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    Passive and Active Inertia Forces in Flexible Body Dynamics

    Source: Journal of Dynamic Systems, Measurement, and Control:;1992:;volume( 114 ):;issue: 004::page 571
    Author:
    W. C. Hsu
    ,
    A. A. Shabana
    DOI: 10.1115/1.2897726
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: This investigation is devoted to a discussion on the effect of the coupling between the longitudinal and transverse displacements of kinematically driven rotating beams. To this end, the inertia forces that act on a flexible body as the result of the finite rotation are categorized into two classes. These are the passive and active inertia forces. While the effect of the active inertia forces of kinematically driven systems is recognized in the absence of external disturbances and nonzero initial conditions, the passive inertia forces of such systems are not recognized in the case of zero initial conditions and in the absence of external excitations. Depending on the assumed displacement field, three classes of mechanical systems are defined in this paper. These are the active, partially active, and passive systems. The active system has a mathematical model in which both passive and active inertia forces are fully presented. In a partially active system, a part of the passive inertia forces and the active inertia forces appear in the mathematical model. The vibration of the kinematically driven passive system is governed by homogeneous equations which contain only the passive inertia forces. In the case of zero initial conditions and in the absence of external excitation, the response of the passive kinematically driven system is zero regardless of the value of the angular velocity. The effect of the inertia forces of the passive system appear as a time varying modification of the system parameters. It is shown in this investigation that a rotating beam model in which the axial deformation is neglected is a partially active or passive system. It is also demonstrated that the neglect of the effect of the longitudinal displacement has two significant effects. It decouples the modes of vibration and makes the form of the complementary solution independent of the sense of rotation. The behavior of the active, partially active, and passive systems when they are subjected to driving constraints (specified motion) is examined and it is shown that the response of the passive system converges to the partially active system if the effect of the initial conditions becomes dominant as compared to the effect of the active inertia forces of the partially active system.
    keyword(s): Inertia (Mechanics) , Force , Flexible body dynamics , Vibration , Displacement , Rotation , Rotating beams , Deformation , Motion AND Equations ,
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      Passive and Active Inertia Forces in Flexible Body Dynamics

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    https://yetl.yabesh.ir/yetl1/handle/yetl/109907
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    • Journal of Dynamic Systems, Measurement, and Control

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    contributor authorW. C. Hsu
    contributor authorA. A. Shabana
    date accessioned2017-05-08T23:37:50Z
    date available2017-05-08T23:37:50Z
    date copyrightDecember, 1992
    date issued1992
    identifier issn0022-0434
    identifier otherJDSMAA-26187#571_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/109907
    description abstractThis investigation is devoted to a discussion on the effect of the coupling between the longitudinal and transverse displacements of kinematically driven rotating beams. To this end, the inertia forces that act on a flexible body as the result of the finite rotation are categorized into two classes. These are the passive and active inertia forces. While the effect of the active inertia forces of kinematically driven systems is recognized in the absence of external disturbances and nonzero initial conditions, the passive inertia forces of such systems are not recognized in the case of zero initial conditions and in the absence of external excitations. Depending on the assumed displacement field, three classes of mechanical systems are defined in this paper. These are the active, partially active, and passive systems. The active system has a mathematical model in which both passive and active inertia forces are fully presented. In a partially active system, a part of the passive inertia forces and the active inertia forces appear in the mathematical model. The vibration of the kinematically driven passive system is governed by homogeneous equations which contain only the passive inertia forces. In the case of zero initial conditions and in the absence of external excitation, the response of the passive kinematically driven system is zero regardless of the value of the angular velocity. The effect of the inertia forces of the passive system appear as a time varying modification of the system parameters. It is shown in this investigation that a rotating beam model in which the axial deformation is neglected is a partially active or passive system. It is also demonstrated that the neglect of the effect of the longitudinal displacement has two significant effects. It decouples the modes of vibration and makes the form of the complementary solution independent of the sense of rotation. The behavior of the active, partially active, and passive systems when they are subjected to driving constraints (specified motion) is examined and it is shown that the response of the passive system converges to the partially active system if the effect of the initial conditions becomes dominant as compared to the effect of the active inertia forces of the partially active system.
    publisherThe American Society of Mechanical Engineers (ASME)
    titlePassive and Active Inertia Forces in Flexible Body Dynamics
    typeJournal Paper
    journal volume114
    journal issue4
    journal titleJournal of Dynamic Systems, Measurement, and Control
    identifier doi10.1115/1.2897726
    journal fristpage571
    journal lastpage579
    identifier eissn1528-9028
    keywordsInertia (Mechanics)
    keywordsForce
    keywordsFlexible body dynamics
    keywordsVibration
    keywordsDisplacement
    keywordsRotation
    keywordsRotating beams
    keywordsDeformation
    keywordsMotion AND Equations
    treeJournal of Dynamic Systems, Measurement, and Control:;1992:;volume( 114 ):;issue: 004
    contenttypeFulltext
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