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    Prediction of Small-Scale Cavitation in a High Speed Flow Over an Open Cavity Using Large-Eddy Simulation

    Source: Journal of Fluids Engineering:;2010:;volume( 132 ):;issue: 011::page 111301
    Author:
    Ehsan Shams
    ,
    Sourabh V. Apte
    DOI: 10.1115/1.4002744
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Large-eddy simulation of flow over an open cavity corresponding to the experimental setup of and (2008, “Cavitation Phenomena Occurring Due to Interaction of Shear Layer Vortices With the Trailing Corner of a Two-Dimensional Open Cavity,” Phys. Fluids, 20(4), p. 041702) is performed. The filtered, incompressible Navier–Stokes equations are solved using a co-located grid finite-volume solver with the dynamic Smagorinsky model for a subgrid-scale closure. The computational grid consists of around 7×106 grid points with 3×106 points clustered around the shear layer, and the boundary layer over the leading edge is resolved. The only input from the experimental data is the mean velocity profile at the inlet condition. The mean flow is superimposed with turbulent velocity fluctuations generated by solving a forced periodic duct flow at a freestream Reynolds number. The flow statistics, including mean and rms velocity fields and pressure coefficients, are compared with the experimental data to show reasonable agreement. The dynamic interactions between traveling vortices in the shear layer and the trailing edge affect the value and location of the pressure minima. Cavitation inception is investigated using two approaches: (i) a discrete bubble model wherein the bubble dynamics is computed by solving the Rayleigh–Plesset and the bubble motion equations using an adaptive time-stepping procedure and (ii) a scalar transport model for the liquid volume fraction with source and sink terms for phase change. Large-eddy simulation, together with the cavitation models, predicts that inception occurs near the trailing edge similar to that observed in the experiments. The bubble transport model captures the subgrid dynamics of the vapor better, whereas the scalar model captures the large-scale features more accurately. A hybrid approach combining the bubble model with the scalar transport is needed to capture the broad range of scales observed in cavitation.
    keyword(s): Scalars , Pressure , Flow (Dynamics) , Cavitation , Bubbles , Cavities , Shear (Mechanics) , Vapors AND Eddies (Fluid dynamics) ,
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      Prediction of Small-Scale Cavitation in a High Speed Flow Over an Open Cavity Using Large-Eddy Simulation

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    https://yetl.yabesh.ir/yetl1/handle/yetl/143405
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    contributor authorEhsan Shams
    contributor authorSourabh V. Apte
    date accessioned2017-05-09T00:38:06Z
    date available2017-05-09T00:38:06Z
    date copyrightNovember, 2010
    date issued2010
    identifier issn0098-2202
    identifier otherJFEGA4-27439#111301_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/143405
    description abstractLarge-eddy simulation of flow over an open cavity corresponding to the experimental setup of and (2008, “Cavitation Phenomena Occurring Due to Interaction of Shear Layer Vortices With the Trailing Corner of a Two-Dimensional Open Cavity,” Phys. Fluids, 20(4), p. 041702) is performed. The filtered, incompressible Navier–Stokes equations are solved using a co-located grid finite-volume solver with the dynamic Smagorinsky model for a subgrid-scale closure. The computational grid consists of around 7×106 grid points with 3×106 points clustered around the shear layer, and the boundary layer over the leading edge is resolved. The only input from the experimental data is the mean velocity profile at the inlet condition. The mean flow is superimposed with turbulent velocity fluctuations generated by solving a forced periodic duct flow at a freestream Reynolds number. The flow statistics, including mean and rms velocity fields and pressure coefficients, are compared with the experimental data to show reasonable agreement. The dynamic interactions between traveling vortices in the shear layer and the trailing edge affect the value and location of the pressure minima. Cavitation inception is investigated using two approaches: (i) a discrete bubble model wherein the bubble dynamics is computed by solving the Rayleigh–Plesset and the bubble motion equations using an adaptive time-stepping procedure and (ii) a scalar transport model for the liquid volume fraction with source and sink terms for phase change. Large-eddy simulation, together with the cavitation models, predicts that inception occurs near the trailing edge similar to that observed in the experiments. The bubble transport model captures the subgrid dynamics of the vapor better, whereas the scalar model captures the large-scale features more accurately. A hybrid approach combining the bubble model with the scalar transport is needed to capture the broad range of scales observed in cavitation.
    publisherThe American Society of Mechanical Engineers (ASME)
    titlePrediction of Small-Scale Cavitation in a High Speed Flow Over an Open Cavity Using Large-Eddy Simulation
    typeJournal Paper
    journal volume132
    journal issue11
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.4002744
    journal fristpage111301
    identifier eissn1528-901X
    keywordsScalars
    keywordsPressure
    keywordsFlow (Dynamics)
    keywordsCavitation
    keywordsBubbles
    keywordsCavities
    keywordsShear (Mechanics)
    keywordsVapors AND Eddies (Fluid dynamics)
    treeJournal of Fluids Engineering:;2010:;volume( 132 ):;issue: 011
    contenttypeFulltext
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