Fusion of cultured dog kidney (MDCK) cells: II. Relationship between cell pH and K+ conductance in response to aldosterone

Summary We have chosen the MDCK cell line to investigate aldosterone action on H⁺ transport and its role in regulating cell membrane K⁺ conductance (G _m ^K ). Cells grown in a monolayer respond to aldosterone indicated by the dose-dependent formation of domes and by the alkalinization of the dome fluid. The pH sensitivity of the plasma membrane K⁺ channels was tested in giant cells fused from individual MDCK cells. Cytoplasmic pH (pH _i ) andG _m ^K were measured simultaneously while the cell interior was acidified gradually by an extracellular acid load. We found a steep signoidal relationship between pH _i andG _m ^K (Hill coefficient 4.4±0.4), indicating multiple H⁺ binding sites at a single K⁺ channel. Application of aldosterone increased pH _i within 120 min from 7.22±0.04 to 7.45±0.02 and from 7.15±0.03 to 7.28±0.02 in the absence and presence of the CO₂/HCO ₃ ^– buffer system, respectively. We conclude that the hormone-induced cytoplasmic alkalinization in the presence of CO₂/ HCO ₃ ^– is limited by the increased activity of a pH _i -regulating HCO ₃ ^– extrusion system. SinceG _m ^K is stimulated half-maximally at the pH _i of 7.18±0.04, internal H⁺ ions could serve as an effective intracellular signal for the regulation of transepithelial K⁺ flux.     

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.     

Differential regulation of membrane potential and conductance via intra-and extracellular pH in fused proximal tubular cells of frog kidney

Intracellular pH (pH _i ), membrane potential (V _m ) and membrane conductance (G _m ) in fused proximal tubular cells of the frog kidney, were determined at three extracellular pH (pH _o ) values, 7.5, 8.5 and 6.5. Imposed changes of pH _o by ±1 pH unit induced parallel but smaller shifts of pH _i . The alkaline milieu hyperpolarized the cells and increased G _m , whereas the acid milieu depolarized and lowered G _m . We subsequently introduced a weak acid and its conjugate base (acetic acid/acetate), or a weak base and its conjugate acid (NH₃/NH ₄ ⁺ ), at pH _o 7.5, 8.5 and 6.5 to shift pH _i -without altering pH _o , or to shift pH _i against imposed changes of pH _o . From these experiments, we observed that under some circumstances V _m varied with pH _o but without G _m or pH _i changes, whereas under other circumstances changes of G _m occurred during alterations of pH _i while pH _o and V _m remained unaltered. At pH _i 6.5 associated with V _m –10 mV, G _m dramatically increased to quasi-infinite values. This increase was not an artifact since G _m returned to its control value following recovery to the control solution or in the presence of hyperosmotic solution. In conclusion, we demonstrate a differential regulation whereby V _m and G _m are controlled by pH _o and pH _i : pH _o modulates mainly V _m , and pH _i modulates chiefly G _m . Furthermore, at pH _i 6.5 and V _m –10 mV, our data reveal a large G _m that tends towards infinite values in a reversible fashion.     

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.     

Effects of pH and light on the membrane conductance measured in the acid and basic zones ofChara

Summary The area-specific coductance of the membrane in the acid and basic zones (denoted byG _A andG _B , respectively) ofChara cells was measured in flowing solutions, containing 5mm zwitterionic buffer, as a function of the external pH(denoted by pH⁰). During illuminationG _A was 1 S/m² for pH⁰ in the range 5 to 8.5, and increased markedly to 3 to 6 S/m² at higher pH₀.G _B , however, was always larger thanG _A during illumination with a typical magnitude of 5 to 15 S/m² for pH⁰ 6 to 12. Thus under many experimental conditions it is possible that there is no single correct value for the membrane area-specific conductance. A flow of current in the external medium between the acid and basic regions was found to be associated with pH banding, and also withG _B exceedingG _A . This current could be present in flowing solutions without added HCO ₃ ^– over a wide range of pH⁰ and at high (25mm) buffer concentration. Combining measurements ofG _A andG _B with measurements of the currents in the acid and basic zones (denoted byJ _A andJ _B , respectively), it was estimated that the resting (i.e. in the absence of net current flow) potential difference (PD) across the membranes within the individual zones (denoted byU _A andU _B ) was –265±20 and –183±5 mV, respectively, during illumination. Upon the removal of illumination at pH⁰-7.5,G _A ,G _B andJ _B were found to decrease rapidly during the initial few hundred seconds. During this period (U _B –V _m ) remained relatively constant. A transient hyperpolarization ofV _m often occurred, the magnitude of which was correlated with the magnitude ofJ _B prior to the removal of illumination. After some 0.5 to 1 ksec of darkness,G _A andG _B had both decreased considerably and nowG _A G _B andU _A U _B V _m . Eventually, after 2 to 8 ksec of darkness, the membrane conductance was effectively homogeneous with a much smaller magnitude (typically<0.2S/m²) andV _m was depolarized by typically 5 to 15 mV.     

Na+-independent,electrogenic Cl- uptake across the posterior gills of the Chinese crab (Eriocheir sinensis): Voltage-clamp and microelectrode studies

Summary Single gill lamellae from posterior gills of Chinese crabs (Eriocheir sinensis) were isolated, separated into halves and mounted in a modified Ussing chamber. Area-related short-circuit current (I_sc) and conductance (G_tot) of this preparation were measured. Epithelial cells were impaled with microelectrodes through the basolateral membrane and cellular potentials (V_i under open- and V_sc under short-circuit conditions) as well as the voltage divider ratios (F_i, F_o) were determined.With NaCl salines on both sides an outside positive PD_te (22±2 mV) and an I_sc (-64±13 A·cm^-2) with a polarity corresponding to an uptake of negative charges (inward negative) were obtained. Trough-like potential profiles were recorded across the preparation under open- as well as short-circuit conditions (V_o=-101±5 mV, external bath as reference; V_i=-78±2 mV, internal bath as reference; V_sc=-80±2 mV, extracellular space as reference). The voltage divider ratios of the external (apical membrane plus cuticle) and internal (basolateral membrane) barrier were F_o=0.92±0.01 and F_i=0.08±0.01, respectively. To investigate a Cl^--related contribution to the above parameters, Na⁺-free solutions in the external bath (basolateral NaCl-saline) were used. Inward negative I_sc under these conditions almost completely depended on external Cl^-. Elimination of Cl^- in the external bath reversed I_sc, and G_tot decreased substantially. Concomitantly, V_sc depolarised and F_o increased. Cl^--dependent current and conductance showed saturation kinetics with increasing external [Cl^-]. Addition of 20 mmol·1^-1 thiocyanate to the external bath had similar, although less pronounced, effects as Cl^- substitution. Equally, external SITS (1 mmol·1^-1) inhibited the current and, concomitantly, G_tot decreased substantially. Addition of 1 mmol·1^-1 acetazolamide to, and omission of NaHCO₃ from, the basolateral bath resulted in a decrease of I_sc while G_tot remained unchanged. The Cl^--channel blocker DPC inhibited I_sc almost completely when added to the basolateral saline, whereas G_tot decreased moderately; however, V_sc depolarised without significant change of F_i. Ouabain had no influence on I_sc and G_tot. Increasing the basolateral [K⁺] resulted in a decrease in I_sc, while G_tot was not affected. At the same time V_sc largely depolarised and F_i decreased. Addition of the K⁺-channel blocker Ba⁺⁺ (5 mmol·1^-1) to the basolateral solution resulted in a two-step alteration of the transepithelial (I_sc, Gtot) and cellular (V_sc, F_i) parameters. The results are discussed with regard to (i) the mechanisms responsible for active transbranchial Cl^- uptake, and (ii) the technical improvement of being able to perform transport studies with crab gill preparations in an Ussing chamber.Abbreviations DMSO dimethylsulfoxide - DPC diphenylamine-2-carboxylate - F _{o, i} voltage divider ratio for external (o) and internal (i) barrier, respectively - G _Cl conductance related to the external [Cl^-] - G _tot total tissue conductance - I _Cl short-circuit current related to the external [Cl^-] - I _sc short-circuit current - PD _te transepithelial potential difference - R _ME resistance of the microelectrode - SITS 4-acetamido-4-isothiocyanato-stilbene-2,2-disulfonic acid - V _{o, i} open-circuit voltage across the external (o) and internal (i) barrier, respectively - V _sc intracellular potential under short-circuit conditions     

Mechanisms of fusicoccin action: evidence for concerted modulations of secondary K+ transport in a higher plant cell

Fusicoccin (FC) has long been known to promote K⁺ uptake in higher plant cells, including stomatal guard cells, yet the precise mechanism behind this enhancement remains uncertain. Membrane hyperpolarization, thought to arise from primary H⁺ pumping stimulated in FC, could help drive K⁺ uptake, but the extent to which FC stimulates influx and uptake frequently exceeds any reasonable estimates from Constant Field Theory based on changes in the free-running membrane potential (V _m) alone; furthermore, unidirectional flux analyses have shown that in the toxin K⁺ (⁸⁶Rb⁺) exchange plummets to 10% of the control (G.M. Clint and E.A.C. MacRobbie 1984, J. Exp. Bot.35 180–192). Thus, the activities of specific pathways for K⁺ movement across the membrane could be modified in FC. We have explored a role for K⁺ channels in mediating these fluxes in guard cells ofVicia faba L. The correspondence between FC-induced changes in chemical (⁸⁶Rb⁺) flux and in electrical current under voltage clamp was followed, using the K⁺ channel blocker tetraethylammonium chloride (TEA) to probe tracer and charge movement through K⁺-selective channels. Parallel flux and electrical measurements were carried out when cells showed little evidence of primary pump activity, thus simplifying analyses. Under these conditions, outward-directed K⁺ channel current contributed appreciably to charge balance maintainingV _m, and adding 10 mM TEA to block the current depolarized (positive-going)V _m; TEA also reduced⁸⁶Rb⁺ efflux by 68–80%. Following treatments with 10 M FC, both K⁺ channel current and⁸⁶Rb⁺ efflux decayed, irreversbly and without apparent lag, to 10%–15% of the controls and with equivalent half-times (approx. 4 min). Fusicoccin also enhanced⁸⁶Rb⁺ influx by 13.9-fold, but the influx proved largely insensitive to TEA. Overall, FC promotednet cation uptake in 0.1 mM K⁺ (Rb⁺), despite membrane potentials which were 30–60 mVpositive of the K⁺ equilibrium potential. These results tentatively link (chemical) cation efflux to charge movement through the K⁺ channels. They offer evidence of an energy-coupled mechanism for K⁺ uptake in guard cells. Finally, the data reaffirm early suspicions that FC alters profoundly the K⁺ transport capacity of the cells, independent of any changes in membrane potential.Abbreviations and symbols E _K equilibrium potential for K⁺ - FC fusicoccin - Hepes 4-(2-hydroxyethyl)-1-piperazineeth-anesulfonic acid - G _m membrane (slope) conductance atV _m - I-V current-voltage (relationship) - apparent rate constant for exchange - K _i ⁺ , K ₀ ⁺ intracellular, extracellular K⁺ (concentration) - TEA tetraethylammonium chloride - V _m free-running membrane potential (difference)     

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.     

Inwardly rectifying potassium current in rabbit osteoclasts: A whole-cell and single-channel study

Summary Ionic conductances of rabbit osteoclasts were investigated using both whole-cell and cell-attached configurations of the patch-clamp recording technique. The predominant conductance found in these cells was an inwardly rectifying K⁺ conductance. Whole-cell currents showed an N-shaped current-voltage (I–13;V) relation with inward current activated at potentials negative to E_K. When external K⁺ was varied, I-V curves shifted 53 mV/10-fold change in [K⁺]_out, as predicted for a K⁺-selective channel. Inward current was blocked by Ba²⁺ and showed a time-dependent decline at negative potentials, which was reduced in Na⁺-free external solution. Inward single-channel currents were recorded in the cell-attached configuration. Single-channel currents were identified as inward-rectifier K⁺ channels based on the following observations: (i) Unitary I-V relations rectified, with only inward current resolved. (ii) Unitary conductance () was 31 pS when recorded in the cell-attached configuration with 140 mm K⁺ in the pipette and was found to be dependent on [K⁺]. (iii) Addition of Ba²⁺ to the pipette solution abolished single-channel events. We conclude that rabbit osteoclasts possess inwardly rectifying K⁺ channels which give rise to the inward current recorded at negative potentials in the whole-cell configuration. This inwardly rectifying K⁺ current may be responsible for setting the resting membrane potential and for dissipating electrical potential differences which arise from electrogenic transport of protons across the osteoclast ruffled border.This work was supported by The Arthritis Society and the Medical Research Council of Canada. M.E.M.K. was supported by a fellowship, S.J.D. a development Grant and S.M.S. a scholarship from the Medical Research Council. We thank Dr. Zu Gang Zheng for help with scanning microscopy.     

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.     

Basolateral K channel activated by carbachol in the epithelial cell line T84

Cholinergic stimulation of chloride secretion involves the activation of a basolateral membrane potassium conductance, which maintains the electrical gradient favoring apical Cl efflux and allows K to recycle at the basolateral membrane. We have used transepithelial short-circuit current (I _SC), fluorescence imaging, and patch clamp studies to identify and characterize the K channel that mediates this response in T₈₄ cells. Carbachol had little effect on I _SC when added alone but produced large, transient currents if added to monolayers prestimulated with cAMP. cAMP also enhanced the subsequent I _SC response to calcium ionophores. Carbachol (100 m) transiently elevated intracellular free calcium ([Ca²⁺] _i ) by 3-fold in confluent cells cultured on glass coverslips with a time course resembling the I _sc response of confluent monolayers that had been grown on porous supports. In parallel patch clamp experiments, carbachol activated an inwardly rectifying potassium channel on the basolateral aspect of polarized monolayers which had been dissected from porous culture supports. The same channel was transiently activated on the surface of subconfluent monolayers during stimulation by carbachol. Activation was more prolonged when cells were exposed to calcium ionophores. The conductance of the inward rectifier in cell-attached patches was 55 pS near the resting membrane potential (–54 mV) with pipette solution containing 150 mm KCl (37°C). This rectification persisted when patches were bathed in symmetrical 150 mm KCl solutions. The selectivity sequence was 1 K > 0.88 Rb > 0.18 Na Cs based on permeability ratios under bi-ionic conditions. The channel exhibited fast block by external sodium ions, was weakly inhibited by external TEA, was relatively insensitive to charybdotoxin, kaliotoxin, 4-aminopyridine and quinidine, and was unaffected by external 10 mm barium. It is referred to as the K_BIC channel based on its most distinctive properties (Ba-insensitive, inwardly rectifying, Ca-activated). Like single K_BIC channels, the carbachol-stimulated I _SC was relatively insensitive to several blockers on the basolateral side and was unaffected by barium. These comparisons between the properties of the macroscopic current and single channels suggest that the K_BIC channel mediates basolateral membrane K conductance in T₈₄ cell monolayers during stimulation by cholinergic secretagogues.We thank Dr. Marcel Crest (Laboratoire de Neurobiologie, CNRS, Marseille) for providing a sample of kaliotoxin. This work was supported by the Canadian Cystic Fibrosis Foundation and the Respiratory Health Network of Centres of Excellence. J.W.H. is a Chercheur-Boursier of the Fonds de la recherche en santé du Québec.     

Transport-dependent alterations of membrane properties of mammalian colon measured using impedance analysis

Summary Direct current (DC) measurement methods have been commonly used to characterize the conductance properties of the mammalian colon. However, these methods provide no information concerning the effects of tissue morphology on the electrophysiological properties of this epithelium. For example, distribution of membrane resistances along narrow fluid-filled spaces such as the lateral intercellular spaces (LIS) or colonic crypts can influence DC measurements of apical and basolateral membrane properties. We used impedance analysis to determine the extent of such distributed resistance effects and to assess the conductance and capacitance properties of the colon. Because capacitance is proportional to membrane area, this method provides new information concerning membrane areas and specific ionic conductances for these membranes.We measured transepithelial impedance under three conditions: (1) control conditions in which the epithelium was opencircuited and bathed on both sides with NaCl–HCO₃ Ringer's solutions, (2) amiloride conditions which were similar to control except that 100 m amiloride was present in the mucosal bathing solution, and (3) mucosal NaCl-free conditions in which mucosal Na and Cl were replaced by potassium and sulfate or gluconate (K⁺ Ringer's). Three morphologically-based equivalent circuit models were used to evaluate the data: (1) a lumped model (which ignores LIS resistance), (2) a LIS distributed model (distributed basolateral membrane impedance) and (3) a crypt-distributed model (distributed apical membrane impedance). To estimate membrane impedances, an independent measurement of paracellular conductance (G _s ) was incorporated in the analysis. Although distributed models yielded improved fits of the data, the distributed and lumped models produced similar estimates of membrane parameters. The predicted effects of distributed resistances on DC microelectrode measurements were largest for the LIS-distributed model. LIS-distributed effects would cause a 12–15% underestimate of membrane resistance ratio (R _a /R _b ) for the control and amiloride conditions and a 34% underestimate for the K Ringer's condition. Distributed resistance effects arising from the crypts would produce a 1–2% overestimate ofR _a /R _b .Apical and basolateral membrane impedances differed in the three different experimental conditions. For control conditions, apical membrane capacitance averaged 21 F/cm² and the mean apical membrane specific conductance (G _a-norm) was 0.17 mS/F. The average basolateral membrane capacitance was 11 F/cm² with a mean specific conductance (G _b-norm) of 1.27 mS/F.G _a-norm was decreased by amiloride or K⁺ ringer's to 0.07 mS/gmF and 0.06 mS/F, respectively. Basolateral conductance was also reduced by amiloride, whereas capacitance was unchanged (G _b-norm=0.97 mS/F). For the K⁺ Ringer's condition, both basolateral conductance and capacitance were greatly increased such thatG _b-norm was not significantly different from the control condition.     

Ca2+-activated K+ conductance of human red cell membranes exhibits two different types of voltage dependence

Summary The voltage dependence for outward-going current of the Ca-activated K⁺ conductance (g _k (Ca)) of the human red cell membrane has been examined over a wide range of membrane potentials (V _m) at constant values of [K⁺]_ex, [K⁺]_c and pH_c, the intact cells being preloaded to different concentrations of ionized calcium. Outward-current conductances were calculated from initial net effluxes of K⁺ and the corresponding (V _m-E_k) values. The basic conductance, defined as the outward-current coductance at (V _m-E_k) 20 mV and [K⁺]_ex 3mM (B. Vestergaard-Bogind, P. Stampe and P. Christophersen,J. Membrane Biol. 95:121–130, 1987) was found to be a function of cellular ionized Ca. At all degrees of Ca activationg _K(Ca) was an apparently linear function of voltage (V _m range –40 to +70 mV), the absolute level as well as the slope decreasing with decreasing activation. In a simple two-state model the constant voltage dependence can, at the different degrees of Ca activation, be accounted for by a Boltzmann-type equilibrium function with an equivalent valence of 0.4, assuming chemical equilibrium atV _m=0 mV. Alternatively, the phenomenon might be explained by a voltage-dependent block of the outward current by an intracellular ion. Superimposed upon the basic conductance is the apparently independent inward-rectifying steep voltage function with an equivalent valence of 5 and chemical equilibrium at the givenE _K value.Abbreviations CCCP carbonyl cyanidem-chlorophenylhydrazone - DIDS 4,4-diisothiocyanostilbene-2,2-disul     

Identification and functional reconstitution of phosphate: Sugar phosphate antiport ofStaphylococcus aureus

Summary Resting cells ofStaphylococcus aureus displayed a phosphate (P_i) exchange that was induced by growth with glucose 6-phosphate (G6P) orsn-glycerol 3-phosphate (G3P). P_i-loaded membrane vesicles from these cells accumulated³²P_i, 2-deoxyglucose 6-phosphate (2DG6P) or G3P by an electroneutral exchange that required no external source of energy. On the other hand, when vesicles were loaded with morpholinopropane sulfonic acid (MOPS), only transport of³²P_i (andl-histidine) was observed, and in that case transport depended on addition of an oxidizable substrate (dl-lactate). In such MOPS-loaded vesicles, accumulation of the organic phosphates, 2DG6P and G3P, could not be observed until vesicles were preincubated with both P_i anddl-lactate to establish an internal pool of P_i. Thistrans effect demonstrates that movement of 2DG6P or G3P is based on an antiport (exchange) with internal P_i.Reconstitution of membrane protein allowed a quantitative analysis of P_i-linked exchange. P_i-loaded proteoliposomes and membrane vesicles had comparable activities for the homologous³²P_iP_i exchange (K _i's of 2.2 and 1.4mm;V _max's of 180 and 83 nmol P_i/min per mg protein), indicating that the exchange reaction was recovered intact in the artificial system. Other work showed that heterologous exchange from either G6P- or G3P-grown cells had a preference for 2DG6P (K _i=27 m) over G3P (K _i=1.3mm) and P_i (K _i=2.2mm), suggesting that the same antiporter was induced in both cases. We conclude that³²P_iP_i exchange exhibited by resting cells reflects operation of an antiporter with high specificity for sugar 6-phosphate. In this respect, P_i-linked antiport inS. aureus resembles other examples in a newly described family of bacterial transporters that use anion exchange as the molecular basis of solute transport.     

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.     

Properties of the phosphate and phosphite transport systems of Phytophthora palmivora

Germlings of Phytophthora palmivora possess at least two systems for the uptake of inorganic phosphate (P_i). The first is synthesized on germination in medium containing 50 M P_i and has a K_m of approx. 30 M (V_max=7–9 nmol P_i/h·10⁶ cells). The second is synthesized under conditions of P_i-deprivation and has a higher affinity for P_i (K_m=1–2 M), but a lower V_max (0.5–2 nmol P_i/h·10⁶ cells). The fungicide phosphite likewise enters the germlings via two different transport systems, the synthesis of which also depends on the concentration of P_i in the medium. The K_m of the lower affinity system is 3 mM (V_max=20 nmol phosphite/h·10⁶ cells) and that of the higher affinity system is 0.6 mM (V_max=12 nmol/h·10⁶ cells). P_i and phosphite are competitive inhibitors for each other's transport in both systems. However, whereas mM concentrations of phosphite are necessary to inhibit P_i transport, only M concentrations of P_i are required to inhibit phosphite transport. A third system of uptake for P_i also exists, since when phosphate-deprived cells are presented with mM concentrations of P_i, they transport the anion at a very high rate (around 100 nmol/h·10⁶ cells). High rates of transport of phosphite are also observed when these cells are presented with mM concentrations of this anion.     

ATP-inhibited and Ca2+-dependent K+ channels in the soma membrane of cultured leech Retzius neurons

The properties of one ATP-inhibited and one Ca²⁺-dependent K⁺ channel were investigated by the patch-clamp technique in the soma membrane of leech Retzius neurons in primary culture. Both channels rectify at negative potentials. The ATP-inhibited K⁺ channel with a mean conductance of 112 pS is reversibly blocked by ATP (K _i = 100 m), TEA (K _i =0.8 mm) and 10 mm Ba²⁺ and irreversibly blocked by 10 nm glibenclamide and 10 m tolbutamide. It is Ca²⁺ and voltage independent. Its open state probability (P _o) decreases significantly when the pH at the cytoplasmic face of inside-out patches is altered from physiological to acid pH values. The Ca²⁺-dependent K⁺ channel with a mean conductance of 114 pS shows a bell-shaped Ca²⁺ dependence of P _o with a maximum at pCa 7–8 at the cytoplasmic face of the membrane. The P _o is voltage independent at the physiologically relevant V range. Ba²⁺ (10 mm) reduces the single channel amplitude by around 25% (ATP, TEA, glibenclamide, tolbutamide, and Ba²⁺ were applied to the cytoplasmic face of the membrane).We conclude that the ATP-dependent K⁺ channel may play a role in maintaining the membrane potential constant—independently from the energy state of the cell. The Ca²⁺-dependent K⁺ channel may play a role in generating the resting membrane potential of leech Retzius neurons as it shows maximum activity at the physiological intracellular Ca²⁺ concentration.This study was supported by the Deutsche Forschungsgemeinschaft (W.-R. Schlue) and by a fellowship of the Konrad-Adenauer-Stiftung (G. Frey). We thank Dr. Draeger (Hoechst AG) for the gift of glibenclamide. The data are part of a future Ph.D. thesis of G. Frey.     

Electrogenic properties of the cloned Na+/glucose cotransporter: II. A transport model under nonrapid equilibrium conditions

Summary The results of the accompanying electrophysiological study of the cloned Na⁺/glucose cotransporter from small intestine (Parent, L., Supplisson, S., Loo, D.D.F., Wright, E.M. (1992) J. Membrane Biol. 125:49–62) were evaluated in terms of a kinetic model. The steady-state and presteady-state cotransporter properties are described by a 6-state ordered kinetic model (mirror symmetry) with a Na⁺:MDG stoichiometry of 2. Carrier translocation in the membrane as well as Na⁺ and sugar binding and dissociation are treated as a function of their individual rate constants. Empty carrier translocation and Na⁺ binding/ dissociation are the only steps considered to be voltage dependent. Currents were associated with the translocation of the negatively charged carrier in the membrane. Negative membrane potential facilitates sugar transport. One numerical solution was found for the 14 rate constants that account quantitatively for our experiment observations: i.e., (i) sigmoidal shape of the sugar-specific current-voltage curves (absence of outward currents and inward current saturation at high negative potentials), (ii) Na⁺ and voltage dependence of K _0.5 ^sugar and i _max ^sugar , (iii) sugar and voltage dependence of K _0.5 ^Na and i _max ^Na , (iv) presteady-state currents and their dependence on external Na⁺, MDG and membrane potential, and (v) and carrier Na⁺ leak current. We conclude that the main voltage effect is on carrier translocation. Na⁺ ions that migrate from the extracellular medium to their binding sites sense 25 to 35% of the transmembrane voltage, whereas charges associated with the carrier translocation experiences 60 to 75% of the membrane electrical field. Internal Na⁺ ion binding is not voltage dependent. In our nonrapid equilibrium model, the rate-limiting step for sugar transport is a function of the membrane potential, [Na]₀ and [MDG]₀. At 0 mV and at saturating [Na]₀ and [MDG]₀, the rate-limiting step for sugar transport is the empty carrier translocation (5 sec^–1). As the membrane potential is made more negative, the empty carrier translocation gets faster and the internal Na⁺ dissociation becomes increasingly rate limiting. However, as [Na]₀ is decreased to less than 10 mm, the rate-limiting step is the external Na⁺ ions binding in the 0 to –150 mV potential range. At 0 mV, the external Na⁺ dissociation constant KNa is 80 mm and decreases to 24 mm at –150 mV. The external sugar dissociation constant KNaS is estimated to be 200 m and voltage independent. Finally, the internal leak pathway (CNa₂ translocation) is insignificant. While we cannot rule out a more complex kinetic model, the electrical properties of the cloned Na⁺/glucose cotransporter are found to be adequately described by this 6-state kinetic model.We are grateful to Drs. A. Berteloot, S. Ciani, and J.-Y. Lapointe for stimulating discussions and thank our colleagues for comments. L.P. was recipient of a post-doctoral fellowship from the Medical Research Council of Canada. This work was supported by a grant from the U.S. Public Health Service DK 19567.     

Electrical characteristics of stomatal guard cells: The ionic basis of the membrane potential and the consequence of potassium chlorides leakage from microelectrodes

The membrane electrical characteristics of stomatal guard cells in epidermal strips from Vicia faba L. and Commelina communis L. were explored using conventional electrophysiological methods, but with double-barrelled microelectrodes containing dilute electrolyte solutions. When electrodes were filled with the customary 1–3 M KCl solutions, membrane potentials and resistances were low, typically decaying over 2–5 min to near-30 mV and <0.2 k·cm² in cells bathed in 0.1 mM KCl and 1 mM Ca²⁺, pH 7.4. By contrast, cells impaled with electrodes containing 50 or 200 mM K⁺-acetate gave values of-182±7 mV and 16±2 k·cm² (input resistances 0.8–3.1 G, n=54). Potentials as high as (-) 282 mV (inside negative) were recorded, and impalement were held for up to 2 h without appreciable decline in either membrane parameter. Comparison of results obtained with several electrolytes indicated that Cl^- leakage from the microelectrode was primarily responsible for the decline in potential and resistance recorded with the molar KCl electrolytes. Guard cells loaded with salt from the electrodes also acquired marked potential and conductance responses to external Ca²⁺, which are tentatively ascribed to a K⁺ conductance (channel) at the guard cell plasma membrane.Measurements using dilute K⁺-acetate-filled electrodes revealed, in the guard cells, electrical properties common to plant and fungal cell membranes. The cells showed a high selectivity for K⁺ over Na⁺ (permeability ratio P_Na/P_K=0.006) and a near-Nernstian potential response to external pH over the range 4.5–7.4 (apparent P_H/P_K=500–600). Little response to external Ca²⁺ was observed, and the cells were virtually insensitive to CO₂. These results are discussed in the context of primary, charge-carrying transport at the guard cell plasma membrane, and with reference to possible mechanisms for K⁺ transport during stomatal movements. They discount previous notions of Ca²⁺-and CO₂-mediated transport control. It is argued, also, that passive (diffusional) mechanisms are unlikely to contribute to K⁺ uptake during stomatal opening, despite membrane potentials which, under certain, well-defined conditions, lie negative of the potassium equilibrium potential likely prevailing.Abbreviations and symbols EGTA ethylene glycol-bis(-aminoethyl ether)-N,N,N,N-tetraacetic acid - Hepes 4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid - Mes 2-(N-morpholino) propanesulfornic acid - E equilibrium potential - G_m membrane conductance - R_in input resistance - V_m membrane potential     

Membrane potential,anion and cation conductances in Ehrlich ascites tumor cell

Summary The fluorescence intensity of the dye 1,1-dipropyloxadicarbocyanine (DiOC₃-(5)) has been measured in suspensions of Ehrlich ascites tumor cells in an attempt to monitor their membrane potential (V _m ) under different ionic conditions, after treatment with cation ionophores and after hypotonic cell swelling. Calibration is performed with gramicidin in Na⁺-free K⁺/choline⁺ media, i.e., standard medium in which NaCl is replaced by KCl and cholineCl and where the sum of potassium and choline is kept constant at 155mm. Calibration by the valinomycin null point procedure described by Lariset al. (Laris, P.C., Pershadsingh, A., Johnstone, R.M., 1976,Biochim. Biophys. Acta 436:475–488) is shown to be valid only in the presence of the Cl^–-channel blocker indacrinone (MK196). Distribution of the lipophilic anion SCN^– as an indirect estimation of the membrane potential is found not to be applicable for the fast changes inV _m reported in this paper. Incubation with DiOC₃-(5) for 5 min is demenstrated to reduce the Cl^– permeability by 26±5% and the NO ₃ ^– permeability by 15±2%, while no significant effect of the probe could be demonstrated on the K⁺ permeability. Values forV _m , corrected for the inhibitory effect of the dye on the anion conductance, are estimated at –61±1 mV in isotonic standard NaCl medium, –78±3 mV in isotonic Na⁺-free choline medium and –46±1 mV in isotonic NaNO₃ medium. The cell membrane is depolarized by addition of the K⁺ channel inhibitor quinine and it is hyperpolarized when the cells are suspended in Na⁺-free choline medium, indicating thatV _m is generated partly by potassium and partly by sodium diffusion. Ehrlich cells have previously been shown to be more permeable to nitrate than to chloride. Substituting NO ₃ ^– for all cellular and extracellular Cl^– leads to a depolarization of the membrane, demonstrating thatV _m is also generated by the anions and that anions are above equilibrium. Taking the previously demonstrated single-file behavior of the K⁺ channels into consideration, the membrane conductances in Ehrlich cells are estimated at 10.4 S/cm² for K⁺, 3.0 S/cm² for Na⁺, 0.6 S/cm² for Cl^– and 8.7 S/cm² for NO ₃ ^– . Addition of the Ca²⁺-ionophore A23187 results in net loss of KCl and a hyperpolarization of the membrane, indicating that the K⁺ permeability exceeds the Cl^– permeability also after the addition of A23187. The K⁺ and Cl^– conductances in A23187-treated Ehrlich cells are estimated at 134 and 30 S/cm², respectively. The membrane potential is depolarized in hypotonically swollen cells, confirming that the increase in the Cl^– permeability following hypotonic exposure exceeds the concommitant increase in the K⁺ permeability. In control experiments where the membrane potentialV _m =E _K =E _Cl =E _Na , it is demonstrated that cell volume changes has no significant effect on the fluorescence signal, apparently because of a large intracellular buffering capacity. The increase in the Cl^– conductances is 68-fold when cells are transferred to a medium with half the osmolarity of the standard medium, as estimated from the net Cl^– efflux and the change inV _m . The concommitant increase in the K⁺ conductance, as estimated from the net K⁺ efflux, is only twofold.