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首页> 外文期刊>Dielectrics and Electrical Insulation, IEEE Transactions on >Surface charge accumulation and partial discharge activity for small gaps of electrode/epoxy interface in sf6 gas
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Surface charge accumulation and partial discharge activity for small gaps of electrode/epoxy interface in sf6 gas

机译:SF6气体中电极/环氧树脂界面的小间隙的表面电荷积累和局部放电活性

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摘要

The electrical insulation reliability of solid spacers in Gas Insulated Switchgears (GISs) is an important issue to achieve a safe operation of such equipment. Among different phenomena, charge accumulation represents the most important matter that can degrade the overall performance of these insulation systems. For this respect, this paper discusses the contribution of partial discharge (PD) activity by ac voltage application to charge accumulation in the small gap at the electrode/epoxy interface as one of the weakest points in GIS solid spacers. The partial discharge inception voltages for non-accumulated charge case (PDIV0) and after exposing to PD activity (PDIVn) are measured among different gap lengths, simulating delamination at the electrode/epoxy interface. The PD activity is generated using applied voltage with 1.2×PDIV0 for all gap lengths examined in this study (50~500 ;C;m). In these measurements, PDIV increased with increasing the number of PD pulses as a result of accumulated charges. The accumulated surface charge density is estimated using the boundary equations and is compared for the different gap lengths. The accumulated charge density was larger for the smaller gap lengths. Comparing PD parameters with accumulated charge density enabled us to identify that the number of negative and positive PD pulses is the main parameter that corresponds to charge accumulation process.
机译:气体绝缘开关设备(GISs)中固体垫片的电绝缘可靠性是实现此类设备安全运行的重要问题。在不同现象中,电荷积累是最重要的问题,它可能会使这些绝缘系统的整体性能下降。为此,本文讨论了通过施加交流电压产生的局部放电(PD)活性对电极/环氧树脂界面小间隙中电荷积累的贡献,这是GIS固体垫片中最弱的点之一。在不同间隙长度之间测量非累积电荷情况下的局部放电起始电压(PDIV0)和暴露于PD活性后的局部放电起始电压(PDIVn),以模拟电极/环氧树脂界面处的分层。 PD活性是通过在本研究中检查的所有间隙长度(50〜500; C; m)使用外加电压为1.2×PDIV0的电压产生的。在这些测量中,由于累积电荷,PDIV随着PD脉冲数的增加而增加。使用边界方程估算累积的表面电荷密度,并比较不同的间隙长度。对于较小的间隙长度,累积的电荷密度较大。将PD参数与累积电荷密度进行比较,使我们能够确定负PD脉冲数和正PD脉冲数是与电荷累积过程相对应的主要参数。

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