Department of Chemical and Biomolecular Engineering, North Carolina State University, Raleigh, North Carolina 27695-7905, USA.
Department of Chemical and Biomolecular Engineering, National University of Singapore, 4 Engineering Drive 4, Singapore 117585.
J Chem Phys. 2018 Aug 28;149(8):084109. doi: 10.1063/1.5037054.
While much work has been reported on the statistical mechanics and molecular simulation of interfaces of planar and spherical geometries, very little has been published on the interfaces of cylindrical geometry. The cylindrical geometry is important for the study of cylindrical micelles and particularly for nano-phases confined within cylindrical pores since the most well-defined porous materials (e.g., carbon and silicon nanotubes, SBA-15 and KIT-6 silicas) that are presently available are of this geometry. In this work, we derive the statistical mechanical equations for the pressure tensor for an interfacial region of cylindrical geometry via the virial route and for the condition of mechanical (hydrostatic) equilibrium. We also report the equation for the surface tension via the mechanical route. Monte Carlo and molecular dynamics simulation results are obtained for two example systems involving a fluid nano-phase of Lennard-Jones argon: a gas-liquid interface of cylindrical geometry and a confined nano-phase within a cylindrical carbon pore. All three diagonal elements of the pressure tensor are reported in each case, the component normal to the interface, = , and the two tangential components = and = , where (, , ) are the usual cylindrical polar coordinates. For the cylindrical pore, the tangential pressures, and , show strong compression in the adsorbed layers, as has been found in slit-shaped and spherical pores.
虽然已经有很多关于平面和球形几何界面的统计力学和分子模拟的工作被报道,但关于圆柱几何界面的工作却很少。圆柱几何对于研究圆柱胶束非常重要,特别是对于受限在圆柱孔内的纳米相,因为目前最明确的多孔材料(例如碳和硅纳米管、SBA-15 和 KIT-6 硅石)都是这种几何形状。在这项工作中,我们通过维里途径推导了圆柱几何界面区域压力张量的统计力学方程,以及力学(静水力学)平衡的条件。我们还通过力学途径报告了表面张力的方程。对于涉及 Lennard-Jones 氩气流体纳米相的两个示例系统,我们获得了蒙特卡罗和分子动力学模拟结果:圆柱几何的气液界面和圆柱碳孔内受限的纳米相。在每种情况下,我们都报告了压力张量的所有三个对角元素,即垂直于界面的分量 = ,以及两个切向分量 = 和 = ,其中(,, )是通常的圆柱极坐标。对于圆柱孔,切向压力 和 ,在吸附层中表现出强烈的压缩,这在狭缝状和球形孔中已经发现。