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Numerical Simulation of the Gas Discharge in a Gas Peaking Switch

机译:气体调峰开关中气体排放的数值模拟

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The gas discharge in a gas peaking switch was divided into three phases as gas breakdown, voltage collapse, and gaseous recovery. The development of the discharge was numerically simulated. Nitrogen and hydrogen at pressure ranging from 30 to 100 atm were chosen as working gases. The breakdown field of nitrogen is much higher than that of hydrogen, and a value of 4 MV/cm is achieved for a 0.6-mm nitrogen gap at the pressure of 100 atm. Depending strongly on the breakdown field, the rise time of the output pulse from the nitrogen gap is much shorter than that from the hydrogen gap. The shortest rise time of 108 ps for 0.6-mm nitrogen gap at the pressure of 100 atm is obtained. The gaseous recovery of the extinguished spark channel depends mainly on the recovery of gas density resulting from the falling of the channel temperature due to the axial heat flow out from the channel through the metal electrodes. Hydrogen is much better than nitrogen for gaseous recovery. Electrode material also plays an important role.
机译:气体峰值开关中的气体放电分为三个阶段,分别为气体击穿,电压崩溃和气体回收。对放电的发展进行了数值模拟。选择压力范围为30至100 atm的氮气和氢气作为工作气体。氮的击穿场远高于氢的击穿场,在100 atm的压力下,0.6 mm的氮间隙可达到4 MV / cm。强烈地取决于击穿场,来自氮间隙的输出脉冲的上升时间比来自氢间隙的输出脉冲的上升时间短得多。在100 atm的压力下,对于0.6 mm的氮气间隙,可获得最短的108 ps上升时间。熄灭的火花通道的气体恢复主要取决于由于轴向热量从通道通过金属电极流出而导致的通道温度下降而导致的气体密度恢复。氢气比氮气要好得多。电极材料也起着重要作用。

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