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Solid-liquid interface free energy in binary systems: Theory and atomistic calculations for the (110) Cu-Ag interface

机译:二元系统中的固液界面自由能:(110)Cu-Ag界面的理论和原子计算

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摘要

We analyze thermodynamics of solid-liquid interfaces in binary systems when the solid is in a nonhydrostatic state of stress. The difficulty lies in the fact that chemical potential of at least one of the chemical components in a nonhydrostatic solid is an undefined quantity. We show, nevertheless, that the interface free energy γ can be defined as excess of an appropriate thermodynamic potential that depends on the chemical potentials in the liquid phase. We derive different forms of the adsorption equation for solid-liquid interfaces, with differential coefficients representing excesses of extensive properties. This leads, in particular, to the formulation of interface stress τ_(ij) as an appropriate excess over nonhydrostatic bulk stresses. The interface stress is not unique unless the solid is in a hydrostatic state of stress. We also derive Gibbs-Helmholtz type equations that can be applied for thermodynamic integration of γ. All thermodynamic relations derived here are presented in forms suitable for atomistic simulations. In particular, the excess quantities can be computed without constructing interface profiles. As an application, we perform semigrand canonical Monte Carlo simulations of the (110) solid-liquid interface in the Cu–Ag system. We show that γ computed by thermodynamic integration along a coexistence path decreases with increasing composition difference between the phases. At the same time, τ_(ij) remains negative (i.e., the interface is in a state of compression), drastically increases in magnitude, and becomes highly anisotropic. Some of the interface excess properties are computed by different methods and demonstrate accurate agreement with each other, confirming the correctness of our analysis.
机译:当固体处于应力的非静水状态时,我们分析了二元系统中固液界面的热力学。困难在于,非静水固体中至少一种化学成分的化学势是不确定的。然而,我们表明,界面自由能γ可以定义为取决于液相化学势的适当热力学势的过量。我们推导了固液界面吸附方程的不同形式,其中微分系数代表了广泛的过剩特性。这尤其导致将界面应力τ_(ij)表示为比非静水整体应力适当的过量。除非固体处于应力的静水状态,否则界面应力不是唯一的。我们还导出了可用于γ的热力学积分的Gibbs-Helmholtz型方程。此处导出的所有热力学关系均以适用于原子模拟的形式表示。特别是,无需构建接口配置文件就可以计算多余的数量。作为应用,我们对Cu-Ag系统中的(110)固液界面进行了半盛大的经典蒙特卡洛模拟。我们表明,沿着共存路径通过热力学积分计算出的γ随着相之间组成差异的增加而减小。同时,τ_(ij)保持负值(即,界面处于压缩状态),幅度急剧增加,并且变得高度各向异性。一些界面多余的属性是通过不同的方法计算的,并且彼此之间显示出精确的一致性,从而证实了我们分析的正确性。

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