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dc.contributor.authorAkhouri, B.P.
dc.contributor.authorSolana Quirós, José Ramón 
dc.contributor.otherUniversidad de Cantabriaes_ES
dc.date.accessioned2023-03-02T15:47:20Z
dc.date.available2023-03-02T15:47:20Z
dc.date.issued2022
dc.identifier.issn0378-4371
dc.identifier.issn1873-2119
dc.identifier.urihttps://hdl.handle.net/10902/27971
dc.description.abstractA third-order perturbation theory is used to obtain the equilibrium properties of Ar, Kr and Xe over wide ranges of temperatures and densities. The theory belongs to the framework of the inverse temperature expansion of the Helmholtz free energy, with the perturbation terms determined from Monte Carlo simulation. The interactions are modeled by an effective two-body Lennard-Jones potential incorporating the main contribution of the three-body interactions. To this end, the ratio of three-body to two-body configuration energies have been determined also from Monte Carlo simulation. The results for the pressure and energy at supercritical temperatures are in quite good agreement with experimental data. The liquid?vapor coexistence is also reproduced fairly well, although for Ar and Kr the critical temperature is slightly overestimated as well as the liquid densities at low temperatures, and the coexistence densities of Xe are slightly overestimated for the vapor and underestimated for the liquid near the critical point. In any case, the calculations show a remarkable improvement in the predicted coexistence curve with including the three-body contribution.es_ES
dc.format.extent12 p.es_ES
dc.language.isoenges_ES
dc.publisherElsevieres_ES
dc.rights© 2022 The Author(s)es_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.sourcePhysica A: Statistical Mechanics and its Applications, 2022, 608 Part 1, 128280-(CORRIGENDUM), 2023, 615, 128528es_ES
dc.subject.otherMonte Carlo simulationes_ES
dc.subject.otherPerturbation theoryes_ES
dc.subject.otherNoble gaseses_ES
dc.subject.otherThree-body interactionses_ES
dc.titleThermodynamic properties of Ar, Kr and Xe from a Monte Carlo-based perturbation theory with an effective two-body Lennard-Jones potentiales_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publisherVersionhttps://doi.org/10.1016/j.physa.2022.128280es_ES
dc.rights.accessRightsopenAccesses_ES
dc.identifier.DOI10.1016/j.physa.2022.128280
dc.type.versionpublishedVersiones_ES


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