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Alternating Current Analysis 253


R.3.61 The example shown in Figure 3.25 uses the Thevenin’s theorem to calculate the cur-
rent IL, assuming that the load is ZL = 4 – j4 Ω.

ANALYTICAL Solution

Source transformation as presented in Chapter 2 can be extended to AC circuits as
indicated as follows:
Note that the current source I, in parallel with the impedance Z 2 , can be trans-
formed into a voltage source in series with Z 2 as shown as follows (see R.3.62):
Therefore,

E 3 = I * Z 2 = (6 + j3)(8 − j4) = 60 V


The circuit of Figure 3.25 is transformed into the circuit shown in Figure 3.26, where
the load ZL is removed, following Thevenin’s theorem. Then,

I 1 40 60
16

100
16

25
4

   AA 625.

Therefore, VTH = (8 − j4)6.25 + j30 − 60 = − 10 + j5 V

E 1 = 40 V

I = 6 + j3 A

Z 1 = 8 + j 4

Z 2 = 8 − j 4

Z 3 = 1 + j 4
E 2 = 30 90 °V

ZL = 4 − j 4

IL

FIGURE 3.25
Network of R.3.61.

E 1 = 40 V

E 2 = 30

Z 1 = 8 + j 4

Z 2 = 8 − j 4

Z 3 = 1 + j 4
90 °V

VTH

I 1


+

E 3 = 60 V

FIGURE 3.26
Thevenin’s model of the circuit diagram of Figure 3.25.
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