The multiscale formulation of large eddy simulation: Decay of homogeneous isotropic turbulence

By Thomas J. R. Hughes, Luca Mazzei, A. Oberai, Alan A. Wray. 2001

453 citations recorded by the source corpus.

Subfields: Computational Mechanics, Computational Theory and Mathematics

View Paper: https://www.semanticscholar.org/paper/26f3129085e9d58a7b6ceb159c4e91c5a3021191

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Computational Mechanics

1. Sanjiva K. Lele
2. Meng Wang
3. Jonathan B. Freund
4. J. Tinsley Oden
5. Serge Prudhomme
6. Robert L. Street
7. Joel H. Ferziger
8. Ming Xue

In Computational Theory and Mathematics

1. Serge Prudhomme
2. J. Tinsley Oden
3. Traian Iliescu
4. Joel H. Ferziger
5. Zhu Wang
6. Sanjiva K. Lele
7. Jeff Borggaard
8. Imran Akhtar

Citations in the corpus

• Explicit Filtering and Reconstruction Turbulence Modeling for Large-Eddy Simulation of Neutral Boundary Layer Flow (2005, methodology): “To facilitate our understanding of the requirements in SFS modeling and especially to improve turbulence models in the near-wall region, it is useful to consider velocity partitioning schemes such as those of Carati et al. (2001), Zhou et al. (2001), and Hughes et al. (2001a,b .”
• COMPUTATIONAL PREDICTION OF FLOW-GENERATED SOUND (2006, methodology): “Other popular SGS models include the scale similarity model (Bardina et al. 1983) and mixed models, approximate deconvolution model (Stolz & Adams 1999), and multiscale LES (Hughes et al. 2001), to name a few.”
• Variational Multiscale Analysis: the Fine-scale Green's Function, Projection, Optimization, Localization, and Stabilized Methods (2007, unknown): “, [11,12,15–17] for application to turbulence modeling).”
• Navier–Stokes Equations with Shear Thinning Viscosity. Regularity up to the Boundary (2009, result): “In order to avoid additional calculations we assume that p ≤ 3. However, this restriction is not at all necessary, in the sense that, basically, the same argument gives similar results for p > 3. The case 2 ≤ p ≤ 3 (specially p = 3) has been applied in the last forty years to model turbulence phenom”
• Mathematical Perspectives on Large Eddy Simulation Models for Turbulent Flows (2004, background): “From numerical tests reported in [31, 33], it is unclear which form of νt performs the best, but from the approximation point of view, we note that in the regions where the solution is smooth, the first form of the subgrid term is O(Hk+1), which is exactly the order of the consistency error of the a”