Jp. Novak, ELECTRIC-POTENTIAL AND CONCENTRATION OF ION SPECIES IN THE PROXIMITY OF A CELL-MEMBRANE - AB-INITIO CALCULATIONS, Journal of theoretical biology, 185(2), 1997, pp. 173-187
The mathematical model of ion transport in the field of electric force
s and diffusion gradients is based on particle conservation equations
and the Poisson equation which governs the distribution of the electri
c potential. Designed for evaluating the currents through passive ion
channels in cellular membranes, the model is formulated in a two-dimen
sional approximation assuming rotational symmetry. Three ionic species
are considered in the present study: sodium, calcium and chlorine. Th
e program developed for the numerical solution is based on a semi-anal
ytical approximation suggested by Gummel & Scharfetter. The present co
ntribution reports calculations of the steady-state distributions of i
onic species induced by an electric field due to a negative potential
drop across the cellular membrane, which represent initial conditions
for future calculations of the time development of the ion flux throug
h the calcium channel. The numerical calculations were performed from
the moment of potential application up to the time 6.2 mu s, when a ne
w steady state is established. At this stage, the maximum values of th
e sodium and calcium concentrations at the membrane surface are about
22% and 47% above the initial values of 145 mM and 1 mM, respectively,
while the chlorine concentration is approximately 18% below. The elec
tric field at the membrane surface is about 6.7 x 10(4) and decreases
exponentially with distance. The length of the boundary layer is about
40 Angstrom. Since the model is based on fundamental principles, it c
an be used for the quantitative solution of any problem possessing rot
ational symmetry where a continuum approach is applicable and some ele
mentary conditions are fulfilled, such as equilibrium (or at least qua
si-equilibrium) of the particle energy distributions with respect to t
ime and electric field, and the assumption that the transport coeffici
ents are defined as functions of the field and their numerical values
are known. (C) 1997 Academic Press Limited.