We consider the so-called G-equation, a level set Hamilton-Jacobi equation, used as a sharp interface model for flame propagation, perturbed by an oscillatory advection in a spatio-temporal periodic environment. Assuming that the advection has suitably small spatial divergence, we prove that, as the size of the oscillations diminishes, the solutions homogenize (average out) and converge to the solution of an effective anisotropic first-order (spatio-temporal homogeneous) level set equation. Moreover we obtain a rate of convergence and show that, under certain conditions, the averaging enhances the velocity of the underlying front. We also prove that, at scale one, the level sets of the solutions of the oscillatory problem converge, at long times, to the Wulff shape associated with the effective Hamiltonian. Finally we also consider advection depending on position at the integral scale.which, in turn, implies that, for all t ≥ 0,Recalling thatH(ν) ≥ |ν| = 1, we find, for all (and, therefore, for all t ≥ 0,Letting λ → 0, we get, for all t ≥ 0 and a new positive constant C,Taking the intersection of the right-hand side over all ν we obtain, by the definition of W, that, for all t ≥ 0, K(t) ⊂ (t + C)W .