The effects of temperature and ions on the current-voltage relation and electrical characteristics of a molluscan neurone

Synaptic connexions of two symmetrically placed giant serotonin-containing neurones

1. Each giant serotonin cell in Helix pomatia makes synaptic connexions with three non-amine-containing neurones: the anterior, middle and posterior buccal cells.2. Individual e.p.s.p.s, of 500-600 msec duration, were observed in both left and right middle cells following each evoked giant serotonin cell action potential. They were facilitated with repetitive stimulation of the giant serotonin cells and summed to give rise to an action potential. The membrane resistance of the middle cells was reduced when the giant serotonin cells were stimulated to fire rapidly. Evidence is presented which suggests that the link between each giant serotonin cell and each middle cell is monosynaptic.3. Iontophoretically applied serotonin produced a depolarizing potential change in the middle cell perikaryon; the response rapidly desensitized on repetitive application.4. Morphine abolished reversibly the middle cell serotonin potential and antagonized transmission from the giant serotonin cells to the middle cells. Lowering the Na concentration of the medium reversibly diminished the size of the serotonin potential and the giant serotonin cell elicited e.p.s.p.s in the middle cells.5. Reserpine, which depletes serotonin in the giant serotonin cell, impaired transmission from these cells to the middle cells.6. The results suggest that serotonin is the synaptic transmitter released from the giant serotonin cells on to the middle cells and that this system is a suitable model for further analysis of the neuronal role of serotonin.

Temperature Sensitivity of Dopaminergic Neurons of the Substantia Nigra Pars Compacta: Involvement of Transient Receptor Potential Channels

Changes in temperature of up to several degrees have been reported in different brain regions during various behaviors or in response to environmental stimuli. We investigated temperature sensitivity of dopaminergic neurons of the rat substantia nigra pars compacta (SNc), an area important for motor and emotional control, using a combination of electrophysiological techniques, microfluorometry, and RT-PCR in brain slices. Spontaneous neuron firing, cell membrane potential/currents, and intracellular Ca2+level ([Ca2+]i) were measured during cooling by ≤10° and warming by ≤5° from 34°C. Cooling evoked slowing of firing, cell membrane hyperpolarization, increase in cell input resistance, an outward current under voltage clamp, and a decrease of [Ca2+]i. Warming induced an increase in firing frequency, a decrease in input resistance, an inward current, and a rise in [Ca2+]i. The cooling-induced current, which reversed in polarity between −5 and −17 mV, was dependent on extracellular Na+. Cooling-induced whole cell currents and changes in [Ca2+]iwere attenuated by 79% in the presence of 2-aminoethoxydiphenylborane (2-APB; 200 μM), and the outward current was reduced by 20% with ruthenium red (100 μM). RT-PCR conducted with tissue punches containing the SNc revealed mRNA expression for TRPV3 and TRPV4 channels, known to be activated in expression systems by temperature changes within the physiological range. 2-APB, a TRPV3 modulator, increased baseline [Ca2+]i, whereas 4αPDD, a TRPV4 agonist, increased spontaneous firing in 7 of 14 neurons tested. We conclude that temperature-gated TRPV3 and TRPV4 cationic channels are expressed in nigral dopaminergic neurons and are constitutively active in brain slices at near physiological temperatures, where they affect the excitability and calcium homeostasis of these neurons.

Millimeter waves thermally alter the firing rate of the Lymnaea pacemaker neuron

The effects of millimeter waves (mm-waves, 75 GHz) and temperature elevation on the firing rate of the BP-4 pacemaker neuron of the pond snail Lymnaea stagnalis were studied by using microelectrode techniques. The open end to a rectangular waveguide covered with a thin Teflon film served as a radiator. Specific absorption rates (SARs), measured in physiological solution at the radiator outlet, ranged from 600 to 4,200 W/kg, causing temperatures rises from 0.3 to 2.2 degrees C, respectively. Irradiation at an SAR of 4200 W/kg caused a biphasic change in the firing rate, i.e., a transient decrease in the firing rate (69 +/- 22% below control) followed by a gradual increase to a new level that was 68 +/- 21% above control. The biphasic changes in the firing rate were reproduced by heating under the condition that the magnitude (2 degrees C) and the rate of temperature rise (0.96 degrees C/s) were equal to those produced by the irradiation (for an SAR of 4,030 W/kg). The addition of 0.05 mM of ouabain caused the disappearance of transient responses of the neuron to the irradiation. It was shown that the rate of temperature rise played an important role in the development of a transient neuronal response. The threshold stimulus for a transient response of the BP-4 neuron found in warming experiments was a temperature rise of 0.0025 degrees C/s.

Electrophysiological and ultrastructural studies on reversible neural conduction disturbance after high voltage discharge

High-voltage condenser discharges exerting a field strength of up to 1000 V/cm (discharge time constant 0.24-8 msec) applied to isolated sciatic frog nerve lead to disturbances of the propagation of action potentials including transient complete block of conduction. Such conduction disturbances are normally reversible within minutes. Inhibition of the activity of the membrane-bound Na+-K+ATPase prevents the recovery from conduction block. Withdrawal of external Ca2+ also prevents recovery, whereas blockade of protein synthesis by cycloheximide has no influence. The velocity of recovery depends on the temperature, with temperature coefficients (Q10) from 1.31 to 1.84 between 2 degrees and 30 degrees C. Transmission electron microscopy of nerves subjected to strong discharges shows alterations of the myelin sheath (splitting and cleft formation) which are, however, not specific for this mechanism of injury. No alterations are seen in the region of the free axoplasmic membrane of the node of Ranvier or in organelles. The results suggest a breakdown of the transmembrane ionic gradient causing the conduction disturbance.

Inward rectifier K+-channel kinetics from analysis of the complex conductance of Aplysia neuronal membrane

Conduction in inward rectifier, K+-channels in Aplysia neuron and Ba++ blockade of these channels were studied by rapid measurement of the membrane complex admittance in the frequency range 0.05 to 200 Hz during voltage clamps to membrane potentials in the range -90 to -40 mV. Complex ionic conductances of K+ and Cl- rectifiers were extracted from complex admittances of other membrane conduction processes and capacitance by vector subtraction of the membrane complex admittance during suppressed inward K+ current (near zero-mean current and in zero [K+]0) from complex admittances determined at other [K+]0 and membrane potentials. The contribution of the K+ rectifier to the admittance is distinguishable in the frequency domain above 1 Hz from the contribution of the Cl- rectifier, which is only apparent at frequencies less than 0.1 Hz. The voltage dependence (-90 to -40 mV) of the chord conductance (0.2 to 0.05 microS) and the relaxation time (4-8 ms) of K+ rectifier channels at [K+]0 = 40 mM were determined by curve fits of admittance data by a membrane admittance model based on the linearized Hodgkin-Huxley equations. The conductance of inward rectifier, K+ channels at a membrane potential of -80 mV had a square-root dependence on external K+ concentration, and the relaxation time increased from 2 to 7.5 ms for [K+]0 = 20 and 100 mM, respectively. The complex conductance of the inward K+ rectifier, affected by Ba++, was obtained by complex vector subtraction of the membrane admittance during blockage of inward rectifier, K+ channels (at -35 mV and [Ba++]0 = 5 mM) from admittances determined at -80 mV and at other Ba++ concentrations. The relaxation time of the blockade process decreased with increases in Ba++ concentration. An open-closed channel state model produces the inductive-like kinetic behavior in the complex conductance of inward rectifier, K+ channels and the addition of a blocked channel state accounts for the capacitive-like kinetic behavior of the Ba++ blockade process.

Copper activates a unique inward current in molluscan neurones

1. Reidentifiable Aplysia neurones were current and voltage clamped in vitro using standard microelectrode techniques. 2. Bath or focal application of Cu2+ at concentrations of 1-100 microM produced a rapid and reversible depolarization of the somal, but not the axonal, membrane potential. The depolarization was accompanied by an increased membrane conductance and activation of an inward current (ICu) which could not be activated by intracellular ionophoretic injection of Cu2+. 3. ICu is carried, in part, by Na+ because the reversal potential of ICu was shifted in a Nernstian fashion by decreasing the extracellular Na+ concentration. The reversal potential of ICu was not affected by removal of extracellular Ca2+ or K+. 4. ICu does not result from (1) activation of known chemically or voltage-gated Na+ conductances, (2) inhibition of the Na+-K+-ATPase or (3) a generalized increase in membrane permeability resulting from lipid peroxidation. 5. A similar inward current was activated by AgNO3 (100 microM) and HgCl2 (100 microM).

Disturbances of neural conduction in isolated frog nerves following exposure to strong electric fields

Frog sciatic nerves were isolated and the middle portion of each exposed to condenser discharges (field strength up to 1000 V/cm; time constants 0.2-8.0 ms) through the bathing fluid. The ability of the nerve to propagate action potentials (AP) was examined by stimulating the proximal end and recording the AP from the distal end of the exposed section. The fraction of the nerve fibers remaining propagative was estimated from the amplitude (or the area) of the compound AP. Strong discharges brought about a total block of propagation lasting for up to 30 minutes, followed by slow, but almost complete, restitution. The restitution was exponential against time and depended on the field strength and duration of the discharge. Discharges equal in energy but different in their voltage--condenser combinations had markedly different actions, with stronger effects being found at higher voltages and vice versa. Hence, the described effects are unlikely to be caused by dissipation of thermal energy only. Other mechanisms (ionic imbalance, dielectric breakdown, punch through) are discussed.

The effects of temperature on synaptic transmission in hippocampal tissue slices

Fully submerged rat hippocampal tissue slices were exposed to temperature changes, and the effects on CA1 pyramidal cell electrophysiology studied. Raising the temperature from 29 to 33 or 37 degrees C simultaneously increased the focal-excitatory postsynaptic potentials and decreased the population spikes. These changes were largely reversible for slices warmed to 33 degrees C, but not for slices warmed to 37 degrees C. During warming transiently increased excitatory transmission was observed; the degree of increased transmission was related to the rate of temperature rise. It is postulated that neuronal membrane hyperpolarization with warming is responsible for several of the effects seen.

From sea lemons to c-waves

This review of retinal pigment epithelial (RPE) physiology pays tribute to Anthony L. F. Gorman, who introduced the author to the giant neuron of Anisodoris nobilis (the sea lemon) and cellular neurobiology. The RPE is an epithelial monolayer with tight junctions, which controls the environment of the photoreceptor outer segments. The apical and basal membranes have different electrical properties and generate a standing potential across the eye. The RPE helps maintain adhesion between the retina and the wall of the eye. Adhesion is weakened by cyanide, low pH or low calcium, but enhanced by ouabain or acetazolamide. The RPE transports water from the subretinal space toward the choroid. This water movement is inhibited by hypoxia or cyanide but enhanced by ouabain or acetazolamide. The c-wave of the electroretinogram is a composite of a cornea-positive wave produced by hyperpolarization of the apical RPE membrane and a cornea-negative wave produced by the Muller cells, both in response to the fall in extracellular potassium that follows illumination of the photoreceptors. The "light response" of the standing potential is produced by depolarization of the basal membrane of the RPE. These examples illustrate how principles of cellular neurophysiology can be applied to questions of clinical relevance.

Inward and outward currents in isolated dendrites of Crustacea coxal receptors

Segments from the nonspiking peripheral dendrites of a crustacean coxal receptor (T fiber) were studied using the voltage clamp technique. The peripheral endings of the T fiber are sensitive to stretch applied to a specialized receptor muscle by rotation of the coxa. The intraganglionary portion of the T fiber is presynaptic to the motor neurons innervating the coxal muscle. Depolarizing commands activated three separate fast channels: (i) a transient inward sodium current, INa, which is blocked by tetrodotoxin (TTX); (ii) a transient outward current, Io1 , having the same voltage-dependent characteristics as INa; and (iii) a second, longer-lasting, outward current, Io2 . Both INa and Io1 were inactivated when segments were clamped at voltages more positive than -50 mV, whereas Io2 could be activated at voltages more positive than -50 mV. Io1 and Io2 were blocked by 4-aminopyridine (4-AP) and by tetraethylammonium (TEA), although Io2 shows a greater sensitivity to TEA than Io1 . It is suggested that Io1 may be a factor in determining the nonspiking behavior of the dendrites and that Io2 may limit the stretch-induced depolarization in the dendrite to a value more negative than that at which the maximum rate of transmitter release occurs. In addition to the three fast currents, the presence of a slow inward and slow outward current could also be demonstrated. The effects of the slow currents were longer in segments cut from the proximal part of the dendrites.

Characterization of a chloride conductance activated by hyperpolarization in Aplysia neurones

A voltage-clamp study was made of some properties of the non-synaptic hyperpolarization-activated Cl- conductance recently described in Aplysia neurones loaded with Cl- ions (Chesnoy-Marchais, 1982). The experiments were performed on an identified family of neurones, which present cholinergic responses allowing an easy measurement of the equilibrium potentials of Cl- (ECl) and K+ ions (EK). The Cl- selectivity of the hyperpolarization-activated conductance was deduced from four observations: (1) the extrapolated reversal potential of the hyperpolarization-activated current, Er, was close to the reversal potential of the cholinergic Cl- response, which is the equilibrium potential for Cl- ions, ECl. (2) Modifications of the intracellular or extracellular Cl- concentration induced changes of the reversal potential Er. (3) A prolonged and intense activation of the current lowered the intracellular Cl- concentration. (4) The current persisted after complete substitution of intracellular and extracellular cations by CS+ ions, as well as after replacement of extracellular Na+ ions by Tris. The steady-state Cl- conductance (gss) increases steeply with hyperpolarization. The kinetics of activation and deactivation are exponential and are characterized by the same voltage-dependent time constant (tau), of the order of a few seconds or fractions of seconds. The curves gss(V) and tau (V) can both be fitted by a two-state model in which the rate constants are exponential functions of the membrane potential (e-fold change for 12-16 mV). The Cl- current is much more affected by changes of the intracellular Cl- concentration than predicted simply from the change in Cl- driving force. Both the conductance and the time constant of activation are strongly modified. Modifications of the extracellular Cl- concentration do not always alter the amplitude of the hyperpolarization-activated Cl- current, but systematically affect its kinetics. The hyperpolarization-activated current is abolished after prolonged exposure of the cell to an artificial sea water where NO3- ions replace Cl- ions, as well as after intracellular injections of NO3- ions. Increasing the external pH shifts the gss(V) and tau (V) curves to the left. Lowering the external pH has reverse but less pronounced effects. In cells which were not loaded with Cl- ions and did not present the hyperpolarization-activated Cl- current, this current could be detected if the hyperpolarizing jump was preceded by short depolarizing pulses. In cells which were loaded with Cl- ions, the Cl- current became larger after a short depolarizing pulse. In the presence of extracellular Co2+ ions, depolarizing pulses no longer increased the Cl- current.(ABSTRACT TRUNCATED AT 400 WORDS)

Serotonin increases an anomalously rectifying K+ current in the Aplysia neuron R15

Previous work has shown that serotonin causes an increase in K+ conductance in the identified Aplysia neuron R15. This response is mediated by cAMP-dependent protein phosphorylation. The results presented here show that the K+ channel modulated by serotonin is an anomalous or inward rectifier (designated IR) that is present in R15 together with the three other distinct K+ channels previously described for this cell. Several lines of evidence indicate that this inward rectifier is partially activated in the resting cell and is further activated by serotonin. Voltage clamp analysis of resting and serotonin-evoked membrane currents at various external K+ concentrations shows that both currents have reversal potentials close to the potassium equilibrium potential, exhibit similar dependences in magnitude on external K+ concentration, and display marked anomalous rectification. The effects of particular monovalent and divalent cations are also similar on the resting and serotonin-evoked currents. Rb+, Cs+, and Ba2+ block both currents while Tl+ can substitute for K+ as a charge carrier and channel activator in both. These properties are characteristics of anomalous rectifiers in other systems. Furthermore, measurement of the voltage dependence of inactivation for the fast transient K+ current shows that this current cannot account for the anomalously rectifying K+ conductance in R15. The inward rectifier is therefore a separate current mediated by its own channels, the activity of which can be modulated by serotonin.

A Cl- conductance activated by hyperpolarization in Aplysia neurones

Although many voltage-gated cation channels have been described and extensively studied in biological membranes, there are very few examples of voltage-gated anion channels. Chloride conductances activated by depolarization have been observed in skate electroplaque and in frog and chick skeletal muscle. A Cl- conductance activated by hyperpolarization has been suggested both for frog muscle treated with acid (pH 5) solutions, and for crayfish muscle where it could account for the fact that the pronounced inward-going rectification of the I-V curve disappears if the fibres have been soaked in a Cl(-)-free solution. More recently, voltage-dependent anion channels extracted from biological membranes have been incorporated into artificial membranes. I now report that in Aplysia neurones, and in particular those in which the internal Cl- concentration has been increased, a Cl- conductance can be observed which is slowly activated by hyperpolarization and shows a vary steep voltage dependence. This time- and voltage-dependent Cl- conductance probably exists also in many other cells. Its presence might explain why it is difficult when using KCl-filled microelectrodes to maintain prolonged hyperpolarizations. This Cl- conductance constitutes a new type of inward-going rectification distinct both from the classical "anomalous rectification' which involves selective K+ channels and from the current termed if in heart muscle that is presently attributed to a cationic conductance.

Temperature acclimation: effects on membrane physiology of an identified snail neuron

The neuronal basis for thermal acclimation was examined by comparing the short- and long-term effects of temperature change on the physiological properties of an identified neuron in the isolated ganglion of Hexis aspersa. Using intracellular electrophysiological techniques, we found that the frequency of spontaneous action potentials and excitability of neurons from warm-acclimated animals was depressed by abruptly cooling from 20 to 5 degrees C. After a 2-wk period of acclimation to 5 degrees C, the levels of spontaneous activity and excitability were comparable to those of warm-acclimated neurons at 20 degrees C. Conversely, abrupt warming of neurons from cold-acclimated animals greatly increased the frequency of spontaneous activity, but after acclimation to 20 degrees C the frequency decreased. Although the duration of the action potential and the cell's electrogenic Na-K pump were temperature sensitive, thermal acclimation had no obvious effects on these parameters. Membrane permeability to Na and PNa/PK decreased with cooling, whereas PRb/PK and PCs/PK increased. Warming had the opposite effect on the relative alkali cation permeability (PX/PK). With acclimation PX/PK underwent compensatory changes.

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.

Effect of membrane potential and internal pH on active sodium-potassium transport and on ATP content in high-potassium sheep erythrocytes

Ouabain-sensitive Na+ and K+ fluxes and ATP content were determined in high potassium sheep erythrocytes at different values of membrane potential and internal pH. Membrane potential was adjusted by suspending erythrocytes in media containing different concentrations of MgCl2 and sucrose. Concomitantly either the external pH was changed sufficiently to maintain a constant internal pH or the external pH was kept constant with a resultant change of internal pH. The erythrocytes were preincubated before the flux experiment started in a medium which produced increased ATP content in order to avoid substrate limitation of the pump. It was found that an increased cellular pH reduced the rates of active transport of Na+ and K+ without significantly altering the ratio of pumped Na+/K+. This reduction was not due to limitation in the supply of ATP although ATP content decreased when internal pH increased. Changes of membrane potential in the range between -10 and +60 mV at constant internal pH did not affect the rates of active transport of Na+ or K+.

Sodium and calcium gating currents in an Aplysia neurone

1. Currents generated by depolarizing the hyperpolarizing voltage pulses were recorded at temperatures of 4--12 degrees C in the voltage-clamped soma of R15 in aplysia abdominal ganglia exposed to solutions which suppressed ionic currents. 2. Subtraction of linear capacitive and leakage currents from current generated by voltage pulses to levels more positive than -20mV revealed non-linear transient outward displacement currents at the onset of the clamp step (on-current) and transient inward displacement currents after the membrane potential returned to the holding potential (off-current). Only on-currents were studied. 3. Pulses to membrane potentials of -20 to 0 mV generated a displacement current with rapid onset and exponential decay. At membrane potentials more positive than o mV a second displacement current with a much slower onset and slower exponential decay was seen. Because the different threshold potentials for the two displacement currents were close to the different threshold potentials for Na and Ca ion currents, the two displacement currents were called Na and Ca 'gating' currents. 4. The amount of charge transfer during Ca gating currents increased sigmoidally with increasing depolarization, reaching a maximum at +30 to +40 mV. Half-maximum charge transfer occurred at +15 mV. 5. Total charge movement during Ca gating currents was maximal with holding potentials of -30 to -40 mV. More positive or more negative holding potentials produced a decrease in charge movement. 6. The time course of the gating currents, but not the total charge displaced, was very sensitive to temperature. The time constant of decay of Ca gating currents had a Q10 of about 3, whereas the total amount of charge displaced had a Q10 of 1.2. 7. The charge transfer during both Na and Ca gating currents and the amplitude of Na and Ca (but not K) ionic currents were reduced in solutions containing 1 mm-n-octanol.

Rectification in Aplysia statocyst receptor cells

1. Membrane slope resistance of Aplysia statocyst receptor cells was measured by passing constant current pulses, using a bridge circuit. In response to downward tilt all cells which responded exhibited depolarization but this could be accompanied by either decrease, increase or no measurable change in slope resistance, depending on resting membrane potential. 2. By altering membrane potential with d.c. and measuring slope resistance with constant current pulses, these cells are shown to exhibit both anomalous and delayed rectification. Either hyperpolarization or depolarization from one potential can cause the slope resistance to decrease by as much as a factor of 5. 3. The response to standard tilt can be changed from an increase in slope resistance to a decrease, or vice versa, by altering membrane potential. 4. When membrane potential was held constant during downward tilt, the slope resistance always decreased. 5. Slope resistance, the voltage response to standard tilts and the amplitude of membrane potential fluctuations all vary with average membrane potential in a similar manner. 6. These findings are incorporated into a circuit model in which anomalous and delayed rectification are represented by voltage-controlled elements. the response to tilt is always modelled as introducing a parallel conductance pathway with a large positive reversal potential. 7. The model demonstrates that slope resistance can be increased by adding a parallel shunt pathway if the latter brings the membrane out of the anomalous rectification region. 8. The model also demonstrates how delayed rectification can greatly alter the reversal potential inferred from measurements at potentials below actual reversal.

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.

Studies on bursting pacemaker potential activity in molluscan neurons. I. Membrane properties and ionic contributions

Bursting pacemaker potential (BPP) activity of identified molluscan neurons has been studied using cells from Aplysia and Otala. The results presented in this paper indicate that (1) a potassium conductance mediates the hyperpolarizing phase of the BPP; (2) the BPP amplitude is directly dependent on [Na+]0; (3) BPP activity requires the presence of divalent cations and is prevented by C02+ and La3+, but not D-600; (4) the apparent increase in membrane resistance during the depolarizing phase of the Bd can be accounted for by the movement of the membrane potential along the non-linear portion of the I-V curve; and (5) non-linear I-V relations and a minimal effective membrane resistance are pre-requisite to BPP generation. Coupled with recent observations on the presence of an inward current in these cells, the results suggest that the mechanisms underlying the BPP are similar to those proposed to describe the myocardial pacemaker potential: the hyperpolarizing phase is due to activation of a potassium conductance which slowly inactivates, resulting in a gradula deplorization until a voltage-dependent inward current is activated which then leads to an increasingly rapid deplorization and initiation of the burst of spikes. It would appear that Na+ may play the major role in carrying the inward current, although a secondary role for divalent cations cannot be discounted.

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).

Steady-state contribution of the sodium pump to the resting potential of a molluscan neurone

1. The electrogenic contribution of the Na(+)-K(+) exchange pump to the membrane potential of the Anisodoris giant neurone (G cell) was examined under steady-state and Na(+) loaded conditions.2. The membrane potential was variable for the first 1-4 hr after impalement, but, in the absence of experimental manipulation, remained constant thereafter. The average membrane potential for ten cells maintained at 11-13 degrees C and measured 5-36 hr after impalement was 55.8 +/- 1.0 mV (S.E. of mean).3. Low concentrations of external ACh caused a reversible increase in membrane Na(+) conductance. Brief exposure to ACh proved a fast and reversible technique to load the cell with Na(+) ions, and transiently stimulate the electrogenic Na(+) pump.4. In ten cells maintained from 5 to 36 hr at 11-13 degrees C the reduction in membrane potential produced by inhibition of the Na(+) pump with ouabain was remarkably constant between cells and averaged + 9.7 mV.5. Cells maintained under steady-state conditions (at 11-13 degrees C) for extended periods of time were shown to be relatively insensitive to changes in temperature and to small changes in external K(+).6. It is estimated that the Na(+)-K(+) exchange pump contributes approximately - 10 mV to the steady-state resting potential of the G cell, and that two Na(+) ions are extruded for every K(+) ion transported into the cell per pump cycle.

Electrogenic sodium pump and high specific resistance in nerve cell bodies of the squid

An electrogenic sodium pump contributes to the membrane potential in squid nerve cell bodies, imparting a temperature dependence to the resting potential that is abolished by strophanthidin. The existence of a potential produced by the pump in the soma but not the axon is correlated with a higher membrane resistance in the soma. Thus, membranes from different parts of a neuron may have functionally significant differences in resistance.

The passive electrical properties of the membrane of a molluscan neurone

1. The passive electrical properties of the membrane of the gastrooesophageal giant neurone (G cell) of the marine mollusc, Anisodoris nobilis were studied with small current steps.2. The membrane transient response can be fitted with a theoretical curve assuming as a model for the cell a sphere (soma) connected to a cable (axon). The axo-somatic conductance ratio (rho), determined by applying this model, is large (approximately 5) and the membrane time constant (tau) is long (approximately 1 sec).3. When the actual surface area of the cell, corrected for surface infoldings, and the spread of current along its axon is taken into account, the electrical measurements imply a specific resistance of the membrane of approximately 1.0 MOmega.cm(2).4. Estimates of specific membrane capacity, either from measurements of the initial portion of the membrane transient or from the ratio of the time constant to the specific membrane resistance are close to the value of 1 muF/cm(2) expected for biological membranes.5. Thus, our measurements of specific capacitance, time constant, length constant and axo-somatic conductance ratio all indicate that the value found for the specific membrane resistance of the G cell, while unexpectedly large, is valid.6. The magnitude of this value suggests that the conductance (permeability) of its membrane to ions is much smaller than that previously assumed for nerve membranes; this small conductance may be related to the larger surface-to-volume ratio of the G cell.

The geometrical factors determining the electrotonic properties of a molluscan neurone

1. Light and electron micrographs of sections of the gastro-oesophageal giant neurone (G cell) of the nudibranch mollusc, Anisodoris nobilis, show that its somatic and axonal membranes are deeply infolded. The surface and volume of its soma and axon have been calculated from measurements taken at the light and electron microscope on sections of the G cell.2. The surface of the soma is approximately 7.5 times as large as that of a sphere having the same volume. For a typical cell the soma has a volume of 1.5 x 10(-5) cm(3) and a surface of 2 x 10(-2) cm(2); the axon has a volume of 5 x 10(-5) cm(3) and a surface of 5 x 10(-1) cm(2).3. Because the axon is star shaped in cross-section, its geometry cannot be described by a single parameter (diameter or radius). Furthermore, the axon is beaded, and both the area (A) and the perimeter (P) of its cross-section change from point to point.4. However, in spite of the apparent irregularity of their cross-sections, all axons examined could be characterized by a constant A/P ratio. This ratio also remains constant when the axons are stretched.5. According to the equations derived in the Appendix, the geometrical factor for the length constant in a folded fibre is H = radical(A/P); therefore, in the G cell the length constant (and hence the conduction velocity) should be independent of the stretch applied to the axon.6. The geometrical factor required to calculate the axonal input conductance is M = radical(A.P). M changes in adjacent segments of the same axon; in each segment its value depends on how much the axon is stretched.7. The input conductance of the whole axon can be calculated by applying a modified form of Rall's equations for dendritic trees. The results suggest that the input conductance of the G cell axon should vary with stretch and should be large in comparison to that of the soma.

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.

Potential-dependent membrane current during the active transport of ions in snail neurones

1. The membrane current caused by the iontophoretic injection of sodium into giant neurones of the snail Helix pomatia was investigated under a long lasting voltage clamp. The inhibition of this current by ouabain (10(-4) M) and by cooling to + 7 degrees C confirmed its link with the active transport of ions. Therefore this current is called the pump current.2. Over the range of membrane potential -40 to -100 mV the changes in the steady current-voltage curves caused by the pump current development were investigated. The pump current was found to be potential-dependent. It decreased with increasing hyperpolarization of the neurone.3. With large hyperpolarizations the current-voltage curves obtained before the sodium injection and after eliciting the pump current coincided with each other. An increase in the membrane conductance was observed over the range of membrane potential corresponding to the pump current display.4. The applied sodium injections did not cause any marked changes in the passive permeability of the membrane. This fact made it possible to measure the charge transferred across the membrane during operation of the pump current. Unlike previous data, the ratio of this value to the charge used to inject sodium into the neurone appeared to be a variable.5. When the preparation was cooled to + 11 degrees C, and also during the first few minutes after the application of a potassium-free solution, both the pump current and the membrane potential at which it disappeared could increase.6. The pump current measurements during a number of transitions from one fixed level of the membrane potential to another showed that the current did not depend upon the potential at which it developed before each transition.7. The data presented allow the suggestion that the potential dependence of the pump current is determined by the changes in the rate of active transport of potassium, while the rate of active transport of sodium remains constant.

The independence of electrogenic sodium transport and membrane potential in a molluscan neurone

1. The current-voltage relations of the Anisodoris giant neurone (G cell) were studied in the presence and absence of Na pump activity.2. Inhibition of the electrogenic Na pump with ouabain had no effect on either the presence at warm temperatures (10-15 degrees C), or absence at cold temperatures (0-5 degrees C), of inward-going rectification.3. Abolition of inward-going rectification in the warm, by replacement of external K with Rb, did not affect the electrogenic Na pump.4. The current generated by the electrogenic pump was essentially constant between the membrane potentials of - 30 and - 100 mV.5. The potential produced by the electrogenic pump can be predicted by a modification of the constant field equation.6. It is estimated that the energy required to extrude Na was between 3160 and 3700 cal/g-atom, and that uncoupled Na efflux during pump activity was typically between 0.2 and 4.0 p-mole/cm(2).sec.