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Pseudo hard-sphere potential for use in continuous molecular-dynamics simulation of spherical and chain molecules

机译:伪硬球势,用于球形和链状分子的连续分子动力学模拟

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We present a continuous pseudo-hard-sphere potential based on a cut-and-shifted Mie (generalized Lennard-Jones) potential with exponents (50, 49). Using this potential one can mimic the volumetric, structural, and dynamic properties of the discontinuous hard-sphere potential over the whole fluid range. The continuous pseudo potential has the advantage that it may be incorporated directly into off-the-shelf molecular-dynamics code, allowing the user to capitalise on existing hardware and software advances. Simulation results for the compressibility factor of the fluid and solid phases of our pseudo hard spheres are presented and compared both to the Carnahan-Starling equation of state of the fluid and published data, the differences being indistinguishable within simulation uncertainty. The specific form of the potential is employed to simulate flexible chains formed from these pseudo hard spheres at contact (pearl-necklace model) for m_c 4, 5, 7, 8, 16, 20, 100, 201, and 500 monomer segments. The compressibility factor of the chains per unit of monomer, m_c, approaches a limiting value at reasonably small values, m_c 50, as predicted by Wertheims first order thermodynamic perturbation theory. Simulation results are also presented for highly asymmetric mixtures of pseudo hard spheres, with diameter ratios of 3:1, 5:1, 20:1 over the whole composition range.
机译:我们基于具有指数(50、49)的平移后的Mie(广义Lennard-Jones)电势,给出了连续的伪硬球电势。利用这一势能可以模拟整个流体范围内不连续硬球势的体积,结构和动力学特性。连续的伪电位的优点是可以直接将其合并到现有的分子动力学代码中,从而使用户可以利用现有的硬件和软件改进。给出了我们的伪硬球体的固相和固相压缩系数的模拟结果,并将其与流体状态的Carnahan-Starling方程和已公开的数据进行了比较,在模拟不确定性内两者之间的差异是无法区分的。使用特定形式的电势来模拟由这些伪硬球在接触时(珍珠项链模型)形成的柔性链,适用于m_c 4、5、7、8、16、20、100、201和500单体链段。如Wertheims一阶热力学扰动理论所预测的,每单位单体链的压缩系数m_c接近极限值,m_c 50很小。还给出了伪硬球的高度不对称混合物的模拟结果,其在整个成分范围内的直径比为3:1、5:1、20:1。

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