Kaintz Anne, Baker Gary, Benesi Alan, Maroncelli Mark
Department of Chemistry, The Pennsylvania State University , University Park, Pennsylvania 16802, United States.
J Phys Chem B. 2013 Oct 3;117(39):11697-708. doi: 10.1021/jp405393d. Epub 2013 Sep 12.
Diffusion coefficients of a variety of dilute solutes in the series of 1-alkyl-1-methylpyrrolidinium bis(trifluoromethanesulfonyl)imides ([Prn1][Tf2N], n = 3, 4, 6, 8, and 10), trihexyltetracedecylphosphonium bis(trifluoromethanesulfonyl)imide [P14,666][Tf2N], and assorted imidazolium ionic liquids are measured using pulsed field gradient (1)H NMR. These data, combined with available literature data, are used to try to uncover the solute and solvent characteristics most important in determining tracer diffusion rates. Discussion is framed in terms of departures from simple hydrodynamic predictions for translational friction using the ratio ζobs/ζSE, where ζobs is the observed friction, determined from the measured diffusion coefficient D via ζobs = kBT/D, and ζSE = 6πηR is the Stokes friction on a sphere of radius R (determined from the solute van der Waals volume) in a solvent with viscosity η. In the case of neutral solutes, the primary determinant of whether hydrodynamic predictions are accurate is the relative size of solute versus solvent molecules. A single correlation, albeit with considerable scatter, is found between ζobs/ζSE and the ratio of solute-to-solvent van der Waals volumes, ζobs/ζSE = {1 + a(VU/VV)(-p)}, with constants a = 1.93 and p = 1.88. In the case of small solutes, the observed friction is over 100-fold smaller than predictions of hydrodynamic models. The dipole moment of the solute has little effect on the friction, whereas solute charge has a marked effect. For monovalent solutes of size comparable to or smaller than the solvent ions, the observed friction is comparable to or even greater than what is predicted by hydrodynamics. These general trends are shown to be quite similar to what is observed for tracer diffusion in conventional solvents.
使用脉冲场梯度(1)H NMR测量了多种稀溶质在一系列1-烷基-1-甲基吡咯烷鎓双(三氟甲磺酰)亚胺([Prn1][Tf2N],n = 3、4、6、8和10)、三己基十四烷基鏻双(三氟甲磺酰)亚胺[P14,666][Tf2N]以及各种咪唑鎓离子液体中的扩散系数。这些数据与现有的文献数据相结合,用于试图揭示在确定示踪剂扩散速率方面最重要的溶质和溶剂特性。讨论围绕使用比率ζobs/ζSE偏离简单流体动力学对平移摩擦的预测展开,其中ζobs是观察到的摩擦,通过ζobs = kBT/D由测量的扩散系数D确定,ζSE = 6πηR是在粘度为η的溶剂中半径为R的球体(由溶质范德华体积确定)上的斯托克斯摩擦。对于中性溶质,流体动力学预测是否准确的主要决定因素是溶质与溶剂分子的相对大小。在ζobs/ζSE与溶质与溶剂范德华体积之比之间发现了单一的相关性,尽管存在相当大的分散性,ζobs/ζSE = {1 + a(VU/VV)(-p)},常数a = 1.93,p = 1.88。对于小溶质,观察到的摩擦比流体动力学模型的预测小100倍以上。溶质的偶极矩对摩擦影响很小,而溶质电荷有显著影响。对于大小与溶剂离子相当或小于溶剂离子的单价溶质,观察到的摩擦与流体动力学预测的相当甚至更大。这些一般趋势与在传统溶剂中示踪剂扩散所观察到的非常相似。