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A Model for Non-Arrhenius Ionic Conductivity

Non-Arrhenius ionic conductivity is observed in various solid electrolytes. The behavior is intriguing, because it limits the magnitude of ionic conductivity at high temperatures. Understanding the nature of this behavior is of fundamental interest and deserves attention. In the present study, the t...

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Autores principales: Aniya, Masaru, Ikeda, Masahiro
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6630995/
https://www.ncbi.nlm.nih.gov/pubmed/31238516
http://dx.doi.org/10.3390/nano9060911
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author Aniya, Masaru
Ikeda, Masahiro
author_facet Aniya, Masaru
Ikeda, Masahiro
author_sort Aniya, Masaru
collection PubMed
description Non-Arrhenius ionic conductivity is observed in various solid electrolytes. The behavior is intriguing, because it limits the magnitude of ionic conductivity at high temperatures. Understanding the nature of this behavior is of fundamental interest and deserves attention. In the present study, the temperature dependence of the ionic conductivity in solids and liquids is analyzed using the Bond Strength–Coordination Number Fluctuation (BSCNF) model developed by ourselves. It is shown that our model describes well the temperature dependence of ionic conductivity that varies from Arrhenius to non-Arrhenius-type behavior. According to our model, the non-Arrhenius behavior is controlled by the degree of binding energy fluctuation between the mobile species and the surroundings. A brief discussion on a possible size effect in non-Arrhenius behavior is also given. Within the available data, the BSCNF model suggests that the size effect in the degree of the non-Arrhenius mass transport behavior in a poly (methyl ethyl ether)/polystyrene (PVME/PS) blend is different from that in a-polystyrene and polyamide copolymer PA66/6I.
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spelling pubmed-66309952019-08-19 A Model for Non-Arrhenius Ionic Conductivity Aniya, Masaru Ikeda, Masahiro Nanomaterials (Basel) Article Non-Arrhenius ionic conductivity is observed in various solid electrolytes. The behavior is intriguing, because it limits the magnitude of ionic conductivity at high temperatures. Understanding the nature of this behavior is of fundamental interest and deserves attention. In the present study, the temperature dependence of the ionic conductivity in solids and liquids is analyzed using the Bond Strength–Coordination Number Fluctuation (BSCNF) model developed by ourselves. It is shown that our model describes well the temperature dependence of ionic conductivity that varies from Arrhenius to non-Arrhenius-type behavior. According to our model, the non-Arrhenius behavior is controlled by the degree of binding energy fluctuation between the mobile species and the surroundings. A brief discussion on a possible size effect in non-Arrhenius behavior is also given. Within the available data, the BSCNF model suggests that the size effect in the degree of the non-Arrhenius mass transport behavior in a poly (methyl ethyl ether)/polystyrene (PVME/PS) blend is different from that in a-polystyrene and polyamide copolymer PA66/6I. MDPI 2019-06-24 /pmc/articles/PMC6630995/ /pubmed/31238516 http://dx.doi.org/10.3390/nano9060911 Text en © 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Aniya, Masaru
Ikeda, Masahiro
A Model for Non-Arrhenius Ionic Conductivity
title A Model for Non-Arrhenius Ionic Conductivity
title_full A Model for Non-Arrhenius Ionic Conductivity
title_fullStr A Model for Non-Arrhenius Ionic Conductivity
title_full_unstemmed A Model for Non-Arrhenius Ionic Conductivity
title_short A Model for Non-Arrhenius Ionic Conductivity
title_sort model for non-arrhenius ionic conductivity
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6630995/
https://www.ncbi.nlm.nih.gov/pubmed/31238516
http://dx.doi.org/10.3390/nano9060911
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