高功率紧凑PFN-Marx发生器研究进展综述

刘世飞; 张建德; 张自成

doi:10.11884/HPLPB202234.210483

高功率紧凑PFN-Marx发生器研究进展综述

doi: 10.11884/HPLPB202234.210483

国防科技大学前沿交叉学科学院，长沙 410073

基金项目: 国家自然科学基金项目（51677190，51707199）；湖南省自然科学基金项目（2017JJ1005）

详细信息

作者简介:
刘世飞，liushifei16@nudt.edu.cn

通讯作者:
张建德，zhangjiande@nudt.edu.cn

中图分类号: TM214
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- 被引次数: 0
出版历程
- 收稿日期: 2021-11-10
- 修回日期: 2022-02-22
- 网络出版日期: 2022-06-15
- 刊出日期: 2022-05-12

Review of high power compact pulse forming network-Marx generators

College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China

摘要

摘要:
PFN-Marx发生器可同时实现升压和脉冲形成，具有紧凑的基因。特别是近年来脉冲储能技术的发展，使得直接利用PFN-Marx发生器驱动各类负载成为现实，因而PFN-Marx发生器逐渐成为国内外研究热点。对国内外的高功率紧凑PFN-Marx发生器的研究进展进行了系统介绍，评述其参数和结构特点。通过总结，从时间发展历程上看，PFN-Marx发生器采用高储能密度器件，装置的储能密度水平在不断地提高，尺寸紧凑化水平也在提高；在追求紧凑化的手段上，PFN-Marx发生器的空间结构的优化设计效果优于PFN网络拓扑参数的优化设计；PFN-Marx发生器采用波形优化方法具有较明显的收益，可有效降低装置紧凑化带来级间分布参数更强耦合的负面影响。同时论文探讨了PFN-Marx发生器的发展趋势，为PFN-Marx发生器的研究和技术路线探索提供参考和依据。
- 高功率 /
- 脉冲形成网络 /
- PFN-Marx发生器 /
- 高储能密度
Abstract:
The pulse forming network (PFN)-Marx generator can realize both integration of pulse modulation and pulse voltage accumulation, exhibiting a the natural “gene” of compactness. In recent years, the pulsed energy storage technology has been developing rapidly, which makes it a reality to use PFN-Marx generators to drive various loads directly. The PFN-Marx generator has gradually become a worldwide research focus. The research progress of high-power compact PFN-Marx generators are systematically introduced in this paper. In summary, judging from the development over time, PFN-Marx generators adopt high-energy-density components and thus improve the energy density level themselves, which makes the generator more and more compact. In the pursuit of compactness, the effect of optimal design of PFN-Marx generator spatial structure is better than optimal design of PFN network topology parameters. The waveform optimization method of the PFN-Marx generator has obvious benefits, which can effectively reduce the negative impact of stray parameters strongly coupling between stages caused by small size of generator. In the meanwhile, this paper discusses the development trend of PFN-Marx generator.
- high power /
- pulse forming network /
- PFN-Marx generator /
- high energy storage density

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图 1 PFN-Marx发生器典型电路图

Figure 1. Typical circuit diagram of PFN-Marx generator

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图 2 NRCC PFN-Marx发生器装置图

Figure 2. NRCC setup diagram of PFN-Marx generator

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图 3 输出电压波形图

Figure 3. Waveform of output pulse

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图 4 AE PFN-Marx发生器装置图

Figure 4. AE setup diagram of PFN-Marx generator

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图 5 输出电压波形图

Figure 5. Waveform of output pulse

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图 6 TTU PFN-Marx发生器装置图

Figure 6. TTU setup diagram of PFN-Marx generator

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图 7 PFN结构图

Figure 7. Structural diagram of a PFN

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图 8 PAL PFN-Marx发生器装置图

Figure 8. PAL setup diagram of PFN-Marx generator

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图 9 输出电压波形图

Figure 9. Waveform of output pulse

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图 10 APELC PFN-Marx发生器电路图

Figure 10. APELC circuit diagram of PFN-Marx generator

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图 11 输出电压波形图

Figure 11. Waveform of output pulse

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图 12 中国工程物理研究院PFN-Marx发生器装置图

Figure 12. CAEP setup diagram of PFN-Marx generator

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图 13 输出电压波形图

Figure 13. Waveform of output pulse

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图 14 印度PFN-Marx发生器装置图

Figure 14. Indian setup diagram of PFN-Marx generator

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图 15 陡化开关及陡化电容

Figure 15. Peaking gap and the peaking capacitor

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图 16 无陡化电容输出电压波形

Figure 16. Waveform of output pulse without peaking capacitor

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图 17 采用陡化电容输出电压波形

Figure 17. Waveform of output pulse with peaking capacitor

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图 18 CEAEA PFN-Marx发生器装置图

Figure 18. CEAEA setup diagram of PFN-Marx generator

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图 19 输出电压波形图

Figure 19. Waveform of output pulse

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图 20 中国工程物理研究院PFN-Marx发生器装置图

Figure 20. CAEP setup diagram of PFN-Marx generator

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图 21 PFN结构图

Figure 21. Structural diagram of a PFN

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图 22 输出电压波形图

Figure 22. Waveform of output pulse

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图 23 国防科技大学PFN-Marx发生器装置图

Figure 23. NUDT setup diagram of PFN-Marx generator

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图 24 输出电压波形图

Figure 24. Waveform of output pulse

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图 25 国防科技大学PFN结构图

Figure 25. NUDT structural diagram of a PFN

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图 26 输出电压波形图

Figure 26. Waveform of output pulse

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表 1 典型装置参数对比

Table 1. Comparison of typical device parameters

setup	year	pulse width/ns	output voltage/kV	rising edge/ns	repetition rate/Hz	peak power/GW	impedance/Ω	energy density/(J·L⁻¹)
NRCC	2001	500	300	15	10	12	7.5	2
AE	2009	1000	500	＜200	5	5	50	2
TTU	2005	200	250	＜80	10	3.3	18.5	10
CAEP	2017	180	980	40	30	16	50	3
CEAEA	2018	85	400	＜5	100	1.6	100	2
NUDT	2020	90	540	45	30	5	50	6.5
Note: NRCC—National Research Council of Canada, AE—Applied Energetics of USA, TTU—Texas Tech University of USA,CAEP—China Academy of Engineering Physics, CEAEA—Commissariat à l’Energie Atomique et aux Energies Alternatives of France, NUDT—National University of Defense Technology of China

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