Ethylene glycol revisited: Molecular dynamics simulations liquid and its hydrogen-bond network

被引:57
|
作者
Kaiser, Alexander [1 ]
Ismailova, Oksana [1 ,2 ]
Koskela, Antti [3 ]
Huber, Stefan E. [1 ]
Ritter, Marcel [4 ]
Cosenza, Biagio [5 ]
Benger, Werner [6 ]
Nazmutdinov, Renat [7 ]
Probst, Michael [1 ]
机构
[1] Univ Innsbruck, Inst Ion Phys & Appl Phys, A-6020 Innsbruck, Austria
[2] Uzbek Acad Sci, Inst Ion Plasma & Laser Technol, Tashkent, Uzbekistan
[3] Univ Innsbruck, Inst Math, A-6020 Innsbruck, Austria
[4] Univ Innsbruck, Inst Basic Sci Engn Sci, A-6020 Innsbruck, Austria
[5] Univ Innsbruck, Inst Comp Sci, A-6020 Innsbruck, Austria
[6] Louisiana State Univ, Ctr Computat & Technol, Baton Rouge, LA 70803 USA
[7] Kazan Natl Res Technol Univ, Kazan 420015, Republic Of Tat, Russia
基金
奥地利科学基金会;
关键词
Ethylene glycol; Molecular dynamics; OPLS-AA force fields; Hydrogen-bonds; Visualization; FORCE-FIELD; CONFORMATIONAL-ANALYSIS; MIXTURES; ALCOHOLS; ENERGY;
D O I
10.1016/j.molliq.2013.05.033
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Molecular dynamics simulations of liquid ethylene glycol described by the OPLS-AA force field were performed to gain insight into its hydrogen-bond structure. We use the population correlation function as a statistical measure for the hydrogen-bond lifetime. In an attempt to understand the complicated hydrogen-bonding, we developed new molecular visualization tools within the Vish Visualization shell and used it to visualize the life of each individual hydrogen-bond. With this tool hydrogen-bond formation and breaking as well as clustering and chain formation in hydrogen-bonded liquids can be observed directly. Liquid ethylene glycol at room temperature does not show significant clustering or chain building. The hydrogen-bonds break often due to the rotational and vibrational motions of the molecules leading to an H-bond half-life time of approximately 1.5 Ps. However, most of the H-bonds are reformed again so that after 50 ps only 40% of these H-bonds are irreversibly broken due to diffusional motion. This hydrogen-bond half-life time due to diffusional motion is 80.3 Ps. The work was preceded by a careful check of various OPLS-based force fields used in the literature. It was found that they lead to quite different angular and H-bond distributions. (C) 2013 The Authors. Published by Elsevier B.V. All rights reserved.
引用
收藏
页码:20 / 29
页数:10
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