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FIGURE 6. Geometry of the sensory field for a specific sensor
r
x0
susceptible to an
agent D distributed over environmental space.
2.251 In some cases it is possible to compute the spatial distribution
of an agent from the known distribution of its effects along a closed surface
of given shape. For instance, the spatial distribution of an electrical poten-
tial
V
x
has a unique solution by solving Laplace's equation
D
V
= 0
for given values
V
x
along a closed orientable surface (electric fish). Other
examples may be cited.
2.252 In some other cases it is possible to compute the spatial dis-
tribution of an agent from its effects on just two small, but distinct regions
on the body. For instance, the (Euclidean, 3-
D
) notion of “depth” is com-
puted by resolving the discrepancy of having the “same scene” represented
as different images on the retinas of the two eyes in binocular animals
(Fig. 7). Let
L
(
x
,
y
) be a postretinal network which computes the relation
“
x
is left of
y
.” While the right eye reports object “
a
” to be to the left of
“
b
,” (
L
r
[
a
,
b
]), the left eye gives the contradictory report of object “
b
” being
to the left of “
a
,” (
L
1
[
b
,
a
]). A network
B
which takes cognizance of the dif-
ferent origin of signals coming from cell groups {
r
x
}
r
and {
r
x
}
1
to the right
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