  Transport theory for an interacting fermionic system is reviewed and applied
to the chiral Lagrangian of the Nambu-Jona-Lasinio model. Two expansions must
be applied: an expansion in the inverse number of colors, $1/N_c$, due to the
nature of the strong coupling theory, and a semiclassical expansion, in powers
of $\hbar$. The quasiparticle approximation is implemented at an early stage,
and spin effects are omitted. The self-energy is evaluated, self-consistently
only in the Hartree approximation, and semi-perturbatively in the collision
integral. In the Hartree approximation, $O((1/N_c)^0)$, the Vlasov equation is
recovered to $O(\hbar^1)$, together with an on-mass shell constraint equation,
that is automatically fulfilled by the quasiparticle ansatz. The expressions
for the self-energy to order $O((1/N_c))$ lead to the collision term. Here one
sees explicitly that particle-antiparticle creation and annihilation processes
are suppressed that would otherwise be present, should an off-shell energy
spectral function be admitted. A clear identification of the $s$, $t$ and $u$
channel scattering processes in connection with the self-energy graphs is made
and the origin of the mixed terms is made evident. Finally, after ordering
according to powers in $\hbar$, a Boltzmann-like form for the collision
integral is obtained.
