Simulation of Stagnation Region Heating in Hypersonic Flow on Tetrahedral Grids

Hypersonic flow simulations using the node based, unstructured grid code FUN3D are presented. Applications include simple (cylinder) and complex (towed ballute) configurations. Emphasis throughout is on computation of stagnation region heating in hypersonic flow on tetrahedral grids. Hypersonic flow over a cylinder provides a simple test problem for exposing any flaws in a simulation algorithm with regard to its ability to compute accurate heating on such grids. Such flaws predominantly derive from the quality of the captured shock. The importance of pure tetrahedral formulations are discussed. Algorithm adjustments for the baseline Roe / Symmetric, Total-Variation-Diminishing (STVD) formulation to deal with simulation accuracy are presented. Formulations of surface normal gradients to compute heating and diffusion to the surface as needed for a radiative equilibrium wall boundary condition and finite catalytic wall boundary in the node-based unstructured environment are developed. A satisfactory resolution of the heating problem on tetrahedral grids is not realized here; however, a definition of a test problem, and discussion of observed algorithm behaviors to date are presented in order to promote further research on this important problem.

[1]  Graham V. Candler,et al.  CFD Validation for Hypersonic Flight: Hypersonic Double-Cone Flow Simulations , 2002 .

[2]  Timothy J. Barth Some notes on shock resolving flux functions. Part 1: Stationary characteristics , 1989 .

[3]  G. Candler,et al.  Data-Parallel Line Relaxation Method for the Navier -Stokes Equations , 1998 .

[4]  Peter A. Gnoffo,et al.  Aerothermodynamic Analyses of Towed Ballutes , 2006 .

[5]  J. A. White,et al.  A Psuedo-Temporal Multi-Grid Relaxation Scheme for Solving the Parabolized Navier-Stokes Equations , 1999 .

[6]  J. Quirk A Contribution to the Great Riemann Solver Debate , 1994 .

[7]  Reuben R. Rohrschneider,et al.  Ultra Lightweight Ballutes for Return to Earth from the Moon , 2006 .

[8]  Ami Harten,et al.  Self adjusting grid methods for one-dimensional hyperbolic conservation laws☆ , 1983 .

[9]  Cheatwood F. McNeil,et al.  User''s Manual for the Langley Aerothermodynamic Upwind Relaxation Algorithm (LAURA) , 1996 .

[10]  Timothy J. Barth,et al.  The design and application of upwind schemes on unstructured meshes , 1989 .

[11]  H. C. Yee,et al.  On symmetric and upwind TVD schemes , 1985 .

[12]  Douglas J. Quattrochi,et al.  Hypersonic heat transfer and anisotropic visualization with a higher order discontinuous Galerkin finite element method , 2006 .

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

[14]  J. L. Hall,et al.  Aerocapture trajectories for spacecraft with large, towed ballutes , 2001 .

[15]  P. Roe Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .

[16]  Peter A. Gnoffo,et al.  Computational Aerothermodynamic Simulation Issues on Unstructured Grids , 2004 .

[17]  Peter A. Gnoffo,et al.  Computational Fluid Dynamics Technology for Hypersonic Applications , 2003 .

[18]  Graham V. Candler,et al.  Development of a hybrid unstructured implicit solver for the simulation of reacting flows over complex geometries , 2004 .

[19]  Peter A. Gnoffo Conservation equations and physical models for hypersonic air flows over the aeroassist flight experiment vehicle , 1989 .

[20]  Peter A. Gnoffo,et al.  Paper 2001-1025 CFD Validation Studies for Hypersonic Flow Prediction , 2022 .

[21]  Peter A. Gnoffo,et al.  Conservation equations and physical models for hypersonic air flows in thermal and chemical nonequilibrium , 1989 .

[22]  Jean-Marc Moschetta,et al.  Shock wave instability and the carbuncle phenomenon: same intrinsic origin? , 2000, Journal of Fluid Mechanics.

[23]  Jeffery L. Hall A REVIEW OF BALLUTE TECHNOLOGY FOR PLANETARY AEROCAPTURE , 2000 .