The results of this analysis can be extended to all circuits, and the equations analogous to Eq. 5.13 can be obtained:
jZjD0 for the circuit Fig. 5.9a, jHjD0 for the circuit Fig. 5.9,
jGjD0 for the circuit Fig. 5.9d, and jAjD0 for the circuit Fig. 5.9e.