Numerical Solution for Supersonic Turbulent Flow over a Compression Ramp

A modified eddy viscosity model is incorporated into the compressible Navier-Stokes equations. The modification attempts to reproduce the response of turbulence to a severe pressure gradient in the flowfield. This relaxation phenomenon is described by an exponential decay of the unperturbed eddy viscosity coefficient downstream of the perturbation in terms of a prescribed length scale. The system of equations is solved by MacCormack's time-splitting explicit numerical scheme for a series of compression corner configurations. Computations are performed for ramp angles varying from 15 to 25° at a Mach number of 2.96 and a Reynolds number of 10 7. Calculations utilizing the modified eddy viscosity for the interacting turbulent flow compare very well with experimental measurements, particularly in the prediction of the upstream pressure propagation and location of the separation and the reattachment points. Good agreement is also attained between the measured and calculated density profiles in the viscous-inviscid interaction region.

[1]  R. W. MacCormack,et al.  Numerical Simulation of Supersonic and Hypersonic Turbulent Compression Corner Flows , 1977 .

[2]  A. Havener,et al.  Supersonic Wind Tunnel Investigations Using Pulsed Laser Holography , 1973 .

[3]  L. Crocco,et al.  A suggestion for the numerical solution of the steady Navier-Stokes equations. , 1965 .

[4]  V. Vatsa,et al.  Numerical Solution of Interacting Supersonic Boundary Layer Flows Including Separation Effects , 1973 .

[5]  A. Havener,et al.  Turbulent Boundary-Layer Flow Separation Measurements Using Holographic Interferometry , 1974 .

[6]  P. Bradshaw Effects of Streamline Curvature on Turbulent Flow. , 1973 .

[7]  J. Carter Numerical solutions of the supersonic, laminar flow over a two-dimensional compression corner , 1973 .

[8]  D. A. Johnson,et al.  A study of shock-wave turbulent boundary layer interaction using laser velocimeter and hot-wire anemometer techniques , 1974 .

[9]  C. Herbert Law,et al.  Supersonic, Turbulent Boundary-Layer Separation , 1974 .

[10]  D. C. Wilcox,et al.  Turbulence-Model Predictions for Turbulent Boundary Layers , 1974 .

[11]  David C. Wilcox,et al.  Numerical Study of Separated Turbulent Flows , 1974 .

[12]  D. Dwoyer SUPERSONIC AND HYPERSONIC TWO-DIMENSIONAL LAMINAR FLOW OVER A COMPRESSION CORNER , 1973 .

[13]  J. Shang,et al.  Numerical Analysis of Eddy Viscosity Models in Supersonic Turbulent Boundary Layers , 1973 .

[14]  R. W. Maccormack,et al.  Numerical solution of the interaction of a strong shock wave with a hypersonic turbulent boundary layer , 1974 .

[15]  D. Rizzetta,et al.  Asymptotic solution for supersonic viscous flow past a compression corner , 1975 .

[16]  Roddam Narasimha,et al.  Equilibrium and relaxation in turbulent wakes , 1972, Journal of Fluid Mechanics.

[17]  R. G. Deissler Evolution of a moderately short turbulent boundary layer in a severe pressure gradient , 1974, Journal of Fluid Mechanics.

[18]  Robert W. MacCormack,et al.  Numerical solution of the interaction of a shock wave with a laminar boundary layer , 1971 .

[19]  Tuncer Cebeci,et al.  Calculation of compressible adiabatic turbulent boundary layers , 1970 .