Hardware Reference
In-Depth Information
12.2.2 Filter Design Using DDCC
A DDCC can be considered to be an extended version of DVCC with one additional
input terminal thereby making V
x
¼
V
y2
+V
y3
). This provides the feasibility
of adding and subtracting signals without requiring any external resistor(s) or
additional hardware and thereby offers additional degrees of freedoms in a number
of applications. A DDCC is characterized by the following hybrid matrix:
(V
y1
2
4
3
5
2
4
3
5
2
4
3
5
I
Y
1
I
Y
2
I
Y
3
V
X
I
Z
V
Y
1
V
Y
2
V
Y
3
I
X
V
Z
00000
00000
00000
1
1100
000
¼
ð
12
:
69
Þ
10
where plus and minus signs represent DDCC+ and DDCC
respectively.
Ibrahim-Kuntman-Cicekoglu all pass filter As an example, we present a
canonic implementation of first order APF in Fig.
12.17b
which has been possible
because of capability of the DDCC and is a special case of the general schematic of
Fig.
12.17a
.
Using ideal DDCC+ as shown in Fig.
12.17
, a routine circuit analysis yields the
following voltage transfer function:
V
o
V
i
¼
sCR
1
ð
12
:
70
Þ
sCR
þ
1
and the phase is given by
2 tan
1
ʦðÞ¼
180
ð
ω
CR
Þ
ð
12
:
71
Þ
An alternative APF by Horng-Hou-Chang-Lin-Shiu-Chiu Another first-order
APF using same number of active and passive elements as in Fig.
12.17
was
proposed by Horng et al. [
37
]. However the circuit suffers from a lack of high
input impedance. A routine circuit analysis of Fig.
12.18
yields the following
voltage transfer function:
V
out
V
i
¼
1
sCR
ð
12
:
72
Þ
1
þ
sCR
From equation (
12.73
), the phase of this first-order APF can be determined as:
2 tan
1
ʦðÞ¼
ð
ω
CR
Þ
ð
12
:
73
Þ
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