Interplay of Pomeranchuk instability (spontaneous symmetry breaking of the Fermi surface) and dwave superconductivity is studied for the repulsive Hubbard model on the square lattice with the dynamical mean field theory combined with the fluctuation exchange approximation (FLEX+DMFT). We show that the four-fold symmetric Fermi surface becomes unstable against a spontaneous distortion into two-fold near the van Hove filling, where the symmetry of superconductivity coexisting with the Pomeranchuk-distorted Fermi surface is modified from the d-wave pairing to (d + s)-wave. By systematically shifting the position of van Hove filling with varied second-and third-neighbor hoppings, we find that the transition temperature T PI c for the Pomeranchuk instability is more sensitively affected by the position of van Hove filling than the superconducting T SC c . This implies that the filling region for strong Pomeranchuk instability and that for the T SC c dome can be separated, and that Pomeranchuk instability can appear even if the peak of T PI c is lower than the peak of T SC c . An interesting finding is that the Fermi surface distortion can enhance the superconducting T SC c in the overdoped regime, which is explained with a perturbational picture for small distortions.