电子能量分布函数对高压高功率微波击穿全局模型的影响

S. Nam, J. Verboncoeur
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引用次数: 49

摘要

对于等离子体放电中的电子能量分布函数(EEDF),大多数体积平均全局模型假设为麦克斯韦分布。然而,在大多数放电中,除非电子-电子碰撞占主导地位,否则电子不处于平衡状态。假设麦克斯韦EEDF会导致等离子体放电的反应速率系数不准确,从而导致错误的击穿行为预测。由于碰撞等离子体的特性强烈依赖于这些系数,因此它们对于正确预测等离子体击穿非常重要。这项工作将证明EEDF对全局模型的影响,并提出一种方法来找到一个近似的EEDF,可以提高全局模型的保真度,用于预测高压状态下的高功率微波(HPM)击穿。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effect of electron energy distribution function on the global model for high power microwave breakdown at high pressures
Most volume-averaged global models assume a Maxwellian distribution for the electron energy distribution function (EEDF) in plasma discharges. The electrons, however, are not in the equilibrium in most discharges unless the electron-electron collision is dominant. The assumption of a Maxwellian EEDF can result in inaccurate reaction rate coefficients for the plasma discharge and lead to the wrong breakdown behavior prediction. Since the collisional plasma properties strongly depend on those coefficients, they are important to predict the plasma breakdown properly. This work will demonstrate the effect of the EEDF on the global model and propose a method to find an approximation of the EEDF that can improve the fidelity of the global model for prediction of high power microwave (HPM) breakdown in the high pressure regime.
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