FULLY DEVELOPED TURBULENT FLOW IN A PLANE CHANNEL COMPUTED AT A REYNOLDS NUMBER OF 5.0E+04 TO COINCIDE WITH EXPERIMENTAL DATA OF LAUFER 1951 32 COMPUTATIONAL GRID POINTS USED --- WALL IS AT y = 0 RESULTS OF DEMUREN AND SARKAR - JFE VOL. 115, PP. 5-12, 1993 *************** TURBULENCE MODEL ******************* Standard k-e turbulence model Normalized Wall Shear Stress -- (U_tau)/(U_b) = 4.40E-02 Computed Profiles of the Mean Velocity and Turbulence Fields y/delta (U_1)/(U_b) k/(U_b)^2 Epsilon*delta/(U_b)^3 1.16E-02 5.97E-01 6.44E-03 1.83E-02 3.53E-02 7.13E-01 6.42E-03 6.94E-03 6.03E-02 7.76E-01 6.12E-03 3.85E-03 8.65E-02 8.20E-01 5.87E-03 2.54E-03 1.14E-01 8.54E-01 5.64E-03 1.85E-03 1.43E-01 8.82E-01 5.43E-03 1.42E-03 1.73E-01 9.06E-01 5.22E-03 1.13E-03 2.05E-01 9.28E-01 5.01E-03 9.19E-04 2.38E-01 9.47E-01 4.79E-03 7.60E-04 2.73E-01 9.64E-01 4.57E-03 6.35E-04 3.10E-01 9.81E-01 4.35E-03 5.34E-04 3.49E-01 9.96E-01 4.12E-03 4.51E-04 3.90E-01 1.01E+00 3.88E-03 3.81E-04 4.32E-01 1.02E+00 3.64E-03 3.22E-04 4.77E-01 1.04E+00 3.39E-03 2.71E-04 5.23E-01 1.05E+00 3.15E-03 2.27E-04 5.68E-01 1.06E+00 2.92E-03 1.92E-04 6.10E-01 1.07E+00 2.72E-03 1.64E-04 6.51E-01 1.07E+00 2.54E-03 1.41E-04 6.90E-01 1.08E+00 2.38E-03 1.22E-04 7.27E-01 1.08E+00 2.25E-03 1.07E-04 7.62E-01 1.09E+00 2.13E-03 9.54E-05 7.95E-01 1.09E+00 2.03E-03 8.58E-05 8.27E-01 1.09E+00 1.96E-03 7.83E-05 8.57E-01 1.10E+00 1.89E-03 7.25E-05 8.86E-01 1.10E+00 1.84E-03 6.81E-05 9.14E-01 1.10E+00 1.81E-03 6.49E-05 9.40E-01 1.10E+00 1.78E-03 6.27E-05 9.65E-01 1.10E+00 1.77E-03 6.13E-05 9.88E-01 1.10E+00 1.76E-03 6.07E-05 ***************************************************** Budget of k - Normalized with (U_b)^3/delta y/delta Diffusion Production Dissipation 1.16E-02 -1.81E-03 2.01E-02 -1.83E-02 3.53E-02 -3.55E-04 7.30E-03 -6.94E-03 6.03E-02 -4.87E-05 3.89E-03 -3.85E-03 8.65E-02 -4.78E-05 2.59E-03 -2.54E-03 1.14E-01 -4.92E-05 1.90E-03 -1.85E-03 1.43E-01 -4.75E-05 1.47E-03 -1.42E-03 1.73E-01 -4.37E-05 1.17E-03 -1.13E-03 2.05E-01 -3.87E-05 9.57E-04 -9.19E-04 2.38E-01 -3.32E-05 7.93E-04 -7.60E-04 2.73E-01 -2.73E-05 6.62E-04 -6.35E-04 3.10E-01 -2.13E-05 5.56E-04 -5.34E-04 3.49E-01 -1.51E-05 4.66E-04 -4.51E-04 3.90E-01 -8.69E-06 3.90E-04 -3.81E-04 4.32E-01 -2.09E-06 3.24E-04 -3.22E-04 4.77E-01 4.68E-06 2.66E-04 -2.71E-04 5.23E-01 1.17E-05 2.15E-04 -2.27E-04 5.68E-01 1.87E-05 1.73E-04 -1.92E-04 6.10E-01 2.52E-05 1.38E-04 -1.64E-04 6.51E-01 3.13E-05 1.10E-04 -1.41E-04 6.90E-01 3.69E-05 8.55E-05 -1.22E-04 7.27E-01 4.18E-05 6.55E-05 -1.07E-04 7.62E-01 4.62E-05 4.92E-05 -9.54E-05 7.95E-01 4.99E-05 3.59E-05 -8.58E-05 8.27E-01 5.30E-05 2.53E-05 -7.83E-05 8.57E-01 5.55E-05 1.70E-05 -7.25E-05 8.86E-01 5.74E-05 1.07E-05 -6.81E-05 9.14E-01 5.88E-05 6.12E-06 -6.49E-05 9.40E-01 5.97E-05 2.96E-06 -6.27E-05 9.65E-01 6.03E-05 1.01E-06 -6.13E-05 9.88E-01 5.97E-05 1.01E-06 -6.07E-05 ***************************************************** Budget of Epsilon - Normalized with (U_b)^4/delta^2 y/delta Diffusion Production Dissipation 1.16E-02 1.76E-02 8.25E-02 -1.00E-01 3.53E-02 3.05E-03 1.14E-02 -1.44E-02 6.03E-02 1.12E-03 3.53E-03 -4.64E-03 8.65E-02 5.00E-04 1.62E-03 -2.12E-03 1.14E-01 2.68E-04 8.95E-04 -1.16E-03 1.43E-01 1.60E-04 5.52E-04 -7.12E-04 1.73E-01 1.04E-04 3.65E-04 -4.69E-04 2.05E-01 7.07E-05 2.53E-04 -3.24E-04 2.38E-01 5.02E-05 1.81E-04 -2.31E-04 2.73E-01 3.69E-05 1.32E-04 -1.69E-04 3.10E-01 2.77E-05 9.83E-05 -1.26E-04 3.49E-01 2.14E-05 7.36E-05 -9.49E-05 3.90E-01 1.68E-05 5.52E-05 -7.20E-05 4.32E-01 1.34E-05 4.13E-05 -5.47E-05 4.77E-01 1.09E-05 3.06E-05 -4.15E-05 5.23E-01 9.09E-06 2.24E-05 -3.15E-05 5.68E-01 7.82E-06 1.64E-05 -2.42E-05 6.10E-01 6.92E-06 1.20E-05 -1.89E-05 6.51E-01 6.25E-06 8.75E-06 -1.50E-05 6.90E-01 5.74E-06 6.32E-06 -1.21E-05 7.27E-01 5.34E-06 4.51E-06 -9.85E-06 7.62E-01 5.03E-06 3.17E-06 -8.20E-06 7.95E-01 4.77E-06 2.18E-06 -6.95E-06 8.27E-01 4.56E-06 1.46E-06 -6.02E-06 8.57E-01 4.39E-06 9.38E-07 -5.33E-06 8.86E-01 4.26E-06 5.70E-07 -4.83E-06 9.14E-01 4.15E-06 3.16E-07 -4.47E-06 9.40E-01 4.08E-06 1.50E-07 -4.23E-06 9.65E-01 4.04E-06 5.06E-08 -4.09E-06 9.88E-01 3.97E-06 5.02E-08 -4.02E-06