Department of Chemistry, Faculty of Science, Kyushu University, Hakozaki, Higashi-ku, Fukuoka 812-8581, Japan.
J Phys Chem B. 2012 Mar 8;116(9):2801-13. doi: 10.1021/jp209561t. Epub 2012 Feb 29.
Liquid structure and the closest ion-ion interactions in a series of primary alkylammonium nitrate ionic liquids [C(n)Am(+)][NO(3)(-)] (n = 2, 3, and 4) were studied by means of high-energy X-ray diffraction (HEXRD) experiments with the aid of molecular dynamics (MD) simulations. Experimental density and X-ray structure factors are in good accordance with those evaluated with MD simulations. With regard to liquid structure, characteristic peaks appeared in the low Q (Q: a scattering vector) region of X-ray structure factors S(Q)'s for all ionic liquids studied here, and they increased in intensity with a peak position shift toward the lower Q side by increasing the alkyl chain length. Experimentally evaluated S(Q(peak))(r(max)) functions, which represent the S(Q) intensity at a peak position of maximum intensity Q(peak) as a function of distance (actually a integration range r(max)), revealed that characteristic peaks in the low Q region are related to the intermolecular anion-anion correlation decrease in the r range of 10-12 Å. Appearance of the peak in the low Q region is probably related to the exclusion of the correlations among ions of the same sign in this r range by the alkyl chain aggregation. From MD simulations, we found unique and rather distorted NH···O hydrogen bonding between C(n)Am(+) (n = 2, 3, and 4) and NO(3)(-) in these ionic liquids regardless of the alkyl chain length. Subsequent ab initio calculations for both a molecular complex C(2)H(5)NH(2)···HONO(2) and an ion pair C(2)H(5)NH(3)(+)···ONO(2)(-) revealed that such distorted hydrogen bonding is specific in a liquid state of this family of ionic liquids, though the linear orientation is preferred for both the N···HO hydrogen bonding in a molecular complex and the NH···O one in an ion pair. Finally, we propose our interpretation of structural heterogeneity in PILs and also in APILs.
一系列伯烷基铵硝酸酯离子液体[C(n)Am(+)] [NO(3)(-)](n = 2,3 和 4)的液体结构和最近的离子-离子相互作用通过高能 X 射线衍射(HEXRD)实验并结合分子动力学(MD)模拟进行了研究。实验密度和 X 射线结构因子与 MD 模拟评估值非常吻合。对于液体结构,在所研究的所有离子液体中,X 射线结构因子 S(Q)'s 的低 Q(Q:散射矢量)区域出现特征峰,并且随着烷基链长度的增加,特征峰的强度增加,峰位置向低 Q 侧移动。实验评估的 S(Q(peak))(r(max))函数表示作为距离(实际上是积分范围 r(max))函数的最大强度 Q(peak)处的 S(Q)强度,表明低 Q 区域的特征峰与 10-12 Å 范围内的阴离子-阴离子相关减少有关。低 Q 区域中峰的出现可能与烷基链聚集排除了同一符号离子之间的相关有关。从 MD 模拟中,我们发现了在这些离子液体中,C(n)Am(+)(n = 2,3 和 4)和 NO(3)(-) 之间存在独特且相当扭曲的 NH···O 氢键,无论烷基链长度如何。对于分子复合物 C(2)H(5)NH(2)···HONO(2)和离子对 C(2)H(5)NH(3)(+)···ONO(2)(-)的从头算计算表明,尽管在分子复合物中 N···HO 氢键和离子对中的 NH···O 氢键都倾向于线性取向,但这种扭曲的氢键在这种离子液体家族的液态中是特定的。最后,我们提出了对 PILs 和 APILs 结构异质性的解释。