  We propose that a specific spatial configuration of lattice sites that
energetically favor {\it 3+} or {\it 4+} Mn ions in moderately doped manganites
constitutes approximately a spatially random two-energy-level system. Such an
effect results in a mechanism of metal-insulator transitions that appears to be
different from both the Anderson transition and the Mott-Hubbard transition.
Correspondingly, a disordered Kondo lattice model is put forward, whose
dynamical mean-field solution agrees reasonably with experiments.
