Surface Breakdown and Surface Discharge Characteristics of Ethylene Propylene Rubber Insulation
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Surface Breakdown and Surface Discharge Characteristics of Ethylene Propylene Rubber Insulation
Vol. 42, Issue 12, Pages: 3924-3933(2016)
作者机构:
太原理工大学煤矿电气设备与智能控制山西省重点实验室
作者简介:
基金信息:
DOI:
CLC:
Published Online:31 December 2016,
Published:2016
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LEI Zhipeng, FENG Chen, SONG Jiancheng, et al. Surface Breakdown and Surface Discharge Characteristics of Ethylene Propylene Rubber Insulation[J]. 2016, 42(12): 3924-3933.
DOI:
LEI Zhipeng, FENG Chen, SONG Jiancheng, et al. Surface Breakdown and Surface Discharge Characteristics of Ethylene Propylene Rubber Insulation[J]. 2016, 42(12): 3924-3933.DOI:
Surface Breakdown and Surface Discharge Characteristics of Ethylene Propylene Rubber Insulation
It is important to understand the surface breakdown characteristics and the surface discharge behavior of ethylene propylene rubber(EPR) insulation material. For this purpose
three different electrode structures
namely
plane to plane electrode
rod to ring electrode
and needle to plane electrode
have been chosen to simulate different electric field distribution. During the experiment
surface breakdown voltage and breakdown tracking under three different electrode structures
by which AC voltage and negative polarity DC voltage are applied
respectively
are measured and analyzed. Then
the discharge patterns of surface discharge under different AC voltage levels are measured
and inception and development processes of surface discharge are also analyzed. The experimental results show that the increase of surface discharge voltage magnitude becomes higher when the electric field distribution is more uniform. Under plane to plane electrode
the inception discharge voltage depends on the gap distance of two electrodes. Moreover
under rod to ring electrode and needle to plane electrode
the inception discharge voltage magnitude is closely related to the inception voltage magnitudeof corona
ranging from 1.9 k V to 2.4 k V. The discharge type and discharge pattern are also different under different electric field distribution and discharge stages. The magnitude of discharge pules is small at the beginning of the surface discharge
about 1.2 V. When the flashover occurs
the discharge distribution is more scattered
and the magnitude of discharge pulses rises to about 43 V. From the above mentioned
the severity degree of surface discharge development can be discriminated.