Yoshida Koji, Yamaguchi Toshio, Kittaka Shigeharu, Bellissent-Funel Marie-Claire, Fouquet Peter
Advanced Materials Institute and Department of Chemistry, Faculty of Science, Fukuoka University, Nanakuma, Jonan-ku, Fukuoka 814-0180, Japan.
J Chem Phys. 2008 Aug 7;129(5):054702. doi: 10.1063/1.2961029.
Thermodynamic, structural, and dynamic properties of heavy water (D(2)O) confined in mesoporous silica glass MCM-41 C10, C12, and C14 were investigated by differential scanning calorimetry, neutron diffraction, and neutron spin echo (NSE) measurements, respectively. The DSC data showed that no crystallization of D(2)O confined in C10 occurs in a temperature range between 298 and 180 K, and that crystalline ice is formed at 204 and 221 K for C12 and C14, respectively. For C10, the neutron radial distribution functions of confined D(2)O suggested a structural change in the supercooled state between 223 and 173 K. For C10 sample, it has been found that the tetrahedral-like water structure is partially enhanced in the central part of pores at 173 K. For all the samples, the intermediate scattering functions from the NSE measurements are fitted by the Kohlrausch-Williams-Watts stretched exponential function which implies that confined supercooled D(2)O exhibits a wide distribution of relaxation times. For C10, C12, and C14 samples, between 298 and 240 K, the relaxation times of supercooled D(2)O follow remarkably well the Vogel-Fulcher-Tamman equation; for C10 sample, below 240 K, the relaxation times of nonfreezing D(2)O show an Arrhenius type behavior. From the present experimental results on calorimetric, structural, and dynamic properties, it has been concluded that supercooled D(2)O confined in MCM-41 C10 experiences a transition from high-density to low-density hydrogen-bonded structure at around 229 K.
分别通过差示扫描量热法、中子衍射和中子自旋回波(NSE)测量,研究了限制在介孔二氧化硅玻璃MCM - 41 C10、C12和C14中的重水(D₂O)的热力学、结构和动力学性质。DSC数据表明,限制在C10中的D₂O在298至180 K的温度范围内不发生结晶,而C12和C14分别在204 K和221 K形成结晶冰。对于C10,受限D₂O的中子径向分布函数表明在223至173 K的过冷状态下结构发生了变化。对于C10样品,发现在173 K时孔中心部分类似四面体的水结构部分增强。对于所有样品,NSE测量得到的中间散射函数由Kohlrausch - Williams - Watts拉伸指数函数拟合,这意味着受限的过冷D₂O表现出宽分布的弛豫时间。对于C10、C12和C14样品,在298至240 K之间,过冷D₂O的弛豫时间非常符合Vogel - Fulcher - Tamman方程;对于C10样品,在240 K以下,未冻结D₂O的弛豫时间表现出阿仑尼乌斯型行为。根据目前关于量热、结构和动力学性质的实验结果,得出结论:限制在MCM - 41 C10中的过冷D₂O在约229 K时经历从高密度到低密度氢键结构的转变。