We embed two 4D chiral multiplets of opposite representations in the 5D N = 2 SU(N+K) gauge theory compactified on an orbifold S¹/(Z₂ × Z′₂). There are two types of orbifold boundary conditions in the extra dimension to obtain the 4D N = 1 SU(N) × SU(K) × U(1) gauge theory from the bulk: in type-I, one has the bulk gauge group at y = 0 and the unbroken gauge group at y = πR/2 while in type-II, one has the unbroken gauge group at both fixed points. In both types of orbifold boundary conditions, we consider the zero mode(s) as coming from a bulk (K+N)-plet and brane fields at the fixed point(s) with the unbroken gauge group. We check the consistency of this embedding of fields by the localized anomalies and the localized FI terms. We show that the localized anomalies in type-I are cancelled exactly by the introduction of a bulk Chern-Simons term. On the other hand, in some class of type-II, the Chern-Simons term is not enough to cancel all localized anomalies even if they are globally vanishing. We also find that for the consistent embedding of brane fields, there appear only the localized log FI terms at the fixed point(s) with a U(1) factor.