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dc.contributor.authorBen Hassine, Bacem
dc.contributor.authorNegrier, Philippe
dc.contributor.authorBarrio Casado, María del
dc.contributor.authorMondieig, Denise
dc.contributor.authorMassip, Stephane
dc.contributor.authorTamarit Mur, José Luis
dc.contributor.otherUniversitat Politècnica de Catalunya. Departament de Física i Enginyeria Nuclear
dc.date.accessioned2015-09-22T11:46:59Z
dc.date.available2016-08-01T00:30:51Z
dc.date.created2015-08-01
dc.date.issued2015-08-01
dc.identifier.citationBen Hassine, B., Negrier, P., Del Barrio, M., Mondieig, D., Massip, S., Tamarit, J. Ll. Phase transition in hydrogen-bonded 1-adamantane-methanol. "Crystal growth and design", 01 Agost 2015, núm. 8, p. 4149-4155.
dc.identifier.issn1528-7483
dc.identifier.urihttp://hdl.handle.net/2117/77015
dc.description.abstractThe polymorphism of 1-adarnantane-methanol C11H18O has been investigated by differential thermal analysis and single-crystal and powder X-ray diffraction. Below the melting temperature (389.5 +/- 0.4 K), this compound exhibits an orthorhombic phase (phase I, Pnnm, Z = 12, Z' = 1.5). The melting enthalpy was determined to be 20.5 +/- 0.4 kJ mol(-1), i.e., with an entropy change of (6.34 +/- 0.13)R, which is much higher than the quoted value from Timmermans for the melting orientationally disordered phases (2.5R), thus supporting the orientationally ordered character of phase I. This orthorhombic phase I exhibits a statistical disorder of the hydrogen atom related to the oxygen atom, due to the position of one independent molecule on the mirror. At ca. 272 K, phase I transforms continuously through an order disorder transition to a low-temperature monoclinic phase II (P2(1)/n, Z = 12, Z' = 3). The monoclinic and orthorhombic phases are related by a group subgroup relationship, which perfectly agrees with the continuous character of the II to I transition. Moreover, by a convenient choice of an order parameter related to the continuous tilt of the c-axis, the critical exponent for this transition is found to be close to the theoretical prediction of the three-dimensional Ising model (with a critical exponent of ca. 0.27).
dc.format.extent7 p.
dc.language.isoeng
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/
dc.subjectÀrees temàtiques de la UPC::Física::Termodinàmica
dc.subjectÀrees temàtiques de la UPC::Enginyeria química::Química física
dc.subject.lcshAtoms
dc.subject.lcshThermochemistry
dc.subject.otherHigh-pressure
dc.subject.otherPlastic crystals
dc.subject.otherMolecular reorientations
dc.subject.otherSubstituted adamantanes
dc.subject.otherDisorder
dc.subject.otherPolymorphism
dc.subject.otherTemperature
dc.subject.otherBehavior
dc.titlePhase transition in hydrogen-bonded 1-adamantane-methanol
dc.typeArticle
dc.subject.lemacÀtoms
dc.subject.lemacTermoquímica
dc.contributor.groupUniversitat Politècnica de Catalunya. GCM - Grup de Caracterització de Materials
dc.identifier.doi10.1021/acs.cgd.5b00764
dc.rights.accessOpen Access
local.identifier.drac16870334
dc.description.versionPostprint (published version)
local.citation.authorBen Hassine, B.; Negrier, P.; Del Barrio, M.; Mondieig, D.; Massip, S.; Tamarit, J. Ll.
local.citation.publicationNameCrystal growth and design
local.citation.volume15
local.citation.number8
local.citation.startingPage4149
local.citation.endingPage4155


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