2001
DOI: 10.1016/s0021-8928(01)00089-2
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Characteristic surfaces in gas flows

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Cited by 3 publications
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“…Indeed, under the Zemplén theorem, D > c(ρ 0 , T 0 ). Then, in view of relation(8), we obtain the chain of inequalitiesD > c(ρ 0 , T 0 ) > c κ (ρ 0 , T 0 ),which implies the evolutionarity of the flow ahead of the traveling-wave front. It should be noted that the need to satisfy the Zemplén theorem in the case of a non-heat-conducting gas [D > c(ρ 0 , T 0 )] determines the value D 0 = c(ρ 0 , T 0 ).…”
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confidence: 94%
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“…Indeed, under the Zemplén theorem, D > c(ρ 0 , T 0 ). Then, in view of relation(8), we obtain the chain of inequalitiesD > c(ρ 0 , T 0 ) > c κ (ρ 0 , T 0 ),which implies the evolutionarity of the flow ahead of the traveling-wave front. It should be noted that the need to satisfy the Zemplén theorem in the case of a non-heat-conducting gas [D > c(ρ 0 , T 0 )] determines the value D 0 = c(ρ 0 , T 0 ).…”
mentioning
confidence: 94%
“…For this system, there are two sound C ± κ -characteristics [8] whose propagation velocity relative to the flow is equal to the sound velocity in the heat-conducting inviscid gas c κ :…”
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confidence: 99%
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