Using singular values to build a subgrid-scale model for large eddy simulations
An eddy-viscosity based, subgrid-scale model for large eddy simulations is derived from the analysis of the singular values of the resolved velocity gradient tensor. The proposed σ-model has, by construction, the property to automatically vanish as soon as the resolved field is either two-dimensiona...
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Veröffentlicht in: | Physics of fluids (1994) 2011-08, Vol.23 (8), p.085106-085106-12 |
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container_title | Physics of fluids (1994) |
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creator | Nicoud, Franck Toda, Hubert Baya Cabrit, Olivier Bose, Sanjeeb Lee, Jungil |
description | An eddy-viscosity based, subgrid-scale model for large eddy simulations is derived from the analysis of the singular values of the resolved velocity gradient tensor. The proposed σ-model has, by construction, the property to automatically vanish as soon as the resolved field is either two-dimensional or two-component, including the pure shear and solid rotation cases. In addition, the model generates no subgrid-scale viscosity when the resolved scales are in pure axisymmetric or isotropic contraction/expansion. At last, it is shown analytically that it has the appropriate cubic behavior in the vicinity of solid boundaries without requiring any ad-hoc treatment. Results for two classical test cases (decaying isotropic turbulence and periodic channel flow) obtained from three different solvers with a variety of numerics (finite elements, finite differences, or spectral methods) are presented to illustrate the potential of this model. The results obtained with the proposed model are systematically equivalent or slightly better than the results from the Dynamic Smagorinsky model. Still, the σ-model has a low computational cost, is easy to implement, and does not require any homogeneous direction in space or time. It is thus anticipated that it has a high potential for the computation of non-homogeneous, wall-bounded flows. |
doi_str_mv | 10.1063/1.3623274 |
format | Article |
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The proposed σ-model has, by construction, the property to automatically vanish as soon as the resolved field is either two-dimensional or two-component, including the pure shear and solid rotation cases. In addition, the model generates no subgrid-scale viscosity when the resolved scales are in pure axisymmetric or isotropic contraction/expansion. At last, it is shown analytically that it has the appropriate cubic behavior in the vicinity of solid boundaries without requiring any ad-hoc treatment. Results for two classical test cases (decaying isotropic turbulence and periodic channel flow) obtained from three different solvers with a variety of numerics (finite elements, finite differences, or spectral methods) are presented to illustrate the potential of this model. The results obtained with the proposed model are systematically equivalent or slightly better than the results from the Dynamic Smagorinsky model. Still, the σ-model has a low computational cost, is easy to implement, and does not require any homogeneous direction in space or time. 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The proposed σ-model has, by construction, the property to automatically vanish as soon as the resolved field is either two-dimensional or two-component, including the pure shear and solid rotation cases. In addition, the model generates no subgrid-scale viscosity when the resolved scales are in pure axisymmetric or isotropic contraction/expansion. At last, it is shown analytically that it has the appropriate cubic behavior in the vicinity of solid boundaries without requiring any ad-hoc treatment. Results for two classical test cases (decaying isotropic turbulence and periodic channel flow) obtained from three different solvers with a variety of numerics (finite elements, finite differences, or spectral methods) are presented to illustrate the potential of this model. The results obtained with the proposed model are systematically equivalent or slightly better than the results from the Dynamic Smagorinsky model. Still, the σ-model has a low computational cost, is easy to implement, and does not require any homogeneous direction in space or time. It is thus anticipated that it has a high potential for the computation of non-homogeneous, wall-bounded flows.</description><subject>Engineering Sciences</subject><subject>Exact sciences and technology</subject><subject>Flows in ducts, channels, nozzles, and conduits</subject><subject>Fluid dynamics</subject><subject>Fluid mechanics</subject><subject>Fluids mechanics</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Isotropic turbulence; homogeneous turbulence</subject><subject>Mechanics</subject><subject>Physics</subject><subject>Turbulence simulation and modeling</subject><subject>Turbulent flows, convection, and heat transfer</subject><issn>1070-6631</issn><issn>1089-7666</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp1kD1PwzAQhi0EEqUw8A-8MDCknD_iOAtSVQFFqtSFztbFdopR2lRxgtR_T9KWMrH4rNPznu4eQu4ZTBgo8cQmQnHBM3lBRgx0nmRKqcvhn0GilGDX5CbGLwAQOVcjslzFsF3T4ekqbOg3Vp2PtK1p0YXKUaSxK9ZNcEm0WHm6qZ2vaFk3tKfXnnrn9n1604fbUG_jLbkqsYr-7lTHZPX68jGbJ4vl2_tsukislHmb-NQpLRx6L_ulCpuidiWWqdRQgs8ht15plArSAjKpncpSLHJkufeQWo5iTB6Pcz-xMrsmbLDZmxqDmU8XZugBaOAy49_sj7VNHWPjy3OAgRmsGWZO1nr24cjucDi4bHBrQzwHuEy55Fr13PORiza0h9P_H3pQbH4Vm4Ni8QOsD4E-</recordid><startdate>20110801</startdate><enddate>20110801</enddate><creator>Nicoud, Franck</creator><creator>Toda, Hubert Baya</creator><creator>Cabrit, Olivier</creator><creator>Bose, Sanjeeb</creator><creator>Lee, Jungil</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><scope>VOOES</scope><orcidid>https://orcid.org/0000-0002-0006-8422</orcidid></search><sort><creationdate>20110801</creationdate><title>Using singular values to build a subgrid-scale model for large eddy simulations</title><author>Nicoud, Franck ; Toda, Hubert Baya ; Cabrit, Olivier ; Bose, Sanjeeb ; Lee, Jungil</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c449t-e5d683daee4663bc5a8dfaf5480f0e909ce68a4605b0748d675ab9a19ee05c2a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Engineering Sciences</topic><topic>Exact sciences and technology</topic><topic>Flows in ducts, channels, nozzles, and conduits</topic><topic>Fluid dynamics</topic><topic>Fluid mechanics</topic><topic>Fluids mechanics</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Isotropic turbulence; homogeneous turbulence</topic><topic>Mechanics</topic><topic>Physics</topic><topic>Turbulence simulation and modeling</topic><topic>Turbulent flows, convection, and heat transfer</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nicoud, Franck</creatorcontrib><creatorcontrib>Toda, Hubert Baya</creatorcontrib><creatorcontrib>Cabrit, Olivier</creatorcontrib><creatorcontrib>Bose, Sanjeeb</creatorcontrib><creatorcontrib>Lee, Jungil</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>Physics of fluids (1994)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nicoud, Franck</au><au>Toda, Hubert Baya</au><au>Cabrit, Olivier</au><au>Bose, Sanjeeb</au><au>Lee, Jungil</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Using singular values to build a subgrid-scale model for large eddy simulations</atitle><jtitle>Physics of fluids (1994)</jtitle><date>2011-08-01</date><risdate>2011</risdate><volume>23</volume><issue>8</issue><spage>085106</spage><epage>085106-12</epage><pages>085106-085106-12</pages><issn>1070-6631</issn><eissn>1089-7666</eissn><coden>PHFLE6</coden><abstract>An eddy-viscosity based, subgrid-scale model for large eddy simulations is derived from the analysis of the singular values of the resolved velocity gradient tensor. The proposed σ-model has, by construction, the property to automatically vanish as soon as the resolved field is either two-dimensional or two-component, including the pure shear and solid rotation cases. In addition, the model generates no subgrid-scale viscosity when the resolved scales are in pure axisymmetric or isotropic contraction/expansion. At last, it is shown analytically that it has the appropriate cubic behavior in the vicinity of solid boundaries without requiring any ad-hoc treatment. Results for two classical test cases (decaying isotropic turbulence and periodic channel flow) obtained from three different solvers with a variety of numerics (finite elements, finite differences, or spectral methods) are presented to illustrate the potential of this model. The results obtained with the proposed model are systematically equivalent or slightly better than the results from the Dynamic Smagorinsky model. Still, the σ-model has a low computational cost, is easy to implement, and does not require any homogeneous direction in space or time. It is thus anticipated that it has a high potential for the computation of non-homogeneous, wall-bounded flows.</abstract><cop>Melville, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.3623274</doi><orcidid>https://orcid.org/0000-0002-0006-8422</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Engineering Sciences Exact sciences and technology Flows in ducts, channels, nozzles, and conduits Fluid dynamics Fluid mechanics Fluids mechanics Fundamental areas of phenomenology (including applications) Isotropic turbulence homogeneous turbulence Mechanics Physics Turbulence simulation and modeling Turbulent flows, convection, and heat transfer |
title | Using singular values to build a subgrid-scale model for large eddy simulations |
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