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    Rolling Bearing Stress Based Life—Part I: Calculation Model

    Source: Journal of Tribology:;2012:;volume( 134 ):;issue: 002::page 21103
    Author:
    L. Houpert
    ,
    F. Chevalier
    DOI: 10.1115/1.4006135
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Rolling contact bearing life is calculated using stresses calculated at the surface and in the volume. Surface stresses account for profile and misalignment as well as asperity deformations. Sub-surface stresses are calculated beneath the asperities (for defining the life of the surface) and deeper in the volume for calculating the life of the volume. The stress-life criterion adopted is the Dang Van one in which the local stabilized shear stress is compared to the material endurance limit defined as a function of the hydrostatic pressure (itself a function of the contact pressure) but also residual stresses and hoop stresses (due to fit). A stress-life exponent c, of the order of 4 (instead of 34/3 in the standard Lundberg and Palmgren model) is used for respecting a local load-life exponent of 10/3 at typical load levels. Life of any circumferential slices of the inner, outer, and roller is defined for obtaining the final bearing life. Trends showing how the bearing life varies as a function of the applied bearing load and Λ ratio (film thickness/RMS roughness height) are given.
    keyword(s): Stress , Pressure AND Bearings ,
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      Rolling Bearing Stress Based Life—Part I: Calculation Model

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/150348
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    • Journal of Tribology

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    contributor authorL. Houpert
    contributor authorF. Chevalier
    date accessioned2017-05-09T00:54:41Z
    date available2017-05-09T00:54:41Z
    date copyrightApril, 2012
    date issued2012
    identifier issn0742-4787
    identifier otherJOTRE9-28789#021103_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/150348
    description abstractRolling contact bearing life is calculated using stresses calculated at the surface and in the volume. Surface stresses account for profile and misalignment as well as asperity deformations. Sub-surface stresses are calculated beneath the asperities (for defining the life of the surface) and deeper in the volume for calculating the life of the volume. The stress-life criterion adopted is the Dang Van one in which the local stabilized shear stress is compared to the material endurance limit defined as a function of the hydrostatic pressure (itself a function of the contact pressure) but also residual stresses and hoop stresses (due to fit). A stress-life exponent c, of the order of 4 (instead of 34/3 in the standard Lundberg and Palmgren model) is used for respecting a local load-life exponent of 10/3 at typical load levels. Life of any circumferential slices of the inner, outer, and roller is defined for obtaining the final bearing life. Trends showing how the bearing life varies as a function of the applied bearing load and Λ ratio (film thickness/RMS roughness height) are given.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleRolling Bearing Stress Based Life—Part I: Calculation Model
    typeJournal Paper
    journal volume134
    journal issue2
    journal titleJournal of Tribology
    identifier doi10.1115/1.4006135
    journal fristpage21103
    identifier eissn1528-8897
    keywordsStress
    keywordsPressure AND Bearings
    treeJournal of Tribology:;2012:;volume( 134 ):;issue: 002
    contenttypeFulltext
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