Generalized Characteristic Interface Conditions for Accurate Multi-block Computation

In a practical computation with a structured grid around a complex body, singular points can be frequently found where an abrupt grid change exists. The grid singularity poses a troublesome problem when some finite difference scheme with high accuracy and resolution is applied. An excellent theory has been proposed, which solve the above singular problem by decomposing a computational domain into two blocks along a line or a surface which contains the singular points and by imposing accurate characteristic-based interface conditions at the block interface. However, the original theory has a limitation on the combination between the adjacent computational coordinate definitions. Concretely, these two coordinates have to be the same direction on the block interface. For a flexible coordinate arrangement without the restriction, the original characteristic-based interface treatment is extended and generalized. Consequently, the coincidence of the computational coordinate definitions becomes unnecessary, and a more flexible multi-block computation can be realized successfully. Numerical test analysis of vortex convection is performed for validation of the new theory, and excellent performance is confirmed as a result.

[1]  T. Poinsot Boundary conditions for direct simulations of compressible viscous flows , 1992 .

[2]  D. Gaitonde,et al.  Pade-Type Higher-Order Boundary Filters for the Navier-Stokes Equations , 2000 .

[3]  J. Kim,et al.  Optimized Compact Finite Difference Schemes with Maximum Resolution , 1996 .

[4]  M.Y. Hussaini,et al.  Low-Dissipation and Low-Dispersion Runge-Kutta Schemes for Computational Acoustics , 1994 .

[5]  Christopher A. Kennedy,et al.  Improved boundary conditions for viscous, reacting, compressible flows , 2003 .

[6]  Robert Prosser,et al.  Improved boundary conditions for the direct numerical simulation of turbulent subsonic flows. I. Inviscid flows , 2005 .

[7]  Miguel R. Visbal,et al.  High-Order Schemes for Navier-Stokes Equations: Algorithm and Implementation Into FDL3DI , 1998 .

[8]  D. Thévenin,et al.  Accurate Boundary Conditions for Multicomponent Reactive Flows , 1995 .

[9]  Josette Bellan,et al.  Consistent Boundary Conditions for Multicomponent Real Gas Mixtures Based on Characteristic Waves , 2002 .

[10]  C. Hirsch,et al.  Numerical Computation of Internal and External Flows. By C. HIRSCH. Wiley. Vol. 1, Fundamentals of Numerical Discretization. 1988. 515 pp. £60. Vol. 2, Computational Methods for Inviscid and Viscous Flows. 1990, 691 pp. £65. , 1991, Journal of Fluid Mechanics.

[11]  J. Kim,et al.  Characteristic Interface Conditions for Multiblock High-Order Computation on Singular Structured Grid , 2003 .

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

[13]  Duck-Joo Lee,et al.  Generalized Characteristic Boundary Conditions for Computational Aeroacoustics, Part 2 , 2000 .

[14]  S. Lele Compact finite difference schemes with spectral-like resolution , 1992 .

[15]  Tim Colonius,et al.  MODELING ARTIFICIAL BOUNDARY CONDITIONS FOR COMPRESSIBLE FLOW , 2004 .

[16]  Duck-Joo Lee,et al.  Implementation of boundary conditions for optimized high-order compact schemes , 1997 .

[17]  Miguel R. Visbal,et al.  On the use of higher-order finite-difference schemes on curvilinear and deforming meshes , 2002 .

[18]  W. Habashi,et al.  2N-Storage Low Dissipation and Dispersion Runge-Kutta Schemes for Computational Acoustics , 1998 .