We calculate the magnetic susceptibility for the CuO2 plane in high-T-
c superconductors based on a two-phase model. Starting from the three-
band Hubbard model we arrive at an explicit expression for the total m
agnetic susceptibility that can be separated into two distinct parts:
(i) an antiferromagnetically correlated Heisenberg type term and (ii)
a renormalized two-dimensional conductive term. The doping dependences
of the antiferromagnetic (Q = (pi, pi)) and metallic like (q = (0, 0)
) contribution to the static magnetic susceptibility are discussed and
compared with experimental results.