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496 ⏐⏐⏐ INDUCTORS<br />

R<br />

1.2 k�<br />

L T<br />

1.01 H<br />

FIG. 12.42<br />

Terminal equivalent of the network of<br />

Fig. 12.41.<br />

E<br />

E<br />

+<br />

10 V<br />

–<br />

I<br />

+<br />

21 V<br />

–<br />

R 1<br />

2 �<br />

The inductor L1 is then in series with the equivalent parallel value, and<br />

LT � L1 � L″ T � 0.56 H � 0.45 H<br />

� 1.01 H<br />

The reduced equivalent network appears in Fig. 12.42.<br />

12.13 R-L AND R-L-C CIRCUITS<br />

WITH dc INPUTS<br />

We found in Section 12.7 that, for all practical purposes, an inductor<br />

can be replaced by a short circuit in a dc circuit after a period of time<br />

greater than five time constants has passed. If in the following circuits<br />

we assume that all of the currents and voltages have reached their final<br />

values, the current through each inductor can be found by replacing<br />

each inductor with a short circuit. For the circuit of Fig. 12.43, for<br />

example,<br />

E 10 V<br />

I1 �����5 A<br />

R1 2 �<br />

I 1<br />

L = 2 H R 2 3 �<br />

+<br />

10 V<br />

–<br />

FIG. 12.43<br />

Substituting the short-circuit equivalent for the inductor for t > 5t.<br />

10 mH<br />

R 1<br />

5 �<br />

E<br />

R 1<br />

2 �<br />

For the circuit of Fig. 12.44,<br />

E 21 V<br />

I �����10.5 A<br />

R2 � R3 2 �<br />

R 2<br />

I1 6 mH<br />

3 �<br />

R 3<br />

6 �<br />

E<br />

+<br />

21 V<br />

–<br />

R 1<br />

5 �<br />

FIG. 12.44<br />

Establishing the equivalent network for t > 5t.<br />

I<br />

I<br />

R 2<br />

I 1<br />

I 1<br />

3 �<br />

2 �<br />

R 2<br />

R 3<br />

3 �<br />

6 �

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