Action of Certain Tropine Esters on Voltage-Clamped Lobster Axon

Tropine p-tolylacetate (TPTA) and its quaternary analogue, tropine p-tolylacetate methiodide (TPTA MeI) decrease the early transient (Na) and late (K) currents in the voltage-clamped lobster giant axon. These agents, which block the nerve action potential, reduce the maximum Na and K conductance increases associated with membrane depolarization. They also slow the rate at which the sodium conductance is increased and shift the (normalized) membrane conductance vs. voltage curves in the direction of depolarization along the voltage axis. All these effects are qualitatively similar to those resulting from the action of procaine on the voltage-clamped axon. One unusual effect of the tropine esters, noticeable particularly at large depolarization steps, is that they cause the late, K current to reach a peak and then fall off with increasing pulse duration. This effect has not been reported to occur as a result of procaine action. Tropine p-chlorophenyl acetate (TPClA), which differs from TPTA only by the substitution of a p-Cl for a p-CH₃ group on the benzene ring, had a negligible effect on axonal excitability.     

Ionic Conductance Changes in Voltage Clamped Crayfish Axons at Low pH

Giant axons from the crayfish have been voltage clamped with an axial wire system. General characterististics of observed ionic currents under normal conditions are similar to those measured in other giant axons and in nodes of Ranvier. As the pH of the external bath is lowered below 7, a marked, reversible slowing of potassium currents is seen with little effect on sodium currents. The steady-state potassium conductance-voltage curve is shifted along the voltage axis in a manner consistent with the development of a hyperpolarizing surface charge. Results suggest that this potential shift accounts for part, though not all, of the observed increase in τ_n. From the behavior of the kinetics of the delayed current with external pH these alterations in potassium conductance are attributed to the titration of a histidine imidazole residue of a membrane protein. Chemical modification of histidine by carbethoxylation at pH 6 slows and strongly depresses potassium currents. The results suggest that in addition to the introduction of electrostatic forces, possibly resulting from a hyperpolarizing surface charge, protonation of a histidine group at low pH also alters the nonelectrostatic chemical interactions determining the ease with which potassium gates open and close. The evidence indicates that the modified histidine residue is closely associated with the membrane components involved in the control of potassium conductance.     

Inactivation of the Sodium Current in Myxicola Giant Axons : Evidence for coupling to the activation process

Experiments were conducted on Myxicola giant axons to determine if the sodium activation and inactivation processes are coupled or independent. The main experimental approach was to examine the effects of changing test pulses on steady-state inactivation curves. Arguments were presented to show that in the presence of a residual uncompensated series resistance the interpretation of the results depends critically on the manner of conducting the experiment. Analytical and numerical calculations were presented to show that as long as test pulses are confined to an approximately linear negative conductance region of the sodium current-voltage characteristic, unambiguous interpretations can be made. When examined in the manner of Hodgkin and Huxley, inactivation in Myxicola is quantitatively similar to that described by the h variable in squid axons. However, when test pulses were increased along the linear negative region of the sodium current-voltage characteristic, steady-state inactivation curves translate to the right along the voltage axis. The shift in the inactivation curve is a linear function of the ratio of the sodium, conductance of the test pulses, showing a 5.8 mv shift for a twofold increase in conductance. An independent line of evidence indicated that the early rate of development of inactivation is a function of the rise of the sodium conductance.     

Effect of calcium upon sodium inactivation in the giant axon ofLoligo pealei

Summary Giant axons ofLoligo pealei were voltage clamped in artificial seawater solutions containing varying concentrations of calcium from 10 to 100mm, and the sodium conductance inactivation was measured with a series of two-pulse experiments. Theh vs. voltage curve showed a shift of about 10 mV in the depolarizing direction on the voltage axis for a tenfold increase in external calcium without substantial alteration in the slope of the voltage dependence. The kinetics of the inactivation process were found to be exponential for hyperpolarizing prepulses, but showed some indication of a sigmoidal decay for depolarizing prepulses in all calcium concentrations employed. Increasing calcium increased the delay in the sigmoidal response. The inactivation time constant _h increased as a function of calcium concentration over the potential range studied, –10 to –90 mV. The values of the rate constants _h and _h are decreased with an increase in calcium and these effects are not consistent with parallel shifts of the rate constant vs. voltage curves along the voltage axis for changes in calcium concentration.Magnesium does not behave as an equimolar substitute for calcium. The effect of a solution containing 10mm calcium and 50mm magnesium is intermediate to that of solutions containing 10 and 30mm calcium alone.Predictions of a recent model for the sodium conductance (Moore, J.W., Cox, E.B., 1976Biophys. J. 16:171) which employs calcium binding were compared with the experimental data.     

Effect of calcium ions on outward currents in the somatic membrane of mollusk giant neurons

Potassium currents through the somatic membrane of giant neurons ofHelix pomatia in normal (10 mM Ca) Ringer's solution and low-calcium (1 mM Ca) solution were studied by the voltage clamp method. With a decrease in the Ca concentration to 1 mM peak potassium conductance versus membrane, potential curves and inactivation curves were shifted along the voltage axis in the negative direction by about 10 mV. Inactivation of the delayed potassium current was slowed in low Ca solution. The effect of a decrease in external calcium concentration on volt-ampere and inactivation characteristics increased with a rise in external pH. These effects of a low Ca concentration on potassium mechanisms of the giant neuron somatic membrane can be attributed to changes in the negative surface potential in the region of the potassium channels.A. A. Bogomolets Institute of Physiology, Academy of Sciences of the Ukrainian SSR, Kiev. Institute of Biology, Hungarian Academy of Sciences, Tihany. Translated from Neirofiziologiya, Vol. 8, No. 4, pp. 400–409, July–August, 1976.     

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

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.     

The influence of protons and zinc ions on the steady-state inactivation of Kv1.3 potassium channels

Using the whole-cell patch-clamp technique, we investigated the influence of extracellular pH and zinc ions (Zn²⁺) on the steady-state inactivation of Kv1.3 channels expressed in human lymphocytes. The obtained data showed that lowering the extracellular pH from 7.35 to 6.8 shifted the inactivation midpoint (V_i) by 17.4 ± 1.12 mV (n = 6) towards positive membrane potentials. This shift was statistically significant (p < 0.05). Applying 100 μM Zn²⁺ at pH 6.8 further shifted the Vi value by 16.55 ± 1.80 mV (n = 6) towards positive membrane potentials. This shift was also statistically significant (p < 0.05). The total shift of the Vi by protons and Zn²⁺ was 33.95 ± 1.90 mV (n = 6), which was significantly higher (p < 0.05) than the shift caused by Zn²⁺ alone. The Zn²⁺-induced shift of the V_i at pH 6.8 was almost identical to the shift at pH = 7.35. Thus, the proton-and Zn²⁺-induced shifts of the V_i value were additive. The steady-state inactivation curves as a function of membrane voltage were compared with the functions of the steady-state activation. The total shift of the steady-state inactivation was almost identical to the total shift of the steady-state activation (32.01 ± 2.10 mV, n = 10). As a result, the “windows” of membrane potentials in which the channels can be active under physiological conditions were also markedly shifted towards positive membrane potentials. The values of membrane voltage and the normalised chord conductance corresponding to the points of intersection of the curves of steady-state activation and inactivation were also calculated. The possible physiological significance of the observed modulatory effects is discussed herein.     

A kinetic analysis of the electrogenic pump ofChara corallina: II. Dependence of the pump activity on external pH

Summary The current-voltage curve of theChara membrane was obtained by applying a slow ramp de- and hyperpolarization by use of voltage clamp. By inhibiting the electrogenic pump with 50m DCCD (dicyclohexylcarbodiimide), theI–V curve approached a steady state within 100 min, which gave thei _d -V curve of the passive diffusion channel. Thei _p -V curve of the electrogenic pump channel was obtained by subtracting the latter from the former. With the increase of external pH, thei _d -V curve showed only a slight change, while thei _p -V curve of the pump channel showed almost a parallel shift, in the hyperpolarizing direction, along the voltage axis in the pH range between 6.5 and 7.5. The sigmoidali _p -V curve in this pH range could be simulated satisfactorily with the five-state model reported previously (U. Kishimoto, N. Kami-ike, Y. Takeuchi & T. Ohkawa,J. Membrane Biol. 80:175–183, 1984) as well as with a lumped two-state model presented in this report. The analysis based on these models suggests that the electrogenic pump of theChara membrane is mainly a 2H⁺/1ATP pump. The forward rate constant in the voltage-dependent step increased with the increase of external pH, while the backward one decreased. On the other hand, the forward rate constant in the voltage-independent step remained almost unchanged with the increase of external pH, while the backward one increased markedly. The pump conductance at the resting membrane potential showed either a slight increase or a decrease with the increase of external pH, depending on the sample. Nevertheless, the pump current showed generally a slight increase with the increase of external pH.     

Changes in membrane hydrogen and sodium conductances during progesterone-induced maturation of Ambystoma oocytes

A voltage-gated hydrogen ion-selective conductance has been previously described in the immature oocyte of the urodele amphibian Ambystoma. The present study was prompted by reports that changes in membrane voltage and internal pH, as well as in internal sodium ion concentration, occur during the hormone-induced maturation of oocytes from other amphibians. As activation of membrane currents might mediate changes in internal ion concentrations in addition to altering the membrane voltage, microelectrode recording techniques have been employed to examine changes in membrane conductances which occur during maturation of Ambystoma oocytes. It was observed that during the first 5 hr of maturation the magnitude of the hydrogen ion conductance gradually decreased, and that subsequently there was an increase in the amplitude of a voltage-dependent noninactivating sodium conductance. After 6 to 7 hr, after the loss of the hydrogen conductance and at about the time of germinal vesicle breakdown, the resting potential of the oocyte spontaneously shifted from approximately -10 mV to approximately +30 mV, where it remained until at least 24 hr after the initiation of maturation. This voltage transition was due to the appearance of mechanisms generating inward current in the oocyte membrane; part of this inward current was due to the tonic activation of the sodium conductance. Changes in internal pH and internal sodium ion concentration occurred during maturation, as judged from shifts in the reversal potentials of both hydrogen and sodium currents. A gradual decrease in internal hydrogen ion concentration was observed up until the time of disappearance of the hydrogen conductance (change in internal pH from about 7.15 in immature oocytes to about 7.40 by 3 hr after application of progesterone). This was followed, as sodium conductance increased, by an apparent rise in the internal sodium ion concentration (from about 6 mM to about 17 mM by 10 hr postprogesterone).     

A kinetic analysis of the electrogenic pump ofChara corallina: I. Inhibition of the pump by DCCD

Summary The current-voltage curve of theChara membrane was obtained by applying a slow ramp depo- and hyperpolarization by use of voltage clamp. With the progress of poisoning by DCCD (dicyclohexylcarbodiimide) theI–V curve moved by about 50 mV (depolarization) along the voltage axis, reducing its slope, and finally converged to thei _d -V curve of the passive diffusion channel. Changes ofi _p -V curve of the electrogenic pump channel could be obtained by subtracting the latter from the former.The sigmoidali _p -V curve could be simulated satisfactorily by adopting a simple reaction kinetic model. Kinetic parameters of the successive changes of state of the H⁺ ATPase could be evaluated. Changes of these kinetic parameters during inhibition gave useful information about the molecular mechanism of the electrogenic pump.Depolarization of the membrane potential, decrease of membrane conductance, and decrease of pump current during inhibition of the pump with DCCD are caused mainly by the decrease of conductance of the pump channel. The decrease of this pump conductance is caused principally by a marked decrease of the rate constant for releasing H⁺ to the outside.     

Voltage gated ionic channels in rat cultured astrocytes, reactive astrocytes and an astrocyte-oligodendrocyte progenitor cell

Astrocytes (both type 1 and type 2), cultured from the central nervous system of newborn or 7 day old rats show voltage gated sodium and potassium channels that are activated when the membrane is depolarized to greater than -40 mV. The sodium channels in these cells have an h-infinity curve similar to that of nodal membranes but the activation (peak current-voltage) curves are shifted along the voltage axis by about +30 mV. These sodium currents are blocked only by high concentrations of tetrodotoxin. The voltage activated potassium currents in both types of astrocyte show at least two components; an inactivating component that is suppressed at holding potentials of greater than -40 mV and a persistent, non-inactivating current. Several types of single channel currents were observed in outside-out membrane patches from type 2 astrocytes. One type of potassium channel showed inactivation on depolarization and may contribute to the whole-cell inactivating current. In contrast, oligodendrocytes showed no obvious voltage gated membrane channels. The properties of the type 2 astrocyte-oligodendrocyte progenitor cell were investigated in two ways: 1) by examination of cells just beginning to differentiate along the "electrically silent" oligodendrocyte pathway or 2) by recording from progenitor cells cultured for 24 hours in the presence of cycloheximide to block the appearance of new membrane channels. In both cases, voltage gated inward (sodium) and outward (potassium) currents were noted. The outward current response showed both an inactivating and a non-inactivating component. Similar voltage activated inward and outward membrane currents were noted in reactive astrocytes freshly isolated (3-6 hours) from lesioned areas of adult rat brains.(ABSTRACT TRUNCATED AT 250 WORDS)     

Magnitude and location of surface charges on Myxicola giant axons

The effects of changes in the concentration of calcium in solutions bathing Myxicola giant axons on the voltage dependence of sodium and potassium conductance and on the instantaneous sodium and potassium current-voltage relations have been measured. The sodium conductance-voltage relation is shifted along the voltage axis by 13 mV in the hyperpolarizing direction for a fourfold decrease in calcium concentration. The potassium conductance-voltage relation is shifted only half as much as that for sodium. There is no effect on the shape of the sodium and potassium instantaneous current-voltage curves: the normal constant-field rectification of potassium currents is maintained and the normal linear relationship of sodium currents is maintained. Considering that shifts in conductances would reflect the presence of surface charges near the gating machinery and that shape changes of instantaneous current-voltage curves would reflect the presence of surface charges near the ionic pores, these results indicate a negative surface charge density of about 1 electronic charge per 120 A2 near the sodium gating machinery, about 1 e/300 A2 for the potassium gating machinery, and much less surface charge near the sodium or potassium pores. There may be some specific binding of calcium to these surface charges with an upper limit on the binding constant of about 0.2 M-1. The differences in surface charge density suggest a spatial separation for these four membrane components.     

Competitive Action of Calcium and Procaine on Lobster Axon : A study of the mechanism of action of certain local anesthetics

Voltage clamp studies with the squid giant axon have shown that changes in the external calcium concentration (Frankenhaeuser and Hodgkin, 1957) shift the sodium and potassium conductance versus membrane potential curves along the potential axis. Taylor (1959) found that procaine acts primarily by reducing the sodium and, to a lesser extent, the potassium conductances. Both procaine and increased calcium also delay the turning on of the sodium conductance mechanism. Calcium and procaine have similar effects on lobster giant axon. In addition, we have observed that the magnitude of the response to procaine is influenced by the external calcium concentration. Increasing external calcium tends to reduce the effectiveness of procaine in decreasing sodium conductance. Conversely, procaine is more effective in reducing the membrane conductance if external calcium is decreased. The amplitude of the nerve action potential reflects these conductance changes in that, for example, reductions in amplitude resulting from the addition of procaine to the medium are partially restored by increasing external calcium, as was first noted by Aceves and Machne (1963). These phenomena suggest that calcium and procaine compete with one another with respect to their actions on the membrane conductance mechanism. The fact that procaine and its analogues compete with calcium for binding to phospholipids in vitro (Feinstein, 1964) suggests that the concept of competitive binding to phospholipids may provide a useful model for interpreting these data.     

Modification of sodium channel gating by lanthanum. Some effects that cannot be explained by surface charge theory

In clonal pituitary (GH3) cells we studied the changes in sodium channel gating caused by substitution of La3+ for Ca2+ ion. Gating of sodium channels was simplified by using intracellular papain to remove inactivation. To quantify La effects, we empirically fitted closing and the late phase of opening of the channels with single exponentials, determined the opening (a) and closing (b) rate, and plotted these rates as a function of Vm (membrane voltage). The midpoint of the fraction open-Vm curve was also determined. Changing from Ca to La shifted the curves for these three measures of Na channel gating along the voltage axis and changed their shape somewhat. Surface charge theory, in the form usually presented, predicts equal shifts of all three curves, with no change in shape. We found, however, that the shift for each of the measurements was different. 2 mM La, for example, shifted opening kinetics by +52 mV (i.e., 52 mV must be added to the depolarization to make activation in 2 mM La as fast as in 2 mM Ca), the fraction open voltage curve by +42.5 mV, and the closing rate curve by +28 mV. The shift was an almost linear function of log [La] for each of the measures. The main finding is that changing from 2 mM Ca to 10 microM La causes a positive shift of the opening rate and fraction open curves, but a negative shift of the closing rate curve. The opposite signs of the two effects cannot be explained in terms of surface charge theory. We briefly discuss some alternatives to this theory.     

Sensitivity of the sodium and potassium channels of Myxicola giant axons to changes in external pH

Myxicola giant axons were studied using standard voltage-clamp techniques in solutions whose pH values ranged from 3.9 to 10.2. Buffer concentrations of 50 mM or greater were necessary to demonstrate the full effect of pH. In acidic solutions the axon underwent a variable depolarization, and both the sodium and potassium conductances were reversibly depressed with approximate pKa's of 4.8 and 4.4, respectively. The voltage dependence of GNa was only slightly altered by acidic conditions, whereas there occurred large shifts in GK along the voltage axis consistent with a substantial decrease in net negative surface charge in the vicinity of the K+ channels. The sodium and potassium activation rate constants were decreased by acidic conditions, but the results could not be described as a simple translation along the voltage axis.     

Effect of extracellular pH on sodium current in isolated,single rat ventricular cells

Summary Effects of extracellular pH on the sodium current (I _Na) of single rat ventricular cells were examined under conditions of voltage clamp and internal perfusion. In this way, pH _i was controlled while pH _o was changed. The combined suction pipette-microelectrode method was used. The suction pipette passed current and perfused the cell's interior; the microelectrode measured membrane potential. Increasing extracellular H⁺ depressedI _Na and slowed inactivation. The current-voltage curves forI _Na and Slowed inactivation. The current-voltage curves forI _Na were shifted to positive and negative potentials at low and high pH _o , respectively. Similar potential shifts were observed in both the conductance voltage curve and the steadystate inactivation voltage curve (h ). Conduction was also depressed at low pH _o . The shifts were probably due to surface charge effects, while the impaired conduction was probably due to protonation of a site in the Na channel.     

Dynamics of potassium ion currents in squid axon membrane. A re-examination.

The original experiments of Cole and Moore (1960. Biophys. J. 1:161-202.), using conditioning and test membrane potentials to examine the dynamics of the potassium channel conductance in the squid axon, have been extended to test voltage levels by the use of tetrodotoxin to block the sodium conductance. The potassium currents for test voltage levels from -20 to +85 mV were superposable by translation along the time axis for all conditions tested: (a) with depolarizing conditioning voltages; (b) with hyperpolarizing conditioning voltages; and (c) in normal and in high potassium external media. The only deviations from superposition seen were when the internal sodium concentration was abnormally high and the potassium currents showed saturation at high levels of depolarization. Some restoration toward normal kinetics could be obtained by rapidly repeated depolarizations.     

Ionic Blockage of Sodium Channels in Nerve

Increasing the hydrogen ion concentration of the bathing medium reversibly depresses the sodium permeability of voltage-clamped frog nerves. The depression depends on membrane voltage: changing from pH 7 to pH 5 causes a 60% reduction in sodium permeability at +20 mV, but only a 20% reduction at +180 mV. This voltage-dependent block of sodium channels by hydrogen ions is explained by assuming that hydrogen ions enter the open sodium channel and bind there, preventing sodium ion passage. The voltage dependence arises because the binding site is assumed to lie far enough across the membrane for bound ions to be affected by part of the potential difference across the membrane. Equations are derived for the general case where the blocking ion enters the channel from either side of the membrane. For H⁺ ion blockage, a simpler model, in which H⁺ enters the channel only from the bathing medium, is found to be sufficient. The dissociation constant of H⁺ ions from the channel site, 3.9 x 10^-6 M (pK_a 5.4), is like that of a carboxylic acid. From the voltage dependence of the block, this acid site is about one-quarter of the way across the membrane potential from the outside. In addition to blocking as described by the model, hydrogen ions also shift the responses of sodium channel "gates" to voltage, probably by altering the surface potential of the nerve. Evidence for voltage-dependent blockage by calcium ions is also presented.     

Intracellular sodium activity and sodium transport inNecturus gallbladder epithelium

Summary Ion-sensitive glass microelectrodes, conventional microelectrodes and isotope flux measurements were employed inNecturus gallbladder epithelium to study intracellular sodium activity, [Na] _i , electrical parameters of epithelial cells, and properties of active sodium transport. Mean control values were: [Na] _i : 9.2 to 12.1mm; transepithelial potential difference, _ms : –1.5 mV (lumen negative); basolateral cell membrane potential, _es : –62 mV (cell interior negative); sodium conductance of the luminal cell membrane,g _Na: 12 mho cm^–2; active transcellular sodium flux, 88 to 101 pmol cm^–2 sec^–1 (estimated as instantaneous short-circuit current). Replacement of luminal Na by K led to a decrease of the intracellular sodium activity at a rate commensurate to the rate of active sodium extrusion across the basolateral cell membrane. Mucosal application of amphotericin B resulted in an increase of the luminal membrane conductance, a rise of intracellular sodium activity, and an increase of short-circuit current and unidirectional mucosa to serosa sodium flux. Conclusions: (i) sodium transport across the basolateral membrane can proceed against a steeper chemical potential difference at a higher rate than encountered under control conditions; (ii) the luminal Na-conductance is too low to accommodate sodium influx at the rate of active basolateral sodium extrusion, suggesting involvement of an electrically silent luminal transport mechanism; (iii) sodium entry across the luminal membrane is the rate-limiting step of transcellular sodium transport and active sodium extrusion across the basolateral cell membrane is not saturated under control conditions.     

Action of extracellular pH on Na+ and K+ membrane currents in the giant axon ofLoligo Vulgaris

Summary Voltage-clamp currents and resting membrane potential of squid giant axons have been studied at extracellular pH varying between 4 and 10. The membrane currents, analyzed according to the Hodgkin-Huxley equations, showed that sodium permeability,P _Na (E), and potassium conductance,g _K (E), curves were shifted toward positive voltages by different amounts and slightly depressed as the external pH was lowered. Under the same conditions, _m(E) and _n(E) were found to be enhanced and shifted to a larger extent in the same direction. The rate constants _m and _n were shifted substantially toward positive voltages, but _m and _n changed hardly at all. The shift of the _m(E) curve was analyzed in terms of a fixed surface charge model; it indicates that unspecific negative groups with an approximate pK_a of 4.5 are located in the vicinity of sodium active sites with an average charge separation of 8 Å. A similar figure is obtained for the potassium system from the shift of the _n(E) curve.