ABSTRACT
Measurements have been made of the extraneuronal potential changes produced by replacement of sodium ions with other organic and inorganic cations in the solution bathing isolated abdominal connectives.
It is concluded that the ionic dependence of the extraneuronal potentials is similar to that of a theoretical model system consisting of a perineurial diffusion barrier in series with a long, narrow channel representing the system of intercellular clefts connecting the inwardly facing surface of the perineurium with the extraaxonal fluid.
On the basis of this model the effect of high external concentrations of, for example, potassium ions would be to depolarize the outwardly facing perineurial cell membranes. The considerable departure of the observed potentials from the values predicted by the Nernst equation can be accounted for in terms of the short-circuiting effect, due to the finite ionic permeability of the tight junctions between perineurial cells. Qualitative predictions can also be made concerning the rates of movement of potassium and sodium ions in the extracellular system.
The terms ‘positivation’ and ‘negativation’ have been preferred to depolarization and hyperpolarization to distinguish the extraneuronal potential changes from the electrical events taking place at the axon membrane level.
Strictly, the equations for the potential difference should be derived from the activities of the ions concerned. It is assumed, for convenience, that these are approximately equal to their concentrations. If the activity coefficients on the two sides of the barrier are similar, the effect of this approximation will not be serious (cf. Moreton, 1968b).
It is assumed that diffusion in the extracellular system is unrestricted (cf. Treherne et al. 1970).