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Renaissance of Bernal's random close packing and hypercritical line in the theory of liquids

dc.contributor.authorFinney, John L.
dc.contributor.authorWoodcock, Leslie
dc.date.accessioned2018-12-07T14:53:19Z
dc.date.available2018-12-07T14:53:19Z
dc.date.issued2014
dc.description.abstractWe review the scientific history of random close packing (RCP) of equal spheres, advocated by J D Bernal as a more plausible alternative to the non-ideal gas or imperfect crystal as a structural model of simple liquids. After decades of neglect, computer experiments are revealing a central role for RCP in the theory of liquids. These demonstrate that the RCP amorphous state of hard spheres can be well defined, is reproducible, and has the thermodynamic status of a metastable ground state. Further evidence from simulations of square-well model liquids indicates an extended role of RCP as an amorphous ground state that terminates a supercooled liquid coexistence line, suggesting likewise for real liquids. A phase diagram involving percolation boundaries has been proposed in which there is no merging of liquid and gas phases, and no critical singularity as assumed by van der Waals. Rather, the liquid phase continuously spans all temperatures, but above a critical dividing line on the Gibbs density surface, it is bounded by a percolation transition and separated from the gas phase by a colloidal supercritical mesophase. The colloidal-like inversion in the mesophase as it changes from gas-in-liquid to liquid-in-gas can be identified with the hypercritical line of Bernal. We therefore argue that the statistical theory of simple liquids should start from the RCP reference state rather than the ideal gas. Future experimental priorities are to (i) find evidence for an amorphous ground state in real supercooled liquids, (ii) explore the microscopic structures of the supercritical mesophase, and (iii) determine how these change from gas to liquid, especially across Bernal's hypercritical line. The theoretical priority is a statistical geometrical theory of RCP. Only then might we explain the coincident values of the RCP packing fraction with Buffon's constant, and the RCP residual entropy with Boltzmann's ideal gas constant.
dc.description.versioninfo:eu-repo/semantics/publishedVersion
dc.identifier.doi10.1088/0953-8984/26/46/463102
dc.identifier.issn0953-8984
dc.identifier.issn1361-648X
dc.identifier.urihttp://hdl.handle.net/10400.1/11451
dc.language.isoeng
dc.peerreviewedyes
dc.publisherIop Publishing Ltd
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.subjectHard-sphere fluid
dc.subjectPercolation transition
dc.subjectEqual spheres
dc.subjectVirial-coefficients
dc.subjectRadial distribution
dc.subjectGlass-transition
dc.subjectPhase-transition
dc.subjectModel
dc.subjectArgon
dc.subjectHeats
dc.titleRenaissance of Bernal's random close packing and hypercritical line in the theory of liquids
dc.typejournal article
dspace.entity.typePublication
oaire.citation.issue46
oaire.citation.startPage463102
oaire.citation.titleJournal of Physics: Condensed Matter
oaire.citation.volume280
person.familyNameWoodcock
person.givenNameLeslie
person.identifier.orcid0000-0003-2350-559X
rcaap.rightsopenAccess
rcaap.typearticle
relation.isAuthorOfPublicationb550a18f-b4d3-4d68-8b8d-84f3373024aa
relation.isAuthorOfPublication.latestForDiscoveryb550a18f-b4d3-4d68-8b8d-84f3373024aa

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