The electrogenic sodium pump and membrane potential of identified neurones in Helix aspersa

Na+/K+-pump and neurotransmitter membrane receptors

Na⁺/K⁺-pump is an electrogenic transmembrane ATPase located in the outer plasma membrane of cells. The Na⁺/K⁺-ATPase pumps 3 sodium ions out of cells while pumping 2 potassium ions into cells. Both cations move against their concentration gradients. This enzyme's electrogenic nature means that it has a chronic role in stabilizing the resting membrane potential of the cell, in regulating the cell volume and in the signal transduction of the cell. This review will mainly consider the role of the Na⁺/K⁺-pump in neurons, with an emphasis on its role in modulating neurotransmitter receptor. Most of the literature on the modulation of neurotransmitter receptors refers to the situation in the mammalian nervous system, but the position is likely to be similar in most, if not all, invertebrate nervous systems.

Dihydrotubastrines: phenethylguanidine analogues from the Indo-Pacific marine sponge Petrosia cf. contignata

Two phenethylguanidine derivatives, 7,8-dihydrotubastrine (1) and 4-deoxy-7,8-dihydrotubastrine (2), along with the sterol xestobergsterol A (3), were isolated from the marine sponge Petrosia cf. contignata. The structures of the new natural products 1 and 2 were based on spectroscopic data and comparison to the literature properties for semisynthetic 1. This is the first example from this compound class with a saturated acyclic C2 unit.

Effects of monensin on the response to low potassium in a molluscan muscle, the radular protractor of Busycon canaliculatum

1. A sucrose gap technique was used to study the effect of a sodium ionophore on the potential changes which occur during superfusion with potassium-free solution. Crucial values were checked with a microelectrode technique. 2. Potassium-free solution induces a complex response consisting of a hyperpolarizing phase (HP) and then a depolarization phase (DP) during exposure to zero K+, followed by a transient extra hyperpolarizing phase (EHP) on readmission of K+. 3. The sodium ionophore, monensin, has the effect of increasing the amplitude of the DP, in perfusion medium of normal Na+ content. This is similar to the effect of treatment with neurohumors and to the after-effect of direct electrical stimulation. The effects of ACh and monensin are additive. 5. These effects are consistent with an action of monensin in increasing Na+ flux in the direction of the concentration gradient and support the hypothesis that neurohumors stimulate the sodium pump by increasing Na+ influx.

Interpretation of current-voltage relationships for "active" ion transport systems: I. Steady-state reaction-kinetic analysis of class-I mechanisms

This paper develops a simple reaction-kinetic model to describe electrogenic pumping and co- (or counter-) transport of ions. It uses the standard steady-state approach for cyclic enzyme- or carrier-mediated transport, but does not assume rate-limitation by any particular reaction step. Voltage-dependence is introduced, after the suggestion of Läuger and Stark (Biochim. Biophys. Acta 211:458-466, 1970), via a symmetric Eyring barrier, in which the charge-transit reaction constants are written as k12 = ko12 exp(zF delta psi/2RT) and k21 = ko21 exp(-zF delta psi/2RT). For interpretation of current-voltage relationships, all voltage-independent reaction steps are lumped together, so the model in its simplest form can be described as a pseudo-2-state model. It is characterized by the two voltage-dependent reaction constants, two lumped voltage-independent reaction constants (k12, k21), and two reserve factors (ri, ro) which formally take account of carrier states that are indistinguishable in the current-voltage (I-V) analysis. The model generates a wide range of I-V relationships, depending on the relative magnitudes of the four reaction constants, sufficient to describe essentially all I-V datas now available on "active" ion-transport systems. Algebraic and numerical analysis of the reserve factors, by means of expanded pseudo-3-, 4-, and 5-state models, shows them to be bounded and not large for most combinations of reaction constants in the lumped pathway. The most important exception to this rule occurs when carrier decharging immediately follows charge transit of the membrane and is very fast relative to other constituent voltage-independent reactions. Such a circumstance generates kinetic equivalence of chemical and electrical gradients, thus providing a consistent definition of ion-motive forces (e.g., proton-motive force, PMF). With appropriate restrictions, it also yields both linear and log-linear relationships between net transport velocity and either membrane potential or PMF. The model thus accommodates many known properties of proton-transport systems, particularly as observed in "chemiosmotic" or energy-coupling membranes.

Characterization of the electrogenic sodium pump in cardiac Purkinje fibres

1. The Na pump is examined in sheep cardiac Purkinje fibres using a two micro-electrode voltage clamp technique.2. After reducing the external K concentration, [K](o), to zero for 2 min or more, subsequent addition of an ;activator cation' (known to activate the Na pump in other preparations) produces a transient increase of outward current. This outward current transient is abolished by 10(-5)M-strophanthidin (cf. Gadsby & Cranefield, 1979a).3. It is concluded that this transient increase of outward current is a result of a transient stimulation of the sodium pump by the raised [Na](i) following exposure to 0-K(o). Although this current transient may reflect the activity of an electrogenic Na pump, it is difficult to use K as the activator cation to establish this point. This is due to the extracellular K depletion that occurs during Na pump reactivation and the subsequent change that this K depletion produces in the current-voltage relationship of the Purkinje fibre.4. Rb(o) or Cs(o) have been used instead of K(o) to reactivate the Na pump when examining the transient increase of outward current. On adding either of these cations after exposing a preparation to a solution without such ;activator cations', the outward current transient is relatively voltage independent over a wide range of potentials (-90 to +10 mV). It is concluded that, following the addition of Rb(o) or Cs(o), the transient increase of outward current is a direct measure of the transient increase of the electrogenic Na pump current.5. Increasing [Rb](o) or [Cs](o) over the range of 0-40 mM increases the rate of decay of the electrogenic Na pump current transient. Using a simple model (cf. Rang & Ritchie, 1968), it is shown that the decay rate constant of the electrogenic Na pump current transient is a good measure of the degree of activation of the external site of the Na pump. At a given concentration of activator cation, Rb(o) produces a greater activation of the Na pump than does Cs(o). The K(0.5) for Rb(o) is 6.3 mM and for Cs(o) is 14.2 mM. Li(o) activates the Na pump more weakly than Rb(o) and Cs(o).6. The coupling ratio of the Na pump is shown to be independent of Rb(o) or Cs(o) over the range 2-40 mM. Furthermore, consistent with the results of Gadsby & Cranefield (1979a), the coupling ratio is independent of Na(i) over the range considered.7. The Q(10) for the electrogenic Na pump current transient varies between 1.6 and 2.3 over the range of temperature 26-46 degrees C.8. A maximum Na pump current of about 0.78 muA cm(-2) is obtained. Assuming a coupling ratio of 3Na/2K, the rate of Na ion transport into the cell is estimated to be about 23 p-mole cm(-2) sec(-1). Assuming a Na pump turnover of 150 sec(-1), we estimate that there are about 1000 Na pump sites per mum(2) of cell surface.9. We conclude that the electrogenic Na pump current transient provides a good measure of the activity of the Na pump when Rb or Cs are used as ;activator cations'. This measure can be used in the intact preparation to investigate the relationship between Na pump rate and other cellular events such as the regulation of tension (Eisner & Lederer, 1980).

Current-voltage relationships for the plasma membrane and its principal electrogenic pump in Neurospora crassa: I. Steady-state conditions

The nonlinear membrane current-voltage relationship (I-V curve) for intact hyphae of Neurospora crassa has been determined by means of a 3-electrode voltage-clamp technique, plus "quasi-linear" cable theory. Under normal conditions of growth and respiration, the membrane I-V curve is best described as a parabolic segment convex in the direction of depolarizing current. At the average resting potential of - 174 mV, the membrane conductance is approximately 190 micronhos/cm2; conductance increase to approximately 240 micronhos/cm2 at -300 mV, and decreases to approximately 130 micronhos/cm2 at 0 mV. Irreversible membrane breakdown occurs at potentials beyond this range. Inhibition of the primary electrogenic pump in Neurospora by ATP withdrawal (with 1 mM KCN) depolarizes the membrane to the range of -40 to -70 mV and reduces the slope of the I-V curve by a fixed scaling factor of approximately 0.8. For wild-type Neurospora, compared under control conditions and during steady-state inhibition by cyanide, the I-V difference curve--presumed to define the current-voltage curve for the electrogenic pump--is a saturation function with maximal current of approximately 20 muA/cm2, a half saturation potential near -300 mV, and a projected reversal potential of ca. -400 mV. This value is close to the maximal free energy available to the pump from ATP hydrolysis, so that pump stoichiometry must be close to 1 H+ extruded:1 ATP split. The time-courses of change in membrane potential and resistance with cyanide are compatible with the steady-state I-V curves, under the assumption the cyanide has no major effects other than ATP withdrawal. Other inhibitors, uncouplers, and lowered temperature all have more complicated effects. The detailed temporal analysis of voltage-clamp data showed three time-constants in the clamping currents: one of 10 msec, for charging the membrane capacitance (0.9 muF/cm/2); a second of 50-75 msec; and a third of 20-30 sec, perhaps representing changes of intracellular composition.

Further studies of the potential-dependence of the sodium-induced membrane current in snail neurones

1. The potential-dependence of the membrane current induced by intracellular injections of sodium ions was studied on giant neurones of the snail Helix pomatia. This current decreases with membrane hyperpolarization at room temperature and can be reversed at sufficiently negative holding potentials. The same injections at 7 degrees C, as well as injections of lithium or potassium ions do not induce membrane currents and do not increase membrane conductance. 2. An increase in the amount of injected sodium changes the potential-dependence of the induced membrane currents. Small injections (about 1 muC) induce a current that does not depend upon the membrane potential. Further increase in the injection size not only increases the induced current but also enhances its potential-dependence and often reveals the existence of a reversal potential. The latter reaches -60 to -65 mV with large sodium injections. 3. An increase in extracellular potassium concentration from 4 to 8 mM shifts the reversal potential 17 mV in the depolarizing direction, and a decrease from 4 to 2 mM shifts it 14 mV in the hyperpolarizing direction. Replacement of potassium by rubidium or elimination of sodium ions from the outside solution, does not affect the induced current or its potential-dependence. 4. The coefficient of electrogenicity (the ratio between the amount of charge transferred by the sodium-induced membrane current and the amount brought into the cell during the injection) increases with an increase in the injection size if the membrane potential is clamped near the resting potential level. This relation is reversed when the holding potential is -80 mV. The reversal takes place at holding potentials near -60 mV. 5. 10 mM TEA does not affect the induced current and its potential-dependence. 6. It is suggested that the potential-dependence of the sodium-induced membrane current is a result of a specific increase in the membrane potassium conductance that is coupled with high activity of the sodium pump.