Fundamental characteristics of arc extinction by magnetic blow-out at DC voltages (<500V) II

K. Sawa, Shigeru Tsujimura, S. Motoda
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引用次数: 9

Abstract

As various DC power supply systems such as photovoltaic power generation, fuel cell and others have become gradually popular, DC current interruption is one of the key technologies for reliability and safety of DC switching devices. In a previous paper a model switch is developed with magnetic blow-out of three levels, and gap length and arc length at arc extinction are obtained by a high-speed camera in range of current less than 4 A and voltage lower than 500V. The gap length and arc length at extinction are much shorter than those without magnetic blow-out.In this paper the interrupted current is expanded to 30A and source voltage is 100, 300 and 500V. The results are compared with previous ones and the followings can be made clear. The gap width at arc extinction is almost independent of interrupted current and source voltage. Those gap width is 0.8, 0.3 and 0.2 mm for magnetic flux densities 19, 53 and 157mT, respectively, and in accordance with the previous values. On the other hand, the arc length becomes longer with interrupted current / source voltage. The maximum length reaches about 60 mm at 500V and 30A for19mT. In addition the change of arc length with time is discussed and the process is found to consist of slow rising and rapid rising intervals.
直流电压(<500V)下磁灭弧的基本特性ⅱ
随着光伏发电、燃料电池等各种直流供电系统的逐步普及,直流电流中断是保证直流开关器件可靠性和安全性的关键技术之一。在前人的研究中,研制了一种三电平磁灭开关模型,在电流小于4 a,电压小于500V的范围内,利用高速摄像机获得了灭弧时的间隙长度和弧长。灭弧时的间隙长度和弧长比无磁灭弧时短得多。本文将中断电流扩展到30A,源电压分别为100v、300v和500V。将所得结果与以往的结果进行比较,可以得出以下结论:消弧处的间隙宽度几乎与中断电流和源电压无关。磁通密度为19、53和157mT时,间隙宽度分别为0.8、0.3和0.2 mm,与前面的值一致。另一方面,弧长随着断流/源电压的增大而增大。在500V, 30A, 19mt时,最大长度约为60mm。讨论了弧长随时间的变化规律,发现电弧弧长可分为慢升段和快升段。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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