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The breakdown voltage and discharge extension of long gaps in nitrogen‐SF6 and air‐SF6 gas mixtures

机译:氮气-SF6和空气-SF6混合气中的长间隙的击穿电压和放电扩展

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The breakdown voltage and the extension of the discharge has been investigated for impulse voltages with rod‐plane gaps of 30 and 50 cm in nitrogen‐SF6 and air‐SF6 mixtures at atmospheric pressure. The addition of 0.4–2% SF6 by volume to nitrogen reduced the 50% breakdown voltage V50 for both polarity impulse voltages below the value for pure nitrogen or pure SF6, typically 50% below the pure SF6 level. However, in air‐SF6 mixtures the opposite effect was found, and a small addition of SF6 (e.g., 1%) increased V50 by typically 80% above that for pure SF6. The extension of the breakdown path has been studied with an image converter and still cameras. In nitrogen‐SF6 mixtures there was a rapid extension of the discharge corresponding to the condition of the minimum breakdown voltage with the 2% SF6 content. The typical discharge extension characteristic in both types of mixtures was an intermittent propagation of the leader accompanied by ball‐like regions of corona streamers at the leader tip. For a 50% SF6–nitrogen mixture, typical pause times between the steps were 1 μsec for negative polarity and 0.08 μsec for positive polarity, and the discharge extension to breakdown was two to three times faster for positive impulses.
机译:对于在大气压下在氮气-SF6和空气-SF6混合物中杆面间隙为30和50 cm的脉冲电压,已经研究了击穿电压和放电范围。向氮气中添加按体积计0.4–2%的SF6,使两种极性脉冲电压的50%击穿电压V50均低于纯氮或纯SF6的值,通常低于纯SF6的水平50%。但是,在空气-SF6混合物中却发现了相反的效果,少量添加SF6(例如1%)会使V50通常比纯SF6升高80%。已经使用图像转换器和静态相机研究了故障路径的扩展。在氮气-SF6混合物中,放电迅速扩展,其对应的最低击穿电压为SF6含量为2%。两种类型的混合物中典型的放电扩展特性是引导线间歇性传播,并在引导线尖端出现电晕带的球形区域。对于50%的SF6-氮气混合物,步骤之间的典型暂停时间对于负极性为1微秒,对于正极性为0.08微秒,对于正脉冲,击穿放电的扩展时间要快两到三倍。

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    《Journal of Applied Physics》 |1977年第8期|P.3281-3287|共7页
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  • 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);
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