孙国祥, 申赛康, 闫家启, 丁卫东. 伪火花放电初始阶段电势势垒形成的仿真研究[J]. 高电压技术, 2022, 48(1): 358-365. DOI: 10.13336/j.1003-6520.hve.20201839
引用本文: 孙国祥, 申赛康, 闫家启, 丁卫东. 伪火花放电初始阶段电势势垒形成的仿真研究[J]. 高电压技术, 2022, 48(1): 358-365. DOI: 10.13336/j.1003-6520.hve.20201839
SUN Guoxiang, SHEN Saikang, YAN Jiaqi, DING Weidong. Simulation Investigation on the Formation of Potential Barrier in the Initial Stage of Pseudospark Discharge[J]. High Voltage Engineering, 2022, 48(1): 358-365. DOI: 10.13336/j.1003-6520.hve.20201839
Citation: SUN Guoxiang, SHEN Saikang, YAN Jiaqi, DING Weidong. Simulation Investigation on the Formation of Potential Barrier in the Initial Stage of Pseudospark Discharge[J]. High Voltage Engineering, 2022, 48(1): 358-365. DOI: 10.13336/j.1003-6520.hve.20201839

伪火花放电初始阶段电势势垒形成的仿真研究

Simulation Investigation on the Formation of Potential Barrier in the Initial Stage of Pseudospark Discharge

  • 摘要: 伪火花放电是一种工作于巴申曲线左半支的特殊低气压放电,在气体开关、电子束源等方面具有重要应用。当气压较低时,伪火花放电在空心阴极放电阶段的末尾会在阴极孔处形成电势势垒,阻碍阴极腔内电子的流出,从而阻碍放电的进一步发展。为研究电势势垒的形成过程,采用粒子模拟和蒙特卡洛碰撞方法(PIC/MCC),建立了与外回路元件相耦合的二维静电等离子体仿真模型。通过研究阴极孔区域的电势与电荷变化,发现当气压较低时虚阳极形成后,阴极孔处电势下降速度过快加速了阴极孔内电子的流出,直至电子消耗殆尽最终形成电势势垒。仿真结果发现:增大气压可以有效增大阴极孔内的电子数、离子数以及电子的碰撞电离率,从而使电势势垒的形成时间不断向后推移乃至完全抑制;虚阳极形成后阴极孔内的碰撞电离主要由空心阴极放电阶段产生的大量自由电子维持,二次电子发射对虚阳极和鞘层电场的维持作用仅占20%。

     

    Abstract: Pseudospark discharge is a kind of special low pressure discharge which works in the left half branch of Paschen curve. It has important applications in gas switch and electron beam sources. When the pressure is low, the potential barrier will be formed at the cathode hole at the end of the hollow cathode discharge stage, which will hinder the outflow of electrons in the cathode cavity and thus hinder the further development of discharge. In order to study the formation process of potential barrier, particle simulation and Monte Carlo collision method (PIC/MCC) are used in this paper to establish a two-dimensional electrostatic plasma simulation model coupled with external circuit elements. By studying the variations of electric potential and charge in the cathode hole area, it is found that when the virtual anode is formed at low pressures, the electric potential at the cathode hole decreases rapidly, which accelerates the outflow of electrons in the cathode hole until the electrons are exhausted and finally forms the electric barrier. The simulation results show that increasing gas pressure can effectively increase the number of electrons, ions and the probability of collision ionization of electrons in the cathode hole, so that the formation time of the barrier can be continuously pushed back or even completely suppressed. After the formation of the virtual anode, the collision ionization in the cathode hole is mainly maintained by a large number of free electrons generated during the discharge stage of the hollow cathode, and the effect of secondary electron emission on the electric field establishment of the virtual anode and sheath layer is only 20%.

     

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