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The current of the i-th electrode is
I electrode
A i
i electrode D
(1.65)
with A i D 2˛ i L denoting the surface of segment i. Thus, one arrives at a set of
coupled differential equations
I electrode
A 1
c 1 dV 1
dt
V 1
C
r m 1 D g 1;2 .V 2 V 1 / C
(1.66)
I electrode
A 2
c 2 dV 2
dt
V 2
C
r m 2 D g 2;1 .V 1 V 2 / C
or equivalently
c 1 dV 1
dt
V 1
V 2 V 1
r 1
C
r M 1 D
C i 1
(1.67)
c 2 dV 2
dt
V 2
V 1 V 2
r 2
C
r M 2 D
C i 2
Next, it is assumed that the current is injected in only one out of the two cylinders,
that is i 2 D 0.Itisassumedthatr 1 D r 2 D r and r M 1
D r M 2
D r M .From
Eqs. ( 1.66 ) and ( 1.67 ) it holds
c 1 dV 1
dt
C c 2 dV 2
dt
V 1 C V 2
r M
C
D i 1
(1.68)
Thus, finally about the segment's resistance one has
V 1
i 1
r M .r C r M /
rC2r M
D
(1.69)
while the variation of voltage V at the i-th segment is generalized as follows
C P k;j V k V j
C j dV j
dt
V j
R j
D
C I j
(1.70)
R jk
where R kj denotes the resistance of the connection between the k-th and the j-th
segment.
1.7.2
Computing Cable's Equation in Neurons
It is assumed that the cable is defined in the interval .0;l/ and that its cross-section
is circular with diameter d.x/. The cable is segmented in n-parts and the distance
from the origin is defined as x j D jh, where h D
l
n is the elementary length. Each
part has surface equal to A j D d j h where d j D d.x j / is the diameter and the
associated surface of the cross-section is equal to d j
4 . It is assumed that the special
resistance and the capacitance of the membrane are c M and r M , respectively, while
 
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