A careful analysis of the three-dimensional structures of liquid iodin
e obtained with the reverse Monte Carlo (RMC) and molecular dynamics (
MD) techniques is presented. The analysis allows one to measure the de
gree of nonuniqueness between the potential and the radial distributio
n functions g(r), in the case of pairwise but not purely site-site int
eractions. The g(r) obtained from MD simulations are used as 'experime
ntal' input data in the RMC procedure and the constraint of rigid mole
cules is imposed. The particle configurations produced by RMC are then
studied by using a recently proposed general method for analysing the
local order in liquids. The same analysis applied to the particle con
figurations produced by the conventional MD simulation yields a set of
partial distribution functions which relates the main features of the
g(r) to microscopic pair geometries. A comparison of the partial g(r)
shows that the three-dimensional structures produced by the MD and RM
C simulations differ significantly. In other words, even if the potent
ial is purely pairwise additive, the use of the atomic radial distribu
tion function as input data and the imposition of atomic constraints w
hich model the molecules as hard dumbbells is not sufficient to bring
the RMC procedure towards the 'true' microscopic structure of the liqu
id. The discrepancies are particularly evident for the elongated confi
gurations, such as the T, L and end-to-end. The use of the centres of
mass distribution functions as additional input data does not yield si
gnificant improvements in the microscopic local order predicted by the
RMC simulation.