In this study, the mean-field Ising model, using the Bogolyubov inequa
lity which has been obtained in the framework of the generalized stati
stical thermodynamics (GST), suitable for non-extensive systems, has b
een investigated. Generalized expressions for the mean-field magnetiza
tion and free energy have been established. These new results have bee
n verified by the fact that they transform to the well-known Boltzmann
-Gibbs results in the q-->1 limiting case. For the index q which chara
cterizes the fractal structure of the magnetic system, an interval has
been established where the generalized mean-field free energy has a m
inimum and mean-field magnetization has a corresponding finite value.
The interval of q is consistent with paramagnetic free spin systems.