首页> 外文会议>2012 IEEE International Conference on Condition Monitoring and Diagnosis. >The effect of needle curvature and aluminum foil on the transition of discharge mechanism under needle-plate configuration
【24h】

The effect of needle curvature and aluminum foil on the transition of discharge mechanism under needle-plate configuration

机译:针板配置下针曲率和铝箔对放电机理转变的影响

获取原文
获取原文并翻译 | 示例

摘要

The measurement system detecting ns discharge current pulse during partial discharge (PD) was constructed to study the effect of the variation of needle curvature and aluminum foil diameter on the discharge parameters. Five types of needle electrode (with the curvature radius of 0.19 mm, 0.40 mm, 0.59 mm, 0.78 mm, 0.98 mm, 1.45 mm) and three types of round aluminum (with the diameter of 5 mm, 8 mm, 12 mm) were employed in our paper. As the area of aluminum foil increased, the peak value and rise part of current pulse increased and the falling part and pulse width decreased. However, the abnormal phenomenon for negative discharge that minimum rise part appeared with relatively small diameter of aluminum foil (5 mm). When no aluminum foil covered the dielectric surface, the peak value of positive discharge current was larger than that of negative one, its slew and falling part were smaller. These could be explained well by the streamer theory. When the aluminum foil covered the dielectric surface, the similar differences between positive discharge and negative one were obtained when the curvature radius was smaller (0.19 mm). However, as curvature radius increased (≥0.98 mm), the distinct result that pulse width of negative discharge was smaller and its current peak value was larger compared with positive discharge. This is explained in terms of the different speed of avalanche development of positive and negative pulses.
机译:构建了局部放电(PD)时检测ns放电电流脉冲的测量系统,以研究针曲率和铝箔直径的变化对放电参数的影响。五种类型的针状电极(曲率半径分别为0.19 mm,0.40 mm,0.59 mm,0.78 mm,0.98 mm,1.45 mm)和三种类型的圆形铝(直径分别为5 mm,8 mm,12 mm)在我们的论文中使用。随着铝箔面积的增加,电流脉冲的峰值和上升部分增大,而下降部分和脉冲宽度减小。但是,铝箔的直径相对较小(5mm)时,出现最小上升部分的负放电异常现象。当没有铝箔覆盖电介质表面时,正放电电流的峰值大于负放电电流的峰值,其斜率和下降部分较小。这些可以用流光理论很好地解释。当铝箔覆盖电介质表面时,曲率半径较小(0.19 mm)时,在正放电和负放电之间将获得相似的差异。但是,随着曲率半径的增加(≥0.98mm),与正放电相比,负放电的脉冲宽度更小并且其电流峰值更大。用正脉冲和负脉冲的雪崩发展的不同速度来解释这一点。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号