Publicação: Modeling the camel-to-bell shape transition of the differential capacitance using mean-field theory and Monte Carlo simulations
dc.contributor.author | Bossa, Guilherme V. [UNESP] | |
dc.contributor.author | Caetano, Daniel L. Z. [UNESP] | |
dc.contributor.author | de Carvalho, Sidney J. [UNESP] | |
dc.contributor.author | Bohinc, Klemen | |
dc.contributor.author | May, Sylvio | |
dc.contributor.institution | North Dakota State University | |
dc.contributor.institution | Universidade Estadual Paulista (Unesp) | |
dc.contributor.institution | University of Ljubljana | |
dc.date.accessioned | 2019-10-06T15:19:07Z | |
dc.date.available | 2019-10-06T15:19:07Z | |
dc.date.issued | 2018-09-01 | |
dc.description.abstract | Abstract.: 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.affiliation | Department of Physics North Dakota State University | |
dc.description.affiliation | Department of Physics São Paulo State University (UNESP) Institute of Biosciences Humanities and Exact Sciences | |
dc.description.affiliation | Faculty of Health Sciences University of Ljubljana, Poljanska 26a | |
dc.description.affiliationUnesp | Department of Physics São Paulo State University (UNESP) Institute of Biosciences Humanities and Exact Sciences | |
dc.identifier | http://dx.doi.org/10.1140/epje/i2018-11723-7 | |
dc.identifier.citation | European Physical Journal E, v. 41, n. 9, 2018. | |
dc.identifier.doi | 10.1140/epje/i2018-11723-7 | |
dc.identifier.issn | 1292-895X | |
dc.identifier.issn | 1292-8941 | |
dc.identifier.scopus | 2-s2.0-85053922139 | |
dc.identifier.uri | http://hdl.handle.net/11449/186897 | |
dc.language.iso | eng | |
dc.relation.ispartof | European Physical Journal E | |
dc.rights.accessRights | Acesso aberto | pt |
dc.source | Scopus | |
dc.subject | Soft Matter: Interfacial Phenomena and Nanostructured Surfaces | |
dc.title | Modeling the camel-to-bell shape transition of the differential capacitance using mean-field theory and Monte Carlo simulations | en |
dc.type | Artigo | pt |
dspace.entity.type | Publication | |
unesp.campus | Universidade Estadual Paulista (UNESP), Instituto de Biociências, Letras e Ciências Exatas, São José do Rio Preto | pt |