Large eddy simulation (LES) has been carried out to investigate the oblique
transition process of a flat-plate boundary layer at a free-stream Mach nu
mber of M proportional to = 4.5 and a Reynolds number of 10,000 based on th
e free-stream velocity and inflow displacement thickness. The numerical sim
ulation is performed using a spatial approach to solve a full compressible
Navier-Stokes system in the curvilinear coordinates. A compact sixth-order
central difference scheme (Lele, 1992) is applied to the wall-normal direct
ion and streamwise direction, the pseudo-spectral method is used in the spa
nwise direction. A compact storage third order Runge-Kutta scheme (Wray, 19
86) is adopted for time-integration. The sub-grid scales are formulated acc
ording to the filtered structure function model (Ducros et ai.: 1996). A pa
ir of oblique first-mode perturbation is imposed on the inflow boundary. Se
veral stages of transition process can be identified, i.e., the linear and
weak nonlinear growth of disturbance, the appearance of staggered Lambda-vo
rtex pattern, the evolution of Lambda-vortex into hairpin vortex, and the b
reak-down of hairpin vortical structures. The organized motions during the
transition are discussed in detail. The vortical and the shear layer struct
ures are compared with the results obtained by Adams and Kleiser (1996) in
their direct numerical simulation based on a temporal approach. The evoluti
on of the averaged quantities, such as the boundary layer thickness are stu
died. The skin friction coefficient and the turbulent mean velocity profile
obtained from the simulation agree well with the Aat-plate theory of Van D
riest (1956).