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    On the Mean Reynolds Equation in the Presence of Surface Roughness: Squeeze-Film Bearing

    Source: Journal of Applied Mechanics:;1981:;volume( 048 ):;issue: 004::page 717
    Author:
    N. Phan-Thien
    DOI: 10.1115/1.3157721
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The mean Reynolds equation in the presence of surface roughness is derived using the techniques developed by Keller. This mean equation is nonlocal in the sense that the mean pressure at all points in the flow field has some effect on the mean pressure at any particular point. The performance of a two-dimensional squeeze film bearing with homogeneous surface roughness is considered next showing that the load is enhanced by a factor of 1 + ε2 a2 S/h2 , where εa is the amplitude of the roughness, h is the film thickness, and S varies between −3 〈m2 〉, for parallel surface roughness, to 6 〈m2 〉 for transverse surface roughness. Here, the bearing surfaces are described by εam1 and h + εam2 and m = m2 − m1 .
    keyword(s): Surface roughness , Bearings , Equations , Pressure , Flow (Dynamics) , Stress AND Film thickness ,
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      On the Mean Reynolds Equation in the Presence of Surface Roughness: Squeeze-Film Bearing

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    http://yetl.yabesh.ir/yetl1/handle/yetl/94015
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    contributor authorN. Phan-Thien
    date accessioned2017-05-08T23:10:08Z
    date available2017-05-08T23:10:08Z
    date copyrightDecember, 1981
    date issued1981
    identifier issn0021-8936
    identifier otherJAMCAV-26188#717_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/94015
    description abstractThe mean Reynolds equation in the presence of surface roughness is derived using the techniques developed by Keller. This mean equation is nonlocal in the sense that the mean pressure at all points in the flow field has some effect on the mean pressure at any particular point. The performance of a two-dimensional squeeze film bearing with homogeneous surface roughness is considered next showing that the load is enhanced by a factor of 1 + ε2 a2 S/h2 , where εa is the amplitude of the roughness, h is the film thickness, and S varies between −3 〈m2 〉, for parallel surface roughness, to 6 〈m2 〉 for transverse surface roughness. Here, the bearing surfaces are described by εam1 and h + εam2 and m = m2 − m1 .
    publisherThe American Society of Mechanical Engineers (ASME)
    titleOn the Mean Reynolds Equation in the Presence of Surface Roughness: Squeeze-Film Bearing
    typeJournal Paper
    journal volume48
    journal issue4
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.3157721
    journal fristpage717
    journal lastpage720
    identifier eissn1528-9036
    keywordsSurface roughness
    keywordsBearings
    keywordsEquations
    keywordsPressure
    keywordsFlow (Dynamics)
    keywordsStress AND Film thickness
    treeJournal of Applied Mechanics:;1981:;volume( 048 ):;issue: 004
    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
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