快速真空断路器开断短路电流电弧演化特性研究

Jianhua Wang, Chen Guan, Bojian Zhang, X. Yao, Zhiyuan Liu, Yingsan Geng
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摘要

摘要快速真空断路器(FVCB)采用电磁斥力驱动,具有极短的开断时间,与控制开关技术配合使用,能以最短的电弧时间开断短路电流。本文的目的是确定具有最小电弧时间的快速真空断路器的电弧演变行为。采用40.5 kV真空灭弧(VI),配置一对CuCr50 (cr50 wt%)轴向磁场(AMF)触头。接触面直径分别为Φ50mm、Φ58和Φ65 mm。用高速摄像机通过VI的玻璃包膜拍摄了拉弧实验中的电弧演化行为。实验结果表明,在一定开弧速度下,当拉弧时间大于临界弧扩散时间时,初始的强弧趋于扩散弧。真空电弧的临界电弧扩散时间定义为电弧从接触分离瞬间发展到出现分离的阴极点。对于Φ50 mm杯型AMF触点,随着打开速度从2.52 m/s增加到4.65 m/s,临界电弧扩散时间从0.7 ms减少到0.46 ms。当打开速度从2.52 m/s增加到4.65 m/s时,Φ58 mm杯型AMF触点的临界电弧扩散时间从1.0 ms减少到0.58 ms。对于Φ65 mm杯型AMF触点,随着打开速度从2.52 m/s增加到4.65 m/s,临界电弧扩散时间从1.30 ms减少到0.64 ms。在相同开启速度下,临界电弧扩散时间随触点直径的增大而增大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Study on Arc Evolution Behaviour of Breaking Short Circuit Current for a Fast Vacuum Circuit Breaker
Abstract A fast vacuum circuit breaker (FVCB), driven by an electromagnetic repulsion mechanism, has an extremely short opening time, and in coordination with the controlled switching technology contributes to breaking a short circuit current with the minimum arcing time. The objective of the paper is to determine the arc evolution behaviour of fast vacuum circuit breakers with a minimum arcing time. A 40.5 kV vacuum interrupter (VI) was used, which was equipped with a pair of CuCr50 (Cr 50 wt%) axial magnetic field (AMF) contacts. The diameters of the contact were Φ50mm, Φ58 mm and Φ65 mm respectively. The arc evolution behaviour in the drawn arc experiment was photographed by a high-speed camera through a glass envelope of the VI. The experiment results showed that an initial intense arc tended to evolve into a diffuse arc when the arcing time is larger than a critical arc diffusion time under a certain opening velocity. The critical arc diffusion time for the vacuum arc is defined as arc evolving from the instant of contact separation to an appearance of separated cathode spots. For a Φ50 mm cup-type AMF contact, the critical arc diffusion time decreases from 0.7 ms to 0.46 ms, with the increase of the opening velocity from 2.52 m/s to 4.65 m/s. What’s more, for a Φ58 mm cup-type AMF contact, the critical arc diffusion time decreases from 1.0 ms to 0.58 ms with the increase of the opening velocity from 2.52 m/s to 4.65 m/s. For a Φ65 mm cup-type AMF contact, the critical arc diffusion time decreases from 1.30 ms to 0.64 ms with the increase of the opening velocity from 2.52 m/s to 4.65 m/s. The critical arc diffusion time increases with the increase of the diameter of the contact under the same opening velocity.
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