Page 375 - Basic Electrical Engineering
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= 10 + j15.7
= 18.6 ∠57.5° Ω
Z = R Ω
3
Total impedance,
or, Z = 4.28 ∠11° + R
Again,
Equating the above two expressions for Z,
4.28 ∠11° + = 9.2
or,
R = 9.2 − 4.28∠11°
= 9.2 − 4.28 (cos 11°+ jsin 11°)
= 9.2 − 4.19 + j 0.8
= 5.01 + j 0.8
Considering the real part, R = 5.01Ω
Example 3.30 In the series–parallel circuit shown in Fig. 3.62, the parallel
branches A and B are in series with branch C. The impedances are Z = (4 +
A

