In this paper, we establish the global existence of a suitable weak solution to the co-rotational Beris-Edwards Q-tensor system modeling the hydrodynamic motion of nematic liquid crystals with either Landau-De Gennes bulk potential in R-3 or Ball-Majumdar bulk potential in T-3, a system coupling the forced incompressible Navier-Stokes equation with a dissipative, parabolic system of Q-tensor Q in R-3, which is shown to be smooth away from a closed set Sigma whose 1-dimensional parabolic Hausdorff measure is zero.