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Pulse and Digital Circuits Venkata Rao K., Rama Sudha K. and Manmadha Rao G.<br />
iv. During the period T < t < 3T/2, that is, between 2 <strong>to</strong> 3 ms, the output decays.<br />
1.0<br />
10<br />
At t = 3 ms v<br />
o<br />
=<br />
f<br />
At 3 ms, the input falls by 100 V. Hence<br />
V g<br />
= V – 100 = 19.73 V<br />
f<br />
V = V e<br />
e = 132.32 (0.9048) = 119.73 V.<br />
v. During 3T /2 < t < 2T, that is, d uring 3 <strong>to</strong> 4 ms, the output decays.<br />
1.0<br />
10<br />
0.1<br />
At t = 2T= 4 ms, v<br />
o<br />
= V<br />
h<br />
= V g<br />
e = 19.73 e =17.85 V.<br />
V<br />
j<br />
= V<br />
h<br />
+ 100 V = 17.85+100=117.85 V.<br />
In a few cycles, the output reaches the steady state.<br />
Steady-state response:<br />
Under steady state, the output is symmetrical with respect <strong>to</strong> zero volts, since the<br />
capaci<strong>to</strong>r blocks dc. Therefore, the dc component in the output is zero.<br />
Let V 1 be the voltage at t = 0<br />
t<br />
<br />
For 0 < t < T/2, v<br />
o<br />
= V1<br />
e<br />
'<br />
0.1<br />
At t = T/2=1 ms, vo<br />
= V1<br />
= V<br />
1e<br />
= 0.905 V<br />
1<br />
'<br />
V<br />
1<br />
= 0.905 V<br />
1<br />
(3)<br />
As the input abruptly falls, output also falls by the same amount <strong>to</strong> V 2 .<br />
(tT / 2)<br />
<br />
For T/2 < t < T v<br />
o<br />
= V<br />
2<br />
e<br />
'<br />
0.1<br />
At t = T, v o<br />
= V 2 = V 2<br />
e = 0.905 V 2<br />
'<br />
V2 = 0.905 V<br />
2<br />
(4)<br />
For symmetrical wave<br />
' '<br />
V<br />
1<br />
= V 2<br />
and V<br />
1<br />
= V2<br />
(5)<br />
'<br />
'<br />
V<br />
1<br />
V2<br />
= 100 V and V1<br />
V 2<br />
= 100 V (6)<br />
'<br />
From (6), we have V1 V2<br />
= 100 V (7)<br />
And from (3), we have V1<br />
= V2<br />
(8)<br />
'<br />
Substituting (8) in (7), we have V<br />
1<br />
+ V 1<br />
= 100 V (9)<br />
'<br />
From (3), we have V<br />
1<br />
= 0.905 V<br />
1<br />
Substituting in (9)<br />
0.905V 1<br />
+ V<br />
1= 100 V<br />
1.905V 1<br />
= 100 V.<br />
'<br />
V<br />
1<br />
=52.49 V and V 1<br />
= 0.905V 1<br />
= (0.905)(52.49)= 47.50 V<br />
' '<br />
From (5) as V<br />
1<br />
= V2<br />
an d V1<br />
= V2<br />
'<br />
V 2<br />
= –52.49 V V 2<br />
= –47.50 V<br />
We can now plot the steady-state response as we know<br />
'<br />
V = 52.49 V<br />
V = 47.50 V<br />
1 1<br />
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