Sudo Seiichi, Tsubotani Sosuke, Shimomura Mayumi, Shinyashiki Naoki, Yagihara Shin
Department of Physics, Tokai University, Hiratsuka, Kanagawa 259-1292, Japan.
J Chem Phys. 2004 Oct 15;121(15):7332-40. doi: 10.1063/1.1796232.
Broadband dielectric measurements for 65 wt % ethylene glycol oligomer (EGO)-water mixtures with one to six repeat units of EGO molecules were performed in the frequency range of 10 microHz-10 GHz and the temperature range of 128-298 K. In the case of the water-EGO mixtures with one and two repeat units of the EGO molecule (small EGO), the shape of the dielectric loss peak of the primary process is asymmetrical about the logarithm of the frequency of maximum loss above the crossover temperature, T(C). The asymmetric process continues to the alpha process at a low frequency, and an additional beta process appears in the frequency range higher than that of the alpha process below T(C). In contrast, the water-EGO mixtures with three or more repeat units of the EGO molecule (large EGO) show a broad and symmetrical loss peak of the primary process above T(C). The symmetric process continues to the beta process, and an additional alpha process appears in the frequency range lower than that of the beta process below T(C). These different scenarios of the alpha-beta separation related to the shape of the loss peak above T(C) are a result of the difference in the cooperative motion of water and solute molecules. The solute and water molecules move cooperatively in the small EGO-water mixtures above T(C), and this cooperative motion leads to the asymmetric loss peak above T(C) and the alpha process below T(C). For the large EGO-water mixtures, the spatially restricted motion of water confined by solute molecules leads to the symmetric loss peak above T(C) and the beta process below T(C).
对含有1至6个EGO分子重复单元的65 wt%乙二醇低聚物(EGO)-水混合物进行了宽带介电测量,测量频率范围为10微赫兹至10吉赫兹,温度范围为128至298K。对于含有1个和2个EGO分子重复单元的水-EGO混合物(小EGO),在交叉温度T(C)以上,主过程的介电损耗峰形状关于最大损耗频率的对数不对称。在低频下,不对称过程延续至α过程,并且在低于T(C)时,在高于α过程的频率范围内出现一个额外的β过程。相比之下,含有3个或更多EGO分子重复单元的水-EGO混合物(大EGO)在T(C)以上显示出一个宽且对称的主过程损耗峰。对称过程延续至β过程,并且在低于T(C)时,在低于β过程的频率范围内出现一个额外的α过程。这些与T(C)以上损耗峰形状相关的α-β分离的不同情况是水和溶质分子协同运动差异的结果。在T(C)以上,溶质和水分子在小EGO-水混合物中协同运动,这种协同运动导致T(C)以上的不对称损耗峰和T(C)以下的α过程。对于大EGO-水混合物,溶质分子限制的水的空间受限运动导致T(C)以上的对称损耗峰和T(C)以下的β过程。