Active transport of potassium by the giant neuron of the aplysia abdominal ganglion

Effects of In Vivo Intracellular ATP Modulation on Neocortical Extracellular Potassium Concentration

Neuronal and glial activity are dependent on the efflux of potassium ions into the extracellular space. Efflux of K is partly energy-dependent as the activity of pumps and channels which are involved in K transportation is ATP-dependent. In this study, we investigated the effect of decreased intracellular ATP concentration ([ATP]i) on the extracellular potassium ion concentration ([K]o). Using in vivo electrophysiological techniques, we measured neocortical [K]o and the local field potential (LFP) while [ATP]i was reduced through various pharmacological interventions. We observed that reducing [ATP]i led to raised [K]o and DC-shifts resembling spreading depolarization-like events. We proposed that most likely, the increased [K]o is mainly due to the impairment of the Na/K ATPase pump and the ATP-sensitive potassium channel in the absence of sufficient ATP, because Na/K ATPase inhibition led to increased [K]o and ATP-sensitive potassium channel impairment resulted in decreased [K]o. Therefore, an important consequence of decreased [ATP]i is an increased [K]o. The results of this study acknowledge one of the mechanisms involved in [K]o dynamics.

Neural shutdown under stress: an evolutionary perspective on spreading depolarization

Neural function depends on maintaining cellular membrane potentials as the basis for electrical signaling. Yet, in mammals and insects, neuronal and glial membrane potentials can reversibly depolarize to zero, shutting down neural function by the process of spreading depolarization (SD) that collapses the ion gradients across membranes. SD is not evident in all metazoan taxa with centralized nervous systems. We consider the occurrence and similarities of SD in different animals and suggest that it is an emergent property of nervous systems that have evolved to control complex behaviors requiring energetically expensive, rapid information processing in a tightly regulated extracellular environment. Whether SD is beneficial or not in mammals remains an open question. However, in insects, it is associated with the response to harsh environments and may provide an energetic advantage that improves the chances of survival. The remarkable similarity of SD in diverse taxa supports a model systems approach to understanding the mechanistic underpinning of human neuropathology associated with migraine, stroke, and traumatic brain injury.

Guanosine 5'-triphosphate analogue activates potassium current modulated by neurotransmitters in Aplysia neurones

1. Identified neurones in the abdominal ganglion of Aplysia californica were voltage clamped in order to investigate how guanosine 5'-O-(3-thiotriphosphate) (GTP-gamma-S), a GTP analogue that irreversibly activates guanine nucleotide-binding (G) proteins, modifies activation by the neuropeptide FMRFamide (Phe-Met-Arg-Phe-NH2) of a slow K+ current resembling the serotonin- and adenosine 3',5'-cyclic monophosphate (cyclic AMP)-sensitive 'S' current, and a similar response to acetylcholine. 2. Ionophoretic or pressure injection of GTP-gamma-S into the cell triggered the slow and irreversible development of a large K+ current, rendered the K+ current responses to FMRFamide and acetylcholine irreversible, and finally, once the GTP-gamma-S-induced current had fully developed, occluded the neurotransmitter responses altogether. 3. The K+ currents activated by GTP-gamma-S and acetylcholine had properties identical to those previously found for the FMRFamide-induced 'S'-like K+ current: they were Ca2+ and voltage independent, relatively insensitive to block by extracellular tetraethylammonium (TEA) and 4-aminopyridine (when high concentrations of acetylcholine were used to overcome an additional block by these agents of the receptor), and suppressed in Ba2+-containing solution, by injection of TEA+ or Cs+ into the cell, and by serotonin and elevation of the intracellular concentration of cyclic AMP. 4. The K+ current responses to FMRFamide and acetylcholine were not additive when the agonist concentrations used were high enough to activate most of the available current. 5. Desensitization of either response did not affect the other, and the effect of acetylcholine, but not that of FMRFamide, could be blocked by the known acetylcholine-receptor blockers phenyltrimethylammonium and TEA. 6. These results suggest that FMRFamide and acetylcholine, acting through different receptors, activate the same 'S'-like K+ current by a mechanism involving a G protein. 7. In addition to activating the slow K+ current, FMRFamide and acetylcholine each activate a faster current in these cells, carried by Na+ in the case of FMRFamide, and by Cl- in the case of acetylcholine. Neither fast response was affected by GTP-gamma-S.

Modulation of potassium conductances by an endogenous neuropeptide in neurones of Aplysia californica

1. Macroscopic and single-channel currents were recorded from voltage-clamped neurones in the abdominal and pleural ganglia of Aplysia californica in order to investigate conductance changes elicited by application of the endogenous peptide FMRFamide (Phe-Met-Arg-Phe-NH2) and related neuropeptides to the cell surface. 2. The Ca-dependent K current, IK(Ca), when elicited at a constant voltage by intracellular injection of Ca2+, was insensitive to FMRFamide or its derivative YGG-FMRFamide (Tyr-Gly-Gly-Phe-Met-Arg-Phe-NH2). 3. Under steady voltage clamp, certain cells responded to a brief puff of FMRFamide or YGG-FMRFamide with a transient outward current lasting about 1 min. Unclamped cells responded with a corresponding hyperpolarization. These responses reversed at about -75 mV. Ion substitution indicated that the current is carried by K+. 4. FMRFamide and YGG-FMRFamide were equally effective in activating the outward current, whereas FMRF, met-enkephalin and leu-enkephalin were ineffective. 5. At voltages negative to -30 mV and, in the absence of extracellular Ca2+, also at more positive potentials, the FMRFamide-sensitive current showed no voltage dependence beyond that predicted from constant-field considerations. 6. The response to FMRFamide was relatively insensitive to extracellular tetraethylammonium (TEA, KD approximately 75 mM) and 4-aminopyridine (4-AP, KD approximately 6 mM). It was suppressed in Ba-containing solutions, but was unaffected by injection of the Ca chelating agent EGTA. The response was blocked by serotonin and other agents known to elevate intracellular adenosine 3',5'-phosphate (cyclic AMP) levels, and by direct injection of cyclic AMP into the cell. 7. In its pharmacological properties and lack of voltage dependence, the FMRFamide-activated current resembles the 'S' current, IK(S), a K current suppressed by application of serotonin in Aplysia neurones. 8. The similarity between the FMRFamide-sensitive current and the 'S' current was confirmed in cell-attached patch-clamp studies, in which activity of 'S' channels was found to be reduced by serotonin, and enhanced by FMRFamide. 9. Thus, FMRFamide may function in Aplysia to counteract the serotonergic modulation of 'S' channels, which has been proposed as a mechanism of presynaptic plasticity in this mollusc.

Increasing external K+ blocks phase shifts in a circadian rhythm produced by serotonin or 8-benzylthio-cAMP

Serotonin (5-HT) phase shifts the circadian rhythm from the isolated eye of Aplysia. The discovery of the mechanisms involved in phase shifting by 5-HT may help elucidate the nature of the circadian oscillator. We have found that 5-HT appears to phase shift by causing a change in membrane K+ conductance. Solutions containing zero K+(0-K+) phase shift the rhythm and the phase response curve (PRC) for 0-K+ is similar to one previously obtained for 5-HT. The similarity in PRCs for 0-K+ and 5-HT suggested that these treatments may be phase shifting the rhythm through a common mechanism. The nonadditivity of phase shifting by 0-K+ and 5-HT supports this suggestion. A common mechanism of action of 5-HT and 0-K+ might be effects on membrane potentials. The possible involvement of a membrane potential change in mediating the effect of 5-HT and the lack of an effect of large reductions in Na+, Cl-, and Ca2+ ions on phase shifting by 5-HT led us to examine the role of K+ ions in phase shifting by 5-HT. A change in K+ conductance may mediate the effects of 5-HT on the rhythm because HiK (30mM) solutions blocked the phase shift normally produced by 5-HT. The conductance change produced by 5-HT may be an increase in K+ conductance which would produce a hyperpolarization and not a decrease in K+ conductance which would produce a depolarization since depolarizing treatments, HiK (30-110mM), had no effect on the rhythm at the phase where 5-HT produces its largest phase shifts. Since we previously found that the effects of 5-HT appear to be mediated by cAMP, we examined whether HiK solutions could block the effects of 8-benzylthio-cAMP on the rhythm. HiK (40mM) blocked the phase shifts normally produced by 8-benylthio-cAMP. Our working hypothesis for the 5-HT phase-shifting pathway based on these results is 5-HT leads to increased cAMP leads to elevates K+ conductance leads to membrane hyperpolarization leads to phase shifts the rhythm.

Voltage, temperature and ionic dependence of the slow outward current in Aplysia burst-firing neurones

1. The slow outward current in Aplysia burst-firing neurones was studied under voltage-clamp conditions. This current, designated Iso, was measured as the incremental outward tail current following small depolarizing commands. 2. Iso was shown to be a pure K+ current, probably activated by the influx of Ca2+ during the depolarizing command (Johnston, 1976). For small depolarizations, the peak conductance was about 10(-7) mhos. 3. The rate of decay of Iso could be fit by a single exponential and was voltage-dependent, increasing with depolarization. 4. The decay rate of Iso was also temperature-dependent, with a Q10 of about 3. The peak conductance, however, was much less temperature-sensitive, with a Q10 of about 1.5. 5. The voltage dependence of decay rate suggested either the presence of a voltage-dependent Ca2+ pump or that the change in intracellular calcium concentration was not the rate-limiting step in the decay of Iso.

Contribution of calcium and potassium permeability changes to the off response of scallop hyperpolarizing photoreceptors

1. The membrane response of the distal photoreceptors in the retina of the scallop Pectin irradians to the termination of a bright white light (off response) is shown to be composed of the decay of the hyperpolarizing receptor potential and an action potential with slow kinetics. 2. The action potential can be produced in darkness in the absence of external Na+ ions by membrane depolarization. 3. The action potential is maintained by replacement of external Ca2+ with Sr2+ or Ba2+, but not by Mg2+. In normal external Ca2+ (9mM), the action potential is abolished by the addition of the Ca2+ inhibitors, La3+, Co2+, and Mn2+ or the organic Ca2+ antagonist D-600. 4. Elevated external Ca2+ concentrations increase the rate of rise and peak amplitude of the action potential as well as the rate of repolarization and after hyperpolarization, but decrease the duration. 5. The rate of rise and peak amplitude of the action potential are increased by the K+ antagonists tetraethylammonium (TEA) 4-amino-phyridine (4-AP), Ba2+ and procaine. The antagonists have different effects on subsequent phases of the response, however. External TEA and Ba2+ increase the duration, but decrease the rate of repolarization and abolish the after hyperpolarization, whereas external 4-AP and procaine increase the rate of repolarization, decrease the duration and increase the after hyperpolarization. 6. The ratio of the Ca2+ to K+ permeability (P Ca/P K) estimated from the constant field equation at the peak of the action potential in different external Ca2+ concentrations is close to 1. 7. The maximum rate of rise and the peak amplitude of the action potential are increased by membrane hyperpolarization and decreased by membrane depolarization. They are decreased by background light intensity relative to their value in the dark. 8. In normal ASW the action potential can be identified during the off response as a small overshoot of membrane potential relative to its value in the dark. 9. The rate of repolarization of the off response in normal ASW is reduced by agents or conditions which inhibit or reduce Ca2+ permeability changes, e.g. external Co2+ and La2+ or zero external Ca2+. 10. Our results suggest that a voltage-dependent increase in membrane permeability to Ca2+ and to K+ ions modifies the repolarizing phase of the receptor potential.

Photoresponses of a sensitive extraretinal photoreceptor in Aplysia

1. The light-evoked membrane current, photo-current, of an extraretinal photo-receptor, the ventral photoresponsive neurone (v.p.n.), in the abdominal ganglion of Aplysia californica, was studied using the voltage clamp method. Flashes and steps of monochromatic light were used as stimuli. 2. Flashes of light 100 msec in duration elicit slowly developing outward currents which peak at 5--10 sec and then return to dark levels within 30--60 sec. 3. The peak of the action spectrum of v.p.n. is at 470 nm and is similar to the peak for R2, another photoresponsive extraretinal Aplysia neurone, and to the peak of absorption spectra of molluscan rhodopsins. V.p.n. also contains membrane-bound cytoplasmic pigmented granules similar to those found in R2, and these are thought to mediate the light response. 4. Photo-current is associated with an increase in membrane conductance. In normal sea water photo-current has a reversal potential at the K equilibrium potential, EK and the reversal potential has a Nernstian relationship with external K concentration. The current--voltage relationships for peak and steady-state photo-current are fitted by the same constant field equation; currents measured when voltage was changed in steps at peak photo-current also have a similar relationship with voltage. The results are similar when saturating or non-saturating light intensities were used. Thus it appears that the light-activated K+ conductance is neither time nor voltage dependent. 5. Minimally detectable responses occurred at flash photon densities of 10(12) photons cm-2 which is 10(-3) that for R2. This value is comparable to those reported for retinal photoreceptors of Pecten irradians, a scallop, and Salpa democratica, a pelagic tunicate, and is lower than values reported for extraretinal photoreceptors such as the pineal photoreceptors of Salmo gairdnerii irideus, the rainbow trout, and the caudal photoreceptor in the sixth abdominal ganglion of Procambarus clarkii, a crayfish. 6. V.p.n. has a linear amplitude response range for low intensities of light and a non-linear range that saturates at high intensities. In the accompanying paper the response wave form and its temperature dependence are interpreted according to a diffusion-based model.

Life time and elementary conductance of the channels mediating the excitatory effects of acetylcholine in Aplysia neurones

1. The excitatory effects of acetylcholine (ACh) on an identified group of Aplysia neurones have been studied under voltage clamp in an attempt to measure the average life time. tau, of the channels opened by ACh and the elementary current, iel, flowing through these channels. The value of tau was determined both from spectral noise analysis and from current relaxations after voltage steps. Both methods lead to similar values. iel was calculated from the ratio of the variance of the ACh induced noise to the mean ACh induced current. 2. tau is increased by hyperpolarization, or by lowering the temperature. At 12 degrees C, tau = 27 msec AT -80 MV, tau = 17 msec at mV. tau is about 5 times smaller at 21 degrees C than at 12 degrees C. 3. iel increases linearly with hyperpolarization. At -80 mV, in Tris-buffered sea water, the mean value of iel was 0.8 X 10)-12) A at 12 degrees C. At 21 degrees C, this value was multiplied by 1.8. 4. The estimate of the ACh reversal potential Erev obtained by extrapolation of the relation between iel and the membrane potential V was + 30 mV. The estimate obtained from the analysis of the instantaneous current changes produced by voltage steps was + 15 mV. The difference between the two values appears to be due to the development of a K curent activated by the entry of Ca into the cell during the ACh response. This current introduces an error in opposite directions into the two estimates of Erev, which can therefore be assumed to be intermediate between + 15 and + 30 mV. An assumed value of + 20 mV yields an elementary conductance of 8 X 10(-12) omega-1 at 12 degrees C in Tris-buffered sea water. 5. The total ACh induced current measured in steady-state conditions increases more with hyperpolarization than does iel. The difference can be entirely accounted for by the fact that hyperpolarization increases tau. 6. When carbachol or tetramethylammonium is applied instead of ACh, the value of iel is identical to that found with ACh, but tau is slightly shorter (about 75%). 7. Inward ACh induced currents can still be observed in solutions where all Na has been replaced by Cs, Mg, or Ca. 8. iel increases when Na is replaced by Cs; it decreases when Na is replaced by Mg or Ca. In all Na-free solutions, tau is larger than in Na sea water: the lengthening of tau is largest for Ca sea water, smallest for Cs sea water. An interpretation of these changes of gamma is proposed. This interpretation may also account for the voltage sensitivity of gamma in normal sea water. 9. Partial replacement of NaCl by TrisCl strikingly reduces the ACh induced current. gamma is not modified by Tris substitution, and the reduction of the total current is entirely accounted for by a steep decrease of iel. Tris does not seem to affect the pore opening and closing processes, but to block the ACh controlled channel.

Properties of internally perfused, voltage-clamped, isolated nerve cell bodies

The membrane properties of isolated neurons from Helix aspersa were examined by using a new suction pipette method. The method combines internal perfusion with voltage clamp of nerve cell bodies separated from their axons. Pretreatment with enzymes such as trypsin that alter membrane function is not required. A platinized platinum wire which ruptures the soma membrane allows low resistance access directly to the cell's interior improving the time resolution under voltage clamp by two orders of magnitude. The shunt resistance of the suction pipette was 10-50 times the neuronal membrane resistance, and the series resistance of the system, which was largely due to the tip diameter, was about 10(5) omega. However, the peak clamp currents were only about 20 nA for a 60-mV voltage step so that measurements of membrane voltage were accurate to within at least 3%. Spatial control of voltage was achieved only after somal separation, and nerve cell bodies isolated in this way do not generate all-or-none action potentials. Measurements of membrane potential, membrane resistance, and membrane time constant are equivalent to those obtained using intracellular micropipettes, the customary method. With the axon attached, comparable all-or-none action potentials were also measured by either method. Complete exchange of Cs+ for K+ was accomplished by internal perfusion and allowed K+ currents to be blocked. Na+ currents could then be blocked by TTX or suppressed by Tris-substituted snail Ringer solution. Ca2+ currents could be blocked using Ni2+ and other divalent cations as well as organic Ca2+ blockers. The most favorable intracellular anion was aspartate-, and the sequence of favorability was inverted from that found in squid axon.

Effects of nystatin on membrane conductance and internal ion activities in Aplysia neurons

Two methods were used to study effects of the antibiotics, nystatin, on giant neurons of Aplysia. In the first method the effects of various concentrations of nystatin on the current-voltage relationship were evaluated at a fixed time after exposure to the antibiotic using a two-microelectrode voltage clamp. Nystatin increased membrane conductance in a dose-dependent manner. The dose-response relation was very steep, with little or no effect below 15 mg/liter and an effect too large to measure at concentrations greater than 30 mg/liter. Upon return to antibiotic-free solution, membrane conductance returned to pre-treatment levels within 30 minutes. The second type of experiment involved use of ion-specific microelectrodes to measure changes of intracellular univalent ion activities which attended the nystatin-induced permeability. Nystatin-induced permeability changes mainly involved univalent cations, but Cl permeability was also increased. Nystatin may therefore be used to selectively rearrange the internal ionic milieu to study the effect of such a change on membrane transport or electrical properties.

Permeability, phase-boundary potential and conductance in a cholinergic channel without constant field

A potassium-selective, chemically excitable channel, whose characteristics cannot be accurately described by constant-field theory, is studied by a new approach based on diffusion theory but with no need for the classical assumptions of constant field, homogeneous membrane, and equal phase-boundary potentials at both interfaces. Permeability is defined, free of these constraints, and the Goldman coefficient is demonstrated to be a special case useful only when the constraints apply. Permeability can be evaluated directly from current-voltage data, and it is found not to be a parameter in this channel, but rather a function of both the voltage and the concentration of the permeant ion. However, it becomes concentration-independent when the membrane voltage is equal to the sum of the phase-boundary potentials. That sum can therefore be determined from these data, and it is -65 mV in this channel. The permeability at that potential is a channel parameter, and equal to 8.66 X 10(-6) cm/s for this channel. A constant field is shown not to exist in this channel and the Goldman coefficient not to be a parameter but a function of potential and concentration. Although errors introduced into this coefficient by nonconstant field and unequal surface potentials partially cancel each other, the coefficient is nevertheless not a correct measure of permeability.

The effect of extracellular potassium on the intracellular potassium ion activity and transmembrane potentials of beating canine cardiac Purkinje fibers

We used open tip microelectrodes containing a K+-sensitive liquid ion exchanger to determine directly the intracellular K+ activity in beating canine cardiac Purkinje fibers. For preparations superfused with Tyrode's solution in which the K+ concentration was 4.0 mM, intracellular K+ activity (ak) was 130.0+/-2.3 mM (mean+/-SE) at 37 degrees C. The calculated K+ equilibrium potential (EK) was -100.6+/-0.5 mV. Maximum diastolic potential (ED) and resting transmembrane potential (EM) were measured with conventional microelectrodes filled with 3 M KCl and were -90.6+/-0.3 and -84.4+/-0.4 mV, respectively. When [K+]o was decreased to 2.0 mM or increased to 6.0, 10.0, and 16.0 mM, ak remained the same. At [K+]o=2.0, ED was -97.3+/-0.4 and Em -86.0+/-0.7 mV; at [K+]o=16.0, ED fell to -53.8+/-0.4 mV and Em to the same value. Over this range of values for [K+]o, EK changed from -119.0+/-0.3 to -63.6+/-0.2 mV. These values for EK are consistent with those previously estimated indirectly by other techniques.

Intracellular calcium and extra-retinal photoreception of Aplysia Giant neurons

The early or "instantaneous" current-voltage relationship for the light-activated potassium current in Aplysia giant neurons was linear during the first second of illumination. However, the light current was greatly reduced or abolished by prolonged hyperpolarization. It was also greatly reduced by the injection of calcium EGTA buffers having calcium activities of 5.6 X 10(-8) M and simulated by injecting buffers with calcium activities of 2.8-5.6 X 10(-7) M. Removal of calcium from the extracellular fluid had no effect. Both the light- and calcium-activated outward potassium currents were reduced by tetraethylammonium (TEA) ions. The light current was not affected by substituting rubidium for potassium nor by substituting either lithium or Tris for sodium. The calcium-activated potassium current persisted when the neuron was cooled to 5 degrees C. However, the light response could no longer be elicited. Light hyperpolarizes Aplysia neurons probably by increasing intracellular calcium activity two-to six-fold which activates a membrane potassium conductance. Calcium levels appear to be restored within the cell and are energy dependent. The light-activated release of calcium is inhibited by cooling. The body wall of Aplysia transmits enough visible or 500 nm light to hyperpolarize some Aplysia giant neurons under ambient conditons. These neurons may be involved in the extraretinal light entrainment that occurs in Aplysia.

Ionic permeabilities of an Aplysia giant neuron

In a giant neuron of Aplysia californica, permeabilities and conductances obtained by measuring net fluxes of Na+, K+ and Cl-minus with ion-specific microelectrodes were compared with those obtained by measuring transmembrane current and potential changes when the three ions were varied in the external solution. Net fluxes were measured with ion-specific microelectrodes, after blocking metabolic processes, thus allowing movement of ions down their electrochemical gradients. Premeabilities and conductances obtained from the "chemical" measurements (i.e., ion-specific electrodes) were generally comparable to the values obtained from "electrical" measurements (i.e., ion-specific electrodes) were generally comparable to the values obtained from "electrical" measurements. Where discrepancies occurred, they could be explained by showing that some of the assumptions necessary to use the "electrical" method were not quantitatively true in this system. The absolute magnitudes of the permeabilities are significantly less than those found in many axonal preparations. There is also a relatively high PNa/PK ratio. The selectivity of the membrane against ions such as Tris" and MeSO3-minus is not good, Tris+ being nearly as permeable as Na+ and MeSO3-minus about one-half as permeables as Cl-minus. These properties may be characteristic of somal membranes.

The membrane of giant molluscan neurons: electrophysiologic properties and the origin of the resting potential

The molluscan neuron, because of its large size and accessibility, has been an important model for studying the electrophysiology of nerve cells. This review catalogs data about specific molluscan neurons, but the greater importance of this material is in the broad picture of how a neuronal membrane maintains internal potential and is responsive to changes in the environment. Electrical properties of the membrane. The mechanisms which contribute to the resting potential in molluscan neurons can be separated into ionic and metabolic components. When the electrogenic sodium pump is eliminated experimentally, the ionic component of the potential follows the constant field equation quite closely. Many of the "constants" and "parameters" which characterize the membrane of molluscan neurons are actually variables which depend upon temperature, ionic environment, and membrane potential. The evaluation of the electrical parameters is complicated by extensive infoldings of the somatic membrane, and by large axons which drain current from the soma. Most molluscan neurons have a very high specific membrane resistance and a correspondingly low potassium permeability. Membrane capacitance is close to the 1 microF/cm2 value which characterizes biological membranes. The current-voltage relation of molluscan neurons may be complicated by inward-going rectification, but if that is inhibited the I-V curve follows the prediction of either the constant field equation or a simple electrical model. Factors which modify membrane behavior. The resting potential of molluscan neurons is very sensitive to changes in temperature and Ko, through a combination of effects upon the electrogenic sodium pump, inward-going rectification, and the membrane "parameters". Inward-going rectification depends upon a rectifying K conductance, and can be eliminated by cold or the removal of Ko. Strong or prolonged currents have time-dependent effects upon the membrane, and excessive polarization leads to a "high conductance state". The underlying (non-rectifying) K permeability of the membrane is relatively insensitive to temperature and ionic changes, whereas the Na permeability increases with warming. Membrane resistance varies with both temperature and ions (because the I-V curve is sensitive to these conditions) but membrane capacitance is relatively insensitive to external factors. Electrogenic sodium transport. Sodium transport is electrogenic in molluscan neurons. It can be stimulated by warm temperatures and an excess of substrate (e.g. high Nai); it can be inhibited by cold, by an absence of substrate (e.g. low Ko), or by pharmacologic agents such as cyanide or ouabain.(ABSTRACT TRUNCATED AT 400 WORDS)

Long-term effect of ouabain and sodium pump inhibition on a neuronal membrane

1. The long-term effects of ouabain on the membrane potential of the Anisodoris giant neurone (G cell) were examined in cells maintained for periods of up to 15 hr at 11-13 degrees C.2. In the presence of ouabain (5 x 10(-4)M), the membrane potential depolarized to a constant level for 1-4 hr, then hyperpolarized for 5-7 hr after which it gradually depolarized again.3. During the hyperpolarizing phase, after 6-8 hr in ouabain, [K](1) fell approximately 50%, [Na](1) increased 50-100% and the P(Na)/P(K) ratio decreased to 25% of its initial value.4. After 8 hr in ouabain the membrane conductance increased two- to fourfold. This increase was independent of temperature and membrane rectification.5. The K permeability (P(K)) was calculated from the constant field equation, and showed a fourfold increase after long-term treatment with ouabain. This rise in P(K) probably underlies the membrane hyperpolarization and the decrease in the P(Na)/P(K) ratio.6. It is suggested that inhibition of the Na(+) pump with ouabain causes a gradual rise in [Na](1) which secondarily leads to Ca(2+) uptake, an increase in [Ca](1), and thereby an increase in P(K).

Cyclic variation of potassium conductance in a burst-generating neurone in Aplysia

1. The hyperpolarization between bursts in the R 15 cell of Aplysia is accompanied by an increase in membrane slope conductance.2. The post-burst hyperpolarization can be observed with ouabain, lithium, or potassium-free solution if artificial inward current is applied. The hyperpolarization can be observed with dinitrophenol or cooling to 10 degrees C, with no injected current. Thus, the hyperpolarization apparently is not due to the cyclic activity of an electrogenic pump.3. A reversal potential for the post-burst hyperpolarization can be demonstrated by passage of inward current during the inter-burst period. The reversal of direction of the potential depends on recent occurrence of a burst.4. The reversal potential varies with external potassium concentration, but not with chloride or sodium.5. The post-burst hyperpolarization is not blocked by external tetraethylammonium at a concentration which greatly prolongs the action potentials.6. During the onset of spike blockage by, and recovery from, calcium-free+tetrodotoxin saline, the bursts of action potentials appear to be driven by endogenous waves of membrane potential.7. The hyperpolarizing phase of the waves in calcium-free+tetrodotoxin medium is accompanied by an increased slope conductance.8. A reversal potential can be demonstrated for the hyperpolarization following a wave in calcium-free+tetrodotoxin medium by applying inward current during the interwave period.9. The waves in calcium-free+tetrodotoxin medium are blocked by ouabain but can be reinstated by artificial hyperpolarization.10. The post-burst hyperpolarization and the post-wave hyperpolarization appear to result from a periodic increase in membrane conductance, primarily to potassium ions.

Light response of a giant Aplysia neuron

Illumination of an Aplysia giant neuron evokes a membrane hyperpolarization which is associated with a membrane conductance increase of 15%. The light response is best elicited at 490 nM: the neuron also has an absorption peak at this wavelength. At the resting potential (-50 to -60 mV) illumination evokes an outward current in a voltage-clamped cell. This current reverses sign very close to E(K) calculated from direct measurements of internal and external K(+) activity. Increases in external K(+) concentration shift the reversal potential of the light-evoked response by the same amount as the change in E(K). Decreases in external Na(+) or Cl(-) do not affect the response. Therefore, the response is attributed to an increase in K(+) conductance. Pressure injection of Ca(2+) into this neuron also hyperpolarizes the cell membrane. This effect is also due largely to an increase in K(+) conductance. The light response after Ca(2+) injection does not appear to be altered. Pressure injection of EGTA abolished or greatly reduced the light response. The effect was reversible. We suggest that light acts upon a single pigment in this neuron, releasing Ca(2+) which in turn increases K(+) conductance, thereby hyperpolarizing the neuronal membrane.

Active transport of chloride by the giant neuron of the Aplysia abdominal ganglion

Internal chloride activity, a(i) (Cl), and membrane potential, E(m), were measured simultaneously in 120 R2 giant neurons of Aplysia californica. a(i) (Cl) was 37.0 +/- 0.8 mM, E(m) was -49.3 +/- 0.4 mv, and E(Cl) calculated using the Nernst equation was -56.2 +/- 0.5 mv. Such values were maintained for as long as 6 hr of continuous recording in untreated neurons. Cooling to 1 degrees -4 degrees C caused a(i) (Cl) to increase at such a rate that 30-80 min after cooling began, E(Cl) equalled E(m). The two then remained equal for as long as 6 hr. Rewarming to 20 degrees C caused a(i) (Cl) to decline, and E(Cl) became more negative than E(m) once again. Exposure to 100 mM K(+)-artificial seawater caused a rapid increase of a(i) (Cl). Upon return to control seawater, a(i) (Cl) declined despite an unfavorable electrochemical gradient and returned to its control values. Therefore, we conclude that chloride is actively transported out of this neuron. The effects of ouabain and 2,4-dinitrophenol were consistent with a partial inhibitory effect. Chloride permeability calculated from net chloride flux using the constant field equation ranged from 4.0 to 36 x 10(-8) cm/sec.