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    Thermoelastic Instability Including Surface Roughness Effects

    Source: Journal of Tribology:;1999:;volume( 121 ):;issue: 004::page 648
    Author:
    J. Y. Jang
    ,
    M. M. Khonsari
    DOI: 10.1115/1.2834118
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: A thermoelastic instability (TEI) analysis is presented for determining the threshold of instability in a friction pair consisting of a conducting surface rubbing against a rough surface with very low thermal conductivity. The theory predicts that TEI is initiated when the operating speed exceeds a limiting value of U* given by: U*/Us = 1 + Λℑ′ where Us is identical to the critical equation developed by Burton (1980) for highly loaded surfaces in contact defined as: Us = 2Ωks/fαE. The dimensionless parameters on the right-hand-side of the above equation emerge from the consideration of the surface roughness and are defined as Λ = σΩE/2χ, and ℑ′ = H o /F′. The results indicate that the magnitude of the applied load and the surface roughness characteristics tend to play an important role in the prediction of the onset of TEI instability.
    keyword(s): Surface roughness , Equations , Friction , Stress AND Thermal conductivity ,
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      Thermoelastic Instability Including Surface Roughness Effects

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    http://yetl.yabesh.ir/yetl1/handle/yetl/122811
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    contributor authorJ. Y. Jang
    contributor authorM. M. Khonsari
    date accessioned2017-05-09T00:00:50Z
    date available2017-05-09T00:00:50Z
    date copyrightOctober, 1999
    date issued1999
    identifier issn0742-4787
    identifier otherJOTRE9-28684#648_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/122811
    description abstractA thermoelastic instability (TEI) analysis is presented for determining the threshold of instability in a friction pair consisting of a conducting surface rubbing against a rough surface with very low thermal conductivity. The theory predicts that TEI is initiated when the operating speed exceeds a limiting value of U* given by: U*/Us = 1 + Λℑ′ where Us is identical to the critical equation developed by Burton (1980) for highly loaded surfaces in contact defined as: Us = 2Ωks/fαE. The dimensionless parameters on the right-hand-side of the above equation emerge from the consideration of the surface roughness and are defined as Λ = σΩE/2χ, and ℑ′ = H o /F′. The results indicate that the magnitude of the applied load and the surface roughness characteristics tend to play an important role in the prediction of the onset of TEI instability.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleThermoelastic Instability Including Surface Roughness Effects
    typeJournal Paper
    journal volume121
    journal issue4
    journal titleJournal of Tribology
    identifier doi10.1115/1.2834118
    journal fristpage648
    journal lastpage654
    identifier eissn1528-8897
    keywordsSurface roughness
    keywordsEquations
    keywordsFriction
    keywordsStress AND Thermal conductivity
    treeJournal of Tribology:;1999:;volume( 121 ):;issue: 004
    contenttypeFulltext
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