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9, 1982, pp. 1182-1187. [2] Weidner E. H. and Drummond J. , “Numerical Study of Staged Fuel Injection for Supersonic Combustion”, AIAA Journal, Vol. 10, 1982, pp. 1426-1431. [3] Clarence F. Chenault and Philip S. Beran, “k-e and Reynolds Stress Turbulence Model Comparisons for Two-Dimensional Injection Flows”, AIAA Journal, Vol. 36, No. 8, 1998, pp. 1401-1412. [4] Grasso F. , “Simulation of Transverse Gas Injection in Turbulent Supersonic Air Flows”, AIAA Journal, Vol. 33, No. 1, 1995, pp. 56-62.

Although the qualitative picture of the shock waves are similar for both turbulence models, the evident divergence of the λ -shaped structure is observed in the turbulent boundary layer, which is more prominent for smaller M∞ Figure 2 (a-c). 75 Fig. 2. Shaded picture of pressure for various Mach number with k − ε , B-L, and k − ε compressibility turbulence models The differences among the models in the boundary layer are also evident in the local Mach number contours. The distribution of the iso-Mach line contours is shown in Figure 3.

2005). "3-D particle image velocimetry of the flow field around a sphere sedimenting near a wall: Part 2. " Journal of Non-Newtonian Fluid Mechanics 127(2-3): 95-106. Tatum, J. , M. V. Finnis, et al. (2007). "3D particle image velocimetry of the flow field around a sphere sedimenting near a wall: Part 1. " Journal of Non-Newtonian Fluid Mechanics 141: 99-115. Westerweel, J. (1997). " Measurement Science and Technology 8: 1379-1392. , D. Dabiri, et al. (1997). " Experiments in Fluids 23: 20-28.

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