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Fig. 5.16 Two distinctly
different floating negative
impedance configurations
using CCII emerging from
the nullor models of
Fig. 5.14
z
z
CCII-
CCII-
y
y
x
x
Z L
2
1
z
z
CCII-
CCII-
y
x
x
y
Z L
2
1
It may be mentioned that the four CCII+ based structures of Fig. 5.13 as well as
the two CCII
based structures of Fig. 5.16 , all are characterized by the terminal
equations: i 1 ¼ i 2 ¼
(
1/Z L )[V 1 -V 2 ] and represent floating impedance
Z L ,
between ports 1 and 2.
In the last, it is also worthwhile to mention that four electronically-controllable
negative resistance converters, each employing two electronically- tunable CCIIs,
have been advanced by Surakampontorn and Thitimajshima in [ 55 ]. Another
scheme of realizing floating current controlled resistance converter using electron-
ically controlled conveyor
(ECC) has been reported by Riewruja
and
Petchmaneelumka in [ 126 ].
5.2.8 Generalized Function Generator
In their seminal 1970 paper where the second generation current conveyor was
introduced (see reference [ 3 ] of Chap. 1) Sedra-Smith demonstrated how CCIIs
along with ideal diodes can be employed to realize a generalized function generator.
Their proposition is shown here in Fig. 5.17
Assuming the diodes to be characterized by the equation
I s e v d =v T
i d ¼
ð
5
:
22
Þ
a straight forward analysis of the circuit, assuming all matched diodes, leads to the
following output equation:
i m 1
1
i m 2
2
i m n
n
I 0 ¼
:::::
ð
5
:
23
Þ
with m 1 þ
 
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