Electrical characteristics of stomatal guard cells: The contribution of ATP-dependent, “Electrogenic” transport revealed by current-voltage and difference-current-voltage analysis

Summary The steady-state, current-voltage (I–V) characteristics of stomatal guard cells fromVicia faba L. were explored by voltage clamp using conventional electrophysiological techniques, but with double-barrelled microelectrodes containing 50mm K⁺-acetate. Attention was focused, primarily, on guard cell response to metabolic blockade. Exposures to 0.3–1.0mm NaCN and 0.4mm salicylhydroxamic acid (SHAM) lead consistently to depolarizing (positive-going) shifts in guard cell potentials (V _m ), as large as +103 mV, which were generally complete within 60–90 sec (mean response half-time, 10.3±1.7 sec); values forV _m in NaCN plus SHAM were close or positive to –100 mV and well removed from the K⁺ equilibrium potential. Guard cell ATP content, which was followed in parallel experiments, showed a mean half-time for decay of 10.8±1.9 ([ATP] _t=0, 1.32±0.28mm; [ATP] _{t=60–180sec}, 0.29±0.40mm). In respiring cells, theI–V relations were commonly sigmoid aboutV _m or gently concave to the voltage axis positive toV _m . Inward- and outward-rectifying currents were also observed, especially near the voltage extremes (nominally –350 and +50 mV). Short-circuit currents (atV=0 mV) were typically about 200–500 mA m^–2. The principal effect of cyanide early on was to linearize theI–V characteristic while shifting it to the right along the voltage axis, to decrease the membrane conductance, and to reduce the short-circuit current by approx. 50–75%. The resulting difference-current-voltage (dI–V) curves (±cyanide) showed a marked sensitivity to voltages negative from –100 mV and, when clamp scans had been extended sufficiently, they revealed a distinct minimum near –300 mV before rising at still more negative potentials. The difference currents, along with changes in guard cell potential, conductance and ATP content are interpreted in context of a primary, ATP-consuming ion pump. FittingdI–V curves to reaction kinetic model for the pump [Hansen, U.-P., et al. (1981)J. Membrane Biol. 63:165; Blatt, M.R. (1986)J. Membrane Biol. 92:91] implicates a stoichiometry of one (+) charge transported outward for each ATP hydrolyzed, with pump currents as high as 200 mA m^–2 at the free-running potential. The analysis indicates that the pump can comprise more than half of the total membrane conductance and argues against modulations of pump activity alone, as an effective means to controlling K⁺ transport for stomatal movements.     

Cell K activity in frog skin in the presence and absence of cell current

Summary Cell K activity,a _k, was measured in the short-circuited frog skin by simultaneous cell punctures from the apical surface with open-tip and K-selective microelectrodes. Strict criteria for acceptance of impalements included constancy of the open-tip microelectrode resistance, agreement within 3% of the fractional apical voltage measured with open-tip and K-selective microelectrodes, and constancy of the differential voltage recorded between the open-tip and the K microelectrodes 30–60 sec after application of amiloride or substitution of apical Na. Skins were bathed on the serosal surface with NaCl Ringer and, to reduce paracellular Cl conductance and effects of amiloride on paracellular conductance, with NaNO₃ Ringer on the apical surface.Under control conditionsa _k ^r was nearly constant among skins (mean±SD=92±8mM, 14 skins) in spite of a wide range of cellular currents (5 to 70 A/cm²). Cell current (and transcellular Na transport) was inhibited by either apical addition of amiloride or substitution of Na by other cations. Although in some experiments the expected small increase ina _k ^r after inhibition of cell current was observed, on the average the change was not significant (98±11mM after amiloride, 101±12mM after Na substitution), even 30 min after the inhibition of cell current. The membrane potential, which in the control state ranged from –42 to –77 mV, hyperpolarized after inhibition of cell current, initially to –109±5mV, then depolarizing to a stable value (–88±5mV) after 15–25 min. At this time K was above equilibrium (E _k=98±2mV), indicating that the active pump mechanism is still operating after inhibition of transcellular Na transport.The measurement ofa _k ^r permitted the calculation of the passive K current and pump current under control conditions. assuming a constant current source with almost all of the basolateral conductance attributable to K. We found a significant correlation between pump current and cell current with a slope of 0.31, indicating that about one-third of the cell current is carried by the pump, i.e., a pump stoichiometry of 3Na/2K.     

Current-voltage relationships and voltage sensitivity of the Cl− pump inHalicystis parvula

Summary The current-voltage (I–V) relationships for internally perfused and nonperfused cells ofHalicystis parvula were determined. In both types of cells theI–V curve shows a conspicuous region of negative slope, beginning at vacuole potentials around –30 mV and continuing to values of +20 to +40mV. The negative slope in perfused cells is abolished by the metabolic inhibitors, darkness and low temperature. In order to determine the origin of this negative slope, we measured the voltage sensitivity of the unidirectional fluxes of Cl^–, Na⁺ and K⁺ in perfused cells. The results show that the Cl^– influx, which is mediated primarily by a Cl^– pump, increases as the vacuole potential is clamped at increasingly morenegative values up to –50 mV, while the other fluxes measured changed in the directions predicted by the change in electrical driving force. The voltage sensitivity of the Cl^– pump quantitatively accounts for the negative slope of theI–V curve. Also, we observed a large transient outward current of 10–20-sec duration following an abrupt depolarization by voltage clamping. This transient current was reduced or abolished by low temperature, which suggests that it may be due to the voltage-sensitive Cl^– pump. Finally, we found an inverse relationship between the transprotoplasm resistance (R _m ) and thePD under standard conditions, which suggests that the activity of the electrogenic Cl^– pump lowerR _m , i.e., it is a conductive pump.     

Patch-clamp study of isolated taste receptor cells of the frog

Summary Taste discs were dissected from the tongue ofR. ridibunda and their cells dissociated by a collagenase/low Ca/mechanical agitation protocol. The resulting cell suspension contained globular epithelial cells and, in smaller number, taste receptor cells. These were identified by staining properties and by their preserved apical process, the tip of which often remained attached to an epithelial (associated) cell. When the patch pipette contained 110mm KCl and the cells were superfused with NaCl Ringer's during whole-cell recording, the mean zero-current potential of 22 taste receptor cells was –65.2 mV and the slope resistance 150 to 750 M. Pulse-depolarization from a holding voltage of –80 mV activated a transient TTX-blockable inward Na current. Activation became noticeable at –25 mV and was half-maximal at –8 mV. Steady-state inactivation was half-maximal at –67 mV and complete at –50 mV. Peak Na current averaged –0.5 nA/cell. The Ca-ionophore A23187 shifted the activation and inactivation curve to more negative voltages. Similar shifts occurred when the pipette Ca was raised. External Ni (5mm) shifted the activation curve towards positive voltages by 10 mV. Pulse depolarization also activated outward K currents. Activation was slower than that of Na current and inactivation slower still. External TEA (7.5mm) and 4-aminopyridine (1mm) did not block, but 5mm Ba blocked the K currents. K-tail currents were seen on termination of depolarizing voltage pulses. A23187 shifted theI _K(V)-curve to more negative voltages. Action potentials were recorded when passing pulses of depolarizing outward current. Of the frog gustatory stimulants, 10mm Ca caused a reversible 5-to 10-mV depolarization in the current-clamp mode. Quinine (0.1mm, bitter) produced a reversible depolarization accompanied by a full block of Na current and, with slower time-course, a partial block of K currents. Cyclic AMP (5mm in the external solution or 0.5 m in the pipette) caused reversible depolarization (to –40 to –20 mV) due to partial blockage of K currents, but only if ATP was added to the pipette solution. Similar responses were elicited by stimulating the adenylate cyclase with forskolin. Blockage of cAMP-phosphodiesterase enhanced the response to cAMP. These results suggest that cAMP may be one of the cytosolic messengers in taste receptor cells. Replacement of ATP by AMP-PNP in the pipette abolished the depolarizing response to cAMP. Inclusion of ATP--S in the pipette caused slow depolarization to –40 to –20 mV, due to partial blockage of K currents. Subsequently, cAMP was without effect. The remaining K currents were blockable by Ba. These results suggest that cAMP initiates phosphorylation of one set of K channels to a nonconducting conformation.     

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

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

A kinetic analysis of the electrogenic pump ofChara corallina: III. Pump activity during action potential

Summary The current-voltage curve (I–V curve) of theChara membrane was obtained by applying a slow ramp hyper- and depolarization by use of voltage clamp. By inhibiting the electrogenic pump with 50m DCCD (dicyclohexylcarbodiimide), theI–V curve approached a steadyI–V curve within two hours, which gave thei _d -V curve of the passive diffusion channel. Thei _p -V curve of the electrogenic pump channel was obtained by subtracting the latter from the former. The sigmoidali _p -V curve could be simulated satisfactorily with a simple reaction kinetic model which assumes a stoichiometric ratio of 2. The emf of the pump (E _p ) is given as the voltage at which the pump current changes its sign. The conductance of the pump (g _p ) can be calculated as the chord conductance from thei _p -V curve, which is highly voltage dependent having a peak at a definite voltage. The changes of emf and conductance during excitation were determined by use of the current clamp (I=0). Since theE _p andg _p (V) are known, the changes, during excitation, of emf (E _d ) and conductance (g _d ) of the passive diffusion channel can be calculated. The marked increase of the membrane conductance and the large depolarization during the action potential are caused by the marked increase of the conductance of the passive diffusion channel and the large depolarization of its emf. The conductance of the electrogenic pump decreases to about half at the peak of action potential, while the pump current increases almost to a saturated level.     

Voltage dependence of current through the Na,K-exchange pump ofRana oocytes

Summary We have studied current (I _Str) through the Na, K pump in amphibian oocytes under conditions designed to minimize parallel undesired currents. Specifically,I _Str was measured as the strophanthidin-sensitive current in the presence of Ba^2–, Cd²⁺ and gluconate (in place of external Cl^–). In addition,I _Str was studied only after the difference currents from successive applications and washouts of strophanthidin (Str) were reproducible. The dose-response relationship to Str in four oocytes displayed a meanK _0.5 of 0.4 m, with 2–5 m producing 84–93% pump' block. From baseline data with 12 Na⁺-preloaded oocytes, voltage clamped in the range [–170, +50 mV] with and without 2–5 m Str, the averageI _Str depended directly onV _m up to a plateau at 0 mV with interpolated zero current at –165 mV. In three oocytes, lowering the external [Na⁺] markedly decreased the voltage sensitivity ofI _p , while producing only a small change in the maximal outwardI _Str. In contrast, decreasing the external [K⁺] from 25 to 2.5mm reducedI _Str at 0 mV without substantially affecting its voltage dependence. At K⁺ concentrations of 1mm, both the absolute value ofI _Str at 0 mV and the slope conductance were reduced. In eight oocytes, the activation of the averagedI _Str by [K⁺] _o over the voltage interval [–30, +30 mV] was well fit by the Hill equation, with K=1.7±0.4mm andnH (the minimum number of K⁺ binding sites) =1.7±0.4. The results unequivocally establish that the cardiotonic-sensitive current ofRana oocytes displays only a positive slope conductance for [K⁺] _o >1mm. There is therefore no need to postulate more than one voltage-sensitive step in the cycling of the Na, K pump under physiologic conditions. The effects of varying external Na⁺ and K⁺ are consistent with results obtained in other tissues and may reflect an ion-well effect.     

Potassium-dependent,bipolar gating of K+ channels in guard cells

Summary Guard cells of higher plants control transpirational water loss and gas exchange for photosynthesis by opening and closing pores in the epidermis of the leaf. To power these turgordriven movements, guard cells accumulate (and lose) 200 to 400mm (1 to 3 pmol/cell) K⁺, fluxes thought to pass through K⁺ channels in the guard cells plasma membrane. Steady-state current-voltage (I–V) relations of intactVicia guard cells frequently show large, outward-going currents at potentials approaching 0 mV. Since this current could be carried by K⁺ channels, its pharmacology and dependence on external K⁺ (K _v ⁺ ) has been examined under voltage clamp over an extended potential range. Measurements were carried out on cells which showed little evidence of primary electrogenic transport, thus simplifying analyses. Clamping these cells away from the free-running membrane potential (V _m ) revealed an outward-rectifying current with instantaneous and time-dependent components, and sensitive to the K⁺ channel blocker tetraethylammonium chloride. The current declined also under metabolic blockade with NaCN and in the presence of diethylstilbesterol, responses which were attributed to secondary effects of these inhibitors. The putative K⁺ current rose with voltage positive toV _m but it decayed over two voltage ranges, one negative toV _m and one near +100 mV, to give steady-stateI–V relations with two regions of negative (slope) conductance. Voltage-dependent and kinetic characteristics of the current were affected by K _v ⁺ and followed the K⁺ equilibrium potential. Against a (presumably) low background of primary ion transport, the K⁺ current contributed appreciably to charge balance atV _m in 0.1mm as well as in 1 to 10mm K _v ⁺ . Thus, gating of these K⁺ channels compensates for the prevailing K⁺ conditions to ensure net K⁺ movement out of the cell.     

Intracellular potassium activity in mammalian proximal tubule: Effect of perturbations in transepithelial sodium transport

Summary Intracellular potassium activity (a _{K i} ) was measured in control conditions in mid-cortical rabbit proximal convoluted tubule using two methods: (i) by determination of the K⁺ equilibrium potential (E _K) using Ba²⁺-induced variations in the basolateral membrane potential (V _BL) during transepithelial current injections and (ii) with double-barrel K-selective microelectrodes. Using the first method, the meanV _BL was –48.5±3.2 mV (n=16) and the meanE _K was –78.4±4.1 mV corresponding to aa _{K i} of 68.7mm. With K-selective microelectrodes,V _BL was –36.6±1.1 mV (n=19),E _K was –64.0±1.1 mV anda _{K i} averaged 40.6±1.7mm. While these lastE _K andV _BL values are significantly lower than the corresponding values obtained with the first method (P<0.001 andP<0.01, respectively), the electrochemical driving force for K transport across the basolateral membrane ( _K =V _BL –E _K) is not significantly different for both techniques (30.1±3.3 mV for the first technique and 27.6±1.8 mV for ion-selective electrodes). This suggests an adequate functioning of the selective barrel but an underestimation ofV _BL by the reference barrel of the double-barrel microelectrode. Such double-barrel microelectrodes were used to measure temporal changes ina _{K i} and _K in different experimental conditions where Na reabsorption rate (J _Na) was reduced.a _{K i} was shown to increase by 12.2±2.7 (n=5) and 14.1±4.4mm (n=5), respectively, whenJ _Na was reduced by omitting in the luminal perfusate: (i) 5.5mm glucose and 6mm alanine and (ii) glucose, alanine, other Na-cotransported solutes and 110mm Na. In terms of the electrochemical driving force for K exit across the basolateral membrane, _K, a decrease of 5.4±2.0 mV (P<0.05,n=5) was measured when glucose and alanine were omitted in the luminal perfusate while _K remained unchanged whenJ _Na was more severely reduced (mean change =–1.7±2.1 mV, NS,n=5). In the latter case, this means that the electrochemical driving force for K efflux across the basolateral membrane has not changed while both the active influx through the Na–K pump and the passive efflux in steady state are certainly reduced. If the main pathway for K transport is through the basolateral K conductance, this implies that this conductance must have decreased in the same proportion as that of the reduction in the Na–K pump activity.     

Apical membrane K conductance in the toad urinary bladder

Summary The conductance of the apical membrane of the toad urinary bladder was studied under voltage-clamp conditions at hyperpolarizing potentials (mucosa negative to serosa). The serosal medium contained high KCl concentrations to reduce the voltage and electrical resistance across the basal-lateral membrane, and the mucosal solution was Na free, or contained amiloride, to eliminate the conductance of the apical Na channels. As the mucosal potential (V _m) was made more negative the slope conductance of the epithelium increased, reaching a maximum at conductance of the epithelium increased, reaching a maximum atV _m=–100 mV. This rectifying conductance activated with a time constant of 2 msec whenV _m was changed abruptly from 0 to –100 mV, and remained elevated for at least 10 min, although some decrease of current was observed. ReturningV _m to+100 mV deactivated the conductance within 1 msec. Ion substitution experiments showed that the rectified current was carried mostly by cations moving from cell to mucosa. Measurement of K flux showed that the current could be accounted for by net movement of K across the apical membrane, implying a voltage-dependent conductance to K (G _K). Mucosal addition of the K channel blockers TEA and Cs had no effect onG _K, while 29mm Ba diminished it slightly. Mucosal Mg (29mm) also reducedG _K, while Ca (29mm) stimulated it.G _K was blocked by lowering the mucosal pH with an apparent pK₁ of 4.5. Quinidine (0.5mm in the serosal bath) reducedG _K by 80%.G _K was stimulated by ADH (20 mU/ml), 8-Br-cAMP (1mm), carbachol (100 m), aldosterone (5×10^–7 m for 18 hr), intracellular Li and extracellular CO₂.     

Kinetics and specificity of the renal Na+/myo-inositol cotransporter expressed in Xenopus Oocytes

The two-microelectrode voltage clamp technique was used to examine the kinetics and substrate specificity of the cloned renal Na⁺/myo-inositol cotransporter (SMIT) expressed in Xenopus oocytes. The steady-state myo-inositol-induced current was measured as a function of the applied membrane potential (V _m ), the external myo-inositol concentration and the external Na⁺ concentration, yielding the kinetic parameters: K _0.5 ^MI , K _0.5 ^Na , and the Hill coefficient n. At 100 mM NaCl, K _0.5 ^MI was about 50 m and was independent of V _m . At 0.5 mm myo-inositol, K _0.5 ^Na ranged from 76 mm at V _m =–50 mV to 40 mm at V _m =–150 mV. n was voltage independent with a value of 1.9±0.2, suggesting that two Na⁺ ions are transported per molecule of myo-inositol. Phlorizin was an inhibitor with a voltage-dependent apparent K _I of 64 m at V _m =–50 mV and 130 m at V _m = –150 mV. To examine sugar specificity, sugar-induced steady-state currents (at V _m =–150 mV) were recorded for a series of sugars, each at an external concentration of 50 mm. The substrate selectivity series was myo-inositol, scyllo-inositol > l-fucose > l-xylose > l-glucose, d-glucose, -methyl-d-glucopyranoside > d-galactose, d-fucose, 3-O-methyl-d-glucose, 2-deoxy-d-glucose > d-xylose. For comparison, oocytes were injected with cRNA for the rabbit intestinal Na⁺/glucose cotransporter (SGLT1) and sugar-induced steady-state currents (at V _m =–150 mV) were measured. For oocytes expressing SGLT1, the sugar selectivity was: d-glucose, -methyl-d-glucopyranoside, d-galactose, d-fucose, 3-O-methyl-d-glucose > d-xylose, l-xylose, 2-deoxy-d-glucose > myo-inositol, l-glucose, l-fucose. The ability of SMIT to transport glucose and SGLT1 to transport myo-inositol was independently confirmed by monitoring the Na⁺-dependent uptake of ³H-d-glucose and ³H-myo-inositol, respectively. In common with SGLT1, SMIT gave a relaxation current in the presence of 100 mm Na⁺ that was abolished by phlorizin (0.5 mm). This transient current decayed with a voltage-sensitive time constant between 10 and 14 msec. The presteady-state current is apparently due to the reorientation of the cotransporter protein in the membrane in response to a change in V _m . The kinetics of SMIT is accounted for by an ordered six-state nonrapid equilibrium model. Present address: W.M. Keck Biotechnology Resource Laboratory, Boyer Center for Molecular Medicine, Rm, 305A, Yale University, 295 Congress Ave., New Haven, Connecticut 06536-0812 Present address: National Institute for Physiological Sciences, Department of Cell Physiology, Okazaka, 444, JapanContributed equally to this workWe thank John Welborn for the HPLC analysis of the sugar substrates. This work was supported by grants from the National Institutes of Health DK19567, DK42479 and NS25554.     

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.     

Current-voltage relationships of potassium channels in the plasmalemma ofAcetabularia

Summary The outer membrane of mechanically prepared protoplasmic droplets fromAcetabularia mediterranea has been investigated by patch-clamp techniques. These membranes are shown to consist of physiologically intact plasmalemma. With the Cl^– pump inhibited, microscopic currents through K⁺-selective channels were studied. These currents compare well with macroscopic K⁺ currents as previously determined by standard microelectrode techniques and tracer flux measurements. There is about one K⁺ channel per m² in the plasmalemma. The current-voltage relationship (I–V curve) of the main open channel (channel A) is sigmoid over a voltage range between about –100 and +100 mV with saturation currents of about ±10 pA. A second species (or different state of channel A) of K⁺-selective channels (channel B) differs from channel A by smaller saturation currents (about ±7 pA) and a much smaller open probability. The open probability of channel A increases from almost zero at large negative voltages to about 1/2 at large positive voltages. Taking the closed times into account, the mean steady-stateI–V curve of channel A displays outward rectification about the equilibrium voltage for K⁺ and negative slope conductance at larger negative voltages. The open channelI–V curve of the open channels A and B, the changes of theI–V curve of the open channel A upon variation of the external K⁺ concentration, as well as the mean steady-stateI–V curves of channel A are described by simple reaction kinetic models, the parameters of which are determined to fit the experimental data. The results are discussed with respect to data from other K⁺ channels in plants and with respect to regulation of the cytoplasmic K⁺ concentration inAcetabularia.     

Current-voltage relationships of a sodium-sensitive potassium channel in the tonoplast ofChara corallina

Summary The membrane of mechanically prepared vesicles ofChara corallina has been investigated by patch-clamp techniques. This membrane consists of tonoplast as demonstrated by the measurement of ATP-driven currents directed into the vesicles as well as by the ATP-dependent accumulation of neutral red. Addition of 1mm ATP to the bath medium induced a membrane current of about 3.2 mA·m^–2 creating a voltage across the tonoplast of about –7 mV (cytoplasmic side negative). On excised tonoplast patches, currents through single K⁺-selective channels have been investigated under various ionic conditions. The open-channel currents saturate at large voltage displacements from the equilibrium voltage for K⁺ with limiting currents of about +15 and –30 pA, respectively, as measured in symmetric 250mm KCl solutions. The channel is virtually impermeable to Na⁺ and Cl^–. However, addition of Na⁺ decreases the K⁺ currents. TheI–V relationships of the open channel as measured at various K⁺ concentrations with or without Na⁺ added are described by a 6-state model, the 12 parameters of which are determined to fit the experimental data.     

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.     

Effect of Na i on activity and voltage dependence of the Na/K pump in adult rat cardiac myocytes

We have measured the voltage dependence of the Na/K pump in isolated adult rat cardiac myocytes using the whole-cell patch-clamp technique. In the presence of 1–2 mM Ba and 0.1 mm Cd and nominally Ca-free, Na/K pump current (I _p) was measured as the change in current due to 1 mM ouabain. Voltage dependence of I _pwas measured between –140 and +40 or +60 mV using square voltage-pulse and voltage-ramp protocols, respectively. With 150 mM extracellular Na (Na _o ) and 5.4 mM extracellular K (K _o ), we found that the Na/K pump shows a strong positive voltage dependence between –140 and 0 mV and is voltage independent at positive potentials. Removing Na _o reduced the voltage dependence at negative potentials with no effect at positive potentials. When K _o was reduced, a negative slope appeared in the current-voltage (I-V) curve at positive potentials. We have investigated whether Na _i (intracellular Na) might also affect the voltage dependence of I _pby varying Na in the patch pipette (Na_pip) between 20 and 85 mM. We found, as expected, that I _pincreased markedly as Na_pip was raised, saturating at about 70 mM Na_pip under these conditions. In contast, while I _psaturated near +20 mV and declined to about 40% of maximum at –120 mV, there was no effect of Na_pip under these conditions. In contrast, while I _psaturated near +20 mV and declined to about 40% of maximum at –120 mV, there was no effect of Na_pip on the voltage dependence of I _p. This suggests that neither Na _i binding to the Na/K pump nor the conformational changes dependent on Na _i binding are voltage dependent. These results are consistent with extracellular ion binding within the field of the membrane but do not rule out the possibility that other steps, such as Na translocation, are also voltage dependent.We wish to thank Ms. Melinda Price, Ms. Meei Liu and Mr. Randall Anderson for their technical assistance. This work was supported in part by National Institutes of Health grant HL44660.     

Amiloride-blockable sodium currents in isolated taste receptor cells

Summary Isolated taste receptor cells from the frog tongue were investigated under whole-cell patch-clamp conditions. With the cytosolic potential head at –80 mV, more than 50% of the cells had a stationary inward Na current of 10 to 700 pA in Ringer's solution. This current was in some cells partially, in others completely, blockable by low concentrations of amiloride. With 110mm Na in the external and 10mm Na in the internal solution, the inhibition constant of amiloride was (at –80 mV) near 0.3 m. In some cells the amiloride-sensitive conductance was Na specific; in others it passed both Na and K. The Na/K selectivity (estimated from reversal potentials) varied between 1 and 100. The blockability bysmall concentrations of amiloride resembled that of channels found in some Na-absorbing epithelia, but the channels of taste cells showed a surprisingly large range of ionic specificities. Receptor cells, whichin situ express these channels in their apical membrane, may be competent to detect the taste quality salty. The same cells also express TTX-blockable voltage-gated Na channels.     

Voltage dependence of theChara proton pump revealed by current-voltage measurement during rapid metabolic blockade with cyanide

Summary It is generally agreed that solute transport across theChara plasma membrane is energized by a proton electrochemical gradient maintained by an H⁺-extruding ATPase. Nonetheless, as deduced from steady-state current-voltage (I-V) measurements, the kinetic and thermodynamic constraints on H⁺-ATPase function remain in dispute. Uncertainties necessarily surround long-term effects of the relatively nonspecific antagonists used in the past; but a second, and potentially more serious problem has sprung from the custom of subtracting, across the voltage spectrum, currents recorded following pump inhibition from currents measured in the control. This practice must fail to yield the trueI-V profile for the pump when treatments alter the thermodynamic pressure on transport.We have reviewed these issues, using rapid metabolic blockade with cyanide and fitting the resultant whole-cellI-V and difference-current-voltage (dI-V) relations to a reaction kinetic model for the pump and parallel, ensemble leak. Measurements were carried out after blocking excitation with LaCl₃, so that steady-state currents could be recorded under voltage clamp between –400 and +100 mV. Exposures to 1mm NaCN (CN) and 0.4mm salicylhydroxamic acid (SHAM) depolarized (positive-going)Chara membrane potentials by 44–112 mV with a mean half time of 5.4±0.8 sec (n=13). ATP contents, which were followed in parallel experiments, decayed coincidently with a mean half time of 5.3±0.9 sec ([ATP] _t=0, 0.74±0.3mm; [ATP] _t=x , 0.23±0.02mm). Current-voltage response to metabolic blockade was described quantitatively in context of these changes in ATP content and the consequent reduction in pump turnover rate accompanied by variable declines in ensemble leak conductance. Analyses ofdI-V curves (±CN+SHAM) as well as of families ofI-V curves taken at times during CN+SHAM exposures indicated a stoichiometry for the pump of one charge (H⁺) transported per ATP hydrolyzed and an equilibrium potential near –420 mV at neutral external pH; under these conditions, the pump accounted for approximately 60–75% of the total membrane conductance nearV _m. Complementary results were obtained also in fitting previously publishedI-V data gathered over the external pH range 4.5–7.5 Kinetic features deduced for the pump were dominated by a slow step preceding H⁺ unloading outside, and by recycling and loading steps on the inside which were in rapid equilibrium. These characteristics predict, in marked contrast to the situation forNeurospora, that cytoplasmic acid loads inChara should shift the pumpI-V curve negative-going along the voltage axis with little change in maximum current output at positive voltages.     

Voltage-dependent calcium and potassium conductances in striated muscle fibers from the scorpion,Centruroides sculpturatus

Ionic currents responsible for the action potential in scorpion muscle fibers were characterized using a three-intracellular microelectrode voltage clamp applied at the fiber ends (8–12°C). Large calcium currents (I _Ca) trigger contractile activation in physiological saline (5 mm Ca) but can be studied in the absence of contractile activation in a low Ca saline (2.5 mm). Barium (Ba) ions (1.5–3 mm) support inward current but not contractile activation.Ca conductance kinetics are fast (time constant of 3 msec at 0 mV) and very voltage dependent, with steady-state conductance increasing e-fold in approximately 4 mV. Half-activation occurs at –25 mV. Neither I _Ca nor I _Ba show rapid inactivation, but a slow, voltage-dependent inactivation eliminates I _Ca at voltages positive to –40 mV. Kinetically, scorpion channels are more similar to L-type Ca channels in vertebrate cardiac muscle than to those in skeletal muscle.Outward K currents turn on more slowly and with a longer delay than do Ca currents, and K conductance rises less steeply with voltage (e-fold change in 10 mV; half-maximal level at 0 mV). K channels are blocked by externally applied tetraethylammonium and 3,4 diaminopyridine.This work was supported by a grant from the NIH (NS-17510) to W.F.G. and a NRSA award to T.S. (GM-09921).     

Sialic acid and the surface charge associated with hyperpolarization-activated,inward rectifying channels

Summary The whole-cell configuration of the patch-clamp technique was used with cultured pacemaker cells from the rabbit sinoatrial node to test the hypothesis that sialic acid residues (NANA) constitute much of the negative surface charge associated with hyperpolarization-activated, inward rectifying channels. Activation-voltage relationships (between –70 and –140 mV) were determined for hyperpolarization-activated (inward rectifying) current (i _f). Addition of 10mm Ca²⁺ shifted the half-activation potential (V _1/2) from –89.5±0.9 mV to –77.9±2.6 mV (P<0.01), confirming the presence of negative fixed charges on the myocytes after 3 to 5 days in culture. Addition of 20mm dimethonium, an organic divalent cation that screens but does not bind to negative surface charge, shiftedV _1/2 from –86.8±1.4 mV to –75.0±1.7 mV (P<0.001) without affecting the amplitude of the current. In contrast, 10mm Ca²⁺ reduced the amplitude ofi _f significantly. Incubation of cells with a highly purified preparation of neuraminidase (0.1–2.0 U/ml, 1 hr, 37°C), an enzyme that selectively removes NANA from glycoproteins and glycolipids, failed to alterV _1/2 or the amplitude ofi _f significantly. Pretreatment of cells with neuraminidase (1.0 U/ml, 1 hr, 37°C) failed to alter the positive shift ofV _1/2 produced by dimethonium. The results suggest that NANA does not constitute the negative surface charge associated with hyperpolarization-activated, inward rectifying channels.