Proceedings of 1998 International Symposium on Electrical Insulating Materials. 1998 Asian International Conference on Dielectr
DOI: 10.1109/iseim.1998.741791
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Study of the time evolution of partial discharge characteristics and interfacial phenomena of simulated XLPE cable joint

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Cited by 10 publications
(3 citation statements)
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“…Another simulation of a pulse with T r of 1ns and T FWHM of 5 ns being assumed to travel along a cable was performed. In fact, the rise time of observed original PD pulse emanating from any insulation defect is about 1 ns [19,20,21]. The result of the relationship between the upper limit of the bandwidth of the pulse with the propagation length is shown in Figure 7.…”
Section: Bandwidth Of Pulse Propagationmentioning
confidence: 95%
“…Another simulation of a pulse with T r of 1ns and T FWHM of 5 ns being assumed to travel along a cable was performed. In fact, the rise time of observed original PD pulse emanating from any insulation defect is about 1 ns [19,20,21]. The result of the relationship between the upper limit of the bandwidth of the pulse with the propagation length is shown in Figure 7.…”
Section: Bandwidth Of Pulse Propagationmentioning
confidence: 95%
“…PDs at the wire edge with a large space for discharge would form the "I" type of cluster, as the discharge intensity tends to be large and the number of pulses tends to he small. On the other hand, those at the body part with a small space for discharge would he form the "-" type of cluster, as such a space would bring small discharge intensity and large number of pulses [4]. Figure 5 shows the transition of Qmax and PD number (n) when 7 kVrms was applied to the sample with 0.15 mm diameter wire.…”
Section: Resultsmentioning
confidence: 99%
“…The shorter exposure time to the discharge leads to the quicker decay of Vi (4). The surface resistance short time after the exposure to the discharge becomes low.…”
mentioning
confidence: 99%