The Optimum Maximum Allowed Displacement in Monte Carlo Simulation of Lennard-Jones Potential Point Particles = الحد الأقصى الأمثل للنزوح المسموح به في محاكاة مونت كارلو لجزيئات لينار جونز النقطية

Iyad Suwan, H. H. Al-Shraydeh, Abdelrahman Abulebdeh
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Abstract

In this paper, periodic systems of N point particles with Lennard-Jones potential are simulated in three dimensional space using Monte Carlo technique. The maximum allowed displacement used in Monte Carlo simulation of any Nparticle system controls the convergence of the calculated potential energy to its physical situation. The optimum maximum allowed displacement associated with 50% acceptance rate is found. Since Lennard-Jones potential is a short range one, it is considered to be zero beyond some cut-off radius. The optimum dimensionless cut-off radius in the Lennard-Jones case is 2.5, which is used in simulations. An explicit mathematical formula for the optimum maximum allowed displacement as a function of both temperature and density is obtained. This formula is predicted by fitting the Monte Carlo results using the fitting tools in Matlab.
在蒙特卡洛模拟模拟中,允许的最大限度迁移移徙是在我们熟悉的情况下发生的。
本文利用蒙特卡罗技术在三维空间中模拟了具有Lennard-Jones势的N点粒子周期系统。蒙特卡罗模拟中使用的最大允许位移控制着计算出的势能收敛到其物理状态。找到了在50%接受率下的最优最大允许排水量。由于伦纳德-琼斯势是近距势,所以在某个截止半径之外,它被认为是零。Lennard-Jones情况下的最佳无量纲截止半径为2.5,并用于模拟。得到了最佳最大允许位移随温度和密度的函数的显式数学公式。利用Matlab中的拟合工具对蒙特卡罗结果进行拟合,预测出该公式。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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