Implicit Large-Eddy Simulation of a Deep Cavity Using High-Resolution Methods

Implicit Large Eddy Simulations of a deep cavity at Mach 0.8 and Reynolds based on cavity length of 860,000 have been conducted using a recently developed Implicit Large Eddy Simulation (ILES) method. The numerical method employed is a new fifth-order accurate in space method where the variable extrapolation has been modified to give greatly improved performance in low Mach regions of the flow, such as areas of turbulent flow, yet retaining the shock capturing capabilities of the original method, and positivity of advected species. The ILES results are compared to experimental measurements by Forestier et al. (J. Fluid Mech.,vol. 475, 2003) of the mean flow field, Reynolds stresses and pressure spectra. The frequency and amplitude of the fundamental modes are predicted to within 2% and 6dB at all grid levels. There is excellent agreement of the mean flow field and Reynolds stresses, demonstrating that there is no need for an explicit subgrid model when using the new reconstruction method for this flow configuration.

[1]  Len G. Margolin,et al.  Implicit Turbulence Modeling for High Reynolds Number Flows , 2001 .

[2]  R. J. R. Williams,et al.  An improved reconstruction method for compressible flows with low Mach number features , 2008, J. Comput. Phys..

[3]  Jinhee Jeong,et al.  On the identification of a vortex , 1995, Journal of Fluid Mechanics.

[4]  A. Gosman,et al.  A comparative study of subgrid scale models in homogeneous isotropic turbulence , 1997 .

[5]  P. Sagaut,et al.  On the Use of Shock-Capturing Schemes for Large-Eddy Simulation , 1999 .

[6]  Steven J. Ruuth,et al.  A New Class of Optimal High-Order Strong-Stability-Preserving Time Discretization Methods , 2002, SIAM J. Numer. Anal..

[7]  Philippe Geffroy,et al.  The mixing layer over a deep cavity at high-subsonic speed , 2003, Journal of Fluid Mechanics.

[8]  M. Visbal,et al.  Compact Difference Scheme Applied to Simulation of Low-Sweep Delta Wing Flow. , 2005 .

[9]  L. Margolin,et al.  Large-eddy simulations of convective boundary layers using nonoscillatory differencing , 1999 .

[10]  F. Grinstein,et al.  Large Eddy simulation of high-Reynolds-number free and wall-bounded flows , 2002 .

[11]  P. Sagaut,et al.  Subgrid-Scale Models for Large-Eddy Simulations of Compressible Wall Bounded Flows , 2000 .

[12]  F. Grinstein,et al.  Recent Progress on MILES for High Reynolds Number Flows , 2002 .

[13]  A. N. Kolmogorov Equations of turbulent motion in an incompressible fluid , 1941 .

[14]  Dimitris Drikakis,et al.  On the implicit large eddy simulations of homogeneous decaying turbulence , 2007, J. Comput. Phys..

[15]  Kyu Hong Kim,et al.  Accurate, efficient and monotonic numerical methods for multi-dimensional compressible flows Part II: Multi-dimensional limiting process , 2005 .

[16]  D. Youngs,et al.  Three-dimensional numerical simulation of turbulent mixing by Rayleigh-Taylor instability , 1991 .

[17]  L. Margolin,et al.  MPDATA: A Finite-Difference Solver for Geophysical Flows , 1998 .

[18]  J. P. Boris,et al.  New insights into large eddy simulation , 1992 .

[19]  P. Sagaut,et al.  Large-eddy simulation of a compressible flow past a deep cavity , 2003 .

[20]  P. Woodward,et al.  Inertial range structures in decaying compressible turbulent flows , 1998 .

[21]  G. Volpe Performance of compressible flow codes at low Mach numbers , 1993 .

[22]  Nikolaus A. Adams,et al.  An adaptive local deconvolution method for implicit LES , 2005, J. Comput. Phys..

[23]  D. Drikakis Advances in turbulent flow computations using high-resolution methods , 2003 .

[24]  J. Rossiter Wind tunnel experiments on the flow over rectangular cavities at subsonic and transonic speeds , 1964 .

[25]  F. Grinstein,et al.  LES of Transition to Turbulence in the Taylor Green Vortex , 2006 .

[26]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme. IV. A new approach to numerical convection , 1977 .

[27]  Javier Jiménez,et al.  The structure of intense vorticity in isotropic turbulence , 1993, Journal of Fluid Mechanics.

[28]  Dimitris Drikakis,et al.  On entropy generation and dissipation of kinetic energy in high-resolution shock-capturing schemes , 2008, J. Comput. Phys..

[29]  Chi-Wang Shu,et al.  Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .

[30]  W. Rider,et al.  High-Resolution Methods for Incompressible and Low-Speed Flows , 2004 .

[31]  D. Drikakis,et al.  Large eddy simulation of compressible turbulence using high‐resolution methods , 2005 .

[32]  Chang-Kee Kim,et al.  Cavity Flows in a Scramjet Engine by the Space-Time Conservation and Solution Element Method , 2004 .

[33]  E. Toro Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .

[34]  Clarence W. Rowley,et al.  Cavity Flow Control Simulations and Experiments , 2005 .

[35]  D. Youngs Application of MILES to Rayleigh-Taylor and Richtmyer Meshkov Mixing (Invited) , 2003 .

[36]  J. Anderson,et al.  Fundamentals of Aerodynamics , 1984 .