Department of Chemistry, Shiraz University, Shiraz 71454, Iran.
J Chem Phys. 2012 Mar 28;136(12):124706. doi: 10.1063/1.3696004.
Bulk and surface properties of the ionic liquids 1-alkyl-3-methyl-imidazolium iodides ([C(n)mim]I) were simulated by classical molecular dynamics using all atom non-polarizable force field (n = 4, butyl; 6, hexyl; 8, octyl). The structure of ionic liquids were initially optimized by density functional theory and atomic charges obtained by CHELPG method. Reduction of partial atomic charges (by 20% for simulation of density and surface tension, and by 10% for viscosity) found to improve the accuracy, while a non-polarizable force field was applied. Additionally, the simulation ensembles approach the equilibrium faster when the charge reduction is applied. By these refined force field parameters, simulated surface tensions in the range of 323-393 k are quite in agreement with the experiments. Simulation of temperature dependent surface tension of [C(4)mim]I well beyond room temperature (up to 700 K) permits prediction of the critical temperature in agreement with that predicted from experimental surface tension data. Simulated densities in the range of 298-450 K for the three ionic liquids are within 0.8% of the experimental data. Structural properties for [C(4)mim]I were found to be in agreement with the results of Car-Parrinello molecular dynamics simulation we performed, which indicates a rather well-structured cation-anion interaction and occurs essentially through the imidazolium ring cation. Diffusion coefficient changes with alkyl chain length in the order of [C(8)mim]I > [C(6)mim]I > [C(4)mim]I for the cation and the anion. Formation of a dense domain in subsurface region is quite evident, and progressively becomes denser as the alkyl chain length increases. Bivariate orientational analysis was used to determine the average orientation of molecule in ionic liquids surface, subsurface, and bulk regions. Dynamic bisector-wise and side-wise movement of the imodazolium ring cation in the surface region can be deduced from the bivariate maps. Atom-atom density profile and bivariate analysis indicate that the imidazolium cation takes a spoon like configuration in the surface region and the tilt of alkyl group is a function length of alkyl chain exposing as linear as possible to the vapor phase.
使用全原子非极化力场(n = 4,丁基;6,己基;8,辛基)通过经典分子动力学模拟了离子液体 1-烷基-3-甲基-咪唑鎓碘化物([C(n)mim]I)的体相和表面性质。通过密度泛函理论优化了离子液体的结构,并通过 CHELPG 方法获得了原子电荷。发现减少部分原子电荷(模拟密度和表面张力时减少 20%,模拟粘度时减少 10%)可以提高准确性,同时应用非极化力场。此外,当应用电荷减少时,模拟集合更快地达到平衡。通过这些改进的力场参数,模拟的 323-393 K 范围内的表面张力与实验相当吻合。模拟[C(4)mim]I 的温度依赖性表面张力远超过室温(高达 700 K),可以预测与实验表面张力数据预测的临界温度一致。对于三种离子液体,在 298-450 K 范围内模拟的密度与实验数据相差在 0.8%以内。对于[C(4)mim]I 的结构性质,与我们进行的 Car-Parrinello 分子动力学模拟的结果一致,这表明阳离子-阴离子相互作用相当有序,主要通过咪唑鎓环阳离子发生。扩散系数随烷基链长度的变化顺序为[C(8)mim]I > [C(6)mim]I > [C(4)mim]I,对于阳离子和阴离子都是如此。在亚表面区域形成密集域是非常明显的,并且随着烷基链长度的增加而变得更加密集。双变量定向分析用于确定离子液体表面、亚表面和体相区域中分子的平均取向。从双变量图谱可以推断出表面区域中咪唑鎓环阳离子的双矢量等分线和侧向运动。原子-原子密度分布和双变量分析表明,在表面区域中,咪唑鎓阳离子呈匙形构型,烷基基团的倾斜是烷基链长度的函数,尽可能呈线性暴露于气相。