Ramp test technique for D.C. partial discharge

R. Bever, J. Westrom
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引用次数: 1

Abstract

There is a relatively little published work [1,2,3,4] on dc partial discharge (P.D.) measurements on practical insulation systems. Compared to the much used technique of ac testing, the number of P.D. pulses are very few, even considerably above inception voltage. The dc inception voltage itself is difficult to determine, consisting of only a very few pulses/minute, and it will only be correct for a fresh, completely discharged dielectric specimen, into which space charge has not yet been injected. For dc partial discharge the quantity φ/ε is the cogent material property factor where φ is the conductivity and ε is the permittivity of the dielectric containing the voids or grain boundaries. This factor represents the inverse of the time constant for charge distribution due to dielectric conductivity [3].
直流局部放电的斜坡试验技术
关于实际绝缘系统的直流局部放电(P.D.)测量,发表的工作相对较少[1,2,3,4]。与常用的交流测试技术相比,脉冲脉冲的数量非常少,甚至大大高于初始电压。直流起始电压本身很难确定,因为每分钟只有很少的脉冲,而且它只对一个新鲜的、完全放电的电介质样品是正确的,其中空间电荷尚未注入。对于直流局部放电,量φ/ε为材料性能因子,其中φ为电导率,ε为含孔洞或晶界的介质的介电常数。该因子表示介电电导率引起的电荷分布的时间常数的倒数[3]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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