Conditioning prepulses and kinetics of potassium conductance in the frog node

Summary The kinetics of potassium conductance were analyzed in response to voltage-clamp steps with holding potential (–75 mV) as initial condition and after a positive prepulse to-wards +45 mV of 10-msec duration. As the potassium reversal potentialE _K altered during potassium current flow, a method to obtain the conductance independent ofE _K was used. Conductance kinetics at 15°C were analyzed according to the Hodgkin-Huxley (HH) model. The time constant of potassium activation, with holding potential as initial condition, is a monotonous decreasing function of membrane potential. Its value ofca. 9 msec at –50 mV decreases to 1 msec at +30 mV. Changes inE _K did not affect the voltage dependency of this time constant. The time constant of potassium deactivation, i.e. the off-response following a 10-msec prepulse towards +45 mV, shows a completely different voltage dependency. At a membrane potential of –90 mV it is approximately 2 msec and gradually increases for more positive voltages towards a maximum value of about 6 msec, that is reached between –5 and 0 mV. At still larger values of membrane voltage this time constant starts to fall again. It is concluded that a HH-model, as applied for a single population of potassium channels, has to be rejected. Computer simulations indicate that an extension to two populations of independent potassium channels, each with HH-kinetics, is also inconsistent with the observed results.     

Slow low-threshold potassium current inHelix pomatia neurons

A low-threshold outward current was studied in the neurons ofHelix pomatia at –70 to –30 mV using a two-electrode voltage clamp technique. In addition to the well-known A current (I _A), a slower outward current calledI _As (slow) was revealed. Activation and inactivation times ofI _As at –40 mV ranged from 90 to 120 msec and from 3 to 5 sec, respectively. The current recovered within 2 to 5 sec after inactivation at –120 mV. Analysis of changes in the reversal potential ofI _As caused by an increase in external potassium concentration suggests a potassium origin forI _As. The curves ofI _As stationary activation and inactivation fit the Boltzmann equation. Deriving from an activation curve, the activation potential for a half-maximum current,, is –40 mV, and the slope factor,k, is –9.8 mV, while those values for the inactivation curve are –84 mV (a half-maximum inactivation) and 7.5 mV.I _As is blocked by 4-aminopyridine (1–30 µM), tetraethylammonium (1 mM), and Ba²⁺ (1 mM), but is resistant to Cs⁺ (1 mM). PeakI _As is not affected either by substitution of external Ca²⁺ for Mg²⁺ or by application of Cd²⁺ (0.5–1.0 mM). The results suggest that activation ofI _As does not require Ca²⁺ entry into the cell.Neirofiziologiya/Neurophysiology, Vol. 25, No. 6, pp. 427–432, November–December, 1993.     

Electrophysiological and Theoretical Analysis of Depolarization-Dependent Outward Currents in the Dendritic Membrane of an Identified Nonspiking Interneuron in Crayfish

Depolarization-dependent outward currents were analyzed using the single-electrode voltage clamp technique in the dendritic membrane of an identified nonspiking interneuron (LDS interneuron) in situ in the terminal abdominal ganglion of crayfish. When the membrane was depolarized by more than 20 mV from the resting potential (65.0 ± 5.7 mV), a transient outward current was observed to be followed by a sustained outward current. Pharmacological experiments revealed that these outward currents were composed of 3 distinct components. A sustained component (I _s) was activated slowly (half rise time > 5 msec) and blocked by 20 mM TEA. A transient component (I _t1) that was activated and inactivated very rapidly (peak time < 2.5 msec, half decay time < 1.2 msec) was also blocked by 20 mM TEA. Another transient component (I _t2) was blocked by 100 M 4AP, activated rapidly (peak time < 10.0 msec) and inactivated slowly (half decay time > 131.8 msec). Two-step pulse experiments have revealed that both sustained and transient components are not inactivated at the resting potential: the half-maximal inactivation was attained at –21.0 mV in I _t1, and –38.0 mV in I _t2. I _s showed no noticeable inactivation. When the membrane was initially held at the resting potential level and clamped to varying potential levels, the half-maximal activation was attained at –36.0 mV in I _s, –31.0 mV in I _t1 and –40.0 mV in I _t2. The activation and inactivation time constants were both voltage dependent. A mathematical model of the LDS interneuron was constructed based on the present electrophysiological records to simulate the dynamic interaction of outward currents during membrane depolarization. The results suggest that those membrane conductances found in this study underlie the outward rectification of the interneuron membrane as well as depolarization-dependent shaping of the excitatory synaptic potential observed in current-clamp experiments.     

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.     

Electrogenic and diffusive components of the membrane ofHydrodictyon africanum

Summary In cells of the freshwater algaHydrodictyon africanum, in solutions where [K⁺]₀=0.1mm and pH₀>7.0, the membrane in the light is hyperpolarized. The membrane potential difference {ie179-1} has values from –180 to –275 mV, more negative than any ion diffusion potential difference, and is predominantly a function of pH₀, and independent of [K⁺]₀. The hyperpolarization of the membrane appears to arise from an electrogenic efflux of H⁺, estimated from voltage-clamp data to be about 8 nmol m^–2 sec^–1 when pH₀=8.5. In the light the membrane conductanceg _m is about 0.084 S m^–2. At light-off, {ie179-2} becomes less negative, with a halftime for change of 15 to 30 sec andg _m decreases by about 0.052 S m^–2. After dark periods of up to 300 sec, {ie179-3} is largely independent of pH₀ for values greater than 6.0 and usually behaves as a combined K⁺ and Na⁺ diffusion potential with permeability ratioP _Na/P _K=0.05 to 0.2. The membrane potassium conductanceg _K has either a low value of 2–6×10^–2 Sm^–2, or a high value of up to 18×10^–2 S m^–2 depending on [K⁺]₀, the transition from low to high values occurring when {ie179-4} moves over a threshold value that is more negative than {ie179-5}, the electrochemical equilibrium potential for K⁺. The time for half-change of the transition is about 30 sec. The results are consistent with a model of the membrane in which the pump electromotive force and conductance are in parallel with diffusive electromotive forces and conductances. When the pump is operating its properties determine membrane properties, and when it is inoperative, or running at a diminished rate, the membrane properties are determined more by the diffusive pathways. Changes in both pump rate andg _K can account for a variety of characteristic changes in membrane PD and conductance occurring in response to ligh-dark changes, changes in light intensity, pasage of externally applied electric current across the membrane and changes in ionic constituents of the external medium.     

Effect of HgCl2 on acetylcholine,carbachol, and glutamate currents ofAplysia neurons

Summary 1. Using conventional two-microelectrode voltage-clamp techniques we studied the effects of inorganic mercury (HgCl₂) on acetylcholine-, carbachol-, and glutamate-activated currents onAplysia neurons. Hg²⁺ was applied with microperfusion.2. Acetylcholine and carbachol activated an inward, sodium-dependent current in the anterior neurons of the pleural ganglion. The medial neurons gave a biphasic current to acetylcholine and carbachol, which was outward at resting membrane potential. The faster component was Cl^– dependent and reversed at about –60 mV, while the slower component was K⁺ dependent and reversed at greater than –80 mV.3. Hg²⁺ (0.1–10 µM) caused a dramatic increase in the acetylcholine- and carbachol-induced inward current in anterior neurons and the fast Cl^– current in medial neurons. With only a 1-min preapplication of Hg²⁺, the acetylcholine- or carbachol-activated sodium or chloride currents were increased to 300% and the effect was only partly reversible. The threshold concentration was 0.1 µM Hg²⁺.4. Contrary to the effects on sodium and chloride currents, concentrations of 0.1–10 µM Hg²⁺ caused a complete and irreversible blockade of K⁺-dependent acetylcholine and carbachol currents. The block of the potassium current was relatively fast and increased with time. The concentration of HgCl₂ that gave a half-maximal blockade of the carbachol-activated potassium current was 0.89 µM. The chloride-dependent current elicited by glutamate on medial neurons was increased by HgCl₂ as well.5. These results suggest that actions at agonist-activated channels must be considered as contributing to mercury neurotoxicity. It is possible that the toxic actions of Hg²⁺ on synaptic transmission at both pre- and postsynaptic sites are important factors in the mechanism of Hg²⁺ toxicity.     

Electrophysiological properties ofDictyostelium derived from membrane potential measurements with microelectrodes

Summary Electrical membrane properties of the cellular slime moldDictyostelium discoideum were investigated with the use of intracellular microelectrodes. The rapid potential transients (1 msec) upon microelectrode penetration of normal cells had a negative-going peak-shaped time course. This indicates that penetration of a cell with a microelectrode causes a rapid depolarization, which can just be recorded by the microelectrode itself. Therefore, the initial (negative) peak potential transient valueE _p (–19 mV) should be used as an indicator of the resting membrane potentialE _m ofD. discoideum before impalement, rather than the subsequent semistationary depolarized valueE _n (–5 mV). Using enlarged cells such as giant mutant cells (E _p=–39 mV) and electrofused normal cells (E _p=–30 mV) improved the reliability ofE _p as an indicator ofE _m. From the data we concluded thatE _m ofD. discoideum cells bathed in (mm) 40 NaCl, 5 KCl and 1 CaCl₂ is at least –50 mV. This potential was shown to be dependent on extracellular potassium. The average input resistanceR _i of the impaled cells was 56 M for normalD. discoideum. However, our analysis indicates that the membrane resistance of these cells before impalement is >1 G. Specific membrane capacitance was 1–3 pF/cm². Long-term recording of the membrane potential showed the existence of a transient hyperpolarization following the rapid impalement transient. This hyperpolarization was associated with an increase inR _i of the impaled cell. It was followed by a depolarization, which was associated with a decrease inR _i. The depolarization time was dependent on the filling of the microelectrode. The present characterization of the electrical membrane properties ofDictyostelium cells is a first step in a membrane electrophysiological analysis of signal transduction in cellular slime molds.     

Expression of low voltage-activated calcium channels inXenopus oocytes

Calcium channels were expressed inXenopus oocytes by means of messenger RNA extracted from the rat thalamo-hypothalamic complex, mRNA(h). Inward barium currents,I _Ba, were recorded in Cl^–-free extracellular solution with 40 mM Ba²⁺ as a charge carrier, using two-microelectrode technique. Depolarizations from a very negative holding potential (V _h=–120 mV) began to activateI _Ba at about –80 mV; this current peaked at –30 to –20 mV and reversed at +50 mV, indicating that I _Ba may be transferred through the low voltage-activated (LVA) calcium channels. The time-dependent inactivation of the current during a prolonged depolarization to –20 mV was quite slow, followed a single exponential decay with a time constant of 1550 msec, and contained a residual component constituting 30% of the maximum amplitude. The current could not be completely inactivated at any holding potential. As expected for LVA current, a steady-state inactivation curve was shifted towards negative potentials. It could be described by the Boltzmann's equation with the half-inactivation potential of –78 mV, slope factor of 15 mV, and residual level of 0.3. ExpressedI _Ba could be blocked by flunarizine (K _d=0.42 µM), nifedipine (K _d=10 µM), and amiloride at a 500 µM concentration. Among the inorganic Ca²⁺ channel blockers, the most potent was La³⁺ (K _d=0.48 µM), while Cd²⁺ and Ni²⁺ were not very selective and almost thousand-fold less effective (K _d=0.52 mM andK _d=0.62 mM, respectively) than La³⁺. Our data show that mRNA(h) induces expression in the oocytes of almost exclusively LVA Ca²⁺ channels with voltage-dependent and pharmacological properties very similar to those observed for T-type Ca²⁺ current in native hypothalamic neurons, though kinetic properties of the expressed and natural currents are somewhat different.Neirofiziologiya/Neurophysiology, Vol. 27, No. 3, pp. 183–189, May–June, 1995.     

Potassium accumulation in growing Methanobacterium thermoautotrophicum and its relation to the electrochemical proton gradient

Cultures of Methanobacterium thermoautotrophicum (Marburg) growing on media low in potassium accumulated the cation up to a maximal concentration gradient ([K⁺]_{intracellular}/[K⁺]_{extracellular}) of approximately 50,000-fold. Under these conditions, the membrane potential was determined by measuring the equilibrium distribution of the lipophilic cation (¹⁴C) tetraphenylphosphonium (TPP⁺). This cation was accumulated by the cells 350-to 1,000-fold corresponding to a membrane potential (inside negative) of 170–200 mV. The pH gradient, as measured by equilibrium distribution of the weak acid, benzoic acid, was found to be lower than 0.1 pH units (extracellular pH=6.8). The addition of valinomycin (0.5–1 nmol/mg cells) to the culture reduced the maximal concentration gradient of potassium from 50,000-to approximately 500-fold, without changing the membrane potential. After dissipation of the membrane potential by the addition of ¹²C-TTP⁺ (2 mol/mg cells) or tetrachlorosalicylanilide (3 nmol/mg cells), a rapid and complete efflux of potassium was observed.These data indicate that potassium accumulation in the absence of valinomycin is not in equilibrium with the membrane potential. It is concluded that at low extracellular K⁺ concentrations potassium is not accumulated by M. thermoautotrophicum via an electrogenic uniport mechanism.Non-common abbreviations TPP⁺ Tetra phenylphosphonium bromide - DTE Dithioerythritol - TCS 3,5,3,4-Tetrachlorosalycylanilide     

Voltage-gated ion conductances corresponding to regenerative positive and negative spikes in the dinoflagellateNoctiluca miliaris

Depolarization-activated and hyperpolarization-activated ion conductances in the membrane of a marine dinoflagellateNoctiluca miliaris were examined under voltage-clamp conditions.Noctiluca exhibited a transient inward current in response to a step depolarization from a holding potential level of –80 mV to a potential level more positive than –50 mV. The I–V relationship for the current exhibited typical N-shaped characteristics similar to those of most excitable membranes. The current was inactivated by a membrane depolarization. The reversal potential of the current shifted in hyperpolarizing direction when the external Na⁺ concentration was lowered. The transient inward current is assumed to be responsible for the Na⁺-dependent positive spike in non-clamped specimens ofNoctiluca.Noctiluca exhibited a transient outward current in response to a step hyperpolarization from a holding potential level of –20 mV to a potential level more negative than –30 mV. The I–V relationship for the current was a typical N-shape as if it was turned 180° around its origin. The outward current showed a two-step exponential time-decay. The outward current was inactivated by a membrane hyperpolarization. The reversal potential shifted in the depolarizing direction when the external Cl^– concentration was lowered. The transient outward current is responsible for the Cl^–-dependent negative spike in non-clamped specimens ofNoctiluca.Abbreviations ASW artificial seawater - TRP tentacle regulating potentials - TTX tetrodotoxin     

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.     

Intracellular potassium activity and the role of potassium in transepithelial salt transport in the human reabsorptive sweat duct

Summary We have measured the intracellular potassium activity, [K⁺]_i and the mechanisms of transcellular K⁺ transport in reabsorptive sweat duct (RSD) using intracellular ion-sensitive microelectrodes (ISMEs). The mean value of [K⁺]_i in RSD is 79.8±4.1mm (n=39). Under conditions of microperfusion, the [K⁺]_i is above equilibrium across both the basolateral membrane, BLM (5.5 times) and the apical membrane, APM (7.8 times). The Na⁺/K⁺ pump inhibitor ouabain reduced [K⁺]_i towards passive distribution across the BLM. However, the [K⁺]_i is insensitive to the Na⁺/K⁺/2 Cl^– cotransport inhibitor bumetanide in the bath. Cl^– substitution in the lumen had no effect on [K⁺]_i. In contrast, Cl^– substitution in the bath (basolateral side) depolarized BLM from –26.0±2.6 mV to –4.7^*±2.4 mV (n=3;^* indicates significant difference) and decreased [K⁺]_i from 76.0±15.2mm to 57.7^* ±12.7mm (n=3). Removal of K⁺ in the bath decreased [K⁺]_i from 76.3±15.0mm to 32.3^*±7.6mm (n=4) while depolarizing the BLM from –32.5±4.1 mV to –28.3^*±3.0 mV (n=4). Raising the [K⁺] in the bath by 10-fold increased [K⁺]_i from 81.7±9.0mm to 95.0^*±13.5mm and depolarized the BLM from –25.7±2.4 mV to –21.3^*±2.9 mV (n=4). The K⁺ conductance inhibitor, Ba²⁺, in the bath also increased [K⁺]_i from 85.8±6.7mm to 107.0^*±11.5mm (n=4) and depolarized BLM from –25.8±2.2 mV to –17.0^*±3.1 mV (n=4). Amiloride at 10^–6 m increased [K⁺]_i from 77.5±18.8mm to 98.8^*±21.6mm (n=4) and hyperpolarized both the BLM (from –35.5±2.6 mV to –47.8^*±4.3 mV) and the APM (from –27.5±1.4 mV to –46.0^* ±3.5 mV,n=4). However, amiloride at 10^–4 m decreased [K⁺]_i from 64.5±0.9mm to 36.0^*±9.9mm and hyperpolarized both the BLM (from –24.7±1.4 mV to –43.5^*±4.2 mV) and APM (from –18.3±0.9 mV to –43.5^*±4.2 mV,n=6). In contrast to the observations at the BLM, substitution of K⁺ or application of Ba²⁺ in the lumen had no effect on the [K⁺]_i or the electrical properties of RSD, indicating the absence of a K⁺ conductance in the APM. Our results indicate that (i) [K⁺]_i is above equilibrium due to the Na⁺/K⁺ pump; (ii) only the BLM has a K⁺ conductance; (iii) [K⁺]_i is subject to modulation by transport status; (iv) K⁺ is probably not involved in carrier-mediated ion transport across the cell membranes; and (v) the RSD does not secrete K⁺ into the lumen.     

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.     

Zinc modulates a-type potassium currents and neuronal excitability in snail neurons

Summary 1. Zinc-induced actions were studied on the A-current and neuronal activity in identified and unidentified nerve cells of the snail,Helix pomatia L., under voltage and current clamp conditions.2. Extracellularly applied Zn²⁺ attenuated the peak amplitude of the A-current in a potential- and dose-dependent way (K _i=1.8 mM at –30 mV,n _H=0.6).3. Attenuation of the A-currents was initiated as Zn²⁺ shifted the potential dependence of both activation and inactivation of the currents toward more positive potential values.4. Zinc concomitantly prolonged the time to peak and decay time constant of the A-currents (K _d=1.7 mM,n _H=1.4) as well.5. Zn²⁺ decreased the resting membrane potential and the spike amplitude and increased the action potential duration and the input resistance of the cells in current clamp experiments.6. A complex action of zinc increased the neuronal excitability, indicating spontaneous and synaptically evoked spike discharges.7. Common and specific zinc binding sites are supposed on vertebrate and invertebrate A-type potassium channel proteins, where binding Zn²⁺ can modulate the gating properties and kinetics of the fast outward potassium currents.     

A voltage-dependent and pH-sensitive proton current in Rana esculenta oocytes

Voltage clamp technique was used to study macroscopic ionic currents in Rana esculenta oocytes. Depolarization steps led to the activation of a single type of outward current (I _out) when contaminant potassium and calcium-dependent chloride currents were pharmacologically inhibited. The voltage threshold of I _out activation was 10 mV and this current, which did not inactivate, presented a deactivation the time constant of 73±21 msec (n=26) corresponding to a membrane voltage of –60 mV. Its reversal potential (E _rev) was dependent on the magnitude of the depolarization and also on pulse duration. These changes in E _rev were thought to reflect intracellular ion depletion occurring during activation of the remaining outward current. Furthermore, the activation threshold of I _out was clearly affected by modifications in extracellular and intracellular H⁺ concentrations. Indeed, intracellular alkalinization (evoked by external application of ammonium chloride) or extracellular acidification induced a rightward shift in the activation threshold while intracellular acidification (evoked by external application of sodium acetate) or extracellular alkalinization shifted this threshold toward a more negative value. Lastly, I _out was dramatically reduced by divalent cations such as Cd²⁺, Ni²⁺ or Zn²⁺ and was strongly decreased by 4 Aminopyridine (4-AP), wellknown H⁺ current antagonists already described in many cell types. Therefore, it was suggested that the outward current was prominently carried by H⁺ ions, which may play a key role in the regulation of intracellular pH and subsequent pH dependent processes in Rana oocyte.     

Whole-cell and single-channel currents across the plasmalemma of corn shoot suspension cells

Summary Whole-cell sealed-on pipettes have been used to measure electrical properties of the plasmalemma surrounding protoplasts isolated from Black Mexican sweet corn shoot cells from suspension culture. In these protoplasts the membrane resting potential (V _m ) was found to be –59±23 mV (n=23) in 1mm K _o ^– . The meanV _m became more negative as [K^–] _o decreased, but was more positive than the K⁺ equilibrium potential. There was no evidence of electrogenic pump activity. We describe four features of the current-voltage characteristic of the plasmalemma of these protoplasts which show voltagegated channel activity. Depolarization of the whole-cell membrane from the resting potential activates time- and voltage-dependent outward current through K⁺-selective channels. A local minimum in the outward current-voltage curve nearV _m =150 mV suggests that these currents are mediated by two populations of K⁺-selective channels. The absence of this minimum in the presence of verapamil suggests that the activation of one channel population depends on the influx of Ca²⁺ into the cytoplasm. We identify unitary currents from two K⁺-selective channel populations (40 and 125 pS) which open when the membrane is depolarized; it is possible that these mediate the outward whole-cell current. Hyperpolarization of the membrane from the resting potential produces time- and voltage-dependent inward whole-cell current. Current activation is fast and follows an exponential time course. The current saturates and in some cases decreases at membrane potentials more negative than –175 mV. This current is conducted by poorly selective K⁺ channels, whereP _Cl/P _K=0.43±0.15. We describe a low conductance (20 pS) channel population of unknown selectivity which opens when the membrane is hyperpolarized. It is possible that these channels mediate inward whole-cell current. When the membrane is hyperpolarized to potentials more negative than –250 mV large, irregular inward current is activated. A third type of inward whole-cell current is briefly described. This activates slowly and with a U-shaped current-voltage curve over the range of membrane potentials –90<V _m <0 mV.     

Membrane responses to changes in the extracellular potassium concentration in isolated hippocampal pyramidal neurons

The responses of freshly isolated hippocampal pyramidal neurons to rapid, elevations of the external potassium concentration ([K⁺] _out ) were investigated using the whole-cell variation of a patch-clamp technique. An elevation of [K⁺] _out induced a two-phase inward current at the membrane potentials more negative than the reversal potential for K ions. This current consisted of a leakage, current and a time-dependent current (τ=40–50 msec at 21°C), the latter designated below asI _ΔK. It displayed first-order activation kinetics that showed neither voltage, nor concentration dependence. The amplitude of this current was determined by the external K⁺ concentration and increased with hyperpolarization. Voltage dependence ofI _ΔK measured within the range from −20 to −120 mV was similar to that for inward rectifier. Activation ofI _ΔK was utterly dependent on Na⁺; substitution of extracellular Na⁺ with choline chloride almost completely depressedI _ΔK.I _ΔK was absent in the cells freshly dissociated from the nodosal and dorsal root ganglia. This suggests that this earlier unrecognized current is instrumental in preserving densely packed hippocampal pyramidal neurons from sudden increases in [K⁺] _out and following spontaneous over-excitation. It prevents the neurons from responding to K⁺-induced depolarizations by slowing down potassium influx.     

Factors controlling the K+ conductance inChara

Summary Previous current/voltage (I/V) investigations of theChara K⁺ state have been extended by increasing the voltage range (up to +200 mV) through blocking the action potential with La³⁺. A region of negative slope was found in theI/V characteristics at positive PD's, similar to that already observed at PD's more negative than the resting level. These decreases in membrane currents at PD's more negative than –150 mV and at PD's close to 0 or positive are thought to arise from the K⁺ channel closure. Both the negative slope regions could be reversibly abolished by 0.1mm K⁺, 20mm Na⁺, more than 10mm Ca²⁺ or 5mm tetraethylammonium (TEA). The K⁺ channels are therefore blocked by TEA, closed by low [K⁺] _o or high [Ca²⁺] _o and are highly selective to K⁺ over Na⁺. With the K⁺ channels closed, the remainingI/V profile was approximately linear over the interval of 400 mV (suggesting a leakage current), but large rectifying currents were observed at PD's more positive than +50 mV. These currents showed a substantial decrease in high [Ca²⁺] _o , sometimes displayed a slight shift to more positive PD's with increasing [K⁺] _o and were unaffected by TEA or changes in [Na⁺] _o . The slope of the linear part of theI/V profile was steeper in low [K⁺] _o than in TEA or high [Na⁺] _o (indicating participation of K⁺, but not Na⁺, in the leak current). Diethylstilbestrol (DES) was employed to inhibit the proton pump, but it was found that the leakage current and later the K⁺ channels were also strongly affected.     

Potassium channels in Eremosphaera viridis

The dependence of the membrane potential of Eremosphaera viridis on different external concentrations of potassium, sodium, calcium, and protons was compared with the diffusion potential measured in the dark and in the presence of NaN₃. In contrast to some other algae, the membrane potential in the light as well as in the dark seemed to be predominantly determined by the calculated diffusion potential and less by an electrogenic pump which, however, seemed to be involved at potassium concentrations >1 mol·m^-3 and at higher pH_os (>pH 6). Furthermore, some characteristics of an action-potential-like response (CAP) triggered by light-off, and independent of the membrane-potential threshold value, were determined. The CAP had a delay period of 5.4 s and needed 4.5 s for polarization to a plateau. On average, the plateau held for 8.8 s and the CAP lasted 37.7 s. The peak amplitudes of CAP (P _AP) exactly followed the Nernst potential of potassium. Other cations like sodium, calcium and protons did not appreciably affect the peak amplitudes of CAP. From these and other results it can be assumed that the CAP is caused by a temporary opening of potassium channels in the plasma membrane of Eremosphaera (Köhler et al., 1983, Planta 159, 165–171). The release of a CAP by light-off has been partly explained by the participation of a transient increase of proton concentration in the cytoplasm. It was possible to trigger a CAP by external pH changes and by the addition of sodium acetate, thus supporting the hypothesis that a pH decrease in the cytoplasm may be one element of the signal transfer from the photosynthetic system to the potassium channels in the plasmalemma. Calcium also seemed to have an influence on triggering the CAP.Abbreviations and symbols CAP chemical-induced action-potential-like response - E _D calculated diffusion potential (mV) - E _D ^* measured diffusion potential (mV) - E _K potassium equilibrium potential (mV) - E _m membrane potential (mV) - P _AP peak of action potential (mV) Part II will appear in Planta, Vol. 167, No. 1, 1986