首页> 外文会议>24th International Symposium on Discharges and Electrical Insulation in Vacuum >Lighting impulse voltage breakdown characteristics of vacuum interrupters with 10 to 50mm contact gaps
【24h】

Lighting impulse voltage breakdown characteristics of vacuum interrupters with 10 to 50mm contact gaps

机译:接触间隙为10至50mm的真空灭弧室的雷电冲击电压击穿特性

获取原文

摘要

The objective of this paper is to understand the standard lighting impulse voltage breakdown characteristics of vacuum interrupters with contact gaps 10 to 50mm and how contact parameters influence the breakdown characteristics. The investigated contact parameters include contact diameter 75mm and 60mm, contact surface roughness 1.6µm and 3.2µm, and contact radius of curvature 6mm and 2mm. Therefore we designed four high-voltage vacuum interrupters in the experiments. The vacuum interrupters were put into a porcelain envelope with SF6 gas as an external insulation of the vacuum interrupters. The contact gaps can be adjusted manually. Negative polarity basic impulse level (BIL) voltage (1.2×50µs) was applied by an up-and-down method. Experimental results revealed the breakdown probability distribution followed a Weibull distribution when the breakdown voltage saturated in the investigated contact gaps 10 to 50mm. And 50% breakdown voltage U50 depends on the contact gap d (10∼50mm), can be expressed by an equation U50=kdα, where α is a power exponent; k denotes a coefficient which is determined by experiments. Within the contact gaps 10 to 50mm, U50 of vacuum interrupter with contact radius of curvature 2mm was significantly higher than that of vacuum interrupter with contact radius of curvature 6mm. And U50 of contact roughness 1.6µm was close to that of contact roughness 3.2µm. U50 of the contact diameter 60mm was close to that of contact diameter 75mm.
机译:本文的目的是了解接触间隙为10至50mm的真空灭弧室的标准照明脉冲击穿电压击穿特性,以及接触参数如何影响击穿特性。研究的接触参数包括接触直径75mm和60mm,接触表面粗糙度1.6μm和3.2μm以及接触曲率半径6mm和2mm。因此,我们在实验中设计了四个高压真空灭弧室。将真空灭弧室放入装有SF 6 气体的瓷质封套中,作为真空灭弧室的外部绝缘材料。接触间隙可以手动调节。通过上下法施加负极性基本脉冲电平(BIL)电压(1.2×50μs)。实验结果表明,当击穿电压在10至50mm的接触间隙中达到饱和时,击穿概率分布遵循Weibull分布。而50%的击穿电压U 50 取决于接触间隙d(10〜50mm),可以用等式U 50 = kd α,其中α是幂指数; k表示通过实验确定的系数。在接触间隙为10至50mm的范围内,接触点曲率半径为2mm的真空灭弧室的U 50 明显高于接触点曲率半径为6mm的真空灭弧室的U 50 。接触粗糙度1.6μm的U 50 接近接触粗糙度3.2μm的U 50 。接触直径60mm的U 50 接近接触直径75mm的U 50

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号