Department of Process Engineering and Applied Science, Dalhousie University, P.O. Box 1000, Halifax, Nova Scotia, Canada B3J 2X4.
J Phys Chem B. 2010 Nov 4;114(43):13786-95. doi: 10.1021/jp1067022.
Molecular dynamics (MD) simulation has been used extensively to study water surfaces. Nevertheless, the quantitative prediction of water surface tension has been controversial, since results from different simulation studies using the same water model may differ considerably. Recent research has suggested that bond flexibility, long-range electrostatic interactions, and certain simulation parameters, such as Lennard-Jones (LJ) cutoff distance and simulation time, may play an important role in determining the simulated surface tension. To gain better insight on the MD simulation of water surfaces, particularly on the prediction of surface tension, we examined seven flexible water models using a consistent set of simulation parameters. The surface tensions of the flexible, extended simple point charge (SPCE-F) model and the flexible three-center (F3C) model at 300 K were found to be 70.2 and 65.3 mN/m, respectively, in reasonable agreement with the experimental value of 71.7 mN/m. More importantly, however, detailed analysis of the interfacial structure and contributions from various interactions have revealed that the surface tension of water is determined by the delicate balance between intramolecular (bond stretching) and intermolecular (LJ) interactions, which reflects both the molecular orientation in the interfacial region and the density variation across the Gibbs dividing surface (GDS). In addition, the water molecules on the liquid side of the GDS were found to lie almost parallel to the surface, which helps to clarify the dual-layer structure suggested by sum-frequency generation spectroscopy. By correlating the simulated surface tensions of the seven water models with selected molecular parameters, it was found that the partial charge distribution in the water molecule is likely a key factor in determining the near-parallel alignment of water molecules with the surface.
分子动力学(MD)模拟已广泛用于研究水表面。然而,对于水表面张力的定量预测一直存在争议,因为使用相同水模型的不同模拟研究的结果可能有很大差异。最近的研究表明,键的柔韧性、长程静电相互作用以及某些模拟参数(如 Lennard-Jones(LJ)截断距离和模拟时间)可能在确定模拟表面张力方面起着重要作用。为了更好地了解水表面的 MD 模拟,特别是表面张力的预测,我们使用一致的模拟参数检查了七种柔性水模型。在 300 K 下,柔性扩展简单点电荷(SPCE-F)模型和柔性三中心(F3C)模型的表面张力分别为 70.2 和 65.3 mN/m,与实验值 71.7 mN/m 吻合良好。然而,更重要的是,对界面结构和各种相互作用的贡献的详细分析表明,水的表面张力取决于分子内(键拉伸)和分子间(LJ)相互作用之间的微妙平衡,这反映了界面区域分子的取向和 Gibbs 分界面(GDS)两侧的密度变化。此外,GDS 液体侧的水分子被发现几乎与表面平行,这有助于澄清和频产生光谱所建议的双层结构。通过将七种水模型的模拟表面张力与选定的分子参数相关联,发现水分子中的部分电荷分布可能是决定水分子与表面近乎平行排列的关键因素。