Zhou Shiqi, Jamnik Andrej
Institute of Modern Statistical Mechanics, Zhuzhou Institute of Technology, Wenhua Road, Zhuzhou city 412008, People's Republic of China.
Phys Rev E Stat Nonlin Soft Matter Phys. 2006 Jan;73(1 Pt 1):011202. doi: 10.1103/PhysRevE.73.011202. Epub 2006 Jan 13.
Results for the density profiles of the Lennard-Jones (LJ) fluid subjected to diverse external fields are presented for the Monte Carlo simulations within the grand canonical ensemble and for the third order and second order perturbation density-functional approximation (DFA). In all cases, the bulk LJ fluid in the particle reservoir to which the nonuniform fluid under consideration is connected, is at the conditions situated at "dangerous" regions of the phase diagram, i.e., near the critical temperature or close to the gas-liquid coexistence curve. It is found that the previously investigated third order and second order perturbation DFA for hard core attractive Yukawa fluid [J. Chem. Phys. 122, 064503 (2005)] can perform successfully also for the nonuniform LJ fluid only on the condition of high accuracy of the required bulk second order direct correlation function. The present report further indicates that the proposed third order and second order perturbation DFA is efficient and suitable for both supercritical and subcritical temperatures.
给出了在巨正则系综下进行蒙特卡罗模拟以及三阶和二阶微扰密度泛函近似(DFA)时,处于不同外场的 Lennard-Jones(LJ)流体的密度分布结果。在所有情况下,所考虑的非均匀流体与之相连的粒子库中的体 LJ 流体,处于相图“危险”区域的条件下,即接近临界温度或靠近气液共存曲线。研究发现,先前针对硬核吸引 Yukawa 流体研究的三阶和二阶微扰 DFA[《化学物理杂志》122, 064503 (2005)],只有在所需体二阶直接相关函数具有高精度的条件下,才能成功用于非均匀 LJ 流体。本报告进一步表明,所提出的三阶和二阶微扰 DFA 对于超临界和亚临界温度都是高效且适用的。