Large-eddy simulation and wall modelling of turbulent channel flow
By D. Chung, Dale I. Pullin. Journal of Fluid Mechanics, 2009
150 citations recorded by the source corpus.
Subfields: Computational Mechanics, Environmental Engineering, Mechanical Engineering
View Paper: https://www.semanticscholar.org/paper/d5a39547f125affa9d372961b6ecff278dedb96e
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
- B. McKeon
- Ivan Marusic
- Philipp Schlatter
- Alexander J Smits
- Nicholas Hutchins
- Javier Jiménez
- Ramis Örlü
- Ati S. Sharma
In Environmental Engineering
- B. McKeon
- Philipp Schlatter
- Ivan Marusic
- Alexander J Smits
- Ramis Örlü
- D. Chung
- Dan S. Henningson
- Nicholas Hutchins
In Mechanical Engineering
- Ivan Marusic
- B. McKeon
- Alexander J Smits
- Philipp Schlatter
- Dan S. Henningson
- Haecheon Choi
- Jungil Lee
- Hyungmin Park
Citations in the corpus
- Simulations of Spatially Evolving Turbulent Boundary Layers up to Reθ = 4300 (2010, methodology): “hybrid approaches such as detached-eddy simulation (DES, Spalart (2009)), or specific near-wall SGS models (Chung and Pullin, 2009).”
- Aerodynamics of Heavy Vehicles (2014, methodology): “…promising WMLES approach is to perform LES with the wall shear stress as the boundary condition at the wall (instead of the no-slip condition) without resolving the near-wall region (Chung & Pullin 2009, Kawai & Larsson 2012, Lee et al. 2013, Nicoud et al. 2001, Schumann 1975, Wang & Moin 2002).”
- High–Reynolds Number Wall Turbulence (2011, background): “In this respect, large-eddy simulation of ABLs may prove to be particularly interesting, as it is always confronted with the physics of high–Reynolds number flows (e.g., see Khanna & Brasseur 1997, 1998; Bou-Zeid et al. 2005, 2008; Chung & Pullin 2009).”
- Large-eddy simulation of large-scale structures in long channel flow (2010, methodology): “To circumvent the inhibitive cost of resolving the near-wall region (Chapman 1979), z h0, we use a wall model (Chung & Pullin 2009) that supplies off-wall slip-velocity boundary conditions at h0 to the interior LES, operating in h0 z 2δ − h0, where z = 0, 2δ locates the walls.”