We analyze a formulation of QED based on the Wilson renormalization gr
oup. Although the ''effective lagrangian'' used at any given scale doe
s not have simple gauge symmetry, we show that the resulting renormali
zed Green's function correctly satisfies Ward identities to all orders
in perturbation theory. The loop expansion is obtained by solving ite
ratively the Polchinski renormalization group equation. We also give a
new simple proof of perturbative renormalizability. The subtractions
in the Feynman graphs and the corresponding counter-terms are generate
d in the process of fixing the physical conditions.