In Figure 19-33, determine I_{n} for the circuit as “seen” by the load resistor. The beige area identifies the portion of the circuit to be nortonized.
In Figure 19-33, determine I_{n} for the circuit as “seen” by the load resistor. The beige area identifies the portion of the circuit to be nortonized.
Short the terminals A and B, as shown in Figure 19-34,
I_{n} is the current through the short and is calculated as follows. First, the total impedance viewed from the source is
Z= X_{C1}+ \frac{RX_{C2}}{R+ X_{C2}}= 50 \angle -90°\Omega + \frac{(56\angle 0°\Omega )(100\angle -90°\Omega )}{56 \ \Omega – j100 \ \Omega }\ \ \ =50 \angle -90°\Omega + 48.9 \angle -29.3°\Omega
\ \ \ =-j50 \ \Omega + 42.6 \ \Omega – j23.9 \ \Omega = 42.6 \ \Omega – j73.9 \ \Omega
Converting to polar form yields
Z=85.3 \angle -60.0°\OmegaNext, the total current from the source is
I_{s}= \frac{V_{s}}{Z}= \frac{6\angle 0° V}{85.3\angle -60.0° \Omega} = 70.3\angle 60.0°mAFinally, apply the current-divider formula to get I_{n} (the current through the short between terminals A and B).
I_{n}= \left( \frac{R}{R+ X_{C2}}\right) I_{s}= \left( \frac{56\angle 0°\Omega }{56 \ \Omega – j100 \ \Omega }\right)70.3\angle 60.0°mA =34.4\angle 121°mAThis is the value for the equivalent Norton current source.