Freezing, melting and structure of ice in a hydrophilic nanopore

纳米孔 熔点 成核 结晶学 材料科学 回转半径 单层 结晶 无定形冰 冰Ih 中子衍射 分子动力学 堆积 冰晶 冰点 分子 化学物理 化学 热力学 晶体结构 纳米技术 复合材料 无定形固体 有机化学 计算化学 聚合物 物理 光学
作者
Emily B. Moore,Ezequiel de la Llave,Kai Welke,Damián A. Scherlis,Valeria Molinero
出处
期刊:Physical Chemistry Chemical Physics [The Royal Society of Chemistry]
卷期号:12 (16): 4124-4124 被引量:289
标识
DOI:10.1039/b919724a
摘要

The nucleation, growth, structure and melting of ice in 3 nm diameter hydrophilic nanopores are studied through molecular dynamics simulations with the mW water model. The melting temperature of water in the pore was T(m)(pore) = 223 K, 51 K lower than the melting point of bulk water in the model and in excellent agreement with experimental determinations for 3 nm silica pores. Liquid and ice coexist in equilibrium at the melting point and down to temperatures as low as 180 K. Liquid water is located at the interface of the pore wall, increasing from one monolayer at the freezing temperature, T(f)(pore) = 195 K, to two monolayers a few degrees below T(m)(pore). Crystallization of ice in the pore occurs through homogeneous nucleation. At the freezing temperature, the critical nucleus contains approximately 75 to 100 molecules, with a radius of gyration similar to the radius of the pore. The critical nuclei contain features of both cubic and hexagonal ice, although stacking of hexagonal and cubic layers is not defined until the nuclei reach approximately 150 molecules. The structure of the confined ice is rich in stacking faults, in agreement with the interpretation of X-ray and neutron diffraction experiments. Though the presence of cubic layers is twice as prevalent as hexagonal ones, the crystals should not be considered defective Ic as sequences with more than three adjacent cubic (or hexagonal) layers are extremely rare in the confined ice.
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