Compressible mixing layer - Linear theory and direct simulation

Results from linear stability analysis are presented for a wide variety of mixing layers, including low-speed layers with variable density and high Mach number mixing layers. The linear amplification predicts correctly the experimentally observed trends in growth rate that are due to velocity ratio, density ratio, and Mach number, provided that the spatial theory is used and the mean flow is a computed solution of the compressible boundary-layer equations. It is found that three-dimensional modes are dominant in the high-speed mixing layer above a convective Mach number of 0.6, and a simple relationship is proposed that approximately describes the orientation of these waves. Direct numerical simulations of the compressible Navier-Stokes equations are used to show the reduced growth rate that is due to increasing Mach number. From consideration of the compressible vorticity equation, it is found that the dominant physics controlling the nonlinear roll-up of vortices in the high-speed mixing layer is contained in an elementary form in the linear eigenfunctions. It is concluded that the linear theory can be very useful for investigating the physics of free shear layers and predicting the growth rate of the developed plane mixing layer

[1]  Sanjiva K. Lele,et al.  Direct numerical simulation of compressible free shear flows , 1989 .

[2]  D. W. Bogdanoff,et al.  Compressibility Effects in Turbulent Shear Layers , 1983 .

[3]  H. Fiedler,et al.  Transport of Heat Across a Plane Turbulent Mixing Layer , 1975 .

[4]  F. White Viscous Fluid Flow , 1974 .

[5]  A. Roshko,et al.  The compressible turbulent shear layer: an experimental study , 1988, Journal of Fluid Mechanics.

[6]  A. Roshko,et al.  On density effects and large structure in turbulent mixing layers , 1974, Journal of Fluid Mechanics.

[7]  N. Sandham,et al.  Growth of oblique waves in the mixing layer at high Mach number , 1989 .

[8]  D. Bogdanoff Interferometric measurement of heterogeneous shear-layer spreading rates , 1984 .

[9]  S. Ragab Instabilities in the free shear layer formed by two supersonic streams , 1988 .

[10]  P. Drazin,et al.  Shear layer instability of an inviscid compressible fluid. Part 2 , 1975, Journal of Fluid Mechanics.

[11]  P. Dimotakis Two-dimensional shear-layer entrainment , 1986 .

[12]  W ThompsonKevin Time-dependent boundary conditions for hyperbolic systems, II , 1987 .

[13]  T. Kubota,et al.  On the instability of inviscid, compressible free shear layers , 1988 .

[14]  A. Michalke,et al.  On the inviscid instability of the hyperbolictangent velocity profile , 1964, Journal of Fluid Mechanics.

[15]  Peter A. Monkewitz,et al.  Influence of the velocity ratio on the spatial instability of mixing layers , 1982 .

[16]  J. A. Fox,et al.  Stability of the laminar mixing of two parallel streams with respect to supersonic disturbances , 1966, Journal of Fluid Mechanics.

[17]  P. Dimotakis,et al.  The mixing layer at high Reynolds number: large-structure dynamics and entrainment , 1976, Journal of Fluid Mechanics.

[18]  Dimitri Papamoschou,et al.  STRUCTURE OF THE COMPRESSIBLE TURBULENT SHEAR LAYER , 1989 .

[19]  N. Sandham,et al.  A numerical investigation of the compressible mixing layer , 1989 .

[20]  K. Thompson Time-dependent boundary conditions for hyperbolic systems, II , 1990 .

[21]  P. Monkewitz,et al.  Absolute and convective instabilities in free shear layers , 1985, Journal of Fluid Mechanics.