We discuss two-dimensional Yang-Mills theories with massless fermions
in arbitrary representations of a gauge group G, It is shown that the
physics (spectrum and interactions) of the massive states in such mode
ls is independent of the detailed structure of the model, and only dep
ends on the gauge group G and an integer k measuring the total anomaly
. The massless physics, which does depend on the details of the model,
decouples (almost) completely from that of the massive one. As an exa
mple, we discuss the equivalence of QCD(2) coupled to fermions in the
adjoint, and fundamental representations.