Difference between revisions of "Sig Turbulence / Flow over Periodic Hills"
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== Motivation == | == Motivation == | ||
− | [[File: | + | [[File:Hilloutlined.jpg|thumb|Figure 1 : Periodic hill]] |
The flow over bodies with massive separation constitutes an important area of applications for LES. In many geometrie we can find this kind of flow like the 2D backward-facing step, the asymmetric diffuser or the periodic hill. We know experimental's data which was made by Almeida et al. [1] but in Mellen and al. [2] et Temmerman et al. [3] we can find that they have an influence of the side wall so the 1995 ERCOFTAC/IAHR workshop have cast a doubt on the true periodicity of the experimental configuration. But we have some data from LES with a good mesh like [[http://cfd.mace.manchester.ac.uk/cgi-bin/cfddb/prpage.cgi?81&LES&database/cases/case81/Case_data&database/cases/case81&cas81_head.html&cas81_desc.html&cas81_meth.html&cas81_data.html&cas81_refs.html&cas81_rsol.html&1&1&1&1&1&unknown]]. Flow over 2D periodic is in fact an experimental configuration with 9 hills. For the computational, we represent this configuration by a channel periodic with two half's hills like on the figure 1. | The flow over bodies with massive separation constitutes an important area of applications for LES. In many geometrie we can find this kind of flow like the 2D backward-facing step, the asymmetric diffuser or the periodic hill. We know experimental's data which was made by Almeida et al. [1] but in Mellen and al. [2] et Temmerman et al. [3] we can find that they have an influence of the side wall so the 1995 ERCOFTAC/IAHR workshop have cast a doubt on the true periodicity of the experimental configuration. But we have some data from LES with a good mesh like [[http://cfd.mace.manchester.ac.uk/cgi-bin/cfddb/prpage.cgi?81&LES&database/cases/case81/Case_data&database/cases/case81&cas81_head.html&cas81_desc.html&cas81_meth.html&cas81_data.html&cas81_refs.html&cas81_rsol.html&1&1&1&1&1&unknown]]. Flow over 2D periodic is in fact an experimental configuration with 9 hills. For the computational, we represent this configuration by a channel periodic with two half's hills like on the figure 1. | ||
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* With near-wall low | * With near-wall low | ||
* With the Spalding Low [4] | * With the Spalding Low [4] | ||
− | * | + | * With the Mahart et al. low [5] |
== Numerical results == | == Numerical results == | ||
+ | |||
+ | Results of the simulations are available in the paper written by Duprat et al. [6] | ||
== References == | == References == | ||
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[1] Almeida, Durao and Heitor, 1993, Experimental thermal and fluid science, Vol. 7, pp. 87-101. | [1] Almeida, Durao and Heitor, 1993, Experimental thermal and fluid science, Vol. 7, pp. 87-101. | ||
− | [2] [http://cfd.mace.manchester.ac.uk/ercoftac/database/cases/case81/Case_ref/IfH_paper.ps | + | [2] Mellen, Frohlich and Rodi, 2000, Large Eddy Simulation of the flow over periodic hills, 16th IMACS World Congress , Lausanne. [http://cfd.mace.manchester.ac.uk/ercoftac/database/cases/case81/Case_ref/IfH_paper.ps] |
− | [3] | + | [3] Temmerman and Leschziner, 2001, Large Eddy Simulation of separated flow in a streamwise periodic channel construction, Int. Symp. on Turbulence and Shear Flow Phenomena, Stockholm, June 27-29. [http://cfd.mace.manchester.ac.uk/ercoftac/database/cases/case81/Case_ref/TSFP2_09032001.ps] |
[4] Spalding, 1961, A single formula for the law of the wall, Jl. Appl. Mech., vol 28, pp. 455-457 | [4] Spalding, 1961, A single formula for the law of the wall, Jl. Appl. Mech., vol 28, pp. 455-457 | ||
− | [5] Manhart Peller and Brun, 2008, Near-wall scaling for turbulent boundary layers with adverse pressure gradient, Theor. Comput. Fluid Dyn., vol 22 , pp. 243-260. | + | [5] Manhart, Peller and Brun, 2008, Near-wall scaling for turbulent boundary layers with adverse pressure gradient, Theor. Comput. Fluid Dyn., vol 22 , pp. 243-260. |
+ | |||
+ | [6] Duprat, Balarac, Métais, Congedo, and Brugière, O., 2011, A wall-layer model for large-eddy simulations of turbulent flows with/out pressure gradient. Physics of Fluids, 23, 015101.[http://pof.aip.org/resource/1/phfle6/v23/i1/p015101_s1] | ||
Back to [[Sig Turbulence]] | Back to [[Sig Turbulence]] |
Latest revision as of 10:05, 5 November 2012
Olivier Brugiere, Universite Joseph Fourier, Grenoble, France
Contents
1 Motivation
The flow over bodies with massive separation constitutes an important area of applications for LES. In many geometrie we can find this kind of flow like the 2D backward-facing step, the asymmetric diffuser or the periodic hill. We know experimental's data which was made by Almeida et al. [1] but in Mellen and al. [2] et Temmerman et al. [3] we can find that they have an influence of the side wall so the 1995 ERCOFTAC/IAHR workshop have cast a doubt on the true periodicity of the experimental configuration. But we have some data from LES with a good mesh like [[1]]. Flow over 2D periodic is in fact an experimental configuration with 9 hills. For the computational, we represent this configuration by a channel periodic with two half's hills like on the figure 1.
The probleme of this flow is the separtion bubble which is due to a adverse pressure gradient that's why this is a test case for many subgrid scale models (SGS) and for near-wall low.
2 Testcase description
2.1 Flow configuration
2.1.1 Geometrical Parameters
- Hill's heigh :
- Streamwise distance :
- Normal wall heigh :
- Spanwise distance :
2.1.2 Boundary condition
- Streamwise condition : periodicity
- Spanwise condition : periodicity
- Normal to streamwise : two walls
2.2 Simulation details
We have make the geometry on Gambit Fig 2 and the mesh is composed by .
The aim of my study is testing a posteriori near-wall low. To compare we are running three cases :
- With near-wall low
- With the Spalding Low [4]
- With the Mahart et al. low [5]
3 Numerical results
Results of the simulations are available in the paper written by Duprat et al. [6]
4 References
[1] Almeida, Durao and Heitor, 1993, Experimental thermal and fluid science, Vol. 7, pp. 87-101.
[2] Mellen, Frohlich and Rodi, 2000, Large Eddy Simulation of the flow over periodic hills, 16th IMACS World Congress , Lausanne. [2]
[3] Temmerman and Leschziner, 2001, Large Eddy Simulation of separated flow in a streamwise periodic channel construction, Int. Symp. on Turbulence and Shear Flow Phenomena, Stockholm, June 27-29. [3]
[4] Spalding, 1961, A single formula for the law of the wall, Jl. Appl. Mech., vol 28, pp. 455-457
[5] Manhart, Peller and Brun, 2008, Near-wall scaling for turbulent boundary layers with adverse pressure gradient, Theor. Comput. Fluid Dyn., vol 22 , pp. 243-260.
[6] Duprat, Balarac, Métais, Congedo, and Brugière, O., 2011, A wall-layer model for large-eddy simulations of turbulent flows with/out pressure gradient. Physics of Fluids, 23, 015101.[4]
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