Thermal Properties and Mixing State of Diol−Water Mixtures Studied by Calorimetry, Large-Angle X-Ray Scattering, and NMR Relaxation
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Differential scanning calorimetry (DSC) has been performed on aqueous mixtures of three diols, which involve a linear carbon chain, HO−(CH2)n−OH (n = 3, 4, and 5), over the whole mole fraction range of diols. The DSC results have shown the alkyl chain parity for the freezing process of the aqueous mixtures: aqueous mixtures of 1,3-propanediol (PrD) and 1,5-pentanediol (PeD) are kept in the supercooled state or vitrified over a wide mole fraction range, while those of 1,4-butanediol (BuD) are easily crystallized. The structure of PrD−water mixtures has been elucidated by using the large-angle X-ray scattering (LAXS) technique. It has been suggested that the structural change of PrD−water mixtures occurs at PrD mole fractions of xPrD = 0.4 and 0.8: in the range of xPrD ≤ 0.4 where the tetrahedral-like structure of water predominates, in the range of 0.4 < xPrD < 0.8 where both PrD and water structures coexist, and in the range of xPrD ≥ 0.8 where the inherent structure of PrD is mainly formed. 17O and 1H NMR relaxation measurements have been made on aqueous mixtures of ethylene glycol (EG, n = 2), PrD, and BuD to clarify the dynamics of H217O and diol molecules. The 17O NMR relaxation rates have suggested that the rotational motion of water molecules is gradually retarded in the diol−water mixtures with increasing diol content and that the restriction of the motion is more remarkable in the order of EG < PrD < BuD. On the basis of all the results, together with comparison with those of methanol−water, ethanol−water, and 1-propanol−water mixtures previously reported, the mixing state of diol−water mixtures has been discussed at the molecular level.

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