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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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