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Application of density functional perturbation theory to pure fluid liquid-vapor interfaces

机译:密度泛函摄动理论在纯流体液汽界面的应用

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Common density functional theories often use the so-called mean-field approximation to the attractive term of the free energy. which is not accurate when compared with molecular dynamics simulations. We applied a modification of this attractive free energy term of a local density functional approach where an analytical representation of the radial distribution function is taken into account. A cutoff Lennard-Jones-12-fi potential. divided according to the Weeks—Chandler— Andersen prescription, is used as the intermolecular interaction force model. This density functional perturbation approach gives the correct phase quilibrium and predicts a surface tension in excellent agreement with recent molecular dynamics simulations. The surface tension of some pure simple fluids is predicted from an intrinsic contribution, obtained b~ the modified density functional perturbation theory. plus contributions due to capillary wave roughening of the surface. The respective Lennard-Jones potential parameters were obtained from fitting to saturated liquid densities of the pure fluids.
机译:常见的密度泛函理论通常使用所谓的平均场近似法来描述自由能的吸引项。与分子动力学模拟相比,这是不准确的。我们对局部密度函数方法的这种有吸引力的自由能项进行了修改,其中考虑了径向分布函数的解析表示。 Lennard-Jones-12-fi的截止电位。根据Weeks-Chandler-Andersen处方进行划分,将其用作分子间相互作用力模型。这种密度泛函摄动方法可提供正确的相位平衡,并预测表面张力,与最近的分子动力学模拟极为吻合。根据修正的密度泛函微扰理论获得的内在贡献,可以预测一些纯简单流体的表面张力。加上由于毛细波使表面粗糙而产生的贡献。通过拟合纯流体的饱和液体密度,获得各自的Lennard-Jones势参数。

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