Compounds containing well-isolated complex magnetic chains are now available from inorganic and molecular chemistry. Interpreting their magnetic behavior generally requires specific models. We propose here a rather general analytical treatment: This model concerns isotropic ferrimagnetic chains, where a single moment, which may be treated classically (subsystem zeta(i)), alternates with a composite subsystem PSI(i) of quantum and/or classical spins. In order to evaluate the zero-field susceptibility, it appears necessary to build up and diagonalize an appropriate Hamiltonian for each subsystem PSI(i). Moreover, one must calculate the first- and second-order derivatives of the eigenvalue E(i,u)(B) with respect to the amplitude B of the applied field. The intervening quantities depend on the angle THETA(i) between zeta(i) and zeta(i+1) and can be expanded in Legendre polynomials. Because of the properties of these functions, the various expansions only require the computation of the first and/or second coefficients. We give a general closed-form expression for the zero-field susceptibility and analyze its behavior in the low-temperature limit by the mean of the correlation length. We treat three relevant examples and describe possible extensions to random distributed classical or quantum spins in linear chains. We also recall an experimental test of this model concerning the compound MnCu2(bapo)(H2O)4.2H2O [where bapo=N,N'-bis (oxamato 1,3-propylene) oxamido].