2011
DOI: 10.1109/temc.2011.2109063
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Some Inferences From Radial Electric Fields Measured Inside the Lightning-Channel Corona Sheath

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Cited by 19 publications
(17 citation statements)
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“…A lot of numerical models were built to study the characteristics of the lightning channel corona sheath, such as sheath radius, sheath expansion velocity, and corona current (Maslowski & Rakov, 2006;Maslowski et al, 2011;Maslowski & Rakov, 2013;Xu & Chen, 2013;Chan et al, 2018).…”
Section: Introductionmentioning
confidence: 99%
“…A lot of numerical models were built to study the characteristics of the lightning channel corona sheath, such as sheath radius, sheath expansion velocity, and corona current (Maslowski & Rakov, 2006;Maslowski et al, 2011;Maslowski & Rakov, 2013;Xu & Chen, 2013;Chan et al, 2018).…”
Section: Introductionmentioning
confidence: 99%
“…Interestingly, the maximum horizontal electric field values during some return strokes were high enough (from 413 kV/m up to more than 520 kV/m) for starting positive breakdown. Time of field relaxation to practically zero level during the overcompensation stage is very similar for all measured waveshapes and is estimated to be approximately 2 ms [23,34]. Hence, one can estimate the decay time constant to be about one-third of this value.…”
Section: Dynamics Of the Corona Sheathmentioning
confidence: 56%
“…Note also that this constant value is assumed to be at the border of the corona sheath which initially expands during the first stage of the return stroke, and then, it shrinks. The radial electric field changes measured at a fixed point of space inside the corona sheath during rocket-and-wire triggered lightning experiments has been discussed in papers [20,23,34].…”
Section: Dynamics Of the Corona Sheathmentioning
confidence: 99%
“…Note that, according to Maslowski and Rakov [2006], the conductivity of corona sheath surrounding the lightning channel at the beginning of the return‐stroke stage is a few μ S/m or so. Further, Maslowski et al [2011] estimated the apparent conductivity of return‐stroke corona sheath to be of the order of 10 −8 S/m. It follows from Figure 6 that the influence of corona sheath conductivity on the nearby ground‐level electric field is negligible, so that the corona sheath can be assumed to be perfectly conducting.…”
Section: Modelmentioning
confidence: 99%