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340 ⏐⏐⏐ NETWORK THEOREMS<br />

R 2<br />

R 2<br />

4 �<br />

I N = 3 A<br />

4 �<br />

R 1<br />

5 �<br />

I<br />

10 A<br />

R N = 2 �<br />

FIG. 9.64<br />

Substituting the Norton equivalent circuit for<br />

the network external to the resistor R L of<br />

Fig. 9.60.<br />

FIG. 9.66<br />

Example 9.12.<br />

R 1<br />

5 �<br />

a<br />

R L<br />

b<br />

R N<br />

9 �<br />

FIG. 9.68<br />

Determining R N for the network of Fig. 9.67.<br />

a<br />

R L<br />

b<br />

a<br />

b<br />

Step 5: See Fig. 9.64. This circuit is the same as the first one considered<br />

in the development of Thévenin’s theorem. A simple conversion<br />

indicates that the Thévenin circuits are, in fact, the same (Fig. 9.65).<br />

EXAMPLE 9.12 Find the Norton equivalent circuit for the network<br />

external to the 9-� resistor in Fig. 9.66.<br />

Solution:<br />

Steps 1 and 2: See Fig. 9.67.<br />

R 2<br />

I N<br />

4 �<br />

3 A<br />

R 1<br />

5 �<br />

I<br />

10 A<br />

a<br />

R N = 2 �<br />

b<br />

a<br />

I N<br />

b<br />

R Th = R N = 2 �<br />

FIG. 9.69<br />

Determining I N for the network of Fig. 9.67.<br />

R 2<br />

4 �<br />

I<br />

b a<br />

I N<br />

R1 10 A<br />

Th<br />

E Th = I N R N = (3 A)(2 �) = 6 V<br />

FIG. 9.65<br />

Converting the Norton equivalent circuit of Fig. 9.64 to a Thévenin<br />

equivalent circuit.<br />

R 2<br />

4 �<br />

R 1<br />

5 �<br />

I<br />

10 A<br />

FIG. 9.67<br />

Identifying the terminals of particular interest for the network of Fig. 9.66.<br />

Step 3: See Fig. 9.68, and<br />

RN � R1 � R2 � 5 ��4 ��9 �<br />

Step 4: As shown in Fig. 9.69, the Norton current is the same as the<br />

current through the 4-� resistor. Applying the current divider rule,<br />

R1I (5 �)(10 A) 50 A<br />

IN � ��� ���5.556 A<br />

5 ��4 � 9<br />

� R1 � R 2<br />

a<br />

b<br />

a<br />

b<br />

5 �

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