Analytic corrections to CFD heating predictions accounting for changes in surface catalysis

A new approach for combining the insight afforded by integral boundary-layer analysis with comprehensive (but time intensive) computational fluid dynamic (CFD) flowfield solutions of the thin-layer Navier-Stokes equations is described. The approach extracts CFD derived quantities at the wall and at the boundary layer edge for inclusion in a post-processing boundary-layer analysis. It allows a designer at a work-station to address two questions, given a single CFD solution. (1) How much does the heating change for a thermal protection system (TPS) with different catalytic properties than was used in the original CFD solution? (2) How does the heating change at the interface of two different TPS materials with an abrupt change in catalytic efficiency? The answer to the second question is particularly important, because abrupt changes from low to high catalytic efficiency can lead to localized increase in heating which exceeds the usually conservative estimate provided by a fully catalytic wall assumption. Capabilities of this approach for application to Reusable Launch Vehicle (RLV) design are demonstrated. If the definition of surface catalysis is uncertain early in the design process, results show that fully catalytic wall boundary conditions provide the best baseline for CFD design points.

[1]  G. Inger,et al.  Nonequilibrium Stagnation Point Boundary Layers with Arbitrary Surface Catalycity , 1963 .

[2]  P. A. Gnoffo,et al.  Point-implicit relaxation strategies for viscous, hypersonic flows , 1989 .

[3]  Aeroassisted Flight Experiment aerodynamic characteristics at flight conditions , 1990 .

[4]  George R. Inger,et al.  Nonequilibrium Boundary-Layer Effects on the Aerodynamic Heating of Hypersonic Waverider Vehicles , 1995 .

[5]  Peter A. Gnoffo,et al.  Navier-Stokes simulations of Orbiter aerodynamic characteristics including pitch trim and bodyflap , 1994 .

[6]  Paul Kolodziej,et al.  Thermal response of integral multicomponent composite thermal protection systems , 1985 .

[7]  J. Elder,et al.  Recombination-Dominated Nonequilibrium Heat Transfer to Arbitrarily Catalytic Hypersonic Vehicles , 1991 .

[8]  Peter Gnoffo,et al.  A code calibration program in support of the Aeroassist Flight Experiment , 1989 .

[9]  C. Angelopoulos High resolution schemes for hyperbolic conservation laws , 1992 .

[10]  R. Goulard,et al.  On Catalytic Recombination Rates in Hypersonic Stagnation Heat Transfer , 1958 .

[11]  Peter A. Gnoffo,et al.  Hypersonic entry heating with discontinuous surface catalycity - A combined analytic/CFD approach , 1996 .

[12]  Paul Kolodziej,et al.  Thermal response of integral multicomponent composite thermal protection systems , 1986 .

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

[14]  Peter A. Gnoffo,et al.  Multiblock analysis for Shuttle Orbiter reentry heating from Mach 24 to Mach 12 , 1994 .

[15]  P. Gnoffo An upwind-biased, point-implicit relaxation algorithm for viscous, compressible perfect-gas flows , 1990 .

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

[17]  Peter A. Gnoffo,et al.  Application of the LAURA code for slender-vehicle aerothermodynamics , 1992 .