Magnetic hysteresis and flux creep characteristics in melt-powder-melt-growth YBa2Cu3O7 with Y2BaCuO5 inclusions were measured between 5 and 80 K for magnetic fields up to 5 T. The critical magnetization current densities which were calculated using the Bean model and the sample dimension show a weak dependence on magnetic field. The J(c) values are of the order of 10(4) A/cm2 at 60 K over the investigated field range. The magnetic relaxation rate Q=-dM/d 1nt first drops monotonically with increasing temperatures and then gradually saturates, which is similar to the behavior of the initial magnetization M0 versus temperature. The normalized relaxation rate S = d 1nM/d 1nt, plotted as a function of temperature, shows a maximum at around 30 K, and the corresponding values of S and T at the maximum are field dependent. A scaling relationship U(eff)(J,H)=U(i)G(T)F(J/J(i))/H0.55, where G(T)=1-(T/T(x))2,F(J/J(i))-(J/J(i))-n, and U(i) and J(i) are scaling constants, is proposed to fit the creep data from which a universal curve is attained. The characteristic temperature T(x) for the scaling function G(T) is determined from the irreversibility line. The current-dependent behavior of U(eff) obtained from this work agrees qualitatively with the result predicted by the theory of collective flux creep and suggests a vortex-glass state at low current density.