The full, three-dimensional Favre-averaged Navier-Stokes equations, coupled
with the second-order Zhang et al. (Zhang, H., So, R., Gatski, T., and Spe
ziale, C.,"A Near-Wall Second-Order Closure for Compressible Turbulent Flow
s," Near-Wall Turbulent Flows, edited by R. So, C. Speziale, and a. Launder
, Elsevier, New York, 1993, ppt 209-218) Reynolds-stress turbulence and K-e
psilon models, were used to numerically simulate a 25 deg, Mach 1.8 injecti
on into a Mach 3.0 crossflow. Detailed comparisons with experimental data w
ere performed. Analysis of the Reynolds-stress turbulence model simulation
results revealed physically consistent and accurate predictions for mean fl
ow and turbulent quantities, whereas the simulations with the K-epsilon mod
el resulted in nonphysical and inconsistent turbulence predictions. Analysi
s of the three-dimensional flowfield simulation with the Reynolds-stress tu
rbulence model shows that the shock structure downstream of the oblique bar
rel shock was a mirrored Image of the leeward side of the oblique barrel sh
ock. Furthermore, the downstream location where vortical motion was initiat
ed in the jet plume was caused by the recompression shock-induced vortices.
These vortices were generated through the combined effects of the inflow a
ir upwash behind the plume and the mirrored oblique barrel shock.