The mechanism of the electrical breakdown of air in uniform fields at voltages up to 400 kv

J. Dutton, W. T. Morris
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引用次数: 20

Abstract

Measurements of pre-breakdown ionization currents in uniform fields in dry air at pressures of about 1600 torr were carried out over a range of voltages from 165 kv to over 400 kv, corresponding to a range of values of the parameter p20d (p20 is the pressure reduced to 20°c and d is the electrode separation) from 500 to 12 600 torr cm. Over the whole range investigated the spatial growth of ionization was found to be in accordance with the well-known generalized Townsend equation. Moreover, at a value of p20ds of 12 200 torr cm (ds is the sparking distance), the sparking potential of 408 ± 9 kv predicted by using the Townsend breakdown criterion was in good agreement with the experimentally measured value of 4034 ± 05 kv. In these experiments the gas pressure and electrode separation were chosen so that the maximum value of the field used was less than about 60 kv cm-1. At this value field emission was negligible compared with the externally generated initial current I0 (similar 10-12 A), and values of I0 of this magnitude were shown, experimentally, not to give rise to significant space-charge effects in the measurement of pre-breakdown ionization. The values of the secondary ionization coefficient ω/ά were found to be markedly dependent on the state of the cathode surface showing that, just as at lower pressures and voltages, the cathode plays an important role in the breakdown process. At higher pressures (similar 5000 torr) and higher pre-breakdown fields (similar 100 kv cm-1) field emission currents of about 10-10 A were observed, which can be accounted for on the basis of the Fowler-Nordheim equation modified to take account of the presence of a thin insulating surface film: this work is currently being extended to the investigation of breakdown in these conditions, when space-charge distortion of the applied field due to high field emission from small cathode areas may become important.
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电压达400千伏的均匀电场中空气电击穿的机理
在干燥空气中的均匀场中,在约1600 torr的压力下,在165 kv到400 kv以上的电压范围内进行了预击穿电离电流的测量,对应于参数p20d (p20是压力降低到20°c, d是电极分离)的值范围从500到12 600 torr cm。在整个研究范围内,发现电离的空间增长符合著名的广义汤森方程。在p20ds为12 200 torr cm (ds为火花距离)时,利用Townsend击穿判据预测的火花电位为408±9 kv,与实验实测值4034±05 kv吻合较好。在这些实验中,气体压力和电极分离的选择使所使用的电场最大值小于约60 kv cm-1。在此值下,与外部产生的初始电流I0(类似于10-12 A)相比,场发射可以忽略不计,并且在实验中表明,该量级的I0值在测量击穿前电离时不会产生明显的空间电荷效应。二次电离系数ω/ α的值明显依赖于阴极表面的状态,这表明,正如在较低的压力和电压下,阴极在击穿过程中起着重要作用。在较高的压力(类似于5000 torr)和较高的预击穿场(类似于100 kv cm-1)下,观察到场发射电流约为10-10 A,这可以根据Fowler-Nordheim方程来解释,该方程经过修改,考虑了薄绝缘表面膜的存在:这项工作目前正在扩展到这些条件下的击穿研究,当小阴极区域的高场发射引起的应用场的空间电荷畸变可能变得重要时。
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