Simulations of a shock emanating from a compression corner and interacting with a fully developed turbulent boundary layer are evaluated herein. Mission-relevant conditions at Mach 7 and Mach 14 are defined for a precompression ramp of a scramjet-powered vehicle. Two compression angles are defined: the smallest to avoid separation losses and the largest to force higher temperature flow physics. The Baldwin-Lomax and the CebeciSmith algebraic models, the one-equation Spalart-Allmaras model with the Catrix-Aupoix compressibility modification, and two-equation models, including the Menter shear stress transport model and the Wilcox k-! 98 and k-! 06 turbulence models, are evaluated. Comparisons are made to existing experimental data and Van Driest theory to provide preliminary assessment of model-form uncertainty. A set of coarse-grained uncertainty metrics are defined to capture essential differences among turbulence models. There is no clearly superior model as judged by these metrics. A preliminary metric for the numerical component of uncertainty in shockturbulent-boundary-layer interactions at compression corners sufficiently steep to cause separation is defined as 55%. This value is a median of differences with experimental data averaged for peak pressure and heating and for extent of separation captured in new grid-converged solutions presented here. Nomenclature c = speed of sound, m=s E = metric of difference between computation and experiment e = static energy, J=kg f = dummy variable for p, q, or H = total enthalpy, J=kg k = turbulent kinetic energy, J=kg L = separation length, m M = Mach number M t = turbulence Mach number, 2k p =c M t0 = critical value of turbulence Mach number used in compressibility correction M = Mach number based on friction velocity, u =c w P = production term in turbulent kinetic energy equation Pr t = turbulent Prandtl number p = pressure, N=m 2 q = heat transfer rate, W=m 2 Re = momentum thickness Reynolds number Re = incompressible momentum thickness Reynolds number T = temperature, K U = u=u , dimensionless velocity u = velocity, m=s u i , u j = velocity component in i and j directions, respectively, m=s u = friction velocity, w = w p V = velocity in freestream, m=s x = distance along wall (flat plate), coordinate in streamwise direction, m x i , x j = coordinates in i and j directions, respectively, m y = distance normal to wall (flat plate), coordinate orthogonal to x, m y = u y=, normalized distance (flat plate) = angle of attack = viscosity, kg=m s = density, kg=m 3 = shear, N=m 2 ij = Reynolds stress tensor k = @u k 1 =@x k1 @u k1 =@x k 1 Subscripts conv = convective e = at edge of boundary layer i = component in i direction j = component in j direction t = turbulent value w = conditions at wall 1 = reference condition in freestream