Regulatory volume increase in Ehrlich ascites tumor cells is mediated by the 1Na ∶ 1K ∶ 2Cl cotransport system

Summary After swelling in hyposmotic solution, Ehrlich ascites tumor cells shrink towards their original volume. Upon restoration of isosmolality (300 mOsm) the cells initially shrink but subsequently recover volume. This regulatory volume increase (RVI) is completely blocked when [Na⁺] _o or [Cl^–] _o is reduced by 50% in the presence of normal [K⁺] _o . With normal [NaCl] _o but less than 2 mm [K⁺] _o , not only is volume recovery blocked but the cells lose KCl and shrink. When [K⁺] _o is increased to 5 mm there is a rapid net uptake of K⁺ and Cl^– which results in volume recovery. This suggests that the reswelling phase requires the simultaneous presence of Na⁺, K⁺, and Cl^–. Although ouabain has no effect on volume recovery, bumetanide completely blocks RVI by inhibiting a cotransport pathway that mediates the net uptake of Na⁺, K⁺ and Cl^– in the ratio of 1Na1K2Cl. Na⁺ that accumulates is then replaced by K⁺ via the Na/K pump.I wish to thank my colleague, Dr. Thomas C. Smith for advice and helpful comments during the course of these studies. The excellent technical assistance provided by Rebecca Corcoran-Merrill is gratefully acknowledged.This investigation was supported by Grant CA 32927 from the National Cancer Institute, U.S. Public Health Service.     

Influence of Some Ions on the Membrane Potential of Ascaris Muscle

The influence of several ions on the membrane potential of the somatic muscle of Ascaris has been investigated by changing their concentration in the surrounding solution. When [K]_o is increased at the expense of [Na]_o leaving [Cl]_o constant, the membrane potential is first seen to increase. [K]_o higher than 45 mM reduces the membrane potential with a slope of 23 mv for a tenfold change in [K]_o. However, when [K]_o is increased keeping [Na]_o and [Cl]_o low and constant, the line relating the membrane potential with log [K]_o has a slope of almost 50 mv. If [Cl]_o is reduced in the absence of external Na, after the [K]_o is increased to 45 mM, the membrane potential decreases with a slope of 59 mv per tenfold change in [Cl]_o in close agreement with the Nernst equation. If Cl^- is replaced by SO₄ ^2-, a depolarization is produced, while chloride replacement by NO₃ ^-, Br^-, and I^- results in a hyperpolarization of the membrane. Removal of the external Na⁺ ions increases the average membrane potential by 17 mv.     

Single-channel analysis of a potassium inward rectifier in myocytes of newborn rat heart

Summary Unitary K⁺ currents in single cells isolated from ventricular muscle of newborn rat hearts were measured in response to different potentials and [K] _o . TheI/V curves were linear for potentials more negative than the zero-current voltage: especially in high [K] _o (150nm KCl), no clear outward currents could be detected indicating a drastic rectification in the inward direction. The channel is mainly selective to K⁺ but Na⁺ ions are also carried (P _Na/P _K=0.056). The channel conductance is proportional to the square root of [K] _o but Na⁺ ions seem to have a facilitatory effect on _K, the single-channel conductance. The channel activity, measured asP _o, i.e. the probability to find the channel in open state, decreased as the membrane was hyperpolarized. This behavior was tentatively explained by an inactivation process as the membrane becomes more negative. The rate constants of the transitions between the different states were calculated according to a C–O–C model. A control of the gating process by permeant ion K⁺ was postulated, based on the increase of one of the rate constants from the closed to the open state with [K] _o . Finally, the macroscopicI/V curves calculated fromP _o and i, the unit current, were found to be characteristic of a ion-blocked inward rectifier.     

Kinetic comparison of ouabain-resistant K:CI fluxes (K:Cl [Co]-transport) stimulated in sheep erythrocytes by membrane thiol oxidation and alkylation

Summary The stimulatory effects of two thiol (SH) group oxidants, methylmethane thiosulfonate (MMTS) and diazene dicarboxylic acid bis [N,N-dimethylamide] (diamide), on the kinetics of ouabain-resistant (OR) K:Cl [co]-transport in low K (LK) sheep red blood cells were compared with the effects of alkylating agents, notably N-ethylmaleimide (NEM). At low concentrations, both MMTS and diamide stimulated K:CI [co]-transportv and with a latency period, as measured by OR zero-trans K efflux and OR uptake of external Rb, Rb_o, as K congener in Cl and NO₃ media. At high concentrations the effect of diamide saturated, and that of MMTS disappeared. The stimulatory effect of MMTS was partially reversed by the reducing agent dithiothreitol (DTT) known to fully restore the diamide-activated K flux (Lauf, J. Memb. Biol. 101:179–188, 1988). In diamide pre-equilibrated LK sheep red cells, the K_m of K:Cl [co]-transport for external Cl, Cl_o, was 84.3 mM, and 18.7 mM for Rb_o, with nearly identical V_max values around 4 mmol Rb/L cells × h for K (Rb) fluxes in Cl and after correction for the small Cl-independent component. Zero net K (Rb) flux existed at K_c (cell K)/Rb_o concentration ratios, [K]_c/[Rb]_c, of 0.8 i.e. when the electrochemical driving forces across the membrane were about equal. The measured K efflux/Rb influx ratios were almost twice those predicted from [K]_c/[Rb]_o and the Cl equilibrium potential suggesting that the diamide-stimulated K (Rb) flux may occur through non-diffusional, carrier-mediated transport. The effects of NEM and of A23187 plus/minus Ca or chelators on K: [co]Cl-transport (Lauf, Am. J. Physiol. 249:C271–278, 1985) consisted primarily of V_max changes. Thus, all chemical interventions resulted in an increase of the number of actively transporting K:Cl [co]-transport units or an augmented turnover number per existing site.     

Stimulation by high external potassium of the sodium efflux in barnacle muscle fibers

Summary Single barnacle muscle fibers fromBalanus nubilus were used to study the effect of elevated external potassium concentration, [K] _o , on Na efflux, membrane potential, and cyclic nucleotide levels. Elevation of [K] _o causes a prompt, transient stimulation of the ouabain-insensitive Na efflux. The minimal effective concentrations is 20mm. The membrane potential of ouabain-treated fibers bathed in 10mm Ca²⁺ artificial seawater (ASW) or in Ca²⁺-free ASW decreases approximately linearly with increasing logarithm of [K] _o . The slope of the plot is slightly steeper for fibers bathed in Ca²⁺-free ASW. The magnitude of the stimulatory response of the ouabain-insensitive Na efflux to 100mmK _o depends on the external Na⁺ and Ca²⁺ concentrations, as well as on external pH, but is independent of external Mg²⁺ concentration. External application of 10^–4 m verapamil virtually abolishes the response of the Na efflux to subsequent K-depolarization. Stabilization of myoplasmic-free Ca²⁺ by injection of 250mm EGTA before exposure of the fiber to 100mm K _o leads to 60% reduction in the magnitude of the stimulation. Pre-injection of a pure inhibitor of cyclic AMP-dependent protein kinase reduces the response of the Na efflux to 100mm K _o by 50%. Increasing intracellular ATP, by injection of 0.5m ATP-Na₂ before elevation of [K] _o , fails to prolong the duration of the stimulation of the Na efflux. Exposure of ouabain-treated, cannulated fibers to 100mm K _o for time periods ranging from 30 sec to 10 min causes a small (60%), but significant, increase in the intracellular content of cyclic AMP with little change in the cyclic GMP level. These results are compatible with the view that the stimulatory response of the ouabain-insensitive Na efflux to high K _o is largely due to a fall in myoplasmicpCa resulting from activation of voltage-dependent Ca²⁺ channels and that an accompanying rise in internal cAMP accounts for a portion of this response.     

The steady-state relationship between sodium and chloride transmembrane electrochemical potential differences inNecturus gallbladder

Summary Intracellular C1, K and Na activities (a _Cl ⁱ ,a _k ⁱ anda _Na ⁱ ) and transmucosal membrane potential (E _m) in epithelial cells ofNecturus gallbladder were measured at different external Na concentrations ([Na]_o), with liquid ion-exchanger and conventional microelectrodes. Bladders were mounted in a divided chamber at 23°C between identical HCO₃-free Ringer solutions containing 5mm K. The pH was 7.2. Tris was substituted for Na. Measurements were made under steady-state conditions as determined by the constancy of the transepithelial potential difference. Both,a _Cl ⁱ anda _Na ⁱ increased in a saturable fashion with [Na]_o.E _m did not change significantly. Average values (±sem) under normal conditions ([Na]_o=100mm) fora _Cl ⁱ ,a _Na ⁱ andE _m were 16.8±0.8mm (n=9), 9.7±0.6mm (n=10) and –52.6±0.6 mV (n=26), respectively. In Na-free mediaa _Cl ⁱ declined to its equilibrium value.a _K ⁱ (96±2mm;n=7) did not change when [Na]_o was varied between 100 and 10mm but decreased to 80±3mm (n=4) in Na-free media.Transmembrane electrochemical potential differences, , for Cl and Na were calculated at four different [Na]_o levels. A highly significant linear relation between and was found, indicating that Cl and Na transport are energetically linked. The results support the view that the energy necessary for intracellular Cl accumulation is derived from the simultaneous dissipation of the chemical potential gradient of Na across the apical membrane and that the coupled entry mechanism is electroneutral.     

Membrane permeability changes in amphibian eggs at ovulation

Electropotential differences between the cytoplasm and external medium have been compared in the mature R. pipiens occyte and the ovulated unfertilized egg as a function of [Na]_o, [K]_o, [Ca]_o and [Cl]_o. In solutions containing 1.0 mM Ca⁺⁺ the oocyte behaved as though it were predominantly permeable to K⁺ and Cl^?, i.e., like a KCl electrode. However, the steady potential decreased with decreasing [Ca]_o and in 5 × 10^?4 mM [Ca]_o the oocyte membrane behaved like a NaCl electrode. Studies on the steady potential as a function of [Na]_o, [K]_o and [Cl]_o in 1.0 mM Ca⁺⁺ or Ca-free solutions suggest that Ca⁺⁺ controls the passive permeability of the oocyte membrane to Na⁺ and Cl^?. In the ovulated unfertilized egg the K⁺ selectivity of the cell membrane disappeared and the system behaved like a NaCl electrode. No effect of external Ca⁺⁺ or K⁺ concentration changes on the steady potential was observed. These results indicate that the ion permeability properties of the ovulated egg are similar to that of the ovarian oocyte in Ca-deficient medium, and suggests that the mechanism of ovulation may involve the removal of Ca⁺⁺ regulation of ion permeability of the egg cell membrane.     

Basolateral membrane potential and conductance in frog skin exposed to high serosal potassium

Summary In studies of apical membrane current-voltage relationships, in order to avoid laborious intracellular microelectrode techniques, tight epithelia are commonly exposed to high serosal K concentrations. This approach depends on the assumptions that high serosal K reduces the basolateral membrane resistance and potential to insignificantly low levels, so that transepithelial values can be attributed to the apical membrane. We have here examined the validity of these assumptions in frog skins (Rana pipiens pipiens). The skins were equilibrated in NaCl Ringer's solutions, with transepithelial voltageV _t clamped (except for brief perturbations V _t) at zero. The skins were impaled from the outer surface with 1.5m KCl-filled microelectrodes (R _el>30 M). The transepithelial (short-circuit) currentl _i and conductanceg _t=–I _t/V _t, the outer membrane voltageV _o (apical reference) and voltage-divider ratio (F _o=V _o/V _t), and the microelectrode resistanceR _el were recorded continuously. Intermittent brief apical exposure to 20 m amiloride permitted estimation of cellular (c) and paracellular (p) currents and conductances. The basolateral (inner) membrane conductance was estimated by two independent means: either from values ofg _i andF _o before and after amiloride or as the ratio of changes (–I _c/V _i) induced by amiloride. On serosal substitution of Na by K, within about 10 min,I _c declined andg _t increased markedly, mainly as a consequence of increase ing _p. The basolateral membrane voltage (V _i(=–V _o) was depolarized from 75±4 to 2±1 mV [mean±sem (n=6)], and was partially repolarized following amiloride to 5±2 mV. The basolateral conductance increased in high serosal K, as estimated by both methods. Essentially complete depolarization of the basolateral membrane and increase in its conductance in response to high [K] were obtained also when the main serosal anion was SO₄ or NO₃ instead of Cl. On clampingV _t over the range 0 to +125 mV in K₂SO₄-depolarized skins, the quasi-steady-stateV _o V _t relationship was linear, with a mean slope of 0.88±0.03. The above results demonstrate that, in a variety of conditions, exposure to high serosal K results in essentially complete depolarization of the basolateral membrane and a large increase in its conductance.     

Action potentials inAcetabularia: Measurement and simulation of voltage-gated fluxes

Summary Amounts and temporal changes of the release of the tracer ions K⁺ (⁸⁶Rb⁺),²²Na⁺, and³⁶Cl^– as well as of H⁺ in the course of action potentials inAcetabularia have been recorded. New results and model calculations confirm in quantitative terms the involvement of three major ion transport systemsX in the plasmalemma: Cl^– pumps, K⁺ channels, and Cl^– channels (which are marked in the following by the prefixes,P, K andC) with their equilibrium voltages _X V _e and voltage/time-dependent conductances, which can be described by the following, first approximation. Let the maximum (ohmic) conductance of each of the three populations of transporter species be about the same (_P L, _KL,_C L=1) but voltage gating be different: the pump ( _{p V e} about –200 mV) being inactivated (open,oclosed,c) at positive going transmembrane voltages,V _m; the K⁺ channels (_K V _e about –100 mV) are inactivated at negative goingV _m; and the Cl^– channels (_C V _e: around 0 mV), which are normally closed (c) at a restingV _m (near_PV_e) go through an intermediate open (o) state at more positiveV _m before they enter a third shut state (s) in series. Model calculations, in which voltage sensitivities are expressed by the factorf=exp(V _mF/(2RT)), simulate, the action potential fairly well with the following parameters (_PK_co10/f ks^–1,_PK_oc1000·f ks^–1,_KK_co200·f ks^–1,_Kk_oc2/f ks^–1,_cK_co500·f ks^–1,_CK_oc5/f ks^–1,_CK_so0.1/f ks^–1,_Ck_os20·f ks^–1). It is also shown that the charge balance for the huge transient Cl^– efflux, which frequently occurs during an action potential, can be accounted for by the observation of a corresponding release of Na⁺.     

Net uptake of potassium in Neurospora. Exchange for sodium and hydrogen ions

Net uptake of potassium by low K, high Na cells of Neurospora at pH 5.8 is accompanied by net extrusion of sodium and hydrogen ions. The amount of potassium taken up by the cells is matched by the sum of sodium and hydrogen ions lost, under a variety of conditions: prolonged preincubation, partial respiratory inhibition (DNP), and lowered [K]_o. All three fluxes are exponential with time and obey Michaelis kinetics as functions of [K]_o. The V _max for net potassium uptake, 22.7 mmoles/kg cell water/min, is very close to that for K/K exchange reported previously (20 mmoles/kg cell water/min). However, the apparent K_m for net potassium uptake, 11.8 mM [K]_o, is an order of magnitude larger than the value (1 mM) for K/K exchange. It is suggested that a single transport system handles both net K uptake and K/K exchange, but that the affinity of the external site for potassium is influenced by the species of ion being extruded.     

Effects of caffeine on crayfish muscle fibers. II. Refractoriness and factors influencing recovery (repriming) of contractile responses

When caffeine evokes a contraction, and only then, crayfish muscle fibers become refractory to a second challenge with caffeine for up to 20 min in the standard saline (5 mM K_o). However, the fibers still respond with contraction to an increase in K_o, though with diminished tension. Addition of Mn slows recovery, but the latter is greatly accelerated during exposure of the fiber to high K_o, or after a brief challenge with high K_o. Neither the depolarization induced by the K, nor the repolarization after its removal accounts for the acceleration, which occurs only if the challenge with K had itself activated the contractile system; acceleration is blocked when contractile responses to K are blocked by reducing the Ca in the bath or by adding Mn. Recovery is accelerated by redistribution of intracellular Cl and by trains of intracellularly applied depolarizing pulses, but not by hyperpolarization. The findings indicate that two sources of Ca can be mobilized to activate the contractile system. Caffeine mobilizes principally the Ca store of the SR. Depolarizations that are induced by high K_o, by transient efflux of Cl, or by intracellularly applied currents mobilize another source of Ca which is strongly dependent upon the entry of Ca from the bathing medium. The sequestering mechanism of the SR apparently can utilize this second source of Ca to replenish its own store so as to accelerate recovery of responsiveness to a new challenge with caffeine.     

Influence of external barium and potassium on potassium efflux in depolarized frog sartorius muscles

Summary Efflux of⁴²K⁺ was measured in frog sartorius muscles equilibrated in depolarizing solutions with external K⁺ concentrations ([K⁺] _o ) between 75 and 300mm and NaCl concentrations of 60, 120, or 240mm. For several combinations of KCl and NaCl, steady-state internal potentials (V _i) were the same for different [K⁺] _o . For the range ofV _i examined, K⁺ efflux occurs principally through the K⁺ inward rectifier channels. When external K⁺ is removedV _i remains constant for 2 to 3 hr because of the high membrane conductance to Cl^–, but K⁺ efflux drops by about one order of magnitude.External Ba²⁺ in the presence or absence of external K⁺ produces an inhibition of K⁺ efflux described by a relation of the formu=(u₁/(1+C)[Ba²⁺] _o ))+u ₂, whereu is the uninhibited fraction of K⁺ efflux;u ₁, u₂ andC are constants; andu ₁+u₂=1.C depends both on [K⁺] _o andV _i. When [K⁺] _o 75mm, increasing [K⁺] _o at constantV _i reduces Ba²⁺ sensitivity. For constantV _i–30 mV, Ba²⁺ sensitivity is less when [K⁺] _o =0 than when [K⁺] _o 75mm. When [K⁺] _o =0, Ba²⁺ sensitivity decreases asV _i is made more positive. The dependence of the Ba²⁺ sensitivity onV _i at constant [K⁺] _o is greater when [K⁺] _o =0 than when [K⁺] _o 75mm.Both the activation of K⁺ efflux by external K⁺ and the Ba²⁺ inhibition of K⁺ efflux can be explained on the basis of two membrane control sites associated with each channel. When both sites are occupied by K⁺, the channels are in a high flux state. When one or both sites are empty, the channels are in a low, nonzero flux state. When Ba²⁺ occupies either site, K⁺ efflux is further reduced. The reduction of Ba²⁺-sensitivity by increasing [K⁺] _o at high [K⁺] _o is attributable to the displacement of Ba²⁺ from the control sites by K⁺. The increased Ba²⁺ sensitivity produced by going from [K⁺] _o =0 to [K⁺] _o >-75mm whenV _i–30 mV is attributable to states in which Ba²⁺ occupies one site and K⁺ the other when [K⁺] _o 0. The smallerV _i dependence of the Ba²⁺ sensitivity when [K⁺] _o 75mm compared to [K⁺] _o =0 is attributable to the necessity that Ba²⁺ displace K⁺ at the control sites when [K⁺] _o is high but not when [K⁺] _o =0.     

N(4)-Tolyl-2-acetylpyridine thiosemicarbazones and their platinum(II,IV) and gold(III) complexes: cytotoxicity against human glioma cells and studies on the mode of action

Complexes [Au(2Ac4oT)Cl][AuCl₂] (1), [Au(H_py2Ac4mT)Cl₂]Cl·H₂O (2), [Au(H_py2Ac4pT)Cl₂]Cl (3), [Pt(H2Ac4oT)Cl]Cl (4), [Pt(2Ac4mT)Cl]·H₂O (5), [Pt(2Ac4pT)Cl] (6) and [Pt(L)Cl₂OH], L = 2Ac4mT (7), 2Ac4oT (8), 2Ac4pT (9) were prepared with N(4)-ortho- (H2Ac4oT), N(4)-meta- (H2Ac4mT) and N(4)-para- (H2Ac4pT) tolyl-2-acetylpyridine thiosemicarbazone. The cytotoxic activities of all compounds were assayed against U-87 and T-98 human malignant glioma cell lines. Upon coordination cytotoxicity improved in 2, 5 and 8. In general, the gold(III) complexes were more cytotoxic than those with platinum(II,IV). Several of these compounds proved to be more active than cisplatin and auranofin used as controls. The gold(III) complexes probably act by inhibiting the activity of thioredoxin reductase enzyme whereas the mode of action of the platinum(II,IV) complexes involves binding to DNA. Cells treated with the studied compounds presented morphological changes such as cell shrinkage and blebs formation, which indicate cell death by apoptosis induction.     

Roles of external and cellular Cl− ions on the activation of an apical electrodiffusional Cl− pathway in toad skin

Summary This study is concerned with the short-circuit current,I _sc, responses of the Cl^–-transporting cells of toad skin submitted to sudden changes of the external Cl^– concentration. [Cl]₀. Sudden changes of [Cl]₀, carried out under apical membrane depolarization, allowed comparison of the roles of [Cl]₀ and [Cl]_cell on the activation of the apical Cl^– pathways. Equilibration of shortcircuited skins symmetrically in K-Ringer's solutions of different Cl^– concentrations permitted adjustment of [Cl]_cell to different levels. For a given Cl^– concentration (in the range of 11.7 to 117mm) on both sides of a depolarized apical membrane, this structure exhibits a high Cl^– permeability,P _(Cl)apical. On the other hand, for the same range of [Cl]_cell but with [Cl]₀=0,P _(Cl)apical is reduced to negligible values. These observations indicate that when the apical membrane is depolarizedP _(Cl)apical is modulated by [Cl]₀; in the absence of external Cl^– ions, intracellular Cl^– is not sufficient to activateP _(Cl)apical. Computer simulation shows that the fast Cl^– currents induced across the apical membrane by sudden shifts of [Cl]₀ from a control equilibrium value strictly follow the laws of electrodiffusion. For each experimental group, the computer-generatedI _sc versus ([Cl]_cell–[Cl]₀) curve which best fits the experimental data can only be obtained by a unique pair ofP _(Cl)apical andR _b (resistance of the basolateral membrane), thus allowing the calculation of these parameters. The electrodiffusional behavior of the net Cl^– flux across the apical membrane supports the channel nature of the apical Cl^– pathways in the Cl^–-transporting cell. Cl^– ions contribute significantly to the overall conductance of the basolateral membrane even in the presence of a high K concentration in the internal solution.     

Effect of metabolic depletion on the furosemide-sensitive Na and K fluxes in human red cells

Summary We report in this paper the effect of metabolic depletion on several modes of furosemide-sensitive (FS) Na and K transport in human red blood cells. The reduction of ATP content below 100 mol/liter cells produced a marked decrease in the maximal activation (V _max) of the outward. FS transport of Na and K into choline medium in the presence of ouabain (0.1 mM) and 1 mM MgCl₂. TheK _0.5 for internal Na to activate the FS Na efflux was not altered by metabolic depletion. However, metabolic depletion markedly decreased the K _i for external K (K _o ) to inhibit the FS Na efflux into choline medium (from 25 to 11 mM). Repletion of ATP content by incubation of cells in a substraterich medium recovered control levels ofV _max of the FS Na and K fluxes and of K _i for external K to inhibit FS Na efflux. TheV _max of FS Na and K influxes was also markedly decreased when the ATP content dropped below 100 mol/liter cells. This was mainly due to a decrease in the inward-coupled transport of K and Na (Na _o -stimulated K influx and the K _o -stimulated Na influx). The FS K _i /K _o exchange pathway of the Na–K cotransport, estimated from the FS K influx from choline-20 mM K _o medium into cells containing 22 mmol Na/liter cells, was also reduced by starvation. Starvation did not inhibit the FS Na _i /Na _o exchange pathway, estimated as FS Na influx from a medium containing 130 mM NaCl into cells containing 22 mmol Na/liter cells. The unidirectional FS²²Na efflux and influx were also measured in control and starved cells containing 22 mmol Na/liter cells, incubated in a Na medium (130 mM) at varying external K (0 to 20 mM). In substrate-fed cells, incubated in the absence of external K, FS Na efflux was larger than Na influx. This FS net Na extrusion (400 to 500 mol/liter cells·hr) decreased when external K was increased, approaching zero around 15 mM K _o . In starved cells the net Na extrusion was markedly decreased and it approached zero at lower K _o than in substrate-fed cells. Our results indicate that the FS Na and K fluxes, and their major component, the gradient driven Na–K–Cl cotransport system, are dependent on the metabolic integrity of the cells.     

Potassium-proton symport inNeurospora: kinetic control by pH and membrane potential

Summary Active transport of potassium in K⁺-starvedNeurospora was previously shown to resemble closely potassium uptake in yeast,Chlorella, and higher plants, for which K⁺ pumps or K⁺/H⁺-ATPases had been proposed. ForNeurospora, however, potassium-proton cotransport was demonstrated to operate, with a coupling ratio of 1 H⁺ to 1 K⁺ taken inward so that K⁺, but not H⁺, moves against its electrochemical gradient (Rodriguez-Navarro et al.,J. Gen. Physiol. 87:649–674).In the present experiments, the current-voltage (I–V) characteristic of K⁺–H⁺ cotransport in spherical cells ofNeurospora has been studied with a voltage-clamp technique, using difference-current methods to dissect it from other ion-transport processes in theNeurospora plasma membrane. Addition of 5-200 M K⁺ to the bathing medium causes 10–150 mV depolarization of the unclamped membrane, and yields a sigmoidI–V curve with a steep slope (maximal conductance of 10–30 S/cm²) for voltages of –300 to –100 mV, i.e., in the normal physiologic range. Outside that range the apparentI–V curve of the K⁺-H⁺ symport saturates for both hyperpolarization and depolarization. It fails to cross the voltage axis at its predicted reversal potential, however, an effect which can be attributed to failure of theI–V difference method under reversing conditions.In the absence of voltage clamping, inhibitors—such as cyanide or vanadate—which block the primary proton pump inNeurospora also promptly inhibit K⁺ transport and K⁺-H⁺ currents. But when voltage clamping is used to offset the depolarizing effects of pump blockade, the inhibitors have no immediate effect on K⁺-H⁺ currents. Thus, the inhibition of K⁺ transport usually observed with these agents reflects the kinetic effect of membrane depolarization rather than any direct chemical action on the cotransport system itself.Detailed study of the effects of [K⁺]_o and pH_o on theI–V curve for K⁺-H⁺ symport has revealed that increasing membrane potential systematicallydecreases the apparent affinity of the transporter for K⁺, butincreases affinity for protons (K _m range: for [K⁺]_o, 15–45 M; for [H⁺]_o, 10–35 nM). This behavior is consistent with two distinct reaction-kinetic models, in which (i) a neutral carrier binds K⁺ first and H⁺ last in the forward direction of transport, or (ii) a negatively charged carrier (–2) binds H⁺ first and K⁺ last.     

Ionic interconversion of pacemaker and nonpacemaker cultured chick heart cells

Trypsin-dispersed cells from hearts (ventricles) of 7 to 8 day chick embryos were cultured 3 to 21 days. The cells became attached to the culture dish and assembled into monolayer communities. By means of a bridge circuit, one microelectrode was used for simultaneously passing current and recording membrane potentials (V_m). The input resistance, calculated by the measured ΔV_m for a known step of current, averaged 10 MΩ. Electrotonic depolarization of nonpacemaker cells had no effect on frequency of firing. Within 2 min after addition of Ba⁺⁺ (5 to 10 mM) to the Tyrode bath, the cells became partially depolarized and quiescent nonpacemaker cells developed oscillations in V_m which led to action potentials. With time, the depolarization became nearly complete and the input resistance increased 2 to 10 times. During such sustained depolarizations, action potentials were no longer produced and often tiny oscillations were observed; however, large action potentials developed during hyperpolarizing pulses. Thus, the automaticity of the depolarized cell became apparent during artificial repolarization. Sr⁺⁺ (5 to 10 mM) initially produced hyperpolarization and induced automaticity in quiescent nonpacemaker cells. Elevated [K⁺]_o (20 to 30 mM) suppressed automaticity of pacemaker cells and decreased R_m concomitantly. Thus, Ba⁺⁺ probably converts nonpacemaker cells into pacemaker cells independently of its depolarizing action. Ba⁺⁺ may induce automaticity and depolarization by decreasing g _K, and elevated [K⁺]_o may depress automaticity by increasing g _K. The data support the hypothesis that the level of g _K determines whether a cell shall function as a pacemaker.     

Cesium,Na+-K+ pump and pacemaker potential in cardiac purkinje fibers

The mechanisms of the hyperpolarizing and depolarizing actions of cesium were studied in cardiac Purkinje fibers perfused in vitro by means of a microelectrode technique under conditions that modify either the Na⁺-K⁺ pump activity or I_f. Cs⁺ (2 mM) inconsistently increased and then decreased the maximum diastolic potential (MDP); and markedly decreased diastolic depolarization (DD). Increase and decrease in MDP persisted in fibers driven at fast rate (no diastolic interval and no activation of I_f). In quiescent fibers, Cs⁺ caused a transient hyperpolarization during which elicited action potentials were followed by a markedly decreased undershoot and a much reduced DD. In fibers depolarized at the plateau in zero [K⁺]_o (no I_f), Cs⁺ induced a persistent hyperpolarization. In 2 mM [K⁺]_o, Cs⁺ reduced the undershoot and suppressed spontaneous activity by hyperpolarizing and thus preventing the attainment of the threshold. In 7 mM [K⁺]_o, DD and undershoot were smaller and Cs⁺ reduced them. In 7 and 10 mM [K⁺]_o, Cs⁺ caused a small inconsistent hyperpolarization and a net depolarization in quiescent fibers; and decreased MDP in driven fibers. In the presence of strophanthidin, Cs⁺ hyperpolarized less. Increasing [Cs⁺]_o to 4, 8 and 16 mM gradually hyperpolarized less, depolarized more and abolished the undershoot. We conclude that in Purkinje fibers Cs⁺ hyperpolarizes the membrane by stimulating the activity of the electrogenic Na⁺-K⁺ pump (and not by suppressing I_f); and blocks the pacemaker potential by blocking the undershoot, consistent with a Cs⁺ block of a potassium pacemaker current.     

Electrical properties of the plasma membrane of microplasmodia ofPhysarum polycephalum

Summary Microplasmodia ofPhysarum polycephalum have been investigated by conventional electrophysiological techniques. In standard medium (30mm K⁺, 4mm Ca⁺⁺, 3mm Mg⁺⁺, 18mm citrate buffer, pH 4.7, 22°C), the transmembrane potential differenceV _m is around –100 mV and the membrane resistance about 0.25 m².V _m is insensitive to light and changes of the Na⁺/K⁺ ratio in the medium. Without bivalent cations in the medium and/or in presence of metabolic inhibitors (CCCP, CN^–, N ₃ ^– ),V _m drops to about 0 mV. Under normal conditions,V _m is very sensitive to external pH (pH _o ), displaying an almost Nernstian slope at pH _o =3. However, when measured during metabolic inhibition,V _m shows no sensitivity to pH _o over the range 3 to 6, only rising (about 50 mV/pH) at pH _o =6. Addition of glucose or sucrose (but not mannitol or sorbitol) causes rapid depolarization, which partially recovers over the next few minutes. Half-maximal peak depolarization (25 mV with glucose) was achieved with 1mm of the sugar. Sugar-induced depolarization was insensitive to pH _o . The results are discussed on the basis of Class-I models of charge transport across biomembranes (Hansen, Gradmann, Sanders and Slayman, 1981,J. Membrane Biol. 63:165–190). Three transport systems are characterized: 1) An electrogenic H⁺ extrusion pump with a stoichiometry of 2 H⁺ per metabolic energy equivalent. The deprotonated form of the pump seems to be negatively charged. 2) In addition to the passive K⁺ pathways, there is a passive H⁺ transport system; here the protonated form seems to be positively charged. 3) A tentative H⁺-sugar cotransport system operates far from thermodynamic equilibrium, carrying negative charge in its deprotonated states.