Fujii Kenta, Seki Shiro, Fukuda Shuhei, Kanzaki Ryo, Takamuku Toshiyuki, Umebayashi Yasuhiro, Ishiguro Shin-ichi
Department of Chemistry and Applied Chemistry, Faculty of Science and Engineering, Saga University, Honjo-machi, Saga 840-8502, Japan.
J Phys Chem B. 2007 Nov 8;111(44):12829-33. doi: 10.1021/jp074325e. Epub 2007 Oct 17.
Anion conformation of a low-viscosity room-temperature ionic liquid 1-ethyl-3-methylimidazolium bis(fluorosulfonyl) imide (EMI+FSI-) has been studied by Raman spectra and theoretical DFT calculations. Three strong Raman bands were found at 293, 328, and 360 cm(-1), which are ascribed to the FSI- ion. These Raman bands show significant temperature dependence, implying that two FSI- conformers coexist in equilibrium. This is supported by theoretical calculations that the FSI- ion is present as either C2 (trans) or C1 (cis) conformer; the former gives the global minimum, and the latter has a higher SCF energy of about 4 kJ mol(-1). Full geometry optimizations followed by normal frequency analyses show that the observed bands at 293, 328, and 360 cm(-1) are ascribed to the C2 conformer. The corresponding vibrations at 305, 320, and 353 cm(-1) were extracted according to deconvolution of the observed Raman bands in the range280-400 cm(-1 )and are ascribed to the C1 conformer. The enthalpy DeltaH degrees of conformational change from C2 to C1 was experimentally evaluated to be ca. 4.5 kJ mol(-1), which is in good agreement with the predicted value by theoretical calculations. The bis(trifluoromethanesulfonyl) imide anion (TFSI-) shows a conformational equilibrium between C1 and C2 analogues (DeltaH degrees = 3.5 kJ mol(-1)). However, the profile of the potential energy surface of the conformational change for FSI- (the F-S-N-S dihedral angle) is significantly different from that for TFSI- (the C-S-N-S dihedral angle).
通过拉曼光谱和理论密度泛函理论(DFT)计算研究了低粘度室温离子液体1-乙基-3-甲基咪唑双(氟磺酰)亚胺(EMI⁺FSI⁻)的阴离子构象。在293、328和360 cm⁻¹处发现了三个强拉曼带,它们归因于FSI⁻离子。这些拉曼带显示出明显的温度依赖性,这意味着两种FSI⁻构象异构体在平衡中共存。理论计算支持这一点,即FSI⁻离子以C2(反式)或C1(顺式)构象异构体形式存在;前者给出全局最小值,后者具有约4 kJ mol⁻¹的较高自洽场(SCF)能量。全几何优化随后进行正则频率分析表明,在293、328和360 cm⁻¹处观察到的谱带归因于C2构象异构体。根据在280 - 400 cm⁻¹范围内观察到的拉曼带的去卷积,提取了在305、320和353 cm⁻¹处的相应振动,并归因于C1构象异构体。从C2到C1的构象变化的焓ΔH°经实验评估约为4.5 kJ mol⁻¹,这与理论计算的预测值非常吻合。双(三氟甲磺酰)亚胺阴离子(TFSI⁻)在C1和C2类似物之间显示出构象平衡(ΔH° = 3.5 kJ mol⁻¹)。然而,FSI⁻(F - S - N - S二面角)构象变化的势能面轮廓与TFSI⁻(C - S - N - S二面角)的显著不同。