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Abstract: this report, the model was tested on various subsonic and transonic flow problems: flat plates, airfoils, wakes, etc. The model consists of a single advectiondiffusion equation with source term for a field variable which is the product of turbulence Reynolds number and kinematic viscosity, e RT . This variable is proportional to the eddy viscosity except very near a solid wall. The model equation is of the form: D( e RT ) Dt =(c ffl 2 f 2 (y + ) \Gamma c ffl 1 ) q e RT P +( + t ... (Update)
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...approximations for rf to 2 D or 3 D arbitraryconnectivity (fully unstructured) meshes. The method is based on the work of Barth [39], who has devised innovative least squares algorithms for the linear and quadratic reconstruction of discrete data on unstructured meshes....
...unnecessarily sacrificing robustness, accuracy, or efficiency. Our current approach has borrowed from the innovative techniques of Barth [1], an example being least squares reconstruction schemes. We have also extended a 3 D unsplit advection technique [20] to unstructured...
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BibTeX entry: (Update)
Barth, T. J., "Aspects of Unstructured Grids and FiniteVolume Solvers for the Euler and Navier-Stokes Equations," Computational Fluid Dynamics, No. 1994--04 in Lecture Series, von Karman Institute for Fluid Dynamics, 1994. http://citeseer.nj.nec.com/barth95aspects.html More
@misc{ barth94aspects,
author = "T. Barth",
title = "Aspects of Unstructured Grids and FiniteVolume Solvers for the Euler and
Navier-Stokes Equations",
text = "Barth, T. J., Aspects of Unstructured Grids and FiniteVolume Solvers for
the Euler and Navier-Stokes Equations, Computational Fluid Dynamics, No.
1994--04 in Lecture Series, von Karman Institute for Fluid Dynamics, 1994.",
year = "1994",
url = "citeseer.nj.nec.com/barth95aspects.html" }
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