yao Li
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Abstract

Electrons can escape from the cathode surface by acquiring enough energy greater than the work function or weakening the potential barrier at the cathode surface through tunneling effects in gas discharges, which plays a dominant role in the plasma-cathode interactions and is a key factor in many plasma phenomena and industrial applications. It is necessary to illustrate the various electron emission mechanisms and corresponding applicable description models to evaluate the impacts on discharge properties, especially for numerical simulation studies. However, most current researches usually rely on previous experience to select the appropriate simplified formula to calculate the electron emission current density, and there is little work that can explicitly give the application range of the simplified formulas for describing electron emission. In this work, the detailed expressions of the simplified formulas valid for field emission to thermo-field emission to thermionic emission typically used in the numerical simulation are proposed, and corresponding application ranges are determined in the framework of the Murphy-Good theory, which is commonly regarded as the general model and to be accurate in the full range of conditions of validity of the theory. The dimensionless parametrization is used to evaluate the emission current density of the Murphy-Good formula and a deviation factor is defined to obtain the application ranges for different work functions (2.5~5 eV), different cathode temperatures (300~6000 K), and different emitted electric field (105 ~1010 V‧m-1). The deviation factor is shown to be a non-monotonic function of the three parameters. A comparative study of particle number densities in atmospheric gas discharge with tungsten cathode is performed based on the one-dimensional implicit particle-in-cell with the Monte Carlo Collision (PIC-MCC) method according to the above application ranges. It is found that small differences in emission current density can lead to variation in the distributions of particle number density due to the change of collisional environment. This present work can provide a theoretical basis to select emission models for the subsequent numerical simulation.
分析从阴极场发射到热场发射再到热离子发射过程的简化模型的应用范围
在气体放电中,电子可以通过获得大于功函数的足够能量或通过隧道效应削弱阴极表面的势垒而从阴极表面逃逸,这在等离子体与阴极的相互作用中起着主导作用,是许多等离子体现象和工业应用中的关键因素。有必要说明各种电子发射机制和相应的适用描述模型,以评估其对放电特性的影响,尤其是对数值模拟研究而言。然而,目前大多数研究通常依靠以往的经验选择合适的简化公式来计算电子发射电流密度,很少有研究能明确给出描述电子发射的简化公式的应用范围。在这项工作中,提出了数值模拟中通常使用的场发射到热场发射再到热离子发射的简化公式的详细表达式,并在墨菲-古德理论的框架内确定了相应的应用范围,该理论通常被认为是通用模型,在理论的全部有效条件范围内都是准确的。利用无量纲参数来评估 Murphy-Good 公式的发射电流密度,并定义了一个偏差因子,从而得出不同功函数(2.5~5 eV)、不同阴极温度(300~6000 K)和不同发射电场(105 ~1010 V‧m-1)下的应用范围。结果表明,偏差因子是这三个参数的非单调函数。根据上述应用范围,基于一维隐式粒子入室与蒙特卡罗碰撞(PIC-MCC)方法,对钨阴极大气气体放电中的粒子数密度进行了比较研究。研究发现,由于碰撞环境的变化,发射电流密度的微小差异会导致粒子数密度分布的变化。本研究可为后续数值模拟选择发射模型提供理论依据。
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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