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Equation of state in the generalized density scaling regime studied from ambient to ultra-high pressure conditions

机译:在从环境到超高压条件下研究的广义密度缩放方案中的状态方程

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In this paper, based on the effective intermolecular potential with well separated density and configuration contributions and the definition of the isothermal bulk modulus, we derive two similar equations of state dedicated to describe volumetric data of supercooled liquids studied in the extremely wide pressure range related to the density range, which is extremely wide in comparison with the experimental range reached so far in pressure-volume-temperature measurements of glass-forming liquids. Both the equations comply with the generalized density scaling law of molecular dynamics versus h(ρ)/T at different densities ρ and temperatures T, where the scaling exponent can be in general only a density function γ (ρ) = d ln h/d ln ρ as recently argued by the theory of isomorphs. We successfully verify these equations of state by using data obtained from molecular dynamics simulations of the Kob-Andersen binary Lennard-Jones liquid. As a very important result, we find that the one-parameter density function h(ρ) analytically formulated in the case of this prototypical model of supercooled liquid, which implies the one-parameter density function γ (ρ), is able to scale the structural relaxation times with the value of this function parameter determined by fitting the volumetric simulation data to the equations of state.We also show that these equations of state properly describe the pressure dependences of the isothermal bulk modulus and the configurational isothermal bulk modulus in the extremely wide pressure range investigated by the computer simulations. Moreover, we discuss the possible forms of the density functions h(ρ) and γ (ρ) for real glass formers, which are suggested to be different from those valid for the model of supercooled liquid based on the Lennard- Jones intermolecular potential.
机译:在本文中,基于有效的分子间电势,具有良好的密度和构型分布,并定义了等温体积模量,我们推导了两个相似的状态方程,专门描述了在与密度范围,与迄今为止在形成玻璃的液体的压力-体积-温度测量中所达到的实验范围相比非常宽。这两个方程均符合在不同密度ρ和温度T下分子动力学与h(ρ)/ T的关系的广义密度标度定律,其中标度指数通常只能是密度函数γ(ρ)= d ln h / d lnρ,最近由同构理论提出来。我们通过使用从Kob-Andersen二元Lennard-Jones液体的分子动力学模拟获得的数据成功验证了这些状态方程。作为一个非常重要的结果,我们发现在这种过冷液体的原型模型的情况下,通过解析公式得出的一参数密度函数h(ρ)可以标定一参数密度函数γ(ρ)。通过将体积模拟数据拟合到状态方程来确定结构弛豫时间,并用该函数参数的值确定状态方程。计算机模拟研究了宽压力范围。此外,我们讨论了用于真实玻璃形成器的密度函数h(ρ)和γ(ρ)的可能形式,这被认为与基于Lennard-Jones分子间电势的过冷液体模型有效的形式不同。

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