Euler and Navier-Stokes leeside flows over supersonic delta wings

Numerical simulations of several distinctly different types of leeside flowfields over higly swept, sharp, leading-edge delta wings in supersonic flow were obtained using Euler and Navier-Stokes solvers. The Euler code was seen to be adequate for predicting primary flow structures (leading-edge vortex and crossflow shock), whereas the Navier-Stokes code was capable of predicting primary and secondary flow structures (i.e., secondary vortex and shock-induced separation). A comparison of laminar and turbulent Navier-Stokes solutions for leading-edge separated flows for which the boundary-layer state was known indicated that the turbulent boundary-layer model is more accurate in predicting the effect of the boundary layer on the flowfield. Also, for several cases, the Navier-Stokes code indicated detailed flow structures not observed in the qualitative experimental data available.

[1]  William H. Mason,et al.  Supersonic, nonlinear, attached-flow wing design for high lift with experimental validation , 1984 .

[2]  C. E. Lan,et al.  VORCAM: A computer program for calculating vortex lift effect of cambered wings by the suction analogy , 1981 .

[3]  R. Sorenson A computer program to generate two-dimensional grids about airfoils and other shapes by the use of Poisson's equation , 1980 .

[4]  W. K. Anderson,et al.  Comparison of Finite Volume Flux Vector Splittings for the Euler Equations , 1985 .

[5]  Richard M. Wood,et al.  Comparison of computations and experimental data for leading edge vortices - Effects of yaw and vortex flaps , 1986 .

[6]  C. E. Brown,et al.  THEORETICAL AND EXPERIMENTAL STUDIES OF CAMBERED AND TWISTED WINGS OPTIMIZED FOR FLIGHT AT SUPERSONIC SPEEDS , 1962 .

[7]  James L. Thomas,et al.  Navier-Stokes computations of lee-side flows over delta wings , 1986 .

[8]  Veer N. Vatsa,et al.  Navier-Stokes computations of prolate spheroids at angle of attack , 1987 .

[9]  R. M. Wood,et al.  Leeside flows over delta wings at supersonic speeds , 1984 .

[10]  M. S. Adams,et al.  Numerical simulation of vortical flow over an elliptical-body missile at high angles of attack , 1986 .

[11]  L. B. Schiff,et al.  Computation of supersonic viscous flows around pointed bodies at large incidence , 1983 .

[12]  A. Stanbrook,et al.  Possible Types of Flow at Swept Leading Edges , 1964 .

[13]  David S. Miller,et al.  Comparison of experimental and numerical results for delta wings with vortex flaps , 1986 .

[14]  Arthur Rizzi,et al.  Computation of inviscid incompressible flow with rotation , 1985, Journal of Fluid Mechanics.

[15]  J. N. Hefner,et al.  Lee-surface vortex effects over configurations in hypersonic flow. , 1972 .

[16]  Philip L. Roe,et al.  A comparison of numerical flux formulas for the Euler and Navier-Stokes equations , 1987 .

[17]  K. Fujii,et al.  Numerical simulation of the viscous flow fields over three-dimensional complicated geometries , 1984 .

[18]  F. G. Blottner,et al.  Variable grid scheme applied to turbulent boundary layers , 1974 .

[19]  Earll M. Murman,et al.  High Resolution Solutions of the Euler Equations for Vortex Flows , 1985 .

[20]  Earll M. Murman,et al.  Total pressure loss in vortical solutions of the conical Euler equations , 1985 .

[21]  J. S. Shang,et al.  Numerical simulation of leading-edge vortex flows , 1984 .

[22]  R. L. Sorenson,et al.  Automatic mesh-point clustering near a boundary in grid generation with elliptic partial differential equations , 1979 .

[23]  Kenneth G. Powell Vortical solutions of the conical Euler equations , 1987 .