广东电网公司电力科学研究院,广州,510080
网络首发:2013-06-10,
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柯春俊 1, 潘成 2, 吴锴 2, 等. 人工气隙面积对局部放电特性的影响[J]. 西安交通大学学报, 2013,47(6):103-108.
Effect of Artificial Void Area on Partial Discharge Characters[J]. 2013, 47(6): 103-108.
柯春俊 1, 潘成 2, 吴锴 2, 等. 人工气隙面积对局部放电特性的影响[J]. 西安交通大学学报, 2013,47(6):103-108. DOI: 10.7652/xjtuxb201306018.
Effect of Artificial Void Area on Partial Discharge Characters[J]. 2013, 47(6): 103-108. DOI: 10.7652/xjtuxb201306018.
为了研究局部放电过程中放电面积对放电特性的影响
通过改变气隙面积来改变放电过程中的表面电荷分布
进而研究其对局部放电强度的影响。当气隙尺寸较大时
流注到达界面后可以自由扩展
放电面积变化范围较大导致放电量变化剧烈。气隙直径减小至1.5 mm后
由于放电面积扩展受到限制
放电量变化范围缩小。当气隙面积进一步减小后
放电量均匀程度进一步增加。用铝箔替代聚乙烯覆盖界面
放电面积保持不变
放电量变化范围达到最小。在气隙直径为0.7 mm时
正负半周期各约有一次放电
且正负放电位置重合
这使得前一次放电的放电量对下一次放电的放电相位的影响变得明显。
To investigate the effect of discharge area on discharge characters during partial discharge(PD)process
the variation of surface charge distribution is obtained via changing the void area
and its effect on PD magnitude is analyzed. When void size gets larger
streamer spreads freely after landing on the interface
and the discharge area varies in a wider range to lead to an intense fluctuation of discharge magnitude. Once the void diameter reduces to 1.5 mm
the variation range of discharge magnitude narrows due to the restriction of discharge area developing. As the void area becomes much smaller
the uniformity of discharge magnitude increases. Replacing the PE with aluminum foil to cover the interface
the variation range of discharge magnitude decreases to the minimum. When the void diameter gets to 0.7 mm
only one discharge takes place in each positive and negative half cycle
and the discharge locations coincide with each other
which results in an obvious effect of the magnitude of the former discharge on the phase of the subsequent discharge.
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