拉普拉斯压力
表面张力
拉普拉斯方程
半径
拉普拉斯变换
热力学
氩
最大气泡压力法
蒸汽压
机械
化学
物理
数学
数学分析
量子力学
微分方程
计算机科学
计算机安全
有机化学
作者
Hong Yan,Jiachen Wei,Shuwen Cui,Shenghua Xu,Zhiwei Sun,Rui Zhu
标识
DOI:10.1134/s0036024416030158
摘要
Debates continue on the applicability of the Young–Laplace equation for droplets, vapor bubbles and gas bubbles in nanoscale. It is more meaningful to find the error range of the Young–Laplace equation in nanoscale instead of making the judgement of its applicability. To do this, for seven liquid argon drops (containing 800, 1000, 1200, 1400, 1600, 1800, or 2000 particles, respectively) at T = 78 K we determined the radius of surface of tension R s and the corresponding surface tension γ s by molecular dynamics simulation based on the expressions of R s and γ s in terms of the pressure distribution for droplets. Compared with the two-phase pressure difference directly obtained by MD simulation, the results show that the absolute values of relative error of two-phase pressure difference given by the Young–Laplace equation are between 0.0008 and 0.027, and the surface tension of the argon droplet increases with increasing radius of surface of tension, which supports that the Tolman length of Lennard-Jones droplets is positive and that Lennard-Jones vapor bubbles is negative. Besides, the logic error in the deduction of the expressions of the radius and the surface tension of surface of tension, and in terms of the pressure distribution for liquid drops in a certain literature is corrected.
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