潘飞, 赵文彬, 毕建刚, 颜湘莲, 李峰, 贾成龙. 交流作用下稍不均匀场中SF6间隙的绝缘恢复特性[J]. 高电压技术, 2025, 51(5): 2550-2560. DOI: 10.13336/j.1003-6520.hve.20240061
引用本文: 潘飞, 赵文彬, 毕建刚, 颜湘莲, 李峰, 贾成龙. 交流作用下稍不均匀场中SF6间隙的绝缘恢复特性[J]. 高电压技术, 2025, 51(5): 2550-2560. DOI: 10.13336/j.1003-6520.hve.20240061
PAN Fei, ZHAO Wenbin, BI Jiangang, YAN Xianglian, LI Feng, JIA Chenglong. Insulation Recovery Characteristics of SF6 Gaps in Slightly Inhomogeneous Fields Under AC Action[J]. High Voltage Engineering, 2025, 51(5): 2550-2560. DOI: 10.13336/j.1003-6520.hve.20240061
Citation: PAN Fei, ZHAO Wenbin, BI Jiangang, YAN Xianglian, LI Feng, JIA Chenglong. Insulation Recovery Characteristics of SF6 Gaps in Slightly Inhomogeneous Fields Under AC Action[J]. High Voltage Engineering, 2025, 51(5): 2550-2560. DOI: 10.13336/j.1003-6520.hve.20240061

交流作用下稍不均匀场中SF6间隙的绝缘恢复特性

Insulation Recovery Characteristics of SF6 Gaps in Slightly Inhomogeneous Fields Under AC Action

  • 摘要: SF6的绝缘恢复特性对气体绝缘组合设备(gas insulator switchgear, GIS)的稳定运行有着重要作用,但目前SF6相关的击穿试验缺乏对绝缘恢复过程的研究。为此利用能够表征流场结构的纹影技术,搭建了研究GIS气室中棒—板间隙击穿后绝缘恢复过程的纹影观测平台,获得了绝缘恢复过程的纹影图像,基于流场中脉动分析的方法定义了纹影图像的波动值,得到了多时间段纹影图像的波动分布图,分析了不同区域的绝缘恢复演化差异,并利用波动值的离散系数定量表征绝缘恢复程度,获取了绝缘恢复的时空规律,最后统计了绝缘恢复时间。试验结果表明:通道击穿后的气流团运动由于工频残压的影响存在扩散和消散两个阶段;绝缘恢复过程中通道内的形态变化存在较大差异,主要体现在板电极上半部分与其它区域的演化差异;通道内不同区域存在绝缘恢复程度的差异,棒电极附近的绝缘恢复较慢;0.2 MPa下的SF6绝缘恢复时间比0.3 MPa下的短但差异不大,气压不是影响绝缘恢复的决定条件。该试验方法和分析结果为稍不均匀场中SF6击穿后的绝缘恢复过程研究提供了参考。

     

    Abstract: The insulation recovery characteristics of SF6 play an important role in the stable operation of GIS, whereas the current SF6-related breakdown test lacks the study of the insulation recovery process. In this paper, we use the rippling technique that can characterize the flow field structure to build a rippling observation platform to study the insulation recovery process after the breakdown of the bar-plate gap in the GIS gas chamber, obtain the rippling image of the insulation recovery process, and define the fluctuation value of the rippling image based on the method of pulsation analysis in the flow field; moreover we obtain the fluctuation map of the rippling image in multiple time intervals, analyze the difference of the evolution of insulation recovery in different areas, and use the discrete coefficient of the fluctuation value to quantify the fluctuation value. The discrete coefficient of the fluctuation value is used to quantitatively characterize the degree of insulation recovery, the temporal and spatial laws of insulation recovery are obtained, and finally the insulation recovery time is counted. The experimental results show that there are two stages of development and dissipation of the air flow mass movement after the channel breakdown due to the influence of the industrial frequency residual pressure. There are large differences in the morphological changes in the channel during the insulation recovery process, which are reflected in the evolutionary differences between the upper part of the plate electrode and other regions. There are differences in the degree of insulation recovery in different regions of the channel, and the insulation recovery near the rod electrode is slower. The insulation recovery time for the SF6 insulation at 2 atmospheres is much longer than that at 3 atmospheres. SF6 insulation recovery time at 2 atmospheres is shorter than that at 3 atmospheres but the difference is not significant, and the air pressure is not a decisive condition affecting insulation recovery. The experimental method and analytical results in this paper provide a reference for the study of insulation recovery process after SF6 breakdown in slightly inhomogeneous field.

     

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