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I
B2
I
B1
X
CCCII−
Y
Z
+
CCCII+
V
in
Z
Z
in
Y
−
X
C
Fig. 9.20 Electronically-tunable grounded inductance
I
B1
X
Z−
DO-CCCII
I
1
V
1
Y
Z+
C
I
B2
I
2
V
2
Z−
Y
DO-CCCII
X
L
I
1
I
2
Z+
V
1
V
2
Fig. 9.21 Current-controlled floating inductance proposed by Sedef et al. [
18
]
A negative floating inductor can be realized from the above configuration
(though not so recognized in [
18
]) by exchanging the Z+ and Z
terminals of
second DO-CCCII as shown in Fig.
9.22
in which case the equivalent floating
inductance is given by:
L
¼
CR
x1
R
x2
þ
ð
R
x3
Þ
ð
9
:
22
Þ
We now present two more circuits proposed by Abuelma
atti and Tasadduq [
20
],
one of which simulates a floating FDNR and the other one a floating synthetic
'
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