Depolarization of the neuronal membrane caused by Co-transport of taurine and sodium

C 1300 neuroblastoma cells were cultured and used to study the effect of sodium dependent taurine transport on the membrane potential. Measuring net accumulation of taurine and the depolarization caused by externally applied taurine, we found both processes become active at an external concentration of taurine of 1 mM or more. Net accumulation had K_m of 13 mM and a V_max of 126 nmol × mg of protein^–1×min^–1. The taurine induced depolarization of the neuroblastoma cell was parallelled by a 25 per cent decrease in its membrane impedance. The transport of taurine, the depolarization caused by taurine and the effect of taurine on the membrane impedance, all, had a similar dependence on the external sodium concentration. Our results on the depolarizing cotransport between taurine and sodium at the neuronal membrane, may illustrate an additional mechanism for the control of the electrical activity of neuronal cells.     

Measurement of membrane potential in polymorphonuclear leukocytes and its changes during surface stimulation

The membrane potential of guinea pig polymorphonuclear leukocytes has been assessed with two indirect probes, tetraphenylphosphonium (TPP⁺) and 3,3′-dipropylthiadicarbocyanine (diS-C₃-(5)). The change in TPP⁺ concentration in the medium was measured with a TPP⁺-selective electrode. By monitoring differences in accumulation of TPP⁺ in media containing low and high potassium concentrations, a resting potential of −58.3 mV was calculated. This potential is composed of a diffusion potential due to the gradient of potassium, established by the Na⁺, K⁺ pump, and an electrogenic potential. The chemotactic peptide fMet-Leu-Phe elicits a rapid efflux of accumulated TPP⁺ (indicative of depolarization) followed by its reaccumulation (indicative of repolarization). In contrast, stimulation with concanavalin A results in a rapid and sustained depolarization without a subsequent repolarization. The results obtained with TPP⁺ and diS-C₃-(5) were comparable. Such changes in membrane potential were observed in the absence of extracellular sodium, indicating that an inward movement of sodium is not responsible for the depolarization. Increasing potassium levels, which lead to membrane depolarization, had no effect on the oxidative metabolism in nonstimulated or in fMet-Leu-Phe-stimulated cells. Therefore, it seems unlikely that membrane depolarization per se is the immediate stimulus for the respiratory burst.     

The Initiation of Spike Potential in Barnacle Muscle Fibers under Low Intracellular Ca++

Electrical properties of the muscle fiber membrane were studied in the barnacle, Balanus nubilus Darw. by using intracellular electrode techniques. A depolarization of the membrane does not usually produce an all-or-none spike potential in the normal muscle fiber even though a mechanical response is elicited. The intracellular injection of Ca⁺⁺-binding agents (K₂SO₄ and K salt of EDTA solution, K₃ citrate solution, etc.) renders the fiber capable of initiating all-or-none spikes. The overshoot of such a spike potential increases with increasing external Ca concentration, the increment for a tenfold increase in Ca concentration being about 29 mv. The threshold membrane potential for the spike and also for the K conductance increase shifts to more positive membrane potentials with increasing [Ca⁺⁺]_out. The removal of Na ions from the external medium does not change the configuration of the spike potential. In the absence of Ca⁺⁺ in the external medium, the spike potential is restored by Ba⁺⁺ and Sr⁺⁺ but not by Mg⁺⁺. The overshoot of the spike potential increases with increasing [Ba⁺⁺]_out or [Sr⁺⁺]_out. The Ca influx through the membrane of the fiber treated with K₂SO₄ and EDTA was examined with Ca⁴⁵. The influx was 14 pmol per sec. per cm² for the resting membrane and 35 to 85 pmol per cm² for one spike. From these results it is concluded that the spike potential of the barnacle muscle fiber results from the permeability increase of the membrane to Ca⁺⁺ (Ba⁺⁺ or Sr⁺⁺).     

Effect of Ethanol on the Sodium and Potassium Conductances of the Squid Axon Membrane

The effects of ethanol on squid giant axons were studied by means of the sucrose-gap technique. The membrane action potential height is moderately reduced and the duration sometimes shortened by ethanol in sea water. Voltage clamp experiments showed that ethanol in sea water reduced the maximum membrane conductances for sodium (g'_Na) and potassium (g'_K). In experiments with multiple application of ethyl alcohol to the same spot of membrane, a reduction of g'_Na to 82 per cent and of g'_K to 80 per cent of their value in sea water was brought about by 3 per cent ethanol (by volume) while 6 per cent caused a decrease of g'_Na to 59 per cent and of g'_K to 69 per cent. Ethanol has no significant effect on the steady-state inactivation of g_Na (as a function of conditioning membrane potential) or on such kinetic parameters as τ_h or the time course of turning on gi g_Na and g_K. It is concluded that ethanol mainly reduces g_Na and g_K in the Hodgkin-Huxley terminology.     

Quinidine blocking of sodium and potassium channels in myelinated nerve fibers

Experiments by the voltage clamp method showed that external application of quinidine (5 × 10^–5 M) to the Ranvier node membrane of the frog nerve fiber inhibitis both sodium and potassium currents. Blocking of the sodium current is considerably intensified by repetitive depolarization of the membrane (1–10 Hz); the rate of development of the block increases with an increase in stimulation frequency. After the end of stimulation the sodium current gradually returns to its initial level (with a time constant of the order of 30 sec at 12°C). Unlike repetitive depolarization with short (5 msec) stimuli, a prolonged shift (1 sec) of potential toward depolarization has no significant effect on quinidine blocking of the sodium current. Analysis of the current-voltage characteristic curves showed that quinidine blocks outward sodium current more strongly than inward. Batrachotoxin protects sodium channels against the blocking action of quinidine in a concentration of 10^–5 M. Inhibition of the outward potassium currents by quinidine is distinctly time-dependent in character: Initially the potassium current rises to a maximum, then falls steadily to a new stationary level. The results agree with the view that quinidine, applied externally, penetrates through the membrane in the basic form and blocks open sodium and potassium channels from within in the charged (protonated) form. The similarity in principle between the action of quinidine and local anesthetics on the sodium suggests that these compounds bind with the same receptor, located in the inner mouth of the sodium channel.A. V. Vishnevskii Institute of Surgery, Academy of Medical Sciences of the USSR, Moscow. Translated from Neirofiziologiya, Vol. 14, No. 3, pp. 324–330, May–June, 1982.     

Early changes in membrane potential of Saccharomyces cerevisiae induced by varying extracellular K+, Na+ or H+ concentrations

Recently we introduced a fluorescent probe technique that makes possible to convert changes of equilibrium fluorescence spectra of 3,3’-dipropylthiadicarbocyanine, diS-C₃(3), measured in yeast cell suspensions under defined conditions into underlying membrane potential differences, scaled in millivolts (Plasek et al. in J Bioenerg Biomembr 44: 559–569, 2012). The results presented in this paper disclose measurements of real early changes of plasma membrane potential induced by the increase of extracellular K⁺, Na⁺ and H⁺ concentration in S. cerevisiae with and without added glucose as energy source. Whereas the wild type and the ?tok1 mutant cells exhibited similar depolarization curves, mutant cells lacking the two Trk1,2 potassium transporters revealed a significantly decreased membrane depolarization by K⁺, particularly at lower extracellular potassium concentration [K⁺]_out. In the absence of external energy source plasma membrane depolarization by K⁺ was almost linear. In the presence of glucose the depolarization curves exhibited an exponential character with increasing [K⁺]_out. The plasma membrane depolarization by Na⁺ was independent from the presence of Trk1,2 transporters. Contrary to K⁺, Na⁺ depolarized the plasma membrane stronger in the presence of glucose than in its absence. The pH induced depolarization exhibited a fairly linear relationship between the membrane potential and the pH_o of cell suspensions, both in the wild type and the Δtrk1,2 mutant strains, when cells were energized by glucose. In the absence of glucose the depolarization curves showed a biphasic character with enhanced depolarization at lower pH_o values.     

p-CMBS Modifies Extrafacial Sulfhydryl Groups at the Chara Plasma Membrane: Activation of Ca2+ Influx and Inhibition of Two Different K+ Currents

The effect of the membrane impermeant sulfhydryl group (SH) reagent, p-chloromercuribenzenesulfonic acid (p-CMBS), on electrical membrane transport properties of the giant alga, Chara corallina, was determined. In an external medium with a high K⁺ concentration (5 mM) cells typically exhibited stable membrane potentials close to the K⁺equilibrium potential. The steady-state current-voltage (I-V) relation could be dissected into two distinct components: an almost linear ohmic leak current and a voltage-dependent K⁺ current. Adding 0.5 mM p-CMBS to the external medium resulted in an immediate, short depolarization transient (resembling the time course of an action potential) and was associated with a slow down of the cytoplasmic streaming velocity. The depolarization, as well as the streaming inhibition, could be abolished by pretreating cells with the Ca²⁺ channel inhibitor, LaCl₃. This suggests that the depolarization transient reflected a p-CMBS induced Ca²⁺ influx, a scenario known to trigger membrane excitation and slow down of cytoplasmic streaming. From the I-V analysis it appeared that p-CMBS also caused a reversible inhibition of two additional transmembrane currents: (1) a reduction of a leak current and (2) a modification of the deactivation kinetics of the voltage-dependent K⁺ channels. From the I-V difference analysis, the inhibited leak current was identified as a K⁺ current, because the reversal potential was close to the estimated K⁺ equilibrium potential. Control experiments have furthermore shown that the mercapto reagent, dithiothreitol, partly reversed the effect of p-CMBS. This strengthens the view that the action of the mercurial is related to a specific and direct modification of SH groups. The p-CMBS-evoked inhibition of K⁺ currents was not abolished by the LaCl₃ pretreatment, which suggests that the effect of the SH reagent is not induced indirectly by p-CMBS-triggered Ca²⁺ influx. Therefore, it is suggested that the mercurial interacts direcly with the K⁺ transport protein.     

Effects of External Calcium Deprivation on Single Muscle Fibers

Deprivation of external calcium causes sudden potentiation of the twitch response of single muscle fibers. The potentiation was 64 ± 8%. Potentiation is simultaneous with membrane depolarization occurring after Ca⁺⁺ removal. This depolarization amounted to 9 ± 2 mv. Ca⁺⁺ removal also alters the action potential. 3 min after calcium withdrawal, action potential amplitude fell by 36 ± 3 mv; maximum rates of rise and fall of the spike decreased by 55 ± 5 and 63 ± 5% respectively. Changes in shape of the A. P. differ from those seen with other potentiators of the twitch response, such as Zn⁺⁺. After short exposure to calcium-free media, potassium-induced contractures show potentiation of peak tension. The S-shaped curve relating potassium contracture tension to log [K]_o shifts to the left after such treatment. Calcium deprivation also increased the rate of relaxation of the contractures. This effect depends on the duration of calcium deprivation, and is probably related to the effect of calcium lack on the membrane. The change in relaxation occurred immediately after calcium deprivation, and was reversed by sudden readmission of calcium. Relaxation of twitch and tetanus responses also were affected by Ca lack, but not as rapidly as potassium contractures. The results suggest that external calcium is not directly involved in the process responsible for tension development, supporting the view that this process is mediated by translocation of intracellular calcium. The relaxation process, however, appears to be rapidly affected by deprivation of external calcium.     

Resting potential of the mouse neuroblastoma cells: II. Significant contribution of the surface potential to the resting potential of the cells under physiological conditions

In the previous paper, we showed that the K⁺ channels of the mouse neuroblastoma cell (clone N-18) are closed at low concentration of external K⁺ ([K⁺]₀) including the physiological concentration for the cells. In the present study, the origin of the resting membrane potential of N-18 cells has been examined. (1) The resting membrane potential of N-18 cells was depolarized by increasing concentration of the polyvalent cations (La³⁺, Fe³⁺, Co²⁺, Ca²⁺, Sr²⁺, Mg²⁺) and by decreasing the pH of the medium. The input membrane resistance was slightly increased during the depolarization. The depolarization was not explained in terms of the diffusion of the cations across the membrane, since the trivalent cations of greater ionic size were effective at much lower concentrations than the divalent cations. The results obtained from the measurements of ⁸⁶Rb efflux suggested that the depolarization cannot be explained in terms of blocking of the K⁺ channels by the cations. (2) An increase in Ca²⁺ concentration from 0.3 to 1.8 mM induced depolarization of about 10 mV at low [K⁺]₀ where the K⁺ channels are closed, but did not induce any depolarization at high [K⁺]₀ where the channels are open. (3) In order to estimate the changes in the zeta-potential, the electrophoretic mobility of N-18 cells was measured under various conditions. There was a close correlation between the changes in the zeta-potential and those in the membrane potential in response to the polyvalent cations and proton. On the other hand, an increase in K⁺-concentration in the medium, which induced a large depolarization in the cells, did not affect the zeta-potential. (4) The results obtained were explained by an electrical circuit model for the membranes of N-18 cells. In this model, an electrical circuit for the membrane part carrying no selective ionic channels, in which changes in the surface potential directly affect the transmembrane potential, is connected in parallel to the usual circuit model representing selective ionic channel systems. It was concluded that the surface potential contributes significantly to the resting membrane potential of N-18 cells at low [K⁺]₀ where the K⁺ channels are closed.     

Latrunculin A depolarizes starfish oocytes

Depolymerization of the actin cytoskeleton may liberate Ca²⁺ from InsP₃-sensitive stores in some cell types, including starfish oocytes, while inhibiting Ca²⁺ influx in others. However, no information is available on the modulation of membrane potential (V_m) by actin. The present study was aimed to ascertain whether the widely employed actin depolymerizing drug, latrunculin A (Lat A), affects V_m in mature oocytes of the starfish Astropecten aranciacus. Lat A induced a membrane depolarization which was mimicked by cytochalasin D, another popular actin disruptor, and prevented by jasplakinolide, a stabilizer of the actin network. Lat A-elicited depolarization consisted in a positive shift in V_m which reached the threshold of activation of voltage-gated Ca²⁺ channels (VGCC), thus triggering an action potential. Lat A-promoted depolarization lacked the action potential in Ca²⁺-free sea water, while it was abolished upon removal of external Na⁺. Moreover, membrane depolarization was prevented by pre-injection of BAPTA and heparin, but not ryanodine. These data indicate that Lat A induces a membrane depolarization by releasing Ca²⁺ from InsP₃Rs. The Ca²⁺ signal in turn activates a Ca²⁺-dependent Na⁺ entry, which causes the positive shift in V_m and stimulates the VGCC.     

Electrophysiological and pharmacological properties of cultured rat thyroid cells

The electrophysiological properties of a hormone-dependent, differentiated thyroid epithelial cell strain were studied using intracellular microelectrodes. The average membrane potential of solitary, isolated cells was –78.4 ± 1.3 mV. The membrane potential depolarized 55 mV per tenfold increase in extracellular potassium concentation. Weak electrical coupling was recorded between contiguous cells. Like tyroid cells in vivo, these cells did not generate action potentials. In some cells a spontaneous, slow transition in the membrane potential from –80mV to –30 mV was accompanied by an increase in input resistance. Membrane potential transitions could be induced by perfusing cells with isotonic Hanks solutions saturated with CO₂ (pH = 5.5) or by perfusing cells with hypotonic Hanks solutions (190–290 mOsm/kg). Membrane potential transitions were due to a decreased potassium permeability. Noradrenaline elicted both a fast depolarization and a slow depolarization. The fast depolarization was due to an increase in conductance of Na⁺ channels and of Cl^– channels. Intracellular injection of Ca⁺⁺ elicited the fast depolarization. Intracellular injection of EGTA or cobalt abolished the fast depolarization. Replacemnt of extracellular Ca⁺⁺ by Mg⁺⁺ did not affect the fast depolarization. Thus, the fast depolarization was due to accumulation of intracellular Ca⁺⁺. The fast depolarization was abolished by the alpha adrenergic blocker phentolamine (10^–6 M), and was not abolished by the beta adrenergic blocker propranolol (10^–5 M).     

Some electrophysiological consequences of electrogenic sodium and potassium transport in cardiac muscle: a theoretical study

A previous paper described a kinetic model for electrogenic sodium-potassium transport in cardiac muscle, combining a thermodynamically-constrained transport model with simple passive permeabilities for sodium and potassium to generate a cardiac action potential (Chapman, Kootsey & Johnson, 1979). The present paper explores the extent to which this simplest of active-passive transport models can account (without further modification) for the electrophysiological behavior of cardiac muscle. The long term (several minutes) changes in the duration of the action potential observed following a change in stimulation rate are predicted by the model through a shift in the steady-state current-voltage relationship caused by small changes in inside ion concentrations. The diastolic hyperpolarization observed following an increase in rate is also predicted, including the linear relationship between the maximum diastolic depolarization and the rate of stimulation. Varying the outside potassium concentration in the model produces changes in the rest potential and current-voltage relationship similar to published data. Deviations from ideal potassium electrode behavior occur at both high and low concentrations because of effects on the pump. The model not only predicts the observed shift of the current-voltage curve in the depolarizing direction with increasing [K⁺]₀, but also the crossing of the curve in normal [K ⁺]₀ without having to assume a variation in g_K. Anoxia was introduced into the model by changing the concentrations of ATP and ADP, thereby enabling the model to account for the rapid diastolic depolarization observed in myocardial ischemia.     

Papaverine reduces the sodium permeability of the apical membrane and the Potassium permeability of the basolateral membrane in isolated frog skin

Summary The effect of papaverine, an inhibitor of the phosphodiesterase responsible for breakdown of cAMP, on the transepithelial sodium transport across the isolated frog skin was investigated.Serosal addition of papaverine caused initially an increase in the short-circuit current (SCC), a doubling of the cellular cAMP content and a depolarization of the intracellular potential under SCC conditions (V _scc).The initial increase in the SCC was followed by a pronounced decrease both in the SCC and in the natriferic action of antidiuretic hormone (ADH), but papaverine had no inhibitory effect on the ability of ADH to increase the cellular cAMP content. As SCC declines, no hyperpolarization was observed.The I/V relationship across the apical membrane during the inhibitory phase, revealed that papaverine reduces the sodium permeability of the apical membrane (P _Na ^a )as well as intracellular sodium concentration. These observations and the previously noted effect of papaverine on V _scc indicates that papaverine must have an effect on the cellular Cl or K permeability.The basolateral Na,K,2Cl cotransporter was blocked with bumetanide, which should bring the cellular chloride in equilibrium. Bumetanide had no effect on basal SCC and V _scc. When papaverine was added to skins preincubated with bumetanide, the effect of papaverine on SCC and V _scc was unchanged. Therefore, the depolarization of V _scc, observed during the papaverine induced inhibition of the SCC, must be due to a reduction in the cellular K permeability.In conclusion, it is suggested that papaverine reduces the sodium permeability of the apical membrane and the potassium permeability of the basolateral membrane of the frog skin epithelium.     

Evidence for amino Acid-h co-transport in oat coleoptiles

Microelectrode and tracer techniques were used to test for possible amino acid-H⁺ co-transport in coleoptiles of Avena sativa L. cv. “Garry.” The amino acid analogue α-aminoisobutyric acid (AIB) caused transient depolarization of the membrane potential. The absolute magnitude of the maximum depolarization was affected by the same factors that affected AIB transport. Both increased with higher concentrations of AIB, increased with higher acidities in the medium, and were enhanced by indoleacetic acid (which hyperpolarized the membrane potential). AIB transport was reduced as K⁺ concentrations in the medium were increased and by the metabolic inhibitor NaN₃, both of which reduce membrane potentials. Our data fit an amino acid-H⁺ co-transport model in which transport is controlled by both the membrane potential and proton concentration components of the chemical potential difference of protons across the coleoptile cell membrane.     

Membrane potentials of BHK (baby hamster kidney) cell line: ionic and metabolic determinants

The transmembrane potential of cells from a continuous cell line (BHK-21) has been investigated by a combination of electrophysiological and flame photometric techniques. The ratio of sodium permeability to potassium permeability (P_Na/P_K) determined from membrane potentials recorded at varying external potassium concentrations was 0.082; from membrane potential measurements and the intracellular sodium and potassium concentrations of cells in 6.8 mM K⁺ media the value was 0.075. The P_Na/P_K ratio was not temperature dependent. Dinitrophenol (1 mM) did not significantly alter the membrane potential of cells incubated for one hour with the inhibitor. However, iodoacetate (1 mM) and sodium fluoride (30 mM) caused a significant depolarization during a one-hour incubation. Measurements of sodium and potassium concentrations during incubation at 4°C showed a decrease in internal potassium and an increase in internal sodium accompanied by a decreased membrane potential. Ion concentrations and membrane potentials were measured in cells recovering at 37°C following 24 hours at 4°C. Membrane potentials in excess of E_K during the first ten minutes of recovery may indicate electrogenic pumping.     

Evidence for cotransport of nitrate and protons in maize roots : I. Effects of nitrate on the membrane potential

The electrical response of nitrate-grown maize (Zea mays L.) roots to 0.1 millimolar nitrate was comprised of two sequential parts: a rapid and transient depolarization of the membrane potential, followed by a slower, net hyperpolarization to a value more negative than the original resting potential. The magnitude of the response was smaller in roots of seedlings grown in the absence of nitrate, but, within 3 hours of initial exposure to 0.1 millimolar nitrate, increased to that of nitrate-grown roots. Chloride elicited a separate electrical response with a pattern similar to that of the nitrate response. However, the results presented in this study strongly indicate that the electrical response to nitrate reflects the activity of a nitrate-inducible membrane transport system for nitrate which is distinct from that for chloride. Inhibitors of the plasmalemma H⁺-ATPase (vanadate, diethylstilbestrol) completely inhibited both parts of the electrical response to nitrate, as did alkaline external pH. The magnitude of the initial nitrate-dependent, membrane potential depolarization was independent of nitrate concentration, but the subsequent nitrate-dependent hyperpolarization showed saturable dependence with an apparent K_m of 0.05 millimolar. These results support a model for nitrate uptake in maize roots which includes a depolarizing NO₃⁻/H⁺ symport. The model proposes that the nitrate-dependent membrane potential hyperpolarization is due to the plasma membrane proton pump, which is secondarily stimulated by the operation of the NO₃⁻/H⁺ symport.     

A study of the crustacean axon repetitive response. 3. A comparison of the effect of veratrine sulfate solution and potassium-rich solutions

The crustacean single nerve fiber gives rise to trains of impulses during a prolonged depolarizing stimulus. It is well known that the alkaloid veratrine itself causes a prolonged depolarization; and consequently it was of interest to investigate the effect of this chemically produced depolarization on repetitive firing in the single axon and compare it with the effect of depolarization by an applied stimulating current or by a potassium-rich solution. It was found that veratrine depolarization, though similar in some respects to a potassium-rich depolarization of depolarizing current effect, was in many respects quite different. (1) At low veratrine concentration, less than 1 Mg%, the negative after potential following a spike action potential was prolonged and augmented. At higher concentrations or after a long period of time, veratrine caused a prolonged steady state depolarization of the membrane, the “veratrine response”. The prolonged plateau depolarization response could be elicited with or without an action potential spike by a short or long duration stimulating pulse, but only if the veratrine depolarization was prevented or offset by an applied conditioning hyperpolarizing inward current. (2) The “veratrine response” resembled the potassium-rich solution response in the plateau-like contour of the depolarization and the very low membrane resistance during this plateau phase. Like the potassium response, it was possible to obtain a typical hyperpolarizing response with an inwardly directed current pulse if applied during the plateau phase. During the negative after potential augmented with veratrine, however, this hyperpolarizing response was not observed. (3) In contrast to the potassium response, however, the “veratrine response” is intimately associated with the sodium concentration in the external medium. The depolarization in millivolts is linearly related to the log of the concentration of external sodium. Moreover, during veratrine action there is a continuous and progressive inactivation of the sodium mechanism which ultimately terminates repetitive firing and abolishes the spike action potential. Then even with conditioning hyperpolarization only the slow response may be elicited in veratrine, occasionally with a spike superimposed if sodium is present, but without repetitive firing. (4) It is concluded that veratrine action is the result of a chemical or metabolic reaction by the alkaloid in the membrane. It is suggested that veratrine may inhibit the sodium extrusion mechanism, or may itself compete for sites in the membrane with calcium and/or sodium. This explains the inhibiting effect of high calcium, the abolition of the “veratrine response” with low temperature and high calcium combined and the progressive inactivation of the sodium system.     

Effects of Sodium Azide on Sodium Fluxes in Frog Striated Muscle

Unidirectional Na fluxes from frog''s striated muscle were measured in the presence of 0 to 5 mM sodium azide. With azide concentrations of 2 and 5 mM the Na efflux was markedly stimulated; the Na efflux with 5 mM azide was about 300 per cent greater than normal. A similar increase was present when all but the 5.0 mM sodium added with azide was replaced by choline. 10^-5 M strophanthidin abolished the azide effect on Na²⁴ efflux. Concentrations of azide of 1.0 mM or less had no effect on Na efflux. The Na influx, on the other hand, was only increased by 41 per cent in the presence of 5 mM NaN₃. From these findings it is concluded that the active transport of Na is stimulated by the higher concentrations of azide. The hypothesis is advanced that the active transport of Na is controlled by the transmembrane potential and that the stimulation of Na efflux is produced as a consequence of the membrane depolarization caused by the azide.     

The ionic basis of the resting potential of molluscan unstriated muscle

Summary The membrane potential (Vm) of unstriated, non-spiking fibres from the buccal retractor muscle of the opisthobranch molluscPhiline aperta is primarily determined by the distribution of the potassium ion across the membrane. In salines where potassium is varied and chloride remains constant or nearly so, the membrane potential varied with log external K⁺ with a slope of 50.6 (±2.3) mV per decade. In chloride-free salines the slope was 48.5 mV per decade. The experiments were conducted at temperatures of 18–20° C.A ten-fold reduction in external chloride concentration depolarised the fibres by around 10 mV, indicating that chloride permeability makes some contribution to Vm. In salines where [K]₀·[Cl]₀ is constant the Nernst slope was 55.8 mV per decade compared with the theoretical value of 58 mV.The experimental data suggest that the internal potassium concentration of the fibres is 247±31 mM and pNa/pK is 0.01, giving a predicted value of Vm in sea water of –72 mV. The membrane potential of 90 fibres measured in sea water was –74.2±1.3 mV. The membrane contains an electrogenic sodium pump which contributes 4–5 mV to the membrane potential.