Voltage droop compensation based on resonant circuit for solid-state Marx generators
-
摘要: 在诸如粒子加速器等应用中，要求高压脉冲的电压、电流顶降尽可能低。减小顶降的常用方法是增加储能电容器的容量，但代价是系统的能效较低、体积较大、功率较高。另一种方法是插入一些特殊级来补偿电压顶降。在固态Marx发生器中，当谐振电感和补偿开关串联起来与普通级中的主电容并联时，就得到了补偿级。本文在16级单极性固态Marx发生器中加入了四个基于谐振电路的补偿级，以补偿不同负载、不同脉宽下的电压顶降。在放电过程中，将正弦电压的近线性部分加到负载上作为补偿，实现了几乎无电压顶降的矩形脉冲。不同的补偿级数可以对电压顶降进行不同程度的补偿，补偿效果也是可调的。此外，只要关断谐振管，这些补偿级也可以作为固态Marx发生器中的普通级工作，从而加以利用。由于谐振补偿级中的电容也与Marx电路中的电容并联充电，因此不需要辅助电源充电。实验结果表明，在400 Ω和5 kΩ阻性负载上，2.5 kV和10.5 kV脉冲的电压顶降分别都能得到理想的补偿。为了获得更好的补偿效果，脉冲宽度应小于正弦电压的近线性部分的长度。Abstract: The voltage droop of high-voltage pulses is required to be as low as possible in many industrial applications including particle accelerators. The commonly used method of reducing the droop is to increase the capacitance of the energy storage capacitors at the price of lower energy efficiency, bigger size, and higher power of the system. Another method is to insert some special stages to compensate for the voltage droop. When a resonant inductor and a switch in series are connected in parallel with the capacitor in a common stage in solid-state Marx generators (SSMGs), a compensation stage is obtained. In this paper, four compensation stages based on resonant circuit have been inserted into a 16-stage SSMG to compensate for the voltage droop with different loads and different pulse widths. The nearly linear part of the sinusoidal voltage is precisely added to the load during discharge as compensation and the rectangular pulsed voltage with little droop can be realized. Different numbers of compensation stages can compensate the droop to different levels, which means the compensation effect is also adjustable. Moreover, these compensation stages can also operate as common stages in Marx generators as long as the resonant circuits are open. Since the capacitors in resonant compensation stages are also charged in parallel with capacitors in common stages, no auxiliary power supply is required. Experimental results show that the droop of 2.5 kV and 10.5 kV pulses can be ideally compensated over 400 Ω and 5 kΩ resistive loads, respectively. The pulse widths should be shorter than the length of the nearly linear part of sinusoidal voltage for better compensation effect.
-
Key words:
- voltage droop compensation /
- Marx generator /
- pulsed power supply /
- resonant circuit
-
图 1 带谐振补偿级的正极性Marx拓扑
Figure 1. Unipolar SSMG with multi-stage voltage droop compensation
图 7 再充电过程和截尾示意图
Figure 7. Recharging operating mode and progress of truncating the wave tail
图 9 带四级谐振补偿的16级Marx发生器实物图
Figure 9. A 16-stage Marx generator with 4 resonant voltage droop compensation stages
图 10 不同负载下的输出电压波形
Figure 10. Voltage waveforms with different voltage droop over (a) 400-Ω and (b) 5-kΩ resistive loads
图 11 补偿后不同负载下的输出电压波形
Figure 11. Voltage waveforms with voltage droop compensation over (a) 400-Ω and (b) 5-kΩ resistive loads
图 12 1至4级补偿的电压波形
Figure 12. Waveforms with different number of stages of resonant voltage droop compensation
图 13 补偿后的2.5 kV电压波形及其第一级谐振电容电压波形
Figure 13. Waveform of the 2.5-kV output voltage after compensation and voltage of its capacitor Cres1
图 14 不同脉宽补偿后的2.5 kV输出电压波形
Figure 14. Waveform of the 2.5-kV output voltage after compensation with different pulse widths
-
[1] Canacsinh H, Redondo L M, Silva J F, et al. Voltage droop compensation based on resonant circuit for generalized high voltage solid-state Marx modulator[C]//2016 IEEE Applied Power Electronics Conference and Exposition (APEC). 2016: 3637-3640. [2] 刘克富. 固态Marx发生器研究进展[J]. 高电压技术, 2015, 41(6):1781-1787. (Liu Kefu. Research progress in solid-state Marx generators[J]. High Voltage Engineering, 2015, 41(6): 1781-1787Liu Kefu. Research progress in solid-state Marx generators[J]. High Voltage Engineering, 2015, 41(6): 1781-1787 [3] 饶俊峰, 邱剑, 刘克富. 脉冲压缩电路磁开关动态特性[J]. 强激光与粒子束, 2012, 24(4):859-862. (Rao Junfeng, Qiu Jian, Liu Kefu. Dynamic characteristics of magnetic switch with pulse compression circuit[J]. High Power Laser and Particle Beams, 2012, 24(4): 859-862 doi: 10.3788/HPLPB20122404.0859Rao Junfeng, Qiu Jian, Liu Kefu. Dynamic characteristics of magnetic switch with pulse compression circuit[J]. High Power Laser and Particle Beams, 2012, 24(4): 859-862 doi: 10.3788/HPLPB20122404.0859 [4] 戴栋, 宁文军, 邵涛. 大气压低温等离子体的研究现状与发展趋势[J]. 电工技术学报, 2017, 32(20):1-9. (Dai Dong, Ning Wenjun, Shao Tao. A review on the state of art and future trends of atmospheric pressure low temperature plasmas[J]. Transactions of China Electrotechnical Society, 2017, 32(20): 1-9Dai Dong, Ning Wenjun, Shao Tao. A review on the state of art and future trends of atmospheric pressure low temperature plasmas[J]. Transactions of China Electrotechnical Society, 2017, 32(20): 1-9 [5] 郑超. 低温等离子体和脉冲电场灭菌技术[D]. 杭州: 浙江大学, 2013Zheng Chao. Non-thermal plasma and pulsed electric field induced disinfection[D]. Hangzhou: Zhejiang University, 2013 [6] Elserougi A A, Faiter M, Massoud A M, et al. A transformerless bipolar/unipolar high-voltage pulse generator with low-voltage components for water treatment applications[J]. IEEE Transactions on Industry Applications, 2017, 53(3): 2307-2319. doi: 10.1109/TIA.2017.2666080 [7] 江伟华. 高重复频率脉冲功率技术及其应用: (6)代表性的应用[J]. 强激光与粒子束, 2014, 26:030201. (Jiang Weihua. Repetition rate pulsed power technology and its applications: (vi) typical applications[J]. High Power Laser and Particle Beams, 2014, 26: 030201 doi: 10.3788/HPLPB20142603.30201Jiang Weihua. Repetition rate pulsed power technology and its applications: (vi) typical applications[J]. High Power Laser and Particle Beams, 2014, 26: 030201 doi: 10.3788/HPLPB20142603.30201 [8] 李军, 严萍, 袁伟群. 电磁轨道炮发射技术的发展与现状[J]. 高电压技术, 2014, 40(4):1052-1064. (Li Jun, Yan Ping, Yuan Weiqun. Electromagnetic gun technology and its development[J]. High Voltage Engineering, 2014, 40(4): 1052-1064Li Jun, Yan Ping, Yuan Weiqun. Electromagnetic gun technology and its development[J]. High Voltage Engineering, 2014, 40(4): 1052-1064 [9] Canacsinh H, Silva F A, Redondo L M, et al. Increasing the voltage droop compensation range in generalized bipolar solid-state Marx modulador[C]//2017 IEEE 21st International Conference on Pulsed Power (PPC). 2017: 1-4. [10] Tang T, Burkhart C, Nguyen M. A vernier regulator for ILC Marx droop compensation[C]//2009 IEEE Pulsed Power Conference. 2009: 1402-1405. [11] Pfeffer H, Bartelson L, Bourkland K, et al. A long pulse modulator for reduced size and cost[C]//Twenty-First International Power Modulator Symposium, Conference. 1994: 48-51. [12] Cassel R L. Pulsed voltage droop compensation for solid state Marx modulator[C]//2008 IEEE International Power Modulators and High-Voltage Conference. 2008: 117-119. [13] Canacsinh H, Silva J F, Redondo L M. Dual resonant voltage droop compensation for bipolar solid-state Marx generator topologies[J]. IEEE Transactions on Plasma Science, 2019, 47(1): 1017-1023. doi: 10.1109/TPS.2018.2868495 [14] Canacsinh H, Silva J F, Redondo L M. PWM voltage droop compensation for bipolar solid-state Marx generator topologies[J]. IEEE Transactions on Plasma Science, 2017, 45(6): 975-980. doi: 10.1109/TPS.2017.2692392 [15] Canacsinh H, Silva F A, Redondo L M, et al. Optimized solid-state bipolar Marx modulador with resonant type droop compensation[C]//2017 IEEE 21st International Conference on Pulsed Power (PPC). 2017: 1-4. [16] Redondo L M, Canacsinh H, Silva J F. Generalized solid-state Marx modulator topology[J]. IEEE Transactions on Dielectrics and Electrical Insulation, 2009, 16(4): 1037-1042. doi: 10.1109/TDEI.2009.5211851 -
下载:
点击查看大图
计量
- 文章访问数: 1180
- HTML全文浏览量: 532
- PDF下载量: 123
- 被引次数: 0
