Large-Eddy Simulation of Transition to Turbulence in Boundary Layers
Author(s) -
Xiulan Huai,
R. D. Joslin,
Ugo Piomelli
Publication year - 1997
Publication title -
theoretical and computational fluid dynamics
Language(s) - English
Resource type - Journals
eISSN - 1432-2250
pISSN - 0935-4964
DOI - 10.1007/s001620050037
Subject(s) - turbulence , laminar flow , large eddy simulation , reynolds averaged navier–stokes equations , mechanics , instability , intermittency , physics , boundary layer , direct numerical simulation , nonlinear system , statistical physics , navier–stokes equations , vortex , mathematics , reynolds number , compressibility , quantum mechanics
Large-eddy simulation (LES) results for laminar-to-turbulent transition in a spatially developing boundary layer are presented. The disturbances are ingested into a laminar flow through an unsteady suction-and- blowing strip. The filtered, three-dimensional time-dependent Navier-Stokes equations are integrated numerically using spectral, high-order finite-differences, and a three-stage low-storage Runge- Kutta/Crank-Nicolson time-advancement method. The buffer-domain technique is used for the outflow boundary condition. The localized dynamic model used to parametrize the subgrid-scale (SGS) stresses begins to have a significant impact at the beginning of the nonlinear transition (or intermittency) region. The flow structures commonly found in experiments are also observed in the present simulation; the computed linear instability modes and secondary instability lambda- vortex structures are in agreement with the experiments, and the streak-like structures and turbulent statistics compare with both the experiments and theory. The physics captured in the present LES are consistent with the experiments and the full Navier-Stokes simulation (DNS), at a signficant fraction of the DNS cost. A comparison of the results obtained with several SGS models shows that the localized model gives accurate results both in a statistical sense and in terms of predicting the dynamics of the energy- carrying eddies, while requiring fewer ad hoc adjustments than the other models.
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