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a
1
1
Y
Y
Y
CCII−
CCII−
Z
CCII−
Z
1
Z
X
X
X
R
4
R
5
R
6
R
1
R
3
R
2
C
3
C
2
C
1
D
L
5uA
b
0A
−5uA
−10uA
−700mV
−400mV
0V
V(C3:2)
400mV
750mV
I (L)
Fig. 8.31 A three phase oscillator converted into a chaotic oscillator using diode inductor
composite proposed by Elwakil and Kennedy (Adapted from [
14
]
1991 Elsevier Science Ltd.)
©
(a) The circuit (b) PSPICE generated V
c3
-I
L
trajectory
biasing supply for CCII
9 V. The circuit (Fig.
8.31b
) was tuned to
obtain different trajectories by adjusting R
z
to different values. The authors have
claimed that using the same technique multiphase oscillators such as six phase
oscillators can also be converted into chaotic oscillators.
Petrzela and Slezak in [
18
] demonstrated that several novel oscillators consisting
of only five CCII+ s can be devised to generate conservative chaotic attractors. In
fact they presented a class of autonomous deterministic dynamical systems with
taken as
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