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806 ⏐⏐⏐ NETWORK THEOREMS (ac)<br />

R 1<br />

R 2<br />

X C I g<br />

+<br />

Eg –<br />

Z Th<br />

FIG. 18.44<br />

Determining the Thévenin impedance for the<br />

network of Fig. 18.40 using the approach<br />

Z Th � E g / I g.<br />

hI R 1 R 2<br />

R 1<br />

X C<br />

FIG. 18.46<br />

Example 18.11.<br />

R 2<br />

X C<br />

Thévenin<br />

Z Th = R 1 � R 2 – jX C<br />

FIG. 18.47<br />

Determining the Thévenin impedance for the<br />

network of Fig. 18.46.<br />

and<br />

�mR2V<br />

�� R1<br />

� R2<br />

E 1<br />

oc ––––<br />

ZTh � � � �mR<br />

� ––––<br />

2V<br />

Isc �� 1<br />

R<br />

� �<br />

1 � R2<br />

(R1 � R2) � j XC � R 1 � R 2 � j X C<br />

Method 3: See Fig. 18.44.<br />

(R 1 � R 2) � j X C<br />

I g �<br />

E g<br />

��<br />

(R1 � R 2) � j X C<br />

Eg and ZTh � �R1�R2� jXC � Ig<br />

Th<br />

In each case, the Thévenin impedance is the same. The resulting<br />

Thévenin equivalent circuit is shown in Fig. 18.45.<br />

Z Th = R 1 � R 2 – jX C<br />

+<br />

–<br />

�R � 2V ETh = Thévenin<br />

R1 + R2 +<br />

FIG. 18.45<br />

The Thévenin equivalent circuit for the network of Fig. 18.40.<br />

EXAMPLE 18.11 Repeat Example 18.10 for the network of Fig.<br />

18.46.<br />

Solution: From Fig. 18.46, ETh is<br />

hR1R2I ETh � Eoc ��hI(R1 � R2) � �<br />

Method 1: See Fig. 18.47.<br />

ZTh � R1 � R2 � j XC Note the similarity between this solution and that obtained for the previous<br />

example.<br />

Method 2: See Fig. 18.48.<br />

I sc �<br />

�hI(R 1 � R 2)<br />

Eoc and ZTh � � � —— � R1 �<br />

�(<br />

R<br />

R2 � j XC Isc<br />

1 � R2)<br />

hI<br />

� �<br />

(R � R ) � j X<br />

1<br />

�(R 1 � R 2)hI<br />

��<br />

(R 1 � R 2) � j X C<br />

2<br />

C<br />

–<br />

� R1 � R 2

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