Sh. Lee et al., MOLECULAR-DYNAMICS SIMULATION OF LIQUID ALKANES .1. THERMODYNAMICS AND STRUCTURES OF NORMAL-ALKANES - N-BUTANE TO N-HEPTADECANE, Bulletin of the Korean Chemical Society, 17(8), 1996, pp. 735-744
We present results of molecular dynamic (MD) simulations for the therm
odynamic and structural properties of liquid n-alkanes, from n-butane
to n-heptadecane, using three different models I-III. Two of the three
classes of models are collapsed atomic models while the third class i
s an atomistically detailed model. Model I is the original Ryckaert an
d Bellemans' collapsed atomic model [Discuss. Faraday Soc. 1978, 66, 9
5] and model II is the expanded collapsed model which includes C-C bon
d stretching and C-C-C bond angle bending potentials in addition to Le
nnard=Jones and torsional potentials of model I. In model III all the
carbon and hydrogen atoms in the monomeric units are represented expli
citly for the alkane molecules. Excellent agreement of the results of
our MD simulations of model I for n-butane with those of Edberg et al.
[J. Chem. Phys. 1986, 84, 6933], who used a different algorithm confi
rms the validity of our algorithms for MD simulations of model II for
14 liquid n-alkanes and of models I and III for liquid n-butane, n-dec
ane, and n-heptadecane. The thermodynamic and structural properties of
models I and II are very similar to each other and the thermodynamic
properties of model III for the three n-alkanes are not much different
from those of models I and II. However, the structural properties of
model III are very different-from those of models I and II as observed
by comparing the radial distribution functions, the average end-to-en
d distances and the root-mean-squared radii of gyrations.