闫家启, 孙国祥, 申赛康, 丁卫东. 伪火花放电初始发展过程的仿真研究[J]. 高电压技术, 2021, 47(7): 2572-2582. DOI: 10.13336/j.1003-6520.hve.20200218
引用本文: 闫家启, 孙国祥, 申赛康, 丁卫东. 伪火花放电初始发展过程的仿真研究[J]. 高电压技术, 2021, 47(7): 2572-2582. DOI: 10.13336/j.1003-6520.hve.20200218
YAN Jiaqi, SUN Guoxiang, SHEN Saikang, DING Weidong. Simulation Investigation on Initial Processes of Pseudospark Discharge[J]. High Voltage Engineering, 2021, 47(7): 2572-2582. DOI: 10.13336/j.1003-6520.hve.20200218
Citation: YAN Jiaqi, SUN Guoxiang, SHEN Saikang, DING Weidong. Simulation Investigation on Initial Processes of Pseudospark Discharge[J]. High Voltage Engineering, 2021, 47(7): 2572-2582. DOI: 10.13336/j.1003-6520.hve.20200218

伪火花放电初始发展过程的仿真研究

Simulation Investigation on Initial Processes of Pseudospark Discharge

  • 摘要: 伪火花放电是一种引燃于空心阴极结构,主放电通道呈现弥散特征的特殊低气压放电,在脉冲放电开关、电子束源等方面具有重要应用。为研究伪火花放电的初始过程,文中采用粒子模拟和蒙特卡洛碰撞方法(particle in cell/Monte Carlo collision, 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。通过研究电子、离子、电势等参量的演变特征,区分出触发电子推进、汤逊放电、虚阳极形成和透入、空心阴极放电、电势陷阱形成、离子耗尽等一系列子阶段,并确认了到达阳极的电子包含高能和低能两个组分。此外,研究了气压和初始电子参数对触发时延和阳极电流峰值的影响规律。仿真结果表明:气压和初始电子参数通过作用于阴极孔附近的离子密度和阴极空腔内部的电子密度分别对触发时延和电子电流峰值产生影响;随着气压、注入电荷量、电子能量和注入时间的增大,以及触发极位置的前移,触发时延不断缩短;随着电子能量的增大和触发极位置的前移,电子电流峰值有可能减小;并且,各参数的变化规律均呈现出饱和趋势。最后,讨论了阴极孔附近的离子耗尽和空心阴极阶段电流淬灭的可能联系,以及外回路电感值和PIC方法对伪火花放电仿真结果的影响。

     

    Abstract: Pseudospark discharge is a special kind of low pressure discharge which is ignited in hollow cathode, and the main discharge channel presents diffused characteristics. It is widely applied in pulsed discharge switch and electron beam sources. In this paper, to study the initial process of pseudospark discharge, a two-dimensional electrostatic plasma simulation model is built based on particle in cell and Monte Carlo collision method (PIC/MCC), which is coupled with external circuit elements. By studying the evolution of electrons, ions and electric potential, a series of sub-phases are distinguished, including trigger electron propagation, Townsend discharge, virtual anode formation and penetration, hollow cathode discharge, formation of potential hump, ion depletion, etc., and it is confirmed that electrons which reach anode consist of high energy and low energy components. In addition, the effects of gas pressure and initial electrons on trigger delay and peak value of anode electron current are studied. The simulation results show that all parameters affect the trigger delay and peak value of electron current, respectively, through the ion density near cathode aperture and the electron density inside the cathode cavity. As the gas pressure, charge amount, electron energy, injection time, and the forward movement of trigger position increase, the trigger delay can be shortened. However, as the electron energy and the forward movement of the trigger position increase, the peak value of electron current may decrease but show a saturation trend. Finally, the possible relationship between ion depletion near cathode aperture and current quenching at hollow cathode phase, as well as the influence of external circuit inductance and PIC method on the simulation results are discussed.

     

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