Considering the disorder caused in manganites by the substitution Mn→Fe or Ga, we accomplish a systematic study of doped manganites begun in previous papers. To this end, a disordered model is formulated and solved using the variational mean-field technique. The subtle interplay between double exchange, superexchange, and disorder causes similar effects on the dependence of T C on the percentage of Mn substitution in the cases considered. Yet, in La 2/3 Ca 1/3 Mn 1Ϫy Ga y O 3 our results suggest a quantum critical point ͑QCP͒ for y Ϸ0.1-0.2, associated to the localization of the electronic states of the conduction band. In the case of La x Ca x Mn 1Ϫy Fe y O 3 ͑with xϭ1/3,3/8) no such QCP is expected.