齐波, 高春嘉, 邢照亮, 陈铮铮, 赵健康, 李成榕. 直流/交流电压下GIS绝缘子表面电荷分布特性[J]. 中国电机工程学报, 2016, 36(21): 5990-6001,6044. DOI: 10.13334/j.0258-8013.pcsee.151934
引用本文: 齐波, 高春嘉, 邢照亮, 陈铮铮, 赵健康, 李成榕. 直流/交流电压下GIS绝缘子表面电荷分布特性[J]. 中国电机工程学报, 2016, 36(21): 5990-6001,6044. DOI: 10.13334/j.0258-8013.pcsee.151934
QI Bo, GAO Chun-jia, XING Zhao-liang, CHEN Zheng-zheng, ZHAO Jian-kang, LI Cheng-rong. Distribution Characteristic for Surface Charge on GIS Insulator Under DC/AC Voltage[J]. Proceedings of the CSEE, 2016, 36(21): 5990-6001,6044. DOI: 10.13334/j.0258-8013.pcsee.151934
Citation: QI Bo, GAO Chun-jia, XING Zhao-liang, CHEN Zheng-zheng, ZHAO Jian-kang, LI Cheng-rong. Distribution Characteristic for Surface Charge on GIS Insulator Under DC/AC Voltage[J]. Proceedings of the CSEE, 2016, 36(21): 5990-6001,6044. DOI: 10.13334/j.0258-8013.pcsee.151934

直流/交流电压下GIS绝缘子表面电荷分布特性

Distribution Characteristic for Surface Charge on GIS Insulator Under DC/AC Voltage

  • 摘要: 为了研究GIS绝缘子在交流电压和直流作用下的表面电荷分布特性,针对实际220 k V GIS盆式绝缘子研制了高分辨率的表面电荷三维测量装置,可以实现绝缘子表面电荷全径向、全圆周的扫描测量,通过实测获得了直流电压和交流电压作用下GIS绝缘子表面电荷的分布特性。研究结果表明:1)直流电压作用下绝缘子表面电荷积聚呈现明显的极性效应:正极性电压下绝缘子表面主要积聚正极性电荷,负极性电压作用下只积聚负极性电荷;无论绝缘子表面积累电荷的极性如何,其密度随着电压幅值的增大而逐渐增多,并且随电压作用时间的增加逐渐增长并趋于饱和。2)在交流电压作用下绝缘子也存在表面电荷积聚的现象,但电荷密度明显小于直流电压作用下的电荷密度;随着电压幅值的增加,电荷密度先升高再减小并趋于稳定。因此,由表面电荷引起的实际设备中的绝缘问题需引起足够重视,该文所得到的直流/交流电压下GIS绝缘子表面电荷分布特性,可为GIS/GIL设备绝缘子的设计优化提供参考。

     

    Abstract: Gas insulated switchgear(GIS) equipment is subject to surface charge accumulation under DC or AC voltages in real operation, which could distort the electric field and incur flashover eventually. With the 3D high-resolution surface charge measurement system established on the actual 220 k V GIS basin insulator, the present research captured the surface charge distribution characteristics of the insulator under DC and AC voltage with high precision by the probe scanning on the insulator surface. The experiment results show that: 1) Surface charge demonstrated obvious polarity effect under DC voltage. Under positive DC voltage, there accumulated mainly positive surface charges, while under negative one, the polarity of accumulated surface charge was all negative. Whatever the polarity of accumulated surface charge is, as the amplitude of applied voltage increased, the amount of accumulated surface charges mounted up and with the voltage application prolonging, the average value of surface charges kept increasing until it reached saturation. 2) Accumulated in the context of AC voltage were mainly negative surface charges with less density compared to the DC scenario. As the amplitude of applied AC voltage grew, the amount of accumulated homogeneous surface charges firstly increased, then decreased, and finally reached saturation. Above all, the insulating issues occurred by the surface charge accumulation require due attention in the application and maintenance of GIS equipment, and the research in this paper can provide a reference for the optimal design of GIS/GIL insulators.

     

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