scholarly journals LOW LEVEL IMPEDANCE CHANGES FOLLOWING THE SPIKE IN THE SQUID GIANT AXON BEFORE AND AFTER TREATMENT WITH "VERATRINE" ALKALOIDS

1953 ◽  
Vol 37 (1) ◽  
pp. 39-51 ◽  
Author(s):  
Abraham M. Shanes ◽  
Harry Grundfest ◽  
Walter Freygang
Keyword(s):  
Sea Water ◽  
Giant Axon ◽  
Squid Giant Axon ◽  
Satisfactory Explanation ◽  
Chloride Permeability ◽  
Potential Oscillations ◽  
Temporal Course ◽  
Before And After ◽  
Conductance Changes ◽  
Conductance Increase

The increase in conductance, which accompanies the spike in the presence of sea water, is followed by a decrease to below the resting level, here designated as the "initial after-impedance," which lasts 3 msec. and is 3 per cent as great as the increase. Treatment with cevadine usually obliterates the latter but leaves the former essentially unaltered. In addition, the alkaloid gives rise to periodic conductance increases followed by a prolonged, exponentially decaying elevated conductance (the "negativity after-impedance") which correspond closely to potential oscillations and to the negative after-potential. These are also only a few per cent of the major conductance change. Veratridine causes a conductance increase which lasts longer and which also conforms closely with earlier after-potential results. Preliminary calculations indicate that the negativity after-impedance and the negative after-potential may be due to the subsidence of an elevated chloride permeability. However, no satisfactory explanation is available for the initial after-impedance or for the temporal course of the conductance changes associated with oscillations in membrane potential.

scholarly journals LONGITUDINAL IMPEDANCE OF THE SQUID GIANT AXON

1941 ◽  
Vol 24 (6) ◽  
pp. 771-788 ◽  
Author(s):  
Kenneth S. Cole ◽  
Richard F. Baker
Keyword(s):  
Sea Water ◽  
Low Frequency ◽  
Giant Axon ◽  
Squid Giant Axon ◽  
Dielectric Characteristics ◽  
Impedance Characteristics ◽  
Longitudinal Impedance ◽  
Electrode Length ◽  
Interpolar Distance ◽  
Inductive Reactance

Longitudinal alternating current impedance measurements have been made on the squid giant axon over the frequency range from 30 cycles per second to 200 kc. per second. Large sea water electrodes were used and the inter-electrode length was immersed in oil. The impedance at high frequency was approximately as predicted theoretically on the basis of the poorly conducting dielectric characteristics of the membrane previously determined. For the large majority of the axons, the impedance reached a maximum at a low frequency and the reactance then vanished at a frequency between 150 and 300 cycles per second. Below this frequency, the reactance was inductive, reaching a maximum and then approaching zero as the frequency was decreased. The inductive reactance is a property of the axon and requires that it contain an inductive structure. The variation of the impedance with interpolar distance indicates that the inductance is in the membrane. The impedance characteristics of the membrane as calculated from the measured longitudinal impedance of the axon may be expressed by an equivalent membrane circuit containing inductance, capacity, and resistance. For a square centimeter of membrane the capacity of 1 µf with dielectric loss is shunted by the series combination of a resistance of 400 ohms and an inductance of one-fifth henry.

scholarly journals Effect of Temperature on the Potential and Current Thresholds of Axon Membrane

1962 ◽  
Vol 46 (2) ◽  
pp. 257-266 ◽  
Author(s):  
Rita Guttman ◽  
Keyword(s):  
Sea Water ◽  
Sucrose Solution ◽  
Giant Axon ◽  
Threshold Current ◽  
Squid Giant Axon ◽  
Effect Of Temperature ◽  
Threshold Potential ◽  
Axon Membrane ◽  
Central Segment ◽  
The Mean

The effect of temperature on the potential and current thresholds of the squid giant axon membrane was measured with gross external electrodes. A central segment of the axon, 0.8 mm long and in sea water, was isolated by flowing low conductance, isoosmotic sucrose solution on each side; both ends were depolarized in isoosmotic KCl. Measured biphasic square wave currents at five cycles per second were applied between one end of the nerve and the membrane of the central segment. The membrane potential was recorded between the central sea water and the other depolarized end. The recorded potentials are developed only across the membrane impedance. Threshold current values ranged from 3.2 µa at 267deg;C to 1 µa at 7.5°C. Threshold potential values ranged from 50 mv at 26°C to 6 mv at 7.5°C. The mean Q10 of threshold current was 2.3 (SD = 0.2), while the Q10 for threshold potentials was 2.0 (SD = 0.1).

The effect of displacement current on the measurement of reversal potential in squid giant axon

1982 ◽  
Vol 60 (12) ◽  
pp. 1541-1544 ◽  
Author(s):  
H. Wodlinger ◽  
H. Kunov ◽  
H. L. Atwood
Keyword(s):  
Voltage Clamp ◽  
Time Constant ◽  
Reversal Potential ◽  
Giant Axon ◽  
Squid Giant Axon ◽  
Displacement Current ◽  
Before And After

The measurement of the sodium reversal potential (Erev), as that potential where the early current reverses during voltage clamp, was found to exceed the true Erev by 4.1 ± 2.4 mV (mean ± SD) in squid giant axon. This error was found in both intact and internally perfused axons and is due to interference from the displacement current. This was shown by subtraction of the current records obtained before and after treatment with tetrodotoxin (TTX). The error in Erev is proportional to [Formula: see text] where Td is the time constant of the displacement current.

scholarly journals Action of External Divalent Ion Reduction on Sodium Movement in the Squid Giant Axon

1961 ◽  
Vol 45 (1) ◽  
pp. 93-103 ◽  
Author(s):  
William J. Adelman ◽  
John W. Moore
Keyword(s):  
Sea Water ◽  
Giant Axon ◽  
Sodium Concentration ◽  
Squid Giant Axon ◽  
Ion Concentration ◽  
Resting Potential ◽  
Slow Increase ◽  
Sodium Permeability ◽  
Sodium Accumulation ◽  
Sodium Flux

Voltage clamp measurements of the sodium potential have been made on the resting squid giant axon to study the effect of variations in external divalent ion concentration upon net sodium flux. From these measurements the intracellular sodium concentration and the net sodium inflow were calculated using the Nernst relation and constant activity coefficients. While an axon bathed in artificial sea water shows a slow increase in internal sodium concentration, the rate of sodium accumulation is increased about two times by reducing external calcium and magnesium concentrations to 0.1 times their normal values. The mean inward net sodium flux increases from a mean control value of 97 pmole/cm2 sec. to 186 pmole/cm2 sec. in low divalent solution. Associated with these effects of external divalent ion reduction are a marked decrease in action potential amplitude, little or no change in resting potential, and a shift along the voltage axis of the curve relating peak sodium conductance to membrane potential similar to that obtained by Frankenhaeuser and Hodgkin (1957). These results implicate divalent ions in long term (minutes to hours) sodium permeability.

scholarly journals Liquid Junction and Membrane Potentials of the Squid Giant Axon

1960 ◽  
Vol 43 (5) ◽  
pp. 971-980 ◽  
Author(s):  
Kenneth S. Cole ◽  
John W. Moore
Keyword(s):  
Membrane Potential ◽  
Sea Water ◽  
Specific Resistance ◽  
Cumulative Effect ◽  
Giant Axon ◽  
Squid Giant Axon ◽  
Liquid Junction ◽  
Axon Membrane ◽  
Best Value ◽  
Liquid Junction Potentials

The potential differences across the squid giant axon membrane, as measured with a series of microcapillary electrodes filled with concentrations of KCl from 0.03 to 3.0 M or sea water, are consistent with a constant membrane potential and the liquid junction potentials calculated by the Henderson equation. The best value for the mobility of an organic univalent ion, such as isethionate, leads to a probably low, but not impossible, axoplasm specific resistance of 1.2 times sea water and to a liquid junction correction of 4 mv. for microelectrodes filled with 3 M KCl. The errors caused by the assumptions of proportional mixing, unity activity coefficients, and a negligible internal fixed charge cannot be estimated but the results suggest that the cumulative effect of them may not be serious.

scholarly journals Ammonium Ion Currents in the Squid Giant Axon

1969 ◽  
Vol 53 (3) ◽  
pp. 342-361 ◽  
Author(s):  
Leonard Binstock ◽  
Harold Lecar
Keyword(s):  
Voltage Clamp ◽  
Ammonium Chloride ◽  
Time Course ◽  
Giant Axon ◽  
Squid Giant Axon ◽  
Ammonium Ion ◽  
Ion Currents ◽  
Potassium Permeability ◽  
Nerve Excitability ◽  
Conductance Changes

Voltage-clamp studies on intact and internally perfused squid giant axons demonstrate that ammonium can substitute partially for either sodium or potassium. Ammonium carries the early transient current with 0.3 times the permeability of sodium and it carries the delayed current with 0.3 times the potassium permeability. The conductance changes observed in voltage clamp show approximately the same time course in ammonium solutions as in the normal physiological solutions. These ammonium ion permeabilities account for the known effects of ammonium on nerve excitability. Experiments with the drugs tetrodotoxin (TTX) and tetraethyl ammonium chloride (TEA) demonstrate that these molecules block the early and late components of the current selectively, even when both components are carried by the same ion, ammonium.

scholarly journals THE EFFECT OF TEMPERATURE, POTASSIUM, AND SODIUM ON THE CONDUCTANCE CHANGE ACCOMPANYING THE ACTION POTENTIAL IN THE SQUID GIANT AXON

1957 ◽  
Vol 41 (2) ◽  
pp. 333-342 ◽  
Author(s):  
E. Amatniek ◽  
W. Freygang ◽  
H. Grundfest ◽  
G. Kiebel ◽  
A. Shanes
Keyword(s):  
Time Course ◽  
Giant Axon ◽  
Membrane Resistance ◽  
Squid Giant Axon ◽  
Effect Of Temperature ◽  
Concentration Of Ions ◽  
Temperature Ranges ◽  
Conductance Changes ◽  
Lower Temperature ◽  
Possible Cause

Conductance changes associated with the response of the squid giant axon have been studied at two temperature ranges (26–27°C.; 9–10°C.) and with modified concentrations of sodium and potassium in the medium. The phase of "initial after-conductance," during which the membrane resistance increases above the resting value, is smaller at the lower temperature. At both temperature ranges it is diminished by doubling K+ in the medium and enhanced by removal of K+. Halving the Na+ of the medium also enhances this phase when K+ is absent, but not otherwise. The time course of the conductance changes alters in form with changes of the external medium. These changes indicate independent changes in the complex of ionic events associated with the response. The experiments therefore confirm the reality of the phase of increased membrane resistance. The magnitude of this change appears to be considerable and requires a transient decrease in the mobility and/or concentration of ions in the membrane. The possible cause of this decrease is discussed.

scholarly journals Ionic Conductance Changes in Lobster Axon Membrane When Lanthanum Is Substituted for Calcium

1966 ◽  
Vol 50 (2) ◽  
pp. 461-471 ◽  
Author(s):  
M. Takata ◽  
W. F. Pickard ◽  
J. Y. Lettvin ◽  
J. W. Moore
Keyword(s):  
Sea Water ◽  
Ionic Currents ◽  
Ionic Conductance ◽  
Membrane Action ◽  
Axon Membrane ◽  
Trivalent Rare Earth ◽  
Sucrose Gap ◽  
Conductance Changes ◽  
Time Courses ◽  
Conductance Increase

The trivalent rare earth lanthanum was substituted for calcium in the sea water bathing the exterior of an "artificial node" of a lobster axon in a sucrose gap. It caused a progressive rise in threshold, and a decrease in the height of the action potential as well as in its rates of rise and fall. Prolonged application produced an excitation block. Voltage-clamp studies of the ionic currents showed that the time courses of the ionic conductance changes for both sodium and potassium were increased. Concurrently, the potentials at which the conductance increases occurred were shifted to more positive inside values for the La+++ sea water. These effects resemble changes resulting from a high external calcium concentration. Over and above this, La+++ also causes a marked reduction in the maximum amount of conductance increase following a depolarizing potential step. Membrane action potentials similar to those observed experimentally in the La+++ solution have been computed with appropriate parameter changes in the Hodgkin-Huxley equations.

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