第一章

M. Lomaev, D. Rybka, V. Tarasenko
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引用次数: 0

摘要

本章介绍了在时间分辨率为100 ps的记录系统下,在非均匀电场中扩散(体积)纳秒级高压放电的实验研究结果。结果表明,在电压脉冲持续时间减小的情况下,获得无附加电离源的扩散放电的条件得到了扩展;具体而言,在常压空气和其他气体中,在短电极间隙内实现了失控电子预电离扩散放电(REP DD)。研究发现,在间隙处达到最大电压后,主要能量沉积到REP DD等离子体中。在脉冲重复率高达1khz和高压下,在氮气、空气和氩气中研究了REP DD。在产生失控电子束和x射线的条件下,CCD相机记录了漫射放电形成的时间及其过渡到火花放电之前的持续时间。在氮气、空气和氩气中,扩散放电在不超过1ns的时间内形成。在不超过1ns的时间内,在氩气和空气中阴极上出现亮点,导致火花通道开始传播。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Chapter 1
This chapter presents the results of experimental investigations of diffuse (volume) nanosecond elevated-pressure discharges in a non-uniform electric field at a time resolution of a recording system being equal to 100 ps. It is shown that conditions of obtaining a diffuse discharge without a source of additional ionization are extended at the voltage pulse duration reduction; specifically, a runaway electron preionized diffuse discharge (REP DD) was realized in atmospheric pressure air and other gases at a short interelectrode gap. It was found that the main energy deposition into the REP DD plasma occurred after attaining maximal voltage at a gap. At pulse repetition rate up to 1 kHz and elevated pressures the REP DD has been studied in nitrogen, air, and argon. In the conditions of generation of runaway electron beams and X-rays, a CCD camera recorded the time of the diffuse discharge formation and its duration prior to its transition to a spark one. In nitrogen, air, and argon the diffuse discharge was formed during the time not exceeding 1 ns. During the time not exceeding 1 ns the bright spots appear on cathode in argon and air resulting in the beginning of the spark channel propagation.
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