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dc.contributor.authorGalteland, Olav
dc.contributor.authorBering, Eivind
dc.contributor.authorKristiansen, Kim
dc.contributor.authorBedeaux, Dick
dc.contributor.authorKjelstrup, Signe
dc.date.accessioned2023-02-13T12:33:39Z
dc.date.available2023-02-13T12:33:39Z
dc.date.created2022-10-04T09:17:19Z
dc.date.issued2022
dc.identifier.citationNanoscale Advances. 2022, 4 (12), 2660-2670.en_US
dc.identifier.urihttps://hdl.handle.net/11250/3050390
dc.description.abstractWe have investigated the state of a nanoconfined fluid in a slit pore in the canonical and isobaric ensembles. The systems were simulated with molecular dynamics simulations. The fluid has a transition to a close-packed structure when the height of the slit approaches the particle diameter. The Helmholtz energy is a non-convex function of the slit height if the number of particles does not exceed that of one monolayer. As a consequence, the Legendre transform cannot be applied to obtain the Gibbs energy. The Gibbs energy of a non-deformable slit pore can be transformed into the Helmholtz energy of a deformable slit pore using the Legendre-Fenchel transform. The Legendre-Fenchel transform corresponds to the Maxwell construction of equal areas.en_US
dc.language.isoengen_US
dc.publisherRoyal Society of Chemistryen_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleLegendre-Fenchel transforms capture layering transitions in porous mediaen_US
dc.title.alternativeLegendre-Fenchel transforms capture layering transitions in porous mediaen_US
dc.typePeer revieweden_US
dc.typeJournal articleen_US
dc.description.versionpublishedVersionen_US
dc.source.pagenumber2660-2670en_US
dc.source.volume4en_US
dc.source.journalNanoscale Advancesen_US
dc.source.issue12en_US
dc.identifier.doi10.1039/d1na00846c
dc.identifier.cristin2058154
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1


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