Effect of various ionic compositions upon the membrane potentials during activation of sea urchin eggs

The membrane potentials of sea urchin (Hemicentrotus pulcherrimus) eggs before and after fertilization and their changes during the membrane elevation induced by intracellular electrical stimulation were recorded in solutions of various ionic compositions. Upon fertilization, the membrane potential (?10 mV) depolarized and reversed polarity by a few mV, then gradually returned to a new steady level ranging between ?50 and ?60 mV. The activation potential is closely associated with a transient increase in the membrane permeability. The potential of the unfertilized egg is hyperpolarized by monovalent anions (Br^?, Cl^? and NO₃^?) and depolarized slightly by K⁺. In contrast, the membrane of the fertilized egg is markedly depolarized by K⁺. Suppression of depolarization associated with an increase of the membrane permeability was recorded in Na-free medium (Tris-HCl). The selective increase in permeability to monovalent anions is thought to alternate with the selective increase in permeability to K⁺through the mediation of a transient increase of Na⁺-permeability at the time of fertilization. No causal relationship between the membrane elevation and the depolarization was established because the breakdown of the cortical granules occurs without depolarization or an increase in membrane permeability.     

The second component of the fertilization potential in sea urchin (Pseudocentrotus depressus) eggs involves both Na+ and K+ permeability

The fertilization potential of the Pseudocentrotus depressus egg involved three transiently depolarizing components which had a different time course and a peak value. Three peaks were at less than 10 sec, 43 ± 4 sec (mean ± SD), and 182 ± 22 sec after the onset of the fertilization potential. Their peak values (mean ± SD) were 37 ± 4, 17 ± 3, and −31 ± 5 mV in standard artificial sea water. The effect of external ions on the membrane potential at the peak of the second component was measured with a conventional voltage-recording microelectrode. The peak value changed 51 mV with a 10-fold change in external Na⁺ concentration. However, it was about 65 mV more negative than the equilibrium potential of Na⁺, assuming that the internal Na⁺ concentration was 13.5 mM. H⁺, Ca²⁺, Mg²⁺, and Cl⁻ did not contribute to the peak value. The peak value was sensitive to the external K⁺ concentration. These data fitted a theoretical line obtained from the Goldman-Hodgkin-Katz equation, using a ratio of P_Na:P_K:P_Cl = 1.1:1.0:0. This means that the permeability to both Na⁺ and K⁺ is responsible for the second component of the fertilization potential. The fertilization potential was also measured in the artificial sea water containing Li⁺ or Cs⁺. The egg at the second component of the fertilization potential was almost equally permeable to Li⁺ as well as Na⁺ or K⁺ and somewhat permeable to Cs⁺. By contrast, the resting membrane potential before fertilization depended to a large extent upon K⁺ permeability.     

Cyanine dye fluorescence used to measure membrane potential changes due to the assembly of complement proteins C5b-9

Summary The fluorescent potentiometric indicator diS–C₃-(5) has been used to investigate changes in membrane potential due to assembly of the C5b-9 membrane attack complex of the complement system. EAC1-7 human red blood cells and resealed erythrocyte ghosts—bearing membrane-assembled C5b67 complexes—were generated by immune activation in C8-deficient human serum. Studies performed with these cellular intermediates revealed that the membrane potential of EAC1-7 red cells and ghosts is unchanged from control red cells (–7 mV) and ghosts (0 mV), respectively. Addition of complement proteins C8 and C9 to EAC1-7 red cells results in a dose-dependent depolarization of membrane potential which precedes hemolysis. This prelytic depolarization of membrane potential—and the consequent onset of hemolysis—is accelerated by raising external [K⁺], suggesting that the diffusional equilibration of transmembrane cation gradients is rate limiting to the cytolytic event. In the case of EAC1-7 resealed ghosts suspended at either high external [K⁺] or [Na⁺], no change in membrane potential (from 0 mV) could be detected after C8/C9 additions. When the membrane potential of the EAC1-7 ghost was displaced from 0 mV by selectively increasing the K⁺ conductance with valinomycin, a dose-dependent depolarization of the membrane was observed upon addition of C8 and C9. In these experiments, lytic breakdown of the ghost membranes was <5%. Conclusions derived from this study include: (i) measured prelytic depolarization of the red cell Donnan potential directly confirms the colloid-osmotic theory of immune cytolysis. (ii) The diffusional transmenbrane equilibration of Na⁺ and K⁺ through the C5b-9 pore results in a dose-dependent depolarization of the membrane potential (E _m ) which appears to be rate-limiting to cytolytic rupture of the target erythrocyte. (iii) Enhanced immune hemolysis observed in high K⁺ media cannot be attributed to cation-selective conductance across the C5b-9 pore, and is probably related to the nearequilibrium condition of potassium-containing red cells when suspended at high external K⁺. These experiments demonstrate that carbocyanine dye fluorescent indicators can be used to monitor electrochemical changes arising from immune damage to the plasma membrane under both cytolytic and noncytolytic conditions. Potential application of this method to the detection of sublytic pathophysiological changes in the plasma membrane of complement-damaged cells are discussed.     

Membrane potential, action potential and activation potential of eggs of the sea urchin, Lytechinus variegatus

Unfertilized Lytechinus variegatus eggs in sea water in their normal physiological state have membrane potentials that approximate ?70 to ?80 mV. This conclusion is based on microelectrode measurements and on computation from the Na⁺ and K⁺ fluxes. The ?8 to ?15 mV values for the membrane potential previously reported and which are generally measured are the consequence of depolarization by impalement. The activation potential in inseminated eggs with an initial membrane potential more negative than ?60 mV is a compound event involving sperm-induced as well as voltage dependent conductance changes. The sperm-induced mechanism is a two-phase conductance increase which involves both Na⁺ and Ca²⁺ during the first phase, and Na⁺ alone during the second phase. In addition, the sperm-induced depolarization at the beginning of the first phase activates a voltage dependent Ca²⁺-conductance mechanism resulting in generation of an action potential.     

Maturation and fertilization of the sea urchin oocyte: An electrophysiological study

Some electrical properties of the sea urchin oocyte during germinal vesicle breakdown (GVBD) and fertilization have been studied using two intracellular electrodes. Oocytes with distinct germinal vesicles have resting potentials of ?70 to ?90 mV and the specific membrane resistance may range from 3 to 10 kΩ·cm². Around rest the I–V relationship is concave toward the axis origin and the membrane is K⁺ selective. A second electrical state, of lower potential and higher resistance, preexists in the membrane. Following GVBD, the K⁺-selective system is lost and the oocyte attains the characteristics of the second state with a resting potential of ?10 to ?50 mV and specific membrane resistance of 10–50 kΩ·cm². At rest the I–V relationship tends to be convex toward the axis origin. The majority of sea urchin eggs (which have undergone GVBD and completed meiosis) have a resting state of ?10 to ?30 mV; 10–50 kΩ·cm². The I–V relationship around rest is convex toward the axis origin and the resting potential is sensitive to changes of Na⁺, Cl^?, and K⁺ in the external medium. There is probably no major change in the electrical properties of the oocyte during the completion of meiosis. A small percentage of eggs from suboptimal animals have high resting potentials of ?70 to ?90 mV and specific membrane resistance of 5–50 kΩ·cm². Such eggs have predominantly K⁺-selective membranes and we suggest that they are either underripe or aged. The first electrical event across the egg plasma membrane during fertilization is a step-like depolarization which occurs about 2 sec after the attachment of the fertilizing spermatozoon to the vitelline layer. There is no change—at the level of the light microscope—either in the egg surface or in the behavior of the spermatozoon until the second event, the fertilization potential (FP), is initiated 11 sec later. The cortical reaction occurs simultaneously with the FP and during the rising phase of the FP the spermatozoon stops gyrating around its point of attachment. Oocytes, which do not have cortical granules, upon insemination exhibit step events but no FP; in contrast artificially activated eggs, either spontaneous or induced by the ionophore A23187, give rise to only the FP. We suggest that the FP is the electrical result of the modification of the egg plasma membrane during cortical exocytosis.     

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.     

K+ and Cl− Conductance of Arabidopsis thaliana Plasma Membrane at Depolarized Voltages

The ion currents, activated by depolarizations, across the plasma membrane of Arabidopsis thaliana cultured cells were studied by means of the patch-clamp technique in the whole-cell configuration. The electrical conductance of the membrane could be shifted from a cation to an anion conducting state by changes in the [K⁺]: [Cl⁻] ratio in the external medium. For ratios between 1:1 and 1:5 the currents were due to K⁺ efflux and for a ratio of 1:10 to Cl⁻ influx. In the cation conducting state the permeability ratio of K⁺ over NH⁺₄ and the alkali metal ions was: K⁺ ≅ NH>Na⁺ ≅ Li⁺ >Cs⁺. In the anion conducting state the permeability of NO⁻₃ was the same as that of Cl⁻. These channels were activated by depolarizations in the range of physiological potentials (-70/-80mV) and, either by mediating the efflux of cations or the influx of anions, they could function to re-hyperpolarize the membrane potential after depolarizations due to the influx of cations or of solutes cotransported with protons and/or to the inhibition of electrogenic pumps.     

Depolarization-induced changes in neurite elongation and intracellular Ca2+ in isolated Helisoma neurons

This study focuses on the effects of K⁺ depolarization on neurite elongation of identified Helisoma neurons isolated into culture. Application of K⁺ to the external medium caused a dose-dependent suppression of neurite elongation. Lower concentrations of K⁺ were associated with a slowing in the rate of neurite elongation, whereas higher concentrations produced neurite retraction. Surprisingly, the effects of K⁺ depolarization were transient, and neurite elongation rates recovered towards control levels within 90 min even though the neurons remained in high-K⁺ solution. Identified neurons differed in the magnitude of their response to K⁺ depolarization; neurite elongation of buccal neuron B4 was inhibited at 5 mM K⁺, but elongation in B5 and B19 was not affected until concentrations of 25 mM. Electrophysiologically, K⁺ application evoked a brief period (5–10 s) of action potential activity that was followed by a steady-state membrane depolarization lasting 2 h or more. The changes in neurite elongation induced by K⁺ depolarization occurred in isolated growth cones severed from their neurites and were blocked by application of calcium antagonists. Intracellular free Ca²⁺ levels in growth cones of B4 and B19 increased and then decreased during the 90-min depolarization, corresponding to the changes in elongation. B4 and B19 showed differences in the magnitude, time course, and spatial distribution of the Ca²⁺ change during depolarization, reflecting their different sensitivities to depolarization.     

The electrical changes accompanying fertilization and cortical vesicle secretion in the medaka egg

The electrical properties of the egg of the medaka, Oryzias latipes, were studied before, during, and after fertilization. The resting potential of the unfertilized egg averaged ?39 ± 9 mV in Yamamoto's Ringers (Y. Ringers), but 20% of the values were between ?50 and ?60 mV. Fertilization triggers a small depolarization of 4 ± 3 mV in 10% Y. Ringers with an average duration of 20 ± 10 sec. The amplitude of this depolarization is independent of [Na⁺]_o, [Ca²⁺]_o, and [Cl^?]_o, so it appears to be due to a nonspecific leak triggered by sperm-egg fusion. The depolarization is followed by a longer hyperpolarizing phase with an average amplitude of 31 ± 12 mV. Recovery from this hyperpolarization has a fast phase lasting 155 ± 18 sec, followed by a slower phase which reaches a steady average membrane potential of ?19 ± 1 mV by 9 min after fertilization. The membrane resistance falls 10-fold during the first 2 min after fertilization, from 40 (1520 kΩ-cm²) to 3 MΩ. This is largely due to an increase in the K⁺ conductance. At the peak of the hyperpolarization, the membrane potential exhibits a 28 mV/decade [K⁺]_o dependence and a 6 mV/decade [Na⁺]_o dependence. The membrane resistance slowly recovers over the next 8 min to a value about 30% larger than before fertilization. The relation of current vs voltage was linear before, during, and after fertilization and indicated a reversal potential of ?98 ± 20 mV for the hyperpolarization peak. The egg's capacitance averaged 0.04 ± 0.01 μF (0.9 μF/cm²) before fertilization and approximately doubles within 90 sec after fertilization. It then decreases over a 9-min period, reaching a value 25% smaller than before fertilization.     

External Mg2+ is required for hyperpolarization to occur in ovulated oocytes of the prawn Palaemon serratus

Immediately after dissection, the ovulated oocyte of the prawn Palaemon serratus had a resting potential E_m of −42 ± 2 mV and a membrane resistance R_m of 15 ± 5 MΩ; the membrane was more permeable to Cl⁻ than to K⁺. The oocyte spontaneously hyperpolarized and E_m gradually reached −70 mV 20–30 min after removal of the oocyte from the female, due to increased membrane permeability to K⁺. However, the hyperpolarization occured only if Mg²⁺ was present in the seawater; external Ca²⁺ was not required. Long-term incubation without external Mg²⁺ depolarized the membrane and increased membrane resistance. After preincubation in Mg²⁺-free ASW, oocytes transferred to standard artificial seawater (ASW) transiently hyperpolarized and then repolarized, before gradually hyperpolarizing to a sustained value of −62 ± mV. The respective roles of external Mg²⁺ and fertilization in eliciting the electrical response of the prawn egg at natural spawning are discussed.     

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.     

Ca2+-activated K+ currents inNecturus choroid plexus

Summary The tight-seal whole-cell recording method has been used to studyNecturus choroid plexus epithelium. A cell potential of –59±2 mV and a whole cell resistance of 56±6 M were measured using this technique. Application of depolarizing step potentials activated voltage-dependent outward currents that developed with time. For example, when the cell was bathed in 110mm NaCl Ringer solution and the interior of the cell contained a solution of 110mm KCl and 5nm Ca²⁺, stepping the membrane potential from a holding value of –50 to –10 mV evoked outward currents which, after a delay of greater than 50 msec, increased to a steady state in 500 msec. The voltage dependence of the delayed currents suggests that they may be currents through Ca²⁺-activated K^_ channels. Based on the voltage dependence of the activation of Ca²⁺-activated K⁺ channels, we have devised a general method to isolate the delayed currents. The delayed currents were highly selective for K⁺ as their reversal potential at different K⁺ concentration gradients followed the Nernst potential for K⁺. These currents were reduced by the addition of TEA⁺ to the bath solution and were eliminated when Cs⁺ or Na⁺ replaced intracellular K⁺. Increasing the membrane potential to more positive values decreased both the delay and the half-times (t _1/2) to the steady value. Increasing the pipette Ca²⁺ also decreased the delay and decreasedt _1/2. For instance, when pipette Ca²⁺ was increased from 5 to 500nm, the delay andt _1/2 decreased from values greater than 50 and 150 msec to values less than 10 and 50 msec. We conclude that the delayed currents are K⁺ currents through Ca²⁺-activated K⁺ channels.At the resting membrane potential of –60 mV, Ca²⁺-activated K⁺ channels contribute between 13 to 25% of the total conductance of the cell. The contribution of these channels to cell conductance nearly doubles with membrane depolarization of 20–30 mV. Such depolarizations have been observed when cerebrospinal fluid (CSF) secretion is stimulated by cAMP and with intracellular Ca²⁺. Thus the Ca²⁺-activated K⁺ channels may play a specific role in maintaining intracellular K⁺ concentrations during CSF secretion.     

Contribution of a H+ pump in determining the resting potential of neuroblastoma cells

The aim of this work was to examine the effects of changes in external K⁺ concentration (K _o ) around its physiological value, of various K⁺ channels blockers, including internal Cs⁺, of vacuolar H⁺-ATPase inhibitors and of the protonophore CCCP on the resting potential and the voltage-dependent K⁺ current of differentiated neuroblastoma x glioma hybrid NG108-15 cells using the whole-cell patch-clamp technique. The results are as follows: (i) under standard conditions (K _o =5 mm) the membrane potential was –60±1 mV. It was unchanged when K _o was decreased to 1 mm and was depolarized by 4±1 mV when K_o was increased to 10 mm. (ii) Internal Cs⁺ depolarized the membrane by 21±3 mV. (iii) The internal application of the vacuolar H⁺-ATPase inhibitors N-ethylmaleimide (NEM), NO ₃ ^– and bafilomycin A1 (BFA) depolarized the membrane by 15±2, 18±2 and 16±2 mV, respectively, (iv) When NEM or BFA were added to the internal medium containing Cs⁺, the membrane was depolarized by 45±1 and 42±2 mV, respectively. (v) The external application of CCCP induced a transient depolarization followed by a prolonged hyperpolarization. This hyperpolarization was absent in BFA-treated cells. The voltage-dependent K⁺ current was increased at negative voltages and decreased at positive voltages by NEM, BFA and CCCP. Taken together, these results suggest that under physiological conditions, the resting potential of NG108-15 neuroblastoma cells is maintained at negative values by both voltage-dependent K⁺ channels and an electrogenic vacuolar type H⁺-ATPase.This work was supported by a grant from INSERM (CRE 91 0906).     

Changes in membrane potential and resistance caused by transient increase of potassium conductance in the unicellular green alga Eremosphaera viridis

The electrophysiological membrane parameters of the unicellular green alga Eremosphaera viridis were determined using an improved computer-supported single-microelectrode technique. These cells developed an average membrane potential of-150 mV in the light and a specific resistance of 1 Ω m² with an external potassium concentration of 1.1 mM and pH 5.5. In the dark, many cells showed a less polarized potential of 30–40 mV and a smaller membrane resistance. At potassium concentrations in the external medium higher than 1 mM, the membrane potential strongly depends on the external potassium content apart from a small electrogenic component. At concentrations lower than 1 mM K⁺, a dependence of the membrane potential upon external potassium concentrations could not be verified. Inserting the internal ion activities in the Goldmann equation shows that, in this range, the proton conductance seems to be predominant over the potassium conductance. Transient changes in the membrane potential and in the membrane resistance were observed after switching off the light, after addition of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea or N,N′-dicyclohexylcarbodiimide, after a sudden decrease in temperature, and after current pulses. These changes resemble the action potentials (AP) found in other plant cells (Chara, Acetabularia). On average, the AP has a delay period of 5.1 s and a duration of 43.8 s showing a sudden decrease and a slower regeneration. The voltage peak during an AP followed exactly the Nernst potential of potassium over a range of external potassium concentrations from 5 μM to 0.2 M. This is true for depolarization or hyperpolarization, depending on the external K⁺-concentration. Tetraethylammonium-hydrogensulphate, a rather specific inhibitor of K⁺ channels in nervous cells, suppressed the AP. The correlation of the appearance of the AP with a short-term opening of potassium channels in the membrane of Eremosphaera is discussed.     

Endothelial cell oxidant generation during K+-induced membrane depolarization

We tested the hypothesis that membrane depolarization may initiate oxidant generation in the endothelial cell. Depolarization was produced in bovine pulmonary arterial endothelial cells (BPAEC) in monolayer culture with varying external K⁺, or with glyburide (10 μM), tetraethylammonium (TEA, 10 mM), gramicidin (1 μM), or nigericin (2 μM). Evaluation of bisoxonol fluorescence of BPAEC indicated concentration-dependent depolarization by high K⁺ (2% change in fluorescence/mV change in membrane potential in the 5.9–48 mM range of K⁺) and essentially complete depolarization with glyburide. Generation of oxidants was assessed with o-phenylenediamine dihydrochloride (o-PD) oxidation in the presence of horseradish peroxidase (HRP). There was a time-dependent increase in o-PD oxidation with 24 mM K⁺, nigericin, and gramicidin over 2 hours compared with control. In 1 hour o-PD oxidation increased 2.8-fold for 24 mM and 3.7-fold for 48 mM K⁺ compared with control. Catalase reduced 24 mM K⁺-induced o-PD oxidation by 50%, while Cu/Zn-superoxide dismutase (SOD) abolished the increase. Oxidation of o-PD was reduced by 57% in the absence of HRP in the system. With K⁺ channel blockade, o-PD oxidation increased 3.8-fold with glyburide and 4.6-fold with TEA compared with control. These data indicate formation of H₂O₂ and possibly other oxidants with depolarization and suggest involvement of K⁺-channels in this process. © 1996 Wiley-Liss, Inc.     

The electrogenic sodium pump of the frog retinal pigment epithelium

Summary It was previously shown that ouabain decreases the potential difference across anin vitro preparation of bullfrog retinal pigment epithelium (RPE) when applied to the apical, but not the basal, membrane and that the net basal-to-apical Na⁺ transport is also inhibited by apical ouabain. This suggested the presence of a Na⁺–K⁺ pump on the apical membrane of the RPE. In the present experiments, intracellular recordings from RPE cells show that this pump is electrogenic and contributes approximately –10 mV to the apical membrane potential (V _AP). Apical ouabain depolarizedV _AP in two phases. The initial, fast phase was due to the removal of the direct, electrogenic component. In the first one minute of the response to ouabain,V _AP depolarized at an average rate of 4.4±0.42 mV/min (n=10, mean ±sem), andV _AP depolarized an average of 9.6±0.5 mV during the entire fast phase. A slow phase of membrane depolarization, due to ionic gradients running down across both membranes, continued for hours at a much slower rate, 0.4 mV/min. Using a simple diffusion model and K⁺-specific microelectrodes, it was possible to infer that the onset of the ouabain-induced depolarization coincided with the arrival of ouabain molecules at the apical membrane. This result must occur if ouabain affects an electrogenic pump. Other metabolic inhibitors, such as DNP and cold, also produced a fast depolarization of the apical membrane. For a decrease in temperature of 10°C, the average depolarization of the apical membrane was 7.1±3.4 mV (n=5) and the average decrease in transepithelial potential was 3.9±0.3 mV (n=10). These changes in potential were much larger than could be explained by the effect of temperature on anRT/F electrodiffusion factor. Cooling the tissue inhibited the same mechanism as ouabain, since prior exposure to ouabain greatly reduced the magnitude of the cold effect. Bathing the tissue in 0mm [K⁺] solution for 2 hr inhibited the electrogenic pump, and subsequent re-introduction of 2mm [K⁺] solution produced a rapid membrane hyperpolarization. We conclude that the electrogenic nature of this pump is important to retinal function, since its contribution to the apical membrane potential is likely to affect the transport of ions, metabolites, and fluid across the RPE.     

Effects of high K+ concentrations on the growth and development of ciliary ganglion neurons in cell culture

Extracts prepared from embryonic eye tissue permit all of the neurons present in embryonic ciliary ganglia to survive and develop in cell culture. High K⁺ concentrations stimulate growth of the neurons in culture above the maximal levels obtained with eye extract alone. Growth in 25 mM K⁺ produced parallel increases in the levels of choline acetyltransferase activity, lactate dehydrogenase activity (a common cytoplasmic enzyme), and total protein synthesis per neuron. The K⁺ effect appears to be mediated by membrane depolarization. Intracellular recording confirmed that the neurons were chronically depolarized in 25 mM K⁺. Veratridine produced the same stimulation of growth, while tetrodotoxin blocked the veratridine effect without preventing the K⁺ effect. Ca²⁺ may also play a role in the K⁺ effect. Two drugs thought to block Ca²⁺ channels (Mg²⁺ and D600) each blocked or reduced in the increase in growth caused by 25 mM K⁺. The drugs did not interfere with neuronal growth in control cultures, indicating that eye extract and membrane depolarization influence neuronal growth by different mechanisms.     

Demonstration of Voltage-Dependent and TTX-Sensitive Na+-Channels in Human Melanocytes

The electrophysiological properties of cultured human melanocytes were investigated using the whole-cell configuration of the patch-clamp technique. Depolarizations to membrane potentials more positive than -30 mV resulted in the rapid development (<1 ms to peak) of an inward current. The maximum peak current was observed at +10 mV and reached an average amplitude of about 270 pA. During the depolarizations, the current inactivated with a time constant of about 2 ms. The current was abolished by the addition of 0.3 μM tetrodotoxin, a blocker of voltage-gated Na⁺-channels, and disappeared when Na⁺ was omitted from the extracellular medium. In addition, the melanocytes contain at least two types of outward K⁺-current. The first type, observed in every cell, was highly sensitive (K_i 1 mM) to the K⁺-channel blocker TEA, required depolarizations beyond zero to be activated and did not inactivate. The second type was less regularly observed (10% of the cells). This current activated at more negative voltages (–20 mV), was resistant to TEA (20 mM) but was blocked by 2 mM 4-aminopyridine and inactivated rapidly during depolarizations. We conclude that human melanocytes are equipped with voltage-dependent Na⁺-channels, a delayed rectifying K⁺-current and a K⁺-current similar to the A-current in neurones.     

Dipole moment changes and voltage dependent membrane capacity of squid axon

Changes in the membrane capacity of squid axons during hyper- and depolarizations are measured between ?160 and +40 mV. After corrections for the series resistance and fringe effect, we found that the membrane capacity increased from 0.68 to 1.2 μF/cm² with depolarization. It was further observed that tetrodotoxin in the external medium eliminated the change in membrane capacity without affecting the conductivity. The voltage-dependent membrane conductivity is, in turn, greatly reduced by the internal cesium ion. These observations clearly indicate that the voltage-dependent membrane capacity and conductivity are closely related to ionic channels. Particularly, the increase in membrane capacity with depolarizations may be due to sodium channels. The change in the dipole moment associated with sodium sites was determined using values of α_{m and}β_m at various depolarizations. We found, based on voltage clamp measurements, that the increase in the dipole moment of the sodium site between ?40 and ?5 mV is 1230 Debye units (D.U.) and 930 D.U. between ?5 and +60 mV, indicating that the depolarization of sodium channels may consist of two different steps.     

Voltage dependent potassium fluxes and the significance of action potentials in Acetabularia

Membrane potential, V_m, and K⁺(⁸⁶Rb⁺) fluxes have been measured simultaneously on individual cells of Acetabularia mediterranea. During resting state (resting potential approx. ?170 mV) the K⁺ influx amounts to 0.24–0.6 pmol · cm^?2 · s^?1 and the K⁺ efflux to 0.2–1.5 pmol · cm^?2 s^?1. According to the K⁺ concentrations inside and outside the cell (40 : 1) the voltage dependent K⁺ flux (zero at V_m = E_K = ?90 mV) is stimulated approx. 40-fold for V_m more positive than E_K.It is calculated that during one action potential (temporary depolarization to V_m more positive than E_K) a cell looses the same amount of K⁺, which leaks in during 10–20 min in the resting state (V_m = ?170 mV). Since action potentials occur spontaneously in Acetabularia, they are therefore suggested to have a significant function for the K⁺ balance of this alga.