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    A Three-Equation Variant of the SST k-ω Model Sensitized to Rotation and Curvature Effects

    Source: Journal of Fluids Engineering:;2011:;volume( 133 ):;issue: 011::page 111201
    Author:
    Tej P. Dhakal
    ,
    D. Keith Walters
    DOI: 10.1115/1.4004940
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: A new variant of the SST k-ω model sensitized to system rotation and streamline curvature is presented. The new model is based on a direct simplification of the Reynolds stress model under weak equilibrium assumptions [York et al. , 2009, “A Simple and Robust Linear Eddy-Viscosity Formulation for Curved and Rotating Flows,” International Journal for Numerical Methods in Heat and Fluid Flow, 19 (6), pp. 745–776]. An additional transport equation for a transverse turbulent velocity scale is added to enhance stability and incorporate history effects. The added scalar transport equation introduces the physical effects of curvature and rotation on turbulence structure via a modified rotation rate vector. The modified rotation rate is based on the material rotation rate of the mean strain-rate based coordinate system proposed by Wallin and Johansson (2002, “Modeling Streamline Curvature Effects in Explicit Algebraic Reynolds Stress Turbulence Models,” International Journal of Heat and Fluid Flow, 23 , pp. 721–730). The eddy viscosity is redefined based on the new turbulent velocity scale, similar to previously documented k-ɛ- υ2 model formulations (Durbin, 1991, “Near-Wall Turbulence Closure Modeling without Damping Functions,” Theoretical and Computational Fluid Dynamics, 3 , pp. 1–13). The new model is calibrated based on rotating homogeneous turbulent shear flow and is assessed on a number of generic test cases involving rotation and/or curvature effects. Results are compared to both the standard SST k-ω model and a recently proposed curvature-corrected version (Smirnov and Menter, 2009, “Sensitization of the SST Turbulence Model to Rotation and Curvature by Applying the Spalart-Shur Correction Term,” ASME Journal of Turbomachinery, 131 , pp. 1–8). For the test cases presented here, the new model provides reasonable engineering accuracy without compromising stability and efficiency, and with only a small increase in computational cost.
    keyword(s): Rotation , Flow (Dynamics) , Turbulence , Eddies (Fluid dynamics) , Viscosity , Kinetic energy , Equations , Stress , Cylinders , Equilibrium (Physics) AND Channel flow ,
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      A Three-Equation Variant of the SST k-ω Model Sensitized to Rotation and Curvature Effects

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    contributor authorTej P. Dhakal
    contributor authorD. Keith Walters
    date accessioned2017-05-09T00:44:09Z
    date available2017-05-09T00:44:09Z
    date copyrightNovember, 2011
    date issued2011
    identifier issn0098-2202
    identifier otherJFEGA4-27497#111201_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/146243
    description abstractA new variant of the SST k-ω model sensitized to system rotation and streamline curvature is presented. The new model is based on a direct simplification of the Reynolds stress model under weak equilibrium assumptions [York et al. , 2009, “A Simple and Robust Linear Eddy-Viscosity Formulation for Curved and Rotating Flows,” International Journal for Numerical Methods in Heat and Fluid Flow, 19 (6), pp. 745–776]. An additional transport equation for a transverse turbulent velocity scale is added to enhance stability and incorporate history effects. The added scalar transport equation introduces the physical effects of curvature and rotation on turbulence structure via a modified rotation rate vector. The modified rotation rate is based on the material rotation rate of the mean strain-rate based coordinate system proposed by Wallin and Johansson (2002, “Modeling Streamline Curvature Effects in Explicit Algebraic Reynolds Stress Turbulence Models,” International Journal of Heat and Fluid Flow, 23 , pp. 721–730). The eddy viscosity is redefined based on the new turbulent velocity scale, similar to previously documented k-ɛ- υ2 model formulations (Durbin, 1991, “Near-Wall Turbulence Closure Modeling without Damping Functions,” Theoretical and Computational Fluid Dynamics, 3 , pp. 1–13). The new model is calibrated based on rotating homogeneous turbulent shear flow and is assessed on a number of generic test cases involving rotation and/or curvature effects. Results are compared to both the standard SST k-ω model and a recently proposed curvature-corrected version (Smirnov and Menter, 2009, “Sensitization of the SST Turbulence Model to Rotation and Curvature by Applying the Spalart-Shur Correction Term,” ASME Journal of Turbomachinery, 131 , pp. 1–8). For the test cases presented here, the new model provides reasonable engineering accuracy without compromising stability and efficiency, and with only a small increase in computational cost.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleA Three-Equation Variant of the SST k-ω Model Sensitized to Rotation and Curvature Effects
    typeJournal Paper
    journal volume133
    journal issue11
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.4004940
    journal fristpage111201
    identifier eissn1528-901X
    keywordsRotation
    keywordsFlow (Dynamics)
    keywordsTurbulence
    keywordsEddies (Fluid dynamics)
    keywordsViscosity
    keywordsKinetic energy
    keywordsEquations
    keywordsStress
    keywordsCylinders
    keywordsEquilibrium (Physics) AND Channel flow
    treeJournal of Fluids Engineering:;2011:;volume( 133 ):;issue: 011
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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