Durig James R, Zheng Chao, Williams Michael J, Stidham Howard D, Guirgis Gamil A
Department of Chemistry, University of Missouri-Kansas City, 5100 Rockhill Road, Kansas City, MO 64110, USA.
Spectrochim Acta A Mol Biomol Spectrosc. 2004 Jun;60(7):1659-76. doi: 10.1016/j.saa.2003.08.024.
The infrared spectra (3200-400 cm(-1)) of krypton solutions of 1,3-difluoropropane, FCH2CH2CH2F, at variable temperatures (-105 to -150 degrees C) have been recorded. Additionally, the infrared spectra (3200-50 cm(-1)) of the gas and solid have been recorded as well as the Raman spectrum of the liquid. From a comparison of the spectra of the fluid phases with that in the solid, all of the fundamental vibrations of the C2 conformer (gauche-gauche) where the first gauche indicates the form for one of the CH2F groups and the second gauche the other CH2F, and many of those for the C1 form (trans-gauche) have been identified. Tentative assignments have been made for a few of the fundamentals of the other two conformers, i.e. C2v (trans-trans) and Cs (gauche-gauche'). By utilizing six pairs of fundamentals for these two conformers in the krypton solutions, an enthalpy difference of 277 +/- 28 cm(-1) (3.31 +/- 0.33 kJ mol(-1)) has been obtained for the C2 versus C1 conformer with the C2 conformer the more stable form. For the C2v conformer, the enthalpy difference has been determined to be 716 +/- 72 cm(-1) (8.57 +/- 0.86 kJ mol(-1)) and for the Cs form 971 +/- 115 cm(-1) (11.6 +/- 1.4 kJ mol(-1)). It is estimated that there is 64 +/- 3% of the C2 form, 34 +/-3% of the C1 form, 1% of the C2v form and 0.6% of the Cs conformer present at ambient temperature. Equilibrium geometries and total energies of the four stable conformers have been determined from ab initio calculations with full electron correlation by the perturbation method to second order as well as by hybrid density functional theory calculations with the B3LYP method using a number of basis sets. The MP2 calculations predict the C1 conformer stability to be slightly higher than the experimentally determined value whereas for the C2v and Cs conformers the predicted energy difference is much larger than the experimental value. The B3LYP calculations predict a better energy difference for both the C1 and C2v as well as for the Cs conformers than the MP2 values. A complete vibrational assignment is proposed for the C2 conformer and many of the fundamentals have been identified for the C1 form based on the force constants, relative intensities and rotational-vibrational band contours obtained from the predicted equilibrium geometry parameters. By combining previously reported rotational constants for the C2 and C1 conformers with ab initio MP2/6-311 + G(d, p) predicted parameters, adjusted r0 parameters have been obtained for both conformers. Comparisons are made with the parameters obtained for some other molecules containing the FCH2 group. The spectroscopic and theoretical results are compared to the corresponding properties for some similar molecules.
记录了1,3 - 二氟丙烷(FCH₂CH₂CH₂F)在氪溶液中于可变温度(-105至-150℃)下的红外光谱(3200 - 400 cm⁻¹)。此外,还记录了该气体和固体的红外光谱(3200 - 50 cm⁻¹)以及液体的拉曼光谱。通过将流体相的光谱与固体中的光谱进行比较,已识别出C₂构象异构体(gauche - gauche,其中第一个gauche表示一个CH₂F基团的形式,第二个gauche表示另一个CH₂F基团的形式)的所有基本振动,以及C₁构象异构体(trans - gauche)的许多基本振动。对其他两种构象异构体,即C₂ᵥ(trans - trans)和Cs(gauche - gauche')的一些基本振动进行了初步归属。通过利用氪溶液中这两种构象异构体的六对基本振动,得出C₂构象异构体与C₁构象异构体的焓差为277 ± 28 cm⁻¹(3.31 ± 0.33 kJ mol⁻¹),其中C₂构象异构体更稳定。对于C₂ᵥ构象异构体,确定其焓差为716 ± 72 cm⁻¹(8.57 ± 0.86 kJ mol⁻¹),对于Cs构象异构体为971 ± 115 cm⁻¹(11.6 ± 1.4 kJ mol⁻¹)。据估计,在环境温度下,C₂构象异构体占64 ± 3%,C₁构象异构体占34 ± 3%,C₂ᵥ构象异构体占1%,Cs构象异构体占0.6%。通过二阶微扰法进行全电子相关的从头算计算以及使用多种基组的B3LYP方法进行杂化密度泛函理论计算,确定了四种稳定构象异构体的平衡几何结构和总能量。MP2计算预测C₁构象异构体的稳定性略高于实验测定值,而对于C₂ᵥ和Cs构象异构体,预测的能量差远大于实验值。B3LYP计算预测的C₁和C₂ᵥ以及Cs构象异构体的能量差比MP2值更好。基于从预测的平衡几何参数获得的力常数、相对强度和转动 - 振动带轮廓,为C₂构象异构体提出了完整的振动归属,并为C₁构象异构体识别了许多基本振动。通过将先前报道的C₂和C₁构象异构体的转动常数与从头算MP2 / 6 - 311 + G(d, p)预测参数相结合,获得了两种构象异构体的调整r₀参数。与一些含有FCH₂基团的其他分子获得的参数进行了比较。将光谱和理论结果与一些类似分子的相应性质进行了比较。