On the judicious use of the k-ε model, wall functions and adaptivity

Abstract This paper shows that accurate predictions of skin friction and Stanton number for a flat plate boundary layer can be achieved with the k – e model of turbulence with wall functions, provided the computational model (turbulence model, geometry, boundary conditions, etc.) is properly defined and that the simulation is grid converged. Emphasis is put on good CFD practices such as verification and validation. Verification allows to obtain numerical predictions with controlled accuracy. Validation of the computational model is thus performed on solid grounds. Predictions of the local skin friction coefficient on the plate were obtained for Reynolds numbers of 2×10 5 and 2×10 6 . In the case Re =2×10 5 , the effects of inlet boundary turbulence Reynolds number, geometry of the plate and type of wall functions are assessed. It is found that an inlet turbulence Reynolds number equal to 10% of the Reynolds number yields realistic results. Significant improvements are achieved if the plate thickness is included in the computational model. Two-velocity scale wall functions prove to be superior to the more popular one-velocity scale wall functions. For the case Re =2×10 6 , predictions of the local skin friction coefficient ( C f ( x )) and the local heat transfer coefficient ( St ( x )) are in good agreement with correlations.

[1]  J. Whitelaw,et al.  Convective heat and mass transfer , 1966 .

[2]  D. Pelletier,et al.  COMPUTATION OF JET IMPINGEMENT HEAT TRANSFER BY AN ADAPTIVE FINITE ELEMENT ALGORITHM , 1998 .

[3]  Dominique Pelletier,et al.  AN ADAPTIVE FINITE ELEMENT METHOD FOR A TWO- EQUATION TURBULENCE MODEL IN WALL-BOUNDED FLOWS , 1997 .

[4]  Dominique Pelletier,et al.  Adaptive remeshing for convective heat transfer with variable fluid properties , 1994 .

[5]  D. Pelletier,et al.  An adaptive finite element method for turbulent heat transfer , 1996 .

[6]  Dominique Pelletier,et al.  A unified approach for adaptive solutions of compressible and incompressible flows , 1997 .

[7]  Dominique Pelletier,et al.  Positivity Preservation and Adaptive Solution for the k-? Model of Turbulence , 1998 .

[8]  William Oberkampf A proposed framework for computational fluid dynamics code calibration and validation , 1993 .

[9]  B. Launder,et al.  The numerical computation of turbulent flows , 1990 .

[10]  William L. Oberkampf,et al.  A proposed methodology for computational fluid dynamics code verification, calibration, and validation , 1995, ICIASF '95 Record. International Congress on Instrumentation in Aerospace Simulation Facilities.

[11]  F. Schultz-grunow New frictional resistance law for smooth plates , 1941 .

[12]  F. Blottner,et al.  Accurate Navier-Stokes results for the hypersonic flow over a spherical nosetip , 1989 .

[13]  Barry W. Boehm,et al.  Software Engineering Economics , 1993, IEEE Transactions on Software Engineering.

[14]  Dominique Pelletier,et al.  Fast, Adaptive Finite Element Scheme for Viscous Incompressible Flows , 1992 .

[15]  D. Pelletier,et al.  Adaptive finite element method for conjugate heat transfer , 1997 .

[16]  M. Nallasamy,et al.  Turbulence models and their applications to the prediction of internal flows: a review , 1987 .

[17]  Patrick J. Roache,et al.  Verification and Validation in Computational Science and Engineering , 1998 .

[18]  Dominique Pelletier,et al.  Prediction of Turbulent Separated Flow in a Turnaround Duct Using Wall Functions and Adaptivity , 2001 .

[19]  P. Raviart,et al.  Conforming and nonconforming finite element methods for solving the stationary Stokes equations I , 1973 .

[20]  T. Hughes,et al.  The Galerkin/least-squares method for advective-diffusive equations , 1988 .

[21]  Donald W. Smith,et al.  Skin-Friction Measurements in Incompressible Flow , 1958 .

[22]  Dominique Pelletier,et al.  Adaptive Finite Element Solution of Compressible Turbulent Flows , 1998 .

[23]  D. Pelletier,et al.  An adaptive finite element method for convective heat transfer with variable fluid properties , 1993 .

[24]  Dominique Pelletier,et al.  ADAPTIVE COMPUTATIONS OF TURBULENT FORCED CONVECTION , 1998 .

[25]  Brian Launder,et al.  Current capabilities for modelling turbulence in industrial flows , 1991 .

[26]  Dominique Pelletier Adaptive finite element computations of complex flows , 1999 .

[27]  Dominique Pelletier,et al.  Compressible heat transfer computations by an adaptive finite element method , 2002 .

[28]  J. Schetz Boundary Layer Analysis , 1992 .

[29]  D. Pelletier,et al.  EFFECTS OF ADAPTIVITY ON FINITE ELEMENT SCHEMES FOR TURBULENT HEAT TRANSFER AND FLOW PREDICTIONS , 2000 .

[30]  Dominique Pelletier,et al.  A General Continuous Sensitivity Equation Formulation for the k-ε Model of Turbulence , 2004 .

[31]  D. Pelletier,et al.  Effects of adaptivity on various finite element schemes for turbulent heat transfer and flow predictions , 1998 .

[32]  A. Bejan Convection Heat Transfer , 1984 .

[33]  Dominique Pelletier,et al.  Adaptive finite element method for thermal flow problems , 1994 .

[34]  Dominique Pelletier,et al.  Adaptive remeshing for viscous incompressible flows , 1990 .

[35]  Dominique Pelletier,et al.  Adaptative remeshing for viscous incompressible flows , 1992 .

[36]  T. Hughes,et al.  Streamline upwind/Petrov-Galerkin formulations for convection dominated flows with particular emphasis on the incompressible Navier-Stokes equations , 1990 .

[37]  Timothy G. Trucano,et al.  Verification and validation. , 2005 .

[38]  Dominique Pelletier,et al.  Adaptive Remeshing for the k-Epsilon Model of Turbulence , 1997 .