Current generated by backward-running electrogenic Na pump in squid giant axons

The Na+,K+-ATPase and its stoichiometric ratio: some thermodynamic speculations

 Almost seventy years after its discovery, the sodium-potassium adenosine triphosphatase (the sodium pump) located in the cell plasma membrane remains a source of novel mechanistic and physiologic findings. A noteworthy feature of this enzyme/transporter is its robust stoichiometric ratio under physiological conditions: it sequentially counter-transports three sodium ions and two potassium ions against their electrochemical potential gradients per each hydrolyzed ATP molecule. Here we summarize some present knowledge about the sodium pump and its physiological roles, and speculate whether energetic constraints may have played a role in the evolutionary selection of its characteristic stoichiometric ratio.

Effect of extracellular volume on the energy stored in transmembrane concentration gradients

The amount of energy that can be retrieved from a concentration gradient across a membrane separating two compartments depends on the relative size of the compartments. Having a larger low-concentration compartment is in general beneficial. It is shown here analytically that the retrieved energy further increases when the high-concentration compartment shrinks during the mixing process, and a general formula is derived for the energy when the ratio of transported solvent to solute varies. These calculations are then applied to the interstitial compartment of the brain, which is rich in Na^{+} and Cl^{-} ions and poor in K^{+}. The reported shrinkage of this compartment, and swelling of the neurons, during oxygen deprivation is shown to enhance the energy recovered from NaCl entering the neurons. The slight loss of energy on the part of K^{+} can be compensated for by the uptake of K^{+} ions by glial cells. In conclusion, the present study proposes that the reported fluctuations in the size of the interstitial compartment of the brain (expansion during sleep and contraction during oxygen deprivation) optimize the amount of energy that neurons can store in, and retrieve from, their ionic concentration gradients.

Measuring enzyme activities in crude homogenates: Na+/K+-ATPase as a case study in optimizing assays

In this review of assays of Na⁺/K⁺-ATPase (NKA), we explore the choices made by researchers assaying the enzyme to investigate its role in physiological regulation. We survey NKA structure and function in the context of how it is typically assayed, and how technical choices influence what can be said about the enzyme. In comparing different methods for extraction and assay of NKA, we identified a series of common pitfalls that compromise the veracity of results. We include experimental work to directly demonstrate how choices in detergents, salts and substrates influence NKA activities measured in crude homogenates. Our review of assay approaches integrates what is known from enzymology, biomedical physiology, cell biology and evolutionary biology, offering a more robust method for assaying the enzyme in meaningful ways, identifying caveats and future directions to explore its structure and function. The goal is to provide the sort of background on the enzyme that should be considered in exploring the function of the enzyme in comparative physiology.

Deceleration of the E1P-E2P transition and ion transport by mutation of potentially salt bridge-forming residues Lys-791 and Glu-820 in gastric H+/K+-ATPase

A lysine residue within the highly conserved center of the fifth transmembrane segment in P(IIC)-type ATPase α-subunits is uniquely found in H,K-ATPases instead of a serine in all Na,K-ATPase isoforms. Because previous studies suggested a prominent role of this residue in determining the electrogenicity of non-gastric H,K-ATPase and in pK(a) modulation of the proton-translocating residues in the gastric H,K-ATPases as well, we investigated its functional significance for ion transport by expressing several Lys-791 variants of the gastric H,K-ATPase in Xenopus oocytes. Although the mutant proteins were all detected at the cell surface, none of the investigated mutants displayed any measurable K(+)-induced stationary currents. In Rb(+) uptake measurements, replacement of Lys-791 by Arg, Ala, Ser, and Glu substantially impaired transport activity and reduced the sensitivity toward the E(2)-specific inhibitor SCH28080. Furthermore, voltage clamp fluorometry using a reporter site in the TM5/TM6 loop for labeling with tetra-methylrhodamine-6-maleimide revealed markedly changed fluorescence signals. All four investigated mutants exhibited a strong shift toward the E(1)P state, in agreement with their reduced SCH28080 sensitivity, and an about 5-10-fold decreased forward rate constant of the E(1)P ↔ E(2)P conformational transition, thus explaining the E(1)P shift and the reduced Rb(+) transport activity. When Glu-820 in TM6 adjacent to Lys-791 was replaced by non-charged or positively charged amino acids, severe effects on fluorescence signals and Rb(+) transport were also observed, whereas substitution by aspartate was less disturbing. These results suggest that formation of an E(2)P-stabilizing interhelical salt bridge is essential to prevent futile proton exchange cycles of H(+) pumping P-type ATPases.

Electrogenic Na+/Ca2+-exchange of nerve and muscle cells

The plasma membrane Na(+)/Ca(2+)-exchanger is a bi-directional electrogenic (3Na(+):1Ca(2+)) and voltage-sensitive ion transport mechanism, which is mainly responsible for Ca(2+)-extrusion. The Na(+)-gradient, required for normal mode operation, is created by the Na(+)-pump, which is also electrogenic (3Na(+):2K(+)) and voltage-sensitive. The Na(+)/Ca(2+)-exchanger operational modes are very similar to those of the Na(+)-pump, except that the uncoupled flux (Na(+)-influx or -efflux?) is missing. The reversal potential of the exchanger is around -40 mV; therefore, during the upstroke of the AP it is probably transiently activated, leading to Ca(2+)-influx. The Na(+)/Ca(2+)-exchange is regulated by transported and non-transported external and internal cations, and shows ATP(i)-, pH- and temperature-dependence. The main problem in determining the role of Na(+)/Ca(2+)-exchange in excitation-secretion/contraction coupling is the lack of specific (mode-selective) blockers. During recent years, evidence has been accumulated for co-localisation of the Na(+)-pump, and the Na(+)/Ca(2+)-exchanger and their possible functional interaction in the "restricted" or "fuzzy space." In cardiac failure, the Na(+)-pump is down-regulated, while the exchanger is up-regulated. If the exchanger is working in normal mode (Ca(2+)-extrusion) during most of the cardiac cycle, upregulation of the exchanger may result in SR Ca(2+)-store depletion and further impairment in contractility. If so, a normal mode selective Na(+)/Ca(2+)-exchange inhibitor would be useful therapy for decompensation, and unlike CGs would not increase internal Na(+). In peripheral sympathetic nerves, pre-synaptic alpha(2)-receptors may regulate not only the VSCCs but possibly the reverse Na(+)/Ca(2+)-exchange as well.

Recent Insights into the Structure and Mechanism of the Sodium Pump

The sodium pump (or Na-K-ATPase) is essential to the function of animal cells. Publication of the related calcium pump (SERCA) structure together with several recent results from a variety of approaches allow us to propose a mechanistic model to answer the question: “How does the sodium pump pump?”

Quaternary organic amines inhibit Na,K pump current in a voltage-dependent manner: direct evidence of an extracellular access channel in the Na,K-ATPase

The effects of organic quaternary amines, tetraethylammonium (TEA) chloride and benzyltriethylammonium (BTEA) chloride, on Na,K pump current were examined in rat cardiac myocytes superfused in extracellular Na(+)-free solutions and whole-cell voltage-clamped with patch electrodes containing a high Na(+)-salt solution. Extracellular application of these quaternary amines competitively inhibited extracellular K(+) (K(+)(o)) activation of Na,K pump current; however, the concentration for half maximal inhibition of Na,K pump current at 0 mV (K(0)(Q)) by BTEA, 4.0 +/- 0.3 mM, was much lower than the K(0)(Q) for TEA, 26.6 +/- 0.7 mM. Even so, the fraction of the membrane electric field dissipated during K(+)(o) activation of Na,K pump current (lambda(K)), 39 +/- 1%, was similar to lambda(K) determined in the presence of TEA (37 +/- 2%) and BTEA (35 +/- 2%), an indication that the membrane potential (V(M)) dependence for K(+)(o) activation of the Na,K pump current was unaffected by TEA and BTEA. TEA was found to inhibit the Na,K pump current in a V(M)-independent manner, i.e., inhibition of current dissipated 4 +/- 2% of the membrane electric field. In contrast, BTEA dissipated 40 +/- 5% of the membrane electric field during inhibition of Na,K pump current. Thus, BTEA inhibition of the Na,K-ATPase is V(M)-dependent. The competitive nature of inhibition as well as the similar fractions of the membrane electric field dissipated during K(+)(o)-dependent activation and BTEA-dependent inhibition of Na,K pump current suggest that BTEA inhibits the Na,K-ATPase at or very near the enzyme's K(+)(o) binding site(s) located in the membrane electric field. Given previous findings that organic quaternary amines are not occluded by the Na,K-ATPase, these data clearly demonstrate that an ion channel-like structure provides access to K(+)(o) binding sites in the enzyme.

Ion channel-like properties of the Na+/K+ Pump

Ion pumps and exchangers are considered to be different from ion channels for two principal reasons. Ion pumps move ions against, whereas ion channels allow ions to move with, the electrochemical potential gradient, and pumps transport ions relatively slowly, approximately 10(2) s(-1), whereas channels conduct ions rapidly, approximately 10(7) s(-1). However, the latter high rate refers only to the open pore, and yet all ion channels contain at least one gate. Not surprisingly, the conformational changes associated with channel gating occur with kinetics similar to those of ion pumping. Indeed, ion pumps may be viewed as ion channels with two gates, one external to, and the other internal to, the ion binding cavity. The simple operational rule for such a pump is that the two gates should never be open simultaneously; otherwise, the pump would become a channel and conduct dissipative fluxes several orders of magnitude larger than, and in the opposite direction to, the active transport fluxes. Analyses of Na(+) ion movements mediated by the Na(+)/K(+) pump under various conditions have suggested that in at least one, short-lived, conformation of the pump, an ion-channel-like structure, closed at its intracellular end, connects the extracellular solution with the ion binding sites deep in the protein core. Here we use the marine toxin, palytoxin, to act on Na(+)/K(+) pumps in outside-out patches excised from cardiac myocytes and so transform the pumps into nonselective cation channels which we study using macroscopic, and single-channel, recording. We find that gating of the palytoxin-induced channels is regulated by the pump's natural ligands. Thus, external K(+) congeners tend to close, and external Na(+) tends to open, an extracellular gate, whereas ATP acts from the cytoplasmic solution to open an intracellular gate. These gating influences echo the normal ion occlusion and deocclusion reactions that first entrap two extracellular K(+) ions within the interior of the pump (between the two gates) and then release them to the cytoplasmic side in a step accelerated by ATP. These results offer the promise of being able to examine ion occlusion and deocclusion steps at the microscopic level in single Na(+)/K(+) pump molecules.

Differential role of KIR channel and Na(+)/K(+)-pump in the regulation of extracellular K(+) in rat hippocampus

Little information is available on the specific roles of different cellular mechanisms involved in extracellular K(+) homeostasis during neuronal activity in situ. These studies have been hampered by the lack of an adequate experimental paradigm able to separate K(+)-buffering activity from the superimposed extrusion of K(+) from variably active neurons. We have devised a new protocol that allows for such an analysis. We used paired field- and K(+)-selective microelectrode recordings from CA3 stratum pyramidale during maximal Schaffer collateral stimulation in the presence of excitatory synapse blockade to evoke purely antidromic spikes in CA3. Under these conditions of controlled neuronal firing, we studied the [K(+)]o baseline during 0.05 Hz stimulation, and the accumulation and rate of recovery of extracellular K(+) at higher frequency stimulation (1-3 Hz). In the first set of experiments, we showed that neuronal hyperpolarization by extracellular application of ZD7288 (11 microM), a selective blocker of neuronal I(h) currents, does not affect the dynamics of extracellular K(+). This indicates that the K(+) dynamics evoked by controlled pyramidal cell firing do not depend on neuronal membrane potential, but only on the balance between K(+) extruded by firing neurons and K(+) buffered by neuronal and glial mechanisms. In the second set of experiments, we showed that di-hydro-ouabain (5 microM), a selective blocker of the Na(+)/K(+)-pump, yields an elevation of baseline [K(+)]o and abolishes the K(+) recovery during higher frequency stimulation and its undershoot during the ensuing period. In the third set of experiments, we showed that Ba(2+) (200 microM), a selective blocker of inwardly rectifying K(+) channels (KIR), does not affect the posttetanus rate of recovery of [K(+)]o, nor does it affect the rate of K(+) recovery during high-frequency stimulation. It does, however, cause an elevation of baseline [K(+)]o and an increase in the amplitude of the ensuing undershoot. We show for the first time that it is possible to differentiate the specific roles of Na(+)/K(+)-pump and KIR channels in buffering extracellular K(+). Neuronal and glial Na(+)/K(+)-pumps are involved in setting baseline [K(+)]o levels, determining the rate of its recovery during sustained high-frequency firing, and determining its postactivity undershoot. Conversely, glial KIR channels are involved in the regulation of baseline levels of K(+), and in decreasing the amplitude of the postactivity [K(+)]o undershoot, but do not affect the rate of K(+) clearance during neuronal firing. The results presented provide new insights into the specific physiological role of glial KIR channels in extracellular K(+) homeostasis.

Electrophysiology of the sodium-potassium-ATPase in cardiac cells

Like several other ion transporters, the Na(+)-K(+) pump of animal cells is electrogenic. The pump generates the pump current I(p). Under physiological conditions, I(p) is an outward current. It can be measured by electrophysiological methods. These methods permit the study of characteristics of the Na(+)-K(+) pump in its physiological environment, i.e., in the cell membrane. The cell membrane, across which a potential gradient exists, separates the cytosol and extracellular medium, which have distinctly different ionic compositions. The introduction of the patch-clamp techniques and the enzymatic isolation of cells have facilitated the investigation of I(p) in single cardiac myocytes. This review summarizes and discusses the results obtained from I(p) measurements in isolated cardiac cells. These results offer new exciting insights into the voltage and ionic dependence of the Na(+)-K(+) pump activity, its effect on membrane potential, and its modulation by hormones, transmitters, and drugs. They are fundamental for our current understanding of Na(+)-K(+) pumping in electrically excitable cells.

Voltage dependence of the apparent affinity for external Na(+) of the backward-running sodium pump

The steady-state voltage and [Na(+)](o) dependence of the electrogenic sodium pump was investigated in voltage-clamped internally dialyzed giant axons of the squid, Loligo pealei, under conditions that promote the backward-running mode (K(+)-free seawater; ATP- and Na(+)-free internal solution containing ADP and orthophosphate). The ratio of pump-mediated (42)K(+) efflux to reverse pump current, I(pump) (both defined by sensitivity to dihydrodigitoxigenin, H(2)DTG), scaled by Faraday's constant, was -1.5 +/- 0.4 (n = 5; expected ratio for 2 K(+)/3 Na(+) stoichiometry is -2.0). Steady-state reverse pump current-voltage (I(pump)-V) relationships were obtained either from the shifts in holding current after repeated exposures of an axon clamped at various V(m) to H(2)DTG or from the difference between membrane I-V relationships obtained by imposing V(m) staircases in the presence or absence of H(2)DTG. With the second method, we also investigated the influence of [Na(+)](o) (up to 800 mM, for which hypertonic solutions were used) on the steady-state reverse I(pump)-V relationship. The reverse I(pump)-V relationship is sigmoid, I(pump) saturating at large negative V(m), and each doubling of [Na(+)](o) causes a fixed (29 mV) rightward parallel shift along the voltage axis of this Boltzmann partition function (apparent valence z = 0.80). These characteristics mirror those of steady-state (22)Na(+) efflux during electroneutral Na(+)/Na(+) exchange, and follow without additional postulates from the same simple high field access channel model (Gadsby, D.C., R.F. Rakowski, and P. De Weer, 1993. Science. 260:100-103). This model predicts valence z = nlambda, where n (1.33 +/- 0.05) is the Hill coefficient of Na binding, and lambda (0.61 +/- 0.03) is the fraction of the membrane electric field traversed by Na ions reaching their binding site. More elaborate alternative models can accommodate all the steady-state features of the reverse pumping and electroneutral Na(+)/Na(+) exchange modes only with additional assumptions that render them less likely.

Sodium dynamics underlying burst firing and putative mechanisms for the regulation of the firing pattern in midbrain dopamine neurons: a computational approach

A physiologically based multicompartmental computational model of a midbrain dopamine (DA) neuron, calibrated using data from the literature, was developed and used to test the hypothesis that sodium dynamics drive the generation of a slow oscillation postulated to underlie NMDA-evoked bursting activity in a slice preparation. The full compartmental model was reduced to three compartments and ultimately to two variables, while retaining the biophysical interpretation of all parameters. A phase-plane analysis then suggested two mechanisms for the regulation of the firing pattern: (1) bursting activity is favored by manipulations that enhance the region of negative slope in the whole-cell IV curve and inhibited by those manipulations, such as increasing linear currents, that tend to dampen this region and (2) assuming a region of negative slope is present in the IV curve, the bias of the system can be altered, either enabling or disabling bursting. The model provides a coherent framework for interpreting the effects of glutamate, aspartate, NMDA, and GABA agonists and antagonists under current-clamp conditions, as well as the effects of NMDA and barium under voltage-clamp conditions.

Voltage-dependent inhibition of the Na+,K+ pump by tetraethylammonium

Tetraethylammonium (TEA+) is an effective inhibitor of a variety of K+ channels, and has been widely used to reduce K+-sensitive background conductances in electrophysiological investigations of the Na+,K+-ATPase. Here we demonstrate by combination of two-electrode voltage clamp (TEVC) and giant patch clamp of Xenopus oocytes, and measurements of the activity of purified ATPase of pig kidney that TEA+ directly inhibits the Na+,K+-ATPase from the outside. The KI value in TEVC experiments at 0 mV is about 10 mM increasing with more negative potentials. A similar voltage-dependent inhibition by TEA+ was observed in the excised membrane patches except that the apparent KI value at 0 mV is about 100 mM, a value nearly identical to that found for inhibition of purified kidney ATPase. The voltage-dependent inhibition can be described by an effective valency of 0.39 and is attributed to an interference with the voltage-dependent binding of K+ at an external access channel. The apparent dielectric length of the access channel for K+ is not affected by TEA+.

Cardiac Na+ pump current-voltage relationships at various transmembrane gradients of the pumped cations

Thermodynamic considerations predict changes of the Na+ pump current (Ip)-voltage (V) relationship of animal cells upon variations of the electrochemical gradients against which cations must be pumped. Experimental data in support of the predictions are sparse. Therefore, the effect on the Ip-V relationship of various electrochemical gradients for pumped Na+ and Cs+ was studied at constant deltaGATP (approximately -39kJ/mol in cardioballs from sheep Purkinje fibres. Control of the subsarcolemmal ionic concentrations during whole-cell recording was ensured by activation of Ip below its half maximal activity or by measuring the initial Ip following reactivation of the Na+/K+ pump. With gradients close to physiological conditions Ip was outward over the entire voltage range and the Ip-V relationship showed a maximum near zero potential. Steepening the ionic gradients diminished the Ip amplitude and outward pump current was no longer detectable between -65 mV and -110 mV. Flattened ionic gradients increased the Ip amplitude and shifted apparently the reversal potential Erev to more negative values. These changes are in line with theoretical considerations. The measured Ip-V relationships were fitted by curves computed on the basis of a simplified Post-Albers scheme of Na+/Cs+ pumping. The increased Ip amplitude at flat ionic gradients was due to a decrease of [Cs+]o for half maximal Ip activation. The maximal Ip amplitude remained unaffected

Change of Na+ pump current reversal potential in sheep cardiac Purkinje cells with varying free energy of ATP hydrolysis

1. The Na(+)-K+ pump current, Ip, of cardioballs from isolated sheep cardiac Purkinje cells was measured at 30-34 degrees C by means of whole-cell recording. 2. Under physiological conditions Ip is an outward current. Experimental conditions which cause a less negative free energy of intracellular ATP hydrolysis (delta GATP) and steeper sarcolemmal gradients for the pumped Na+ and Cs+ ions evoked an Ip in the inward direction over a wide range of membrane potentials. The reversal of the Ip direction was reversible. 3. The inwardly directed Ip increased with increasingly negative membrane potentials and amounted to -0.13 +/- 0.03 microA cm-2 (mean +/- S.E.M.; n = 6) at -95 mV. 4. The reversal potential (Erev) of Ip was studied as a function of delta GATP at constant sarcolemmal gradients of the pumped cations. 5. In order to vary delta GATP the cell interior was dialysed with patch pipette solutions containing 10 mM ATP and different concentrations of ADP and inorganic phosphate. The media were composed to produce delta GATP levels of about -58, -49 and -39 kJ mol-1. 6. A less negative delta GATP shifted Erev to more positive membrane potentials. From measurements of Ip as a function of membrane potential Erev was estimated to be -195, -115 and -60 mV at delta GATP levels of approximately -58, -49 and -39 kJ mol-1, respectively. The calculated Erev amounted to -224 mV at delta GATP approximately -58 kJ mol-1, -126 mV at delta GATP approximately 49 kJ mol-1 and -24 mV at delta GATP approximately -39 kJ mol-1. 7. Possible reasons for the discrepancy between estimated and calculated Erev values are discussed. 8. Shifting delta GATP to less negative values not only altered Erev but also diminished Ip at each membrane potential tested. The maximal Ip (Ip,max), which can be activated by external Cs+ (Cs+o), decreased under these conditions, whereas [Cs+]o causing half-maximal Ip activation remained unchanged. Similarly, the voltage dependence of Ip activation by Cs+o was unaffected. 9. It is concluded that Erev of Ip varies with delta GATP at constant sarcolemmal gradients of the pumped cations. This agrees with thermodynamic considerations.

Basolateral Na(+)-H+ antiporter. Mechanisms of electroneutral and conductive ion transport

The basolateral Na-H antiporter of the turtle colon exhibits both conductive and electroneutral Na+ transport (Post and Dawson. 1992. American Journal of Physiology. 262:C1089-C1094). To explore the mechanism of antiporter-mediated current flow, we compared the conditions necessary to evoke conduction and exchange, and determined the kinetics of activation for both processes. Outward (cell to extracellular fluid) but not inward (extracellular fluid to cell) Na+ or Li+ gradients promoted antiporter-mediated Na+ or Li+ currents, whereas an outwardly directed proton gradient drove inward Na+ or Li+ currents. Proton gradient-driven, "counterflow" current is strong evidence for an exchange stoichiometry of > 1 Na+ or Li+ per proton. Consistent with this notion, outward Na+ and Li+ currents generated by outward Na+ or Li+ gradients displayed sigmoidal activation kinetics. Antiporter-mediated proton currents were never observed, suggesting that only a single proton was transported per turnover of the antiporter. In contrast to Na+ conduction, Na+ exchange was driven by either outwardly or inwardly directed Na+, Li+, or H+ gradients, and the activation of Na+/Na+ exchange was consistent with Michaelis-Menten kinetics (K1/2 = 5 mM). Raising the extracellular fluid Na+ or Li+ concentration, but not extracellular fluid proton concentration, inhibited antiporter-mediated conduction and activated Na+ exchange. These results are consistent with a model for the Na-H antiporter in which the binding of Na+ or Li+ to a high-affinity site gives rise to one-for-one cation exchange, but the binding of Na+ or Li+ ions to other, lower-affinity sites can give rise to a nonunity, cation exchange stoichiometry and, hence, the net translocation of charge. The relative proportion of conductive and nonconductive events is determined by the magnitude and orientation of the substrate gradient and by the serosal concentration of Na+ or Li+.

Osmotic strength differentiates between two types of calcium transport pathways regulating catecholamine secretion from cultured bovine chromaffin cells

Calcium transport and catecholamine secretion was measured in cultured bovine chromaffin cells. Calcium ions which entered the cells following stimulation with either nicotine or 50 mM KCl (high potassium) triggered catecholamine release, but then inactivated the secretory process. The nicotine and the high potassium-induced calcium transport mechanisms were mechanistically distinct, but functionally dependent on each other. The specific evidence is that whereas the high potassium-induced Ca2+ influx was found to be inhibited by hyperosmotic medium, the nicotine-stimulated calcium influx was unaffected under these conditions. High potassium and nicotine-stimulated catecholamine release were also differently affected by hyperosmotic medium. While potassium-stimulated catecholamine release was profoundly inhibited by hyperosmolarity, nicotine-stimulated release was only moderately inhibited. Sequential treatments of cells with nicotine and high potassium, under isotonic physiological conditions, indicate that there is a functional, biochemical communication between the otherwise mechanistically distinct calcium channels. Calcium ions which were found to inactivate these channels may be the basis for such communication.

When is an inhibitory synapse effective?

Interactions between excitatory and inhibitory synaptic inputs on dendrites determine the level of activity in neurons. Models based on the cable equation predict that silent shunting inhibition can strongly veto the effect of an excitatory input. The cable model assumes that ionic concentrations do not change during the electrical activity, which may not be a valid assumption, especially for small structures such as dendritic spines. We present here an analysis and computer simulations to show that for large Cl- conductance changes, the more general Nernst-Planck electrodiffusion model predicts that shunting inhibition on spines should be much less effective than that predicted by the cable model. This is a consequence of the large changes in the intracellular ionic concentration of Cl- that can occur in small structures, which would alter the reversal potential and reduce the driving force for Cl-. Shunting inhibition should therefore not be effective on spines, but it could be significantly more effective on the dendritic shaft at the base of the spine. In contrast to shunting inhibition, hyperpolarizing synaptic inhibition mediated by K+ currents can be very effective in reducing the excitatory synaptic potentials on the same spine if the excitatory conductance change is less than 10 nS. We predict that if the inhibitory synapses found on cortical spines are to be effective, then they should be mediated by K+ through GABAB receptors.

Interactions of TPA and insulin on Na+ transport across frog skin

The phorbol ester 12-O-tetradecanoylphorbol 13-acetate (TPA) activates protein kinase C (PKC) and produces an early stimulation of Na+ transport across frog skin. The ionic basis for this stimulation was studied with combined transepithelial and intracellular electrical measurements. In an initial series of experiments, TPA approximately doubled the amiloride-sensitive short-circuit current (ISC), apical Na+ permeability (PapNa), and apical membrane conductance without affecting the basolateral membrane conductance. The apical effects led to a marked depolarization of the short-circuited skin and a small increase in intracellular Na+ concentration. TPAs increase of PapNa was sufficient to explain the stimulation of basolateral Na+ transport when both the voltage and substrate dependence of the pump were taken into account. After the early stimulation, TPA later depressed ISC. Added at this point (congruent to 1-2 h after TPA administration), insulin had no effect on ISC, whereas a partial response to vasopressin was still observed. Measured either early or late after TPA addition, the phorbol ester reduced insulin binding by congruent to 40%. Insofar as 60% of the specific binding is retained, the abolishment of insulin's natriferic response is unlikely to result from the TPA-induced reduction in hormonal binding. The data provide further support for the concept that activation of PKC produces an early stimulation of Na+ transport by increasing apical Na+ permeability, and that part of insulin's natriferic effect may be mediated by PKC activation.

Voltage dependence of Na/K pump current in Xenopus oocytes

Stage V and VI (Dumont, J.N., 1972, J. Morphol. 136:153-180) oocytes of Xenopus laevis were treated with collagenase to remove follicular cells and were placed in K-free solution for 2 to 4 days to elevate internal [Na]. Na/K pump activity was studied by restoring the eggs to normal 3 mM K Barth's solution and measuring membrane current-voltage (I-V) relationships before and after the addition of 10 microM dihydroouabain (DHO) using a two-microelectrode voltage clamp. Two pulse protocols were used to measure membrane I-V relationships, both allowing membrane currents to be determined twice at each of a series of membrane potentials: (i) a down-up-down sequence of 5 mV, 1-sec stair steps and (ii) a similar sequence of 1-sec voltage pulses but with consecutive pulses separated by 4-sec recovery periods at the holding potential (-40 mV). The resulting membrane I-V relationships determined both before and during exposure to DHO showed significant hysteresis between the first and second current measurements at each voltage. DHO difference curves also usually showed hysteresis indicating that DHO caused a change in a component of current that varied with time. Since, by definition, the steady-state Na/K pump I-V relationship must be free of hysteresis, the presence of hysteresis in DHO difference I-V curves can be used as a criterion for excluding such data from consideration as a valie measure of the Na/K pump I-V relationship. DHO difference I-V relationships that did not show hysteresis were sigmoid functions of membrane potential when measured in normal (90 mM) external Na solution. The Na/K pump current magnitude saturated near 0 mV at a value of 1.0-1.5 microA cm-2, without evidence of negative slope conductance for potentials up to +55 mV. The Na/K pump current magnitude in Na-free external solution was approximately voltage independent. Since these forward-going Na/K pump I-V relationships do not show a region of negative slope over the voltage range -110 to +55 mV, it is not necessary to postulate the existence of more than one voltage-dependent step in the reaction cycle of the forward-going Na/K pump.

Potassium translocation by the Na+/K+ pump is voltage insensitive

The voltage dependence of steady and transient changes in Na+/K+ pump current, in response to step changes in membrane potential, was investigated in guinea pig ventricular myocytes voltage clamped and internally dialyzed under experimental conditions designed to support four separate modes of Na+/K+ pump activity. Voltage jumps elicited transient pump currents when the pump cycle was running forward or backward, or when pumps were limited to Na+ translocation, but not when they were made to carry out K+/K+ exchange. This result indicates that K+ translocation involves no net charge movement across the membrane field and is therefore voltage insensitive. The transient pump currents seen during Na+/K+ transport demonstrate that both forward and reverse pump cycles are rate limited not by the voltage-dependent step but by a voltage-independent step, probably K+ translocation. These findings severely constrain kinetic models of Na+/K+ pump activity.

D2O and the sodium pump in squid nerve membrane

In 10 K artificial seawater (ASW), D2O replacement reduced the Na efflux of squid axons by about one third. In 0 K ASW, D2O replacement had little effect. D2O reduced the K+ sensitivity of the efflux but increased the affinity for K+. A 4 degrees decrease in temperature mimicked the effects of D2O. When axons were injected with arginine, to decrease the ATP/ADP ratio, they lost K+ sensitivity in normal ASW, as expected. Their efflux into 0 K ASW became D2O sensitive. The results are discussed in terms of conformational changes in the Na pump molecular complex.

Fast charge translocations associated with partial reactions of the Na,K-pump: I. Current and voltage transients after photochemical release of ATP

Nonstationary electric currents are described which are generated by the Na,K-pump. Flat membrane sheets 0.2-1 micron in diameter containing a high density of oriented Na,K-ATPase molecules are bound to a planar lipid bilayer acting as a capacitive electrode. In the aqueous phase adjacent to the bound membrane sheets, ATP is released within milliseconds from an inactive, photolabile precursor ("caged" ATP) by an intense flash of light. After the ATP-concentration jump, transient current and voltage signals can be recorded in the external circuit corresponding to a translocation of positive charge across the pump protein from the cytoplasmic to the extracellular side. These electrical signals which can be suppressed by inhibitors of the Na,K-ATPase require the presence of Na+ but not of K+ in the aqueous medium. The intrinsic pump current Ip(t) can be evaluated from the recorded current signal, using estimated values of the circuit parameters of the compound membrane system. Ip(t) exhibits a biphasic behavior with a fast rising period, followed by a slower decline towards a small quasi-stationary current. The time constant of the rising phase of Ip(t) is found to depend on the rate of photochemical ATP release. Further information on the microscopic origin of the current transient can be obtained by double-flash experiments and by chymotrypsin modification of the protein. These and other experiments indicate that the observed charge-translocation is associated with early events in the normal transport cycle. After activation by ATP, the pump goes through the first steps of the cycle and then enters a long-lived state from which return to the initial state is slow.

The effect of membrane potential on the mammalian sodium-potassium pump reconstituted into phospholipid vesicles

1. We have studied effects of electrical diffusion potentials on active Na+-K+ exchange in phospholipid vesicles reconstituted with pig kidney Na+, K+-ATPase. 2. Diffusion potentials, negative inside, were established using outwardly directed K+ gradients plus valinomycin or Li+ gradients plus a Li+ ionophore, AS701. Measurement of fluorescence changes of the carbocyanine dye DiS-C3-(5) showed that the ionophores generated potentials of the expected orientation and of sufficient stability for their effects on active transport to be assessed. Measurement of rates of passive 22Na+ fluxes, over a wide range of diffusion potentials, were consistent with the quantitative predictions of the constant-field flux equation. This result demonstrates that values of diffusion potentials calculated from the Nernst or constant-field equation are accurate. 3. In some conditions, the inside-negative potential (-130 to -180 mV) accelerated the rate of ATP-dependent Na+-K+ exchange on inside-out-oriented pumps, compared to 'control' without the ionophores. Reduction in the size of the diffusion potentials by addition to the medium of Li+ with AS701 or Cs+ with the valinomycin progressively annulled the acceleratory effects, consistent with these being true effects of a change in membrane potentials. 4. At saturating cytoplasmic Na+ and ATP concentrations, the diffusion potential accelerated ATP-dependent Na+-K+ exchange by up to about 30% compared to control but this effect disappeared at rate-limiting ATP concentrations (approximately 1 microM). 5. Using prior knowledge of rate-limiting steps, we interpret this finding to mean that the conformational transition E2(2K)----E12K associated with transport of two K+ ions is voltage insensitive while E1P(3Na)----E2P3Na associated with transport of three Na+ ions is voltage sensitive. The simplest explanation is that the net charge in the transport domain of the protein when no ions, 2K+ or 3Na+ are bound is -2, 0 and +1 respectively. 6. The accelerating effect of the negative-inside diffusion potential on Na+-K+ exchange is greater at limitingly low cytoplasmic Na+ concentrations than at saturating cytoplasmic Na+ concentrations. Cytoplasmic Na+ activation curves show that the diffusion potential increases the apparent cytoplasmic Na+ affinity and reduces the sigmoidicity of cytoplasmic Na+ activation. 7. A kinetic analysis reveals that this effect on apparent affinity is due to an increase in intrinsic Na+ binding and occurs in addition to the effect on a transport rate constant.(ABSTRACT TRUNCATED AT 400 WORDS)

The effects of membrane potential on active and passive sodium transport in Xenopus oocytes

1. The effects of membrane potential on the Na+-K+ pump were studied by measuring membrane current and 22Na+ efflux in voltage-clamped Xenopus oocytes. The effects of inhibiting the Na+-K+ pump with strophanthidin were examined. 2. Strophanthidin produced an inward shift of membrane current which reversed on removal of the drug. In control oocytes the magnitude of this current was not significantly affected by changing membrane potential over the range -20 to -160 mV. 3. In another series of experiments the intracellular Na+ concentration ([Na+]i) was elevated either by overnight Na+-K+ pump inhibition (strophanthidin or exposure to K+-free solutions) or by loading with nystatin. This Na+-loading increased the magnitude of the strophanthidin-sensitive current. The ratio of strophanthidin-sensitive 22Na+ efflux:strophanthidin-sensitive current was consistent with that expected from a 3Na+-2K+ exchange. 4. When [Na+]i was elevated the strophanthidin-sensitive current was sensitive to changes of membrane potential. Hyperpolarization from -20 to -80 mV decreased the current to 60% of control. It is suggested that the current is not sensitive to membrane potential at normal [Na+]i because the over-all reaction is rate limited by the availability of intracellular Na+. 5. The application of strophanthidin decreased the rate of 22Na+ efflux. Both the strophanthidin-insensitive and the strophanthidin-sensitive components of efflux were sensitive to changes of membrane potential. The strophanthidin-insensitive component was not greatly affected by hyperpolarization from -40 to -160 mV but was increased by depolarization to +40 mV. 6. In Na+-loaded oocytes, the strophanthidin-sensitive component of 22Na+ efflux was inhibited by hyperpolarization negative from -40 mV. Hyperpolarization from -40 to -160 mV decreased the efflux by 54 +/- 5%. Over the limited range of potentials for which a comparison could be made, the effects on 22Na+ efflux were somewhat less than on the electrogenic Na+-K+ pump current. On average there was no significant effect of depolarizing from 0 to +40 mV. However, in some experiments a clear inhibition of the efflux was observed. If the oocytes were not Na+ loaded there was no significant effect of membrane potential on the strophanthidin-sensitive Na+ efflux. 7. These results show that the effects of membrane potential on the net reaction of the Na+-K+ pump (as measured by the electrogenic current) result partly from an inhibition of the forward mode of operation. However, there is also evidence to suggest a contribution from stimulation of the reverse reaction.

The role of the sodium pump during prolonged end-plate currents in guinea-pig diaphragm

1. Depolarization caused by carbachol or decamethonium is followed by spontaneous recovery of membrane potential in the presence of the drug. The involvement of the Na pump in this recovery has been investigated in guinea-pig diaphragm at 37 degrees C. 2. Restoration of potassium ions (K+) to the bathing solution gives a rapid recovery of membrane potential which is compatible with a component of recovery of potential being attributable to an electrogenic ion pump and from which a Na pump current of over 60 nA has been estimated. 3. The maintenance of membrane potential in the presence of depolarizing drugs is interpreted in terms of a residual rate of channel opening at a time when the membrane potential is restored, balanced by Na pump action producing tubular depletion of K+. To account for these results a Na pump conductance has been added to a model circuit of drug action. 4. The peak end-plate current produced by carbachol (80 microM) is 100 nA (n = 11) as recorded by the voltage clamp technique; similar estimates may be obtained from measurements of input resistance which falls to 31% of the initial value (n = 5). In muscles desensitized by carbachol for 30 min the end-plate current is 11 nA. 5. In normal muscle removal of K+ from the bathing solution produces a reversible hyperpolarization. In muscles where the membrane potential has recovered in the continued presence of the drug, a hyperpolarization is also found on removal of K+. Withdrawal of K+ during the early stage of spontaneous recovery of potential produces a depolarization or an arrest of the spontaneous repolarization. These results are interpreted in terms of the Na pump producing different effects during the course of spontaneous repolarization. 6. Indirect evidence for K+ depletion in the transverse tubules by the Na pump is provided by an increased resistance to inward current following brief exposure to carbachol or decamethonium. A similar mechanism is used to interpret both the observed change in end-plate revérsal potential to a more negative value and the marked diminution in the amplitude of the action potential at the end-plate during drug action.

The plasma membrane ATPase of Neurospora: a proton-pumping electroenzyme

Probably the best marker enzyme for plasma membranes of eukaryotic cells is a magnesium-dependent, vanadate-inhibited ATPase whose primary function is the transmembrane transport of cations. In animal cells, different species of the enzyme transport different cations: sodium ions released in unequal exchange for potassium ions, calcium ions extruded alone (perhaps), or protons secreted in equal exchange for potassium ions. But in plants and fungi only proton secretion has been clearly demonstrated. A useful model cell for studying the proton-secreting ATPase has been the ascomycete fungus Neurospora, in which the enzyme drives an outward current of protons that can exceed 50 microA/cm2 and can support membrane potentials greater than 300 mV. Both thermodynamic and kinetic studies have shown that the proton-pumping ATPase of Neurospora normally transports only a single proton for each ATP molecule split; and kinetic modelling studies have suggested (contrary to conventional assumptions) that the fast steps in the overall reaction are transmembrane transit of the proton and its dissociation following transport, while the slow steps are the binding of protons and/or ATP. The primary structure of the Neurospora enzyme, recently deduced by gene sequencing, is very close to that of the yeast (Saccharomyces) enzyme, and the hydropathic patterns for both closely resemble those for the animal-cell plasma-membrane ATPases. All of these enzymes appear to have 6-10 membrane-spanning alpha-helices, plus a large cytoplasmic headgroup which bears the catalytic nucleotide-binding site. Structural data, taken together with the electrical-kinetic behavior, suggest that the catalytic headgroup functions as an energized gate for protons. From a geometric point of view, action of such a gate would transfer the membrane field across the "transported" ion, rather than vice versa.

Voltage dependence of the rheogenic Na+/K+ ATPase in the membrane of oocytes of Xenopus laevis

Electrophysiological experiments were performed to analyze the Na+/K+-ATPase in full-grown prophase-arrested oocytes of Xenopus laevis. If the Na+/K+-ATPase is inhibited by dihydroouabain (DHO), the resting potential of the membrane of Na+-loaded oocytes may depolarize by nearly 50 mV. This hyperpolarizing contribution to the resting potential depends on the degree of activation of the Na+/K+-ATPase and varies with intracellular Na+ activity (aiNa) and extracellular K+ (K+o). It is concluded that variations of aiNa among different oocytes are primarily responsible for the variations of resting potentials measured in oocytes of X. laevis. Under voltage-clamp conditions, the DHO-sensitive current also exhibits dependence on aiNa that may be described by a Hill equation with a coefficient of 2. This current will be shown to be identical with the electrogenic current generated by the 3Na+/2K+ pump. The voltage dependence of the pump current was investigated at saturating values of aiNa (33 mmol/liter) and of K+o (3 mmol/liter) in the range from -200 to +100 mV. The current was found to exhibit a characteristic maximum at about +20 mV. This is taken as evidence that in the physiological range at least two steps within the cycle of the pump are voltage dependent and are oppositely affected by the membrane potential.

Cell sodium activity and sodium pump function in frog skin

Cell Na activity, acNa, was measured in the short-circuited frog skin by simultaneous cell punctures from the apical surface with open-tip and Na-selective microelectrodes. Skins were bathed on the serosal surface with NaCl Ringer and, to reduce paracellular conductance, with NaNO3, Ringer on the apical surface. Under control conditions acNa averaged 8 +/- 2 mM (n = 9, SD). Apical addition of amiloride (20 microM) or Na replacement reduced acNa to 3 mM in 6-15 min. Sequential decreases in apical [Na] induced parallel reductions in acNa and cell current, Ic. On restoring Na after several minutes of exposure to apical Na-free solution Ic rose rapidly (approximately less than 30 sec) to a stable value while acNa increased exponentially, with a time constant of 1.8 +/- 0.7 min (n = 8). Analysis of the time course of acNa indicates that the pump Na flux is linearly related to acNa in the range 2-12 mM. These results indicate that acNa plays an important role in relating apical Na entry to basolateral active Na flux.

Voltage dependence of Na/K pump current in isolated heart cells

The Na/K pump usually pumps more Na+ out of the cell than K+ in, and so generates an outward component of membrane current which, in the heart, can be an important modulator of the frequency and shape of the cardiac impulse. Because it is electrogenic, Na/K pump activity ought to be sensitive to membrane potential, and it should decline with hyperpolarization. However, such voltage dependence of outward pump current has yet to be demonstrated, one reason being the technical difficulty of accurately measuring pump current over a sufficiently wide voltage range. The whole-cell patch-clamp technique allows effective control of both intracellular and extracellular solutions as well as membrane voltage. Applying this technique to myocardial cells isolated from guinea pig ventricle, we have measured Na/K pump current between -140 mV and +60 mV, after minimizing passive currents flowing through Ca2+, K+ and Na+ channels. We report here that strongly activated pump current shows marked voltage dependence; it declines steadily from a maximal level near 0 mV, becoming very small at -140 mV. Pump current-voltage relationships will provide essential information for testing models of the Na/K pump mechanism and for predicting pump-mediated changes in the electrical activity of excitable cells.

Na-Ca exchange: stoichiometry and electrogenicity

This review discusses the evidence concerning the stoichiometry of Na-Ca exchange. In particular we consider whether the Na-Ca exchange has been shown to transport more than two Na+ ions per Ca2+ ion and therefore whether it generates an electric current. The first part of this review discusses both direct and indirect evidence concerning the stoichiometry of the exchange and its possible voltage dependence. We find that, although there is some evidence suggesting that more than two Na+ ions may exchange for each Ca2+ ion, most of the available evidence is equivocal and cannot fix the stoichiometry precisely. Furthermore, using a simple and explicit circulating carrier model for the Na-Ca exchange, we show that the effect of membrane potential on the Na-Ca exchange may be considerably more complicated than is generally believed. In particular we find that both electrogenic and electroneutral exchanges will be affected by membrane potential. We therefore conclude that the demonstration of the voltage dependence of the Na-Ca exchange does not necessarily imply that it is electrogenic. Additionally, this analysis shows that, apart from a restricted range near thermodynamic equilibrium, it is impossible to predict either the magnitude or the direction of the effects of membrane potential on the exchange. In the second part of the review we consider whether any known membrane currents may be attributed to Na-Ca exchange. We show, in contrast to previous suggestions, that the Na-Ca exchange can theoretically produce a current that appears to be activated by intracellular Ca and that has a reversal potential. However, the experimental demonstration that a given current is produced by Na-Ca exchange is hampered by the existence of other Ca- and Na-dependent currents. In conclusion, we feel that there is no evidence that allows any particular membrane current to be unambiguously identified with the Na-Ca exchange.

Effects of barium and ion substitutions in artificial blood on endocochlear potential

Previously, a qualitative assessment was made (Marcus, D.C. (1984): Am. J. Physiol. 247, C240-C246) of the ion-selective properties of the cells bounding the cochlear duct by observing the effects of ion substitutions in the perilymph on the transepithelial potential difference (endocochlear potential; EP). Contributions by the marginal cells of the stria vascularis to the observed changes in the EP may have been masked, however, due to their 'isolation' from the perilymph by a continuous layer of basal cells. Since the ionic milieu of the basolateral membranes of the marginal cells is controlled more directly by the blood supply than by the perilymph, we report here on the effects of ion substitutions via vascular perfusion. Elevated K (substituted for Na or N-methyl-D-glucamine; NMDG) or Ba caused marked depression of the EP. Decreased Na or Cl (replaced by NMDG and gluconate, respectively) also depressed the EP. These changes in the EP were distinctly different from those observed previously by perilymphatic perfusion, and were interpreted in terms of a modified model of the strial marginal cells.