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FIGURE 4. Two finite state machines (
E
) (W) connected via delays (black
semicircles).
v
(
t
),
z
(
t
), z(
t
), i.e., expressing these variables explicitly as functions of time,
is purely mathematical. In other words, the “meta-system” (
E
W) composed
of the subsystems
E
and W, is physically as well as mathematically “closed,”
and its behavior is completely determined for all times. Moreover, if at a
particular time, say
t
= 0 (initial condition), the values of all variables
u
(0),
v
(0),
z
(0), z(0) are known, it is also completely predictable. Since this meta-
system is without input, it churns away according to its own rules, coming
ultimately to a static or dynamic equilibrium, depending on the rules and
the initial conditions.
In the general case the behavior of such systems has been extensively
studied by computer simulation (Walker, 1965; Ashby and Walker, 1966;
Fitzhugh, 1963), while in the linear case the solutions for Eqs. (28) can be
obtained in straight-forward manner, particularly if the recursions can be
assumed to extend over infinitesimally small steps:
dw
dt
(
)
=
()
+
wwt
¢=
+
D
wt
D
(29)
Under these conditions the four Eqs. (28) become
4
Â
a
1
w
-
w
(30)
i
i
j
j
j
=
where the
w
i
(
i
= 1, 2, 3, 4) are now the real numbers and replace the four
variables in question,
w
.
represents the first derivative with respect to time,
and the 16 coefficients
a
ij
(
i
,
j
= 1, 2, 3, 4) define the four linear functions
under consideration. This system of simultaneous, first-order, linear differ-
ential equations is solved by
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