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    Special Cases of Friction and Applications

    Source: Journal of Mechanical Design:;1984:;volume( 106 ):;issue: 002::page 256
    Author:
    F. L. Litvin
    ,
    J. J. Coy
    DOI: 10.1115/1.3258588
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Two techniques for reducing friction forces are presented. The techniques are applied to the generalized problem of reducing the friction between kinematic pairs which connect a movable link to a frame. The basic principles are: (a) Let the movable link be supported by two bearings where the relative velocities of the link with respect to each bearing are of opposite directions. Thus the resultant force (torque) of friction acting on the link due to the bearings is approximately zero. Then, additional perturbation of motion parallel to the main motion of the movable link will require only a very small force. (b) Let the perturbation in motion be perpendicular to the main motion. Equations are developed which explain these two methods. The results are discussed in relation to friction in geared couplings, gyroscope gimbal bearings, and a rotary conveyer system. Design examples are presented.
    keyword(s): Friction , Motion , Bearings , Force , Torque , Structural frames , Design , Couplings AND Equations ,
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      Special Cases of Friction and Applications

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    contributor authorF. L. Litvin
    contributor authorJ. J. Coy
    date accessioned2017-05-08T23:18:32Z
    date available2017-05-08T23:18:32Z
    date copyrightJune, 1984
    date issued1984
    identifier issn1050-0472
    identifier otherJMDEDB-28040#256_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/98808
    description abstractTwo techniques for reducing friction forces are presented. The techniques are applied to the generalized problem of reducing the friction between kinematic pairs which connect a movable link to a frame. The basic principles are: (a) Let the movable link be supported by two bearings where the relative velocities of the link with respect to each bearing are of opposite directions. Thus the resultant force (torque) of friction acting on the link due to the bearings is approximately zero. Then, additional perturbation of motion parallel to the main motion of the movable link will require only a very small force. (b) Let the perturbation in motion be perpendicular to the main motion. Equations are developed which explain these two methods. The results are discussed in relation to friction in geared couplings, gyroscope gimbal bearings, and a rotary conveyer system. Design examples are presented.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleSpecial Cases of Friction and Applications
    typeJournal Paper
    journal volume106
    journal issue2
    journal titleJournal of Mechanical Design
    identifier doi10.1115/1.3258588
    journal fristpage256
    journal lastpage260
    identifier eissn1528-9001
    keywordsFriction
    keywordsMotion
    keywordsBearings
    keywordsForce
    keywordsTorque
    keywordsStructural frames
    keywordsDesign
    keywordsCouplings AND Equations
    treeJournal of Mechanical Design:;1984:;volume( 106 ):;issue: 002
    contenttypeFulltext
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