聚有机磷腈气体渗透性的原子模拟。第1部分。保利(dibutoxyphosphazenes)

J.R. Fried, P. Ren
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引用次数: 37

摘要

采用COMPASS分子力学力场进行分子模拟,研究了He、Ne、O2、N2、CH4和CO2六种气体分子在聚[双(正丁氧基)磷腈](PnBuP)和聚[双(中丁氧基)磷腈](PsBuP)中的自扩散和溶解度系数。通过分子动力学(NVT系综)得到扩散系数,模拟时间为3ns。用大正则蒙特卡罗(GCMC)方法计算了溶解度系数。两种模拟的结果大体上与实验数据一致,但PsBuP中气体溶解度的模拟结果除外,其中与数据的差异可能归因于实验样品的微结晶度。在扩散系数的情况下,扩散系数与扩散气体有效直径的平方成正比。同样,通过GCMC模拟吸附等温线得到的溶解度系数与Lennard-Jones势井深度参数ε /k之间也存在良好的相关性。采用Gusev和Suter过渡状态模型确定PnBuP、PsBuP和聚双(异丁氧基)磷腈(PiBuP)的自由体积和自由体积分布。发现给定气体在聚磷腈中的扩散系数与其可接近的自由体积分数呈指数相关。由硬球液体自扩散的Cohen-Turnbull理论推导出的可接近自由体积分布模型与模拟结果拟合得很好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The atomistic simulation of the gas permeability of poly(organophosphazenes). Part 1. Poly(dibutoxyphosphazenes)

Self-diffusion and solubility coefficients of six gas molecules (He, Ne, O2, N2, CH4, and CO2) in two poly(dibutoxyphosphazenes)—poly[bis(n-butoxy)phosphazene] (PnBuP) and poly[bis(sec-butoxy)phosphazene] (PsBuP)—have been investigated by means of molecular simulation using the COMPASS molecular mechanics force field. Diffusion coefficients were obtained from molecular dynamics (NVT ensemble) using up to 3 ns simulation time. Solubility coefficients were obtained by means of a Grand Canonical Monte Carlo (GCMC) method. Results of both simulations were in generally good agreement with experimental data with the exception of the simulation results for gas solubility in PsBuP where differences from the data may be attributed to microcrystallinity of the experimental sample. In the case of diffusivity, diffusion coefficients correlated well with the square of the effective diameter of the diffusing gas. Similarly a good correlation was found between the solubility coefficients obtained by GCMC simulation of sorption isotherms and the Lennard-Jones potential well depth parameter, ϵ/k.

The transition-state model of Gusev and Suter was used to determine free volume and free volume distribution for PnBuP, PsBuP, and poly[bis(iso-butoxy)phosphazene] (PiBuP). The diffusion coefficient for a given gas in each polyphosphazene was found to correlate exponentially with its accessible free volume fraction. A model for the distribution of accessible free volume, derived from the Cohen–Turnbull theory for the self diffusion of a liquid of hard spheres, was found to provide excellent fit with the simulation results.

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