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Molecular dynamics simulation of the diffusion of nanoconfined fluids

机译:纳米密闭流体扩散的分子动力学模拟

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A new molecular dynamics simulation technique for simulating fluids in confinement [H. Eslami, F. Mozaffari, J. Moghadasi, F. Müller-Plathe, J. Chem. Phys. 129 (2008) 194702] is employed to simulate the diffusion coefficient of nanoconfined Lennard-Jones fluid. The diffusing fluid is liquid Ar and the confining surfaces are solid Ar fcc (100) surfaces, which are kept frozen during the simulation. In this simulation just the fluid in confinement is simulated at a constant temperature and a constant parallel component of pressure, which is assumed to be equal to the bulk pressure. It is shown that the calculated parallel (to the surfaces) component of the diffusion coefficients depends on the distance between the surfaces (pore size) and shows oscillatory behavior with respect to the intersurface separations. Our results show that on formation of well-organized layers between the surfaces, the parallel diffusion coefficients decrease considerably with respect to the bulk fluid. The effect of pressure on the parallel diffusion coefficients has also been studied. Better organized layers, and hence, lower diffusion coefficients are observed with increasing the pressure.
机译:一种用于模拟流体的新的分子动力学模拟技术[H. Eslami,F.Mozaffari,J.Moghadasi,F.Müller-Plathe,J.Chem。物理129(2008)194702]被用于模拟纳米约束的伦纳德-琼斯流体的扩散系数。扩散流体为液态Ar,封闭表面为固态Ar fcc(100)表面,在模拟过程中保持冻结状态。在此模拟中,仅在恒定温度和恒定平行压力分量(假定等于总体压力)下模拟处于限制状态的流体。结果表明,所计算的扩散系数的平行于(平行于表面)分量取决于表面之间的距离(孔尺寸),并显示出相对于表面间间距的振荡行为。我们的结果表明,在表面之间形成井井有条的层时,平行扩散系数相对于大体积流体会大大降低。还研究了压力对平行扩散系数的影响。随着压力的增加,更好的组织层,因此观察到较低的扩散系数。

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