  We discuss a generalization of the conventional bosonization procedure to the
case of current-current interactions which get their natural representation in
terms of current instead of fermion number density operators. A consistent
bosonization procedure requires a geometrical quantization of the hamiltonian
action of $W_\infty$ on its coadjoint orbits. An integrable example of a
nontrivial realization of this symmetry is presented by the Calogero-Sutherland
model. For an illustrative nonintegrable example we consider transverse gauge
interactions and calculate the fermion Green function.
