Depolarization of macrophage polykaryons in the absence of external sodium induces a cyclic stimulation of a calcium-activated potassium conductance

Macrophage polykaryons associated with the foreign body granuloma display several electrophysiological properties when studied with intracellular microelectrodes. One of the most evident properties is the slow hyperpolarization (2-5 s long, 10-60 mV amplitude), due to transient openings of Ca2+-dependent K+ channels, that is similar to those observed in macrophages. How this oscillation of membrane potential is triggered is not well known and the only way to repeatedly activate it under experimental control is through the intracellular injection of Ca2+. Although this technique is important for understanding the properties of the K+ channels, no information has been obtained about the way Ca2+ levels are raised and controlled in the cytosol. Slow hyperpolarizations can also be triggered by electrical stimulation, but reproducibility is low with cells bathed in physiological solutions. We then decided to investigate the effect of depolarization on the electrophysiological properties of macrophage polykaryons exposed to bathing solutions of several ionic compositions. We show in this paper that cell membrane depolarization induced by a long current pulse can trigger several patterns of membrane potential changes and that, in the absence of extracellular Na+, repetitive oscillations of decaying amplitudes are observed in almost all the cells. They are very similar to the slow hyperpolarizations, are dependent on the presence of extracellular Ca2+, and are blocked by quinine and D-600. Whole-cell patch clamp recording under voltage clamp conditions showed an outward current that oscillates and that also exhibits decaying amplitudes. The data presented here indicate that these oscillations are a consequence of the cyclic opening of the Ca2+-activated K+ channels and support the hypothesis that favors the participation of Ca2+ channels and of the Ca2+/Na+ exchange system in their triggering. These two mechanisms are not enough to explain either why the K+ channels close or why the membrane potential returns to the original level at the end of each cycle. The possibility of using these oscillations as a model to study the slow hyperpolarization is discussed.     

Spontaneous action potentials and resting potential shifts in fertilized eggs of the tunicate Clavelina

Electrical activity in the fertilized egg of the tunicate Clavelina was studied with microelectrode recording and voltage clamp techniques. The resting potential could assume either of two stable values (approximately ?70 or ?30 mV) and could be shifted between these values by direct current stimulation. Spontaneous shifts between two stable resting potentials were also seen. Egg cells produced action potentials spontaneously and in response to depolarizing stimuli. Inward currents were carried by both Na and Ca ions and a prominent outward potassium current was seen with depolarization to voltages above ?15 mV. The steady-state current-voltage relationship (I–V curve) of the membrane showed two voltages where the net membrane current equaled zero: approximately ?35 and ?70 mV. Between these two voltages, membrane current was inward and carried by noninactivating Na and Ca currents. Inward rectification, which was blocked by external Rb, occurred at voltages below ?70 mV. The voltage dependence of inward rectification is thought by the authors to be important for establishing the more negative resting potential; it is also thought the presence of inward current which does not inactivate completely at voltages more negative than about ?20 mV is an important determinant of the more depolarized resting potential.     

Inositol trisphosphate-induced hyperpolarization in rat dorsal root ganglion neurons.

Inositol 1,4,5-trisphosphate (1,4,5-InsP3) was perfused into rat dorsal root ganglion (DRG) neurons by whole-cell patch-clamp electrodes, while measuring the membrane potential. This operation evoked a transient (2-3 min) membrane hyperpolarization of about -15 mV (from -42 mV) followed by a depolarization. The membrane hyperpolarization was abolished when 30 mM EGTA was perfused together with 1,4,5-InsP3 or when 0.2 mM quinine was added to the bath solution. The hyperpolarizing response was enhanced when a low-Ca2+ EGTA-free intracellular solution was used. Two InsP2 isomers induced a different response. Our results suggest that the hyperpolarization is due to 1,4,5-InsP3-induced Ca2+ release which may trigger Ca-sensitive K+ channels to open. Present results show that cultured DRG neurons are able to respond to 1,4,5-InsP3 perfusion in the whole-cell configuration.     

TheBulla ocular circadian pacemaker

In an effort to understand the cellular basis of entrainment of circadian oscillators we have studied the role of membrane potential changes in the neurons which comprise the ocular circadian pacemaker of Bulla gouldiana in mediating phase shifts of the ocular circadian rhythm. We report that: 1. Intracellular recording was used to measure directly the effects of the phase shifting agents light, serotonin, and 8-bromo-cAMP on the membrane potential of the basal retinal neurons. We found that light pulses evoke a transient depolarization followed by a smaller sustained depolarization. Application of serotonin produced a biphasic response; a transient depolarization followed by a sustained hyperpolarization. Application of a membrane permeable analog of the intracellular second messenger cAMP, 8-bromo-cAMP, elicited sustained hyperpolarization, and occasionally a weak phasic depolarization. 2. Changing the membrane potential of the basal retinal neurons directly and selectively with intracellularly injected current phase shifts the ocular circadian rhythm. Both depolarizing and hyperpolarizing current can shift the phase of the circadian oscillator. Depolarizing current mimics the phase shifting action of light, while hyperpolarizing current produces phase shifts which are transposed approximately 180 degrees in circadian time to depolarization. 3. Altering BRN membrane potential with ionic treatments, depolarizing with elevated K+ seawater or hyperpolarizing with lowered Na+ seawater, produces phase shifts similar to current injection. 4. The light-induced depolarization of the basal retinal neurons is necessary for phase shifts by light. Suppressing the light-induced depolarization with injected current inhibits light-induced phase shifts. 5. The ability of membrane potential changes to shift oscillator phase is dependent on extracellular calcium. Reducing extracellular free Ca++ from 10 mM to 1.3 X 10(-7) M inhibits light-induced phase shifts without blocking the photic response of the BRNs. The results indicate that changes in the membrane potential of the pacemaker neurons play a critical role in phase shifting the circadian rhythm, and imply that a voltage-dependent and calcium-dependent process, possibly Ca++ influx, shifts oscillator phase in response to light.     

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.     

Mechanism of trace hyperpolarization of the action potential of snail giant neurons]

Depolarization current decreases and hyperpolarization current increases the amplitude of tracing hyperpolarization of the neuron action potential. Calcium-defficient solution supresses the tracing depolarization, and turns the rhythmical activity of the neuron into the flashlike one. An increase of outer concentration of potassium ions decreases the tracing depolarization. The latter is suppressed completely when the membrane behaves as a potassium electrode. The suppressing effect of the increase of potassium outer concentration on tracing hyperpolarization decreases with a decrease of calcium ions content in the medium. When an active release of sodium ions from the cell is inhibited with DNP and substitution of sodium ions by lithium ions the tracing hyperpolarization of the action potential is suppressed. The tracing hyperpolarization is also suppressed during the shunting of the electrogenic effect of potassium pump with the outcoming current of chlorine ions. It is suggested that the tracing hyperpolarization of the single action potential is due to the calcium-dependent fraction of electrogenic release of sodium ions from the cell.     

Contributions of various ions to the resting and action potentials of crayfish medial giant axons

Summary The membrane of crayfish medial giant axons is permeable at rest to ions in the rank K>Na>Ca>Cl. With K present, variation of the other ions has little or no effect, but with K absent the axon hyperpolarizes when Na is reduced or eliminated by replacement with Tris (slope ca. 30 mV/decade Na₀). The hyperpolarization is independent of the presence of Cl or its absence (substitution with methanesulfonate or isethionate). The resistance increases progressively as Na is removed. These changes persist after the spike is blocked with tetrodotoxin. An increase in Ca causes depolarization (slope ca. 20 mV/decade) provided K, Na and Cl are all absent, but in the presence of Cl there is little or no change in membrane potential on increasing Ca to 150mm. The depolarization induced by Ca is associated with an increased resistance. Spike electrogenesis involves Ca activation as well as Na activation, but the after-depolarization at the end of the spike is due to a conductance increase for Ca. Two alternative equivalent circuits for the resting and active membrane are discussed.     

Control of action potential-driven calcium influx in GT1 neurons by the activation status of sodium and calcium channels

An analysis of the relationship between electrical membrane activity and Ca2+ influx in differentiated GnRH-secreting (GT1) neurons revealed that most cells exhibited spontaneous, extracellular Ca(2+)-dependent action potentials (APs). Spiking was initiated by a slow pacemaker depolarization from a baseline potential between -75 and -50 mV, and AP frequency increased with membrane depolarization. More hyperpolarized cells fired sharp APs with limited capacity to promote Ca2+ influx, whereas more depolarized cells fired broad APs with enhanced capacity for Ca2+ influx. Characterization of the inward currents in GT1 cells revealed the presence of tetrodotoxin-sensitive Na+, Ni(2+)-sensitive T-type Ca2+, and dihydropyridine-sensitive L-type Ca2+ components. The availability of Na+ and T-type Ca2+ channels was dependent on the baseline potential, which determined the activation/inactivation status of these channels. Whereas all three channels were involved in the generation of sharp APs, L-type channels were solely responsible for the spike depolarization in cells exhibiting broad APs. Activation of GnRH receptors led to biphasic changes in cytosolic Ca2+ concentration ([Ca2+]i), with an early, extracellular Ca(2+)-independent peak and a sustained, extracellular Ca(2+)-dependent phase. During the peak [Ca2+]i response, electrical activity was abolished due to transient hyperpolarization. This was followed by sustained depolarization of cells and resumption of firing of increased frequency with a shift from sharp to broad APs. The GnRH-induced change in firing pattern accounted for about 50% of the elevated Ca2+ influx, the remainder being independent of spiking. Basal [Ca2+]i was also dependent on Ca2+ influx through AP-driven and voltage-insensitive pathways. Thus, in both resting and agonist-stimulated GT1 cells, membrane depolarization limits the participation of Na+ and T-type channels in firing, but facilitates AP-driven Ca2+ influx.     

Parallel oscillations of intracellular calcium activity and mitochondrial membrane potential in mouse pancreatic B-cells

Insulin secretion in normal B-cells is pulsatile, a consequence of oscillations in the cell membrane potential (MP) and cytosolic calcium activity ([Ca(2+)](c)). We simultaneously monitored glucose-induced changes in [Ca(2+)](c) and in the mitochondrial membrane potential DeltaPsi, as a measure for ATP generation. Increasing the glucose concentration from 0.5 to 15 mM led to the well-known hyperpolarization of DeltaPsi and ATP-dependent lowering of [Ca(2+)](c). However, as soon as [Ca(2+)](c) rose due to the opening of voltage-dependent Ca(2+) channels, DeltaPsi depolarized and thereafter oscillations in [Ca(2+)](c) were parallel to oscillations in DeltaPsi. A depolarization or oscillations of DeltaPsi cannot be evoked by a substimulatory glucose concentration, but Ca(2+) influx provoked by 30 mM KCl was followed by a depolarization of DeltaPsi. The following feedback loop is suggested: Glucose metabolism via mitochondrial ATP production and closure of K(+)(ATP) channels induces an increase in [Ca(2+)](c). The rise in [Ca(2+)](c) in turn decreases ATP synthesis by depolarizing DeltaPsi, thus transiently terminating Ca(2+) influx.     

Properties of the slow excitatory postsynaptic potential in mammalian sympathetic ganglion cells

Two types of slow excitatory postsynaptic potentials (EPSPs) with different properties were found in neurons of the rabbit superior cervical sympathetic ganglion. In our group of neurons slow EPSPs increased during artificial hyperpolarization and decreased during depolarization of the membrane. The input resistance of the cells fell or remained unchanged during the development of slow EPSPs. In the second group of cells slow EPSPs increased during depolarization and decreased during hyperpolarization. The reversal potential of these responses, determined by extrapolation, was –78.9±3.6 mV. Depolarization responses to activation of muscarinic cholinergic receptors by acetylcholine or carbachol developed in 53% of neurons with an increase in input resistance and had a reversal potential of –83.2±6.7 mV. It is suggested that in cells of the first group the ionic mechanism of the slow EPSPs is similar to that of the fast EPSPs, whereas in cells of the second group its main component is a decrease in the potassium conductance of the membrane.A. A. Bogomolets Institute of Physiology, Academy of Sciences of the Ukrainian SSR, Kiev. Translated from Neirofiziologiya, Vol. 13, No. 4, pp. 371–379, July–August, 1981.     

A low voltage-activated calcium conductance in embryonic chick sensory neurons.

Isolated Ca currents in cultured dorsal root ganglion (DRG) cells were studied using the patch clamp technique. The currents persisted in the presence of 30 microM tetrodotoxin (TTX) or when external Na was replaced by choline. They were fully blocked by millimolar additions of Cd2+ and Ni2+ to the bath. Two components of an inward-going Ca current were observed. In 5 mM external Ca, a current of small amplitude, turned on already during steps changes to -60 mV membrane potential, leveled off at -30 mV to a value of approximately 0.2 nA. A second, larger current component, which resembled the previously described Ca current in other cells, appeared at more positive voltages (-20 to -10 mV) and had a maximum approximately 0 mV. The current component activated at the more negative membrane potentials showed the stronger dependence on external Ca. The presence of a time- and a voltage-dependent activation was indicated by the current's sigmoidal rise, which became faster with increased depolarization. Its tail currents were generally slower than those associated with the Ca currents of larger amplitude. From -60 mV holding potential, the maximum obtainable amplitude of the low depolarization-activated current was only one-tenth of that achieved from a holding potential of -90 mV. Voltage-dependent inactivation of this current component was fast compared with that of the other component. The properties of this low voltage-activated and fully inactivating Ca current suggest it is the same as the inward current that has been postulated in several central neurons (Llinas, R., and Y. Yarom, 1981, J. Physiol. (Lond.), 315:569-584), which produce depolarizing potential waves and burst-firing only when membrane hyperpolarization precedes.     

Caffeine-induced oscillations of the membrane potential inAplysia neurons

It has been found in culturedAplysia neurons, including L7 and L2–L6 neurons, that bath application of 40 mM caffeine evokes oscillations of the membrane potential (MP) with the amplitude of about 40 mV. The frequency of oscillations, on the crest of which action potentials (AP) arise, varied from 0.2 to 0.5 sec¹. The effect of caffeine was completely reversible. The MP waves demonstrated high sensitivity to membrane polarization: artificial depolarization increased the frequency of oscillations, while even subtle hyperpolarization resulted in a decrease in the frequency up to their complete disappearance. External application of CdCl₂ (1 mM), a nonspecific blocker of calcium channels, or ryanodine (50 μM, 20 min), release of Ca²⁻ from the intracellular stores, replacement of Ca²⁺ in the external medium by Mg²⁻, or Na⁺ by Li⁺, did not exert visible effect on the parameters of MP waves. It was concluded that Ca ions (changing of intracellular concentration of which is due to such processes as inward calcium current, ryanodine-sensitive caffeine-induced calcium release from the intracellular, stores, sodium-calcium exchange through the plasma membrane) do not play any significant part in generation of the MP waves. The most probable mechanism of caffeine-induced oscillations in the studied nerve cells is inhibition of voltage-activated outward potassium current and, as could be seen from our mathematical modeling, slowdown of inactivation of inward sodium current. It seems likely that these oscillations have a purely membrane origin. Neirofiziologiya/Neurophysiology, Vol. 32, No. 2, pp. 102–111, March–April, 2000.     

Mechanisms of membrane potential oscillation in bursting neurons on the snail,Helix pomatia

• 1.1. The mechanism of generation of membrane potential (MP) oscillations was studied in identified bursting neurons from the snail Helix pomatia.
• 2.2. Long-lasting stimulation of an identified peptidergic interneuron produced a persistent bursting activity in a non-active burster.
• 3.3. External application of calcium channel blockers (1 mM Cd²⁺ or 5 mM La²⁺) resulted in a transient increase in the slow-wave amplitude and subsequent prevention of pacemaker activity generation in bursting neurons. Application of these blockers together with endogenous neuropeptide initiating bursting activity generation, increased MP wave amplitude without prevention of bursting activity generation.
• 4.4. Replacement of all NaCl in normal Ringer's solution with isoosmotic CaCl₂, glucose or Tris-HCl produced a reversible block of bursting activity generation. Stationary current-voltage relation (CVR) of bursting neuron membrane has a region of negative resistance (NRR) and does not intersect the potential axis in threshold region for action potential (AP) generation in normal Ringer's solution. In Na-free solution stationary CVR is linear and intersects the potential axis near — 52 mV.
• 5.5. Novel potential- and time-dependent outward (E_rev = − 58 mV) current, I_B, activated by hyperpolarization was found in the bursting neuron membrane. Having achieved a maximal value, this current decayed with a time constant of about 1 sec. Hyperpolarization inactivated maximal conductance, g_B, responsible for I_B, and depolarization abolished inactivation of g_B.
• 6.6. Short-lasting (0.01 sec) hyperpolarization of the bursting neuron membrane by inward current pulse induced the development of prolonged hyperpolarization wave lasting up to 10 sec.
• 7.7. These results suggest that: (a) persistent bursting activity of RPal neuron in the snail Helix pomatia is not endogenous but is due to a constant activation of peptidergic synaptic inputs of these neurons; (b) Ca²⁺ ions do not play a pivotal role in the ionic mechanism of MP oscillations but play a determining role in the process of secretion of a peptide initiating bursting activity by the interneuron presynaptic terminal; (c) depolarizing phase of the MP wave is due to specific properties of stationary CVR and hyperpolarization phase is due to regenerative properties of hyperpolarization-activated outward current I_B. The minimal mathematical version of MP oscillations based on the experimental data is presented.

     

In vivo electrophysiological evidences for cortical neuron-glia interactions during slow (<1 Hz) and paroxysmal sleep oscillations.

The cortical activity results from complex interactions within networks of neurons and glial cells. The dialogue signals consist of neurotransmitters and various ions, which cross through the extracellular space. Slow (<1 Hz) sleep oscillations were first disclosed and investigated at the neuronal level where they consist of an alternation of the membrane potential between a depolarized and a hyperpolarized state. However, neuronal properties alone could not account for the mechanisms underlying the oscillatory nature of the sleeping cortex. Here I will show the behavior of glial cells during the slow sleep oscillation and its relationship with the variation of the neuronal membrane potential (pairs of neurons and glia recorded simultaneously and intracellularly) suggesting that, in contrast with previous assumptions, glial cells are not idle followers of neuronal activity. I will equally present measurements of the extracellular concentration of K(+) and Ca(2+), ions known to modulate the neuronal excitability. They are also part of the ionic flux that is spatially buffered by glial cells. The timing of the spatial buffering during the slow oscillation suggests that, during normal oscillatory activity, K(+) ions are cleared from active spots and released in the near vicinity, where they modulate the excitability of the neuronal membrane and contribute to maintain the depolarizing phase of the oscillation. Ca(2+) ions undergo a periodic variation of their extracellular concentration, which modulates the synaptic efficacy. The depolarizing phase of the slow oscillation is associated with a gradual depletion of the extracellular Ca(2+) promoting a progressive disfacilitation in the network. This functional synaptic neuronal disconnection is responsible for the ending of the depolarizing phase of the slow oscillation and the onset of a phasic hyperpolarization during which the neuronal network is silent and the intra- and extracellular ionic concentrations return to normal values. Spike-wave seizures often develop during sleep from the slow oscillation. Here I will show how the increased gap junction communication substantiates the facility of the glial syncytium to spatially buffer K(+) ions that were uptaken during the spike-wave seizures, and therefore contributing to the long-range recruitment of cortical territories. Similar mechanisms as those described during the slow oscillation promote the periodic (2-3 Hz) recurrence of spike-wave complexes.     

Veratridine-induced oscillations in membrane potential of cultured rat skeletal muscle: Role of the Na-K pump

1. The acute effects of veratridine on membrane potential (Em) and Na-K pump activity in cultured skeletal muscle were examined. 2. At a concentration of 10(-4) M, veratridine caused depolarization of Em and a decrease in Na-K pump activity. At concentrations of 10(-5) and 10(-6) M, veratridine caused oscillations of Em and an increase in Na-K pump activity compared to untreated, control cells. The oscillations consisted of depolarization to about -40 mV followed by hyperpolarization to about -90 mV; the level of hyperpolarization was higher at 37 than at 23 degrees C. 3. Veratridine-induced oscillations could be prevented by pretreatment with tetrodotoxin (10(-6) M) and blocked or prevented by ouabain, which depolarizes Em of cultured myotubes. In contrast, depolarization of Em to -60 mV by excess K+ did not alter the amplitude or frequency of the oscillations. 4. The results demonstrate that veratridine-induced increase in Na influx both depolarizes cultured myotubes and increases the activity of the Na-K pump, which repolarizes Em to levels higher than control. This sequence accounts for veratridine-induced oscillations in Em. High concentrations of veratridine cause only depolarization of Em and inhibition of Na-K pump activity.     

The action of substance P on neurons of the myenteric plexus of the guinea-pig small intestine.

Extracellular and intracellular recordings were made in vitro from single neurons of the myenteric plexus of the guinea-pig small intestine. Synthetic substance P was applied to the neurons by means of the perfusing solution or by electrophoresis from micropipettes. Extracellular recording showed that substance P (100 pm-30 nm), applied by perfusion, increased the firing rate of myenteric neurons. Intracellular recording indicated that perfusion with substance P caused a dose-dependent membrane depolarization which was unaffected by hexamethonium, hyoscine, naloxone or baclofen. The depolarization was also evoked by electrophoretic application of substance P. It was associated with an increase in membrane resistance, augmented by membrane depolarization and reduced by membrane hyperpolarization. The relation between the substance P reversal potential and the logarithm of the extracellular potassium concentration was linear with a slope of 54 mV/log10[K+], which indicates that substance P inactivates the resting potassium conductance of the myenteric neurons. This effect on ion conductance is the same as that of an unknown substance that mediates slow synaptic excitations with the myenteric plexus.     

Is inward calcium current in crayfish muscle membrane constituted of one or two components?

Two inward currents were observed in crayfish muscle membrane during depolarization steps by the method described by Adrian et al. (1970). Under voltage clamp conditions, hyperpolarization steps elicited a large current (leak current If), associated with an inward voltage dependent current. This inward current was inhibited by niflumic acid (NA), a drug known to block Cl---HCO-3 exchange (Cousin et Motais 1982; Br?lè et al. 1983b). Dynamic outward currents triggered by depolarizing steps were inhibited to a great extent by TEA, the not inhibited portion disappearing when procaine (2 mmol/l) was added to external solution. In the presence of TEA, procaine and NA, it was thus possible to dissect the regenerative calcium current (ICa) into two components: a "fast component" (ICa1) and a "slow component" (ICa2). The reversal potential of ICa was 65 mV (for [Ca]0 = 2.8 mmol/l), and [Ca]i could be calculated to be 1.6 X 10(-5) mol/l. This value of [Ca]i is the same as calculated from values reported by Hencek and Zachar (1977). ICa1 was triggered at a threshold membrane potential of -45 mV and ICa2 at -30 mV. Moreover, the inactivation kinetics for ICa1 was faster than that for ICa2. Our results are in perfect agreement with those obtained by Zahradník and Zachar (1982) who postulated two populations of calcium channels.     

"Action potentials" in Neurospora crassa, a mycelial fungus.

Occasional spontaneous "action potentials" are found in mature hyphae of the fungus Neurospora crassa. They can arise either from low-level sinusoidal oscillations of the membrane potential or from a linear slow depolarization which accelerates into a rapid upstroke at a voltage 5-20 mV depolarized from the normal resting potential (near-180 mV). The "action potentials" are long-lasting, 1-2 min and at the peak reach a membrane potential near-40 mV. A 2-to 8-fold increase of membrane conductance accompanies the main depolarization, but a slight decrease of membrane conductance occurs during the slow depolarization. Two plausible mechanisms for the phenomenon are (a) periodic increases of membrane permeability to inorganic ions, particularly H+ or Cl- and (b) periodic decreases in activity of the major electrogenic pump (H+) or the Neurospora membrane, coupled with a nonlinear (inverse signoid) current-boltage relationship. Identification of action potential-like disturbances in fungi means that such behavior has now been found in all major biologic taxa which have been probed with suitable electrodes. As yet there is no obvious function for the events in fungi.     

Membrane currents induced by inflow of sodium ions into mollusk giant neurons

Membrane currents induced by inflow of sodium ions were investigated in giant neurons of the molluskHelix pomatia during tetanic stimulation or prolonged membrane depolarization under voltage clamp conditions. The membrane current thus produced consists of two components, a fast component with a reversal potential close to the potassium equilibrium potential, and a slow component only slightly dependent on membrane potential in the region from −50 to −90 mV. Addition of strophanthin K to the external solution, or replacement of sodium in the external solution by lithium or calcium abolished the slow component of the membrane current and reduced the fast component. It is concluded that the slow component appears as the result of activation of the sodium pump under electrogenic conditions, where-as the fast component arises as the result of an increase in potassium permeability, possibly coupled with intensive activity of this pump.     

Slowly activating K+ channels in rat olfactory receptor neurons.

Patch-clamp techniques were used to investigate slowly activating, Ca(2+)-insensitive K+ channels of isolated rat olfactory receptor neurons. These channels had a unitary conductance of 135 pS and were only found in a small proportion (less than 5%) of membrane patches. Upon depolarization to voltages more positive than -50 mV, the channels activated gradually over a period of at least 10 s. When hyperpolarized to negative voltages, channel activity deactivated in a slow but voltage-dependent manner. These channels may underlie a slowly activating K+ current that is observed in approximately 30% of whole-cell recordings. Similar single channels have been reported in smooth muscle cells, but this is the first demonstration of these channels in any type of neuron. The channels may contribute to the spike frequency adaptation and post-stimulus hyperpolarization that are observed during the excitatory response to odorants. They may also contribute to cell repolarization following large odorant-stimulated receptor currents.