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Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)]
Ionic liquids have been suggested as new engineering fluids, namely in the area of heat transfer, as alternatives to current biphenyl and diphenyl oxide, alkylated aromatics and dimethyl polysiloxane oils, which degrade above 200 °C and pose some environmental problems. Recently, we have proposed 1-...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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MDPI
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7570973/ https://www.ncbi.nlm.nih.gov/pubmed/32962096 http://dx.doi.org/10.3390/molecules25184290 |
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author | Lozano-Martín, Daniel Inês Cardoso Vieira, Salomé Paredes, Xavier Vitoriano Lourenço, Maria José Nieto de Castro, Carlos A. Sengers, Jan V. Massonne, Klemens |
author_facet | Lozano-Martín, Daniel Inês Cardoso Vieira, Salomé Paredes, Xavier Vitoriano Lourenço, Maria José Nieto de Castro, Carlos A. Sengers, Jan V. Massonne, Klemens |
author_sort | Lozano-Martín, Daniel |
collection | PubMed |
description | Ionic liquids have been suggested as new engineering fluids, namely in the area of heat transfer, as alternatives to current biphenyl and diphenyl oxide, alkylated aromatics and dimethyl polysiloxane oils, which degrade above 200 °C and pose some environmental problems. Recently, we have proposed 1-ethyl-3-methylimidazolium methanesulfonate, [C(2)mim][CH(3)SO(3)], as a new heat transfer fluid, because of its thermophysical and toxicological properties. However, there are some interesting points raised in this work, namely the possibility of the existence of liquid metastability below the melting point (303 K) or second order-disorder transitions (λ-type) before reaching the calorimetric freezing point. This paper analyses in more detail this zone of the phase diagram of the pure fluid, by reporting accurate thermal-conductivity measurements between 278 and 355 K with an estimated uncertainty of 2% at a 95% confidence level. A new value of the melting temperature is also reported, T(melt) = 307.8 ± 1 K. Results obtained support liquid metastability behaviour in the solid-phase region and permit the use of this ionic liquid at a heat transfer fluid at temperatures below its melting point. Thermal conductivity models based on Bridgman theory and estimation formulas were also used in this work, failing to predict the experimental data within its uncertainty. |
format | Online Article Text |
id | pubmed-7570973 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-75709732020-10-28 Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] Lozano-Martín, Daniel Inês Cardoso Vieira, Salomé Paredes, Xavier Vitoriano Lourenço, Maria José Nieto de Castro, Carlos A. Sengers, Jan V. Massonne, Klemens Molecules Article Ionic liquids have been suggested as new engineering fluids, namely in the area of heat transfer, as alternatives to current biphenyl and diphenyl oxide, alkylated aromatics and dimethyl polysiloxane oils, which degrade above 200 °C and pose some environmental problems. Recently, we have proposed 1-ethyl-3-methylimidazolium methanesulfonate, [C(2)mim][CH(3)SO(3)], as a new heat transfer fluid, because of its thermophysical and toxicological properties. However, there are some interesting points raised in this work, namely the possibility of the existence of liquid metastability below the melting point (303 K) or second order-disorder transitions (λ-type) before reaching the calorimetric freezing point. This paper analyses in more detail this zone of the phase diagram of the pure fluid, by reporting accurate thermal-conductivity measurements between 278 and 355 K with an estimated uncertainty of 2% at a 95% confidence level. A new value of the melting temperature is also reported, T(melt) = 307.8 ± 1 K. Results obtained support liquid metastability behaviour in the solid-phase region and permit the use of this ionic liquid at a heat transfer fluid at temperatures below its melting point. Thermal conductivity models based on Bridgman theory and estimation formulas were also used in this work, failing to predict the experimental data within its uncertainty. MDPI 2020-09-18 /pmc/articles/PMC7570973/ /pubmed/32962096 http://dx.doi.org/10.3390/molecules25184290 Text en © 2020 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 Lozano-Martín, Daniel Inês Cardoso Vieira, Salomé Paredes, Xavier Vitoriano Lourenço, Maria José Nieto de Castro, Carlos A. Sengers, Jan V. Massonne, Klemens Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title | Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title_full | Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title_fullStr | Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title_full_unstemmed | Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title_short | Thermal Conductivity of Metastable Ionic Liquid [C(2)mim][CH(3)SO(3)] |
title_sort | thermal conductivity of metastable ionic liquid [c(2)mim][ch(3)so(3)] |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7570973/ https://www.ncbi.nlm.nih.gov/pubmed/32962096 http://dx.doi.org/10.3390/molecules25184290 |
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