Laboratory of Computational Science and Modeling, Institute of Materials, École Polytechnique Fédérale de Lausanne, 1015 Lausanne, Switzerland.
J Chem Phys. 2018 Jun 21;148(23):231102. doi: 10.1063/1.5038396.
The curvature dependence of interfacial free energy, which is crucial in quantitatively predicting nucleation kinetics and the stability of bubbles and droplets, is quantified by the Tolman length δ. For solid-liquid interfaces, however, δ has never been computed directly due to various theoretical and practical challenges. Here we perform a direct evaluation of the Tolman length from atomistic simulations of a solid-liquid planar interface in out-of-equilibrium conditions, by first computing the surface tension from the amplitude of thermal capillary fluctuations of a localized version of the Gibbs dividing surface and by then calculating how much the surface energy changes when it is defined relative to the equimolar dividing surface. We computed δ for a model potential, and found a good agreement with the values indirectly inferred from nucleation simulations. The agreement not only validates our approach but also suggests that the nucleation free energy of the system can be perfectly described using classical nucleation theory if the Tolman length is taken into account.
界面自由能的曲率依赖性在定量预测成核动力学和气泡和液滴的稳定性方面至关重要,其由 Tolman 长度 δ 来量化。然而,由于各种理论和实际挑战,对于固-液界面,δ 从未被直接计算过。在这里,我们通过首先从局部化 Gibbs 分界面的热毛细涨落幅度计算表面张力,然后计算当相对于等摩尔分界面定义时表面能的变化量,从非平衡条件下的固-液平面界面的原子模拟中直接评估 Tolman 长度。我们为模型势计算了 δ,并发现与从成核模拟间接推断的值吻合良好。这种一致性不仅验证了我们的方法,还表明如果考虑 Tolman 长度,系统的成核自由能可以通过经典成核理论得到完美描述。