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Gas discharge in a gas peaking switch

机译:气体峰值开关中的气体排放

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The gas discharge in a gas peaking switch was experimentally studied and numerically simulated. For Simulation, the discharge was divided into two phases, gas breakdown and voltage collapse. The criterion for an electron avalanche to transit to streamer was considered as the criterion of gas breakdown. The spark channel theory developed by Rompe-Weizel was used to calculate the spark resistance. It was found that the prepulse considerably lowers the voltage pulse applied to the gap. Even for a given input pulse, the voltage pulse applied to a peaking gap is different for different gap distance due to existence of a different prepulse. In this case, the breakdown voltage of it gas peaking gap depends on gas pressure and gap distance, individually. For nitrogen pressure varying from 3 Wit to 10 Wit and gap distance from 0.6 mm to 1.2 mm, the peak electric field higher than 2 MV/cm was achieved when breakdown. The output 10% to 90% rise time, t(r), varies from 145 ps to 192 ps. As gas pressure increases, t(r) decreases, which can be explained by the fact that the breakdown field increases with the increase of gas pressure. It was found in experiment that the jitter in t(r) could be attributed to the jitter in breakdown field. Instead of getting longer, the averaged experimental t(r) gets shorter as gap distance increases front 0.6 rum to 1.2 mm, which differs from the results of calculation and indicates there may exist something. other than electric field, that is also related to t(r). The reason for this difference may lies in the inverse coefficient of spark resistance varying with gap distance. On the whole, the results from the calculations agree with the experimental ones.
机译:对气体峰值开关中的气体排放进行了实验研究和数值模拟。为了进行仿真,将放电分为两个阶段:气体击穿和电压崩溃。电子雪崩转移到流光的标准被认为是气体击穿的标准。由Rompe-Weizel开发的火花通道理论用于计算火花阻力。已经发现,预脉冲大大降低了施加到间隙的电压脉冲。即使对于给定的输入脉冲,由于存在不同的预脉冲,对于不同的间隙距离,施加到峰值间隙的电压脉冲也会不同。在这种情况下,其气体峰值间隙的击穿电压分别取决于气体压力和间隙距离。对于从3 Wit到10 Wit的氮气压力和从0.6 mm到1.2 mm的间隙距离,击穿时可实现高于2 MV / cm的峰值电场。输出10%至90%的上升时间t(r)在145 ps至192 ps之间变化。随着气压的增加,t(r)减小,这可以通过以下事实来解释:击穿场随着气压的增加而增加。在实验中发现,t(r)中的抖动可归因于击穿场中的抖动。随着间隙距离将前端0.6 rum增大到1.2 mm,平均实验t(r)不再变长,这与计算结果有所不同,表明可能存在某些东西。除了电场,它也与t(r)有关。这种差异的原因可能在于火花电阻的反系数随间隙距离而变化。总体而言,计算结果与实验结果吻合。

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