  We study the phase structure of full QCD within the canonical ensemble with
respect to triality in a lattice formulation. The procedure for the calculation
of the effective potentials in this case is given. As an example we consider
the three dimensional SU(2) gauge model at finite temperatures in the strong
coupling region. The potential exhibits a deconfinement phase transition unlike
the similar potential obtained in the grand canonical ensemble which
demonstrates explicit Z(N) symmetry breaking at any temperature. Furthermore,
we investigate the effective potential with the chiral condensate included. In
contradiction to other authors, we find chiral symmetry restoration in all
triality sectors. In the scheme with massless staggered fermions we observe
chiral symmetry restoration accompanying a deconfinement phase transition of
first order. Above the critical point, besides two Z(2) symmetric "deconfining"
vacua there exists a metastable "confining" vacuum in a wide region of
parameters. Such a picture could be interpreted as an indication on a mixed
state of hadrons and quarks in the vicinity of the critical line.
