We study the Schwinger-Dyson equation for the fermion self-energy in m
assless and massive QED2, in the ladder approximation. When the fermio
n is massless (and the photon massless or massive), we check the relia
bility of this approximation by comparing its solutions with the exact
ones. They agree only when the photon is massless. For a massive ferm
ion and massless photon, we show that there is no consistent solution
at all, the infrared divergences introduced by the approximation forbi
dding even the trivial solution. When both fermion and photon are mass
ive, we find a non-perturbative (extra) fermion mass generation (which
survives in the limit when the bare mass of the fermion tends to zero
). We argue that, in this case, the ladder approximation will provide
reliable results if the bare masses of the fields are large compared w
ith the (dimensionful) coupling constant.