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    Postbuckling of Elastic Columns with Second-Mode Imperfection

    Source: Journal of Engineering Mechanics:;2006:;Volume ( 132 ):;issue: 008
    Author:
    Raymond H. Plaut
    ,
    David A. Dillard
    ,
    Lawrence N. Virgin
    DOI: 10.1061/(ASCE)0733-9399(2006)132:8(898)
    Publisher: American Society of Civil Engineers
    Abstract: Initial imperfections of columns are often assumed to have the shape of the first buckling mode. In this technical note, the imperfection has the shape of the second mode. An elastica analysis is performed, and numerical results are obtained for two cases with the use of a shooting method. For the example of a pinned column, bifurcation occurs at a load slightly higher than the critical load for the perfect system. With further increase in load, the deflection changes smoothly from an antisymmetric shape with one node to a shape with no nodes. For the cantilevered-column example, a limit point occurs just beyond the critical load for the perfect system, and the equilibrium shape jumps from one state to another. As the load is increased further, the deflection passes smoothly to the other side of the column and loses its inflection point.
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      Postbuckling of Elastic Columns with Second-Mode Imperfection

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    contributor authorRaymond H. Plaut
    contributor authorDavid A. Dillard
    contributor authorLawrence N. Virgin
    date accessioned2017-05-08T22:40:58Z
    date available2017-05-08T22:40:58Z
    date copyrightAugust 2006
    date issued2006
    identifier other%28asce%290733-9399%282006%29132%3A8%28898%29.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/86298
    description abstractInitial imperfections of columns are often assumed to have the shape of the first buckling mode. In this technical note, the imperfection has the shape of the second mode. An elastica analysis is performed, and numerical results are obtained for two cases with the use of a shooting method. For the example of a pinned column, bifurcation occurs at a load slightly higher than the critical load for the perfect system. With further increase in load, the deflection changes smoothly from an antisymmetric shape with one node to a shape with no nodes. For the cantilevered-column example, a limit point occurs just beyond the critical load for the perfect system, and the equilibrium shape jumps from one state to another. As the load is increased further, the deflection passes smoothly to the other side of the column and loses its inflection point.
    publisherAmerican Society of Civil Engineers
    titlePostbuckling of Elastic Columns with Second-Mode Imperfection
    typeJournal Paper
    journal volume132
    journal issue8
    journal titleJournal of Engineering Mechanics
    identifier doi10.1061/(ASCE)0733-9399(2006)132:8(898)
    treeJournal of Engineering Mechanics:;2006:;Volume ( 132 ):;issue: 008
    contenttypeFulltext
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