By using the tight-binding Hamiltonian and non-equilibrium Green’s function methods, the Seebeck and Nernst effects of α-T3 lattice nanoribbons are investigated, in which the lattice interpolates between graphene and the dice lattice via the parameter α. It is found that for α=0, i.e. graphene, flat bands are always present in the band structure. The Seebeck and Nernst coefficients are consistent with those in graphene. When α is non-zero at zero magnetic field, the Seebeck coefficient is an odd function of the Fermi energy. It produces a very large and wide first peak within the band gap for the zigzag boundary. Under the influence of magnetic fields, the first peak of the Seebeck coefficient in the bandgap region increases with α increasing. For the Nernst effect, the zeroth peak of the Nernst coefficient becomes very higher as α increases and then splits when α reaches a certain value. The post-split peak decreases with α increasing for the zigzag boundary, but continues to become wider and higher for the armchair boundary.