Striolo A, Chialvo A A, Gubbins K E, Cummings P T
Department of Chemical Engineering, Vanderbilt University, Nashville, Tennesse 37235-1604, USA.
J Chem Phys. 2005 Jun 15;122(23):234712. doi: 10.1063/1.1924697.
Grand canonical Monte Carlo simulations are performed to study the adsorption of water in single-walled (6:6), (8:8), (10:10), (12:12), and (20:20) carbon nanotubes in the 248-548 K temperature range. At room temperature the resulting adsorption isotherms in (10:10) and wider single-walled carbon nanotubes (SWCNs) are characterized by negligible water uptake at low pressures, sudden and complete pore filling once a threshold pressure is reached, and wide adsorption/desorption hysteresis loops. The width of the hysteresis loops decreases as pore diameter narrows and it becomes negligible for water adsorption in (8:8) and (6:6) SWCNs. Results for the isosteric heat of adsorption, density profiles along the pore axis and across the pore radii, order parameter across the pore radii, and x-ray diffraction patterns are presented. Layered structures are observed when the internal diameter of the nanotubes is commensurate to the establishment of a hydrogen-bonded network. The structure of water in (8:8) and (10:10) SWCNs is ordered when the temperature is 298 and 248 K, respectively. By simulating adsorption isotherms at various temperatures, the hysteresis critical temperature, e.g., the lowest temperature at which no hysteresis can be detected, is determined for water adsorbed in (20:20), (12:12), and (10:10) SWCNs. The hysteresis critical temperature is lower than the vapor-liquid critical temperature for bulk Simple Point Charge-Extended (SPCE) water model.
进行巨正则蒙特卡罗模拟,以研究在248 - 548 K温度范围内,水在单壁(6:6)、(8:8)、(10:10)、(12:12)和(20:20)碳纳米管中的吸附情况。在室温下,(10:10)及更宽的单壁碳纳米管(SWCNs)中得到的吸附等温线的特征是,在低压下吸水量可忽略不计,一旦达到阈值压力,会突然且完全充满孔隙,并且有宽的吸附/解吸滞后环。随着孔径变窄,滞后环的宽度减小,对于(8:8)和(6:6)SWCNs中的水吸附,滞后环宽度变得可忽略不计。给出了吸附等量热、沿孔轴和跨孔半径的密度分布、跨孔半径的序参量以及X射线衍射图谱的结果。当纳米管的内径与氢键网络的建立相称时,会观察到分层结构。当温度分别为298 K和248 K时,(8:8)和(10:10)SWCNs中的水结构是有序的。通过模拟不同温度下的吸附等温线,确定了(20:20)、(12:12)和(10:10)SWCNs中水吸附的滞后临界温度,即无法检测到滞后现象的最低温度。对于体相简单点电荷扩展(SPCE)水模型,滞后临界温度低于气液临界温度。