首页> 外文期刊>The Journal of Chemical Physics >Water in carbon nanotubes: Adsorption isotherms and thermodynamic properties from molecular simulation - art. no. 234712
【24h】

Water in carbon nanotubes: Adsorption isotherms and thermodynamic properties from molecular simulation - art. no. 234712

机译:碳纳米管中的水:分子模拟的吸附等温线和热力学性质-艺术。没有。 234712

获取原文
获取原文并翻译 | 示例
           

摘要

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 (SPC/E) water model. (C) 2005 American Institute of Physics.
机译:进行了大规范的蒙特卡洛模拟,以研究水在单壁(6:6),(8:8),(10:10),(12:12)和(20:20)碳纳米管中的水吸附。 248-548 K的温度范围。在室温下,在(10:10)和更宽的单壁碳纳米管(SWCN)中产生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,孔就会突然完全填充,并且吸附/解吸范围宽磁滞回线。磁滞回线的宽度随着孔径的减小而减小,并且对于(8:8)和(6:6)SWCN中的吸水率可以忽略不计。给出了等排吸附热的结果,沿孔轴和整个孔半径的密度分布,整个孔半径的有序参数以及X射线衍射图。当纳米管的内径与氢键网络的建立相称时,观察到层状结构。当温度分别为298 K和248 K时,(8:8)和(10:10)SWCN中的水结构是有序的。通过模拟各种温度下的吸附等温线,确定了吸附在(20:20),(12:12)和(10:10)中的水的滞后临界温度,例如无法检测到滞后的最低温度。 SWCN。对于大容量简单点电荷扩展(SPC / E)水模型,滞后临界温度低于汽液临界温度。 (C)2005美国物理研究所。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号