平行极板电极间N2负流光的二维模拟

Zheng Dian-chun, Zhu Shi-hua, Zhang Zhong-lin, Lv Shu-ming
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引用次数: 1

摘要

为了深入理解氮介质中流光放电的行为,建立了基于电子、离子连续方程与泊松方程耦合的气体放电二维自一致流体模型。本文通过数值模拟研究了负流放电的等离子体通道。基于全二维有限元法,编制了求解空间电荷电场作用下带电粒子连续方程的程序。给出了纯N2中平行极板电极间圆柱对称流线的二维模拟结果。用数值方法观察了负流的形成和传播。利用该模型对空间电场分布、空间离子分布和漂移速度进行了预测。研究了初始条件和外加电压对流光特性的影响。结果表明:随着负流光的传播,流光尖端的空间电场和电子、离子密度增大;随着初始电离密度的增大,流线尖端的空间电子密度和电场也随之增大。流的传播速度和其他特性受初始电荷分布直径的影响。负流光的电离密度、电子密度梯度和尖端电场随外加电场的增大而增大。
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Two-dimensional simulation of the negative streamer in N2 between parallel-plate electrodes
With the purpose of deeply understanding behavior of streamer discharge in nitrogen-dielectric, the two-dimensional and self-consistent fluid model of the gas discharge was established based on the electron and ion continuity equations coupled to Poisson's equation. The plasma channel of the negative streamer discharge is studied in this paper by numerical simulation. A program based on the finite element method in its full two-dimension form is developed and employed for the solution of continuity equations of charged particles under the effect of space-charge electric field. Results of two-dimensional simulation of cylindrically symmetric streamer in pure N2 between parallel-plate electrodes are presented. The formation and propagation of negative streamer in numerically was observed. The space electric field distribution, space ions distribution and drift velocity were predicted by the model. The influence of initial conditions and applied voltages on the streamer characteristic was also investigated. The results show that the space electric field and electrons and ions density at the tip of the streamer increase with the propagation of negative streamer. The space electrons density and electric field at the tip of streamer increase, when the ionization density in the initial increase. The propagation velocity and other characteristics of the streamer are influenced by the diameter of the initial charge distribution. For negative streamer, the ionization density and electron density gradient and electric field at the tip increase with increasing applied field.
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