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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