窄间隙击穿电压特性

S. Hong
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引用次数: 1

摘要

在常温和均匀场条件下,大多数气体在压力达到几个大气压时的静态击穿符合帕申定律。然而,在非常小的间距或高压的情况下,会观察到与Paschen定律的偏离。研究表明,这种偏差与高电场有关,通常大于105v /cm。1,2对于2 - 3 mil的间隙,静电击穿时的电场强度接近105v /cm。在冲击浪涌条件下,电压上升速率≥100 V/μs,电场强度可以更高。在接下来的章节中,将描述在窄间隙(0.8 ~ 6 mils)内测量不同电压上升速率(600 V/S和100 V/μS)下击穿电压的实验安排。在室温下,在压力从400到1000托的气体中进行了碳涂层铜电极的研究。将介绍氩气、氩氖混合物、氖气、氮气和空气的数据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Breakdown voltage characteristics in a narrow gap
Static breakdown in most gases is in accordance with the Paschen's law for pressures up to a few atmospheres, at normal temperatures and uniform-field. However, departures from Paschen's law are observed notably for very small spacing or high pressure. Studies have indicated that the deviation is associated with high electric field, usually greater than 105 V/cm.1,2 For gaps of 2–3 mils, the electric field strength at static breakdown is close to 105 V/cm. Under impulse surge conditions, voltage rise rates of ≥ 100 V/μs, the electric field strength can be higher. In the following sections, an experimental arrangement to measure breakdown voltage at different rates of voltage rise (600 V/S and 100 V/μS) in a narrow gap (0.8 to 6 mils) will be described. Studies were made with carbon coated copper electrodes in a gas at pressures from 400 to 1000 torr at room temperature. Data will be presented for argon, argon-neon mixtures, neon, nitrogen and air.
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