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基于Marx的任意极性方波脉冲电源设计

姜松 黄利飞 饶俊峰 王永刚 李孜

姜松, 黄利飞, 饶俊峰, 等. 基于Marx的任意极性方波脉冲电源设计[J]. 强激光与粒子束, 2022, 34: 055001. doi: 10.11884/HPLPB202234.210405
引用本文: 姜松, 黄利飞, 饶俊峰, 等. 基于Marx的任意极性方波脉冲电源设计[J]. 强激光与粒子束, 2022, 34: 055001. doi: 10.11884/HPLPB202234.210405
Jiang Song, Huang Lifei, Rao Junfeng, et al. Design of arbitrary polarity rectangular pulse power supply based on Marx[J]. High Power Laser and Particle Beams, 2022, 34: 055001. doi: 10.11884/HPLPB202234.210405
Citation: Jiang Song, Huang Lifei, Rao Junfeng, et al. Design of arbitrary polarity rectangular pulse power supply based on Marx[J]. High Power Laser and Particle Beams, 2022, 34: 055001. doi: 10.11884/HPLPB202234.210405

基于Marx的任意极性方波脉冲电源设计

doi: 10.11884/HPLPB202234.210405
基金项目: 上海市扬帆计划项目(19YF1435000)
详细信息
    作者简介:

    姜 松,jecifer@163.com

    通讯作者:

    饶俊峰,jfrao@usst.edu.cn

  • 中图分类号: TM832

Design of arbitrary polarity rectangular pulse power supply based on Marx

  • 摘要: 设计了一种基于Marx电路的方波脉冲电源,该电源采用磁环隔离驱动方案与全桥Marx电路相结合,实现了正极性、负极性和双极性高压方波脉冲的输出,解决了常规脉冲电源只能输出特定极性脉冲的限制。对电路的运行模式经行了理论分析,并搭建了16级实验样机。实验结果表明:在空载条件下,实现了频率1 kHz,幅值10 kV的正极性、负极性及双极性高压方波脉冲输出。其最小脉宽1 µs,极性可调。该脉冲电源结构紧凑,可以实现输出电压、脉宽、脉冲极性可调。最后使用该方波脉冲电源驱动平行板介质阻挡放电反应器。结果表明:该方波脉冲电源可以作为介质阻挡放电驱动源。
  • 图  1  Marx主电路

    Figure  1.  Marx circuit

    图  2  Marx主电路两级子模块

    Figure  2.  Two-stage sub-modules of Marx circuit

    图  3  传统控制方案时序图

    Figure  3.  Time sequence diagram of traditional control scheme

    图  4  改进不同脉冲极性控制时序图

    Figure  4.  Time sequence diagram of improved control signal

    图  5  驱动电路图

    Figure  5.  Drive circuit diagram

    图  6  实验硬件平台

    Figure  6.  Experimental hardware platform

    图  7  不同脉宽下输出脉冲波形

    Figure  7.  Output pulse waveform under different pulse widths

    图  8  不同极性下的输出电压波形

    Figure  8.  Output voltage waveforms under different polarity

    图  9  1kHz下输出电压波形

    Figure  9.  1 kHz output voltage waveforms

    图  10  不同极性脉冲下介质阻挡放电电压电流波形

    Figure  10.  Voltage and current waveforms of dielectric barrier discharge under different polarity pulses

    图  11  不同极性脉冲下介质阻挡放电

    Figure  11.  Dielectric barrier discharge under different polarity pulses

  • [1] Yang W X, Sun M X, Song H J, et al. A novel method to synthesize luminescent silicon carbide nanoparticles based on dielectric barrier discharge plasma[J]. J. Mater. Chem. C, 2020, 8(47): 16949-16956. doi: 10.1039/D0TC04658B
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    [11] Canacsinh H, Redondo L M, Silva J F. Marx-type solid-state bipolar modulator topologies: performance comparison[J]. IEEE Transactions on Plasma Science, 2012, 40(10): 2603-2610. doi: 10.1109/TPS.2012.2190944
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    [13] 葛劲伟, 姜松, 饶俊峰, 等. 全固态高压双极性方波脉冲叠加器的研制[J]. 高电压技术, 2019, 45(04):1305-1312. (Ge Jinwei, Jiang Song, Rao Junfeng, et al. Development of all-solid-state bipolar pulse adder with high voltage rectangular wave pulses output[J]. High Voltage Engineering, 2019, 45(04): 1305-1312
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出版历程
  • 收稿日期:  2021-09-10
  • 修回日期:  2021-12-20
  • 录用日期:  2022-02-22
  • 网络出版日期:  2022-03-02
  • 刊出日期:  2022-05-15

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