We report on a study of a classical, finite system of confined particl
es in two dimensions with a two-body repulsive interaction. We first d
evelop a simple analytical method for obtaining equilibrium configurat
ions and energies for a few particles. When the confinement is harmoni
c, we prove that the first transition from a single shell occurs when
the number of particles changes from five to six. The shell structure
in the case of an arbitrary number of particles is shown to be indepen
dent of the strength of the interaction and dependent only on its func
tional form. It is also found to be independent of the magnetic field
strength when this is included. We further study the effect of the fun
ctional form of the confinement potential on the shell structure. Fina
lly, we report some interesting results obtained when a three-body int
eraction is included, albeit in a particular model.