Digital Signal Processing Reference
In-Depth Information
Solution: Let the capacitor initial voltage be V o (volts). After the switch is closed,
a d.c. voltage of V volts will suddenly be applied, hence, v i (t) = Vu(t) volts.
i ð t Þ¼ i C ð t Þ¼ C dv C ð t Þ
dt
L
Tables I ð s Þ¼ C ½ sV C ð s Þ v C ð 0 Þ¼ C ½ sV C ð s Þ V o ;
|{z}
current through C
or simply:
I ¼ C ½ sV C V o
ð 1 Þ
v c ¼ v i iR L V C ¼ V i IR ¼ V = s IR
ð 2 Þ
From ( 1 ), ( 2 ) we get:
I ¼ 1
R
V V o
s þ 1 = RC ¼ I o
1
s þ 1 = RC
ð 3 Þ
[where I o = (V - V o )/R.]
From Tables: i(t) = I o e -t/RC u(t) amperes.
Substituting ( 3 )in( 2 ) we get: V C ¼ V ½ s
s þ 1 = RC þ V o
1
s þ 1 = RC
From Tables: v c (t) = [V(1 - e -t/RC )+V o e -t/RC ]u(t) volts.
Tutorial 18
Q: The switch S in Fig. 1 below has been closed for a long time. Find the current
across the capacitor after the switch is opened at t = 0.
+ R 1
+ R 2
ν c
+
+
i ( t )
ν i
V (d.c.)
S
C
L
_
_
_
ν L
+
(1)
Solution: As the switch was closed for a long time, both v C (0 - ) and i L (0 - ) are
zero. Even if there was an initial voltage V o on C and an initial current I o in L when
S was closed, the final current and voltages in the right loop will all be zero. This is
due to the consumption of energy by R 2 . To prove this, consider the right loop
where the switch has been closed as shown in Fig. 2 .
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