Simultaneous changes in the equilibrium potential and potassium conductance in voltage clamped Ranvier node in the frog.

1. In voltage clamped myelinated nerve fibres, the K+ conductance has been calculated from current recordings obtained in low and high K+ media, taking into account the changes in EK resulting from accumulation of depletion of K+ ions near to nodal membrane. 2. At the end of a depolarization, the instantaneous K+ current reverses at a potential (instantaneous reversal potential) differing from the Nernst potential calculated using the external and internal bulk concentrations (theoretical Nernst potential). During a depolarization, EK, as estimated from the instantaneous reversal potential, changes continuously. This change depends on the size, the duration and the direction of the time dependent K+ current. The variation of EK is attributed to continuous changes in K+ concentration near the membrane during voltage pulses which turn on the K+ conductance. 3. The chord conductance [GK = IK/(E‐EK), as calculated using the instantaneous reversal potential values for EK, has been analysed as a function of time and membrane potential. As previously reported it increases with the initial K+ concentration in the external medium. 4. The time course of the K+ current depends on both the kinetics of the conductance increase and the rate of change in the driving force for K. The kinetics of the conductance increase can satisfactorily be described by a single exponential function following a delay after the onset of the depolarizing voltage clamp pulse. 5. This delay increases when the holding potential is made more negative. It decreases with membrane depolarization and it is independent of the external K+ concentration. At a given membrane potential, the turning on of the K+ conductance is found to be faster at high than at low external K+ concentrations. 6. At repolarization the turning off of the conductance cannot be described by a single exponential function. It is faster at low than at high external K+ concentrations. 7. The results suggest that the change in K+ conductance proceeds in a multi‐step transition or (and) that the K+ conductance is determined by several types of K+ channels.

[1]  J. Dubois Evidence for the existence of three types of potassium channels in the frog Ranvier node membrane. , 1981, The Journal of physiology.

[2]  J. Dubois,et al.  POST‐TETANIC MEMBRANE POTENTIAL IN SINGLE AXON AND MYELINATED NERVE TRUNK , 1980, Annals of the New York Academy of Sciences.

[3]  T. Begenisich Conditioning hyperpolarization-induced delays in the potassium channels of myelinated nerve. , 1979, Biophysical journal.

[4]  B. Krylov,et al.  Spike frequency adaptation in amphibian sensory fibres is probably due to slow K channels , 1978, Nature.

[5]  Y. Palti,et al.  Cole-Moore effect in the frog node. , 1978, Proceedings of the National Academy of Sciences of the United States of America.

[6]  G. Bruin,et al.  Potassium ion noise currents and inactivation in voltage-clamped node of Ranvier , 1977, Nature.

[7]  Y. Palti,et al.  Effect of conditioning potential on potassium current kinetics in the frog node. , 1976, Biophysical journal.

[8]  R. Keynes,et al.  The temporal and steady‐state relationships between activation of the sodium conductance and movement of the gating particles in the squid giant axon. , 1976, The Journal of physiology.

[9]  Francisco Bezanilla,et al.  Charge Movement Associated with the Opening and Closing of the Activation Gates of the Na Channels , 1974, The Journal of general physiology.

[10]  B. Hille Potassium Channels in Myelinated Nerve , 1973, The Journal of general physiology.

[11]  B. Hille,et al.  The Inner Quaternary Ammonium Ion Receptor in Potassium Channels of the Node of Ranvier , 1972, The Journal of general physiology.

[12]  B. Hille Charges and Potentials at the Nerve Surface : Divalent ions and pH , 1968 .

[13]  J. Moore,et al.  Potassium ion current in the squid giant axon: dynamic characteristic. , 1960, Biophysical journal.

[14]  A. Hodgkin,et al.  The after‐effects of impulses in the giant nerve fibres of Loligo , 1956, The Journal of physiology.

[15]  A. Hodgkin,et al.  The effect of sodium ions on the electrical activity of the giant axon of the squid , 1949, The Journal of physiology.

[16]  Y. Palti,et al.  Diffusion of ions in myelinated nerve fibers. , 1979, Biophysical journal.

[17]  B. Frankenhaeuser,et al.  A quantitative description of potassium currents in myelinated nerve fibres of Xenopus laevis , 1963, The Journal of physiology.

[18]  B. Frankenhaeuser,et al.  Potassium permeability in myelinated nerve fibres of Xenopus laevis , 1962, The Journal of physiology.

[19]  Ada Frances Johnson,et al.  Diffusion of Ions , 1918 .