27th Aerospace Sciences Meeting 1989
DOI: 10.2514/6.1989-668
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A Navier-Stokes solver for high speed equilibrium flows and application to blunt bodies

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Cited by 22 publications
(13 citation statements)
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“…This is the physical behavior you would expect for a blunt body bow shock when comparing results using perfect gas properties to equilibrium air properties [Anderson 1989]. within the numerical convergence criteria used in the two simulations and the ability of the author to read the plots provided by Prabhu (1989) From Figure 4.2 it can be seen that using perfect gas properties causes the temperature in the stagnation region to be more than twice that using equilibrium air properties. This occurs since the perfect gas model does not account for all the modes of energy storage of the molecules.…”
Section: Inviscid Blunt Bodymentioning
confidence: 94%
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“…This is the physical behavior you would expect for a blunt body bow shock when comparing results using perfect gas properties to equilibrium air properties [Anderson 1989]. within the numerical convergence criteria used in the two simulations and the ability of the author to read the plots provided by Prabhu (1989) From Figure 4.2 it can be seen that using perfect gas properties causes the temperature in the stagnation region to be more than twice that using equilibrium air properties. This occurs since the perfect gas model does not account for all the modes of energy storage of the molecules.…”
Section: Inviscid Blunt Bodymentioning
confidence: 94%
“…To verify the inviscid part of the AVUS code the results are compared to the results of Prabhu et al (1989) for a two-dimensional blunt body. To verify the viscous part of the code, results are compared to those of Rosen (1991) for supersonic and hypersonic laminar flow over a flat plate, and to those of Tannehill et al (1990) for hypersonic, laminar flow over a two-dimensional wedge and axisymmetric cone.…”
Section: Adding Chemical Equilibrium To Avusmentioning
confidence: 99%
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“…within the numerical convergence criteria used in the two simulations and the ability of the author to read the plots provided by Prabhu (1989) From Figure 4.2 it can be seen that using perfect gas properties causes the temperature in the stagnation region to be more than twice that using equilibrium air properties. This occurs since the perfect gas model does not account for all the modes of energy storage of the molecules.…”
mentioning
confidence: 99%
“…procedure to generate equilibrium air thermodynamic properties that were then curve ®tted to simulate numerically high-temperature shock tube¯ows. As another representative example, Prabhu et al 3 and Yee et al 4 use the Srinivasan curve ®ts for their numerical predictions of inviscid and viscous hypersonic¯ows. If a set of curve ®ts in turn depends on exponential correlations for the equilibrium constants, then when improved correlations become available, the curve ®ts will have to be revised.…”
Section: Introductionmentioning
confidence: 99%