We reconsider the problem of quantising a particle on the D-dimensional sph
ere. Adopting a Lagrangian method of reducing the degrees of freedom, the q
uantum Hamiltonian is found to be the usual Schrodinger operator without an
y curvature term. The equivalence with the Dirac Hamiltonian approach is de
monstrated, either in the cartesian or in the curvilinear basis. We also br
iefly comment on the path integral approach.