Most available intermolecular potentials assume rigid monomers. Such an ass
umption is a reflection of a trivial observation that if monomer degrees of
freedom are considered, the dimensionality of an intermolecular potential
increases dramatically even for few-atom monomers. This puts strict limits
on the sizes of clusters with flexible monomers that can be treated by ab i
nitio methods since the number of grid points needed to Dt a potential surf
ace quickly becomes enormous. Most of the literature flexible-monomer poten
tials were obtained from the so-called site-site rigid-monomer potentials b
y simply allowing the sites to move with atomic nuclei as the monomers are
deformed. This simple atom-following approach has been investigated in the
present work, using water dimer and Ar-HF as test systems, and shown to be
not adequate. A method has been proposed which uses properties of isolated
flexible monomers to improve upon the atom-following approach without perfo
rming any dimer calculations outside the rigid-monomer grid. The method is
shown to give for Ar-HF a 3D representation of the dispersion energy that s
hould be adequate for HF motion in the ground and first excited vibrational
states.