1965
DOI: 10.1038/2071085a0
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Variation of Breakdown Voltage of a Positive-point/Plane Gap with Applied Voltage Waveshape

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Cited by 9 publications
(1 citation statement)
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“…Thus a pulse of fast rise time applied to a small atmospheric-pressure gap usually requires larger voltages for breakdown; while with very large gaps the well-known 'U' curve (Bazelyan et al 1961) is obtained (where the breakdown voltage passes through a minimum with increasing rise time). Even though in the latter example the gap geometry (positive-point, negative-plane) is very different from that considered in this paper, this example is still very interesting, since a convincing explanation has been given in terms of space-charge dynamics with, in this case, the space charge arising from a prebreakdown corona (Boylett et al 1965). The concept of the all-important nature of the space charge in determining the electric field is shared in common with the present paper.…”
Section: Influence Of Transients Upon Breakdownmentioning
confidence: 72%
“…Thus a pulse of fast rise time applied to a small atmospheric-pressure gap usually requires larger voltages for breakdown; while with very large gaps the well-known 'U' curve (Bazelyan et al 1961) is obtained (where the breakdown voltage passes through a minimum with increasing rise time). Even though in the latter example the gap geometry (positive-point, negative-plane) is very different from that considered in this paper, this example is still very interesting, since a convincing explanation has been given in terms of space-charge dynamics with, in this case, the space charge arising from a prebreakdown corona (Boylett et al 1965). The concept of the all-important nature of the space charge in determining the electric field is shared in common with the present paper.…”
Section: Influence Of Transients Upon Breakdownmentioning
confidence: 72%