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Nanosecond pulse discharges in C3F8‐Ar mixtures

机译:C3F8连字符;氩混合物中的纳秒脉冲放电

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摘要

In this paper we present results from experiments to determine the behavior of C3F8‐Ar mixtures as filling gases in a uniform‐field spark gap subjected to high voltage, nanosecond pulses. The gas pressure ranges from 500 to 960 Torr and the overvoltage ranges from 50 to 300. The electrode separation is 1 cm.U‐Virradiation has been used prior to the arrival of the pulse to the gap. In general, the discharge consists of very large numbers of closely packed filaments with the overall diameter being less than or equal to approximately 1 cm. The initial rate of current rise at the load is large (∼1012A/sec). Subsequently, a phase of relatively constant current is observed the length of which changes with the concentration of C3F8. This phase has large resistance and the energy deposited into the discharge ranges from 6 to 20 of the energy in the incident pulse, as the concentration of C3F8increased from 30 to 100. The final state of conduction of the discharge is an arc. In light of these observations, the behavior of self‐ and nonself‐sustained discharges is discussed.
机译:在本文中,我们介绍了实验结果,以确定C3F8&连字符;Ar混合物在均匀的&连字符;场火花隙中填充气体的行为,并受到高压,纳秒脉冲的影响。气体压力范围为 500 至 960 Torr,过电压范围为 50 至 300 Percnt;。电极间隔为1厘米。通常,放电由大量紧密堆积的细丝组成,总直径小于或等于约 1 厘米。负载处的初始电流上升速率很大(∼1012A/秒)。随后,观察到一个相对恒定的电流相,其长度随C3F8的浓度而变化。该相具有较大的电阻,沉积到放电中的能量范围为入射脉冲中能量的6%至20%;,因为C3F8的浓度从30%增加到100%。放电的最终传导状态是电弧。根据这些观察结果,讨论了自我连字符和非自我持续放电的行为。

著录项

  • 来源
    《journal of applied physics》 |1984年第5期|1391-1397|共页
  • 作者

    E. E. Kunhardt; M. G. White;

  • 作者单位
  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 英语
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