TY - JOUR
T1 - Potassium currents and conductance. Comparison between motor and sensory myelinated fibers
AU - Palti, Y.
AU - Moran, N.
AU - Stämpfli, R.
PY - 1980
Y1 - 1980
N2 - The potassium conductance system of sensory and motor fibers from the frog Rana esculenta were studied and compared by means of the voltage clamp. The potassium ion accumulation was first estimated from the currents and reversal potentials within the framework of both a three-compartment model and diffusion-in-an-unstirred-layer model. The potassium conductance parameters were then computed using the measured currents and corrected ionic driving forces. It was found that the potassium accumulation is faster and more pronounced in sensory fibers, the voltage dependency of the potassium conductance is steeper in sensory fibers, the maximal potassium conductance, corrected for accumulation, is approximately 1.1 S/cm2 in sensory and 0.55 S/cm2 in motor fibers, and that the conductance time constants, tau n, are smaller in sensory than in motor fibers. These differences, which increase progressively with depolarization, are not detectable for depolarization of 50 mV or smaller. The interpretation of these findings in terms of different types of potassium channels as well as their implications with regard to the differences between the excitability phenomena in motor and sensory fibers are discussed.
AB - The potassium conductance system of sensory and motor fibers from the frog Rana esculenta were studied and compared by means of the voltage clamp. The potassium ion accumulation was first estimated from the currents and reversal potentials within the framework of both a three-compartment model and diffusion-in-an-unstirred-layer model. The potassium conductance parameters were then computed using the measured currents and corrected ionic driving forces. It was found that the potassium accumulation is faster and more pronounced in sensory fibers, the voltage dependency of the potassium conductance is steeper in sensory fibers, the maximal potassium conductance, corrected for accumulation, is approximately 1.1 S/cm2 in sensory and 0.55 S/cm2 in motor fibers, and that the conductance time constants, tau n, are smaller in sensory than in motor fibers. These differences, which increase progressively with depolarization, are not detectable for depolarization of 50 mV or smaller. The interpretation of these findings in terms of different types of potassium channels as well as their implications with regard to the differences between the excitability phenomena in motor and sensory fibers are discussed.
UR - http://www.scopus.com/inward/record.url?scp=0019129572&partnerID=8YFLogxK
U2 - 10.1016/S0006-3495(80)85029-6
DO - 10.1016/S0006-3495(80)85029-6
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C2 - 6973371
AN - SCOPUS:0019129572
SN - 0006-3495
VL - 32
SP - 955
EP - 966
JO - Biophysical Journal
JF - Biophysical Journal
IS - 3
ER -