2018
DOI: 10.1007/s10973-018-7169-z
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A thermodynamic model for the plasma kernel volume and temperature resulting from spark discharge at high pressures

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Cited by 6 publications
(1 citation statement)
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“…This was already noted by Ko et al [29], who proposed a much more reasoned set of initial conditions based on previous solutions of cylindrical shockwave equations that allow for a mass increase in the activated plasma volume. This solution has been expanded on by Meyer and Wimmer [32] to include the use of air plasma properties for better estimating the post-cooldown temperature 𝑇 𝑖 , and it requires solving three relatively simple equations: { π‘Ÿ 𝑖,𝑐𝑦𝑙 = 0.5π‘Ÿ 𝑐 = 0. Using the present method and πœ‚ 𝑏𝑑 β‰… 1 (see Section 3), for air at the same conditions as above the results are π‘Ÿ 𝑖,𝑐𝑦𝑙 = 0.825 mm, 𝑑 𝑖 = 7.12 ΞΌs, and 𝑇 𝑖 = 6,139 K, all of which fully consistent with heat diffusion models but stemming from a much sounder procedure.…”
Section: Initial Conditions: the Breakdown Modelmentioning
confidence: 99%
“…This was already noted by Ko et al [29], who proposed a much more reasoned set of initial conditions based on previous solutions of cylindrical shockwave equations that allow for a mass increase in the activated plasma volume. This solution has been expanded on by Meyer and Wimmer [32] to include the use of air plasma properties for better estimating the post-cooldown temperature 𝑇 𝑖 , and it requires solving three relatively simple equations: { π‘Ÿ 𝑖,𝑐𝑦𝑙 = 0.5π‘Ÿ 𝑐 = 0. Using the present method and πœ‚ 𝑏𝑑 β‰… 1 (see Section 3), for air at the same conditions as above the results are π‘Ÿ 𝑖,𝑐𝑦𝑙 = 0.825 mm, 𝑑 𝑖 = 7.12 ΞΌs, and 𝑇 𝑖 = 6,139 K, all of which fully consistent with heat diffusion models but stemming from a much sounder procedure.…”
Section: Initial Conditions: the Breakdown Modelmentioning
confidence: 99%