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Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)

[Image: see text] The preparation of pure cubic ice without hexagonal stacking faults has been realized only recently by del Rosso et al. (Nat. Mater.2020, 19, 663−66832015533) and Komatsu et al. (Nat. Commun.2020, 11, 46432015342). With our present calorimetric study on the transition from pure cub...

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Autores principales: Tonauer, Christina M., Yamashita, Keishiro, Rosso, Leonardo del, Celli, Milva, Loerting, Thomas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10240532/
https://www.ncbi.nlm.nih.gov/pubmed/37227149
http://dx.doi.org/10.1021/acs.jpclett.3c00408
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author Tonauer, Christina M.
Yamashita, Keishiro
Rosso, Leonardo del
Celli, Milva
Loerting, Thomas
author_facet Tonauer, Christina M.
Yamashita, Keishiro
Rosso, Leonardo del
Celli, Milva
Loerting, Thomas
author_sort Tonauer, Christina M.
collection PubMed
description [Image: see text] The preparation of pure cubic ice without hexagonal stacking faults has been realized only recently by del Rosso et al. (Nat. Mater.2020, 19, 663−66832015533) and Komatsu et al. (Nat. Commun.2020, 11, 46432015342). With our present calorimetric study on the transition from pure cubic ice to hexagonal ice we are able to clarify the value of the enthalpy change ΔH(c→h) to be −37.7 ± 2.3 J mol(–1). The transition temperature is identified as 226 K, much higher than in previous work on ice I(sd). This is due to a catalytic effect of hexagonal faults on the transition, but even more importantly due to a relaxation exotherm that was not properly identified in the past.
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spelling pubmed-102405322023-06-06 Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h) Tonauer, Christina M. Yamashita, Keishiro Rosso, Leonardo del Celli, Milva Loerting, Thomas J Phys Chem Lett [Image: see text] The preparation of pure cubic ice without hexagonal stacking faults has been realized only recently by del Rosso et al. (Nat. Mater.2020, 19, 663−66832015533) and Komatsu et al. (Nat. Commun.2020, 11, 46432015342). With our present calorimetric study on the transition from pure cubic ice to hexagonal ice we are able to clarify the value of the enthalpy change ΔH(c→h) to be −37.7 ± 2.3 J mol(–1). The transition temperature is identified as 226 K, much higher than in previous work on ice I(sd). This is due to a catalytic effect of hexagonal faults on the transition, but even more importantly due to a relaxation exotherm that was not properly identified in the past. American Chemical Society 2023-05-25 /pmc/articles/PMC10240532/ /pubmed/37227149 http://dx.doi.org/10.1021/acs.jpclett.3c00408 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Tonauer, Christina M.
Yamashita, Keishiro
Rosso, Leonardo del
Celli, Milva
Loerting, Thomas
Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title_full Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title_fullStr Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title_full_unstemmed Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title_short Enthalpy Change from Pure Cubic Ice I(c) to Hexagonal Ice I(h)
title_sort enthalpy change from pure cubic ice i(c) to hexagonal ice i(h)
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10240532/
https://www.ncbi.nlm.nih.gov/pubmed/37227149
http://dx.doi.org/10.1021/acs.jpclett.3c00408
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