Takamuku Toshiyuki, Kumai Takashi, Yoshida Koji, Otomo Toshiya, Yamaguchi Toshio
Department of Chemistry and Applied Chemistry, Faculty of Science and Engineering, Saga University, Honjo-machi, Saga 840-8502, Japan.
J Phys Chem A. 2005 Sep 1;109(34):7667-76. doi: 10.1021/jp051470o.
To clarify the structure of solvent clusters formed in halogenoethanol-water mixtures at the molecular level, large-angle X-ray scattering (LAXS) measurements have been made at 298 K on 2,2,2-trifluoroethanol (TFE), 2,2,2-trichloroethanol (TCE), and their aqueous mixtures in the TFE and TCE mole fraction ranges of 0.002 < or = x(TFE) < or = 0.9 and 0.5 < or = x(TCE) < or = 0.9, respectively. The radial distribution functions (RDFs) for TFE-water mixtures have shown that the structural transition from inherent TFE structure to the tetrahedral-like structure of water takes place at x(TFE) approximately 0.2. In the TCE-water mixtures inherent TCE structure remains in the range of 0.5 < or = x(TCE) < or = 1. Small-angle neutron scattering (SANS) experiments have been performed on CF(3)CH(2)OD- (TFE-d(1)-) D(2)O and CF(3)CD(2)OH- (TFE-d(2)-) H(2)O mixtures in the TFE mole fraction range of 0.05 < or = x(TFE) < or = 0.8. The SANS results in terms of the Ornstein-Zernike correlation length have revealed that TFE and water molecules are most heterogeneously mixed with each other in the TFE-water mixture at x(TFE) approximately 0.15, i.e., both TFE clusters and water clusters are most enhanced in the mixture. To evaluate the dynamics of TFE and ethanol (EtOH) molecules in TFE-water and ethanol-water mixtures, respectively, (1)H NMR relaxation rates for the methylene group within alcohol molecules have been measured by using an inversion-recovery method. The alcohol concentration dependence of the relaxation rates for the TFE-water and ethanol-water mixtures has shown a break point at x(TFE) approximately 0.15 and x(EtOH) approximately 0.2, respectively, where the structural transition from alcohol clusters to the tetrahedral-like structure of water takes place. On the basis of the present results, the most likely structure models of solvent clusters predominantly formed in TFE-water and TCE-water mixtures are proposed. In addition, effects of halogenation of the hydrophobic groups on clustering of alcohol molecules are discussed from the present results, together with the previous ones for ethanol-water and 1,1,1,3,3,3-hexafluoro-2-propanol- (HFIP-) water mixtures.
为了在分子水平上阐明卤代乙醇 - 水混合物中形成的溶剂簇的结构,在298 K下对2,2,2 - 三氟乙醇(TFE)、2,2,2 - 三氯乙醇(TCE)及其在TFE和TCE摩尔分数范围分别为0.002≤x(TFE)≤0.9和0.5≤x(TCE)≤0.9的水性混合物进行了大角度X射线散射(LAXS)测量。TFE - 水混合物的径向分布函数(RDFs)表明,从固有的TFE结构到水的四面体状结构的结构转变发生在x(TFE)约为0.2处。在TCE - 水混合物中,固有的TCE结构在0.5≤x(TCE)≤1的范围内保持。在TFE摩尔分数范围为0.05≤x(TFE)≤0.8的CF(3)CH(2)OD - (TFE - d(1)-)D(2)O和CF(3)CD(2)OH - (TFE - d(2)-)H(2)O混合物上进行了小角度中子散射(SANS)实验。根据奥恩斯坦 - 泽尔尼克相关长度的SANS结果表明,TFE和水分子在x(TFE)约为0.15的TFE - 水混合物中彼此混合最不均匀,即TFE簇和水簇在混合物中都得到最大增强。为了分别评估TFE - 水和乙醇 - 水混合物中TFE和乙醇(EtOH)分子的动力学,使用反转恢复方法测量了醇分子中亚甲基的(1)H NMR弛豫率。TFE - 水和乙醇 - 水混合物弛豫率的醇浓度依赖性分别在x(TFE)约为0.15和x(EtOH)约为0.2处显示出一个断点,此时从醇簇到水的四面体状结构发生结构转变。基于目前的结果,提出了在TFE - 水和TCE - 水混合物中主要形成的溶剂簇的最可能结构模型。此外,结合先前关于乙醇 - 水和1,1,1,3,3,3 - 六氟 - 2 - 丙醇 - (HFIP - )水混合物的结果,从目前的结果讨论了疏水基团卤化对醇分子聚集的影响。