Zhou Shiqi, Jamnik Andrej
Research Institute of Modern Statistical Mechanics, Zhuzhou Institute of Technology, Wenhua Road, Zhuzhou City 412008, People's Republic of China.
J Chem Phys. 2005 Feb 8;122(6):064503. doi: 10.1063/1.1843814.
Because of the scarcity of available simulation data for confined hard-core attractive Yukawa model fluid, extensive Monte Carlo (MC) simulation research for this fluid under the influence of various external potentials were carried out. The present MC simulation results were employed to test a performance of the third-order perturbation density functional theory (DFT) based on a high order direct correlation function (DCF) [S. Zhou and E. Ruckenstein, Phys. Rev. E. 61, 2704 (2000)]. It was found that the present perturbation DFT formalism is soundly structured only if the imported second-order DCF is reliable. In this case, the accuracy of the results can be satisfactory or even very high for various types of external potentials. Further, the associated adjustable parameter can be universal, i.e., independent of the particular external field responsible for the generation of a nonuniform density profile. Dependence of both the maintenance of the reliability of the formalism and holding of the universality of the adjustable parameter on the accuracy of the imported bulk second-order DCF can be strengthened by the large difference between the external field investigated and that caused by a single hard wall used for specification of the adjustable parameter. In case the gaseous density in the subcritical region is below the coexistence density, an excellent performance of the present formalism is observed even for the mean spherical approximation's second-order DCF as an input. This advantageous property, combined with the fact that the present formalism needs only the second-order DCF of fluid at the coexistence state as an input, enables the present formalism to be a very good theoretical tool for the investigations of wetting and prewetting transitions.
由于受限硬核吸引 Yukawa 模型流体的可用模拟数据稀缺,因此对该流体在各种外部势影响下进行了广泛的蒙特卡罗(MC)模拟研究。利用当前的 MC 模拟结果来测试基于高阶直接相关函数(DCF)的三阶微扰密度泛函理论(DFT)的性能 [S. Zhou 和 E. Ruckenstein,《物理评论 E》61,2704(2000)]。发现只有当引入的二阶 DCF 可靠时,当前的微扰 DFT 形式才具有合理的结构。在这种情况下,对于各种类型的外部势,结果的准确性可以令人满意甚至非常高。此外,相关的可调参数可以是通用的,即独立于负责产生非均匀密度分布的特定外部场。所研究的外部场与用于指定可调参数的单个硬壁所引起的外部场之间的巨大差异,可以增强形式可靠性的维持和可调参数通用性的保持对引入的体二阶 DCF 准确性的依赖性。在亚临界区域的气体密度低于共存密度的情况下,即使将平均球近似的二阶 DCF 作为输入,也能观察到当前形式的出色性能。这种有利特性,再加上当前形式仅需要共存状态下流体的二阶 DCF 作为输入这一事实,使得当前形式成为研究润湿和预润湿转变的非常好的理论工具。