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dc.contributor.authorBarry J. Coxen_US
dc.contributor.authorDuangkamon Baowanen_US
dc.contributor.authorWolfgang Bacsaen_US
dc.contributor.authorJames M. Hillen_US
dc.contributor.otherThe University of Adelaideen_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherUniversite de Toulouseen_US
dc.contributor.otherUniversity of South Australiaen_US
dc.date.accessioned2018-11-23T09:55:13Z-
dc.date.available2018-11-23T09:55:13Z-
dc.date.issued2015-01-01en_US
dc.identifier.citationRSC Advances. Vol.5, No.71 (2015), 57515-57520en_US
dc.identifier.issn20462069en_US
dc.identifier.other2-s2.0-84936971223en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84936971223&origin=inwarden_US
dc.identifier.urihttp://repository.li.mahidol.ac.th/dspace/handle/123456789/35724-
dc.description.abstract© The Royal Society of Chemistry 2015. Variational calculus is employed to determine the folding behaviour of a single graphene sheet. Both the elastic and van der Waals energies are taken into account, and from these considerations the shape of the curve is determined. By prescribing that the separation distance between the folded graphene in the parallel region is 3.32 Å, an arbitrary constant arising by integrating the Euler-Lagrange equation is determined, and the full parametric representations for the folding conformation are derived. Using typical values of the bending rigidity in the range of 0.800-1.60 eV, the shortest stable folded graphene sheets are required to be at least 6.5-10 nm in length.en_US
dc.rightsMahidol Universityen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84936971223&origin=inwarden_US
dc.subjectChemical Engineeringen_US
dc.subjectChemistryen_US
dc.titleRelating elasticity and graphene folding conformationen_US
dc.typeArticleen_US
dc.rights.holderSCOPUSen_US
dc.identifier.doi10.1039/c5ra08276een_US
Appears in Collections:Scopus 2011-2015

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