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Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity
Regelation, i.e., ice melts under compression and freezes again when the pressure is relieved, remains puzzling since its discovery in 1850’s by Faraday. Here we show that hydrogen bond (O:H-O) cooperativity and its extraordinary recoverability resolve this anomaly. The H-O bond and the O:H nonbond...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4563362/ https://www.ncbi.nlm.nih.gov/pubmed/26351109 http://dx.doi.org/10.1038/srep13655 |
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author | Zhang, Xi Huang, Yongli Sun, Peng Liu, Xinjuan Ma, Zengsheng Zhou, Yichun Zhou, Ji Zheng, Weitao Sun, Chang Q. |
author_facet | Zhang, Xi Huang, Yongli Sun, Peng Liu, Xinjuan Ma, Zengsheng Zhou, Yichun Zhou, Ji Zheng, Weitao Sun, Chang Q. |
author_sort | Zhang, Xi |
collection | PubMed |
description | Regelation, i.e., ice melts under compression and freezes again when the pressure is relieved, remains puzzling since its discovery in 1850’s by Faraday. Here we show that hydrogen bond (O:H-O) cooperativity and its extraordinary recoverability resolve this anomaly. The H-O bond and the O:H nonbond possesses each a specific heat η(x)(T/Θ(Dx)) whose Debye temperature Θ(Dx) is proportional to its characteristic phonon frequency ω(x) according to Einstein’s relationship. A superposition of the η(x)(T/Θ(Dx)) curves for the H-O bond (x = H, ω(H) ~ 3200 cm(−1)) and the O:H nonbond (x = L, ω(L) ~ 200 cm(−1), Θ(DL) = 198 K) yields two intersecting temperatures that define the liquid/quasisolid/solid phase boundaries. Compression shortens the O:H nonbond and stiffens its phonon but does the opposite to the H-O bond through O-O Coulomb repulsion, which closes up the intersection temperatures and hence depress the melting temperature of quasisolid ice. Reproduction of the T(m)(P) profile clarifies that the H-O bond energy E(H) determines the T(m) with derivative of E(H) = 3.97 eV for bulk water and ice. Oxygen atom always finds bonding partners to retain its sp(3)-orbital hybridization once the O:H breaks, which ensures O:H-O bond recoverability to its original state once the pressure is relieved. |
format | Online Article Text |
id | pubmed-4563362 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-45633622015-09-15 Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity Zhang, Xi Huang, Yongli Sun, Peng Liu, Xinjuan Ma, Zengsheng Zhou, Yichun Zhou, Ji Zheng, Weitao Sun, Chang Q. Sci Rep Article Regelation, i.e., ice melts under compression and freezes again when the pressure is relieved, remains puzzling since its discovery in 1850’s by Faraday. Here we show that hydrogen bond (O:H-O) cooperativity and its extraordinary recoverability resolve this anomaly. The H-O bond and the O:H nonbond possesses each a specific heat η(x)(T/Θ(Dx)) whose Debye temperature Θ(Dx) is proportional to its characteristic phonon frequency ω(x) according to Einstein’s relationship. A superposition of the η(x)(T/Θ(Dx)) curves for the H-O bond (x = H, ω(H) ~ 3200 cm(−1)) and the O:H nonbond (x = L, ω(L) ~ 200 cm(−1), Θ(DL) = 198 K) yields two intersecting temperatures that define the liquid/quasisolid/solid phase boundaries. Compression shortens the O:H nonbond and stiffens its phonon but does the opposite to the H-O bond through O-O Coulomb repulsion, which closes up the intersection temperatures and hence depress the melting temperature of quasisolid ice. Reproduction of the T(m)(P) profile clarifies that the H-O bond energy E(H) determines the T(m) with derivative of E(H) = 3.97 eV for bulk water and ice. Oxygen atom always finds bonding partners to retain its sp(3)-orbital hybridization once the O:H breaks, which ensures O:H-O bond recoverability to its original state once the pressure is relieved. Nature Publishing Group 2015-09-09 /pmc/articles/PMC4563362/ /pubmed/26351109 http://dx.doi.org/10.1038/srep13655 Text en Copyright © 2015, 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 Zhang, Xi Huang, Yongli Sun, Peng Liu, Xinjuan Ma, Zengsheng Zhou, Yichun Zhou, Ji Zheng, Weitao Sun, Chang Q. Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title | Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title_full | Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title_fullStr | Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title_full_unstemmed | Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title_short | Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
title_sort | ice regelation: hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4563362/ https://www.ncbi.nlm.nih.gov/pubmed/26351109 http://dx.doi.org/10.1038/srep13655 |
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