Question 10.8: a) For the circuit shown in Fig. 10.20, determine the impeda...

a) For the circuit shown in Fig. 10.20, determine the impedance Z_{L} that results in maximum average power transferred to Z_{L}.
b) What is the maximum average power transferred to the load impedance determined in (a)?

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a) We begin by determining the Thévenin equivalent with respect to the load terminals a, b. After two source transformations involving the 20 V source, the 5Ω resistor, and the 20Ω resistor, we simplify the circuit shown in Fig. 10.20 to the one shown in Fig. 10.21. Then,

\pmb{V}_{Th}=\frac{16 \angle 0°}{4 + j3 – j6}\left(-j6\right)

= 19.2 \angle -53.13° = 11.52 – j15.36 V.

We find the Thévenin impedance by deactivating the independent source and calculating the impedance seen looking into the terminals a and b. Thus,

\pmb{Z}_{Th}=\frac{\left(-j6\right) \left(4 + j3\right) }{4 + j3 – j6}= 5.76 – j1.68 \Omega.

For maximum average power transfer, the load impedance must be the conjugate of \pmb{Z}_{Th}, so

Z_{L} = 5.76 + j1.68 \Omega.

b) We calculate the maximum average power delivered to Z_{L} from the circuit shown in Fig. 10.22, in which we replaced the original network with its Thévenin equivalent. From Fig. 10.22, the rms magnitude of the load current I is

\pmb{I}_{eff}=\frac{\frac{19.2}{\sqrt{2}}}{2\left(5.76\right)}=1.1785 A .

The average power delivered to the load is

P = I^{2}_{eff}(5.76) = 8 W.

10.21
10.22

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