1988
DOI: 10.1063/1.341285
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Circuit model of surface arcing

Abstract: An electrical breakdown on a highly charged dielectric surface can result in a discharge along the surface, i.e., a flashover arc. We construct a simple circuit model for such an arc: the discharge of a capacitor C (related to the initial charged area) through a series inductor L and resistor R (related to the arc considered as a plasma). The arc current assumes a very simple form over most of its dynamic range, and such measured arc quantities as total charge transport, pulse width, peak current, and rise tim… Show more

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Cited by 6 publications
(2 citation statements)
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“…The pulse power source is represented by the discharging of a capacitor C, while the current pulse is represented as a series combination of an inductance L and a resistance R, as developed by Robiscoe et al [25], [26]. A large shunt resistance R s is used to allow a secondary current I s to drain the capacitor, even if the pulse current I is zero.…”
Section: B Current Pulse Operation and Simulationmentioning
confidence: 99%
“…The pulse power source is represented by the discharging of a capacitor C, while the current pulse is represented as a series combination of an inductance L and a resistance R, as developed by Robiscoe et al [25], [26]. A large shunt resistance R s is used to allow a secondary current I s to drain the capacitor, even if the pulse current I is zero.…”
Section: B Current Pulse Operation and Simulationmentioning
confidence: 99%
“…Payan et al, proposed an equivalent circuit of solar array suitable to set-up an external circuit during a test for the secondary arc 3) . Robiscoe et al, used a simple LCR circuit to model a surface flashover discharge on dielectric surface 4) . In the present paper,…”
Section: Introductionmentioning
confidence: 99%