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自触发驱动的全固态Marx发生器
引用本文:饶俊峰,李恩成,王永刚,姜松,李孜.自触发驱动的全固态Marx发生器[J].强激光与粒子束,2021,33(2):025001-1-025001-7.
作者姓名:饶俊峰  李恩成  王永刚  姜松  李孜
作者单位:上海理工大学 机械工程学院,上海 200093
基金项目:国家自然科学基金青年基金项目(51707122);国家重点研发计划数字诊疗专项(2019YFC0119100);上海市青年科技英才扬帆计划(19YF1435000)
摘    要:随着全固态高压脉冲发生器在材料改性、生物医学和工业等领域上的广泛应用,全固态脉冲发生器正朝着小型化、智能化和模块化方向发展。为了进一步减小电源的体积、降低成本,提出了一种自触发驱动的正极性全固态Marx发生器的拓扑。只需提供一路隔离信号控制一级放电开关管的导通和关断,通过级间电容对相邻级的放电管门极自动充电和放电,使其依次导通和关断。这种拓扑使得Marx发生器中的多个开关管的驱动电路简单很多,无需提供隔离供电的多路驱动电源,且避免了开关的动态、静态均压问题。基于这种拓扑搭建了一台17级的正极性Marx发生器样机,且电压幅值和脉宽都连续可调,在10 kΩ纯阻性负载上输出10 kV、重复频率100 Hz的正极性高压脉冲,脉冲前沿约为328 ns。样机体积小巧、工作稳定,验证了该方案的可行性。

关 键 词:自触发驱动    Marx发生器    脉冲发生器    脉冲功率
收稿时间:2020-07-30

Self-triggering all-solid-state Marx generator
Institution:School of Mechanical Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
Abstract:With the wide application of all-solid-state high-voltage pulse generators in the fields of material modification, biomedicine and industry, all-solid-state pulse generators are developing in the direction of miniaturization, intelligence and modularization. To further reduce the volume and cost of the power supply, this paper proposes a positive self-triggering all-solid-state Marx generator topology. It only needs to provide an isolated signal to control the turn-on and turn-off of discharging switch in the first stage, and the gates of the adjacent-stage discharging switches will be automatically charged and discharged through the inter-stage capacitors, so that they turn on and off one by one. This topology makes the driving circuit of the multiple switches in the Marx generators much simpler and does not need to provide a multi-channel driving power supply with isolated power supplies, and also avoids the dynamic and static voltage balancing problems of the switches. Based on this topology, a 17-stage positive polarity Marx generator prototype is built, and the voltage amplitudes and pulse widths are continuously adjustable. It outputs 10 kV positive high-voltage pulses at a repetition frequency of 100 Hz over a 10 kΩ resistive load. The leading edge is approximately 328 ns. The prototype is small in size and stable in work, which verifies the feasibility of this topology.
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