We prove the perturbative renormalizability of Euclidean QED(4) using
flow equations, i.e. with the aid of the Wilson renormalization group
adapted to perturbation theory. As compared to Phi(4)(4) the additiona
l difficulty to overcome is that the regularization violates gauge inv
ariance. We prove that there exists a class of renormalization conditi
ons such that the renormalized Green functions satisfy the QED Ward id
entities and such that they are infrared finite at nonexceptional mome
nta. We give bounds on the singular behaviour at exceptional momenta (
due to the massless photon) and comment on the adaptation to the case
when the fermions are also massless.