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1106 ⏐⏐⏐ PULSE WAVEFORMS AND THE R-C RESPONSE<br />

V<br />

v C<br />

5t<br />

T 2 < 5t<br />

vC 5t<br />

V<br />

0 T T 2T t<br />

2<br />

5t<br />

T/2 < 5t<br />

0 T T 2T 3T<br />

t<br />

2<br />

(a)<br />

T 2 = 5t<br />

(a)<br />

If T/2 < 5t or T < 10t, the voltage v C will not reach its final value during<br />

the first pulse (Fig. 24.29), and the discharge cycle will not return<br />

to zero volts. In fact, the initial value for each succeeding pulse will<br />

change until steady-state conditions are reached. In most instances, it is<br />

a good approximation to assume that steady-state conditions have been<br />

established in five cycles of the applied waveform.<br />

V<br />

R<br />

– V<br />

R<br />

FIG. 24.29<br />

v C and i C for T/2 < 5t.<br />

V<br />

R<br />

i C<br />

FIG. 24.28<br />

v C and i C for T/2 � 5t.<br />

i C<br />

5t<br />

0 T<br />

2<br />

T 2T t<br />

– V<br />

R<br />

5t<br />

(b)<br />

0 T T 2T 3T t<br />

2<br />

As the frequency increases and the period decreases, there will be a<br />

flattening of the response for vC until a pattern like that in Fig. 24.30<br />

results. Figure 24.30 begins to reveal an important conclusion regarding<br />

the response curve for vC: Under steady-state conditions, the average value of vC will equal the<br />

average value of the applied square wave.<br />

V<br />

v C<br />

T 2

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