Department of Chemistry, Graduate School of Science and Engineering, Tokyo Institute of Technology, 2-12-1 O-okayama, Meguro-ku, Tokyo 152-8551, Japan.
J Phys Condens Matter. 2010 Aug 18;22(32):325103. doi: 10.1088/0953-8984/22/32/325103. Epub 2010 Jul 7.
Enthalpy relaxation processes proceeding in ethylene glycol (EG) aqueous solutions [(EG)(x)(H(2)O)(1 - x)] within silica-gel nanopores were studied by adiabatic calorimetry. While the x = 0.25 solution within pores with diameter of 52 nm showed a glass transition at T(g) = 139 K, ageing of the solution at 160 K caused a phase separation to reveal glass transitions at T(g) = 145 and 160 K for EG-rich and water-rich regions, respectively: the water molecules are understood to form a more developed hydrogen-bond network, and consequently force the EG molecules in between the water-rich regions. The T(g) = 160 K is in good agreement with the T(g) value of the internal (not interfacial) water confined within pores with thickness of 1.1 nm. The ageing further remarkably diminished the T(g) = 115 K glass transition. This indicates that, while the molecules responsible for the glass transition are the mobile water ones forming a lower number of hydrogen bonds than four, the fraction of such water molecules is reduced in association with the development of the network and the glass transition is absent in bulk pure water. When the same x = 0.25 solution was confined within 1.1- and 12 nm pores, the water molecules developed a hydrogen-bond network in the pore centre due to the presence of the pore wall and pushed the EG molecules onto the pore surface even at higher temperatures: the water-rich region gave T(g) = 155 K close to 160 K. It is concluded that the hydrogen-bond network inherent to water structure is developed/collapsed remarkably in the range near x = 0; consequently, the composition dependence of T(g) in the bulk system deviates sharply in the range from the Gordon-Taylor empirical law followed for large x > 0.2.
通过绝热量热法研究了在二氧化硅凝胶纳米孔中的乙二醇(EG)水溶液[(EG)(x)(H(2)O)(1 - x)]中的焓松弛过程。当直径为 52nm 的孔中的 x = 0.25 溶液显示玻璃化转变温度 T(g) = 139K 时,溶液在 160K 下老化会导致相分离,分别在 EG 丰富区和水丰富区显示玻璃化转变温度 T(g) = 145 和 160K:水分子被理解为形成更发达的氢键网络,从而迫使 EG 分子位于水丰富区之间。T(g) = 160K 与厚度为 1.1nm 的孔内(非界面)水的 T(g) = 160K 值吻合较好。老化进一步显著降低了 T(g) = 115K 的玻璃化转变温度。这表明,虽然负责玻璃化转变的分子是形成氢键数量少于四个的可移动水分子,但随着网络的发展,这种水分子的分数减少,并且在纯水中不存在玻璃化转变。当相同的 x = 0.25 溶液被限制在 1.1nm 和 12nm 的孔内时,水分子由于孔壁的存在在孔中心形成氢键网络,并将 EG 分子推到孔表面,即使在较高温度下也是如此:水丰富区给出的 T(g) = 155K 接近 160K。可以得出结论,在 x = 0 附近的范围内,水结构中固有的氢键网络得到了显著的发展/崩溃,因此,在从遵循 Gordon-Taylor 经验定律的大 x > 0.2 到 bulk 系统的 T(g)的组成依赖性在该范围内急剧偏离。