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dc.contributor.authorMcHugh, Kevin A.
dc.contributor.authorDowell, Earl H.
dc.date.accessioned2022-02-04T22:58:34Z
dc.date.available2022-02-04T22:58:34Z
dc.date.copyright2/1/2020 12:00:00 AM
dc.date.issued2020
dc.identifier.issn1555-1415
dc.identifier.othercnd_015_02_021003.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4275822
dc.description.abstractA free–free beam with a compressive follower force applied to one end exhibits interesting flutter and limit cycle oscillation (LCO) responses. Here, the derivation from Lagrange's equations is given for the nonlinear inextensible beam with such a force applied. The inextensibility constraint is met with a Lagrange multiplier added to the Lagrangian, and the beam allowed three rigid body modes in planar motion in addition to its elastic deformation. The Rayleigh–Ritz modal expansion method and the Runge–Kutta method are used to calculate time histories of the forced beam response. This new model is validated against classical results for the stability boundary and new LCO bifurcation diagrams are computed.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleNonlinear Response of an Inextensible, Free–Free Beam Subjected to a Nonconservative Follower Force
dc.typeJournal Paper
dc.journal.volume15
dc.journal.issue2
dc.journal.titleJournal of Computational and Nonlinear Dynamics
dc.identifier.doi10.1115/1.4045532
dc.journal.fristpage021003-1
dc.journal.lastpage021003-12
dc.page12
dc.treeJournal of Computational and Nonlinear Dynamics:;2020:;volume( 015 ):;issue: 002
dc.contenttypeFulltext


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