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dn
dt =
n 1
n
n n
(7)
dm
dt =
m 1
m
m m
(15)
dh
dt =
h 1
h
h h
(16)
and
10
exp V + 10
V
+
10
n =
001
(12)
1
0125 exp V
80
n =
(13)
25
exp V + 25
V +
10
m =
01
(20)
1
4 exp V
18
m =
(21)
h = 007 exp V
(23)
20
1
exp V + 30
10 +
h =
(24)
1
The first four of these equations are the differential equations which govern
the system's behavior. The many computer simulations of the H and H model
involve programs that repeatedly step through those first four equations (see
Fodor, 2005, for one example).
Equation [26] is then applied to the action potential. We are most interested
in the 'propagated action potential,' as distinguished from a uniform membrane
 
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