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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Modified free volume theory of self-diffusion and molecular theory of shear viscosity of liquid carbon dioxide
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Modified free volume theory of self-diffusion and molecular theory of shear viscosity of liquid carbon dioxide

机译:液态二氧化碳自扩散的修正自由体积理论和剪切粘度分子理论

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In previous work on the density fluctuation theory of transport coefficients of liquids, it was necessary to use empirical self-diffusion coefficients to calculate the transport coefficients (e.g., shear viscosity of carbon dioxide). In this work, the necessity of empirical input of the self-diffusion coefficients in the calculation of shear viscosity is removed, and the theory is thus made a self-contained molecular theory of transport coefficients of liquids, albeit it contains an empirical parameter in the subcritical regime. The required self-diffusion coefficients of liquid carbon dioxide are calculated by using the modified free volume theory for which the generic van der Waals equation of state and Monte Carlo simulations are combined to accurately compute the mean free volume by means of statistical mechanics. They have been computed as a function of density along four different isotherms and isobars. A Lennard-Jones site-site interaction potential was used to model the molecular carbon dioxide interaction. The density and temperature dependence of the theoretical self-diffusion coefficients are shown to be in excellent agreement with experimental data when the minimum critical free volume is identified with the molecular volume. The self-diffusion coefficients thus computed are then used to compute the density and temperature dependence of the shear viscosity of liquid carbon dioxide by employing the density fluctuation theory formula for shear viscosity as reported in an earlier paper (J. Chem. Phys. 2000, 112, 7118). The theoretical shear viscosity is shown to be robust and yields excellent density and temperature dependence for carbon dioxide. The pair correlation function appearing in the theory has been computed by Monte Carlo simulations.
机译:在先前关于液体传输系数的密度波动理论的工作中,必须使用经验自扩散系数来计算传输系数(例如,二氧化碳的剪切粘度)。在这项工作中,消除了在计算剪切粘度时以经验值输入自扩散系数的必要性,因此该理论成为了液体输运系数的独立分子理论,尽管该理论中包含了经验参数。亚临界政权。液态二氧化碳所需的自扩散系数是使用修正的自由体积理论计算的,该理论将通用的范德华状态方程和蒙特卡洛模拟相结合,以借助统计力学准确地计算平均自由体积。它们是沿着四个不同的等温线和等压线作为密度的函数进行计算的。 Lennard-Jones的位-位相互作用势用于模拟分子二氧化碳的相互作用。当用分子体积确定最小临界自由体积时,理论上自扩散系数的密度和温度依赖性与实验数据非常吻合。如此计算出的自扩散系数随后被用于计算液态二氧化碳的剪切粘度的密度和温度依赖性,方法是采用密度波动理论公式计算剪切粘度,如先前论文中所述(J. Chem。Phys。2000, 112,7118)。理论剪切粘度显示出很强的稳定性,并且对二氧化碳产生出色的密度和温度依赖性。该理论中出现的对相关函数已通过蒙特卡洛模拟进行了计算。

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