Enhancement of USM3D Unstructured Flow Solver for High-Speed High-Temperature Shear Flows

Large temperature and pressure fluctuations have a profound effect on turbulence development in transonic and supersonic jets. For high-speed, high-temperature jet flows, standard turbulence models lack the ability to predict the observed mixing rate of a shear layer. Several proposals to address this deficiency have been advanced in the literature to modify the turbulence transport equations in a variety of ways. In the present study, some of the most proven and simple modifications to two-equation turbulence models have been selected and implemented in NASA's USM3D tetrahedral Navier-Stokes flow solver. The modifications include the addition of compressibility correction and pressure dilatation terms in the turbulence transport equations for high-speed flows, and the addition of a simple modification to the Boussinesq's closure model coefficient for high-temperature jets. The efficacy of the extended models is demonstrated by comparison with experimental data for two supersonic axisymmetric jet test cases at design pressure ratio.

[1]  W. Jones,et al.  The prediction of laminarization with a two-equation model of turbulence , 1972 .

[2]  J. M. Eggers,et al.  Velocity profiles and eddy viscosity distributions downstream of a Mach 2.22 nozzle exhausting to quiescent air , 1966 .

[3]  Karen A. Deere,et al.  Propulsion Simulations Using Advanced Turbulence Models with the Unstructured Grid CFD Tool, TetrUSS , 2004 .

[4]  Neal T. Frink,et al.  Upwind Scheme for Solving the Euler Equations on Unstructured Tetrahedral Meshes , 1992 .

[5]  Meng-Sing Liou,et al.  A Continuing Search for a Near-Perfect Numerical Flux Scheme. Part 1; [AUSM+] , 1994 .

[6]  Samareh Jamshid,et al.  GridTool: A Surface Modeling and Grid Generation , 2022 .

[7]  J. Lumley,et al.  A new Reynolds stress algebraic equation model , 1994 .

[8]  Yildirim Suzen,et al.  Investigation of Supersonic Jet Exhaust Flow by One-and Two-Equation Turbulence Models , 1998 .

[9]  Neal T. Frink,et al.  Tetrahedral Unstructured Navier-Stokes Method for Turbulent Flows , 1998 .

[10]  Shahyar Pirzadeh,et al.  Unstructured Viscous Grid Generation by Advancing-Layers Method , 1993 .

[11]  Gordon Erlebacher,et al.  The analysis and modelling of dilatational terms in compressible turbulence , 1989, Journal of Fluid Mechanics.

[12]  A Boundary Condition for Simulation of Flow Over Porous Surfaces , 2001 .

[13]  Paresh Parikh,et al.  The NASA tetrahedral unstructured software system (TetrUSS) , 2000, The Aeronautical Journal (1968).

[14]  S. Girimaji Fully explicit and self-consistent algebraic Reynolds stress model , 1995 .

[15]  David C. Wilcox,et al.  Progress in hypersonic turbulence modeling , 1991 .

[16]  S. Pirzadeh Structured background grids for generation of unstructured grids by advancing front method , 1991 .

[17]  Richard L. Campbell,et al.  Implementation of Flow Tripping Capability in the USM3D Unstructured Flow Solver , 2006 .

[18]  F. Menter Improved two-equation k-omega turbulence models for aerodynamic flows , 1992 .

[19]  W. K. Anderson,et al.  An implicit upwind algorithm for computing turbulent flows on unstructured grids , 1994 .

[20]  P. Roe CHARACTERISTIC-BASED SCHEMES FOR THE EULER EQUATIONS , 1986 .

[21]  Michael A. Leschziner,et al.  Average-State Jacobians and Implicit Methods for Compressible Viscous and Turbulent Flows , 1997 .

[22]  P. Spalart A One-Equation Turbulence Model for Aerodynamic Flows , 1992 .

[23]  Steven J. Massey,et al.  Temperature Corrected Turbulence Model for High Temperature Jet Flow , 2003 .

[24]  Neal T. Frink,et al.  Progress Toward Overset-Grid Moving Body Capability for USM3D Unstructured Flow Solver , 2005 .

[25]  N T Frink,et al.  Recent Progress Toward a Three-Dimensional Unstructured Navier-Stokes Flow Solver , 1994 .