Department of Chemical Engineering, National Taiwan University, Taipei 10617, Taiwan.
J Phys Chem B. 2010 Aug 26;114(33):10804-13. doi: 10.1021/jp102874s.
The key factors that affect the growth of methane hydrates are identified using molecular dynamics simulations. The three-phase molecular models consisting of methane gas, liquid water, and solid hydrate phase are used in this study. The melting temperatures of such a model at different pressures are found to be in good agreement with experiment. The growth rate of methane hydrate is found to be dominated by (1) the solubility of methane in the liquid phase, (2) the diffusivity of methane in water, and (3) the adsorption of methane by methane-filled incomplete water cages at the solid-liquid interface. The solubility, and hence the growth rate, increases with the partial pressure of methane in the vapor phase. The mass transport resistance from adsorption and the diffusion of methane are two competing factors, with the adsorption of methane at the interface found to be the rate-limiting step. The presence of a high concentration of incomplete clathrate hydrate cages presents strong affinity to dissolved methane at temperatures below the melting point. In addition to methane adsorption, water molecules must be expelled to form the complete clathrate cages. Both processes lead to a methane concentration minimum at 5-9 A in front of the growing interface. The methane concentration minimum provides the driving force for methane transport from the bulk to the interface. There are two types of solid layers of methane hydrate in the (1,0,0) direction. The growths of these layers are different, highly correlated, and affected by the methane concentration. A detailed mechanism of the layer growth is deduced from our simulations.
使用分子动力学模拟确定了影响甲烷水合物生长的关键因素。本研究使用了由甲烷气体、液态水和固态水合物相组成的三相分子模型。发现该模型在不同压力下的熔化温度与实验结果吻合良好。甲烷水合物的生长速率主要受以下三个因素影响:(1)甲烷在液相中的溶解度;(2)甲烷在水中的扩散系数;(3)甲烷在固-液界面处充满甲烷的不完全水笼中的吸附作用。溶解度,进而生长速率,随气相中甲烷的分压增加而增加。甲烷在界面上的吸附和扩散的传质阻力是两个相互竞争的因素,界面处的甲烷吸附被发现是限速步骤。在低于熔点的温度下,大量存在的不完全笼形水合物笼对溶解的甲烷具有很强的亲和力。除了甲烷吸附外,还必须排出水分子以形成完整的笼形水合物笼。这两个过程导致在生长界面前 5-9Å处甲烷浓度达到最小值。甲烷浓度最小值为甲烷从主体向界面传输提供了驱动力。在 (1,0,0) 方向上存在两种类型的甲烷水合物固体层。这些层的生长方式不同,高度相关,并受甲烷浓度的影响。从我们的模拟中推导出了层生长的详细机制。