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A graphical representation of the input-output relationship of this
element according to eq. (47) is given in fig. 16 for three different values of
m (0; 0.2; 0.5). For small m (m<0.05) the element is linear with threshold
x
o
= 1. For large m (ª 0.5) the element is an almost perfect “All or Nothing”
device with threshold
1
1 m
.
x
o
=
(48)
-
For values of m in the range 0.1 Æ 0.5 the element displays a logarithmic
transfer function. Indeed, it can easily be shown that in the “vicinity” of
1
1mm
.
x
ª
(49)
(
)
-
Eq. (47) can be approximated by
yKx
o
=
ln
,
(50)
1
4
m
K
=
.
(51)
2
[
]
(
)
(
)
1
-
m
ln
1
-
m
It may be noted that this “vicinity” extends over an appreciable range as
can be seen by the approximation according to (50) which in fig. 16 is super-
imposed in thin line over the exact curves given in bold line.
With the choice of the parameter m we are in a position to change the
transfer function of this element considerably. We suggest the following
nomenclature for the elements that arise for different values of m:
FIGURE 16. Transfer function of an
integrating element under various
operating conditions (m) (bold line),
and approximation by a logarithmic
function (thin line).
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