Department of Mechanical Engineering, Osaka University, 2-1 Yamadaoka, Suita 565-0871, Japan.
Institute of Fluid Science, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan.
J Chem Phys. 2019 Jan 28;150(4):044701. doi: 10.1063/1.5053881.
In this study, we carried out molecular dynamics simulations of a cylindrical Lennard-Jones droplet on a flat and smooth solid surface and showed that Young's equation as the relation among solid-liquid, solid-vapor, and liquid-vapor interfacial tensions γ, γ, and γ, respectively, was applicable only under a very restricted condition. Using the fluid stress-tensor distribution, we examined the force balance in the surface-lateral direction exerted on a rectangular control volume set around the contact line. As the mechanical route, the fluid stress integrals along the two control surfaces normal to the solid-fluid interface were theoretically connected with γ and γ relative to the solid-vacuum interfacial tension γ by Bakker's equation extended to solid-related interfaces via a thought experiment, for which the position of the solid-fluid interface plane was defined at the limit that the fluid molecules could reach. On the other hand, the fluid stress integral along the control surface lateral to the solid-fluid interface was connected with γ by the Young-Laplace equation. Through this connection, we showed that Young's equation was valid for a system in which the net lateral force exerted on the fluid molecules from the solid surface was zero around the contact line. Furthermore, we compared γ - γ and γ - γ obtained by the mechanical route with the solid-liquid and solid-vapor works of adhesion obtained by the dry-surface method as one of the thermodynamic routes and showed that both routes resulted in a good agreement. In addition, the contact angle predicted by Young's equation with these interfacial tensions corresponded well to the apparent droplet contact angle determined by using the previously defined position of the solid-fluid interface plane; however, our theoretical derivation indicated that this correspondence was achieved because the zero-lateral force condition was satisfied in the present system with a flat and smooth solid surface. These results indicated that the contact angle should be predicted not only by the interfacial tensions but also by the pinning force exerted around the contact line.
在这项研究中,我们对圆柱形 Lennard-Jones 液滴在平坦光滑固体表面上进行了分子动力学模拟,结果表明,杨氏方程分别作为固-液、固-气和液-气界面张力γ、γ和γ之间的关系,仅在非常有限的条件下适用。通过分析流体应力张量的分布,我们研究了围绕接触线设置的矩形控制体积周围在表面横向方向上对液滴施加的力平衡。作为力学途径,通过 Bakker 方程将沿两个垂直于固-液界面的控制面的流体应力积分与相对于固-真空界面张力γ的γ和γ理论上联系起来,通过思想实验将该方程扩展到与固体相关的界面,其中固-液界面平面的位置定义为流体分子可以到达的极限位置。另一方面,沿垂直于固-液界面的控制面的流体应力积分与γ通过 Young-Laplace 方程联系起来。通过这种联系,我们证明了杨氏方程对于在接触线周围从固体表面向流体分子施加的净横向力为零的系统是有效的。此外,我们通过力学途径得到的γ-γ和γ-γ与通过干表面方法得到的固-液和固-气粘附功进行了比较,这是热力学途径之一,并表明两种途径都得到了很好的一致性。此外,杨氏方程预测的接触角与使用先前定义的固-液界面平面位置确定的表观液滴接触角非常吻合;然而,我们的理论推导表明,这种对应关系是因为在具有平坦光滑固体表面的本系统中满足了零横向力条件。这些结果表明,接触角不仅应该由界面张力来预测,还应该由围绕接触线施加的钉扎力来预测。