Gating characteristics of a steeply voltage-dependent gap junction channel in rat Schwann cells.
Open Access
- 1 November 1993
- journal article
- research article
- Published by Rockefeller University Press in The Journal of general physiology
- Vol. 102 (5), 925-946
- https://doi.org/10.1085/jgp.102.5.925
Abstract
The gating properties of macroscopic and microscopic gap junctional currents were compared by applying the dual whole cell patch clamp technique to pairs of neonatal rat Schwann cells. In response to transjunctional voltage pulses (V(j)), macroscopic gap junctional currents decayed exponentially with time constants ranging from < 1 to < 10 s before reaching steady-state levels. The relationship between normalized steady-state junctional conductance (G(ss)) and (V(j)) was well described by a Boltzmann relationship with e-fold decay per 10.4 mV, representing an equivalent gating charge of 2.4. At V(j) > 60 mV, G(ss) was virtually zero, a property that is unique among the gap junctions characterized to date. Determination of opening and closing rate constants for this process indicated that the voltage dependence of macroscopic conductance was governed predominantly by the closing rate constant. In 78% of the experiments, a single population of unitary junctional currents was detected corresponding to an unitary channel conductance of approximately 40 pS. The presence of only a limited number of junctional channels with identical unitary conductances made it possible to analyze their kinetics at the single channel level. Gating at the single channel level was further studied using a stochastic model to determine the open probability (P(o)) of individual channels in a multiple channel preparation. P(o) decreased with increasing V(j) following a Boltzmann relationship similar to that describing the macroscopic G(ss) voltage dependence. These results indicate that, for V(j) of a single polarity, the gating of the 40 pS gap junction channels expressed by Schwann cells can be described by a first order kinetic model of channel transitions between open and closed states.Keywords
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