炸药驱动冲击波铁电发生器脉冲充电电容器组

S. Shkuratov, E. Talantsev, J. Baird, L. Altgilbers, A. Stults
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引用次数: 3

摘要

采用超小型爆炸冲击波铁电发生器作为自主一次电源,对不同电容的电容器组进行充电。feg利用Pb(Zr52Ti48)O3 (PZT)多晶铁电陶瓷的纵向(当激波沿偏振矢量P传播时)激波去极化。PZT磁盘的直径范围从25到27毫米,三种不同的厚度:0.65,2.1和5.1毫米。实验表明,在充电过程中,feg能够产生峰值振幅达0.3 MW的脉冲功率。给出了电容CL = 2.25、4.5、9.0、18.0和36.0 nF时feg到电容器组的充电电压、电荷转移和能量转移的结果。实验数据分析表明,不同类型的铁电载能元件从FEG到电容器组的最大能量传输是不同的,并且与电容器组的电容有关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Pulse Charging of Capacitor Bank by Explosive-Driven Shock Wave Ferroelectric Generator
Ultracompact explosive-driven shock wave ferroelectric generators (FEGs) were used as autonomous primary power sources for charging capacitor banks of different capacitance. The FEGs utilized longitudinal (when the shock wave propagates along the polarization vector P) shock wave depolarization of Pb(Zr52Ti48)O3 (PZT) polycrystalline ferroelectric ceramic. PZT disks having diameters ranging from 25 to 27 mm and three different thicknesses: 0.65, 2.1, and 5.1 mm. It was experimentally shown that during the charging process the FEGs were capable of producing pulsed power with peak amplitudes up to 0.3 MW. Results for charging voltage, electric charge transfer and energy transfer from the FEGs to the capacitor banks of capacitances CL = 2.25, 4.5, 9.0, 18.0, and 36.0 nF are presented. Analysis of the experimental data shows that the maximum energy transfer from the FEG to the capacitor bank differs for each type of ferroelectric energy-carrying element, and is dependent upon the capacitance of the capacitor banks.
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