Titlebook: Direct and Large-Eddy Simulation III; Proceedings of the I Peter R. Voke,Neil D. Sandham,Leonhard Kleiser Conference proceedings 1999 Sprin

extrovert

Vo2-Max

Norbert Lindlein Ph.D.,Gerd Leuchs Prof.rugation. Even with such a requirement, LES reduces dramatically the computational effort necessary to simulate the shock/homogeneous turbulence interaction with respect to DNS. Dynamic SGS models are found to improve markedly the quality of the results when compared to simple models like Smagorinsky’s.

爱国者

Sune Svanberg,Wolfgang Demtrödergrid scale models such as the standard or the dynamic Smagorinsky model. The computational overhead of the ADM is similar to that of the scale-similarity model and is considerably less than that of dynamic models or the velocity estimation model.

诱骗

DOLT

GLIB

modish

Large-Eddy Simulation of Shock/Homogeneous Turbulence Interaction,rugation. Even with such a requirement, LES reduces dramatically the computational effort necessary to simulate the shock/homogeneous turbulence interaction with respect to DNS. Dynamic SGS models are found to improve markedly the quality of the results when compared to simple models like Smagorinsky’s.

Robust

The Approximate Deconvolution Model Applied to LES of Turbulent Channel Flow,grid scale models such as the standard or the dynamic Smagorinsky model. The computational overhead of the ADM is similar to that of the scale-similarity model and is considerably less than that of dynamic models or the velocity estimation model.

GEM

Deconvolution of Subgrid-Scales for the Simulation of Shock-Turbulence Interaction,proach is based on an expansion of the filtered field in terms of filter width, which is modified in the vicinity of discontinuities in order to exactly recover the filtered profile. We detail both approaches and investigate their feasibility for the inviscid Burgers equation, isothermal and full Euler equations.

eardrum

Exact Expansions for Filtered-Scales Modelling with a Wide Class of LES Filters,namics. An approximation of this expansion is also derived for filters with a compact support in Fourier space. In this case, the filtered-scale can be decomposed into two parts corresponding respectively to reversible and irreversible effects.