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首页> 外文期刊>The Journal of Chemical Physics >Magnitude and orientation dependence of intermolecular interaction of perfluoropropane dimer studied by high-level ab initio calculations: Comparison with propane dimer
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Magnitude and orientation dependence of intermolecular interaction of perfluoropropane dimer studied by high-level ab initio calculations: Comparison with propane dimer

机译:高水平从头算研究全氟丙烷二聚体分子间相互作用的幅度和方向依赖性:与丙烷二聚体的比较

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摘要

Intermolecular interaction energies of 12 orientations of C3F8 dimers were calculated with electron correlation correction by the second-order Moller-Plesset perturbation method. The antiparallel C-2h dimer has the largest interaction energy (-1.45 kcal/mol). Electron correlation correction increases the attraction considerably. Electrostatic energy is not large. Dispersion is mainly responsible for the attraction. Orientation dependence of the interaction energy of the C3F8 dimer is substantially smaller than that of the C3H8 dimer. The calculated interaction energy of the C3F8 dimer at the potential minimum is 78% of that of the C3H8 dimer (-1.85 kcal/mol), whereas the interaction energies of the CF4 and C2F6 dimers are larger than those of the CH4 and C2H6 dimers. The intermolecular separation in the C3F8 dimer at the potential minimum is substantially larger than that in the C3H8 dimer. The larger intermolecular separation due to the steric repulsion between fluorine atoms is the cause of the smaller interaction energy of the C3F8 dimer at the potential minimum. The calculated intermolecular interaction energy potentials of the C3F8 dimers using an all atom model OPLS-AA (OPLS all atom model) force field and a united atom model force field were compared with the ab initio calculations. Although the two force fields well reproduces the experimental vapor and liquid properties of perfluoroalkenes, the comparison shows that the united atom model underestimates the potential depth and orientation dependence of the interaction energy. The potentials obtained by the OPLS-AA force field are close to those obtained by the ab initio calculations. (C) 2004 American Institute of Physics.
机译:利用二阶Moller-Plesset摄动法,通过电子相关校正,计算了C3F8二聚体12个取向的分子间相互作用能。反平行C-2h二聚体具有最大的相互作用能(-1.45 kcal / mol)。电子相关校正大大增加了吸引力。静电能量不大。分散主要是吸引力的原因。 C3F8二聚体的相互作用能的取向依赖性基本上小于C3H8二聚体的取向能。计算出的C3F8二聚体在最小电势下的相互作用能为C3H8二聚体(-1.85 kcal / mol)的78%,而CF4和C2F6二聚体的相互作用能大于CH4和C2H6二聚体的相互作用能。 C3F8二聚体在最小电位下的分子间间距明显大于C3H8二聚体中的分子间间距。由于氟原子之间的空间排斥而导致的较大的分子间分离是导致C3F8二聚体在电势最小值处较小的相互作用能的原因。将使用全原子模型OPLS-AA(OPLS全原子模型)力场和联合原子模型力场计算出的C3F8二聚体的分子间相互作用能势与从头算计算进行了比较。尽管这两个力场很好地再现了全氟烯烃的实验汽和液性能,但比较表明,联合原子模型低估了相互作用能的潜在深度和取向依赖性。 OPLS-AA力场获得的电势与从头算计算获得的电势接近。 (C)2004年美国物理研究所。

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