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Research of the anti-resonance pulse forming network and its application in the Marx generator

Published online by Cambridge University Press:  17 October 2016

Z.-L. Pan ,
J.-H. Yang  and
X.-B. Cheng
Z.-L. Pan
Affiliation:
College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, People's Republic of China
J.-H. Yang
Affiliation:
College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, People's Republic of China
X.-B. Cheng*
Affiliation:
College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, People's Republic of China
*
Address correspondence and reprint requests to: X.-B. Cheng, College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, People's Republic of China. E-mail: [email protected]
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Abstract

An anti-resonance pulse forming network (PFN) has been designed, analyzed, and tested for its application in generating quasi-square pulses. According to the circuit simulations, a compact generator based on two/three-section network was constructed. Two-section network is applied in the generator due to its compact structure, while three-section network is employed for generating pulses with higher quality. When two-section network is applied in the generator, the full-width at half-maximum of the load pulse is 400 ns, at the same time, its rise time, flat top and fall time are 90, 180 and 217 ns, respectively. When the three-section network is applied with the same pulse width of the load pulse, the rise time of the output decreases to 60 ns, while the flat top increases to 240 ns and the fall time reduces to 109 ns. Meanwhile, this kind of network could be used to shape the output pulses of generators whose equivalent circuit is LC series discharge network, such as MARX generator, into quasi-square pulses. And the preliminary experiment demonstrates that anti-resonance network could work well on four-stage Marx generators. A sine pulse generated by the four-stage Marx generator is shaped into a quasi-square pulse with voltage of 11.8 kV and pulse width about 110 ns based on two-section anti-resonance network.

Keywords

Anti-resonance networkQuasi-square pulsePulse generatorCompactMarx generator
Type
Research Article
Information
Laser and Particle Beams , Volume 34 , Issue 4 , December 2016 , pp. 675 - 686
Copyright
Copyright © Cambridge University Press 2016 

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References

REFERENCES

Caballero, L.S. & Smith, P.W. (2009). Compact pulsed-power generators for z-pinch applications – the starfish series. IEEE Trans. Plasma Sci. 37, 1948–1953.CrossRefGoogle Scholar
Clementson, J., Rahbarnia, K., Grulke, O. & Klinger, T. (2014). Design of A, B, and C pulse forming networks using the VINPFN application. IEEE Trans. Power Electr. 29, 5673–5679.Google Scholar
Domonkos, M.T., Heidger, S., Brown, D., Parker, J.V. & Gregg, C.W. (2010). Submicrosecond pulsed power capacitors based on novel ceramic technologies. IEEE Trans. Plasma Sci. 38, 2686–2693.Google Scholar
Hammon, J., Lam, S.K., Drury, D. & Ingram, M. (1997). Compact 1 MV, 10 Hz pulser. IEEE Pulsed Power Conf. vol. 1, 147–152.CrossRefGoogle Scholar
Kekez, M.M. (2001). A compact quasi-square waveform 15 kJ generator:15 ns risetime, 7.5 Ω load impedance and 100–500 ns pulse width. Pulse Power Plasma Sci. 2, 1027–1030.Google Scholar
Kim, A.A., Mazarakis, M.G., Sinebryukhov, V.A., Volkov, S.S., Kondratiev, S.S., Alexeenko, V.M., Bayol, F., Demol, G. & Stygar, W.A. (2012). Quasi-square pulse linear transformer driver. Phys. Rev. ST Accel. Beams 15, 040401.Google Scholar
Li, H., Ryoo, H.J., Kim, J.S., Rim, G.H., Kim, Y.B. & Deng, J. (2009). Development of rectangle-pulse Marx generator based on PFN. IEEE Trans. Plasma Sci. 37, 190–194.CrossRefGoogle Scholar
Nunnally, W.C. (2005). Critical component requirements for compact pulse power system architectures. IEEE Trans. Plasma Sci. 33, 1262–1267.Google Scholar
Pan, M.J. & Randall, C.A. (2010). A brief introduction to ceramic capacitors. IEEE Electr. Insul. Mag. (USA) 26, 44–50.Google Scholar
Sharma, S.K., Deb, P., Sharma, A., Shukla, R., Prabaharan, T., Adhikary, B. & Shyam, A. (2012). Note: Compact helical pulse forming line for the generation of longer duration rectangular pulse. Rev. Sci. Instrum. 83, 066103.CrossRefGoogle ScholarPubMed
Tewari, S.V., Umbarkar, S.B., Agarwal, R., Saroj, P.C., Sharma, A., Mittal, K.C. & Mangalvedekar, A. (2013). Development and analysis of PFN based compact Marx generator using finite integration technique for an antenna load. IEEE Trans. Plasma Sci. 41, 2684–2690.Google Scholar
White, H.J., Gillette, P.R. & Lebacqz, J.V. (1948). The pulse forming network. In Pulse Generators (Glasoe, G.N. and Lebacqz, V., Eds.), pp. 175–224. New York: McGraw-Hill.Google Scholar
Zhang, H., Yang, J., Lin, J. & Yang, X. (2013). A compact bipolar pulse-forming network-Marx generator based on pulse transformers. Rev. Sci. Instrum. 84, 114705.Google Scholar