The isoscalar monopole(ISM) and dipole(ISD) excitations in 12 C are theoretically investigated with the shifted antisymmetrized molecular dynamics(AMD) plus 3α-cluster generator coordinate method(GCM). The small amplitude vibration modes are described by coherent one-particle onehole excitations expressed by small shift of single-nucleon Gaussian wave functions within the AMD framework, whereas the large amplitude cluster modes are incorporated by superposing 3α-cluster wave functions in the GCM. The coupling of the excitations in the intrinsic frame with the rotation and parity transformation is taken into account microscopically by the angular-momentum and parity projections. The present calculation describes the ISM and ISD excitations in a wide energy region covering cluster modes in the low-energy region and the giant resonances in the high-energy region, though the quantitative description of the high-energy part is not satisfactory. The lowenergy ISM and ISD strengths of the cluster modes are enhanced by the radial motion of α clusters, and they split into a couple of states because of the angular motion of α clusters. The low-energy ISM strengths exhaust 26% of the EWSR, which is consistent with the experimental data for the 12 C(0 + 2 ;7.65 MeV) and 12 C(0 + 3 ;10.3 MeV) measured by (e, e ′ ), (α, α ′ ), and ( 6 Li, 6 Li ′ ) scatterings. In the calculated low-energy ISD strengths, two 1 − states (the 1 − 1 and 1 − 2 ) with the significant strengths are obtained in E = 10 − 15 MeV. It is indicated that the ISD excitations can be a good probe to experimentally search for new cluster states such as the 12 C(1 − 2 ) obtained in the present calculation.