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Competing coexisting phases in 2D water
The properties of bulk water come from a delicate balance of interactions on length scales encompassing several orders of magnitudes: i) the Hydrogen Bond (HBond) at the molecular scale and ii) the extension of this HBond network up to the macroscopic level. Here, we address the physics of water whe...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4869029/ https://www.ncbi.nlm.nih.gov/pubmed/27185018 http://dx.doi.org/10.1038/srep25938 |
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author | Zanotti, Jean-Marc Judeinstein, Patrick Dalla-Bernardina, Simona Creff, Gaëlle Brubach, Jean-Blaise Roy, Pascale Bonetti, Marco Ollivier, Jacques Sakellariou, Dimitrios Bellissent-Funel, Marie-Claire |
author_facet | Zanotti, Jean-Marc Judeinstein, Patrick Dalla-Bernardina, Simona Creff, Gaëlle Brubach, Jean-Blaise Roy, Pascale Bonetti, Marco Ollivier, Jacques Sakellariou, Dimitrios Bellissent-Funel, Marie-Claire |
author_sort | Zanotti, Jean-Marc |
collection | PubMed |
description | The properties of bulk water come from a delicate balance of interactions on length scales encompassing several orders of magnitudes: i) the Hydrogen Bond (HBond) at the molecular scale and ii) the extension of this HBond network up to the macroscopic level. Here, we address the physics of water when the three dimensional extension of the HBond network is frustrated, so that the water molecules are forced to organize in only two dimensions. We account for the large scale fluctuating HBond network by an analytical mean-field percolation model. This approach provides a coherent interpretation of the different events experimentally (calorimetry, neutron, NMR, near and far infra-red spectroscopies) detected in interfacial water at 160, 220 and 250 K. Starting from an amorphous state of water at low temperature, these transitions are respectively interpreted as the onset of creation of transient low density patches of 4-HBonded molecules at 160 K, the percolation of these domains at 220 K and finally the total invasion of the surface by them at 250 K. The source of this surprising behaviour in 2D is the frustration of the natural bulk tetrahedral local geometry and the underlying very significant increase in entropy of the interfacial water molecules. |
format | Online Article Text |
id | pubmed-4869029 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-48690292016-06-01 Competing coexisting phases in 2D water Zanotti, Jean-Marc Judeinstein, Patrick Dalla-Bernardina, Simona Creff, Gaëlle Brubach, Jean-Blaise Roy, Pascale Bonetti, Marco Ollivier, Jacques Sakellariou, Dimitrios Bellissent-Funel, Marie-Claire Sci Rep Article The properties of bulk water come from a delicate balance of interactions on length scales encompassing several orders of magnitudes: i) the Hydrogen Bond (HBond) at the molecular scale and ii) the extension of this HBond network up to the macroscopic level. Here, we address the physics of water when the three dimensional extension of the HBond network is frustrated, so that the water molecules are forced to organize in only two dimensions. We account for the large scale fluctuating HBond network by an analytical mean-field percolation model. This approach provides a coherent interpretation of the different events experimentally (calorimetry, neutron, NMR, near and far infra-red spectroscopies) detected in interfacial water at 160, 220 and 250 K. Starting from an amorphous state of water at low temperature, these transitions are respectively interpreted as the onset of creation of transient low density patches of 4-HBonded molecules at 160 K, the percolation of these domains at 220 K and finally the total invasion of the surface by them at 250 K. The source of this surprising behaviour in 2D is the frustration of the natural bulk tetrahedral local geometry and the underlying very significant increase in entropy of the interfacial water molecules. Nature Publishing Group 2016-05-17 /pmc/articles/PMC4869029/ /pubmed/27185018 http://dx.doi.org/10.1038/srep25938 Text en Copyright © 2016, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Zanotti, Jean-Marc Judeinstein, Patrick Dalla-Bernardina, Simona Creff, Gaëlle Brubach, Jean-Blaise Roy, Pascale Bonetti, Marco Ollivier, Jacques Sakellariou, Dimitrios Bellissent-Funel, Marie-Claire Competing coexisting phases in 2D water |
title | Competing coexisting phases in 2D water |
title_full | Competing coexisting phases in 2D water |
title_fullStr | Competing coexisting phases in 2D water |
title_full_unstemmed | Competing coexisting phases in 2D water |
title_short | Competing coexisting phases in 2D water |
title_sort | competing coexisting phases in 2d water |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4869029/ https://www.ncbi.nlm.nih.gov/pubmed/27185018 http://dx.doi.org/10.1038/srep25938 |
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