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Measurement of the conductance of the sodium channel from current fluctuations at the node of Ranvier.
Author(s) -
Conti F,
Hille B,
Neumcke B,
ner W,
Stämpfli R
Publication year - 1976
Publication title -
the journal of physiology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.802
H-Index - 240
eISSN - 1469-7793
pISSN - 0022-3751
DOI - 10.1113/jphysiol.1976.sp011616
Subject(s) - conductance , chemistry , noise (video) , spectral line , tetrodotoxin , analytical chemistry (journal) , depolarization , sodium channel , molecular physics , atomic physics , physics , sodium , biophysics , condensed matter physics , organic chemistry , chromatography , astronomy , artificial intelligence , computer science , image (mathematics) , biology
Single myelinated nerve fibres of Rana esculenta were investigated under voltage clamp conditions at 13 degrees C. Fluctuations of steady‐state membrane current were measured during the last 152 msec of 190‐225 msec pulses depolarizing the membrane by 8‐48 mV. Noise power spectral densities were calculated in the frequency range of 6‐6‐6757 Hz. 2. External application of 150 nM tetrodotoxin (TTX) and/or 10 mM tetraethylammonium (TEA) ion reduced the current fluctuations. The difference of current noise spectra measured in the presence and absence of TTX (TEA) was not changed by the presence of TEA (TTX) during both measurements, and was taken as the spectrum of the Na (K) current fluctuations. 3. Residual current noise during application of both TTX and TEA was, except for some excess noise at the low and high frequency ends of the spectrum, similar to the noise measured from a passive nerve model and could be understood in terms of Nyquist noise of the known resistances and the amplifier noise. 4. Na current fluctuation spectra were interpreted as the sum N/f+SNa(f) where SNa(F) represents the spectrum expected for a set of equal, independent Na channels with only two conductance states (open or closed) which follow Hodgkin‐Huxley kinetics. With values of hinfinity, tauh and minfinity measured from macroscopic Na currents, the measured spectra were fitted well by optimizing N, SNa(0) and taum. Values of taum obtained by this method were in fair agreement with values found from macroscopic currents. 5. The 1/f component of Na current noise was roughly proportional to the square of the steady‐state Na current, I2. The mean value of N/I2 was (1‐1 +/‐ 0‐3) X 10(‐4). 6. The current carried by a single Na channel was calculated from fitted spectra and steady‐state Na currents measured simultaneously with the current fluctuations. The single channel conductance gamma normalized to zero absolute membrane potential was calculated. The average gamma from twelve measurements at depolarizations of 8‐40 mV was 7‐9 +/‐ 0‐9 pS (S.E. of mean). The apparent value of gamma was smallest with small depolarizations. Variations of the assumed kinetic properties of the model did not drastically affect the single channel conductance. 7. External application of 0‐1 mM‐Ni ion lengthened taum in the macroscopic currents and in the fluctuation spectra and enhanced both the steady‐state Na current and the current fluctuations. In Ni‐treated nodes gamma was smaller than in normal nodes.