1981
DOI: 10.1175/1520-0469(1981)038<2056:ccolc>2.0.co;2
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Convective Cooling of Lightning Channels

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Cited by 61 publications
(35 citation statements)
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“…Increasing the temperature to 3000 K increases the production rate of NO such that the total number of available nitrogen atoms is converted to NO in 2.60 × 10 −6 s. At 4000 K, NO production rates are the greatest (Table 2 and Fig. 3), in agreement with Picone et al (1981). It should again be noted that total conversion of nitrogen atoms does not imply total conversion of all nitrogen to NO; the quantity of NO produced is limited by the dissociation of nitrogen molecules.…”
Section: Resultssupporting
confidence: 53%
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“…Increasing the temperature to 3000 K increases the production rate of NO such that the total number of available nitrogen atoms is converted to NO in 2.60 × 10 −6 s. At 4000 K, NO production rates are the greatest (Table 2 and Fig. 3), in agreement with Picone et al (1981). It should again be noted that total conversion of nitrogen atoms does not imply total conversion of all nitrogen to NO; the quantity of NO produced is limited by the dissociation of nitrogen molecules.…”
Section: Resultssupporting
confidence: 53%
“…Air within the hot core mixes with surrounding air (Picone et al, 1981), providing a supply of reactants in the near vicinity. Ice crystals in the surrounding corona sheath would survive, and are still in sufficient proximity to the lightning channel to participate in catalytic reactions.…”
Section: Stability Of Ice Crystals At High Temperaturesmentioning
confidence: 99%
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“…The experimental data do not support this possibility, however. 5 Another possibility is the rapid movemeit of the discharge current axis which could result from magnetic forces present when the current is nonnegligible. This could, in turn, displace the surrounding air sufficiently to produce some long-term mixing motion.…”
Section: [I Mechanisms For Convective Coolingmentioning
confidence: 89%
“…(As a result the channel's cooling and expansion rates speed up significantly) This kind of a cooling regime may be realized, for instance, after the interruption of powerful spark discharges [34][35][36][37], pulse arcs and laser sparks [37,38]. It is possible (It may be supposed) that the dynamics of the channel decay of natural lightning as well as that in a long artificial spark, which models it, is also defined by the formation of a turbulent flow in the after-discharge channel [39]. The dependence of the gas cooling process characteristics on a relatively small residual current in the channel has been demonstrated for the first time in (paper) reference [40].…”
Section: Eoard-jiht Ras-istc May 2013mentioning
confidence: 99%