Intracellular Na+ and K+ activities and membrane conductances in the collecting tubule of Amphiuma

Membrane potentials and conductances, and intracellular ionic activities were studied in isolated perfused collecting tubules of K+-adapted Amphiuma. Intracellular Na+ (aNai) and K+ (aKi) activities were measured, using liquid ion-exchanger double-barreled microelectrodes. Apical and basolateral membrane conductances were estimated by cable analysis. The effects of inhibition of the apical conductance by amiloride (10(-5) M) and of inhibition of the basolateral Na-K pump by either a low K+ (0.1 mM) bath or by ouabain (10(-4) M) were studied. Under control conditions, aNai was 8.4 +/- 1.9 mM and aKi 56 +/- 3 mM. With luminal amiloride, aNai decreased to 2.2 +/- 0.4 mM and aKi increased to 66 +/- 3 mM. Ouabain produced an increase of aNai to 44 +/- 4 mM, and a decrease of aKi to 22 +/- 6, and similar changes were observed when the tubule was exposed to a low K+ bath solution. During pump inhibition, there was a progressive decrease of the K+-selective basolateral membrane conductance and of the Na+ permeability of the apical membrane. A similar inhibition of both membrane conductances was observed after pump inhibition by low K+ solution. Upon reintroduction of K+, a basolateral membrane hyperpolarization of -23 +/- 4 mV was observed, indicating an immediate reactivation of the electrogenic Na-K pump. However, the recovery of the membrane conductances occurred over a slower time course. These data imply that both membrane conductances are regulated according to the intracellular ionic composition, but that the basolateral K+ conductance is not directly linked to the pump activity.     

Stoichiometry and voltage dependence of the sodium pump in voltage- clamped, internally dialyzed squid giant axon

The stoichiometry and voltage dependence of the Na/K pump were studied in internally dialyzed, voltage-clamped squid giant axons by simultaneously measuring, at various membrane potentials, the changes in Na efflux (delta phi Na) and holding current (delta I) induced by dihydrodigitoxigenin (H2DTG). H2DTG stops the Na/K pump without directly affecting other current pathways: (a) it causes no delta I when the pump lacks Na, K, Mg, or ATP, and (b) ouabain causes no delta I or delta phi Na in the presence of saturating H2DTG. External K (Ko) activates Na efflux with Michaelis-Menten kinetics (Km = 0.45 +/- 0.06 mM [SEM]) in Na-free seawater (SW), but with sigmoid kinetics in approximately 400 mM Na SW (Hill coefficient = 1.53 +/- 0.08, K1/2 = 3.92 +/- 0.29 mM). H2DTG inhibits less strongly (Ki = 6.1 +/- 0.3 microM) in 1 or 10 mM K Na-free SW than in 10 mM K, 390 mM Na SW (1.8 +/- 0.2 microM). Dialysis with 5 mM each ATP, phosphoenolpyruvate, and phosphoarginine reduced Na/Na exchange to at most 2% of the H2DTG-sensitive Na efflux. H2DTG sensitive but nonpump current caused by periaxonal K accumulation upon stopping the pump, was minimized by the K channel blockers 3,4-diaminopyridine (1 mM), tetraethylammonium (approximately 200 mM), and phenylpropyltriethylammonium (20-25 mM) whose adequacy was tested by varying [K]o (0-10 mM) with H2DTG present. Two ancillary clamp circuits suppressed stray current from the axon ends. Current and flux measured from the center pool derive from the same membrane area since, over the voltage range -60 to +20 mV, tetrodotoxin-sensitive current and Na efflux into Na-free SW, under K-free conditions, were equal. The stoichiometry and voltage dependence of pump Na/K exchange were examined at near-saturating [ATP], [K]o and [Na]i in both Na-free and 390 mM Na SW. The H2DTG-sensitive F delta phi Na/delta I ratio (F is Faraday's constant) of paired measurements corrected for membrane area match, was 2.86 +/- 0.09 (n = 8) at 0 mV and 3.05 +/- 0.13 (n = 6) at -60 to -90 mV in Na-free SW, and 2.72 +/- 0.09 (n = 7) at 0 mV and 2.91 +/- 0.21 (n = 4) at -60 mV in 390 mM Na SW. Its overall mean value was 2.87 +/- 0.07 (n = 25), which was not significantly different from the 3.0 expected of a 3 Na/2 K pump.(ABSTRACT TRUNCATED AT 400 WORDS)     

K dependence of the Na-K pump is abnormal in erythrocytes from patients with cystic fibrosis and obligate heterozygotes

The affinity of the Na-K pump for K was significantly (P less than .001) lower in erythrocytes from patients with cystic fibrosis (Km 4.6 +/- 0.35 mM; n = 26) or from heterozygotes (Km 3.9 +/- 0.57 mM; n = 12) than in controls (Km 2.2 +/- 0.10 mM; n = 20). The affinity of the Na-K pump for K was lower in normal erythrocytes than in normal fibroblasts which may explain the variability in the severity of involvement of different organs in cystic fibrosis. We have now shown in human skin fibroblasts and erythrocytes, that the K affinity of the Na-K pump is lower in patients with cystic fibrosis than in controls. Since the abnormality is also present in erythrocytes from heterozygotes who are clinically normal, it is likely that this abnormality is closely related to the genetic defect in cystic fibrosis.     

Rheogenic transport in the renal proximal tubule

The electrophysiology of the renal Na-K ATPase was studied in isolated perfused amphibian proximal tubules during alterations in bath (serosal) potassium. Intracellular and extracellular ionic activity measurements permitted continuous evaluation of the Nernst potentials for Na+, K+, and Cl- across the basolateral membrane. The cell membrane and transepithelial potential differences and resistances were also determined. Return of K to the basal (serosal) solution after a 20-min incubation in K-free solution hyperpolarized the basolateral membrane to an electrical potential that was more negative than the Nernst potential for either Na, Cl, or K. This constitutes strong evidence that at least under stimulated conditions the Na-K ATPase located at the basolateral membrane of the renal proximal tubule mediates a rheogenic process which directly transfers net charge across the cell membrane. Interpretation of these data in terms of an electrical equivalent circuit permitted calculation of both the rheogenic current and the Na/K coupling ratio of the basolateral pump. During the period between 1 and 3 min after pump reactivation by return of bath K, the basolateral rheogenic current was directly proportional to the intracellular Na activity, and the pump stoichiometry transiently exceeded the coupling ratio of 3Na to 2K reported in other preparations.     

Stimulation of vascular Na-K pump with subpressor angiotensin II in rats.

The effect of subpressor doses of angiotensin II (ANG II) on vascular Na-K pump activity and Na-H exchange, two transmembrane signals of trophic stimulation of vascular muscle, was investigated. Male Sprague-Dawley rats (350-400 g) were given subpressor doses of ANG II by osmotic minipump intraperitoneally for 24 hr or 7-10 days. Control rats received sham procedure/vehicle infusion. Na-K pump activity (86Rb uptake), total and intracellular (Li exchange at 4 degrees C) Na content, and amiloride-sensitive and -insensitive Na uptake of aortas were measured ex vivo. Ouabain-sensitive 86Rb uptake of aortas of rats receiving 80-100, 160-180, and 240-260 ng/kg.min-1 of ANG II for 24 hr was 26.6 +/- 3.5, 28.8 +/- 3.4, and 29.1 +/- 2.6 nmol/mg dry wt.15 min-1 (mean +/- SD, n = 7-12), respectively, compared with 25.2 +/- 3.8 in controls (n = 23, P less than 0.01). These increases were maintained at 7-10 days. After 24 hr and 7-10 days of ANG II treatment, the total Na content of aortas was increased by 9.2% (P less than 0.01) and 7.6% (P less than 0.02), respectively, without a change in intracellular Na content, indicating accumulation of excess extracellular Na. Total and amiloride-sensitive Na uptake of the aorta was unchanged after 24 hr or 7-10 days of ANG II administration. The dry weight of anatomically defined segments of the aorta was 40 +/- 3.8 mg/kg body wt (n = 25) after 24 hr and 42 +/- 4.4 (n = 20) after 7-10 days of ANG II administration, compared with 37 +/- 4.8 (n = 15, P less than 0.05) and 37 +/- 4.9 (n = 17, P less than 0.01) in appropriate controls. Increased Na-K pump activity may signal the onset of trophic stimulation of vascular muscle by ANG II.     

Effects of L-alanine on membrane potential, potassium (86Rb) permeability and cell volume in hepatocytes from Raja erinacea

Isolated hepatocytes from the elasmobranch Raja erinacea were examined for their regulatory responses to a solute load following electrogenic uptake of L-alanine. The transmembrane potential (Vm) was measured with glass microelectrodes filled with 0.5 M KCl (75 to 208 M omega in elasmobranch Ringer's solution) and averaged -61 +/- 16 mV (S.D.; n = 68). L-Alanine decreased (depolarized) Vm by 7 +/- 3 and 18 +/- 2 mV at concentrations of 1 and 10 mM, respectively. Vm did not repolarize to control values during the 5-10 min impalements, unless the amino acid was washed away from the hepatocytes. The depolarizing effect of L-alanine was dependent on external Na+, and was specific for the L-isomer of alanine, as D- and beta-alanine had no effect. Hepatocyte Vm also depolarized on addition of KCN or ouabain, or when external K+ was increased. Rates of 86Rb+ uptake and efflux were measured to assess the effects of L-alanine on Na+/K+-ATPase activity and K+ permeability, respectively. Greater than 80% of the 86Rb+ uptake was inhibited by 2 mM ouabain, or by substitution of choline+ for Na+ in the incubation media. L-Alanine (10 mM) increased 86Rb+ uptake by 18-49%, consistent with an increase in Na+/K+ pump activity, but had no effect on rubidium efflux. L-Alanine, at concentrations up to 20 mM, also had no measurable effect on cell volume as determined by 3H2O and [14C]inulin distribution. These results indicate that Na+-coupled uptake of L-alanine by skate hepatocytes is rheogenic, as previously observed in other cell systems. However, in contrast to mammalian hepatocytes, Vm does not repolarize for at least 10 min after the administration of L-alanine, and changes in cell volume and potassium permeability are also not observed.     

A model study of the contribution of active Na-K transport to membrane repolarization in cardiac cells

A biochemical model of active Na-K transport in cardiac cells was studied in conjunction with a representation of the passive membrane currents and ion concentration changes. The active transport model is based on the thermodynamic and kinetic properties of a six-step reaction scheme for the Na,K-ATPase. It has a fixed Na:K stoechiometry of 3:2, and its activation is governed by three parameters: membrane potential intracellular Na+ concentration, and interstitial K+ concentration. The Na-K pump current is directly proportional to the density of Na,K-ATPase molecules. The passive membrane currents and ion concentration changes involve only Na+ and K+ ions, and no attempt was made to provide a precise representation of Ca2+ currents or Ca2+ concentration changes. The surface-to-volume ratio of the interstitial compartment is 55 times larger than that of the intracellular compartment. The flux balance conditions are such that the original equilibrium concentration values are re-established at each stimulation cycle. The underlying assumptions of the model were checked against experimental measurements on Na-K pump activity in a variety of preparations. In addition, the qualitative validation of the model was carried out by comparing its behavior following sudden frequency shifts to corresponding experimental observations. The overall behavior of the model is quite satisfactory and it is used to provide the following indications: (1) when the intracellular and interstitial volumes are relatively large, the ion concentration transients are small and the pumping rate depends essentially on average concentration levels. (2) An increase in internal Na+ concentration potentiates the response of the Na-K pump to rapid membrane depolarizations. (3) When the internal Na+ concentration is large enough, the Na-K pump current transient plays an important role in shaping the plateau and repolarization phase of the action potential. (4) A rapid increase in external K+ concentration during voltage clamp in multicellular preparations could saturate the Na-K pump response and lead to a fairly linear dependence of the pump activity on the internal Na+ concentration.     

Models of the Na-K pump in cardiac muscle predict the wrong intracellular Na+ activity

The Na-K pump in cardiac Purkinje strands has been carefully studied with voltage clamp and Na+-selective microelectrodes. In three of these studies both the rate of change of intracellular Na+ activity, a(Nai), after pump blockade, and the time constant of reduction of a(Nai) after an Na+ load were measured. These two parameters can be employed with a formalism relating pump activity to a(Nai) in order to predict the a(Nai) in the steady state. Several formalisms were tested: (a) a first-order dependence on a(Nai); (b) a model based on the assumption of a single, saturable, Na+-binding site that must be occupied for transport to occur; (c) a model based on n equivalent, saturable, Na+ binding sites per pump molecule all of which must be occupied for transport to occur. The first two models predicted an a(Nai) that is far below the value of about 6 mM that is experimentally obtained. The third model would work for n greater than or equal to 4. These results suggest that either the cardiac Na-K pump is not well described by available Na-K pump models for n less than 4 or that the measured Na+ influx rate, extrusion rate or a(Nai) are in error.     

An upper limit for the electrogenic Na-K pump contribution to maximum diastolic potential in feline cardiac Purkinje fibers in steady state

We have estimated an upper limit for the electrogenic contribution of the Na-K pump to diastolic transmembrane potential. We simultaneously monitored the maximum diastolic potential and the extracellular space potassium activity during exposure to a very high concentration of ouabain. Exposure to ouabain caused a depolarization of approximately 3 mV (n = 33 experiments) over 34 +/- 3 s (mean +/- standard error) prior to any change in extracellular K activity. In four experiments, we monitored intracellular sodium activity and observed it to rise with approximately the same temporal lag (delay = 26 +/- 7 s). We also measured relative membrane conductance in one series of experiments and observed it to decrease to 91 +/- 2% of its control value by the time extracellular space K began to rise. Following the initial increase in extracellular space K activity the subsequent membrane depolarization is shown to be accurately predicted solely from the measured increase in extracellular space K activity as calculated from the Goldman equation. Limitations of the method and possible interpretations of the data are discussed. We interpret this ouabain-induced depolarization that occurs prior to the rise in external K to be an upper limit to the Na-K pump's electrogenic contribution to steady-state membrane potential.     

The measurement of intracellular sodium activities in the bullfrog by means of double-barreled sodium liquid ion-exchanger microelectrodes.

A double-barreled Na+-selective microelectrode was constructed with monensin as a liquid ion exchanger. The HCl-treated monensin was dissolved in a solvent (Corning 477317) at 10% (weight/weight). Internal reference solution of its ionic barrel was mixture of 0.49 M NaCl and 0.01 M KCl, the pH being adjusted to 3 with 0.1 M citrate-HCl buffer, whereas that of the PD barrel was 0.5 M KCl. Average slope and selectivity ratio (Na+/K+) tested on 10 different microelectrodes were -57.5 +/- 1.87 mV/P(Na) (SEM) and 6.7 +/- 0.44, respectively. The electrical resistance was an order of 10(10) ohm and the response time was less than 10 sec. Using this microelectrode, a free flow micropuncture experiment was carried out in the bullfrog kidney and the intracellular Na+ activity as well as the membrane PD was determined on the proximal tubular cell. Average value (+/- SEM, n = 15) for the intracellular Na+ and K+ was 20.7 +/- 1.56 mEq/L and 61.2 +/- 1.16 mEq/L, respectively, and -68.7 +/- 0.88 mV for the peritubular membrane PD. There was a significant negative correlation between Na+ and K+ activities within the cell, i.e., the lower the ionic activity of cellular Na+ was, the higher the cellular K+, and vice versa, the sum of these two being kept nearly constant. The above finding may be somehow related to the isosmosis in the reabsorptive process across the proximal tubular epithelium.     

Evidence for a modulatory effect of external potassium ions on ionic current mediated by the cardiac Na+-Ca2+ exchanger

The aim of this study was to investigate whether or not the activity of the cardiac Na(+)-Ca(2+) exchanger might be directly sensitive to external K(+) concentration ([K(+)](e)). Measurements of whole-cell exchanger current (I(NaCa)) were made at 37 degrees C from guinea-pig isolated ventricular myocytes, using whole-cell patch clamp recording with major interfering conductances blocked. Changing [K(+)](e) from 0 to 5mM significantly reduced both outward and inward exchange currents in a time-dependent manner. Various [K(+)](e) between 1 and 15 mM were tested and the inhibitory effect was observed to be concentration-dependent. At steady-state, 5mM [K(+)](e) decreased the density of Ni(2+)-sensitive current by 52.8+/-4.3% (mean+/-S.E.M., n=6) and of 0Na0Ca-sensitive current by 39.0+/-4.4% (n=5). The possibility that the inhibitory effect of external K(+) on I(NaCa) might wholly or in part be secondary to activation of the sarcolemmal Na(+)-K(+) pump was investigated by testing the effect of K(+) addition in the presence of a high concentration of strophanthidin (500 microM). Ni(2+)-sensitive I(NaCa) was still observed to be sensitive to external K(+) (I(NaCa) decreased by 39.4+/-9.4%, n=4), suggesting that the inhibitory effect could occur independently of activation of the Na(+)-K(+) pump. The effect of external K(+) on I(NaCa) was verified using a baby hamster kidney (BHK) cell line stably expressing the cardiac Na(+)-Ca(2+) exchanger isoform, NCX1. Similar to native I(NaCa), NCX1 current was also suppressed by [K(+)](e). However, [K(+)](e) did not alter current amplitude in untransfected BHK cells. The effect of [K(+)](e) on I(NaCa) could not be attributed to simply adding any monovalent cation back to the external solution, since it was not reproduced by application of equimolar Li(+), Cs(+) and TEA(+). Rb(+), however, could mimic the effect of K(+). Collectively, these data suggest that external K(+) at physiologically and pathologically relevant concentrations might be able to modulate directly the activity of the cardiac Na(+)-Ca(2+) exchanger.     

Negative potential level in the outer layer of the toad skin.

The isolated skin of the toad Bufo marinus ictericus when impaled from the outer surface by glass microelectrodes filled with 3 M KCl shows a voltage profile which is a continuous function of the depth of impalement. The superficial intraepithelial potential difference measured with reference to the external solution (PDi) is negative with NaCl-Ringer's solution on both sides of the skin, displaying a minimum of -26.7+/-3.6 mV at 6+/-2 mum. Null value is obtained at 19+/-3 mum, with positive values for deeper impalements. Indications of cell impalements (abrupt voltage and resistance jumps) were frequently observed at sites deeper than 25 mum from the outer surface. Measurements of the electrical resistance between the microelectrode and the external solution, made with single- and double-barreled microelectrodes, showed great discrepancies, which may be attributed to distinct pathways of different resistances in the stratum corneum. PDi measured at a depth of 5 mum was a logarithmic function of Na2SO4 or K2SO4 concentration in the external solution, increasing in negativity with a reduction in concentration. Substitution of Na by K in the external solution had only minor effects on PDi. Acidification of the external solution from pH 9 is accompanied by a reduction in the negative value of PDi. At pH 3 PDi was positive. PDi was interpreted as a diffusion potential at the tip of the microelectrode due to KCl diffusion from the electrode into the matrix of the stratum corneum. Differences in K and Cl mobilities, responsible for the origin of PDi, were attributed to fixed charges in the matrix of the stratum corneum, with density and polarity determined by their degree of proponation, controlled by the hydrogen ion concentration of the external solution. Skin potential, short-circuit current and their relationship to PDI were discussed.     

Measurement of Na-K pump current in acinar cells of rat lacrimal glands.

Isolated cells from rat lacrimal glands were voltage clamped using the tight-seal whole-cell recording technique. The intracellular solution contained ATP and an elevated Na concentration (70 mM). Removing external K ions elicited an inward current shift. Ouabain (0.5 mM) induced an inward current shift of identical amplitude, but with slower kinetics. In the presence of ouabain, removal of K ions did not alter the cell current. The potassium- and ouabain-sensitive current was outward between -120 and +20 mV, and its amplitude decreased below -60 mV. This current was highly sensitive to temperature, and was not affected by blockers of the K channels which are present in these cells. It was attributed to an inhibition of the Na-K pump. The Na-K pump current was estimated to be 15 pA for an average acinar cell at physiological temperature, with 70 mM internal Na ions and 20 mM external K ions. Implications of this value in terms of electrolyte secretion are discussed.     

Intracellular activities of chloride, potassium and sodium ions in rabbit corneal epithelium

The mechanism of ion transport in the epithelium of rabbit cornea was studied by determining the intracellular ion activity of Cl-, Na+ and K+ under various conditions. Ionic activities were measured by means of microelectrodes containing liquid ion-exchangers selective for Cl-, Na+ or K+. The Cl- activity in basal cells of the epithelium in Na+ containing bathing solutions amounts to 28 +/- 2 mM (n = 11). This value is 1.9-times greater than expected on the basis of passive distribution across the tear side membrane. This finding suggests the existence of a Cl- accumulating process. Replacement of Na+ in the aqueous bathing solution by choline or tetraethylammonium results in a reversible decrease in Cl- activity to 22 +/- 1 mM (n = 11, P less than 0.025). The ratio of observed and predicted Cl- activity decreased significantly from 1.9 to 1.4 (P less than 0.05). The decrease in Cl- activity due to Na+ replacement was rather slow. In contrast, after readmittance of Na+ to the aqueous bathing solution, Cl- activity rose to a stable level within 30 min. These results indicate involvement of Na+ in Cl- accumulation into the basal cells of the epithelium. The K+ and Na+ activities of the basal cells of rabbit corneal epithelium in control bathing solutions were 75 +/- 4 mM (n = 13) and 24 +/- 3 mM (n = 12), respectively. The results can be summarized in the following model for Cl- transport across corneal epithelium. Cl- is accumulated in the basal cells across the aqueous side membrane, energized by a favourable Na+ gradient. Cl- will subsequently leak out across the tear side membranes. Na+ is extruded again across the aqueous side membrane of the epithelium by the (Na+ + K+)-ATPase.     

Transmembrane Na+ and Ca2+ electrochemical gradients in cardiac muscle and their relationship to force development

Na+- and CA2+-sensitive microelectrodes were used to measure intracellular Na+ and Ca2+ activities (alpha iCa) of sheep ventricular muscle and Purkinje strands to study the interrelationship between Na+ and Ca2+ electrochemical gradients (delta muNa and delta muCa) under various conditions. In ventricular muscle, alpha iNa was 6.4 +/- 1.2 mM and alpha iCa was 87 +/- 20 nM ([Ca/+] = 272 nM). A graded decrease of external Na+ activity (alpha oNa) resulted in decrease of alpha iNa, and increase of alpha iCa. There was increase of twitch tension in low- alpha oNa solutions, and occasional increase of resting tension in 40% alpha oNa. Increase of external Ca2+ (alpha oCa) resulted in increase of alpha iCa and decrease of alpha iNa. Decrease of alpha oCa resulted in decrease of alpha iCa and increase of alpha iNa. The apparent resting Na-Ca energy ratio (delta muCa/delta muNa) was between 2.43 and 2.63. When the membrane potential (Vm) was depolarized by 50 mM K+ in ventricular muscle, Vm depolarized by 50 mV, alpha iNa decreased, and alpha iCa increased, with the development of a contracture. The apparent energy coupling ratio did not change with depolarization. 5 x 10(-6) M ouabain induced a large increase in alpha iNa ad alpha iCa, accompanied by an increase in twitch and resting tension. Under the conditions we have studied, delta muNa and delta muCa appeared to be coupled and n was nearly constant at 2.5, as would be expected if the Na-Ca exchange system was able to set the steady level of alpha iCa. Tension threshold was about 230 nM alpha iCa. The magnitude of twitch tension was directly related to alpha iCa.     

Electrogenic Na?K pump current in rat skeletal myoballs

Catecholamines and insulin have been reported to hyperpolarize skeletal muscle fibers via stimulation of the electrogenic Na-K pump (Flatman and Clausen, 1979, Nature, 281:580–581). Therefore, the electrogenic Na-K pump current was investigated in cultured colcemid-treated rat skeletal myoballs using whole-cell voltage clamp. Skeletal muscles were taken from newborn rat hindlegs, trypsin digested, and cultured. By day 7, all myoblast cells fused into myotubes. After treatment with the microtubule disrupter colcemid (10^?7 M) for 2 days, some of the myotubes became transformed into spherical myoballs, having an average diameter of 41.2 ± 1.5 μm (n = 21). The resting membrane potential averaged -56.8 ± 1.7 mV (n = 40). Ouabain (1 mM) quickly depolarized the myoballs to -51.1 ± 1.1 mV (n = 27), showing the existence of an electrogenic Na-K pump in the skeletal myoball preparation. The values for the specific membrane resistance and capacitance were 5.5 ± 1.0 KΩ-cm² (n = 21) and 3.7 ± 0.3 μF/cm² (n = 21), respectively. The pump current averaged 0.28 ± 0.03 pA/pF (n = 10), with the membrane potential at -60 mV and 10 mM intrapipette Na⁺. The Na-K pump contribution to resting membrane potential was calculated to be 5.7 mV, matching the ouabain-induced rapid depolarization. When the Na-K pump was stimulated with 50 mM intrapipette Na⁺, the pump current was about doubled (0.52 ± 0.08 pA/pF; n = 10). Isoproterenol (1 μM) and 8-Br-cAMP (1 mM) also significantly increased pump current by 50% (0.42 ± 0.04 pA/pF; n = 9) and 64% (0.46 ± 0.09 pA/pF; n = 7), respectively. In contrast, although insulin and phorbol ester also increased pump current, this increase was not statistically significant. The ineffectiveness of insulin and phorbol ester may be due to colcemid interfering with Na-K pump translocation from internal vesicles to the sarcolemma. © 1994 wiley-Liss, Inc.     

Na,K pump stimulation by intracellular Na in isolated, intact sheep cardiac Purkinje fibers

Regulation of the Na,K pump in intact cells is strongly associated with the level of intracellular Na+. Experiments were carried out on intact, isolated sheep Purkinje strands at 37 degrees C. Membrane potential (Vm) was measured by an open-tipped glass electrode and intracellular Na+ activity (aNai) was calculated from the voltage difference between an Na+-selective microelectrode (ETH 227) and Vm. In some experiments, intracellular potassium (aiK) or chloride (aCli) was measured by a third separate microelectrode. Strands were loaded by Na,K pump inhibition produced by K+ removal and by increasing Na+ leak by removing Mg++ and lowering free Ca++ to 10(-8) M. Equilibrium with outside levels of Na+ was reached within 30-60 min. During sequential addition of 6 mM Mg++ and reduction of Na+ to 2.4 mM, the cells maintained a stable aNai ranging between 25 and 90 mM and Vm was -30.8 +/- 2.2 mV. The Na,K pump was reactivated with 30 mM Rb+ or K+. Vm increased over 50-60 s to -77.4 +/- 5.9 mV with Rb+ activation and to -66.0 +/- 7.7 mV with K+ activation. aiNa decreased in both cases to 0.5 +/- 0.2 mM in 5-15 min. The maximum rate of aiNa decline (maximum delta aNai/delta t) was the same with K+ and Rb+ at concentrations greater than 20 mM. The response was abolished by 10(-5) M acetylstrophantidin. Maximum delta aNai/delta t was independent of outside Na+, while aKi was negatively correlated with aNai (aKi = 88.4 - 0.86.aNai). aCli decreased by at most 3 mM during reactivation, which indicates that volume changes did not seriously affect aNai. This model provided a functional isolation of the Na,K pump, so that the relation between the pump rate (delta aNai/delta t) and aiNa could be examined. A Hill plot allowed calculation of Vmax ranging from 5.5 to 27 mM/min, which on average is equal to 25 pmol.cm-2.s-1.K 0.5 was 10.5 +/- 0.6 mM (the aNai that gives delta aNai/delta t = Vmax/2) and n equaled 1.94 +/- 0.13 (the Hill coefficient). These values were not different with K+ or Rb+ as an external activator. The number of ouabain-binding sites equaled 400 pmol.g-1, giving a maximum Na+ turnover of 300 s-1. The Na,K pump in intact Purkinje strands exhibited typical sigmoidal saturation kinetics with regard to aNai as described by the equation upsilon/Vmax = aNai(1.94)/(95.2 + aNai(1.94)). The maximum sensitivity of the Na,K pump to aiNa occurred at approximately 6 mM.     

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

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

Characteristics of an inhibitor of the Na+/K+ pump in human cerebrospinal fluid

Human cerebrospinal fluid (CSF) inhibits the Na+/K+ pump in human red cells and the activity of purified Na+/K+-ATPase (Halperin, J. A., Shaeffer, R., Galvez, L., and Malavé, S. (1985) Proc. Natl. Acad. Sci. U.S. A. 80, 6102-6104, 1983; Halperin, J. A., Martin, A. M., and Malavé, S. (1985) Life Sci. 37, 561-566. We describe here some properties of the CSF inhibitor of the Na+/K+ pump. Active material was extracted from human CSF with 50% methanol and then concentrated and desalted by ultrafiltration. This extract inhibited, in a dose-dependent manner, the ouabain-sensitive influx of K+ into human red cells and the activity of purified Na+/K+-ATPase. Partial separation of the inhibitory activity was achieved by gel filtration and reverse-phase high performance liquid chromatography. Inhibition of both pump and enzyme was specific in that other red cell membrane transport systems or enzymes examined were not influenced by CSF extracts. Dialysis and ultrafiltration experiments indicate that the molecular weight of the inhibitor is approximately equal to 600. The inhibitory activity is sensitive to proteolytic enzymes indicating that the inhibitor might be a small peptide. In the presence of CSF extract the K0.5 for external K+ to stimulate the Na+/K+ pump increased from 1.4 to 3.1 mM, suggesting that the CSF inhibitor competes with external K+ for stimulation of the pump. We estimate that the concentration of the inhibitor in CSF might be approximately equal to 50 pg/ml, a value close to the concentration of other active peptides found in human CSF.     

Saturation of the internal sodium site of the sodium pump can distort estimates of potassium affinity.

The Na+/K+ exchange pump in cardiac Purkinje strands has been well studied with the voltage clamp and Na+-selective microelectrodes. Models describing the observed results suggest that the pump rate can be considered proportional to [Na+]i over the range examined and depends on external [K+] in accordance with Michaelis-Menten kinetics. Estimates of the external [K+] that achieves a half-maximal pump rate (Km) range from 0.9 to 6.3 mM depending on the preparation and method of estimation. Here we show that much of the variability in the estimates of the Km can be eliminated when saturation of the internal Na+ pump site is taken into account. If the half-activation concentration for saturation of this Na+ site is sufficiently high (greater than 20 mM), removal of intracellular Na+ in response to a Na+ load will approximate first-order kinetics. Under these conditions however, Na+ saturation will nevertheless cause large systematic errors in estimates of the K+ dependence of pump activity.