  We apply the finite-element lattice equations of motion for quantum
electrodynamics given in the first paper in this series to examine anomalies in
the current operators. By taking explicit lattice divergences of the vector and
axial-vector currents we compute the vector and axial-vector anomalies in two
and four dimensions. We examine anomalous commutators of the currents to
compute divergent and finite Schwinger terms. And, using free lattice
propagators, we compute the vacuum polarization in two dimensions and hence the
anomaly in the Schwinger model. A discussion of our choice of gauge-invariant
current is provided.
