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The EXP pair-potential system. III. Thermodynamic phase diagram

机译:exp配对潜在系统。 III。 热力学相图

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This paper determines the thermodynamic phase diagram of the EXP system of particles interacting by the purely repulsive exponential pair potential. The solid phase is face-centered cubic (fcc) at low densities and pressures. At higher densities and pressures, the solid phase is body-centered cubic (bcc) with a re-entrant liquid phase at the highest pressures simulated. The investigation first identifies the phase diagram at zero temperature at which the following four crystal structures are considered: fcc, bcc, hexagonal close packed, and cubic diamond. There is a T = 0 phase transition at pressure 2.651 x 10(-3) with the thermodynamically stable structure being fcc below and bcc above this pressure. The densities of the two crystal structures at the phase transition are 1.7469 x 10(-2) (fcc) and 1.7471 x 10(-2) (bcc). At finite temperatures, the fcc-bcc, fcc-liquid, and bcc-liquid coexistence lines are determined by numerical integration of the Clausius-Clapeyron equation and validated by interface-pinning simulations at selected state points. The bcc-fcc phase transition is a weak first-order transition. The liquid-fcc-bcc triple point, which is determined by the interface-pinning method, has temperature 5.9 x 10(-5) and pressure 2.5 x 10(-6); the triple-point densities are 1.556 x 10(-3) (liquid), 1.583 x 10(-3) (bcc), and 1.587 x 10(-3) (fcc). (C) 2019 Author(s).
机译:本文确定由纯粹斥力指数对潜在相互作用粒子的EXP系统的热力学相图。固相是面心在低密度和压力立方(fcc)。在更高的密度和压力,固相是体心立方(BCC)与模拟的最高压力重入液相。调查首先识别在零温度下的相图在该以下四种晶体结构被认为是:FCC,BCC,密排六方和立方金刚石。有一个在压力2.651×10(-3)具有热力学稳定的结构是面心立方下面和BCC这个压力以上的T = 0的相变。在相变两个晶体结构的密度1.7469×10(-2)(FCC)和1.7471×10(-2)(BCC)。在有限的温度下,FCC-BCC,FCC-液体,和BCC-液共存线由克劳修斯 - 克拉贝龙方程的数值积分来确定,并通过在选择状态点接口钉扎仿真验证。密件抄送-FCC相变是弱一阶过渡。液体FCC-BCC三相点,这是由接口钉扎法测定,具有温度5.9×10(-5)和压力为2.5×10(-6);三重点密度是1.556×10(-3)(液体),1.583×10(-3)(BCC),和1.587×10(-3)(FCC)。 (c)2019年作者。

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