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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