具有微尺度间隙的平面电极在空气中的暗弧转换*

Andrew D. Strongrich, Gayathri Shivkumar, Alina A. Alexeenko, D. Peroulis
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引用次数: 0

摘要

在Paschen定律预测的阈值电压下,由于电子冲击电离和二次电子发射产生的电子雪崩而发生电击穿。对于典型的气体放电,击穿标志着汤森暗放电制度的结束,然后是正常的辉光制度,其中电流在长电压范围内保持恒定。对于这样的放电,电极护套由二次电子维持,护套厚度对应于给定气体压力1下斯托列托夫点处的电极间隙。在微尺度的电极间隙,电子从阴极的量子隧穿,称为场发射,变得重要,从而降低击穿电压。这遵循修改后的Paschen曲线2。然而,在某些结构中,即平面电极,击穿后不是正常的发光状态,而是直接过渡到电弧状态,其中电流峰值达到高值3。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Dark-to-Arc Transition in Air for Planar Electrodes with Microscale Gaps *
Electrical breakdown at threshold voltages predicted by Paschen's law occurs due to electron avalanches created by electron impact ionization and secondary electron emission from the electrodes. For a typical gas discharge, breakdown marks the end of the Townsend dark discharge regime and is followed by the normal glow regime where the current stays constant over a long range of voltages. For such a discharge, the electrode sheath is sustained by secondary electrons and the sheath thickness corresponds to the electrode gap at Stoletov's point for a given gas pressure 1. At microscale electrode gaps, quantum tunneling of electrons from the cathode, termed field emission, becomes significant thereby reducing the breakdown voltage. This follows the modified Paschen curve 2. However, breakdown in some configurations, namely planar electrodes, is not followed by the normal glow regime, but transitions directly into the arc regime where the current spikes to high values 3.
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