University of Lille, Faculty of Sciences and Technologies, LASIR (UMR CNRS A8516), Bât. C5, Cité Scientifique, 59655, Villeneuve d'Ascq Cedex, France.
Phys Chem Chem Phys. 2018 Aug 29;20(34):21890-21902. doi: 10.1039/c8cp03546f.
The changes of the local structure in the binary mixture of 1-butyl-3-methylimidazolium hexafluorophosphate (BmimPF6) ionic liquid and acetonitrile are investigated over the entire composition range. Two charge distribution models of the ions are considered: in the first one, the atomic fractional charges of the cations and anions are kept equal with those in the neat ionic liquid, and hence they are independent from the mole fraction of the ionic liquid, while in the second one the charge distribution is scaled up by a mole fraction dependent factor. The sum of these charges converge to +1e and -1e on the cation and anion, respectively, at infinite dilution. All the other interactions and geometry parameters of the ions (i.e., Lennard-Jones, bond stretching, angle bending and dihedral parameters) are identical in the two cases. The effect of the fractional charge distribution on the hydrogen bonding between the counterions themselves and between the ions and solvent molecules, as well as on the stacking interactions between the cations, is analyzed. To this end, two distances, characteristic of the hydrogen bond formed by the donor moiety and its nearest neighbor acceptor, as well as a coordinate system that defines unambiguously the orientation between a reference cation and its nearest neighbor, are introduced. It is shown that, with the variable charge model, the neighboring cation-anion pairs maintain their relative arrangement similar to the neat ionic liquid down to an ionic liquid mole fraction of xIL = 0.10, whereas in the case of the constant charge model such changes occur already at xIL = 0.20. Furthermore, the analysis of the first and the second nearest neighbor distance distributions of an anion around a reference cation indicates that, at this mole fraction range, there are two different preferred arrangements of the anions around the cations. In the first one, similarly to the local structure around a reference cation in the neat ionic liquid, the anion forms a distorted hydrogen bond with the cation, while in the second one the anion is located farther from the cation, forming no hydrogen bond with it. The relative population of these two types of preferred nearest neighbor cation-anion arrangements is found to be sensitive to further decrease of the ionic liquid mole fraction. These findings correlate with experimental results concerning the behavior of many physical chemical properties (e.g., excess volume, excess viscosity, chemical shift, infrared and Raman vibrational mode shifts, diffusion, etc.) that were found to undergo a drastic change in this mole fraction range. Our results show that in this composition range a transition occurs from the situation where the macroscopic physical chemical properties of the system are determined primarily by the cation-anion hydrogen bonding interactions to that where they are determined by the solvation of the cation and the anion by the molecular solvent.
研究了 1-丁基-3-甲基咪唑六氟磷酸盐(BmimPF6)离子液体与乙腈二元混合物在整个组成范围内局部结构的变化。考虑了两种离子的电荷分布模型:在第一种模型中,阳离子和阴离子的原子分数电荷与纯离子液体中的电荷相等,因此它们与离子液体的摩尔分数无关,而在第二种模型中,电荷分布由摩尔分数相关因子放大。在无限稀释时,这些电荷在阳离子和阴离子上分别收敛到+1e 和-1e。两种情况下离子的所有其他相互作用和几何参数(即 Lennard-Jones、键拉伸、角度弯曲和二面角参数)都是相同的。分析了分数电荷分布对反离子之间以及离子与溶剂分子之间氢键以及阳离子堆积相互作用的影响。为此,引入了两个距离,分别特征于供体部分与其最近邻受体形成的氢键,以及一个明确定义参考阳离子与其最近邻之间取向的坐标系。结果表明,在可变电荷模型中,相邻的阴阳离子对保持其相对排列类似于纯离子液体,直到离子液体摩尔分数 xIL = 0.10,而在常数电荷模型中,这种变化在 xIL = 0.20 时就已经发生。此外,对参考阳离子周围阴离子的第一和第二近邻距离分布的分析表明,在这个摩尔分数范围内,阴离子在阳离子周围有两种不同的优先排列方式。在第一种方式中,与纯离子液体中参考阳离子周围的局部结构类似,阴离子与阳离子形成扭曲的氢键,而在第二种方式中,阴离子离阳离子更远,与阳离子不形成氢键。这两种类型的优先近邻阳离子-阴离子排列的相对比例发现对离子液体摩尔分数的进一步降低很敏感。这些发现与许多物理化学性质(如过量体积、过量粘度、化学位移、红外和拉曼振动模式位移、扩散等)的实验结果相关,这些性质在这个摩尔分数范围内发生了剧烈变化。我们的结果表明,在这个组成范围内,系统的宏观物理化学性质主要由阴阳离子氢键相互作用决定的情况发生了转变,变为由阳离子和阴离子被分子溶剂溶剂化决定的情况。