Determine the y parameters for the two-port shown in Fig. 19.17 .
We follow the same procedure as in the previous example. To get y_{11} and y_{21} , we use the circuit in Fig. 19.18(a), in which port 2 is short-circuited and a current source is applied to port 1. At node 1,
\frac{V_{1} – V_{o}}{8} = 2 I_{1} + \frac{V_{o}}{2} + \frac{V_{o} – 0}{4}
But I_{1} = \frac{V_{1} – V_{o}}{8} ; therefore ,
0 = \frac{V_{1} – V_{o}}{8} + \frac{3V_{o}}{4}
0 = V_{1} – V_{o} + 6V_{o} ⇒ V_{1} = – 5V_{o}
Hence,
I_{1} = \frac{ -5V_{o} – V_{o}}{8} = – 0.75V_{o}
and
y_{11} = \frac{I_{1}}{V_{1}} = \frac{-0.75 V_{o}}{-5 V_{o}} = 0.15 S
At node 2,
\frac{V_{o} – 0 }{4} + 2I_{1} + I_{2} = 0
or
-I_{2} = 0.25V_{o} – 1.5V_{o} = – 1.25V_{o}
Hence,
y_{21} = \frac{I_{2}}{V_{1}} = \frac{ 1.25V_{o}}{- 5V_{o}}= – 0.25 S
Similarly, we get y_{12} and y_{22} using Fig. 19.18(b). At node 1,
\frac{0 – V_{o}}{8} = 2I_{1} + \frac{V_{o}}{2} + \frac{V_{o} – V_{2}}{4}
But I_{1} = \frac{0 – V_{o}}{8} ; therefore,
0 = – \frac{V_{o}}{8} + \frac{V_{o}}{2} + \frac{V_{o} – V_{2}}{4}
or
0 = – V_{o} + 4V_{o} + 2V_{o} – 2V_{2} ⇒ V_{2} = 2.5V_{o}
Hence,
y_{12} = \frac{I_{1}}{V_{2}} = \frac{- V_{o}/8}{2.5V_{o}}= – 0.05 S
At node 2,
\frac{V_{o} – V_{2}}{4} + 2I_{1} + I_{2} = 0
or
-I_{2} = 0.25V_{o} – \frac{1}{4} (2.5V_{o}) – \frac{2V_{o}}{8} = – 0.625V_{o}
Thus,
y_{22} = \frac{I_{2}}{V_{2}} = \frac{ 0.625V_{o}}{2.5V_{o}} = 0.25 S
Notice that y_{12} ≠ y_{21} in this case, since the network is not reciprocal.