Ouabain on active transepithelial sodium transport in frog skin: studies with microelectrodes

Studies were done with isolated frog skin to determine the effects of 10(-4) M ouabain on the electrophysiological parameters of outer and inner barriers of the Na-transporting cells. Microelectrodes were used to impale the skins from the outer surface to determine the intracellular voltages (Vsco) under conditions of short-circuiting and under conditions where a voltage clamp was used to vary the transepithelial voltage, VT. From this, the electrical resistances of outer (Rfo) and inner (RI) barriers were estimated. In addition, the driving force for active transepithelial Na transport (ENa = E'1) was estimated from the values of VT when the Vo = 0 mV (Helman and Fisher. 1977. J. Gen. Physiol. 69: 571-604). Studies were done with skins bathed with the usual 2.4 meq/liter [K]i in the inner solution as well as with reduced [K]i of 0.5 and 0 meq/liter. Characteristically, the responses to ouabain could be described by an initial rapid phase (5-10 min) during which time the Ri was increased markedly and the E'1 was decreased from control values. Thereafter, during the slow phases of the response, the resistances of both outer and inner barriers increased continuously and markedly with time leading ultimately to essentially complete inhibition of the short-circuit current. Similar studies were done with skins exposed to 10(-4) M amiloride in the outer solution. Although estimates of Ri could not be obtained under these conditions, the effects on the Vsco and E'1 were similar to those observed for the Na-transporting skins. However, the magnitudes of the effects were less and relatively slower than observed for the Na-transporting skins. The results of these studies were analyzed within the context of a proposed electrical model that takes into account the observation that the magnitude of the voltage at the inner barrier appears to exceed the equilibrium potential for K especially when transepithelial Na transport is inhibited at the apical barrier of the cells.     

Electrochemical potentials in frog skin: inferences for electrical and mechanistic models

To evaluate possible mechanisms of transport at apical and basolateral barriers of Na transporting cells of epithelia, it is necessary to know the difference of electrochemical potentials at each barrier. A reevaluation in light of new data of intracellular voltages of frog skin leads to fundamental questions concerning the origin of the voltages at both inner and outer barriers of this tissue. Whereas the inner barrier is highly selective for K, confirming the observations of Koefoed-Johnsen and Ussing, the voltage across the inner barrier, Vi, especially in the absence of transepithelial Na transport, may be greater than the Nernst equilibrium potential for K estimated from the maximum values of intracellular [K] reported in the literature. Consequently, it is proposed that the Na:K pumps may, under some conditions, behave not only as a Na:K exchange pump but also as a cation extrusion pump for K especially when intracellular [Na] falls to low levels. In order to explain the relationship between Na entry and the voltage at the outer barrier, it is proposed that the conductance of the outer barrier is voltage dependent, in line with previous observations of the nonlinear electrical behavior of the apical barrier of Na transporting cells. Thus, the outer barrier may behave as a simple voltage independent resistor with a Thévenin electromotive force of zero at negative intracellular voltages despite the existence of a chemical potential for Na at this barrier.     

Intracellular voltage of isolated epithelia of frog skin: apical and basolateral cell punctures

Isolated epithelia of frog skin were prepared with collagenase, and the cells were punctured with intracellular microelectrodes across their apical (outer) and basolateral (inner) surfaces. Regardless of the route of cell puncture, the intracellular voltage (Vosc) in short- circuited isolated epithelia was markedly negative, averaging -70.4 mV for apical punctures and -91.6 mV for basolateral punctures. As in intact epithelia, amiloride outside caused the Vosc to become more negative (means of -96.7 and -101.8 mV), with a concomitant increase in the resistance of the apical barrier. Increasing the [K)i of the basolateral solution from 2.4 to 8.0 or 14.4 mM caused rapid step depolarization (5-10 s) of the Vosc under transepithelial Na transporting and amiloride-inhibited conditions of Na transport, with the delta Vosc ranging between 23.9 and 68.3 mV per decade change of [K]i. The finding that the Vosc of isolated epithelia of frog skin is independent of the route of cell penetration is consistent with the notion that the cells of the stratified epithelium are electrically coupled (functional syncitium). Moreover, the isolated epithelium can serve as a useful preparation, especially in studies designed to investigate the properties of the basolateral surfaces of cells.     

Microelectrode studies of the effect of lanthanum on the electrical potential and resistance of outer and inner cell membranes of isolated frog skin

Microelectrodes were used to investigate the effect of 0.5 mM mucosal lanthanum (La3+) on the intracellular potential and the resistance of outer and inner isolated frog skin (Rana esculenta) cell membranes. Under short-circuit conditions, the transapical membrane potential Vsco (mean value = -65.4 +/- 3.2 mV, inside negative) hyperpolarized to -108.7 +/- 2.3 mV in control skins, after addition of the sodium blocker amiloride. Current-voltage curves for the outer and inner membranes were constructed from the amiloride-inhibitable current versus the outer membrane potential Vo or the inner membrane potential Vi. The outer, and to a lesser degree the inner, membrane showed a characteristic nonlinearity with two slope resistances. Addition of La3+ to the outer medium increased the short-circuit current to 190% of the control value. Vsco concomitantly changed to -28 +/- 3.5 mV and outer and inner membrane resistances fell, considerably attenuating the nonlinearity seen in control skins. La3+ is suggested to raise the conductance by its effect on the surface potential. A secondary long-term inhibitory effect of La3+ on short-circuit current has been observed. It is ascribed to the penetration of La3+ into the sodium channels.     

Potential dependence of unidirectional chloride fluxes across isolated frog skin

Isolated frog skins were voltage clamped at transepithelial potentials (Vt) ranging from -60 mV to 60 mV to measure transepithelial 36Cl- fluxes from the apical to the basolateral bathing solution (J13) and in the opposite direction (J31). The potential dependence of fluxes obtained in Na+-free choline Ringer's indicates the presence of conductive and nonconductive components that probably correspond to fluxes through paracellular and cellular pathways, respectively. Rectification of fluxes with reversal of the potential reflects a structural asymmetry, presumably in surface charge density. The data are consistent with a charge density of one negative charge per 280 A2 on the apical side. A new model for passive Cl- transport was developed that includes surface charge asymmetry and specifically accounts for the observed variation of conductance with potential. In normal frog Ringer's, J13 was larger than J31 at zero potential (active Cl- transport), J13 rose exponentially with increasing positive potential to reach a maximum at 40 mV (approximately open-circuit), and the predicted partial Cl- conductance exceeded the measured conductance leading to the conclusion that when J13 is largely driven by Na+ transport, much of the coupling occurs via nonconductive pathways. Theophylline stimulates Cl- transport that also occurs via nonconductive pathways as Vt becomes more positive.     

Effects of antidiuretic hormone upon electrical potential and resistance of apical and basolateral membranes of frog skin

Summary The effect of ADH upon the intracellular potential and the resistance of inner and outer borders of the transport pathway was investigated on isolated skins ofRana temporaria. Within 40 min after ADH (100-300 mU/ml), the intracellular potential under short-circuit conditions decreased to about 40% of the control value (–79±4 mV), concomitant with an increase in the short-circuit current to about 160% of the control value. Amiloride, applied when steady values under ADH had been reached, caused an immediate rise of the intracellular potential to values typical for control conditions. This confirms (i) the intracellular location of the microelectrode and the absence of impalement artifacts, and (ii) the ineffectiveness of ADH upon the electromotive forces of the inner border. ADH had no effect upon the intracellular potential after blockage of the Na entry by Amiloride. The equilibrium potential of the outer border was estimated to be about +20 mV under the influence of ADH. As this value is considerably less positive than might be expected for the chemical potential of Na, a significant contribution of ions other than Na to the outer border conductance and equilibrium potential is implicated. The resistance of the outer border was more significantly decreased than that of the active transcellular pathway after ADH due to an increase in the inner border resistance, which exceeded that of the outer border after ADH. The effect of ADH upon the outer membrane characteristics would be underestimated by a factor of two, if the alterations of the electrical potential difference were not taken into consideration.     

Current-voltage relations of the apical and basolateral membranes of the frog skin

We determined the current-voltage (I-V) relations of the apical and basolateral barriers of frog skins by impaling the cells with an intracellular microelectrode and assuming that the current across the cellular pathway was equal to the amiloride-inhibitable current. We found that: (a) The responses in transepithelial current and intracellular potential to square pulses of transepithelial potential (VT) varied markedly with time. (b) As a consequence of these transient responses, the basolateral I-V relation was markedly dependent on the time of sampling after the beginning of each pulse. The apical I-V plot was much less sensitive to the time of sampling within the pulse. (c) The I-V data for the apical barrier approximated the I-V relations calculated from the Goldman constant field equation over a relatively wide range of membrane potentials (+/- 100 mV). (d) A sudden reduction in apical bath [Na+] resulted in an increase in apical permeability and a shift in the apical barrier zero-current potential (Ea) toward less positive values. The shift in Ea was equivalent to a change of 45 mV for a 10-fold change in apical [Na+]. (e) The transient responses of the skin to square VT pulses were described by the sum of two exponentials with time constants of 114 and 1,563 ms, which are compatible with the time constants that would be produced by an RC circuit with capacitances of 65 and 1,718 microF. The larger capacitance is too large to identify it comfortably with a true dielectric membrane capacitance.     

Membrane responses to large hyperpolarizations in trabecles and single cells of frog atrium

Atrial trabeculae (studied in voltage-clamping conditions and in the presence of 0.5 mmol/l BaCl2 to abolish gK1) responded to 1 s hyperpolarizations to beyond approximately E = -140 mV (from HP of about E = -80 mV) with an inwardly directed current increasing with time. Quite similar results were obtained with enzymatically dissociated frog atrial cells studied in whole cell voltage clamp with a patch-clamp pipette. This behaviour could be accounted for by assuming the presence of an "if" current at this quite negative range of potentials or by the fact that the cell membrane may undergo reversible electropermeabilization when its potential is brought to values negative to about -140 mV (St?mpfli 1958). When a brief (1 ms) and large (150 mV) hyperpolarization was applied 1 s before the test pulse, an inwardly directed current increasing with time was elicited by test pulses to beyond approximately E = -120 mV. This current was neither abolished in the presence of 1 mmol/l CsCl nor greatly reduced in the absence of Na+ ions, unlike "if" (Di Francesco 1981). We conclude that this current having a time course similar to that of "if" is of different nature and we argue that it might be accounted for by electropermeabilization of the membrane (reversible within about 2.5 min) due to the electrical shock represented by a brief and large hyperpolarization.     

Action Potential in the Trap-lobes of Aldrovanda vesiculosa

The trap of Aldrovanda vesiculosa, an aquatic insectivorousplant, consists of a pair of lobes (trap-lobes) which bordereach other at the midrib. The central portion of the lobe iscomposed of three cell layers, an inner and outer epidermisenclosing a single middle layer of relatively large cells, whereasthe marginal portion consists only of the two epidermal celllayers. Intracellular potentials of these cells were measuredby the microelectrode technique. All the cells of the lobeswere excitable and had identical membrane potentials at rest( –110 mV) and during action (amplitude, 130 mV). Theaction potential of each cell was elicited by bending a sensoryhair, one of many standing on the inner surface of the centralportion, or by injecting an outward current into another cellin the lobe. Action potentials were propagated throughout thetrap-lobes at a rate of about 8 cm/sec. The maximum rising ratewas 2.7 V/sec and the duration of the action potential was 1sec. (Received August 8, 1981; Accepted October 15, 1981)     

Voltage-clamp of cut-end skeletal muscle fibre: a diffusion experiment

Membrane potential and current were studied in cut end fibres of frog skeletal muscle under current and voltage clamp conditions, by the double sucrose gap technique. Similar action potentials were recorded under current clamp conditions with either the microelectrode or the double sucrose gap techniques. Under voltage clamp conditions, the control of the membrane potential was maintained adequately. The early current was sensitive to both TTX and external Na concentration suggesting that the current was carried by Na ions. Sodium current (INa) was subsequently analysed using the Hodgkin-Huxley formulae. INa half-activation and inactivation occurred at -34 mV and -60 mV, respectively. Na-rich solution applied internally by diffusion through cut ends produced a reduction of INa associated with a shift of the sodium current reversal potential (VNa) towards more negative membrane potentials. This suggested that the sodium electromotive force was reduced by the increase in internal Na content of the fibre. Iodate applied externally changed neither the activation nor the inactivation time courses of INa, but reduced the peak current. Conversely, internally applied by diffusion from the cut end of skeletal muscle fibre, iodate slowed down the time course of INa inactivation and decreased the current peak. In conclusion, the double sucrose gap technique adapted to cut end frog skeletal muscle fibre allows a satisfactory analysis of INa.     

A study of the "outward potassium channel" (OPC) in the frog oocyte. I. A study of the "cell-attached" configuration

A single channel current was studied in the membrane of the immature oocyte of the european frog (Rana esculenta) by using the "patch clamp" technique in the "cell attached" configuration. Single channel activity appeared as short outward currents when membrane potential was made positive inside; full activation required seconds to be complete, no inactivation being appreciable. Deactivation (or current block) upon membrane repolarization was so fast that no inward current could be detected in any case. The reversal potential, estimated by interpolating the I/V diagrams, was -30 mV using standard Ringer as electrode filling solution, and the elementary conductance was 95 pS. Neither reversal potential nor elementary conductance were affected by removal of external Ca2+ (Mg2+ or Ba2+ substitution) or external Cl- (methanesulphonate substitution). The reversal potential moved towards positive potentials by substituting external Na+ with K+, the magnitude of the shifts being consistent with a ratio PK/PNa = 6.4. A distinctive property of the current/voltage relation for this K-current is its anomalous bell-shape, the outward current displaying a maximum at membrane potentials around 75 mV with standard Ringer as electrode filling solution and tending to zero with more positive potentials.     

Binding of [3H]ouabain to split frog skin: the role of the Na,K-ATPase in the generation of short circuit current

The binding of [3H]ouabain to the serosal side was studied in a chambered preparation of frog skin, free of connective tissue, while the short circuit (Isc) was concurrently monitored. Both ouabain binding and Isc inhibition proceeded as hyperbolic functions of time. A plot of the number of ouabain molecules bound vs. the corresponding values of Isc inhibition (percent) yielded a straight line, yet showed that one-third of the binding occurred before any inhibition of Isc. Upon separation of the skins into two groups based upon initial Isc(Isci)--high, greater than 20 microamperemeter/cm2 and low, less than 10 microamperemeter/cm2, we observed two distinct populations. The high Isci skins bound very little ouabain before inhibition of Isc whereas low Isci skins bound one-half of the total number of sites before exhibiting any inhibition of Isc. These observations strongly suggest that (a) the Na,K-ATPase is directly involved in the generation of Isc, and (b) at low Isc, inhibition of some pumps by ouabain causes a "recruitment" of other pumps to increase their turnover rate and maintain Isc relatively unaffected. In addition, the binding of ouabain also displayed various characteristics that were consistent with known properties of the Na,K-ATPase: (a) increased intracellular K/Na concentrations, whether achieved through the addition of amiloride or removal of Na from the outside medium, led to a significant decrease in ouabain binding rate relative to paired controls; and (b) ouabain binding, either with normal or decreased intracellular Na, was significantly reduced in the presence of elevated K in the serosal bathing medium. Finally, the number of ouabain molecules bound to the frog skins was not correlated with their initial Isc values, indicating that the spontaneous skin-to-skin variation in Isc was not related to the number of functional pump sites but, rather, to their turnover rate.     

Some kinetic and steady-state properties of sodium channels after removal of inactivation

To study the kinetic and steady-state properties of voltage-dependent sodium conductance activation, squid giant axons were perfused internally with either pronase or N-bromoacetamide and voltage clamped. Parameters of activation, tau m and gNa(V), and deactivation, tau Na, were measured and compared with those obtained from control axons under the assumption that gNa oc m3h of the Hodgkin-Huxley scheme. tau m(V) values obtained from the turn-on of INa agree well with control axons and previous determinations by others. tau Na(V) values derived from Na tail currents were also unchanged by pronase treatment and matched fairly well previously published values. tau m(V) obtained from 3 x tau Na(V) were much larger than tau m(V) obtained from INa turn-on at the same potentials, resulting in a discontinuous distribution. Steady-state In (gNa/gNa max - gNa) vs. voltage was not linear and had a limiting logarithmic slope of 5.3 mV/e-fold gNa. Voltage step procedures that induce a second turn-on of INa during various stages of the deactivation (Na tail current) process reveal quasiexponential activation at early stages that becomes increasingly sigmoid as deactivation progresses. For moderate depolarizations, primary and secondary activation kinetics are superimposable. These data suggest that, although m3 can describe the shape of INa turn-on, it cannot quantitatively account for the kinetics of gNa after repolarization. Kinetic schemes for gNa in which substantial deactivation occurs by a unique pathway between conducting and resting states are shown to be unlikely. It appears that the rate-limiting step in linear kinetic models of activation may be between a terminal conducting state and the adjacent nonconducting intermediate.     

Altered sodium and gating current kinetics in frog skeletal muscle caused by low external pH

The effect of low pH on the kinetics of Na channel ionic and gating currents was studied in frog skeletal muscle fibers. Lowering external pH from 7.4 to 5.0 slows the time course of Na current consistent with about a +25-mV shift in the voltage dependence of activation and inactivation time constants. Similar shifts in voltage dependence adequately describe the effects of low pH on the tail current time constant (+23.3 mV) and the gating charge vs. voltage relationship (+22.1 mV). A significantly smaller shift of +13.3 mV described the effect of pH 5.0 solution on the voltage dependence of steady state inactivation. Changes in the time course of gating current at low pH were complex and could not be described as a shift in voltage dependence. tau g, the time constant that describes the time course of the major component of gating charge movement, was slowed in pH 5.0 solution by a factor of approximately 3.5 for potentials from -60 to +45 mV. We conclude that the effects of low pH on Na channel gating cannot be attributed simply to a change in surface potential. Therefore, although it may be appropriate to describe the effect of low pH on some Na channel kinetic properties as a "shift" in voltage dependence, it is not appropriate to interpret such shifts as a measure of changes in surface potential. The maximum gating charge elicited from a holding potential of -150 mV was little affected by low pH.(ABSTRACT TRUNCATED AT 250 WORDS)     

Saxitoxin blocks batrachotoxin-modified sodium channels in the node of Ranvier in a voltage-dependent manner.

The inhibition by saxitoxin (STX) of single Na channels incorporated into planar lipid bilayers and modified by batrachotoxin (BTX) previously has been shown to be voltage dependent (Krueger, B.K.,J.F. Worley, and R. J. French, 1983, Nature [Lond.], 303:172-175; Moczydlowski, E., S. Hall, S. S. Garber, G. S. Strichartz, and C. Miller, 1984, J. Gen. Physiol., 84:687-704). We tested for such a voltage dependence of STX block of the Na current in voltage-clamped frog nodes of Ranvier. The block by STX of normal Na channels showed no modulation in response to maintained (20 s) changes of the membrane potential or to a train of brief pulses to potentials more positive than the holding potential. However, when the nodal channels were modified by BTX, the train of pulses produced a modulation of the block of the Na current by STX. The modulation of STX block depended on the voltage of the conditioning pulses and this voltage dependence agreed well with that predicted from the single channel studies over the membrane potential range used in those studies. In addition, we found that the voltage dependence of STX block was manifest only at potentials equal to or more positive than required to activate the channels. Most of the apparent differences among data from single channels in bilayers, equilibrium binding studies of STX, and the experiments described here are resolved by the hypotheses that (a) STX binding to open channels is voltage dependent, and (b) the affinities of STX for closed and inactivated channels are independent of voltage, equal, and less than the open channel affinity at potentials less than 0 mV. Whether these hypotheses apply to the STX block of all Na channels or just of BTX-modified channels remains to be determined.     

Effects of membrane surface charge and calcium on the gating of rat brain sodium channels in planar bilayers [published erratum appears in J Gen Physiol 1989 Apr;93(4):following 760]

The voltage-dependent gating of single, batrachotoxin-activated Na channels from rat brain was studied in planar lipid bilayers composed of negatively charged or neutral phospholipids. The relationship between the probability of finding the Na channel in the open state and the membrane potential (Po vs. Vm) was determined in symmetrical NaCl, both in the absence of free Ca2+ and after the addition of Ca2+ to the extracellular side of the channel, the intracellular side, or both. In the absence of Ca2+, neither the midpoint (V0.5) of the Po vs. Vm relation, nor the steepness of the gating curve, was affected by the charge on the bilayer lipid. The addition of 7.5 mM Ca2+ to the external side caused a depolarizing shift in V0.5. This depolarizing shift was approximately 17 mV in neutral bilayers and approximately 25 mV in negatively charged bilayers. The addition of the same concentration of Ca2+ to only the intracellular side caused hyperpolarizing shifts in V0.5 of approximately 7 mV (neutral bilayers) and approximately 14 mV (negatively charged bilayers). The symmetrical addition of Ca2+ caused a small depolarizing shift in Po vs. Vm. We conclude that: (a) the Na channel protein possesses negatively charged groups on both its inner and outer surfaces. Charges on both surfaces affect channel gating but those on the outer surface exert a stronger influence. (b) Negative surface charges on the membrane phospholipid are close enough to the channel's gating machinery to substantially affect its operation. Charges on the inner and outer surfaces of the membrane lipid affect gating symmetrically. (c) Effects on steady-state Na channel activation are consistent with a simple superposition of contributions to the local electrostatic potential from charges on the channel protein and the membrane lipid.     

Localization of Na+-pump sites in frog skin

The localization of Na+-pump sites (Na+-K+-ATPase) in the frog skin epithelium was determined by a freeze-dry radioautographic method for identifying [3H]ouabain-binding sites. Ventral pelvic skins of Rana catesbeiana were mounted in Ussing chambers and exposed to 10(-6) M [3H]ouabain for 120 min, washed in ouabain-free Ringer's solution for 60 min, and then processed for radioautography. Ouabain-binding sites were localized on the inward facing (serosal) membranes of all the living cells. Quantitative analysis of grain distribution showed that the overwhelming majority of Na+-pump sites were localized deep to the outer living cell layer, i.e., in the stratum spinosum and stratum germinativum. Binding of ouabain was correlated with inhibition of Na+ transport. Specificity of ouabain binding to Na+-K+-ATPase was verified by demonstrating its sensitivity to the concentration of ligands (K+, ATP) that affect binding of ouabain to the enzyme. Additional studies supported the conclusion that the distribution of bound ouabain reflects the distribution of those pumps involved in the active transepithelial transport of Na+. After a 30-min exposure to [3H]ouabain, Na+ transport declined to a level that was significantly less than that in untreated paired controls, and analysis of grain distribution showed that over 90% of the ouabain-binding sites were localized to the inner cell layers. Furthermore, in skins where Na+ transport had been completely inhibited by exposure to 10(-5) M ouabain, the grain distribution was identical to that in skins exposed to 10(-6) M. The results support a model which depicts all the living cell layers functioning as a syncytium with regard to the active transepithelial transport of Na+.     

Effect of oxytocin on the electrical potential and ion permeability of the apical membrane of frog gall bladder epithelial cells

The influence of oxytocin on the intracellular Na+ and K+ concentrations, the level of transmembrane potential differences, and on the relative ionic permeability (PNa/PK) of the apical zones of the superficial epithelium membrane was studied in experiments on the isolated frog gallbladder (GB). Oxytocine introduced into the outer incubation solution in a dose of 20 mulliunits/ml caused a reduction of transmembrane potential difference, and an increase of PNa/pk coefficient and an insignificant shift of the Na+ and K+ concentrations in the intracellular medium. Thirty minutes after the oxytocine action of the organ the membrane potential (MP) of the cells decreased from 52.7 mV to 38.7 mV (the cell is negatively charged inside), and PNa/PK increased from 0,083 (control) to 0,175 (test) with a simultaneous increase in the intracellular Na+ concentration by 18.3 milliequiv./kg of (H2O)i. Such a shift in the intracellular Na+ and K+ concentrations may cause a decrease of the MP by only--0.7 mV, but actually the membrane potential decreased by--14.0 mV. Thus, the reduction of the transmembrane potential difference results from increase of PNa/PK under the influence of oxytocine. No electrogenic ionic transport through the apical membrane of frog gallbladder epithelial cells was revealed.     

A study of the "outward potassium channel" (OPC) in the frog oocyte. II. A study of the "inside-out" configuration

The single K-channel current reported in a previous note was also studied in "outside-out" conditions. The electrode filling solutions used for the "cell-attached" experiments faced in this case the intracellular side of the membrane patches, the extracellular side facing the bath saline, i.e. Ringer standard. The most significant observations were obtained with filling solutions with varying proportions in K/Na concentrations solutions. In the absence of Na+ ([K+] = 110 mM), the elementary conductance was still around 90 pS and the I/V diagram was again somewhat bell shaped, though the distinctive reduction of the elementary conductance began at more positive potentials (+110 mV). No inward current could be detected upon membrane repolarization also in this case. The rectification became less evident and conductance increased with increasing Na+ concentration in the filling solution, until the I/V curve became a linear one and conductance was 270 pS with standard Ringer. Distinct inward elementary currents were evident upon repolarization in these conditions. Thus a complex interaction between Na+ and K+ takes place for conduction through the outward K channel in the frog oocyte, both cations probably competing for at least one active site inside. Another interesting observation concerns the process of gating of the OPC: the open times of the elementary currents were in fact much greater in outside out experiments as compared to cell-attached experiments, probably due to the presence of Ca++ in contact with the inner membrane side. Even increasing Na+ concentration prolonged the open time duration. The gating of the OPC in the membrane was not only voltage dependent, but also Ca++ and Na+ dependent.     

A glutamine to glutamate mutation at position 170 (Q170E) in the rabbit Na+/glucose cotransporter, rSGLT1, enhances binding affinity for Na+

Using cysteine mutagenesis and chemical modification by methanethiosulfonate derivatives, it was demonstrated that the external putative loop, joining transmembrane segments (TM's) IV-V of rabbit Na+/glucose cotransporter, rSGLT1, forms part of a Na+ binding and voltage sensing domain. Within this region, exposure to cationic (2-aminoethyl)methanethiosulfonate hydrobromide (MTSEA) inhibited F163C, A166C, and L173C, but anionic sodium (2-sulfonatoethyl)methanethiosulfonate (MTSES) had no effect. Unexpectedly, MTSEA had no effect on Q170C; however, MTSES profoundly altered Q170C charge transfer and turnover, leaving Na+ and sugar binding affinity unchanged, but mutation of glutamine to anionic glutamate (Q170E) shifted V(0.5) to positive potentials, suggesting enhanced Na+ affinity. To clarify the role of glutamine 170 in Na+ interaction, we embarked on a more detailed investigation of Q170E using the two-microelectrode voltage clamping in Xenopus oocytes. Compared to wild-type (wt) rSGLT1, Q170E exhibits (i) a 2-fold decrease in methyl alpha-D-glucopyranoside affinity (-150 to -90 mV), (ii) a 5-fold increase in Na+ affinity (-150 to -100 mV) with less voltage dependency, (iii) reduced Na+ leak, and (iv) two transient current decay constants (tau(fast), tau(slow)) compared to three (tau(fast), tau(medium), tau(slow)) for wt, and computer simulation of Q170E pre-steady-state currents with a four-state kinetic model yields parameters similar to wt SGLT1, except for a reduced Na+ debinding rate constant compared to wt. Taken together, the data strengthen the conclusion that residue 170 lies in the Na+ pathway and provide the first evidence that it participates in determining Na+ binding.