We propose a classical constrained Hamiltonian theory for the spin. Af
ter the Dirac treatment we show that due to the existence of second-cl
ass constraints the Dirac brackets of the proposed theory represent th
e commutation relations for the spin. We show that the corresponding p
artition function, obtained via the Fadeev-Senjanovic procedure, coinc
ides with that obtained using coherent states. We also evaluate this p
artition function for the case of a single spin in a magnetic field.