Hiickel model with one-s-electron per atom is used to study the geometries and electroniC structures of clusters of 9 to 22 atoms. '!\vo different optimization schemes for obtaining the ground states are used; (i) minimization of., an approximate Hiickel ground state energy starting from a random geometry and (ii) simulated annealing. Both methods give similar and new ground state geometries for clusters with 10 to. 14 atoms. All clusters with more than 10 atoms will be distorted if the bond distance is allowed to vary ±5.5%. The ground states of clusters with atoms 10, 11, 12, and 14 are found to have the N = 9 cluster as the basic building block, whereas the, N = 13 c1usteris a distorted cuboctahedron. As a general trend, the deformation of clusters i~creases from atom number B to 14 and shrinks again from 15 to'20 atoms, in accordance with jeIiium m<;>del results. .These constraints make the Hiickel model difficult. The simpiest model is to require that all nearest neighbor 'distances :are the same (rmin=rmax). This is a hard sphere model, where only the touching spheres are nearest neighbors. This model