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    Artificially Thickened Turbulent Boundary Layers for Studying Heat Transfer and Skin Friction on Rough Surfaces

    Source: Journal of Fluids Engineering:;1983:;volume( 105 ):;issue: 002::page 146
    Author:
    P. M. Ligrani
    ,
    R. J. Moffat
    ,
    W. M. Kays
    DOI: 10.1115/1.3240954
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Thermal and hydrodynamic characteristics of boundary layers developing over uniform spheres roughness with momentum thicknesses as large as 1.43 cm are presented. To obtain thick hydrodynamic boundary layers, an artificial thickening device is employed. The normalized velocity and turbulence profiles produced using this device are two-dimensional and self-preserving. The turbulent transport and structural characteristics are representative of normal behavior to the level of spectra of the longitudinal velocity fluctuations. In the artificially thickened layers, the effect of the unheated starting length (ξ > 0, Δ < δ) on thermal boundary layer properties is present. Turbulent Prandtl number profiles are generally unaffected by the magnitude of the unheated starting length, whereas measured Stanton numbers, show different behavior as the unheated starting length varies. In thermal boundary layers which would have the same thickness as the augmented hydrodynamic layers (Δ ≃ δ), Stanton numbers are shown to be the same as skin friction coefficients, and are then provided for boundary layers much thicker than those previously studied. As fully rough boundary layers develop downstream and δ/ks increases, Cf /2 is proportional to δ2 −b where b = 0.175. In order for such U∞ = constant, thick, rough wall layers to develop far enough downstream to reach smooth behavior where b = 0.250, ks Uτ /ν must become small, and b must increase from 0.175 to become greater than 0.250 in the transitionally rough regime.
    keyword(s): Heat transfer , Surface roughness , Skin friction (Fluid dynamics) , Boundary layer turbulence , Boundary layers , Turbulence , Thermal boundary layers , Prandtl number , Thickness , Momentum , Spectra (Spectroscopy) AND Fluctuations (Physics) ,
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      Artificially Thickened Turbulent Boundary Layers for Studying Heat Transfer and Skin Friction on Rough Surfaces

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/97271
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    • Journal of Fluids Engineering

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    contributor authorP. M. Ligrani
    contributor authorR. J. Moffat
    contributor authorW. M. Kays
    date accessioned2017-05-08T23:15:48Z
    date available2017-05-08T23:15:48Z
    date copyrightJune, 1983
    date issued1983
    identifier issn0098-2202
    identifier otherJFEGA4-26996#146_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/97271
    description abstractThermal and hydrodynamic characteristics of boundary layers developing over uniform spheres roughness with momentum thicknesses as large as 1.43 cm are presented. To obtain thick hydrodynamic boundary layers, an artificial thickening device is employed. The normalized velocity and turbulence profiles produced using this device are two-dimensional and self-preserving. The turbulent transport and structural characteristics are representative of normal behavior to the level of spectra of the longitudinal velocity fluctuations. In the artificially thickened layers, the effect of the unheated starting length (ξ > 0, Δ < δ) on thermal boundary layer properties is present. Turbulent Prandtl number profiles are generally unaffected by the magnitude of the unheated starting length, whereas measured Stanton numbers, show different behavior as the unheated starting length varies. In thermal boundary layers which would have the same thickness as the augmented hydrodynamic layers (Δ ≃ δ), Stanton numbers are shown to be the same as skin friction coefficients, and are then provided for boundary layers much thicker than those previously studied. As fully rough boundary layers develop downstream and δ/ks increases, Cf /2 is proportional to δ2 −b where b = 0.175. In order for such U∞ = constant, thick, rough wall layers to develop far enough downstream to reach smooth behavior where b = 0.250, ks Uτ /ν must become small, and b must increase from 0.175 to become greater than 0.250 in the transitionally rough regime.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleArtificially Thickened Turbulent Boundary Layers for Studying Heat Transfer and Skin Friction on Rough Surfaces
    typeJournal Paper
    journal volume105
    journal issue2
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.3240954
    journal fristpage146
    journal lastpage153
    identifier eissn1528-901X
    keywordsHeat transfer
    keywordsSurface roughness
    keywordsSkin friction (Fluid dynamics)
    keywordsBoundary layer turbulence
    keywordsBoundary layers
    keywordsTurbulence
    keywordsThermal boundary layers
    keywordsPrandtl number
    keywordsThickness
    keywordsMomentum
    keywordsSpectra (Spectroscopy) AND Fluctuations (Physics)
    treeJournal of Fluids Engineering:;1983:;volume( 105 ):;issue: 002
    contenttypeFulltext
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    yabeshDSpacePersian
     
    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
    yabeshDSpacePersian