Idrissi Abdenacer, Marekha B, Kiselev M, Jedlovszky Pál
Laboratoire de Spectrochimie Infrarouge et Raman (UMR CNRS A8516), Université Lille 1, Science et Technologies, 59655 Villeneuve d'Ascq Cedex, France.
Phys Chem Chem Phys. 2015 Feb 7;17(5):3470-81. doi: 10.1039/c4cp04839c. Epub 2014 Dec 23.
Molecular dynamics simulations of water-DMSO mixtures, containing 10, 20, 30, 40, 50, 60, 70, 80, and 90 mol% DMSO, respectively, have been performed on the isothermal-isobaric (N,p,T) ensemble at T = 298 K and at the pressure equal to the experimental vapor pressure at each mixture composition. In addition, simulations of the two neat systems have also been performed for reference. The potential models used in the simulations are known to excellently reproduce the mixing properties of these compounds. The simulation results have been analyzed in detail by means of the Voronoi polyhedra (VP) of the molecules. Distributions of the VP volume and the asphericity parameter as well as that of the radius of the spherical intermolecular voids have been calculated. Detailed analyses of these distributions have revealed that both molecules prefer to be in an environment consisting of both types of molecules, but the affinity of DMSO for mixing with water is clearly stronger than that of water for mixing with DMSO. As a consequence, the dilution of the two neat liquids by the other component has been found to follow different mechanisms: when DMSO is added to neat water small domains of neat-like water persist up to the equimolar composition, whereas no such domains are found when neat DMSO is diluted by water. The observed behaviour is also in line with the fact that the main thermodynamic driving force behind the full miscibility of water and DMSO is the energy change accompanying their mixing, and that the entropy change accompanying this mixing is negative in systems of low and positive in systems of high DMSO mole fractions. Finally, we have found a direct evidence for the existence of strong hydrogen bonded complexes formed by one DMSO and two water molecules, but it has also been shown that these complexes are in equilibrium with single (monomeric) water and DMSO molecules in the mixed systems.
分别对含有10%、20%、30%、40%、50%、60%、70%、80%和90%二甲基亚砜(DMSO)的水 - DMSO混合物进行了分子动力学模拟,模拟是在等温等压(N,p,T)系综下,温度T = 298 K且压力等于各混合物组成下的实验蒸气压的条件下进行的。此外,还对两种纯物质体系进行了模拟以供参考。模拟中使用的势模型能够出色地再现这些化合物的混合性质。通过分子的Voronoi多面体(VP)对模拟结果进行了详细分析。计算了VP体积、非球形度参数以及球形分子间空隙半径的分布。对这些分布的详细分析表明,两种分子都倾向于处于由两种类型分子组成的环境中,但DMSO与水混合的亲和力明显强于水与DMSO混合的亲和力。因此,发现两种纯液体被另一种组分稀释遵循不同的机制:当向纯水添加DMSO时,类似纯水的小区域一直持续到等摩尔组成,而当纯水稀释纯DMSO时则未发现此类区域。观察到的行为也与以下事实相符:水和DMSO完全互溶背后的主要热力学驱动力是它们混合时伴随的能量变化,并且这种混合伴随的熵变在低DMSO摩尔分数体系中为负,在高DMSO摩尔分数体系中为正。最后,我们找到了由一个DMSO和两个水分子形成强氢键复合物存在的直接证据,但也表明这些复合物在混合体系中与单个(单体)水和DMSO分子处于平衡状态。