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.     

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.     

Whole-cell and single-channel currents across the plasmalemma of corn shoot suspension cells

Summary Whole-cell sealed-on pipettes have been used to measure electrical properties of the plasmalemma surrounding protoplasts isolated from Black Mexican sweet corn shoot cells from suspension culture. In these protoplasts the membrane resting potential (V _m ) was found to be –59±23 mV (n=23) in 1mm K _o ^– . The meanV _m became more negative as [K^–] _o decreased, but was more positive than the K⁺ equilibrium potential. There was no evidence of electrogenic pump activity. We describe four features of the current-voltage characteristic of the plasmalemma of these protoplasts which show voltagegated channel activity. Depolarization of the whole-cell membrane from the resting potential activates time- and voltage-dependent outward current through K⁺-selective channels. A local minimum in the outward current-voltage curve nearV _m =150 mV suggests that these currents are mediated by two populations of K⁺-selective channels. The absence of this minimum in the presence of verapamil suggests that the activation of one channel population depends on the influx of Ca²⁺ into the cytoplasm. We identify unitary currents from two K⁺-selective channel populations (40 and 125 pS) which open when the membrane is depolarized; it is possible that these mediate the outward whole-cell current. Hyperpolarization of the membrane from the resting potential produces time- and voltage-dependent inward whole-cell current. Current activation is fast and follows an exponential time course. The current saturates and in some cases decreases at membrane potentials more negative than –175 mV. This current is conducted by poorly selective K⁺ channels, whereP _Cl/P _K=0.43±0.15. We describe a low conductance (20 pS) channel population of unknown selectivity which opens when the membrane is hyperpolarized. It is possible that these channels mediate inward whole-cell current. When the membrane is hyperpolarized to potentials more negative than –250 mV large, irregular inward current is activated. A third type of inward whole-cell current is briefly described. This activates slowly and with a U-shaped current-voltage curve over the range of membrane potentials –90<V _m <0 mV.     

Microelectrode characterization of the basolateral membrane of rabbit S3 proximal tubule

Summary The purpose of this study was to characterize the basolateral membrane of the S3 segment of the rabbit proximal tubule using conventional and ion-selective microelectrodes. When compared with results from S1 and S2 segments, S3 cells under control conditions have a more negative basolateral membrane potential (V _bl=–69 mV), a higher relative potassium conductance (t _K=0.6), lower intracellular Na⁺ activity (A _Na=18.4mm), and higher intracellular K⁺ activity (A _K=67.8mm). No evidence for a conductive sodium-dependent or sodium-independent HCO ₃ ^– pathway could be demonstrated. The basolateral Na–K pump is inhibited by 10^–4 m ouabain and bath perfusion with a potassium-free (0-K) solution. 0-K perfusion results inA _Na=64.8mm,A _K=18.5mm, andV _bl=–28 mV. Basolateral potassium channels are blocked by barium and by acidification of the bathing medium. The relative K⁺ conductance, as evaluated by increasing bath K⁺ to 17mm, is dependent upon the restingV _bl in both S2 and S3 cells. In summary, the basolateral membrane of S3 cells contains a pump-leak system with similar properties to S1 and S2 proximal tubule cells. The absence of conductive bicarbonate pathways results in a hyperpolarized cell and larger Na⁺ and K⁺ gradients across the cell borders, which will influence the transport properties and intracellular ion activities in this tubule segment.     

Transport Systems of Ventricaria ventricosa: I/V Analysis of Both Membranes in Series as a Function of [K+] o

The current-voltage (I/V) profiles of Ventricaria (formerly Valonia) membranes were measured at a range of external potassium concentrations, [K⁺] _o , from 0.1 to 100 mm. The conductance-voltage (G/V) characteristics were computed to facilitate better resolution of the profile change with time after exposure to different [K⁺] _o . The resistance-voltage (R/V) characteristics were computed to attempt resolution of plasmalemma and tonoplast. Four basic electrophysiological stages emerged: (1) Uniform low resistance between −60 and +60 mV after the cell impalement. (2) High resistance between +50 and +150 for [K⁺] _o from 0.1 to 1.0 mm and hypotonic media. (3) High resistance between −150 and −20 mV for [K⁺] _o of 10 mm (close to natural seawater) and hypertonic media. (4) High resistance between −150 and +170 mV at [K⁺] _o of 100 mm. The changes between these states were slow, requiring minutes to hours and sometimes exhibiting spontaneous oscillations of the membrane p.d. (potential difference). Our analysis of the I/V data supports a previous hypothesis, that Ventricaria tonoplast is the more resistive membrane containing a pump, which transports K⁺ into the vacuole to regulate turgor. We associate state (1) with the plasmalemma conductance being dominant and the K⁺ pump at the tonoplast short-circuited probably by a K⁺ channel, state (2) with the K⁺ pump ``off' or short-circuited at p.d.s more negative than +50 mV, state (3) with the K<sup>+</sup> pump ``on,' and state (4) with the pump dominant, but affected by high K⁺. A model for the Ventricaria membrane system is proposed. Received: 5 November 1998/Revised: 11 May 1999     

The relationship between ATP and an electrogenic pump in the plasma membrane ofNeurospora crassa

Summary Sudden respiratory blockade has been used to study rapid changes of the resting membrane potential, of intracellular adenosine 5-triphosphate (ATP) levels, and of pyridine nucleotide reduction inNeurospora crassa. Membrane depolarization occurs with a first-order rate constant of 0.167 sec^–1, following a lag period of about 4 sec, at 24°C (ambient temperature). This depolarization is several-fold too slow to be directly linked to electron transfer, as judged from the rate of pyridine nucleotide reduction, but has essentially the same rate constant as the decay of ATP. The latter process, however, shows no lag period after the respiratory inhibitor is introduced. Plots of membrane potential versus the intracellular ATP concentration yield saturation curves which are readily fitted by a Michaelis equation, to which is added a constant term representing the diffusion component of membrane potential. Parameters obtained from such fits indicate the maximal voltage which the pump can develop at high ATP levels to be 300 to 350 mV, with an apparentK _1/2 of 2.0mm. The data strongly suggest that an electrogenic ion pump in the plasma membrane ofNeurospora is fueled by ATP; comparison of the measured membrane potentials with the energy available from hydrolysis of ATP indicates that two ions could be pumped for each molecule of ATP split.     

Analog circuit of theAcetabularia membrane

Summary The high membrane potential ofAcetabularia (E _m=–170 mV) is due to an electrogenic pump in parallel with the passive diffusion system (E _d=–80 mV) which could be studied separately in the cold, when the pump is blocked. Electrical measurements under normal conditions show that the pump pathway consists of its electromotive forceE _p with two elementsP ₁ andP ₂ in series;P ₂ is shunted by a large capacitance (C _p=3 mF cm^–2). The nonlinear current-voltage relationship ofP ₁ (light- and temperature-sensitive) could be determined separately; it reflects the properties of a carrier-mediated electrogenic pump. The value ofE _p (–190 mV) indicates a stoichiometry of 21 between electrogenically transported charges and ATP. The electrical energy, normally stored inC _p, compares well with the metabolic energy, stored in the ATP pool. The nonlinear current-voltage relationship ofP ₂ (attributed to phosphorylating reactions) is also sensitive to light and temperature and is responsible for the region of negative conductance of the overall current-voltage relationship. The power of the pump (1 W cm^–2) amounts to some percent of the total energy turnover. The high Cl^– fluxes (1 nmol cm^–2 sec^–1) and the electrical properties of the plasmalemma are not as closely related as assumed previously. For kinetic reasons, a direct and specific Cl^– pathway between the vacuole and outside is postulated to exist.     

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.     

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.     

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.     

Implications of an anomalous intracellular electrical response in bullfrog corneal epithelium

Summary The ionic dependencies of the transepithelial and intracellular electrical parameters were measured in the isolated frog cornea. In NaCl Ringer's the intracellular potential differenceV _sc measured under short-circuit conditions depolarized by nearly the same amount after either increasing the stromal-side KCl concentration from 2.5 to 25mm or exposure to 2mm BaCl₂ (K⁺ channel blocker). With Ba²⁺ the depolarization of theV _sc by 25mm K⁺ was reduced to one-quarter of the control change. If the Cl-permselective apical membrane resistanceR _o remained unchanged, the relative basolateral membrane resistanceR _i, which includes the lateral intercellular space, increased at the most by less than twofold after Ba²⁺. These effects in conjunction with the depolarization of theV _sc by 62 mV after increasing the stromal-side K⁺ from 2.5 to 100mm in Cl-free Ringer's as well as the increase of the apparent ratio of membrane resistances (a=R _o/R_i) from 13 to 32 are all indicative of an appreciable basolateral membrane K⁺ conductance. This ratio decreased significantly after exposure to either 25mm K⁺ or Ba²⁺. The decline ofR _o/R_i with 25mm K⁺ appears to be anomalous since this decrease is not consistent with just an increase of basolateral membrane conductance by 25mm K⁺, but rather perhaps a larger decrease ofR _o thanR _iAlso an increase of lateral space resistance may offset the effect of decreasingR _i with 25mm K⁺. In contrast,R _o/R_i did transiently increase during voltage clamping of the apical membrane potential differenceV _o and exposure to 25mm K⁺ on the stromal side. This increase and subsequent decrease ofR _o/R_i supports the idea that increases in stromal K⁺ concentration may produce secondary membrane resistance changes. These effects onR _o/R_i show that the presence of asymmetric ionic conductance properties in the apical and basolateral membranes can limit the interpretative value of this parameter. The complete substitution of Na⁺ withn-methyl-glucamine in Cl-free Ringer's on the stromal side hyperpolarized theV _sc by 6 mV whereas 10^–4 m ouabain depolarized theV _sc by 7 mV. Thus the basolateral membrane contains K⁺, Na⁺ and perhaps Cl^– pathways in parallel with the Na/K pump component.     

Ca2+-activated K+ channels in the apical membrane ofNecturus choroid plexus

Summary The properties of Ca²⁺-activated K⁺ channels in the apical membrane of theNecturus choroid plexus were studied using single-channel recording techniques in the cell-attached and excised-patch configurations. Channels with large unitary conductances clustered around 150 and 220 pS were most commonly observed. These channels exhibited a high selectivity for K⁺ over Na⁺ and K⁺ over Cs⁺. They were blocked by high cytoplasmic Na⁺ concentrations (110mm). Channel activity increased with depolarizing membrane potentials, and with increasing cytoplasmic Ca²⁺ concentrations. Increasing Ca²⁺ from 5 to 500nm, increased open probability by an order of magnitude, without changing single-channel conductance. Open probability increased up to 10-fold with a 20-mV depolarization when Ca²⁺ was 500nm. Lowering intracellular pH one unit, decreased open probability by more than two orders of magnitude, but pH did not affect single-channel conductance. Cytoplasmic Ba²⁺ reduced both channel-open probability and conductance. The sites for the action of Ba²⁺ are located at a distance more than halfway through the applied electric field from the inside of the membrane. Values of 0.013 and 117mm were calculated as the apparent Ba²⁺ dissociation constants (K _d (0 mV) for the effects on probability and conductance, respectively. TEA⁺ (tetraethylammonium) reduced single-channel current. Applied to the cytoplasmic side, it acted on a site 20% of the distance through the membrane, with aK _d (0 mV)=5.6mm. A second site, with a higher affinity,K _d (0 mV)=0.23mm, may account for the near total block of chanel conductance by 2mm TEA⁺ applied to the outside of the membrane. It is concluded that the channels inNecturus choroid plexus exhibit many of the properties of maxi Ca²⁺-activated K⁺ channels found in other tissues.     

High-conductance K+ channel in pancreatic islet cells can be activated and inactivated by internal calcium

Summary The Ca²⁺-activated K⁺ channel in rat pancreatic islet cells has been studied using patch-clamp single-channel current recording in excised inside-out and outside-out membrane patches. In membrane patches exposed to quasi-physiological cation gradients (Na⁺ outside, K⁺ inside) large outward current steps were observed when the membrane was depolarized. The single-channel current voltage (I/V) relationship showed outward rectification and the null potential was more negative than –40 mV. In symmetrical K⁺-rich solutions the single-channelI/V relationship was linear, the null potential was 0 mV and the singlechannel conductance was about 250 pS. Membrane depolarization evoked channel opening also when the inside of the membrane was exposed to a Ca²⁺-free solution containing 2mm EGTA, but large positive membrane potentials (70 to 80 mV) were required in order to obtain open-state probabilities (P) above 0.1. Raising the free Ca²⁺ concentration in contact with the membrane inside ([Ca²⁺]_i) to 1.5×10^–7 m had little effect on the relationship between membrane potential andP. When [Ca²⁺]_i was increased to 3×10^–7 m and 6×10^–7 m smaller potential changes were required to open the channels. Increasing [Ca²⁺]_i further to 8×10^–7 m again activated the channels, but the relationship between membrane potential andP was complex. Changing the membrane potential from –50 mV to +20 mV increasedP from near 0 to 0.6 but further polarization to +50 mV decreasedP to about 0.2. The pattern of voltage activation and inactivation was even more pronounced at [Ca²⁺]_i=1 and 2 m. In this situation a membrane potential change from –70 to +20 mV increasedP from near 0 to about 0.7 but further polarization to +80 mV reducedP to less than 0.1. The high-conductance K⁺ channel in rat pancreatic islet cells is remarkably sensitive to changes in [Ca²⁺]_i within the range 0.1 to 1 m which suggests a physiological role for this channel in regulating the membrane potential and Ca²⁺ influx through voltage-activated Ca²⁺ channels.     

Voltage dependence of Na/K pump current inXenopus oocytes

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

Chloride channels in human platelets: Evidence for activation by internal calcium

Summary Whole-cell patch-clamp recordings were made from freshly isolated human platelets. The pipette contained a high concentration of divalent cations, which permitted easy disruption of cell-attached membrane patches by suction. Single-channel currents were measured when the pipette contained isotonic BaCl₂ or MgCl₂ saline; over 30 sec –5 min an increasing number of channels appeared until conductance steps through individual channels could no longer be distinguished. The current-voltage relationship was curvilinear; chord conductance at –35 mV was 25 pS increasing to 45 to 52 pS at +45 mV. Ion substitution experiments showed the current to be primarily carried by Cl^–.E _rev was shifted 30 mV/10-fold change in external Cl^– (replaced by gluconate), was similar with BaCl₂ or MgCl₂ in the pipette and was not significantly shifted by replacing external Na⁺ with K⁺. Addition of 1mm BAPTA to the MgCl₂ pipette saline prevented activation of Cl^– currents; with isotonic CaCl₂ internal saline, current appeared immediately upon patch rupture, suggesting that the Cl^– channels are dependent on internal Ca²⁺, 5-nitro-2-(3-phenylpropylamino)-benzoate, reported to block a Cl^– conductance in studies of rat epithelial cells, caused a potent flickery block and may be a useful tool with which to investigate the physiological role of Cl^– currents in human platelets.     

Analysis and use of the perforated patch technique for recording ionic currents in pancreaticβ-cells

Summary To investigate the voltage dependence of the Na^–/K^– pump, current-voltage relations were determined in prophasearrested oocytes ofXenopus laevis. All solutions contained 5mm Ba^2– and 20mm tetraethylammonium (TEA) to block K^– channels. If. in addition, the Na⁺/K⁺ pump is blocked by ouabain, K⁺-sensitive currents no larger than 50 nA/cm² remain. Reductions in steady-state current (on the order of 700 nA/cm²) produced by 50 m ouabain or dihydro-ouabain or by K⁺ removal, therefore, primarily represent current generated by the Na^–/K^– pump. In Na^–-free solution containing 5mm K⁺, Na⁺/K⁺ pump current is relatively voltage independent over the potential range from –160 to +40 mV. If external [K⁺] is reduced below 0.5mm, negative slopes are observed over this entire voltage range. Similar results are seen in Na⁺- and Ca²⁺-free solutions in the presence of 2mm Ni²⁺, an experimental condition designed to prevent Na⁺/Ca²⁺ exchange. The occurrence of a negative slope can be explained by the voltage dependence of the apparent affinity for activation of the Na⁺/K⁺ pump by external K⁺, consistent with the existence of an external ion well for K^– binding. In 90mm Na⁺, 5mm K⁺ solution, Na⁺/K⁺ pump current-voltage curves at negative membrane potentials have a positive slope and can be described by a monotonically increasing sigmoidal function. At an extracellular [K⁺] of 1.3mm, a negative slope was observed at positive potentials. These findings suggest that in addition to a voltage-dependent step associated with Na⁺ translocation, a second voltage-dependent step that is dependent on external [K⁺], possibly external K⁺ binding, participates in the overall reaction mechanism of the Na⁺/K⁺ pump.     

Ca2+-activated K+ conductance of the human red cell membrane: Voltage-dependent Na+ block of outward-going currents

Summary Human red cells were prepared with various cellular Na⁺ and K⁺ concentrations at a constant sum of 156mm. At maximal activation of the K⁺ conductance,g _K(Ca), the net efflux of K⁺ was determined as a function of the cellular Na⁺ and K⁺ concentrations and the membrane potential,V _m , at a fixed [K⁺]_ex of 3.5mm.V _m was only varied from (V _m –E _K)25 mV and upwards, that is, outside the range of potentials with a steep inward rectifying voltage dependence (Stampe & Vestergaard-Bogind, 1988).g _K(Ca) as a function of cellular Na⁺ and K⁺ concentrations atV _m =–40, 0 and 40 mV indicated a competitive, voltage-dependent block of the outward current conductance by cellular Na⁺. Since the present Ca²⁺-activated K⁺ channels have been shown to be of the multi-ion type, the experimental data from each set of Na⁺ and K⁺ concentrations were fitted separately to a Boltzmann-type equation, assuming that the outward current conductance in the absence of cellular Na⁺ is independent of voltage. The equivalent valence determined in this way was a function of the cellular Na⁺ concentration increasing from 0.5 to 1.5 as this concentration increased from 11 to 101mm. Data from a previous study of voltage dependence as a function of the degree of Ca²⁺ activation of the channel could be accounted for in this way as well. It is therefore suggested that the voltage dependence ofg _K(Ca) for outward currents at (V _m –E _K)>25 25 mV reflects a voltage-dependent Na⁺ block of the Ca²⁺-activated K⁺ channels.     

Ca2+-activated K+ currents inNecturus choroid plexus

Summary The tight-seal whole-cell recording method has been used to studyNecturus choroid plexus epithelium. A cell potential of –59±2 mV and a whole cell resistance of 56±6 M were measured using this technique. Application of depolarizing step potentials activated voltage-dependent outward currents that developed with time. For example, when the cell was bathed in 110mm NaCl Ringer solution and the interior of the cell contained a solution of 110mm KCl and 5nm Ca²⁺, stepping the membrane potential from a holding value of –50 to –10 mV evoked outward currents which, after a delay of greater than 50 msec, increased to a steady state in 500 msec. The voltage dependence of the delayed currents suggests that they may be currents through Ca²⁺-activated K^_ channels. Based on the voltage dependence of the activation of Ca²⁺-activated K⁺ channels, we have devised a general method to isolate the delayed currents. The delayed currents were highly selective for K⁺ as their reversal potential at different K⁺ concentration gradients followed the Nernst potential for K⁺. These currents were reduced by the addition of TEA⁺ to the bath solution and were eliminated when Cs⁺ or Na⁺ replaced intracellular K⁺. Increasing the membrane potential to more positive values decreased both the delay and the half-times (t _1/2) to the steady value. Increasing the pipette Ca²⁺ also decreased the delay and decreasedt _1/2. For instance, when pipette Ca²⁺ was increased from 5 to 500nm, the delay andt _1/2 decreased from values greater than 50 and 150 msec to values less than 10 and 50 msec. We conclude that the delayed currents are K⁺ currents through Ca²⁺-activated K⁺ channels.At the resting membrane potential of –60 mV, Ca²⁺-activated K⁺ channels contribute between 13 to 25% of the total conductance of the cell. The contribution of these channels to cell conductance nearly doubles with membrane depolarization of 20–30 mV. Such depolarizations have been observed when cerebrospinal fluid (CSF) secretion is stimulated by cAMP and with intracellular Ca²⁺. Thus the Ca²⁺-activated K⁺ channels may play a specific role in maintaining intracellular K⁺ concentrations during CSF secretion.     

Intracellular chloride and potassium ions in relation to excitability ofChara membrane

Summary Internodal cells ofChara australis were made tonoplast-free by replacing the cell sap with EGTA-containing media; then the involvement of internal Cl^– and K⁺ in the excitation of the plasmalemma was studied.[Cl^–] _i was drastically decreased by perfusing the cell interior twice with a medium lacking Cl^–. The lowered [Cl^–] _i was about 0.01mm. Cells with this low [Cl^–] _i generated action potential and showed anN-shapedV–I curve under voltage clamped depolarization like Cl^–-rich cells containing 13 or 29mm Cl^–.E _m at the peak of the action potential was constant at [Cl^–] _i between 0.01 and 29mm. The possibility that the plasmalemma becomes as permeable to other anions as to Cl^– during excitation is discussed.At [Cl^–] _i higher than 48mm, cells were inexcitable. When anions were added to the perfusion medium to bring the K⁺ concentration to 100mm, NO ₃ ^– , F^–, SO ₄ ^2– , acetate, and propionate inhibited the generation of action potentials like Cl^–, while methane sulfonate, PIPES, and phosphate did not inhibit excitability.The duration of the action potential depended strongly on the intracellular K⁺ concentration. It decreased as [K⁺] _i (K-methane sulfonate) increased. Increase in [Na⁺] _i (Na-methane sulfonate) also caused its decrease, although this effect was weaker than that of K⁺. The action of these monovalent cations on the duration of the action potential is the opposite of their action on the membrane from the outside (cf. Shimmen, Kikuyama & Tazawa, 1976,J. Membrane Biol. 30:249).     

Intracellular potassium activity and the role of potassium in transepithelial salt transport in the human reabsorptive sweat duct

Summary We have measured the intracellular potassium activity, [K⁺]_i and the mechanisms of transcellular K⁺ transport in reabsorptive sweat duct (RSD) using intracellular ion-sensitive microelectrodes (ISMEs). The mean value of [K⁺]_i in RSD is 79.8±4.1mm (n=39). Under conditions of microperfusion, the [K⁺]_i is above equilibrium across both the basolateral membrane, BLM (5.5 times) and the apical membrane, APM (7.8 times). The Na⁺/K⁺ pump inhibitor ouabain reduced [K⁺]_i towards passive distribution across the BLM. However, the [K⁺]_i is insensitive to the Na⁺/K⁺/2 Cl^– cotransport inhibitor bumetanide in the bath. Cl^– substitution in the lumen had no effect on [K⁺]_i. In contrast, Cl^– substitution in the bath (basolateral side) depolarized BLM from –26.0±2.6 mV to –4.7^*±2.4 mV (n=3;^* indicates significant difference) and decreased [K⁺]_i from 76.0±15.2mm to 57.7^* ±12.7mm (n=3). Removal of K⁺ in the bath decreased [K⁺]_i from 76.3±15.0mm to 32.3^*±7.6mm (n=4) while depolarizing the BLM from –32.5±4.1 mV to –28.3^*±3.0 mV (n=4). Raising the [K⁺] in the bath by 10-fold increased [K⁺]_i from 81.7±9.0mm to 95.0^*±13.5mm and depolarized the BLM from –25.7±2.4 mV to –21.3^*±2.9 mV (n=4). The K⁺ conductance inhibitor, Ba²⁺, in the bath also increased [K⁺]_i from 85.8±6.7mm to 107.0^*±11.5mm (n=4) and depolarized BLM from –25.8±2.2 mV to –17.0^*±3.1 mV (n=4). Amiloride at 10^–6 m increased [K⁺]_i from 77.5±18.8mm to 98.8^*±21.6mm (n=4) and hyperpolarized both the BLM (from –35.5±2.6 mV to –47.8^*±4.3 mV) and the APM (from –27.5±1.4 mV to –46.0^* ±3.5 mV,n=4). However, amiloride at 10^–4 m decreased [K⁺]_i from 64.5±0.9mm to 36.0^*±9.9mm and hyperpolarized both the BLM (from –24.7±1.4 mV to –43.5^*±4.2 mV) and APM (from –18.3±0.9 mV to –43.5^*±4.2 mV,n=6). In contrast to the observations at the BLM, substitution of K⁺ or application of Ba²⁺ in the lumen had no effect on the [K⁺]_i or the electrical properties of RSD, indicating the absence of a K⁺ conductance in the APM. Our results indicate that (i) [K⁺]_i is above equilibrium due to the Na⁺/K⁺ pump; (ii) only the BLM has a K⁺ conductance; (iii) [K⁺]_i is subject to modulation by transport status; (iv) K⁺ is probably not involved in carrier-mediated ion transport across the cell membranes; and (v) the RSD does not secrete K⁺ into the lumen.