The in-plane resistivity rho(a)(T) and the out-of-plane resistivity rho(c)(T) have been systematically measured for Bi2Sr2CaCu2O8+delta Single crystals with their oxygen contents precisely controlled. In the underdoped region, deviation from T-linear in-plane resistivity, which evidences the opening of the ''spin gap,'' is clearly observed, while the out-of-plane resistivity is well reproduced by the activation-type phenomenological formula rho(c)(T)=(a/T)exp(Delta/T) + c. In contrast to the YBa2Cu3O7-delta system, we find that the onset of the semiconducting rho(c)(T) does not coincide with the opening of the spin gap seen in the rho(c)(T) in this Bi2Sr2CaCu2O8+delta system.