A general noncommutative quantum mechanical system in a central potential V
= V(r) in two dimensions is considered. The spectrum is bounded from below
and, for large values of the anticommutative parameter theta, we find an ex
plicit expression for the eigenvalues. In fact, any quantum mechanical syst
em with these characteristics is equivalent to a commutative one in such a
way that the interaction V(r) is replaced by V = V((H) over cap (HO), (L) o
ver cap (z)), where (H) over cap (HO) is the Hamiltonian of the two-dimensi
onal harmonic oscillator and (L) over cap (z) is the z component of the ang
ular momentum. For other finite values of theta the model can be solved by
using perturbation theory.