This paper describes a novel method for predicting the crystal structu
re of organic molecular materials which employs a series of successive
approximations to focus on structures of high probability, without re
sorting to a brute force search and energy minimization of all possibl
e structures. The problem of multiple local minima is overcome by assu
ming that the crystal structure is closely packed, thereby eliminating
217 of the 230 possible space groups. Configurations within the 13 re
maining space groups are searched by rotating the reference molecule a
bout Cartesian axes in rotational increments of 15 degrees. Initial en
ergy minimization is performed using (6-12) Lennard-Jones pair potenti
als to produce a set of closely packed structures. The structures are
then refined with the introduction of a Coulombic potential calculated
using molecular multipole moments. This method has successfully locat
ed local minima which correspond to the observed crystal structures of
several saturated and unsaturated hydrocarbons with no a priori infor
mation provided. For large polycyclic aromatic hydrocarbons, additiona
l refinements of the energy calculations are required to distinguish t
he experimental structure from a small number of closely packed struct
ures. Our methodology for a priori crystal structure prediction repres
ents the most efficient algorithm presented to date, in a field where
the first successes have only been described within the past year and
have been few and far between. Since our algorithm is capable of locat
ing a large number of reasonable structures with similar energy in a s
hort period of time, and is more likely to locate a minimum correspond
ing to the experimental structure, our program provides a superior fra
mework to determine the level of theory required to calculate the inte
rmolecular potential. For all but highly asymmetric hydrocarbons, howe
ver, distinguishing the observed structure from a large number of high
ly probable structures requires more rigorously calculated intermolecu
lar interactions than pair potentials, plus an ad hoc electrostatic po
tential, and is thus beyond the scope of this paper. All calculations
were performed on the Ohio Supercomputer Center's Gray Y-MP.