Large eddy simulation of flow transition in a compressible flat-plate boundary layer at Mach 4.5

被引:2
|
作者
Shan, H [1 ]
Jiang, L [1 ]
Liu, C [1 ]
机构
[1] Louisiana Tech Univ, Coll Engn & Sci, Ctr Numer Simulat & Modeling, Ruston, LA 71272 USA
关键词
large eddy simulation; filtered structure function model; flat-plate boundary layer flow; flow transition; compressible flow Navier-Stokes equations; compact finite difference scheme;
D O I
10.1080/10618569908940888
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
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 number of M proportional to = 4.5 and a Reynolds number of 10,000 based on the free-stream velocity and inflow displacement thickness. The numerical simulation 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 direction and streamwise direction, the pseudo-spectral method is used in the spanwise direction. A compact storage third order Runge-Kutta scheme (Wray, 1986) is adopted for time-integration. The sub-grid scales are formulated according to the filtered structure function model (Ducros et ai.: 1996). A pair of oblique first-mode perturbation is imposed on the inflow boundary. Several stages of transition process can be identified, i.e., the linear and weak nonlinear growth of disturbance, the appearance of staggered Lambda-vortex pattern, the evolution of Lambda-vortex into hairpin vortex, and the break-down of hairpin vortical structures. The organized motions during the transition are discussed in detail. The vortical and the shear layer structures are compared with the results obtained by Adams and Kleiser (1996) in their direct numerical simulation based on a temporal approach. The evolution of the averaged quantities, such as the boundary layer thickness are studied. The skin friction coefficient and the turbulent mean velocity profile obtained from the simulation agree well with the Aat-plate theory of Van Driest (1956).
引用
收藏
页码:25 / 41
页数:17
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