28th International Symposium on Shock Waves 2012
DOI: 10.1007/978-3-642-25685-1_144
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Triple–Shock–Wave Configurations: Comparison of Different Thermodynamic Models for Diatomic Gases

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Cited by 3 publications
(2 citation statements)
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“…The zero-order problem is confined to determination of the flow downstream the shock parameters: pressure p, density ρ, velocity polar angle Θ and magnitude V , and the discontinuity inclination angle σ and the flow deflection angle β. Since the shock intensity J and its inclination angle σ for the given incoming flow parameters are interdependent (for instance, Mostovykh & Uskov 2011), the shock can be specified by any of these values; this fact is used later on. Note that in the zero-order problem the input parameters Θ and χ influence only on the angle Θ value:…”
Section: Differential Dynamic Compatibility Conditions On Shock Wavesmentioning
confidence: 99%
See 1 more Smart Citation
“…The zero-order problem is confined to determination of the flow downstream the shock parameters: pressure p, density ρ, velocity polar angle Θ and magnitude V , and the discontinuity inclination angle σ and the flow deflection angle β. Since the shock intensity J and its inclination angle σ for the given incoming flow parameters are interdependent (for instance, Mostovykh & Uskov 2011), the shock can be specified by any of these values; this fact is used later on. Note that in the zero-order problem the input parameters Θ and χ influence only on the angle Θ value:…”
Section: Differential Dynamic Compatibility Conditions On Shock Wavesmentioning
confidence: 99%
“…, A 8 , B 1 , B 2 in these expansions for different gases are cited in (McBride et al 1963;McBride, Gordon & Reno 1993). This model was previously considered by the authors in (Uskov & Mostovykh 2011). In this paper, oxygen is taken as a calorically imperfect gas; a comparison of its enthalpy and entropy with a diatomic perfect gas is shown in figure 2.…”
Section: Consequentlymentioning
confidence: 99%