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通过分子动力学模拟研究溶剂化壳层动力学与超临界水和苯的平动及转动动力学的关系。

Solvation shell dynamics studied by molecular dynamics simulation in relation to the translational and rotational dynamics of supercritical water and benzene.

作者信息

Yoshida Ken, Matubayasi Nobuyuki, Nakahara Masaru

机构信息

Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan.

出版信息

J Chem Phys. 2007 Nov 7;127(17):174509. doi: 10.1063/1.2780871.

DOI:10.1063/1.2780871
PMID:17994829
Abstract

The solvation shell dynamics of supercritical water is analyzed by molecular dynamics simulation with emphasis on its relationship to the translational and rotational dynamics. The relaxation times of the solvation number (tau S), the velocity autocorrelation function (tau D), the angular momentum correlation function (tau J), and the second-order reorientational correlation function (tau 2R) are studied at a supercritical temperature of 400 degrees C over a wide density region of 0.01-1.5 g cm(-3). The relaxation times are decomposed into those conditioned by the solvation number n, and the effect of the short-ranged structure is examined in terms of its probability Pn of occurrence. In the low to medium-density range of 0.01-0.4 g cm(-3), the time scales of water dynamics are in the following sequence: tau D>tau S approximately or > tau J approximately or > tau 2R. This means that the rotation in supercritical water is of the "in-shell" type while the translational diffusion is not. The comparison to supercritical benzene is also performed and the effect of hydrogen bonding is examined. The water diffusion is not of the in-shell type up to the ambient density of 1.0 g cm(-3), which corresponds to the absence of the transition from the collision to the Brownian picture, whereas such transition is present in the case of benzene. The absence of the transition in water comes from the fast reorganization of the hydrogen bonds and the enhanced mobility of the solvation shell in supercritical conditions.

摘要

通过分子动力学模拟分析了超临界水的溶剂化壳层动力学,重点关注其与平动和转动动力学的关系。在400℃的超临界温度下,于0.01 - 1.5 g cm⁻³的宽密度范围内研究了溶剂化数的弛豫时间(τS)、速度自相关函数(τD)、角动量相关函数(τJ)和二阶重取向相关函数(τ2R)。将弛豫时间分解为由溶剂化数n决定的那些,并根据其出现概率Pn来考察短程结构的影响。在0.01 - 0.4 g cm⁻³的低至中密度范围内,水动力学的时间尺度顺序如下:τD > τS ≈ τJ ≈ τ2R。这意味着超临界水中的转动是“壳内”型的,而平动扩散不是。还进行了与超临界苯的比较,并考察了氢键的影响。直至1.0 g cm⁻³的环境密度,水的扩散都不是壳内型的,这对应于从碰撞图像到布朗图像的转变不存在,而在苯的情况下存在这种转变。水中这种转变的不存在源于氢键的快速重组以及超临界条件下溶剂化壳层流动性的增强。

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