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Mechanism of impulse voltage breakdown in high voltage vacuum interrupters with long contact gap

机译:接触间隙长的高压真空灭弧室的脉冲电压击穿机理

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The objective of this paper is to propose a breakdown mechanism of lightning impulse voltage in high voltage vacuum interrupters (VIs) with long contact gap by complementing the Cranberg "clump" hypothesis with an impulse voltage and a non-uniform field. The Cranberg "clump" hypothesis assumed that the vacuum breakdown was due to the loosely adhering microscopic particles under a DC voltage and a uniform field. The microscopic particles might be torn from an electrode surface at a critical voltage. We considered the microscopic particles located at the area with the maximum electric field had the highest possibility to be accelerated. Therefore, the transit process of the micro-particles to the opposing electrodes was under a non-uniform field distribution driven by an impulse voltage. The rise rate of the impulse voltage applied was also considered. As a result, it was found that the breakdown voltage of a vacuum gap depends upon a 0.76 power of the gap length for the plate-to-plate contacts. The diameter of the contacts was 60 mm. The contact radius of curvature was 6 mm. In the same conditions, our previous experimental results showed that the impulse breakdown voltage was in a range of 0.70 to 0.79 power of the contact gap. So the experimental results supported the Cranberg hypothesis in its extension to the impulse breakdown under non-uniform field in high-voltage VIs. Thereafter, this proposed breakdown mechanism is a complement to the Cranberg "clump" hypothesis in terms of impulse voltage breakdown under a non-uniform field in high voltage VIs.
机译:本文的目的是通过用脉冲电压和非均匀电场对Cranberg“团块”假设进行补充,提出具有长接触间隙的高压真空灭弧室(VI)的雷电冲击电压的击穿机理。 Cranberg“团块”假说假设真空破坏是由于在直流电压和均匀电场下松散粘附的微观颗粒引起的。微观粒子可能会在临界电压下从电极表面撕下。我们认为位于最大电场区域的微观粒子被加速的可能性最高。因此,微粒向相对电极的迁移过程处于由脉冲电压驱动的非均匀场分布下。还考虑了施加的脉冲电压的上升速率。结果发现,真空间隙的击穿电压取决于板对板接触的间隙长度的0.76次方。触点的直径为60毫米。接触曲率半径为6mm。在相同条件下,我们先前的实验结果表明,脉冲击穿电压在接触间隙功率的0.70至0.79的范围内。因此,实验结果支持Cranberg假设,将其扩展到高压VI中非均匀电场下的脉冲击穿。此后,就高压VI中非均匀场下的脉冲电压击穿而言,这种击穿机制是对Cranberg“团块”假设的补充。

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