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...

全面介紹

Saved in:
書目詳細資料
Main Authors: Zhang, Xi, Huang, Yongli, Sun, Peng, Liu, Xinjuan, Ma, Zengsheng, Zhou, Yichun, Zhou, Ji, Zheng, Weitao, Sun, Chang Qing
其他作者: School of Electrical and Electronic Engineering
格式: Article
語言:English
出版: 2015
在線閱讀:https://hdl.handle.net/10356/103525
http://hdl.handle.net/10220/38766
標簽: 添加標簽
沒有標簽, 成為第一個標記此記錄!
id sg-ntu-dr.10356-103525
record_format dspace
spelling sg-ntu-dr.10356-1035252022-02-16T16:29:57Z 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 Qing School of Electrical and Electronic Engineering 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 ηx(T/ΘDx) whose Debye temperature ΘDx is proportional to its characteristic phonon frequency ωx according to Einstein’s relationship. A superposition of the ηx(T/ΘDx) curves for the H-O bond (x = H, ωH ~ 3200 cm−1) and the O:H nonbond (x = L, ωL ~ 200 cm−1, ΘDL = 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 Tm(P) profile clarifies that the H-O bond energy EH determines the Tm with derivative of EH = 3.97 eV for bulk water and ice. Oxygen atom always finds bonding partners to retain its sp3-orbital hybridization once the O:H breaks, which ensures O:H-O bond recoverability to its original state once the pressure is relieved. Published version 2015-10-01T07:24:45Z 2019-12-06T21:14:33Z 2015-10-01T07:24:45Z 2019-12-06T21:14:33Z 2015 2015 Journal Article Zhang, X., Huang, Y., Sun, P., Liu, X., Ma, Z., Zhou, Y., et al. (2015). Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity. Scientific Reports, 5, 13655-. 2045-2322 https://hdl.handle.net/10356/103525 http://hdl.handle.net/10220/38766 10.1038/srep13655 26351109 en Scientific Reports 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/ application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
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 ηx(T/ΘDx) whose Debye temperature ΘDx is proportional to its characteristic phonon frequency ωx according to Einstein’s relationship. A superposition of the ηx(T/ΘDx) curves for the H-O bond (x = H, ωH ~ 3200 cm−1) and the O:H nonbond (x = L, ωL ~ 200 cm−1, ΘDL = 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 Tm(P) profile clarifies that the H-O bond energy EH determines the Tm with derivative of EH = 3.97 eV for bulk water and ice. Oxygen atom always finds bonding partners to retain its sp3-orbital hybridization once the O:H breaks, which ensures O:H-O bond recoverability to its original state once the pressure is relieved.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Zhang, Xi
Huang, Yongli
Sun, Peng
Liu, Xinjuan
Ma, Zengsheng
Zhou, Yichun
Zhou, Ji
Zheng, Weitao
Sun, Chang Qing
format Article
author Zhang, Xi
Huang, Yongli
Sun, Peng
Liu, Xinjuan
Ma, Zengsheng
Zhou, Yichun
Zhou, Ji
Zheng, Weitao
Sun, Chang Qing
spellingShingle Zhang, Xi
Huang, Yongli
Sun, Peng
Liu, Xinjuan
Ma, Zengsheng
Zhou, Yichun
Zhou, Ji
Zheng, Weitao
Sun, Chang Qing
Ice Regelation: Hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity
author_sort Zhang, Xi
title 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_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_sort ice regelation: hydrogen-bond extraordinary recoverability and water quasisolid-phase-boundary dispersivity
publishDate 2015
url https://hdl.handle.net/10356/103525
http://hdl.handle.net/10220/38766
_version_ 1725985532095234048