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Modeling the camel-to-bell shape transition of the differential capacitance using mean-field theory and Monte Carlo simulations

dc.contributor.authorBossa, Guilherme V. [UNESP]
dc.contributor.authorCaetano, Daniel L. Z. [UNESP]
dc.contributor.authorde Carvalho, Sidney J. [UNESP]
dc.contributor.authorBohinc, Klemen
dc.contributor.authorMay, Sylvio
dc.contributor.institutionNorth Dakota State University
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.contributor.institutionUniversity of Ljubljana
dc.date.accessioned2019-10-06T15:19:07Z
dc.date.available2019-10-06T15:19:07Z
dc.date.issued2018-09-01
dc.description.abstractAbstract.: Mean-field electrostatics is used to calculate the differential capacitance of an electric double layer formed at a planar electrode in a symmetric 1:1 electrolyte. Assuming the electrolyte is also ion-size symmetric, we derive analytic expressions for the differential capacitance valid up to fourth order in the surface charge density or surface potential. Our mean-field model accounts exclusively for electrostatic interactions but includes an arbitrary non-ideality in the mixing entropy of the mobile ions. The ensuing criterion for the camel-to-bell shape transition of the differential capacitance is analyzed using commonly used mixing models (one based on a lattice gas and the other based on the Carnahan-Starling equation of state) and compared with Monte Carlo simulations. We observe a reasonable agreement between all our mean-field models and the simulation data for the camel-to-bell shape transition. The absolute value of the differential capacitance for an uncharged (or weakly charged) electrode is, however, not reproduced by our mean-field approaches, not even upon introducing a Stern layer with a thickness equal of the ion radius. We show that, if a Stern layer is introduced, its thickness dependence on the ion size is non-monotonic or, depending on the salt concentration, even inversely proportional.en
dc.description.affiliationDepartment of Physics North Dakota State University
dc.description.affiliationDepartment of Physics São Paulo State University (UNESP) Institute of Biosciences Humanities and Exact Sciences
dc.description.affiliationFaculty of Health Sciences University of Ljubljana, Poljanska 26a
dc.description.affiliationUnespDepartment of Physics São Paulo State University (UNESP) Institute of Biosciences Humanities and Exact Sciences
dc.identifierhttp://dx.doi.org/10.1140/epje/i2018-11723-7
dc.identifier.citationEuropean Physical Journal E, v. 41, n. 9, 2018.
dc.identifier.doi10.1140/epje/i2018-11723-7
dc.identifier.issn1292-895X
dc.identifier.issn1292-8941
dc.identifier.scopus2-s2.0-85053922139
dc.identifier.urihttp://hdl.handle.net/11449/186897
dc.language.isoeng
dc.relation.ispartofEuropean Physical Journal E
dc.rights.accessRightsAcesso abertopt
dc.sourceScopus
dc.subjectSoft Matter: Interfacial Phenomena and Nanostructured Surfaces
dc.titleModeling the camel-to-bell shape transition of the differential capacitance using mean-field theory and Monte Carlo simulationsen
dc.typeArtigopt
dspace.entity.typePublication
unesp.campusUniversidade Estadual Paulista (UNESP), Instituto de Biociências, Letras e Ciências Exatas, São José do Rio Pretopt

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