1993
DOI: 10.21236/ada266748
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Turbulence and Transition Modeling for High-Speed Flows

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Cited by 135 publications
(206 citation statements)
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“…This term couples the turbulent fluctuations to the mean flow by assuming that such fluctuations generate additional stresses or produce momentum transport [170]. There are two major methods to provide closure for the Reynolds stress terms in the Navier-Stokes equation, as fully described in [171] and [170]. However, to compute this term, additional equations are required.…”
Section: Turbulence Modeling Considerationsmentioning
confidence: 99%
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“…This term couples the turbulent fluctuations to the mean flow by assuming that such fluctuations generate additional stresses or produce momentum transport [170]. There are two major methods to provide closure for the Reynolds stress terms in the Navier-Stokes equation, as fully described in [171] and [170]. However, to compute this term, additional equations are required.…”
Section: Turbulence Modeling Considerationsmentioning
confidence: 99%
“…This term is the major problem of turbulence modeling because it requires to be solved in order to compute the mean flow field variables. This is achieved by multiplying the equation by a fluctuating property and performs time averaging for the resulting equation [171]. There are two major methods to provide closure for the Reynolds stress terms in the Navier-Stokes equation, as fully described in [171] and [170].…”
Section: Turbulence Modeling Considerationsmentioning
confidence: 99%
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“…The k-ω model was firstly created independently by Kolmogorov and later by Saffman (1970), Wilcox has continually refined and improved the model during the past three decades and demonstrated its accuracy for a wide range of turbulent flow (Wilcox and Alber, 1972;Wilcox, 1988;Wilcox, 2006). The latest version was put forward in 2006, termed as Wilcox (2006) k-ω model, the turbulent eddy viscosity:…”
Section: Governing Equations and Turbulence Modelsmentioning
confidence: 99%