Studies on Electrogenesis under High K+ Concentrations in Internodal Cells of Chara corallina

+ concentration ([K⁺]_o) on the membrane potential (E_m) of Chara corallina was studied. E_m more negative than -100 mV was maintained even at 100 mM [K⁺]_o. Addition of Ca²⁺ to the external medium further increased this tendency. However, E_m responded sensitively to the increase in [K⁺]_o, when the electrogenic proton pump of the plasma membrane was inhibited by treating cells with dicyclohexylcarbodiimide, an inhibitor of proton pump. Analysis using equivalent circuit model of the plasma membrane suggested that the electrogenic proton pump was activated by the increase in [K⁺]_o. In the presence of 100 mM K⁺, action potentials were generated by electric stimuli. The ionic mechanism of generation of action potentials in the presence of K⁺ at high concentration was discussed. Received 3 October 2000/ Accepted in revised form 6 January 2001     

High-conductance K+ channel in pancreatic islet cells can be activated and inactivated by internal calcium

Summary The Ca²⁺-activated K⁺ channel in rat pancreatic islet cells has been studied using patch-clamp single-channel current recording in excised inside-out and outside-out membrane patches. In membrane patches exposed to quasi-physiological cation gradients (Na⁺ outside, K⁺ inside) large outward current steps were observed when the membrane was depolarized. The single-channel current voltage (I/V) relationship showed outward rectification and the null potential was more negative than –40 mV. In symmetrical K⁺-rich solutions the single-channelI/V relationship was linear, the null potential was 0 mV and the singlechannel conductance was about 250 pS. Membrane depolarization evoked channel opening also when the inside of the membrane was exposed to a Ca²⁺-free solution containing 2mm EGTA, but large positive membrane potentials (70 to 80 mV) were required in order to obtain open-state probabilities (P) above 0.1. Raising the free Ca²⁺ concentration in contact with the membrane inside ([Ca²⁺]_i) to 1.5×10^–7 m had little effect on the relationship between membrane potential andP. When [Ca²⁺]_i was increased to 3×10^–7 m and 6×10^–7 m smaller potential changes were required to open the channels. Increasing [Ca²⁺]_i further to 8×10^–7 m again activated the channels, but the relationship between membrane potential andP was complex. Changing the membrane potential from –50 mV to +20 mV increasedP from near 0 to 0.6 but further polarization to +50 mV decreasedP to about 0.2. The pattern of voltage activation and inactivation was even more pronounced at [Ca²⁺]_i=1 and 2 m. In this situation a membrane potential change from –70 to +20 mV increasedP from near 0 to about 0.7 but further polarization to +80 mV reducedP to less than 0.1. The high-conductance K⁺ channel in rat pancreatic islet cells is remarkably sensitive to changes in [Ca²⁺]_i within the range 0.1 to 1 m which suggests a physiological role for this channel in regulating the membrane potential and Ca²⁺ influx through voltage-activated Ca²⁺ channels.     

Fractional contribution of major ions to the membrane potential of Drosophila melanogaster oocytes

In ovarian follicles of Drosophila melanogaster, ion substitution experiments revealed that K⁺ is the greatest contributor (68%) in setting oocyte steady‐state potential (E_m), while Mg²⁺ and a metabolic component account for the rest. Because of the intense use made of Drosophila ovarian follicles in many lines of research, it is important to know how changes in the surrounding medium, particularly in major diffusible ions, may affect the physiology of the cells. The contributions made to the Drosophila oocyte membrane potential (E_m) by [Na⁺]_o, [K⁺]_o, [Mg²⁺]_o, [Ca²⁺]_o, [Cl^?]_o, and pH (protons) were determined by substitutions made to the composition of the incubation medium. Only K⁺ and Mg²⁺ were found to participate in setting the level of E_m. In follicles subjected to changes in external pH from the normal 7.3 to either pH 6 or pH 8, E_m changed rapidly by about 6 mV, but within 8 min had returned to the original E_m. Approximately half of all follicles exposed to reduced [Cl^?]_o showed no change in E_m, and these all had input resistances of 330 kΩ or greater. The remaining follicles had smaller input resistances, and these first depolarized by about 5 mV. Over several minutes, their input resistances increased and they repolarized to a value more electronegative than their value prior to reduction in [Cl^?]_o. Together, K⁺ and Mg²⁺ accounted for up to 87% of measured steady‐state potential. Treatment with sodium azide, ammonium vanadate, or chilling revealed a metabolically driven component that could account for the remaining 13%. © 2009 Wiley Periodicals, Inc.     

Excitability of Paramecium and the significance of negative surface charges

Summary On the basis of a model presented in a previous paper (Hook and Hildebrand, 1979) the influence of external cation concentrations [K⁺]₀, [Ca²⁺]₀ and of membrane voltage V_m (i.e. the actual potential difference between the two membrane faces) on the locomotor behavior of Paramecium is theoretically analyzed. In an extended model system we discuss the negative feedback of intraciliary calcium [Ca²⁺]_i on the excitability of the ciliary membrane. While a fast blocking of Ca channels is mediated by increased [Ca²⁺]_i and accounts for the short duration of action potentials, a slow [Ca²⁺ ]_i-dependent denaturation of channel molecules is assumed to determine excitability changes of Paramecium on a long time scale.It is emphasized that the duration of long-lasting ciliary reversal which reflects the excitability is not a direct function of the cation ratio J_u [K⁺]₀/[Ca²⁺] ₀ ^1/2 but rather of the membrane potential V_m.Introduction of negative surface charges can well explain why for a series of different [K⁺]₀, [Ca²⁺]₀ but constant J_a value the excitability is unchanged despite corresponding shifts in measured membrane potentials.     

Quantitative analysis of depolarization-induced ATP release from mouse brain synaptosomes: External calcium dependent and independent processes

Summary We and others have shown previously that ATP is secreted from mouse brain synaptosomes following depolarization of the membrane by high [K⁺] ₀ and the time course can be monitored accurately by measuring the light emitted from luciferin-luciferase included in the reaction medium. In the present work we have evaluated the relative importance of [Ca²⁺] ₀ and membrane potential on the ATP secretion process by modelling the time course of ATP release under different conditions. After correction of the records for destruction of released ATP by synaptosomal ecto-ATPase activity, we found that ATP secretion occurs by an apparent first order process. We also established that, in addition to the classical [Ca²⁺] ₀ -dependent mode, ATP secretion also occurred in the absence of extracellular calcium ([Ca²⁺] ₀ < 1 m). Upon lowering the extracellular Ca²⁺ concentration, both the rate and the extent of ATP secretion decreased. To assess the contribution of membrane potential to the release rate we measured ATP secretion at membrane potentials determined by extracellular [K⁺] ₀ (or [Rb⁺] ₀ ) as defined by the distribution of the carbocyanine dye, diSC₃(5). Rate constants computed from measured secretion curves revealed that this parameter was essentially independent of membrane potential in the absence of [Ca²⁺] ₀ . Noise analysis of the light signal showed that the variance increased upon stimulation by high [K⁺] ₀ , suggesting that both modes of secretion are quantal. Thus, we conclude that the rate of ATP secretion from nerve terminals depends upon Ca²⁺ entry but not on membrane potential, per se     

Effect of external K+, Ca2+, and Ba2+ on membrane potential and ionic conductance in rat astrocytes

Summary 1. The purpose of this study was (a) to identify if astrocytes show a similar non-Nernstian depolarization in low K⁺ or low Ca²⁺ solutions as previously found in human glial and glioma cells, and (b) to analyze the influence of the K⁺ conductance on the membrane potential of astrocytes.2. The membrane potential (E_m) and the ionic conductance were studied with whole-cell patch-clamp technique in neonatal rat astrocytes (5–9 days in culture) and in human glioma cells (U-251MG).3. In 3.0 mM K⁺, E_m was –75 ± 1.0 mV (mean ± SEM,n=39) in rat astrocytes and –79 ± 0.7 mV (n=5) in U-251MG cells. In both cell types E_m changed linearly to the logarithm of [K⁺]₀ between 3.0 and 160 mM K⁺. K⁺ free medium caused astrocytes to hyperpolarize to –93 ± 2.7 mV (n=21) and U-251MG cells to depolarize to –27 ± 2.1 mV (n=3).4. The I-E curve did not show inward rectification in astrocytes at this developmental stage. The slope conductance (g) exhibited only a small decrease (–19%) in K⁺ free solution and no significant change in 160 mM K⁺.5. Ba²⁺ (1.0 mM) depolarized astrocytes to –45 ± 2.9 mV (n=11), decreasing the slope conductance (g) by 42.4 ± 8.3% (n=11). Ca²⁺ free solution depolarized astrocytes to –53 ± 3.4 mV (n=12) and resulted in a positive shift of the I-E curve, increasing g by 15.3 ± 8.2% (n=8).6. Calculations indicated that a block of K⁺ channels explains the depolarizing effect of Ba²⁺. The effects of K⁺ free or Ca²⁺ free solutions on E_m can be explained by a transformation of K⁺ channels to non-specific leakage channels. That astrocytes show a different reaction to low K⁺ than glioma cells can be related to the lack of inwardly rectifying K⁺ channels in astrocytes at this developmental stage.     

Permeation of Ca2+ through K+ channels in the plasma membrane of Vicia faba guard cells

Summary The whole-cell patch-clamp method has been used to measure Ca²⁺ influx through otherwise K⁺-selective channels in the plasma membrane surrounding protoplasts from guard cells of Vicia faba. These channels are activated by membrane hyperpolarization. The resulting K⁺ influx contributes to the increase in guard cell turgor which causes stomatal opening during the regulation of leaf-air gas exchange. We find that after opening the K⁺ channels by hyperpolarization, depolarization of the membrane results in tail current at voltages where there is no electrochemical force to drive K⁺ inward through the channels. Tail current remains when the reversal potential for permeant ions other than Ca²⁺ is more negative than or equal to the K⁺ equilibrium potential (–47 mV), indicating that the current is due to Ca²⁺ influx through the K⁺ channels prior to their closure. Decreasing internal [Ca²⁺] (Ca _i ) from 200 to 2 nm or increasing the external [Ca²⁺] (Ca _o ) from 1 to 10 mm increases the amplitude of tail current and shifts the observed reversal potential to more positive values. Such increases in the electrochemical force driving Ca²⁺ influx also decrease the amplitude of time-activated current, indicating that Ca²⁺ permeation is slower than K⁺ permeation, and so causes a partial block. Increasing Ca _o also (i) causes a positive shift in the voltage dependence of current, presumably by decreasing the membrane surface potential, and (ii) results in a U-shaped current-voltage relationship with peak inward current ca. –160 mV, indicating that the Ca^2– block is voltage dependent and suggesting that the cation binding site is within the electric field of the membrane. K⁺ channels in Zea mays guard cells also appear to have a Ca _i -, and Ca _o -dependent ability to mediate Ca²⁺ influx. We suggest that the inwardly rectiying K⁺ channels are part of a regulatory mechanism for Ca _i . Changes in Ca _o and (associated) changes in Ca _i regulate a variety of intracellular processes and ion fluxes, including the K⁺ and anion fluxes associated with stomatal aperture change.This work was supported by grants to S.M.A. from NSF (DCB-8904041) and from the McKnight Foundation. K.F.-G. is a Charles Gilbert Heydon Travelling Fellow. The authors thank Dr. R. MacKinnon (Harvard Medical School) and two anonymous reviewers for helpful comments.     

The Extracellular K+ Concentration Dependence of Outward Currents through Kir2.1 Channels Is Regulated by Extracellular Na+ and Ca2+

It has been known for more than three decades that outward Kir currents (I_K1) increase with increasing extracellular K⁺ concentration ([K⁺]_o). Although this increase in I_K1 can have significant impacts under pathophysiological cardiac conditions, where [K⁺]_o can be as high as 18 mm and thus predispose the heart to re-entrant ventricular arrhythmias, the underlying mechanism has remained unclear. Here, we show that the steep [K⁺]_o dependence of Kir2.1-mediated outward I_K1 was due to [K⁺]_o-dependent inhibition of outward I_K1 by extracellular Na⁺ and Ca²⁺. This could be accounted for by Na⁺/Ca²⁺ inhibition of I_K1 through screening of local negative surface charges. Consistent with this, extracellular Na⁺ and Ca²⁺ reduced the outward single-channel current and did not increase open-state noise or decrease the mean open time. In addition, neutralizing negative surface charges with a carboxylate esterifying agent inhibited outward I_K1 in a similar [K⁺]_o-dependent manner as Na⁺/Ca²⁺. Site-directed mutagenesis studies identified Asp¹¹⁴ and Glu¹⁵³ as the source of surface charges. Reducing K⁺ activation and surface electrostatic effects in an R148Y mutant mimicked the action of extracellular Na⁺ and Ca²⁺, suggesting that in addition to exerting a surface electrostatic effect, Na⁺ and Ca²⁺ might inhibit outward I_K1 by inhibiting K⁺ activation. This study identified interactions of K⁺ with Na⁺ and Ca²⁺ that are important for the [K⁺]_o dependence of Kir2.1-mediated outward I_K1.     

Influence of ionic environment on the relationship between pre- and postsynaptic potentials

The effects of various ions on the relationship between pre- and postsynaptic potentials were studied using untreated squid giant synapses, or those injected presynaptically with tetraethylammonium ions (TEA) in the presence of 10^?6 g/ml tetrodotoxin (TTX). The synaptic transfer function was, in general, augmented by increasing [Ca²⁺]₀ or by reducing [Mg²⁺]₀. Opposite results were found by lowering either [Na⁺]₀ or [Ca²⁺]₀, or by increasing [K⁺]₀ or [Mg²⁺]₀. When [Ca²⁺]₀ was removed, presynaptically applied depolarizations failed to produce both “On-” and “Off-PSP's.” Electrophoretically injected Ca²⁺ into the presynaptic terminal reduced synaptic transmission. The minimal level of presynaptic membrane potential produced by an applied outward current pulse, which suppressed On-PSP completely, averaged 106 mV inside positive (ranging between 52–205 mV from 12 preparations). The potential level was shifted more negatively on lowering [Ca²⁺]₀ and more positively in high [Ca²⁺]₀-media. However, altering the [Na⁺]₀ did not change the suppression level appreciably. Under these ionic circumstances the maximum amplitude of On-PSP, as well as Off-PSP, was markedly changed, but the level of the presynaptic depolarization required to evoke a maximum On-PSP appeared to be unchanged, and the average value was 50 mV from the resting membrane potential level. Although the data are only qualitative, they appear to support the “Ca hypothesis” for the transmitter release and its shut-off mechanism. Replacement of 423 mM Cl^? by Br^? or with isethionate did not affect synaptic transmission.     

A study of the current-voltage relationships of electrogenetic active and passive membrane elements in riccia fluitans

Potassium- and proton-dependent membrane potential, conductance, and current-voltage characteristics (I–V curves) have been measured on rhizoid cells of the liverwort Riccia fluitans. The potential difference (E_m) measured with microelectrodes across plasmalemma and tonoplast is depolarized to the potassium-sensitive diffusion potential (E_D) in the presence of 1 mM NaCN, 1 mM NaN₃, or at temperatures below 6°C. Whereas the temperature change from 25°C to 5°C decreases the membrane conductance (g_m) from 0.71 to 0.43 S ? m^?2, 1 mM NaCN increases g_m by about 25%. The membrane displays potassium-controlled rectification which gradually disappears at temperatures below 5°C. The potassium pathway can be described by an equivalent circuit of a diode and an ohmic resistor in parallel. In the potential interval of E_D ± 100 mV the measured I-V curves roughly fit the theoretical curves obtained from a modified diode equation. ⁸⁶Rb⁺(K⁺)-influx is voltage sensitive: In the presence of 1 mM NaCN, ⁸⁶Rb⁺-influx follows a hyperbolic function corresponding to a low conductance at low [K⁺]_o and high conductance at high [K⁺]_o. On the contrary ⁸⁶Rb⁺-influx is linear with [K⁺]_o when pump activity is normal. It is believed that there are two K⁺-transport pathways in the Riccia membrane, one of which is assigned to the low conductance (0.2 S · m^?2), the other to a temperature-dependent facilitated diffusion system with a higher conductance (7.7 S · m^?2). The electrogenic pump essentially acts as a current source and consumes about 39% of the cellular ATP-turnover. In the presence of 30 μM CCCP the saturation current of 0.1 A · m^?2 is doubled to about 0.2 A · m^?2, and the electromotive force of ?360 mV switches to ?250 mV. It is suggested that this may be due to a change in stoichiometry from one to two transported charges per ATP hydrolyzed.     

Effects of extracellular calcium and protons on osteoclast potassium currents

During resorption of mineralized tissues, osteoclasts are exposed to marked changes in the concentration of extracellular Ca²⁺ and H⁺. We examined the effects of these cations on two types of K⁺ currents previously described in these cells. Whole-cell patch clamp recordings of membrane currents were made from osteoclasts freshly isolated from neonatal rats. In control saline (1 mm Ca²⁺, pH 7.4), the voltage-gated, outwardly rectifying K⁺ current activates at approximately 45 mV and the conductance is half-maximally activated at –29 mV (V _0.5). Increasing [Ca²⁺]_out rapidly and reversibly shifted the current-voltage (I–V) relation to more positive potentials. Current at –29 mV decreased to 28 and 9% of control current at 5 and 10 mm [Ca²⁺]_out, respectively. This effect of elevating [Ca²⁺]_out was due to a positive shift of the K⁺ channel voltage activation range. Zn²⁺ or Ni²⁺ (5 to 500 m) also shifted the I–V relation to more positive potentials and had additional effects consistent with blockade of the K⁺ channel. Based on the extent to which these divalent cations affected the voltage activation range of the outwardly rectifying K⁺ current, the potency sequence was Zn²⁺ > Ni²⁺ > Ca²⁺. Lowering or raising extracellular pH also caused shifts of the voltage activation range to more positive or negative potentials, respectively. In contrast to their effects on the outwardly rectifying K⁺ current, changes in the concentration of extracellular H⁺ or Ca²⁺ did not shift the voltage activation range of the inwardly rectifying K⁺ current. These findings are consistent with Ca²⁺ and other cations affecting voltage-dependent gating of the osteoclast outwardly rectifying K⁺ channel through changes in surface charge.This work was supported by The Arthritis Society and the Medical Research Council of Canada. S.M.S. is supported by a Scientist Award and S.J.D. by a Development Grant from the Medical Research Council.     

Comparative study of the effects of cromakalim (BRL 34915) and diazoxide on membrane potential, [Ca2+] i and ATP-sensitive potassium currents in insulin-secreting cells

Summary Patch-clamp and single cell [Ca²⁺] _i measurements have been used to investigate the effects of the potassium channel modulators cromakalim, diazoxide and tolbutamide on the insulin-secreting cell line RINm5F. In intact cells, with an average cellular transmembrane potential of –62±2 mV (n=42) and an average basal [Ca²⁺] _i of 102±6nm (n=37), glucose (2.5–10mm): (i) depolarized the membrane, through a decrease in the outward K_ATP current, (ii) evoked Ca²⁺ spike potentials, and (iii) caused a sharp rise in [Ca²⁺] _i . In the continued presence of glucose both cromakalim (100–200 m) and diazoxide (100 m) repolarized the membrane, terminated Ca²⁺ spike potentials and attenuated the secretagogue-induced rise in [Ca²⁺] _i . In whole cells (voltage-clamp records) and excised outside-out membrane patches, both cromakalim and diazoxide enhanced the current by opening ATP-sensitive K⁺ channels. Diazoxide was consistently found to be more potent than cromakalim. Tolbutamide, a specific inhibitor of ATP-sensitive K⁺ channels, reversed the effects of cromakalim on membrane potential and K_ATP currents.     

Fluid shear stress induces calcium transients in osteoblasts through depolarization of osteoblastic membrane

Intracellular calcium transient ([Ca²⁺]_i transient) induced by fluid shear stress (FSS) plays an important role in osteoblastic mechanotransduction. Changes of membrane potential usually affect [Ca²⁺]_i level. Here, we sought to determine whether there was a relationship between membrane potential and FSS-induced [Ca²⁺]_i transient in osteoblasts. Fluorescent dyes DiBAC₄(3) and fura-2 AM were respectively used to detect membrane potential and [Ca²⁺]_i. Our results showed that FSS firstly induced depolarization of membrane potential and then a transient rising of [Ca²⁺]_i in osteoblasts. There was a same threshold for FSS to induce depolarization of membrane potential and [Ca²⁺]_i transients. Replacing extracellular Na⁺ with tetraethylammonium or blocking stretch-activated channels (SACs) with gadolinium both effectively inhibited FSS-induced membrane depolarization and [Ca²⁺]_i transients. However, voltage-activated K⁺ channel inhibitor, 4-Aminopyridine, did not affect these responses. Removing extracellular Ca²⁺ or blocking of L-type voltage-sensitive Ca²⁺ channels (L-VSCCs) with nifedipine inhibited FSS-induced [Ca²⁺]_i transients in osteoblasts too. Quantifying membrane potential with patch clamp showed that the resting potential of osteoblasts was −43.3 mV and the depolarization induced by FSS was about 44 mV. Voltage clamp indicated that this depolarization was enough to activated L-VSCCs in osteoblasts. These results suggested a time line of Ca²⁺ mobilization wherein FSS activated SACs to promote Na⁺ entry to depolarize membrane that, in turn, activated L-VSCCs and Ca²⁺ influx though L-VSCCs switched on [Ca²⁺]_i response in osteoblasts.     

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.     

Influence of Ca on the plasma membrane potential and electrogenic uptake of glycine by myeloma cells. Involvement of a Ca-activated K channel

The involvement of Ca²⁺-activated K⁺ channels in the regulation of the plasma membrane potential and electrogenic uptake of glycine in SP 2/0-AG14 lymphocytes was investigated using the potentiometric indicator 3,3′-diethylthiodicarbocyanine iodide. The resting membrane potential was estimated to be −57 ± 6 mV (n = 4), a value similar to that of normal lymphocytes. The magnitude of the membrane potential and the electrogenic uptake of glycine were dependent on the extracellular K⁺ concentration, [K⁺]_o, and were significantly enhanced by exogenous calcium. The apparent V_max of Na⁺-dependent glycine uptake was doubled in the presence of calcium, whereas the K_0.5 was not affected. Ouabain had no influence on the membrane potential under the conditions employed. Additional criteria used to demonstrate the presence of Ca²⁺-activated K⁺ channels included the following: (1) addition of EGTA to calcium supplemented cells elicited a rapid depolarization of the membrane potential that was dependent on [K⁺]_o; (2) the calmodulin antagonist, trifluoperazine, depolarized the membrane potential in a dose-dependent and saturable manner with an IC₅₀ of 9.4 μM; and (3) cells treated with the Ca²⁺-activated K⁺ channel antagonist, quinine, demonstrated an elevated membrane potential and depressed electrogenic glycine uptake. Results from the present study provide evidence for Ca²⁺-activated K⁺ channels in SP 2/0-AG14 lymphocytes, and that their involvement regulates the plasma membrane potential and thereby the electrogenic uptake of Na⁺-dependent amino acids.     

Pacemaking mechanism of the afterdischarge of the ovulation hormone-producing caudo-dorsal cells in the gastropod mollusc Lymnaea stagnalis

The ovulation hormone-producing caudo-dorsal cells (CDC) of Lymnaea stagnalis have three states of excitability (active, inhibited, and resting), which are related to the egg-laying cycle. Active state CDC produce a firing pattern of prolonged spiking activity (1 spike/2 s), which in the animal occurs shortly before egg laying. In preparations it is evoked as an afterdischarge upon repetitive stimulation of CDC. The afterdischarge is not synaptically driven, but rests on a pacemaking mechanism. CDC are silent in the inhibited and resting states, which follow egg laying. In these states the membrane potential is mainly dependent on [K⁺]₀. In the active state the ratio of the K⁺, Na⁺, and Ca²⁺ permeabilities has changed considerably, probably resulting from an increased permeability to Na⁺ and Ca²⁺. The firing rate in the afterdischarge is dependent on the membrane potential, which is confirmed experimentally by varying [K⁺]₀.[Na⁺]₀ and [Ca²⁺]₀ directly influence the firing rate. Firing stops in Na⁺-free saline, but is enhanced by Ca²⁺-free or high-Mg²⁺ saline. TTX does not affect firing. Relatively high concentrations of Co²⁺ and La³⁺ (2 × 10^?3M) strongly inhibit CDC. Regular firing can be changed into bursting by various means, such as high K⁺ or addition of 1 mM Ba²⁺. Bursting normally occurs at the beginning of the afterdischarge. Postburst hyperpolarizations are reduced in Ca²⁺-free saline and by low Co²⁺ (10^?4-5 10^?4M). Active CDC are driven by a pacemaking mechanism constituted by a voltage-dependent Na⁺/Ca²⁺ channel and a Ca²⁺-dependent K⁺ channel, thus resembling that of bursting pacemakers. The pacemaking mechanism is inactive in the resting and inhibited state.     

Effect of cytoplasmic acidification on the membrane potential of T-lymphocytes: Role of trace metals

Summary The effect of lowering intracellular pH on the membrane potential (E _m ) of rat thymic lymphocytes was studied using the potential-sensitive dyebis-oxonol. Cells were acid loaded by addition of the electroneutral K⁺/H⁺ exchanging ionophore nigericin. Acidification to pH 6.3 in Na⁺-free solution resulted in a biphasic change inE _m : an early transient hyperpolarization followed by a sustained depolarization. These changes were associated with a rise in cytosolic free Ca²⁺ ([Ca²⁺] _i ). The hyperpolarization was eliminated when the change in [Ca²⁺] _i was prevented using BAPTA, an intracellular Ca²⁺ chelator. Moreover, a similar hyperpolarization was elicited by elevation of [Ca²⁺] _i at physiological pH _i using ionomycin, suggesting involvement of Ca²⁺-activated K⁺ channels. In contrast, the depolarization phase could not be mimicked by raising [Ca²⁺] _i with ionomycin. However, intracellular BAPTA effectively inhibited the acidificationinduced depolarization. Inhibition was also obtained by extracellular addition of EGTA or dithiothreitol, even when the external free Ca²⁺ concentration remained unaltered. These observations suggested a possible role of contaminating trace metals. Cytosolic acidification is envisaged to induce intracellular accumulation of one or more trace metals, which induces the observed changes inE _m . Accordingly, similar changes inE _m can be induced without acidification by the addition of small amounts of Cu²⁺ to the medium. The ionic basis of theE _m changes induced by acidification and the significance of these observations are discussed.     

Simulation of intracellular Ca2+ oscillation in a sympathetic neurone

Three different theoretical models were considered for the mechanism of the oscillation of the intracellular free Ca²⁺ ([Ca²⁺]_i) linked to the K⁺ conductance of the plasma membrane (G_K) observed in bullfrog sympathetic ganglion cells. The models assumed a Ca²⁺-induced Ca²⁺ release mechanism, an active Ca²⁺ uptake mechanism at a Ca²⁺ reservoir site in the ganglion cell, and a Michaelis—Menten type relationship between [Ca²⁺]_i and G_K. Including both active and passive Ca²⁺ transport mechanisms at the plasma membrane, either a one-compartment model or a two-compartment model for the intracellular Ca²⁺ store reconstructed successfully the [Ca²⁺]_i oscillation and rhythmic membrane hyperpolarizations observed in the ganglion cell, and simulated most of their characteristics. On the other hand, a two-compartment model disregarding of Ca²⁺ transport at the plasma membrane failed to reproduce the oscillations of [Ca²⁺]_i and membrane potential.     

Ca2+-activated K+ conductance of the human red cell membrane: Voltage-dependent Na+ block of outward-going currents

Summary Human red cells were prepared with various cellular Na⁺ and K⁺ concentrations at a constant sum of 156mm. At maximal activation of the K⁺ conductance,g _K(Ca), the net efflux of K⁺ was determined as a function of the cellular Na⁺ and K⁺ concentrations and the membrane potential,V _m , at a fixed [K⁺]_ex of 3.5mm.V _m was only varied from (V _m –E _K)25 mV and upwards, that is, outside the range of potentials with a steep inward rectifying voltage dependence (Stampe & Vestergaard-Bogind, 1988).g _K(Ca) as a function of cellular Na⁺ and K⁺ concentrations atV _m =–40, 0 and 40 mV indicated a competitive, voltage-dependent block of the outward current conductance by cellular Na⁺. Since the present Ca²⁺-activated K⁺ channels have been shown to be of the multi-ion type, the experimental data from each set of Na⁺ and K⁺ concentrations were fitted separately to a Boltzmann-type equation, assuming that the outward current conductance in the absence of cellular Na⁺ is independent of voltage. The equivalent valence determined in this way was a function of the cellular Na⁺ concentration increasing from 0.5 to 1.5 as this concentration increased from 11 to 101mm. Data from a previous study of voltage dependence as a function of the degree of Ca²⁺ activation of the channel could be accounted for in this way as well. It is therefore suggested that the voltage dependence ofg _K(Ca) for outward currents at (V _m –E _K)>25 25 mV reflects a voltage-dependent Na⁺ block of the Ca²⁺-activated K⁺ channels.     

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.