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Molecular Dynamics Simulation of the Cage Effect in a Wide Packing Fraction Range

机译:宽填料分数范围内笼式效应的分子动力学模拟

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The self-diffusion coefficient and particle residence time in the first coordination shell of its neighbours were investigated by molecular dynamics simulation with the packing fraction of the model system ranging from 0.1 to 0.8. The residence time distribution spans several orders of magnitude and broadens with the system packing fraction. The distribution exhibits a maximum localized in the short residence time region. The average residence time correlates with the conventionally-used intermolecular correlation time governed by the mutual particle translational diffusion. It was shown that the use of the coordination number as an argument for all searched parameters is the obvious representation of the cage effect onset. The agreement of the self-diffusion coefficient with one of the recent theories is excellent in most of the density range, including the start of the glass transition, with the largest divergence only observed for the rare gas state. The same conclusion is true for the simulated and theoretical values of the caging number, which is nearly five, defining the start of the system liquefaction.
机译:通过分子动力学模拟研究了其邻居的第一协调壳中的自扩散系数和颗粒停留时间,其模型系统的填充部分范围为0.1至0.8。停留时间分配跨越几个数量级并随系统包装分数拓宽。分布在短暂停留时间区域中呈现最大局部。平均停留时间与由相互粒子平移扩散控制的常规使用的分子间相关时间相关。结果表明,使用协调号作为所有搜索参数的参数是笼效应发作的明显表示。自扩散系数与最近理论之一的协议在大多数密度范围内具有优异的优异,包括玻璃化转变的开始,仅针对稀有气态观察到最大的发散。对于持续数量的模拟和理论值,相同的结论是近五个,定义了系统液化的开始。

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