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Absolute entropy and free energy of fluids using the hypothetical scanning method.I.Calculation of transition probabilities from local grand canonical partition functions

机译:使用假设扫描方法计算流体的绝对熵和自由能I.根据局部大正则分配函数计算跃迁概率

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The hypothetical scanning (HS)method provides the absolute entropy and free energy from a Boltzmann sample generated by Monte Carlo,molecular dynamics or any other exact simulation procedure.Thus far HS has been applied successfully to magnetic and pol;ymer chain models;in this paper and the following one it is extended to fluid systems by treating a lennard-jones model of argon.With HS a probability P_i approximating the Boltzmann probability of system configuration i is calculated with a stepwise reconstruction procedured,based on adding atoms gradually layer-by-layer to an initially empty voume,where theky are replaced in their positions at i.At each step a transition probability (TP) is obtained from local grand canonical partition functions calculated over a limited space of the still unvisited (future)volume,tjhe larger this space the better the approximation.P i is the product of the step TPs,where In P_i is an upper bound of the absolute entropy,,which leads to upper and lover bounds for the free energy.We demonstrate that very good results for the entropy and the free energy can be obtained for a wide range of densities of the argon system by calculation TPs that are based on only a very limited future volume.
机译:假设扫描(HS)方法提供了由蒙特卡洛,分子动力学或任何其他精确模拟程序生成的玻尔兹曼样本的绝对熵和自由能。因此,到目前为止,HS已成功应用于磁链和高分子链模型中。本文通过处理氩的lennard-jones模型将其扩展到流体系统。在HS的基础上,通过逐步添加原子,通过逐步重构的方法,计算出近似于系统结构的玻尔兹曼概率i的概率P_i到初始为空的体,在第i步中将theky替换为它们的位置。在每个步骤中,从在尚未访问的(未来)体积的有限空间上计算出的局部大规范划分函数中获得过渡概率(TP)此空间越大,逼近度越好。Pi是步长TP的乘积,其中In P_i是绝对熵的上限,从而导致上界和下界我们证明通过计算仅基于非常有限的未来体积的TP可以在很大范围的氩气系统密度下获得非常好的熵和自由能结果。

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