Department of Chemistry, University of Iowa, Iowa City, Iowa 52242, USA.
J Phys Chem B. 2013 Jan 31;117(4):1130-5. doi: 10.1021/jp311032p. Epub 2013 Jan 22.
X-ray scattering experiments and molecular dynamics simulations have been performed to investigate the structure of four room temperature ionic liquids (ILs) comprising the bis(trifluoromethylsulfonyl)amide (NTf(2)(-)) anion paired with the triethyloctylammonium (N(2228)(+)) and triethyloctylphosphonium (P(2228)(+)) cations and their isoelectronic diether analogs, the (2-ethoxyethoxy)ethyltriethylammonium (N(222(2O2O2))(+)) and (2-ethoxyethoxy)ethyltriethylphosphonium (P(222(2O2O2))(+)) cations. Agreement between simulations and experiments is good and permits a clear interpretation of the important topological differences between these systems. The first sharp diffraction peak (or prepeak) in the structure function S(q) that is present in the case of the liquids containing the alkyl-substituted cations is absent in the case of the diether substituted analogs. Using different theoretical partitioning schemes for the X-ray structure function, we show that the prepeak present in the alkyl-substituted ILs arises from polarity alternations between charged groups and nonpolar alkyl tails. In the case of the diether substituted ILs, we find considerable curling of tails. Anions can be found with high probability in two different environments: close to the cationic nitrogen (phosphorus) and also close to the two ether groups. For the two diether systems, anions are found in locations from which they are excluded in the alkyl-substituted systems. This removes the longer range (polar/nonpolar) pattern of alternation that gives rise to the prepeak in alkyl-substituted systems.
已进行 X 射线散射实验和分子动力学模拟,以研究四种室温离子液体(ILs)的结构,这些 ILs 包括双(三氟甲基磺酰基)酰胺(NTf(2)(-))阴离子与三乙基辛基铵(N(2228)(+))和三乙基辛基膦(P(2228)(+))阳离子及其等电子二醚类似物,即(2-乙氧基乙氧基)乙基三乙基铵(N(222(2O2O2))(+))和(2-乙氧基乙氧基)乙基三乙基膦(P(222(2O2O2))(+))阳离子。模拟与实验之间的一致性很好,能够清楚地解释这些体系之间重要的拓扑差异。在含有烷基取代阳离子的液体中存在结构函数 S(q)中的第一尖锐衍射峰(或预峰),而在二醚取代类似物中则不存在。使用 X 射线结构函数的不同理论划分方案,我们表明,烷基取代 ILs 中存在的预峰源自带电基团和非极性烷基尾之间的极性交替。在二醚取代的 ILs 中,我们发现尾巴有很大的卷曲。阴离子可以在两种不同的环境中以高概率存在:靠近阳离子氮(磷),也靠近两个醚基团。对于两个二醚体系,阴离子位于在烷基取代体系中被排除的位置。这消除了导致烷基取代体系中预峰的长程(极性/非极性)交替模式。