Development of Roe-type scheme for all-speed flows based on preconditioning method

The problems of mixed low-speed/high-speed flows are not solved properly with existing compressible method. Based on preconditioning technology, a new scheme, All-Speed-Roe scheme, is proposed. Compared with Roe scheme, it decreases the effect of acoustic speed in its numerical dissipation when Mach numbers decrease. Compared with traditional preconditioned Roe scheme, it overcomes the limit of being cut-off by the global Mach number through modifying the eigenvalues only and has the good convergence acceleration rate for low-Mach-number flows through multiplying the spatial residual by the preconditioner. From another perspective, All-Speed-Roe scheme suggests that there is no necessity to replace the physical acoustic speed in denominator with pseudo-acoustic speed. In theory, All-Speed-Roe scheme is suitable for all speed flow calculations with capturing shock and simulating low-Mach-number flows. The numerical results of Euler nozzle flow, RANS of NASA rotor 37 flow, Euler simulation, Large Eddy Simulation (LES) and Detached Eddy Simulation (DES) of high-loaded blade T106 flow show that All-Speed-Roe scheme can replace traditional preconditioned Roe scheme because it is easier for programming, more robust in computations, more accurate in spatial, and has good convergence rate.

[1]  David L. Darmofal,et al.  The Importance of Eigenvectors for Local Preconditioners of the Euler Equations , 1996 .

[2]  C. Rhie,et al.  Numerical Study of the Turbulent Flow Past an Airfoil with Trailing Edge Separation , 1983 .

[3]  H. Guillard,et al.  On the behaviour of upwind schemes in the low Mach number limit , 1999 .

[4]  J. Edwards,et al.  Low-Diffusion Flux-Splitting Methods for Flows at All Speeds , 1997 .

[5]  Wayne A. Smith,et al.  Preconditioning Applied to Variable and Constant Density Flows , 1995 .

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

[7]  John D. Denton,et al.  Lessons from rotor 37 , 1997 .

[8]  P. Sagaut,et al.  Large Eddy Simulation of Flow Around an Airfoil Near Stall , 2002 .

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

[10]  Xue-song Li,et al.  An All-Speed Roe-type scheme and its asymptotic analysis of low Mach number behaviour , 2008, J. Comput. Phys..

[11]  XueSong Li,et al.  Preconditioning method and engineering application of large eddy simulation , 2008 .

[12]  E. Turkel,et al.  PRECONDITIONING TECHNIQUES IN COMPUTATIONAL FLUID DYNAMICS , 1999 .

[13]  Javier Jiménez,et al.  Transition to turbulence in two-dimensional Poiseuille flow , 1990, Journal of Fluid Mechanics.

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

[15]  C. L. Merkle,et al.  The application of preconditioning in viscous flows , 1993 .

[16]  Meng-Sing Liou,et al.  A sequel to AUSM, Part II: AUSM+-up for all speeds , 2006, J. Comput. Phys..

[17]  P. Sagaut,et al.  High-Resolution Large-Eddy Simulation of Flow Around Low-Pressure Turbine Blade , 2003 .

[18]  P. Spalart,et al.  A New Version of Detached-eddy Simulation, Resistant to Ambiguous Grid Densities , 2006 .

[19]  Z. Wang A fast flux-splitting for all speed flow , 1997 .

[20]  Cord-Christian Rossow,et al.  A flux-splitting scheme for compressible and incompressible flows , 2000 .

[21]  Pierre Sagaut,et al.  An algorithm for unsteady viscous flows at all speeds , 2000 .

[22]  E. Turkel,et al.  Preconditioned methods for solving the incompressible low speed compressible equations , 1987 .

[23]  Vittorio Puoti,et al.  Preconditioning Method for Low-Speed Flows , 2001 .