We study the finite quark mass effects of the low-energy QCD using the impr
oved ladder Schwinger-Dyson and Bethe-Salpeter equations which are derived
in the manner consistent with the vector and axial-vector Ward-Takahashi id
entities. The nonperturbative mass-independent renormalization allows us to
calculate the quark condensate for a nonzero quark mass. We explicitly sho
w that the partial conservation of axial-vector current relation holds. The
key ingredients are the Cornwall-Jackiw-Tomboulis effective action, the ge
neralized Noether current, and the introduction of the regularization funct
ion to the Lagrangian. Reasonable values of the pion mass, the pion decay c
onstant, and the quark condensate are obtained with a rather large Lambda(Q
CD). The pion mass square and the pion decay constant are almost proportion
al to the current quark mass up to the strange quark mass region. It sugges
ts that the chiral perturbation is applicable up to the strange quark mass
region. We study the validity of the approximation often used in solving th
e Bethe-Salpeter equations too. [S0556-2813(99)03703-6].