Abstract
The movement of ions in the aqueous medium as they approach the mouth
(radius a) of a conducting membrane channel is analyzed. Starting
with the Nernst-Planck and Poisson equations, we derive a nonlinear
integrodifferential equation for the electric potential, phi(r),
a less than or equal to r less than infinity. The formulation allows
deviations from charge neutrality and dependence of phi(r) on ion
flux. A numerical solution is obtained by converting the equation
to an integral equation that is solved by an iterative method for
an assumed mouth potential, combined with a shooting method to adjust
the mouth potential until the numerical solution agrees with an asymptotic
expansion of the potential at r-a much greater than lambda (lambda
= Debye length). Approximate analytic solutions are obtained by assuming
charge neutrality (L�uger, 1976) and by linearizing. The linear approximation
agrees with the exact solution under most physiological conditions,
but the charge-neutrality solution is only valid for r much greater
than lambda and thus cannot be used unless a much greater than lambda.
Families of curves of ion flux vs. potential drop across the electrolyte,
phi(infinity)-phi (a), and of permeant ion density at the channel
mouth, n1(a), vs. flux are obtained for different values of a/lambda
and S = a d phi/dr(a). If a much greater than lambda and S = O, the
maximum flux (which is approached when n1(a)----0) is reduced by
50\% compared to the value predicted by the charge-neutrality solution.
Access resistance is shown to be a factor a/2 (a + lambda) times
the published formula (Hille, 1968), which was derived without including
deviations from charge neutrality and ion density gradients and hence
does not apply when there is no counter-ion current. The results
are applied to an idealized diffusion-limited channel with symmetric
electrolytes. For S = O, the current/voltage curves saturate at a
value dependent on a/lambda; for S greater than O, they increase
linearly for large voltage.
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