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    Energy Redistribution Between the Mean and Pulsating Flow Field in a Separated Flow Region

    Source: Journal of Fluids Engineering:;2014:;volume( 136 ):;issue: 011::page 111105
    Author:
    Dol, Sharul S.
    ,
    Salek, M. Mehdi
    ,
    Martinuzzi, Robert J.
    DOI: 10.1115/1.4026923
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: One of the main features of the backwardfacing step (BFS) low frequency pulsatile flow is the unsteadiness due to the convection of vortical (coherent) structures, which characterize the flow dynamics in the shear layer. The physics of the flow field is analyzed by looking at energy redistribution between the mean and pulsating flow field obtained via a particle image velocimeter (PIV) using the concept of a triple decomposition. The total fluctuating kinetic budget is calculated and discussed for a mean Reynolds number of 100 and for 0.035 ≤ St ≤ 2.19. The effects that these coherent structures have on the fluctuating kinetic energy production, dissipation, and transport mechanism are examined. The results provide insight into the physics of the flow and suggest reasons for vortex growth and decay. Fluctuating kinetic energy is generally produced at the separated shear layers and transported towards the core flow and then to the upper and lower walls where viscosity dissipates the energy. The remaining energy is transported streamwise and decays as it is convected downstream (St = 0.4 and 1 cases). It was also found that the pressurevelocity correlation diffusion plays a significant role in the transport of kinetic energy and Reynolds stresses, especially in the separated shear layer. More energy was dissipated at the walls for the high Strouhal number case St = 2.19 due to the transverse pressure diffusion term being increasingly dominant. This could be the reason why the convected primary vortices were much smaller in size and weaker with no upper wall vortices formed at this pulsation Strouhal number. The shear production for St = 0.035 was very minimal; thus, the vortices died down quickly even before the shedding could happen. Finally, the pressurestrain correlation term was found to be significant in redistributing the kinetic energy from ucomponent to vcomponent.
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      Energy Redistribution Between the Mean and Pulsating Flow Field in a Separated Flow Region

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    contributor authorDol, Sharul S.
    contributor authorSalek, M. Mehdi
    contributor authorMartinuzzi, Robert J.
    date accessioned2017-05-09T01:08:51Z
    date available2017-05-09T01:08:51Z
    date issued2014
    identifier issn0098-2202
    identifier otherfe_136_11_111105.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/155077
    description abstractOne of the main features of the backwardfacing step (BFS) low frequency pulsatile flow is the unsteadiness due to the convection of vortical (coherent) structures, which characterize the flow dynamics in the shear layer. The physics of the flow field is analyzed by looking at energy redistribution between the mean and pulsating flow field obtained via a particle image velocimeter (PIV) using the concept of a triple decomposition. The total fluctuating kinetic budget is calculated and discussed for a mean Reynolds number of 100 and for 0.035 ≤ St ≤ 2.19. The effects that these coherent structures have on the fluctuating kinetic energy production, dissipation, and transport mechanism are examined. The results provide insight into the physics of the flow and suggest reasons for vortex growth and decay. Fluctuating kinetic energy is generally produced at the separated shear layers and transported towards the core flow and then to the upper and lower walls where viscosity dissipates the energy. The remaining energy is transported streamwise and decays as it is convected downstream (St = 0.4 and 1 cases). It was also found that the pressurevelocity correlation diffusion plays a significant role in the transport of kinetic energy and Reynolds stresses, especially in the separated shear layer. More energy was dissipated at the walls for the high Strouhal number case St = 2.19 due to the transverse pressure diffusion term being increasingly dominant. This could be the reason why the convected primary vortices were much smaller in size and weaker with no upper wall vortices formed at this pulsation Strouhal number. The shear production for St = 0.035 was very minimal; thus, the vortices died down quickly even before the shedding could happen. Finally, the pressurestrain correlation term was found to be significant in redistributing the kinetic energy from ucomponent to vcomponent.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleEnergy Redistribution Between the Mean and Pulsating Flow Field in a Separated Flow Region
    typeJournal Paper
    journal volume136
    journal issue11
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.4026923
    journal fristpage111105
    journal lastpage111105
    identifier eissn1528-901X
    treeJournal of Fluids Engineering:;2014:;volume( 136 ):;issue: 011
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
    yabeshDSpacePersian