强激光与粒子束, 2010, 22 (2): 447, 网络出版: 2010-05-28   

赝火花开关放电的蒙特卡罗粒子模拟

Particle-in-cell simulation of pseudospark switch based on particle-in-cell plus Monte-Carlo collision method
作者单位
1 中国工程物理研究院 应用电子学研究所,四川 绵阳 621900
2 中国工程物理研究院 研究生部,北京 100088
摘要
采用粒子模拟和蒙特卡罗相结合的方法,应用静电求解模型,对赝火花开关初始放电过程进行了模拟。赝火花开关初始放电过程主要由汤森放电过程、等离子体形成、空心阴极效应和场致发射引发主放电组成;等离子体形成和空心阴极效应对赝火花开关的发展导通具有至关重要的作用。改变赝火花开关工作参数,如气压、电极孔径、阳极电压和阴极腔中初始粒子密度,研究其对赝火花开关电子峰值电流形成时间的影响。结果表明:随着气压、电极孔径、阳极电压和初始粒子密度的增大,赝火花开关电子峰值电流形成时间减小。
Abstract
The initial discharge process of pseudospark switch has been simulated via a electrostatic particle-in-cell plus Monte-Carlo collision method. The pseudospark discharge process mainly consists of Townsend process,plasma formation,hollow cathode effect and main discharge induced by field emission. The plasma formation and hollow cathode effect are critical for the conduction. Then the parameters,i.e. gas pressure,electrode borehole diameter,anode voltage and initial particle density,were varied and their effect on the forming time of electron peak current of the pseudospark switch was investigated. The results show that as the parameters increase,the forming time of electron peak current lessens.
参考文献

[1] 邱毓昌. 伪火花开关的发展与应用[J]. 电工电能新技术,1997,(4):10-13.(Qiu Yuchang. Development and applications of pseudospark switches.Advanced Technology of Electrical Engineering and Energy,1997,(4):10-13)

[2] Destler W W,Segalov Z,Rodgers J,et al. High power,high brightness electron beam generation in a pulse-line pseudospark discharge[J].Appl Phys Lett,1993,62(4):1739-1741.

[3] 江兴流. 赝火花强流脉冲粒子束及其应用[C]//全国高功率粒子束十年文集.1995.(Jiang Xingliu. Intense current pulsed electron beam and application of pseudospark//The Decade Selected Works of High Pulsed Power in China.1995)

[4] Donko Z,Ioannis G M. Hybrid model of a rectangular hollow cathode discharge[J].Phys Rev Lett,1998,57(6):7126-7137.

[5] 祝大军,刘盛纲,石金水,等. 假火花开关初始放电过程的理论计算[J]. 强激光与粒子束,1996,8(1):123-130.(Zhu Dajun,Liu Shenggang,Shi Jinshui,et al. The theoretical computation of initial pseudospark switch discharge process.High Power Laser and Particle Beams,1996,8(1):123-130)

[6] 赖建军,余建华,黄建军,等. 空心阴极直流放电的二维自洽模型描述和阴极溅射分析[J]. 物理学报,2001,50(8):1528-1533. (Lai Jianjun,Yu Jianhua,Huang Jianjun,et al. Self-consistent description of a DC hollow cathode discharge and analysis of cathode sputtering.Acta Physica Sinica,2001,50(8):1528-1533)

[7] Boeuf J P,Pitchford L C. Pseudospark discharges via computer simulation[J].IEEE Trans on Plasma Sci,1991,19(4):286-296.

[8] Choi P,Chuaqui H,Favre M,et al. Breakdown formation in a transient hollow cathode discharge[J].IEEE Trans on Plasma Sci,1995,23(6):221-228.

[9] Cetiner S O,Stoltz P,Messmer P. Dependence of electron peak current on hollow cathode dimensions and seed electron energy in a pseudospark discharge[J].Journal of Applied Physics,2008,103:023304

秦风, 常安碧, 丁恩燕, 罗敏. 赝火花开关放电的蒙特卡罗粒子模拟[J]. 强激光与粒子束, 2010, 22(2): 447. Qin Feng, Chang Anbi, Ding Enyan, Luo Min. Particle-in-cell simulation of pseudospark switch based on particle-in-cell plus Monte-Carlo collision method[J]. High Power Laser and Particle Beams, 2010, 22(2): 447.

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