Cx. Liang et al., FORCE-FIELD STUDIES OF CHOLESTEROL AND CHOLESTERYL ACETATE CRYSTALS AND CHOLESTEROL CHOLESTEROL INTERMOLECULAR INTERACTIONS, Journal of computational chemistry, 16(7), 1995, pp. 883-897
To model the physical properties of sterols and related species, an al
l-atom Class II force field has been derived based on the recently rep
orted CFF93 force field for hydrocarbons. It has been tested using bot
h energy minimization and molecular dynamics (MD) simulations of the l
ow-temperature neutron-diffraction structure of cholesteryl acetate cr
ystals and the X-ray diffraction crystal structure of cholesterol. Thu
s these studies test the techniques and limitations of high-accuracy c
rystal simulations as well. Employing energy minimization, all cell ve
ctors and volumes were reproduced to within 2.4% of experimental value
s. For cholesteryl acetate, the root mean square (rms) deviations betw
een the calculated and experimental bond lengths, angles, and torsions
of nonhydrogen atoms are 0.013 Angstrom, 1.2 degrees, and 2.4 degrees
, respectively. The corresponding maximum deviations are also very sma
ll: 0.027 Angstrom for bond length, 3.2 degrees for angle, and 7.6 deg
rees for torsion. For cholesterol, good agreement between the calculat
ed and experimental structures was found only when the parison was lim
ited to atoms with relatively small thermal factors (B-eq < 15 Angstro
m(2)). It was found that for both systems, the MD averaged structures
were in better agreement with the experimental ones than the energy mi
nimized structures, since the rms deviations in atom positions are sma
ller for the MD-averaged structures (0.064 Angstrom for cholesteryl ac
etate and 0.152 Angstrom for cholesterol) than those for the minimized
structures (0.178 Angstrom for cholesteryl acetate and 0.189 Angstrom
for cholesterol). The force field was then applied to isolated molecu
les focusing on the rigidity of the cholesteryl ring and cholesterol-c
holesterol interaction energies, It is concluded that the cholesteryl
ring is fairly rigid since no major conformational change was observed
during an MD simulation of a single cholesterol molecule in vacuo at
500 K, in agreement with condensed phase experiments. Calculations of
cholesterol-cholesterol pairs suggest that there are only four low-ene
rgy configurations and that it is more useful to describe each molecul
e as having a plane (flat face) and two grooves rather than as having
two (one flat and one rough) faces. This provides some insight into th
e equilibrium crystal structures. Limited results from a modified Clas
s I (CVFF) force field are presented for comparison. (C) 1995 by John
Wiley and Sons, Inc.