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双层冰相变的微秒级分子动力学模拟:受限水中的动力学约束

Microsecond-Scale Molecular Dynamics Simulation of Phase Transition of a Bilayer Ice: Kinetic Constraints in Confined Water.

作者信息

Zhu Weiduo, Li Yiyao, Wang Haidi, Chen Zhao, Liu Xiaofeng, Li Zhongjun, Zhao Wenhui, Zeng Xiao Cheng

机构信息

Department of Physics, Hefei University of Technology, Hefei, Anhui 230009, China.

Department of Materials Science & Engineering, City University of Hong Kong, Kowloon, Hong Kong 999077, China.

出版信息

J Phys Chem B. 2025 Jun 19;129(24):5989-5997. doi: 10.1021/acs.jpcb.5c01346. Epub 2025 Jun 9.

DOI:10.1021/acs.jpcb.5c01346
PMID:40489677
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12183707/
Abstract

In this study, we investigate the phase behavior of water confined between two parallel smooth walls by using both classical molecular dynamics (MD) simulations and machine-learned potential (MLP) MD simulations. Particular attention is focused toward the water-to-ice phase transition below the freezing point. Three distinct two-dimensional (2D) bilayer (BL) crystalline ice phases are observed, namely, bilayer hexagonal ice (BL-ice I), bilayer very high-density ice (BL-VHDI), and a newly found bilayer penta-hexa ice (BL-PHI). The latter consists of interlocked pentagonal and hexagonal rings. The transition from liquid to BL-PHI is weakly first-order, and typically, the BL-PHI emerges at intermediate to high lateral pressures (400 to 900 MPa) after microsecond-scale simulations, highlighting its relatively slow formation process. Compared to BL-ice I and BL-VHDI, BL-PHI exhibits much higher diffusion activation energy and hence a much slower freezing rate. Additionally, the transition temperatures of all three bilayer ices are pressure-dependent. These findings provide new insights into the complex behavior of nanoconfined water.

摘要

在本研究中,我们通过使用经典分子动力学(MD)模拟和机器学习势(MLP)MD模拟,研究了限制在两个平行光滑壁之间的水的相行为。特别关注低于冰点的水到冰的相变。观察到三种不同的二维(2D)双层(BL)结晶冰相,即双层六方冰(BL-冰I)、双层极高密度冰(BL-VHDI)和新发现的双层五-六冰(BL-PHI)。后者由互锁的五边形和六边形环组成。从液体到BL-PHI的转变是弱一级的,通常在微秒级模拟后,BL-PHI在中等至高横向压力(400至900MPa)下出现,突出了其相对缓慢的形成过程。与BL-冰I和BL-VHDI相比,BL-PHI表现出更高的扩散活化能,因此冻结速率更慢。此外,所有三种双层冰的转变温度都与压力有关。这些发现为纳米限域水的复杂行为提供了新的见解。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/cbbc777657e4/jp5c01346_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/ae3495137045/jp5c01346_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/93f667f25868/jp5c01346_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/860c83a305ca/jp5c01346_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/12915f054ae1/jp5c01346_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/ce82bdc09891/jp5c01346_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/cbbc777657e4/jp5c01346_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/ae3495137045/jp5c01346_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/93f667f25868/jp5c01346_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/860c83a305ca/jp5c01346_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/12915f054ae1/jp5c01346_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/ce82bdc09891/jp5c01346_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4431/12183707/cbbc777657e4/jp5c01346_0006.jpg

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本文引用的文献

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