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Fig. 1.4
Electric circuit consisting of ion channels in cell's membrane
V M E k
r k
I k D
(1.20)
By applying Kirchhoff's law in the loop, in the transient stage, one gets [ 16 , 65 ]
I capac C I k )c M dV M
dt
.V M E k /
r k
C
D 0
(1.21)
that is
c M dV M
dt
V M E k
r k
D
Dg k .V M E k /
(1.22)
For example, in the case of N D 3 ion channels of the Cl, K and Na type it holds
that the aggregate ions current is
V M E Cl
R Cl
V M E K
R K
V M E Na
R Na
I ion D
(1.23)
or using the normalized conductance coefficients g Cl , g K , and g Na and the normal-
ized capacitance c M one has
I ion Dg Cl .V M E Cl / g K .V M E K / g Na .V M E Na /
(1.24)
Equivalently, assuming an external input current I (normalized per surface of the
membrane), it holds that [ 16 , 65 ]
I.t/
A
c M dV M
dt
Dg Cl .V M E Cl / g K .V M E K / g Na .V M E Na / C
(1.25)
where A denoted membrane's surface (Fig. 1.4 ). Using the notation
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