Large-eddy simulation of a compressible flow past a deep cavity
By L. Larchevêque, Pierre Sagaut, I. Mary, O. Labbé, P. Comte. 2003
234 citations recorded by the source corpus.
Subfields: Computational Mechanics, Environmental Engineering
View Paper: https://www.semanticscholar.org/paper/2d3feca128d2b9e4e80af2d56b4b3677f16a709e
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In Computational Mechanics
- Tim Colonius
- G. Brès
- Sanjiva K. Lele
- Pierre Sagaut
- Sébastien Deck
- L. Jacquin
- N. Chauvet
- L. Larchevêque
In Environmental Engineering
Citations in the corpus
- Analysis of the flow and mass transfer processes for the incompressible flow past an open cavity with a laminar and a fully turbulent incoming boundary layer (2006, methodology): “The momentum thickness growth rate is around 0.01 for x/D < 0.7 and close to 0.036 for 1 < x/D < 1.7 which is within the typical range (0.03–0.04) expected for turbulent incoming boundary layers (Gloerfelt et al. 2002; Larcheveque et al. 2003, 2004; Forestier et al. 2003).”
- Computational aeroacoustics: progress on nonlinear problems of sound generation (2004, methodology): “[403] Larchevêque L, Sagaut P, Mary I, Labbe O, Comte P.”
- The mixing layer over a deep cavity at high-subsonic speed (2003, methodology): “This would concern the formation of structure S3 (see Larchevêque et al. 2003).”
- Zonal Detached Eddy Simulation of a Controlled Propulsive Jet (2007, methodology): “This well-tried solver has been notably used to compute a LES of the flow over a cavity at highReynolds number [25], a zonal DES of transonic buffet over a supercritical airfoil [14], a zonal DES of the flow around a high-lift configuration [15], several hybrid RANS/LES of supersonic base flows [26]”
- Large-eddy simulation of a compressible flow in a three-dimensional open cavity at high Reynolds number (2004, methodology): “As a conclusion, it is possible to state that grid convergence for the flow (in an LES sense) is reached.”
- Three-dimensional instabilities in compressible flow over open cavities (2008, result): “These results are of the same order as the spreading rates measured in experiments (Sarohia 1975) and numerical simulations (Rowley et al. 2002; Larchevêque et al. 2003).”