2018 AIAA Aerospace Sciences Meeting 2018
DOI: 10.2514/6.2018-2085
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Supersonic Modes in Hot-Wall Hypersonic Boundary Layers with Thermochemical Nonequilibrium Effects

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Cited by 19 publications
(15 citation statements)
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“…Rather, it is the collective interaction of mode S, mode F1, and the slow acoustic spectrum that causes the supersonic mode in this case. 19 have noted, there is a modal energy exchange causing a resonant amplification of the stable mode F1 disturbance. This interaction acts as a source term and causes sound to radiate away from the wall.…”
Section: A Case 1 Unsteady Dns Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…Rather, it is the collective interaction of mode S, mode F1, and the slow acoustic spectrum that causes the supersonic mode in this case. 19 have noted, there is a modal energy exchange causing a resonant amplification of the stable mode F1 disturbance. This interaction acts as a source term and causes sound to radiate away from the wall.…”
Section: A Case 1 Unsteady Dns Resultsmentioning
confidence: 99%
“…where U is the state vector of conserved quantities, W is the source terms, and F j and G j are the inviscid and viscous flux vectors, respectively. For further details of the governing equations and thermochemical model, see the work of Knisely and Zhong 19,47 and Mortensen. 46…”
Section: Governing Equations and Gas Modelmentioning
confidence: 99%
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“…where U is the state vector of conserved quantities, W is the source terms, and F j and G j are the inviscid and viscous flux vectors, respectively. For further details of the governing equations and thermochemical model, see the work of Knisely and Zhong 25,33 and Mortensen. 39…”
Section: Governing Equations and Gas Modelmentioning
confidence: 99%
“…Depending on the flow parameters, the excited mode can become supersonic far downstream in vicinity of the upper neutral branch curve. In addition, in 2018 Knisely and Zhong 25 performed thermochemical nonequilibrium LST and DNS studies using similar hot wall flow conditions on a 5-degree half-angle blunt cone and confirmed the existence of the supersonic mode, although it was quite weak and was due to the interaction of mode S, mode F1, and the slow acoustic continuous spectrum. This phenomenon may be attributed to the real gas effect and may have been overlooked in previous simulations assuming chemical equilibrium.…”
Section: Introductionmentioning
confidence: 96%