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dc.creatorGrabovsky, Y
dc.creatorHarutyunyan, D
dc.date.accessioned2021-02-03T17:30:50Z
dc.date.available2021-02-03T17:30:50Z
dc.date.issued2016-02-01
dc.identifier.issn0938-8974
dc.identifier.issn1432-1467
dc.identifier.doihttp://dx.doi.org/10.34944/dspace/5760
dc.identifier.otherDA5PZ (isidoc)
dc.identifier.urihttp://hdl.handle.net/20.500.12613/5778
dc.description.abstract© 2015, Springer Science+Business Media New York. In this paper, we continue the development of mathematically rigorous theory of “near-flip” buckling of slender bodies of arbitrary geometry, based on hyperelasticity. In order to showcase the capabilities of this theory, we apply it to buckling of axially compressed circular cylindrical shells. The theory confirms the classical formula for the buckling load, whereby the perfect structure buckles at the stress that scales as the first power of shell’s thickness. However, in the case of imperfections of load, the theory predicts scaling instability of the buckling stress. Depending on the type of load imperfections, buckling may occur at stresses that scale as thickness to the power 1.5 or 1.25, corresponding to the lower and upper ends, respectively, of the historically accumulated experimental data.
dc.format.extent83-119
dc.language.isoen
dc.relation.haspartJournal of Nonlinear Science
dc.relation.isreferencedbySpringer Science and Business Media LLC
dc.subjectBuckling
dc.subjectCylindrical shell
dc.subjectInstability
dc.subjectSecond variation
dc.subjectCritical load imperfection sensitivity
dc.subjectScaling exponents
dc.titleScaling Instability in Buckling of Axially Compressed Cylindrical Shells
dc.typeArticle
dc.type.genreJournal Article
dc.relation.doi10.1007/s00332-015-9270-9
dc.ada.noteFor Americans with Disabilities Act (ADA) accommodation, including help with reading this content, please contact scholarshare@temple.edu
dc.date.updated2021-02-03T17:30:47Z
refterms.dateFOA2021-02-03T17:30:50Z


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