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354 ⏐⏐⏐ NETWORK THEOREMS<br />

I 1<br />

R 1<br />

I 2<br />

R 2<br />

1 6<br />

and Req � �— � — �<br />

7<br />

� 7<br />

1<br />

�<br />

GT<br />

� S<br />

6<br />

so that<br />

�<br />

40 V<br />

I2� � � � ���2 A<br />

20 �<br />

40<br />

� V<br />

7<br />

——<br />

� 6<br />

�<br />

4<br />

� � � �1 � �<br />

7 7<br />

40<br />

� V<br />

7<br />

——<br />

� 6<br />

Eeq �<br />

Req � R3 � � � 2 �<br />

7<br />

which agrees with the result obtained in Example 8.18.<br />

b. Let us now simply apply the proper equation, Eq. (9.12):<br />

Eeq � � � V<br />

and<br />

1 6<br />

Req � � �— � — �<br />

7<br />

�<br />

which are the same values obtained above.<br />

7<br />

1<br />

——<br />

6<br />

� � S<br />

6 � 6 � � � 1<br />

6 � �<br />

1<br />

——<br />

1<br />

�<br />

1 � � � � 1<br />

6 � �<br />

�<br />

40<br />

—<br />

7<br />

30<br />

V<br />

� � �<br />

6 �<br />

10<br />

V<br />

�<br />

6 �<br />

——<br />

6<br />

�<br />

6 � � � � 1<br />

6 � �<br />

5 V<br />

��� � �<br />

1 �<br />

10<br />

V<br />

�<br />

6 �<br />

——<br />

1<br />

�<br />

1 � � � � 1<br />

6 � �<br />

The dual of Millman’s theorem (Fig. 9.92) appears in Fig. 9.102. It<br />

can be shown that I eq and R eq, as in Fig. 9.102, are given by<br />

I 3<br />

R 3<br />

R L<br />

FIG. 9.102<br />

The dual effect of Millman’s theorem.<br />

Th<br />

�I1R1 � I2R2 � I3R3 Ieq � ���<br />

(9.14)<br />

R1 � R2 � R3 and Req � R1 � R2 � R3 (9.15)<br />

The derivation will appear as a problem at the end of the chapter.<br />

9.7 SUBSTITUTION THEOREM<br />

The substitution theorem states the following:<br />

If the voltage across and the current through any branch of a dc<br />

bilateral network are known, this branch can be replaced by any<br />

I eq<br />

R eq<br />

R L

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