Find the z parameters for the circuit in Fig. 19.52 at ω = 10^{6} rad/s.
Notice that we used dc analysis in Example 19.15 because the circuit in Fig. 19.49 is purely resistive. Here, we use ac analysis at f = ω/2π = 0.15915 MHz, because L and C are frequency dependent. In Eq. (19.3), we defined the z parameters as
\begin{matrix}z_{11} = \frac{V_{1}}{I_{1}} \mid_{I_{2} = 0} , z_{12} = \frac{V_{1}}{I_{2}} \mid_{I_{1} = 0} \\\\ z_{21} = \frac{V_{2}}{I_{1}} \mid_{I_{2} = 0} , z_{22} = \frac{V_{2}}{I_{2}} \mid_{I_{1} = 0}\end{matrix}\quad (19.3) \\
z_{11} = \frac{V_1}{I_1}|_{I_2=0} ,\quad z_{21} = \frac{V_2}{I_1}|_{I_2=0}
This suggests that if we let I_{1} = 1 A and open-circuit the output port so that I_{2} = 0 , then we obtain
z_{11} = \frac{V_{1}}{1} and z_{21} = \frac{V_{2}}{1}
We realize this with the schematic in Fig. 19.53(a). We insert a 1-A ac current source IAC at the input terminal of the circuit and two VPRINT1 pseudocomponents to obtain V_{1} and V_{2} The attributes of each VPRINT1 are set as AC = yes, MAG = yes and PHASE = yes to print the magnitude and phase values of the voltages. We select Analysis/Setup/AC Sweep and enter 1 as Total Pts, 0.1519MEG as Start Freq, and 0.1519MEG as Final Freq in the AC Sweep and Noise Analysis dialog box. After saving the schematic, we select Analysis/Simulate to simulate it. We obtain V_{1} and V_{2} from the output file. Thus,
z_{11} = \frac{V_{1}}{1} = 19.70 \underline{/175.7°} Ω , z_{21} = \frac{V_{2}}{1} = 19.79 \underline{/170.2° } Ω
In a similar manner, from Eq. (19.3),
z_{12} = \frac{V_{1}}{I_{2}} \mid_{I_{1} = 0} , z_{22} = \frac{V_{2}}{I_{2}} \mid_{I_{1} = 0}
suggesting that if we let I_{2} = 1 A and open-circuit the input port,
z_{12} = \frac{V_{1}}{1} and z_{22} = \frac{V_{2}}{1}
This leads to the schematic in Fig. 19.53(b). The only difference between this schematic and the one in Fig. 19.53(a) is that the 1-A ac current source IAC is now at the output terminal. We run the schematic in Fig. 19.53(b) and obtain V_{1} and V_{2} from the output file. Thus,
z_{12} = \frac{V_{1}}{1} = 19.70 \underline{/175.7°} Ω , z_{22} = \frac{V_{2}}{1} = 19.56 \underline{/175.7° } Ω