Departamento de Química Inorgánica, Analítica, y Química Física-INQUIMAE, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Ciudad Universitaria, Pab. II, Buenos Aires C1428EHA, Argentina.
J Chem Phys. 2010 Jul 21;133(3):034513. doi: 10.1063/1.3462964.
Molecular dynamics simulations of water in cylindrical hydrophilic pores with diameters of 1.5 and 3 nm were performed to explore the phase behavior and the nucleation dynamics of the confined fluid as a function of the percentage of volume filled f. The interactions of water with the pore wall were considered to be identical to the interactions between water molecules. At low water contents, all the water is adsorbed to the surface of the pore. A second phase consisting of a liquid plug appears at the onset filling for capillary condensation, f(onset)=27% and 34% for the narrow and wide pores, respectively. In agreement with experimental results for silica pores, the liquid phase appears close to the equilibrium filling f(eq) in the 1.5 nm pore and under conditions of strong surface supersaturations for the 3 nm pore. After condensation, two phases, a liquid plug and a surface-adsorbed phase, coexist in equilibrium. Under conditions of phase coexistence, the water surface density Gamma(coex) was found to be independent of the water content and the diameter of the pore. The value of Gamma(coex) found in the simulations (approximately 3 nm(-2)) is in good agreement with experimental results for silica pores, suggesting that the interactions of water with silica and with itself are comparable. The surface-adsorbed phase at coexistence is a sparse monolayer with a structure dominated by small water clusters. We characterize the density and structure of the liquid and surface phases, the nucleation mechanism of the water plug, and the effect of surface hydrophilicity on the two-phase equilibrium and hysteresis. The results are discussed in light of experiments and previous simulations.
采用直径为 1.5nm 和 3nm 的亲水圆柱形孔进行了水分子的分子动力学模拟,以研究受限流体的相行为和形核动力学作为填充体积分数 f 的函数。水分子与孔壁的相互作用被认为与水分子之间的相互作用相同。在低含水量时,所有的水都被吸附在孔的表面。在毛细凝结开始填充时,出现第二相,包含一个液塞,对于窄孔和宽孔,分别在填充分数 f(onset)=27%和 34%时出现。与二氧化硅孔的实验结果一致,在 1.5nm 孔中,在接近平衡填充 f(eq)的条件下,以及在 3nm 孔中在强表面过饱和度的条件下,出现液相。凝结后,两个相,一个液塞和一个表面吸附相,处于平衡共存状态。在相共存的条件下,发现水的表面密度 Gamma(coex)与含水量和孔的直径无关。模拟中发现的 Gamma(coex)值(约为 3nm(-2)))与二氧化硅孔的实验结果非常吻合,表明水与二氧化硅和自身的相互作用相当。在共存时的表面吸附相是一个稀疏的单层,结构由小的水分子簇主导。我们描述了液相等温线和表面相的密度和结构、水塞的形核机制,以及表面亲水性对两相平衡和滞后的影响。结果根据实验和以前的模拟进行了讨论。