1985
DOI: 10.1109/tpas.1985.319182
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Dielectric Phase in an SF6 Model Breaker

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Cited by 9 publications
(7 citation statements)
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“…The recovery curve features great similarity with experimental curves previously found for SF 6 [2][3][4] or other insulating gases recovering more slowly [25][26][27], for a variety of gas pressure and test gap configurations. In fact, Figure 9 presents also the SF 6 normalized recovery curves obtained by other research groups: Schoetzau et al (SCO) using an industrial circuit-breaker with double gas flow arrangement [3], and Stokes et al (STO) [4] based on an experimental simulation with metal vapor pollution.…”
Section: Dielectric Recovery Characteristics Of Sfsupporting
confidence: 81%
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“…The recovery curve features great similarity with experimental curves previously found for SF 6 [2][3][4] or other insulating gases recovering more slowly [25][26][27], for a variety of gas pressure and test gap configurations. In fact, Figure 9 presents also the SF 6 normalized recovery curves obtained by other research groups: Schoetzau et al (SCO) using an industrial circuit-breaker with double gas flow arrangement [3], and Stokes et al (STO) [4] based on an experimental simulation with metal vapor pollution.…”
Section: Dielectric Recovery Characteristics Of Sfsupporting
confidence: 81%
“…In fact, Figure 9 presents also the SF 6 normalized recovery curves obtained by other research groups: Schoetzau et al (SCO) using an industrial circuit-breaker with double gas flow arrangement [3], and Stokes et al (STO) [4] based on an experimental simulation with metal vapor pollution.…”
Section: Dielectric Recovery Characteristics Of Sfmentioning
confidence: 97%
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“…Time scales for thermal reignition in well-designed SF 6 circuit breakers are typically in the range of a few microseconds [23]. However, the transition regime between thermal and dielectric breakdown (referred to as Paschen by Schoetzau) regimes during which temperatures above 1500 K exist has been found to last up to 200 µs for a model double flow circuit breaker in SF 6 by Schoetzau [24]. It is likely that this time scale extends considerably in case of an unblown, free burning arc in a very small electrode gap (i.e.…”
Section: Example Validation Measurementsmentioning
confidence: 99%
“…In fact, study of the plasma mean temperature evolution shows that 300 ms after arc extinction the estimated value decays below the SF 6 molecule dissociation limit (of about 2100 K) [13]. For such conditions the post-arc dielectric strength of the recovering plasma is proportional to gas density as has been shown by other research groups [15][16][17]. The ignition of this last phase depends on factors acting in the breaker chamber such as gas flow or gas pollution by metal vapor.…”
Section: Sf 6 Recovery Characteristicsmentioning
confidence: 82%