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0.16
0.14
0.12
0.1
0.08
0.06
0.04
0.02
0
10
20
30
40
50
60
70
80
time
Fig. 1.5
Diagram of membrane's voltage variation
1.3
Describing Membrane's Voltage Dynamics with Cable's
Equation
The previous analysis has considered that the neurons have a spherical shape. This
assumption does not hold for neurons' axon and in the case of neurons' dendrites
where the neurons' shape is better approximated by a cylinder. In the latter case it
is considered that the neurons have the shape of a long cylinder or cable, or cable of
radius a as depicted in Fig. 1.6 .
The equation of the membrane's voltage according to the cable's model is a
partial differential equation that describes the voltage's spatiotemporal variation
V M .x;t/. Voltage V M .x;t/ depends also on the coaxial currents I L that pass
through the cell [ 21 ].
The aggregate resistance of the cable, for radius a and length x is given by
r L x
˛ 2
R L D
(1.33)
where r L is a special resistance. According to Ohm's law, for the change of voltage
along the cables's axis holds [ 16 , 65 ]
V M .x C x;t/ V M .x;t/ DI L .x;t/R L DI L .x;t/ x
˛ 2 r L
(1.34)
 
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