Kajiya Daisuke, Saitow Ken-ichi
Natural Science Center for Basic Research and Development (N-BARD), Hiroshima University, Higashi-hiroshima, Hiroshima 739-8526, Japan.
J Phys Chem B. 2009 Oct 8;113(40):13291-9. doi: 10.1021/jp903240v.
Vibrational Raman spectra of the C horizontal lineC stretching modes of cis- and trans-1,2-dichloroethylene (C(2)H(2)Cl(2)) were measured in supercritical carbon dioxide (CO(2)). The spectra were collected at a fixed solute mole fraction by varying the fluid density by a factor of 20. As the density increased, the peak frequencies of the C horizontal lineC stretching modes shifted toward the low-energy side at isotherms of reduced temperature, T(r) = T/T(c) = 1.02, 1.06, and 1.20. By analyzing these density dependences using the perturbed hard-sphere theory, we decomposed the shifts into attractive and repulsive components. The repulsive shifts of cis-C(2)H(2)Cl(2) were almost equivalent to those of trans-C(2)H(2)Cl(2). However, the attractive shifts of nonpolar trans-C(2)H(2)Cl(2) were significantly greater than those of polar cis-C(2)H(2)Cl(2) at all densities and temperatures. To evaluate the difference in the isomers, we calculated the attractive shifts of the C horizontal lineC stretching modes of each isomer, composing of dispersion, dipole-induced-dipole, and dipole-quadrupole interactions between solute C(2)H(2)Cl(2) and solvent CO(2) molecules. These three interactions were quantified by considering molecular configurations and orientations, and solvation structures around the isomers were elucidated by 3D schematic diagrams. As a result, it was shown that the anisotropic solvation structure around trans-C(2)H(2)Cl(2) was responsible for the larger attractive shifts in the supercritical CO(2). The difference of solvation structures between the isomers was significant at T(r) = 1.02 but became minor as the temperature increased to T(r) = 1.20.
在超临界二氧化碳(CO₂)中测量了顺式和反式-1,2-二氯乙烯(C₂H₂Cl₂)的C≡C伸缩振动模式的拉曼光谱。通过将流体密度变化20倍,在固定溶质摩尔分数下收集光谱。随着密度增加,在折合温度T(r)=T/Tc = 1.02、1.06和1.20的等温线上,C≡C伸缩振动模式的峰值频率向低能侧移动。通过使用微扰硬球理论分析这些密度依赖性,我们将位移分解为吸引和排斥分量。顺式-C₂H₂Cl₂的排斥位移几乎与反式-C₂H₂Cl₂的排斥位移相当。然而,在所有密度和温度下,非极性反式-C₂H₂Cl₂的吸引位移明显大于极性顺式-C₂H₂Cl₂的吸引位移。为了评估异构体之间的差异,我们计算了每个异构体的C≡C伸缩振动模式的吸引位移,其由溶质C₂H₂Cl₂和溶剂CO₂分子之间的色散、偶极-诱导偶极和偶极-四极相互作用组成。通过考虑分子构型和取向对这三种相互作用进行了量化,并通过三维示意图阐明了异构体周围的溶剂化结构。结果表明,反式-C₂H₂Cl₂周围的各向异性溶剂化结构是超临界CO₂中较大吸引位移的原因。异构体之间的溶剂化结构差异在T(r)=1.02时很显著,但随着温度升高到T(r)=1.20时变得很小。