The standard mean field approach neglects the random disordering of ma
gnetic and nonmagnetic ions with the sublattice of the mixed-spinel fe
rrites. It is known that this disordering can lead to real effects. A
mean field theory is developed in which local field fluctuations arisi
ng from the random disordering of the magnetic ions within a sublattic
e acts on the spins located within the other sublattice. It is seen th
at the fluctuations lead to a lowering of the values of the spins at i
ntermediate temperatures.