2015
DOI: 10.1007/s00193-015-0615-y
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Interaction theory of hypersonic laminar near-wake flow behind an adiabatic circular cylinder

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Cited by 19 publications
(2 citation statements)
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“…Obviously, an increase in the Mach number Ma ∞ leads to a higher curvature of the detached shock. Hinman et al [37] performed numerical simulations at an even higher Mach number Ma ∞ = 10 and Re D = 5.5 × 10 4 , where the flow structure is somehow similar compared to Figure 21. However, there are noticeable differences in the flow structure, namely the lid separation shock, which connects the recirculation region with the oblique shock and there is more curvature in the detached shock due to the high Mach number.…”
Section: Kármán Vortex Streetmentioning
confidence: 84%
“…Obviously, an increase in the Mach number Ma ∞ leads to a higher curvature of the detached shock. Hinman et al [37] performed numerical simulations at an even higher Mach number Ma ∞ = 10 and Re D = 5.5 × 10 4 , where the flow structure is somehow similar compared to Figure 21. However, there are noticeable differences in the flow structure, namely the lid separation shock, which connects the recirculation region with the oblique shock and there is more curvature in the detached shock due to the high Mach number.…”
Section: Kármán Vortex Streetmentioning
confidence: 84%
“…A fully coupled fluid-solid approach for upward flame spread has been developed within Sutherland's law [18,65], and α is obtained by / ( ) Cp α λ ρ = , where λ is the thermal conductivity obtained by the modified eucken correction [65], and the specific heat at constant pressure Cp is calculated by [18,65]. D is given as D =α .…”
Section: Discussionmentioning
confidence: 99%