Voltage-clamped Squid Giant Axons Research Articles

Silvio Weidmann 1921–2005

Silvio Weidmann’s death on July 11, 2005, brings to a close a heroic period for cellular cardiac electrophysiology. Silvio was the first to record accurate cardiac transmembrane action potentials and to identify the roles of sodium and potassium currents in excitation, conduction, and repolarization in cardiac cells. From his experiments in the 1950’s has grown the entire field of cardiac electrophysiology. His ideas and their influence on those who entered the field after him set the standard for progress in the last half-century. The field is now a cornerstone of clinical cardiac care. ⇓ Dr Silvio Weidmann. Photograph courtesy of Ruth Weidmann. Silvio graduated from the University of Bern Medical School in 1946, after interruptions for service in the Swiss Army. In 1948 he went from Uppsala to Cambridge, England, to work with future Nobel laureate Alan Hodgkin—an experience that set the stage for Silvio’s major contributions. After four years back in Bern, …

Single ion occupancy and steady-state gating of Na channels in squid giant axon.

The properties of the small fraction of tetrodotoxin (TTX)-sensitive Na channels that remain open in the steady state were studied in internally dialyzed voltage clamped squid giant axons. The observed Ussing flux ratio exponent (n′) of 0.97 ± 0.03 (calculated from simultaneous measurements of TTX-sensitive current and 22Na efflux) and nonindependent behavior of Na current at high internal [Na] are explained by a one-site (“1s”) permeation model characterized by a single effective binding site within the channel pore in equilibrium with internal Na ions (apparent equilibrium dissociation constant K Nai(0) = 0.61 ± 0.08 M). Steady-state open probability of the TTX-sensitive channels can be modeled by the product p a p ∞, where p a represents voltage-dependent activation described by a Boltzmann distribution with midpoint V a = −7 mV and effective valence z a = 3.2 (Vandenberg, C.A., and F. Bezanilla. 1991. Biophys. J. 60:1499–1510) coupled to voltage-independent inactivation by an equilibrium constant (Bezanilla, F., and C.M. Armstrong. 1977. J. Gen. Physiol. 70:549–566) K eq = 770. The factor p ∞ represents voltage-dependent inactivation with empirical midpoint V ∞= −83 ± 5 mV and effective valence z ∞ = 0.55 ± 0.03. The composite p a p ∞ 1s model describes the steady-state voltage dependence of the persistent TTX-sensitive current well.

Killing K channels with TEA+.

Tetraethylammonium (TEA+) is widely used for reversible blockade of K channels in many preparations. We noticed that intracellular perfusion of voltage-clamped squid giant axons with a solution containing K+ and TEA+ irreversibly decreased the potassium current when there was no K+ outside. Five minutes of perfusion with 20 mM TEA+, followed by removal of TEA+, reduced potassium current to < 5% of its initial value. The irreversible disappearance of K channels with TEA+ could be prevented by addition of > or = 10 mM K+ to the extracellular solution. The rate of disappearance of K channels followed first-order kinetics and was slowed by reducing the concentration of TEA+. Killing is much less evident when an axon is held at -110 mV to tightly close all of the channels. The longer-chain TEA+ derivative decyltriethylammonium (C10+) had irreversible effects similar to TEA+. External K+ also protected K channels against the irreversible action of C10+. It has been reported that removal of all K+ internally and externally (dekalification) can result in the disappearance of K channels, suggesting that binding of K+ within the pore is required to maintain function. Our evidence further suggests that the crucial location for K+ binding is external to the (internal) TEA+ site and that TEA+ prevents refilling of this location by intracellular K+. Thus in the absence of extracellular K+, application of TEA+ (or C10+) has effects resembling dekalification and kills the K channels.

Prepubertal height velocity references over a wide age range.

<h3>ABSTRACT</h3> The block of voltage-dependent sodium channels by saxitoxin (STX) and tetrodotoxin (TTX) was investigated in voltage-clamped squid giant axons internally perfused with a variety of permeant monovalent cations. Substitution of internal Na⁺ by either NH₄⁺ or N₂H₅⁺ resulted in a reduction of outward current through sodium channels under control conditions. In contrast, anomalous increases in both inward and outward currents were seen for the same ions if some of the channels were blocked by STX or TTX, suggesting a relief of block by these internal cations. External NH₄⁺ was without effect on the apparent magnitude of toxin block. Likewise, internal inorganic monovalent cations were without effect, suggesting that proton donation by NH₄⁺ might be involved in reducing toxin block. Consistent with this hypothesis, decreases in internal pH mimicked internal perfusion with NH₄⁺ in reducing toxin block. The interaction between internally applied protons and externally applied toxin molecules appears to be competitive, as transient increases in sodium channel current were observed during step increases in intracellular pH in the presence of a fixed STX concentration. In addition to these effects on toxin block, low internal pH produced a voltage-dependent block of sodium channels and enhanced steady-state inactivation. Elevation of external buffer capacity only marginally diminished the modulation of STX block by internal NH₄⁺, suggesting that alkalinization of the periaxonal space and a resultant decrease in the cationic STX concentration during NH₄⁺ perfusion may play only a minor role in the effect. These observations indicate that internal monovalent cations can exert trans-channel influences on external toxin binding sites on sodium channels.

Na + conductance and the threshold for repetitive neuronal firing

The Hodgkin-Huxley equation for electrogenesis in the voltage clamped squid giant axon was used to predict the effect of altering maximal Na + conductance ( g Na max +) on the repetitive firing process. The main finding was that increasing g Na max +, without changing any other membrane parameter, reduced the threshold current required to evoke repetitive firing. That is, it rendered the membrane hyperexcitable. Threshold for evoking single action potentials was also affected, but much less so. Other consequences of increasing g Na max + were decrease in the minimum sustainable rhythmic firing frequency (mRFF), a monotonic increase in firing frequency at any given suprathreshold stimulus intensity, an increase in the current value at which intense depolarizing stimuli block rhythmogenesis, an increase in the maximal sustainable firing frequency using intense currents (MRFF), and the consequent expansion of the dynamic range for stimulus encoding. Thus, the control of g Na max + through the regulation of Na + channel synthesis and membrane incorporation at sites of rhythmogenesis (e.g. axon hillock-initial segment region, or peripheral sensory endings) is a potential regulatory mechanism for neuronal excitability and stimulus encoding.

Blocking of the sodium channel by external Tris in the squid giant axon

The macroscopic current carried by Na + ions was recorded in voltage-clamped squid giant axons that were dialysed with a mixture of CsF and NaF, and bathed in chloride solutions in which the sodium current (1 Na ) was reduced by partly blocking the sodium channels with tetrodotoxin, or by replacing four fifths of the Na + either with choline or with tris buffer at pH 7.3. The permeability coefficient (TNa fast) for the fast-inactivating current was unchanged on substitution of choline for sodium in the bathing solution, but in the high-Tris bathing solution, TNa fagt was reduced in a voltage-dependent manner, so that the permeability relative to normal rose from 0.2 at —40 m V to 0.8 at +100 mV. The coefficie10t TNa non for the non-inactivating current behaved in a similar way, except that the permeability ratio fell between test potentials of —40 and + 10 mV instead of rising. The blocking effect of Tris was unaffected by temperature, but there was some interaction with that of internal tetramethylammonium ions.

Asymmetrical properties of the Na-Ca exchanger in voltage-clamped, internally dialyzed squid axons under symmetrical ionic conditions.

In this work we have investigated whether the asymmetrical properties of the Na/Ca exchange process found in intact preparations are intrinsic to the exchange protein(s) or the result of the asymmetric ionic environment normally prevailing in living cells. The activation of the Na/Ca exchanger by Ca2+ ions, monovalent cations, ATP gamma S and the effect of membrane potential on the different operational modes of the exchanger (Nao/Cai, Cao/Nai, Cao/Cai, and Nao/Nai) was studied in voltage-clamped squid giant axons externally perfused and internally dialyzed with symmetrical ionic solutions. Under these conditions: (a) Ca ions activate with higher affinity from the inside (K1/2 = 22 microM) than from the outside (K1/2 = 300 microM); (b) experiments measuring the Cao-dependent Ca efflux in the conditions Lio-Trisi, Lio-Lii, Triso-Trisi, and Triso-Lii, show that the activating monovalent cation site on the exchanger faces the external surface; (c) ATP gamma S activates the Cao-dependent Ca efflux (Cao/Cai exchange) only at nonsaturating [Ca2+]i. Its effect appears to be on the Ca transport site since no alteration in the apparent affinity of the activating monovalent cation site was observed. The above results show that the Na/Ca exchange process is indeed a highly asymmetric transport mechanism. Finally, the voltage dependence of the components of the different exchange modes was measured over the range of +20 to -40 mV. The voltage dependence (approximately 26% change/25 mV) was found to be similar for all modes of operation of the exchanger except Nao/Nai exchange, which was found to be voltage insensitive. The sensitivity of the Cao/Cai exchange to voltage was found to be the same in the presence and in the complete absence of monovalent cations. This finding does not support the proposition that the voltage sensitivity of the Cao/Cao exchange is induced by the binding and transport of an external monovalent cation.

Stoichiometry and voltage dependence of the sodium pump in voltage-clamped, internally dialyzed squid giant axon.

The stoichiometry and voltage dependence of the Na/K pump were studied in internally dialyzed, voltage-clamped squid giant axons by simultaneously measuring, at various membrane potentials, the changes in Na efflux (delta phi Na) and holding current (delta I) induced by dihydrodigitoxigenin (H2DTG). H2DTG stops the Na/K pump without directly affecting other current pathways: (a) it causes no delta I when the pump lacks Na, K, Mg, or ATP, and (b) ouabain causes no delta I or delta phi Na in the presence of saturating H2DTG. External K (Ko) activates Na efflux with Michaelis-Menten kinetics (Km = 0.45 +/- 0.06 mM [SEM]) in Na-free seawater (SW), but with sigmoid kinetics in approximately 400 mM Na SW (Hill coefficient = 1.53 +/- 0.08, K1/2 = 3.92 +/- 0.29 mM). H2DTG inhibits less strongly (Ki = 6.1 +/- 0.3 microM) in 1 or 10 mM K Na-free SW than in 10 mM K, 390 mM Na SW (1.8 +/- 0.2 microM). Dialysis with 5 mM each ATP, phosphoenolpyruvate, and phosphoarginine reduced Na/Na exchange to at most 2% of the H2DTG-sensitive Na efflux. H2DTG sensitive but nonpump current caused by periaxonal K accumulation upon stopping the pump, was minimized by the K channel blockers 3,4-diaminopyridine (1 mM), tetraethylammonium (approximately 200 mM), and phenylpropyltriethylammonium (20-25 mM) whose adequacy was tested by varying [K]o (0-10 mM) with H2DTG present. Two ancillary clamp circuits suppressed stray current from the axon ends. Current and flux measured from the center pool derive from the same membrane area since, over the voltage range -60 to +20 mV, tetrodotoxin-sensitive current and Na efflux into Na-free SW, under K-free conditions, were equal. The stoichiometry and voltage dependence of pump Na/K exchange were examined at near-saturating [ATP], [K]o and [Na]i in both Na-free and 390 mM Na SW. The H2DTG-sensitive F delta phi Na/delta I ratio (F is Faraday's constant) of paired measurements corrected for membrane area match, was 2.86 +/- 0.09 (n = 8) at 0 mV and 3.05 +/- 0.13 (n = 6) at -60 to -90 mV in Na-free SW, and 2.72 +/- 0.09 (n = 7) at 0 mV and 2.91 +/- 0.21 (n = 4) at -60 mV in 390 mM Na SW. Its overall mean value was 2.87 +/- 0.07 (n = 25), which was not significantly different from the 3.0 expected of a 3 Na/2 K pump.(ABSTRACT TRUNCATED AT 400 WORDS)

Simultaneous measurement of changes in current and tracer flux in voltage-clamped squid giant axon

A method is described for the simultaneous measurement of changes in membrane current and unidirectional radiotracer flux in internally dialyzed voltage-clamped squid giant axons. The small currents that are produced by electrogenic transport processes or steady-state ionic currents can be resolved using this method. Because the use of grounded guard electrodes in the end pools is not, by itself, an adequate means of eliminating end-effects, two ancillary end pool clamp circuits are described to eliminate extraneous current flow from the ends of the axon. The end pool voltage-clamp circuits serve to minimize net current flow between the end pools and center pool, and employ stable, low-impedance calomel electrodes to monitor the potentials of the end and center pools. The adequacy of the method is demonstrated by experiments in which unidirectional 22Na efflux and current, flowing through tetrodotoxin (TTX)-sensitive Na channels into Na-free seawater, under K-free conditions, are shown to be equal. The equality of unidirectional TTX-sensitive flux and current is maintained over the entire range of membrane potentials examined (-60 to +20 mV). The method has been applied to a series of experiments in which the voltage dependence and stoichiometry of the Na/K pump have been measured (Rakowski et al., 1989), and can be applied in general to the simultaneous measurement of changes in current and flux of other electrogenic transport processes, and of currents through ionic channels that open under steady-state conditions.

Effects of arachidonic acid and the other long-chain fatty acids on the membrane currents in the squid giant axon.

The effects of arachidonic acid and some other long-chain fatty acids on the ionic currents of the voltage-clamped squid giant axon were investigated using intracellular application of the test substances. The effects of these acids, which are usually insoluble in solution, were examined by using alpha-cyclodextrin as a solvent, alpha-cyclodextrin itself had no effect on the excitable membrane. Arachidonic acid mainly suppresses the Na current but has little effect on the K current. These effects are completely reversed after washing with control solution. The concentration required to suppress the peak inward current by 50% (ED50) was 0.18 mM, which was 10 times larger than that of medium-chain fatty acids like 2-decenoic acid. The Hill number was 1.5 for arachidonic acid, which is almost the same value as for medium-chain fatty acids. This means that the mechanisms of the inhibition are similar in both long- and medium-chain fatty acids. When the long-chain fatty acids were compared, the efficacy of suppression of Na current was about the same value for arachidonic acid, docosatetraenoic acid and docosahexaenoic acid. The suppression effects of linoleic acid and linolenic acid on Na currents were one-third of that of arachidonic acid. Oleic acid had a small suppression effect and stearic acid had almost no effect on the Na current. The currents were fitted to equations similar to those proposed by Hodgkin and Huxley (Hodgkin, A.L., Huxley, A.F. (1952) J. Physiol (London) 117:500-544) and the change in the parameters of these equations in the presence of fatty acids were calculated.(ABSTRACT TRUNCATED AT 250 WORDS)

Interactions of pyrethroids and octylguanidine with sodium channels of squid giant axons

Kinetics of pyrethroid-modified sodium channels and the interaction of N-octylguanidine with the modified channels have been studied with internally perfused and voltage-clamped squid giant axons. The pyrethroids used were 1R- cis-phenothrin; IR- cis-permethrin; 1R- cis-cyphenothrin; and 1R- cis-deltamethrin. Modification of sodium channels by pyrethroids resulted in marked slowing of opening and closing kinetics. The rate at which sodium channels arrived at the open pyrethroid-modified state during a depolarizing step was independent of the concentration of pyrethroids applied. The time of exposure to pyrethroids required for the pyrethroid-induced sodium tail current following a step depolarization to reach a steady-state amplitude was independent of the frequency of short (5ms) depolarizing pulses, and in the pronase-treated axons was independent of the membrane potential (0 mV or– 90 mV). We conclude that sodium channels are modified by pyrethroids primarily in the closed resting state. A small fraction of sodium channels is modified in the open state. The dose-response curve for N-octylguanidine block of sodium channels was not shifted by pyrethroids. The rate at which the pyrethroid-modified sodium channels were blocked by octylguanidine during a depolarizing step depended neither on the concentration of pyrethroids nor on the depolarizing potential, but depended on the concentration of octylguanidine. The time course of the pyrethroid-induced slow sodium tail current was not altered by octylguanidine. We conclude that the actions of pyrethroids and N-octylguanidine on sodium channels are independent of each other.

Kinetics of activation of the potassium conductance in the squid giant axon

A quantitative re-investigation of the time course of the initial rise of the potassium current in voltage-clamped squid giant axons is described. The n4 law of the Hodgkin-Huxley equations was found to be well obeyed only for the smallest test pulses, and for larger ones a good fit of the inflected rise required use of the expression (1-exp[-t/tau n1])X-1(1-exp[-t/tau n2]), where both of the time constants and the power X varied with the size of the test pulse. Application of a negative prepulse produced a delay in the rise resulting mainly from an increase of X from a value of about 3 at -70 mV to 8 at -250 mV, while tau n1 remained constant and tau n2 was nearly doubled. The process responsible for generating this delay was switched on with a time constant of 8 ms at 4 degrees C, which fell to about 1 ms at 15 degrees C. Analysis of the inward tail currents at the end of a voltage-clamp pulse showed that there was a substantial external accumulation of potassium owing to the restriction of its diffusion out of the Schwann cell space, which, when duly allowed for, roughly doubled the calculated value of the potassium conductance. Computations suggested that the principal effect of such a build-up of [K]o would be to reduce the fitted values of tau n1 and tau n2 to two-thirds or even half their true sizes, while the power X would generally be little changed; but it would not affect the necessity to introduce a second time constant, nor would it invalidate our findings on the effect of negative prepulses.

The mechanisms of sodium current inhibition by benzocaine in the squid giant axon

(1) The effects of benzocaine on the ionic currents in the voltage-clamped squid giant axon have been examined under various conditions; intact axons, axons internally perfused with CsF and axons dialysed with tetraethylammonium ions were used. (2) Both the steady state outward (potassium) current and the early transient (sodium) current were reduced by ca. 50% by benzocaine (1 mM). (3) Plots of the changes produced by benzocaine (1 mM) in the Hodgkin-Huxley parameters for the steady state activation (m infinity), the steady state inactivation (h infinity) and the time constants (tau m and tau h) for activation and inactivation of the sodium current are shown. The m infinity and h infinity curves are shifted in positive and negative directions respectively on the voltage axis. The time constants are not greatly affected. (4) In axons in which the sodium current inactivation had been largely removed by treatment with chloramine T, the sodium current was still reduced by ca. 50% by 1 mM benzocaine and the positive shift in activation remained unchanged. (5) The dependence on benzocaine concentration (for less than or equal to 2 mM) of the peak sodium current reduction and the shift in steady state inactivation have been determined. (6) It is concluded that in the squid axon the effects on inactivation are not the main reason for the reduction of the sodium current by benzocaine and that, in common with many other neutral anaesthetics, there are at least two sites at which benzocaine acts.

Local anaesthetic effects of benzene and structurally related molecules, including benzocaine, on the squid giant axon

(1). The effects of benzene and several of its derivatives on sodium currents in the voltage-clamped squid giant axon have been studied. Substances tested were benzene, aniline, benzyl alcohol, propiophenone, 4-amino-propiophenone, methyl benzoate, ethyl benzoate, and 4-amino ethyl benzoate (benzocaine). (2.) All substances tested reduced the sodium current in both intact axons and axons internally perfused with CsF. (3.) There were four major actions of benzene on the sodium current: (a) an increase in the resting level of inactivation, (b) an increase in the depolarization required to produce the maximum current, (c) a decrease in the maximum sodium conductance, and (d) an increase in the rate of inactivation. (4.) 4-amino ethyl benzoate (benzocaine) had actions on the sodium current which were very similar to those of benzene with the exception that the rate of inactivation was scarcely affected and, at comparable shifts, the slope of the steady state inactivation curve was slightly smaller. (5.) The results obtained with the substances structurally intermediate between benzene and 4-amino ethyl benzoate allow some conclusions to be drawn as to the role of each functional group.

The actions of halogenated ethers on the ionic currents of the squid giant axon

The effects of fourteen halogenated ethers on the sodium and potassium currents of voltage-clamped squid giant axons have been examined. Effects under open-circuit were also studied. In voltage-clamped axons, the ethers tended to reduce potassium currents at least as much, if not more, than sodium currents. This finding distinguishes the halogenated ethers from many other general anaesthetics. Certain, but not all, halogenated ethers induced a pronounced maximum in potassium current traces as a function of time. This property can be formally described if an inactivation term is added to the Hodgkin-Huxley equation for potassium currents. Large shifts in the sodium-current inactivation parameter h infinity were produced in some instances. Two fully halogenated methyl ethyl ethers, known to produce convulsions in mice, depressed both sodium and potassium currents, but with a very slow time course of action. The electrophysiological effects of the halogenated ethers investigated appear to depend on the position and number of hydrogen bonds that can be formed.

Nerve membrane sodium channels as the target site of brevetoxins at neuromuscular junctions

Actions of two structurally related toxins, T-17 and brevetoxin-B, isolated from the red-tide dinoflagellate, Ptychodiscus brevis, were studied on the giant axon of the squid and the neuromuscular junctions of the frog and rat. T-17 toxin caused a large increase in the frequency of miniature endplate potentials at nanomolar concentrations. In one typical case with a frog endplate, the frequency increased from 1.9 s-1 before application of 3.5 nM T-17 to 69.3 s-1 within 5 min after application. In the rat muscle, the mean frequency increased from 1.39 s-1 in control to 11.93 s-1 after application of 23.2 nM T-17. The increase in miniature endplate potential frequency was reversed by the addition of 1 microM tetrodotoxin, and was not observed in a solution containing elevated Mg2+ and reduced Ca2+ concentrations. External or internal application of T-17 toxin (2-5 microM) or brevetoxin-B (10-30 microM) to intact or internally perfused squid axons caused a depolarization of the membrane. This depolarization was abolished by the removal of external Na+ or by addition of tetrodotoxin to the external solution. In voltage clamped squid giant axons, exposure to T-17 toxin or brevetoxin-B increased the non-inactivating component of the tetrodotoxin-sensitive sodium current. The sodium current was activated at potentials 15 to 40 mV more negative than control. It is proposed that these toxins modify a fraction of the sodium channels to a form which opens at potentials more negative than normal and which inactivates to a lesser extent. This mechanism would predict a depolarization of the nerve membrane at the neuromuscular junction, thus explaining the increased discharge of transmitter.

Modulation of aminopyridine block of potassium currents in squid axon

Aminopyridines are known to block potassium (K) currents in excitable membranes in a manner dependent upon membrane potential, such that the block is relieved by depolarization and restored upon repolarization. In the present study, the effects of aminopyridines on voltage-dependent potassium (K) channels were examined in internally perfused, voltage-clamped squid giant axons. The time course of block restoration after conditioning depolarization was found to be modulated by membrane electric field, K-channel gating, and external cations. Depolarized holding potentials accelerated block restoration without altering steady-state block levels, suggesting that the voltage dependence of block restoration may be related to K channel gating rather than drug binding per se. In support of this notion, low external calcium concentration, which shifts the voltage dependence of K-channel gating to more negative potentials, also accelerated block restoration. Conversely, the relationship between the rate of block restoration and membrane holding potential was shifted in the depolarizing direction by phloretin, an agent that shifts the dependence of K-channel opening on membrane potential in a similar manner. Modification of K-channel gating also was found to alter the rate of block restoration. Addition of internal zinc or internal treatment with glutaraldehyde slowed the time course of both K-channel activation and aminopyridine block restoration. Aminopyridines also were found to interact in the K channel with external Cs+, NH4+, and Rb+, each of which slowed aminopyridine block restoration. Our results suggest that aminopyridines enter and occlude K channels, and that the availability of the binding site may be modulated by channel gating such that access is limited by the probability of the channel reaching an intermediate closed state at the resting potential.

The pH dependence of the tetrodotoxin-blockade of the sodium channel and implications for toxin binding

On the internally perfused, voltage-clamped squid giant axon, the effect of pH on the potency of tetrodotoxin in blocking the sodium current has been re-examined at pH 7.8 and 8.8. Confirming previous studies, tetrodotoxin is weaker at pH 8.8, when the deprotonated C-10 -OH makes the toxin molecule a zwitterion. In contrast to previous studies, our results, based on full dose-response relations, show that the relative potency at the two pH values appreciably exceeds the ratio of the abundance of the protonated C-10 form. In a medium of lowered ionic strength, tetrodotoxin is weaker, and the relative potency at pH 7.8 and 8.8 approaches the ratio of the relative abundance of the C-10 -OH. The results are believed to support hydrogen bonding at C-10 as a contributing factor in the binding of tetrodotoxin to the membrane receptor.

Interactions of permeant cations with sodium channels of squid axon membranes

To determine how the permeant cations interact with the sodium channel, the instantaneous current-voltage (I-V) relationship, conductance-ion concentration relationship, and cation selectivity of sodium channels were studied with internally perfused, voltage clamped squid giant axons in the presence of different permeant cations in the external solution. In Na-containing media, the instantaneous I-V curve was almost linear between +60 and -20 mV, but deviated from the linearity in the direction to decrease the current at more negative potentials. The linearity of instantaneous I-V curve extended to more negative potentials with lowering the external Ca concentration. The I-V curve in Li solution was almost the same as that in Na solution. The linearity of the I-V curve improved in NH4 solution exhibiting only saturation at -100 mV with no sign of further decrease in current at more negative potentials. Guanidine and formamidine further linearized the instantaneous I-V curve. The conductance of the sodium channels as measured from the tail current saturated at high concentrations of permeant cations. The apparent dissociation constants determined from the conductance-ion concentration curve at -60 mV were as follows: Na, 378 mM; Li, 247 mM; NH4, 174 mM; guanidine, 111 mM; formamidine, 103 mM. The ratio of the test cation permeability to the sodium permeability as measured from the reversal potentials of tail currents varied with the test cation concentration and/or the membrane potential. These observations are incompatible with the independence principle, and can be explained on the basis of the Eyring's rate theory. It is suggested that the slope of the instantaneous I-V curve is determined by the relative affinity of permeant cations and blocking ions (Ca) for the binding site in the sodium channel. The ionic selectivity of the channel depends on the energy barrier profile of the channel.

Further evidence that membrane thickness influences voltage-gated sodium channels

The short-chain phospholipid, diheptanoyl phosphatidylcholine, at 520 microM, reduced the maximum inward sodium current in voltage-clamped squid giant axons by greater than 50%. Analysis of these currents by means of the Hodgkin-Huxley equations showed this reduction to be mainly the result of a large depolarizing shift in the voltage dependence of the steady state activation parameter, m infinity. The voltage dependence of the steady state inactivation parameter, h infinity, was also moved in the depolarizing direction and the axonal membrane capacitance per unit area measured at 100 kHz was increased. A longer chain length derivative, didecanoyl phosphatidylcholine, had no significant effect on the axonal sodium current at concentrations of 3.7 and 18.5 microM. Dioctanoyl phosphatidylcholine was intermediate in its effects, 200 microM producing approximately the same current suppression as 520 microM diheptanoyl phosphatidylcholine, together with depolarizing shifts in m infinity and h infinity. These effects may be contrasted with those of the normal and cyclic alkanes (1-3), which tend to move both m infinity and h infinity in the hyperpolarizing direction and to reduce the capacitance per unit area at 100 kHz. The above results are all consistent with the hypothesis that small hydrocarbons thicken, while short-chain phospholipids thin, the axonal membrane. Thus membrane thickness changes may be of considerable importance in determining the behavior of the voltage-gated sodium channel.