交直流叠加电压下环氧树脂膜局部放电感应电流的特性

Tianxin Zhuang, Xuze Gao, M. Ren, Siyun Wang, Junkai Huang
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引用次数: 0

摘要

电力电子设备和换流站设备的绝缘经常处于交直流叠加电压下。了解交直流联合励磁下的局部放电特性对电力电子器件的绝缘设计具有重要意义。以往的研究主要集中在交流或直流电压下的随机特性和机制,而对交直流叠加电场下pd诱导电荷运动的研究较少。电荷运动包括局部放电的瞬态行为和缓慢运动,可以分别用局部放电的瞬态电流和过量电流来表征。本文将交直流复合电压施加于一对夹在环氧膜上的电极上。采用灵敏高频Rogowski线圈和容电阻并联阻抗同时测量瞬态放电电流和放电过程中的过量电流。通过从总电流中减去容性电流,可以测量出多余的电流。测量时,先将交流电压设为交流PDIV的1.5倍,然后逐渐升高直流电压。结果表明,随着直流偏置的增大,局部放电事件的相位分布扩大,但平均局部放电电流和过量电流均低于纯交流电场下的平均局部放电电流和过量电流。当直流电压上升到接近交流电压峰值时,只观察到很少的局部放电事件,当直流电压上升到交流电压峰值以上时,表面闪络开始发生。实验证明,附加的直流电压在一定程度上抑制了交流电压激发的电晕放电,但如果直流偏置超过交流幅值,也可能导致表面闪络。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Characteristics of the Partial Discharge-induced Current along Epoxy resin film under Superimposed AC- DC Voltage
Insulation of power electronic devices and converter station equipment is often under superimposed AC-DC voltage. The understanding of PD characteristics under AC-DC combined excitation plays an important role in designing the insulation of power electronic device. Previous researches focused on the stochastic features and mechanism under AC or DC voltages, while little attention was paid to the PD-induced charge movements under superimposed AC-DC field. The charge movements include the transient behavior of PD and the slow movement, which can be characterized by the transient PD current and the excess current respectively. In this paper, a composite AC-DC voltage is applied to a pair of rod-plane electrodes sandwiching epoxy film. And a sensitive high-frequency Rogowski coil and a capacitor-resistor shunt impedance are used to simultaneously measure the transient PD current and the excess current during PD. The excess current can be measured by cancelling the capacitive current from the total current. In the measurement, first set the AC voltage at 1.5 times the AC PDIV, then gradually raise the DC voltage up. The results show that, as the DC bias increases, the phase distributions of PD events are expanded, but the average PD currents and excess currents are lower than that under the pure AC electric field. Moreover, only few PD events are observed when the DC voltage rises close to the peak of AC voltage, and the surface flashover starts once the DC voltage rises above the peak of AC voltage. It is proved that the additional DC voltage suppress the corona discharge excited by the AC voltage to a certain extent, but it may also result in surface flashover if the DC bias exceeds the AC amplitude.
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