1996
DOI: 10.1541/ieejpes1990.116.4_482
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Impulse Creeping Discharge Phenomena on Aerial Insulated Wire under Dry and Wet Conditions

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Cited by 16 publications
(26 citation statements)
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“…In the case of T f = 1.2 µs, there exist two regions where the length of discharges increases and decreases at V m ≤ 50 kV and V m > 50 kV, respectively. This phenomenon was described in detail in our previous paper [8]. On the other hand, for T f = 2.0 to 6.0 µs, the lengths in the range V m ≤ 70 kV increased with increasing V m in almost the same manner, but at V m > 70 kV, the lengths decreased for T f = 2.0 and 4.0 µs, and increased for T f = 6.0 µs.…”
Section: Relationship Between Peak Value Of Applied Impulse Voltage Asupporting
confidence: 67%
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“…In the case of T f = 1.2 µs, there exist two regions where the length of discharges increases and decreases at V m ≤ 50 kV and V m > 50 kV, respectively. This phenomenon was described in detail in our previous paper [8]. On the other hand, for T f = 2.0 to 6.0 µs, the lengths in the range V m ≤ 70 kV increased with increasing V m in almost the same manner, but at V m > 70 kV, the lengths decreased for T f = 2.0 and 4.0 µs, and increased for T f = 6.0 µs.…”
Section: Relationship Between Peak Value Of Applied Impulse Voltage Asupporting
confidence: 67%
“…This behavior of the positive ions brings about the violent jumping phenomena at the creeping discharge tip [ Fig. 6(a)] [8]. Then the positive ion density decreases rapidly at the tip of the creeping leader and a rapid potential drop occurs in the leader, and since the electron emissions arising from the leader tip are restrained, the creeping discharge stops progressing.…”
Section: (Ii) Negative Creeping Dischargesmentioning
confidence: 99%
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“…There are some reports on such linear discharges [2][3][4][5], but their detailed properties are still not fully understood. In the past, we have measured the properties of creeping streamers over wire surfaces initiating from the free ends of the binding wire just after the flashover of the post insulator surface, in order to contribute to countermea-sures against creeping events in aerial distribution systems [6][7][8][9][10]. Creeping discharge phenomena on the wire surface due to actual lightning could be reproduced in the laboratory by applying to the central line of the cable impulse voltages that simulated inductive lightning surges after grounding of the binding wire.…”
Section: Introductionmentioning
confidence: 99%
“…Creeping discharge phenomena on the wire surface due to actual lightning could be reproduced in the laboratory by applying to the central line of the cable impulse voltages that simulated inductive lightning surges after grounding of the binding wire. In our previous papers [7][8][9], a standard lightning impulse voltage was used to simulate an inductive lightning surge. It has been reported that an inductive lightning surge that penetrates to the central line causes an increase of the central line potential, so that the electric fields on the cable surface are altered and a significant negative creeping discharge is included.…”
Section: Introductionmentioning
confidence: 99%