COVOLUME-DUAL VARIABLE METHOD FOR THERMALLY EXPANDABLE FLOW ON UNSTRUCTURED TRIANGULAR GRIDS

SUMMARY Finite difference like discretizations are developed for the time dependent Navier-Stokes equations and the thermal energy equation. The flow is assumed to be thermally expandable, that is, the density varies only with temperature. A new pointwise first order upwind scheme for convection is presented which is of nonnegative type. Also presented are new approaches to reconstructing the velocity vector field from the covolume primitive variables. The resulting difference equations reproduce linear flow fields.

[1]  T. A. Porsching,et al.  Numerical simulation of confined unsteady aerodynamical flows , 1987 .

[2]  Claude Berge,et al.  Programming, games and transportation networks , 1966 .

[3]  D. F. Watson Computing the n-Dimensional Delaunay Tesselation with Application to Voronoi Polytopes , 1981, Comput. J..

[4]  W. Frey Selective refinement: A new strategy for automatic node placement in graded triangular meshes , 1987 .

[5]  R. A. Nicolaides,et al.  Flow discretization by complementary volume techniques , 1989 .

[6]  R. H. MacNeal,et al.  An asymmetrical finite difference network , 1953 .

[7]  W. Y. Soh,et al.  Time-Dependent viscous incompressible Navier-Stokes equations: the finite difference Galerkin formulation and streamfunction algorithms , 1989 .

[8]  T. Taylor,et al.  Computational methods for fluid flow , 1982 .

[9]  T. A. Porsching,et al.  A network method for homogeneous, thermally expandable two-phase flow on unstructured triangular grids , 1994 .

[10]  Robin Sibson,et al.  Locally Equiangular Triangulations , 1978, Comput. J..

[11]  T. A. Porsching,et al.  DUVAL: a computer program for the numerical solution of two-dimensional, two-phase flow problems. Final report , 1982 .

[12]  R. Nicolaides Direct discretization of planar div-curl problems , 1992 .

[13]  T. A. Porsching,et al.  ON A NETWORK METHOD FOR UNSTEADY INCOMPRESSIBLE FLUID FLOW ON TRIANGULAR GRIDS , 1992 .

[14]  T. Porsching,et al.  Numerical Analysis of Partial Differential Equations , 1990 .

[15]  John W. Goodrich,et al.  Unsteady solution of incompressible Navier-Stokes equations , 1988 .

[16]  T. S. Lee,et al.  Laminar fluid convection between concentric and eccentric heated horizontal rotating cylinders for low‐Prandtl‐number fluids , 1992 .

[17]  A. B. Stephens,et al.  A finite difference galerkin formulation for the incompressible Navier-Stokes equations☆ , 1984 .

[18]  C. Hall Numerical Solution of Navier–Stokes Problems by the Dual Variable Method , 1985 .

[19]  D. Ewing,et al.  Rules governing the numbers of nodes and elements in a finite element mesh , 1970 .

[20]  James C. Cavendish,et al.  SOLUTION OF INCOMPRESSIBLE NAVIER‐STOKES EQUATIONS ON UNSTRUCTURED GRIDS USING DUAL TESSELLATIONS , 1992 .

[21]  John Burkardt,et al.  The dual variable method for the solution of compressible fluid flow problems , 1986 .

[22]  T. Porsching A network model for two‐fluid, two‐phase flow , 1985 .

[23]  T. Porsching A Finite Difference Method for Thermally Expandable Fluid Transients , 1977 .

[24]  Karl Gustafson,et al.  Graph Theory and Fluid Dynamics , 1985 .

[25]  T. Porsching,et al.  An application of network' theory to the solution of implicit Navier-Stokes difference equations , 1981 .

[26]  J. Cavendish,et al.  The dual variable method for solving fluid flow difference equations on Delaunay triangulations , 1991 .

[27]  F. Harlow,et al.  Numerical Calculation of Time‐Dependent Viscous Incompressible Flow of Fluid with Free Surface , 1965 .