# Johnson-King model

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 Revision as of 04:20, 24 November 2005 (view source)Suneesh (Talk | contribs) (→References)← Older edit Latest revision as of 05:48, 17 January 2012 (view source)Tnnandi (Talk | contribs) (5 intermediate revisions not shown) Line 1: Line 1: + {{Turbulence modeling}} + + It is also categorized as half-equation model, because it essentially solves for an Ordinary Differential Equation (ODE) rather than a Partial Differential Equation (PDE) (Normally for popular turbulence models transport equations are solved which are PDE's). This model solves for a transport equation for the maximum shear stress. It was not developed to be a universal model, rather to solve only for turbulent boundary layer flows with strong adverse pressure gradient. + == References == == References == *Johnson, D.A. and King, L.S. A mathematically simple turbulence closure model for attached and separated turbulent boundary layers, AIAA Journal, 23, 1684-1692, 1985. *Johnson, D.A. and King, L.S. A mathematically simple turbulence closure model for attached and separated turbulent boundary layers, AIAA Journal, 23, 1684-1692, 1985. + [[Category:Turbulence models]] - ---- + {{stub}} - Return to [[Turbulence modeling]] +

## Latest revision as of 05:48, 17 January 2012

It is also categorized as half-equation model, because it essentially solves for an Ordinary Differential Equation (ODE) rather than a Partial Differential Equation (PDE) (Normally for popular turbulence models transport equations are solved which are PDE's). This model solves for a transport equation for the maximum shear stress. It was not developed to be a universal model, rather to solve only for turbulent boundary layer flows with strong adverse pressure gradient.

## References

• Johnson, D.A. and King, L.S. A mathematically simple turbulence closure model for attached and separated turbulent boundary layers, AIAA Journal, 23, 1684-1692, 1985.