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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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