在MD模拟中扩散系数的系统大小依赖:纯密度流体的简单校正公式
1Joint Institute for High Temperatures, Russian Academy of Sciences, Moscow 125412, Russia.
The journal of physical chemistry. B
|January 3, 2024
概括
一个新的公式从分子动力学 (MD) 模拟中纠正自我扩散系数. 这种校正考虑了系统大小,提高了热力学极限中的密度液体的准确性.
科学领域:
- 计算物理学的计算物理.
- 化学物理 化学物理
- 材料科学是一种材料科学.
背景情况:
- 分子动力学 (MD) 模拟对于理解液体特性至关重要.
- 模拟通常使用周期性边界条件,引入有限大小的效果.
- 准确的自我扩散系数对于运输现象研究至关重要.
研究的目的:
- 为自我扩散系数开发一个实际的校正公式.
- 为了将模拟结果与热力学极限联系起来.
- 提供一种方法来提高密集液体的MD模拟的准确性.
主要方法:
- 一个校正公式的推导:D = D0(1 - γN^-1/3).
- 公式应用于纯密度流体.
- 使用不同系统大小和几何形状的分子动力学模拟进行验证.
主要成果:
- 建立了一个简单,实用的公式来纠正有限大小的效应.
- 校正因子 γ 取决于模拟细胞的几何形状.
- γ 1.0 对于常见的立方模拟细胞几何.
- 该公式的有效性得到了最近的MD模拟结果的证实.
结论:
- 拟议的公式准确地纠正了MD模拟中的自我扩散系数.
- 这种修正弥合了模拟数据和热力学极限之间的差距.
- 这些发现提高了MD模拟密集流体运输特性的可靠性.
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