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12.8 INITIAL VALUES<br />

This section will parallel Section 10.9 (Initial Values—Capacitors) on<br />

the effect of initial values on the transient phase. Since the current<br />

through a coil cannot change instantaneously, the current through a<br />

coil will begin the transient phase at the initial value established by<br />

the network (note Fig. 12.23) before the switch was closed. It will<br />

then pass through the transient phase until it reaches the steady-state<br />

(or final) level after about five time constants. The steady-state level of<br />

the inductor current can be found by simply substituting its shortcircuit<br />

equivalent (or R l for the practical equivalent) and finding the<br />

resulting current through the element.<br />

Using the transient equation developed in the previous section, an<br />

equation for the current i L can be written for the entire time interval of<br />

Fig. 12.23; that is,<br />

i L � I i � (I f � I i)(1 � e �t/t )<br />

with (I f � I i) representing the total change during the transient phase.<br />

However, by multiplying through and rearranging terms:<br />

we find<br />

i L � I i � I f � I f e �t/t � I i � I ie �t/t<br />

� I f � I f e �t/t � I ie �t/t<br />

i L � I f � (I i � I f)e �t/t<br />

(12.12)<br />

If you are required to draw the waveform for the current i L from initial<br />

value to final value, start by drawing a line at the initial value and<br />

steady-state levels, and then add the transient response (sensitive to the<br />

time constant) between the two levels. The following example will clarify<br />

the procedure.<br />

EXAMPLE 12.5 The inductor of Fig. 12.24 has an initial current level<br />

of 4 mA in the direction shown. (Specific methods to establish the initial<br />

current will be presented in the sections and problems to follow.)<br />

a. Find the mathematical expression for the current through the coil<br />

once the switch is closed.<br />

b. Find the mathematical expression for the voltage across the coil during<br />

the same transient period.<br />

c. Sketch the waveform for each from initial value to final value.<br />

Solutions:<br />

a. Substituting the short-circuit equivalent for the inductor will result in<br />

a final or steady-state current determined by Ohm’s law:<br />

E<br />

16 V 16 V<br />

If ����� ���1.78 mA<br />

R1 � R2 2.2 k��6.8 k� 9 k�<br />

The time constant is determined by<br />

L 100 mH 100 mH<br />

t ����� ���11.11 ms<br />

RT 2.2 k��6.8 k� 9 k�<br />

i L<br />

INITIAL VALUES ⏐⏐⏐ 485<br />

Ii initial<br />

conditions<br />

transient<br />

response<br />

steady-state<br />

region<br />

0 t<br />

FIG. 12.23<br />

Defining the three phases of a transient waveform.<br />

R 1<br />

2.2 k�<br />

E 16 V L = 100 mH<br />

R 2<br />

6.8 k�<br />

FIG. 12.24<br />

Example 12.5.<br />

I f<br />

i L<br />

4 mA<br />

+<br />

v L<br />

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