Molecular mechanics simulations within the field of the mean (when disorder
is present) crystal lattice have been used to settle most of the ambiguiti
es inherent to the interpretation of the diffraction experiments on (E)-sti
lbenes. A dynamic process can be inferred by diffraction methods only if it
leaves a track in the atomic displacement parameters or gives rise to some
disorder or to some anomaly in the bonding parameters. However, since diff
raction experiments map (according to Boltzmann's statistics) only the bott
om of the local minima of the potential energy surface, many possible sourc
es of misunderstanding are present. Indeed, the coupling of molecular mecha
nics to Kitaigorodsky's atom-atom pairwise potential approach, offering a d
etailed description of the solid-state trajectories (and of the involved en
ergy changes) of(E)-stilbenes, has allowed a rationalization of the observe
d dynamic molecular disorder, which differently affects different crystal s
ites, and has led to a quantitative description of the anomalous temperatur
e dependence of the ethylene bonding parameters in these compounds.