Abstract

Large eddy simulations (LES) of low-speed, wall-bounded turbulent flows were conducted by numerically integrating the compressible Navier-Stokes equations in a generalized curvilinear coordinate system. An ecient numerical scheme based on a third-order additive semi-implicit Runge-Kutta method for time advancement and a sixth-order accurate, compact finite-dierence scheme for spatial discretization were used. The convective terms in the wall-normal direction were treated implicitly to remove the time-step limitation associated with the use of fine meshes in the near-wall region for high Reynolds number viscous flows. The dynamic Smagorinsky subgrid-scale eddy viscosity model was used to close the filtered equations. Generalized characteristic-based nonreflecting boundary conditions were used together with an exit zone featuring grid stretching and enhanced damping. The accuracy and eciency of the numerical scheme was assessed by a simple model acoustic problem and by comparing LES predictions for fully-developed turbulent channel flow and turbulent separated flow in an asymmetric diuser to previous direct numerical simulation (DNS) and experimental data, respectively. LES predictions for both flows were in reasonable agreement with the DNS and experimental mean velocity and turbulence statistics. The findings suggest that the numerical approach employed here oers comparable accuracy to similar recent studies at approximately one-third of the computational cost and may provide both an accurate and ecient way to conduct computational aeroacoustics studies for low Mach number, confined turbulent flows.

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