Department of Physics, Meiji University, 1-1-1 Higashimita, Tama-ku, Kawasaki 214-8571, Japan.
J Phys Chem B. 2009 Nov 19;113(46):15304-11. doi: 10.1021/jp905233n.
Clathrate hydrates are known to form a thin film along a guest/host boundary. We present here the first report of tetrahydrofuran (THF) clathrate hydrate formation in a THF/water concentration boundary layer. We found that the THF-water system also forms a hydrate film separating the guest/host phases. The lateral growth rate of the film increases as supercooling increases. The thickness of the film at the growth tip decreases as supercooling and the lateral growth rate increase. These tendencies are consistent with reports of experiments for other hydrates and predictions of heat-transfer models. After film formation and slight melting, two types of growth modes are observed, depending on temperature T. At T = 3.0 degrees C, the film slowly thickens. The thickening rate is much lower than the lateral growth rate, as reported for other hydrates. At T < or = 2.0 degrees C, however, the growth mode transitions spontaneously from film growth to continuous nucleation, and an agglomerate of small polycrystalline hydrates forms in each phase. Grain boundaries in the film and pore spaces in the agglomerate act as paths for permeation of each liquid. Timing when continuous nucleation starts is dominantly controlled by the time of initiation of liquid permeation through the film. Digital particle image velocimetry analysis of the agglomerate shows that it expands not by growth at the advancing front but rather by continuous nucleation in the interior. Expansion rates of the agglomerate tend to be higher for the cases of multipermeation paths in the film and the thinner film. We suppose that the growth mode transition to continuous nucleation is caused by the memory effect due to slight melting of the hydrate film.
笼形水合物已知沿客体/主体边界形成一层薄膜。本文首次报道了四氢呋喃(THF)在 THF/水浓度边界层中形成笼形水合物。我们发现 THF-水体系也形成了分离客体/主体相的水合物膜。随着过冷度的增加,膜的侧向生长速率增加。随着过冷度和侧向生长速率的增加,生长尖端处膜的厚度减小。这些趋势与其他水合物的实验报告和传热模型的预测一致。在膜形成和轻微融化后,观察到两种类型的生长模式,这取决于温度 T。在 T = 3.0°C 时,膜缓慢变厚。增厚速率远低于侧向生长速率,与其他水合物的报告一致。然而,在 T ≤ 2.0°C 时,生长模式自发从膜生长转变为连续成核,在每个相中形成小多晶水合物的团聚体。膜中的晶界和团聚体中的孔隙作为每种液体渗透的路径。连续成核开始的时间主要由液体通过膜渗透开始的时间控制。对团聚体的数字粒子图像测速分析表明,它不是通过前沿的生长而是通过内部的连续成核来扩展。对于膜中存在多条渗透路径和膜较薄的情况,团聚体的扩展速率往往更高。我们假设生长模式向连续成核的转变是由于水合物膜的轻微融化引起的记忆效应。