Direct numerical simulation and large-eddy simulation of wake vortices : going from laboratory conditions to flight conditions

This paper aims at presenting DNS and LES as applied to the simulation of vortex wakes: in laboratory conditions (moderate to medium Reynolds numbers) and up to real aircraft conditions (high to very high Reynolds numbers). Only incompressible ∞ows are considered. DNS and LES are able to capture complex 3-D physics provided one uses high quality numerical methods: methods with negligible numerical dissipation (i.e., methods that conserve energy in absence of viscosity and/or subgrid modelling) and with low dispersion errors (to properly transport complex vortical structures). Methods that can do that are: spectral methods, high order flnite difierence methods, and vortex-in-cell (VIC) methods. As the problems of interest are of large spatial extent and contain vortices with small cores, it is also essential that the methods be e-ciently parallelized. As to LES of wake vortex ∞ows, this require subgrid scale (SGS) models that are essentially inactive during the gentle, well-resolved, phases of the ∞ow and within the vortex cores, and that become active only during the complex turbulent phases of the ∞ow. The recent multiscale models, that act solely on the high wavenumbers modes of the LES, are seen to be most appropriate. We present some illustrative examples of DNS and LES results that were obtained within our group.

[1]  Thomas J. R. Hughes,et al.  Large eddy simulation of turbulent channel flows by the variational multiscale method , 2001 .

[2]  Grégoire Winckelmans,et al.  Vortex methods and their application to trailing wake vortex simulations , 2005 .

[3]  F. Nicoud,et al.  Subgrid-Scale Stress Modelling Based on the Square of the Velocity Gradient Tensor , 1999 .

[4]  Leonhard Kleiser,et al.  High-pass filtered eddy-viscosity models for large-eddy simulations of transitional and turbulent flow , 2005 .

[5]  M. Lesieur,et al.  Large-eddy simulation of transition to turbulence in a boundary layer developing spatially over a flat plate , 1996, Journal of Fluid Mechanics.

[6]  Donald B. Bliss,et al.  The instability of short waves on a vortex ring , 1974, Journal of Fluid Mechanics.

[7]  Charles H. K. Williamson,et al.  Cooperative elliptic instability of a vortex pair , 1998, Journal of Fluid Mechanics.

[8]  David Fabre,et al.  Optimal perturbations in a four-vortex aircraft wake in counter-rotating configuration , 2002, Journal of Fluid Mechanics.

[9]  Fred H. Proctor,et al.  Wake Vortex Transport and Decay in Ground Effect: Vortex Linking with the Ground , 2000 .

[10]  John C. LaRue,et al.  The decay power law in grid-generated turbulence , 1990, Journal of Fluid Mechanics.

[11]  G. S. Winckelmans,et al.  Comparison of recent dynamic subgrid-scale models in turbulent channel flow , .

[12]  Thomas J. R. Hughes,et al.  The multiscale formulation of large eddy simulation: Decay of homogeneous isotropic turbulence , 2001 .

[13]  B. Geurts,et al.  Direct and large-eddy simulation IV , 2001 .

[14]  Laurent Bricteux,et al.  Simulation of three-dimensional wake vortices in ground effect with a fourth order incompressible code , 2006 .

[15]  Daniel W. Meyer,et al.  High-Pass Filtered Eddy-Viscosity Models for LES , 2004 .

[16]  Hervé Jeanmart,et al.  Assessment of some models for LES without/with explicit filtering , 2001 .

[17]  A. W. Vreman The filtering analog of the variational multiscale method in large-eddy simulation , 2003 .

[18]  Grégoire Winckelmans,et al.  Investigation of multiscale subgrid models for LES of instabilities and turbulence in wake vortex systems , 2007 .

[19]  Oleg V. Vasilyev High Order Finite Difference Schemes on Non-uniform Meshes with Good Conservation Properties , 2000 .

[20]  Cooperative elliptic instability of a vortex pair , 1998 .

[21]  Saad A. Ragab,et al.  The three-dimensional interaction of a vortex pair with a wall , 1997 .