A further study of numerical errors in large-eddy simulations
By Fotini K. Chow, Parviz Moin. 2003
278 citations recorded by the source corpus.
Subfields: Atmospheric Science, Computational Mechanics
View Paper: https://www.semanticscholar.org/paper/fe714d61a7da68c30d4f3a8fc102bdda4fd3f86c
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atmospheric Science
- E. Patton
- Markus Klein
- Ming Xue
- Joel H. Ferziger
- Robert L. Street
- Heinz Pitsch
- Guillaume Blanquart
- Olivier Desjardins
In Computational Mechanics
- Olivier Desjardins
- Heinz Pitsch
- E. Taşkinoğlu
- Robert L. Street
- Markus Klein
- E. Patton
- Guillaume Blanquart
- Joel H. Ferziger
Citations in the corpus
- An Attempt to Assess the Quality of Large Eddy Simulations in the Context of Implicit Filtering (2005, result): “[ 5 , 6]. Also Ribault et al. [25] report similar findings for a plane jet.”
- Explicit Filtering and Reconstruction Turbulence Modeling for Large-Eddy Simulation of Neutral Boundary Layer Flow (2005, methodology): “In addition, there are errors due to aliasing effects, though these are not as important in finite-difference as in spectral codes (Chow and Moin 2003).”
- The Effect of Mesh Resolution on Convective Boundary Layer Statistics and Structures Generated by Large-Eddy Simulation (2011, background): “discretization errors are intertwined since both depend explicitly on the mesh spacing (Chow and Moin 2003; Meyers et al. 2007; Geurts and Fröhlich 2002).”
- A posteriori study using a DNS database describing fluid disintegration and binary-species mixing under supercritical pressure: heptane and nitrogen (2010, background): “For a sixth-order Padé scheme, this ratio must be ̄ 2 xLES (Ghosal 1996; Chow & Moin 2003), and the present choice is ̄ = 2 xLES , meaning that the smallest resolved eddy is represented by at least two grid points.”
- High order conservative finite difference scheme for variable density low Mach number turbulent flows (2007, methodology): “In order to further analyze the a priori properties of these schemes, the study of aliasing errors proposed by Kravchenko and Moin [2] is extended here to include the fourth and sixth order schemes.”