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494 ⏐⏐⏐ INDUCTORS<br />

E Th<br />

26.4 V<br />

R Th<br />

10.4 k�<br />

FIG. 12.37<br />

Thévenin equivalent circuit for the network of<br />

Fig. 12.36 for t ≥ 0 s.<br />

L<br />

i L<br />

680 mH<br />

6 mA<br />

a. Find the initial current through the coil. Pay particular attention to its<br />

direction.<br />

b. Find the mathematical expression for the current i L following the<br />

closing of the switch S 2.<br />

c. Sketch the waveform for i L.<br />

Solutions:<br />

a. Using Ohm’s law, the initial current through the coil is determined<br />

by<br />

E 6 V<br />

Ii ��� ��� ��6 mA<br />

R3 1 k�<br />

b. Applying Thévenin’s theorem:<br />

RTh � R1 � R2 � 2.2 k��8.2 k��10.4 k�<br />

ETh � IR1 � (12 mA)(2.2 k�) � 26.4 V<br />

The Thévenin equivalent network appears in Fig. 12.37.<br />

The steady-state current can then be determined by substituting<br />

the short-circuit equivalent for the inductor:<br />

E 26.4 V<br />

If �����2.54 mA<br />

RTh 10.4 k�<br />

The time constant:<br />

t � � �65.39 ms<br />

Applying Eq. (12.12):<br />

iL � If � (Ii � If)e �t/t<br />

L 680 mH<br />

� �<br />

RTh 10.4 k�<br />

� 2.54 mA � (�6 mA � 2.54 mA)e<br />

�t/(65.39 ms)<br />

� 2.54 mA � 8.54 mAe<br />

c. Note Fig. 12.38.<br />

3<br />

2<br />

1<br />

0<br />

–1<br />

–2<br />

–3<br />

–4<br />

–5<br />

–6 mA<br />

i L (mA)<br />

1τ τ<br />

τ τ = 65.39 �s �<br />

�t/65.39 ms<br />

2τ τ 3τ τ 4τ τ 5τ τ<br />

FIG. 12.38<br />

The current i L for the network of Fig. 12.37.<br />

2.54 mA<br />

t

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