Dynamical chiral symmetry breaking in the discretized light-cone quantizati
on method is investigated in detail using a chiral Yukawa model closely rel
ated to the Nambu-Jona-Lasinio model. By classically solving three constrai
nts characteristic of the light-front formalism, we show that the chiral tr
ansformation defined on the light front is equivalent to the usual one when
the bare mass is absent. A quantum analysis demonstrates that a nonperturb
ative mean-field solution to the "zero-mode constraint'' for a scalar boson
a can develop a nonzero condensate [sigma] = -(lambda/N)[<(Psi)over bar>Ps
i] not equal 0 while a perturbative solution cannot. This description is du
e to our identification of the "zero-mode constraint" with the gap equation
. The mean-field calculation clarifies unusual chiral transformation proper
ties of the fermionic field, which resolves a seeming inconsistency between
the triviality of the null-plane chiral charge Q(5)(LF)\0] = 0 and the non
zero condensate [<(Psi)over bar>Psi] not equal 0. We also calculate masses
of scalar and pseudoscalar bosons for both symmetric and broken phases, and
eventually derive the relation of partial conservation of axial vector cur
rent and nonconservation of Q(5)(LF) in the broken phase.