Monte Carlo simulation of branched alkanes and long chain N-alkanes with anisotropic united atoms intermolecular potential

被引:77
作者
Bourasseau, E
Ungerer, P
Boutin, A
Fuchs, AH
机构
[1] Univ Paris 11, CNRS, UMR 8000, Chim Phys Lab, F-91405 Orsay, France
[2] Inst Francais Petr, F-92852 Rueil Malmaison, France
关键词
Gibbs ensemble Monte Carlo simulations; anisotropic united atoms potential; long linear alkanes; branched alkanes;
D O I
10.1080/08927020290018723
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The anisotropic united atoms potential for linear alkanes proposed by Ungerer (J Chem. Phys., 112, 5499, 2000), called AUA4, has been used to predict several equilibrium properties (vapour pressure, vaporisation enthalpies, and liquid densities) of alkanes by Gibbs ensemble Monte Carlo simulation. In order to extend the potential to branched alkanes, potential parameters for the CH group have been determined by optimisation on the basis of equilibrium properties of isobutane, keeping the same parameters as AUA4 for the CH3 groups. The resulting CH parameters form a regular sequence with those previously determined for CH3 and CH2 groups, so that a physically consistent parameter set is obtained. Simulations have been performed at temperatures ranging from 450 to 800 K for long n-alkanes (C20, C25 and C30) and from 350 to 450 K for four heptane isomers (n-heptane, 2-methylhexane, 2,4-dimethylpentane and 2-ethylpentane). In order to achieve internal relaxation of long chains with a good efficiency, a specific Monte Carlo move was used in which a united atom is rotated around its nearest neighbours. Equilibrium properties of long chain alkanes are well predicted, and small differences between heptane isomers are represented with a good accuracy. It is concluded that the AUA4 potential shows an interesting degree of transferability.
引用
收藏
页码:317 / 336
页数:20
相关论文
共 28 条
[1]  
Allen M. P., 1987, Computer Simulation of Liquids
[2]  
DELHOMMELLE J, 2000, TEHSIS U PARIS SUB O
[3]   SIMULATION OF POLYETHYLENE ABOVE AND BELOW THE MELTING-POINT [J].
DEPABLO, JJ ;
LASO, M ;
SUTER, UW .
JOURNAL OF CHEMICAL PHYSICS, 1992, 96 (03) :2395-2403
[4]   A CONCERTED ROTATION ALGORITHM FOR ATOMISTIC MONTE-CARLO SIMULATION OF POLYMER MELTS AND GLASSES [J].
DODD, LR ;
BOONE, TD ;
THEODOROU, DN .
MOLECULAR PHYSICS, 1993, 78 (04) :961-996
[5]   Fluid transport properties by equilibrium molecular dynamics. I. Methodology at extreme fluid states [J].
Dysthe, DK ;
Fuchs, AH ;
Rousseau, B .
JOURNAL OF CHEMICAL PHYSICS, 1999, 110 (08) :4047-4059
[6]   A new intermolecular potential model for the n-alkane homologous series [J].
Errington, JR ;
Panagiotopoulos, AZ .
JOURNAL OF PHYSICAL CHEMISTRY B, 1999, 103 (30) :6314-6322
[7]  
FRANCIS, 1926, J CHEM SOC, V129, P1420
[8]  
GMEHLING J, 1985, CODATA BULL, V58, P56
[9]   OPTIMIZED INTERMOLECULAR POTENTIAL FUNCTIONS FOR LIQUID HYDROCARBONS [J].
JORGENSEN, WL ;
MADURA, JD ;
SWENSON, CJ .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1984, 106 (22) :6638-6646
[10]   DIRECT EVALUATION OF PHASE COEXISTENCE BY MOLECULAR SIMULATION VIA INTEGRATION ALONG THE SATURATION LINE [J].
KOFKE, DA .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (05) :4149-4162