Active and passive Na+ fluxes across the basolateral membrane of rabbit urinary bladder

Summary The apical membrane of rabbit urinary bladder can be functionally removed by application of nystatin at high concentration if the mucosal surface of the tissue is bathed in a saline which mimics intracellular ion concentrations. Under these conditions, the tissue is as far as the movement of univalent ions no more than a sheet of basolateral membrane with some tight junctional membrane in parallel. In this manner the Na⁺ concentration at the inner surface of the basolateral membrane can be varied by altering the concentration in the mucosal bulk solution. When this was done both mucosal-to-serosal²²Na flux and net change in basolateral current were measured. The flux and the current could be further divided into the components of each that were either blocked by ouabain or insensitive to ouabain. Ouabain-insensitive mucosal-to-serosal Na⁺ flux was a linear function of mucosal Na⁺ concentration. Ouabain-sensitive Na⁺ flux and ouabain-sensitive, Na⁺-induced current both display a saturating relationship which cannot be accounted for by the presence of unstirred layers. If the interaction of Na⁺ with the basolateral transport process is assumed to involve the interaction of some number of Na⁺ ions,n, with a maximal flux,M _max, then the data can be fit by assuming 3.2 equivalent sites for interaction and a value forM _max of 287.8pm cm^–2 sec^–1 with an intracellular Na concentration of 2.0mm Na⁺ at half-maximal saturation. By comparing these values with the ouabain-sensitive, Na⁺-induced current, we calculate a Na⁺ to K⁺ coupling ratio of 1.40±0.07 for the transport process.     

Basolateral membrane potential of a tight epithelium: Ionic diffusion and electrogenic pumps

Summary The contribution of specific ions to the conductance and potential of the basolateral membrane of the rabbit urinary bladder has been studied with both conventional and ion-specific microelectrode techniques. In addition, the possibility of an electrogenic active transport process located at the basolateral membrane was studied using the polyene antibiotic nystatin. The effect of ion-specific microelectrode impalement damage on intracellular ion activities was examined and a criterion set for acceptance or rejection of intracellular activity measurements. Using this criterion, we found (K⁺)=72mm and (Cl^–)=15.8mm. Cl^– but not K⁺ was in electrochemical equilibrium across the basolateral membrane. The selective permeability of the basolateral membrane was measured using microelectrodes, and the data analyzed using the Goldman, Hodgkin-Katz equation. The sodium to potassium permeability ratio (P _Na/P _K) was 0.044, and the chloride to potassium permeability ratio (P _Cl/P _K) was 1.17. Since K⁺ was not in electrochemical equilibrium, intracellular (K⁺) is maintained by active metabolic processes, and the basolateral membrane potential is a diffusion potential with K⁺ and Cl^– the most permeable ions. After depolarizing the basolateral membrane with high serosal potassium bathing solutions and eliminating the apical membrane as a rate limiting step for ion movement using the polyene antibiotic nystatin, we found that the addition of equal aliquots of NaCl to both solutions caused the basolateral membrane potential to hyperpolarize by up to 20 mV (cell interior negative). This popential was reduced by 80% within 3 min of the addition of ouabain to the serosal solution. This hyperpolarization most probably represents a ouabain sensitive active transport process sensitive to intracellular Na⁺. An equivalent electrical circuit for Na⁺ transport across rabbit urinary bladder is derived, tested, and compared to previous results. This circuit is also used to predict the effects that microelectrode impalement damage will have on individual membrane potentials as well as time-dependent phenomena; e.g., effect of amiloride on apical and basolateral membrane potentials.     

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.     

Papaverine reduces the sodium permeability of the apical membrane and the Potassium permeability of the basolateral membrane in isolated frog skin

Summary The effect of papaverine, an inhibitor of the phosphodiesterase responsible for breakdown of cAMP, on the transepithelial sodium transport across the isolated frog skin was investigated.Serosal addition of papaverine caused initially an increase in the short-circuit current (SCC), a doubling of the cellular cAMP content and a depolarization of the intracellular potential under SCC conditions (V _scc).The initial increase in the SCC was followed by a pronounced decrease both in the SCC and in the natriferic action of antidiuretic hormone (ADH), but papaverine had no inhibitory effect on the ability of ADH to increase the cellular cAMP content. As SCC declines, no hyperpolarization was observed.The I/V relationship across the apical membrane during the inhibitory phase, revealed that papaverine reduces the sodium permeability of the apical membrane (P _Na ^a )as well as intracellular sodium concentration. These observations and the previously noted effect of papaverine on V _scc indicates that papaverine must have an effect on the cellular Cl or K permeability.The basolateral Na,K,2Cl cotransporter was blocked with bumetanide, which should bring the cellular chloride in equilibrium. Bumetanide had no effect on basal SCC and V _scc. When papaverine was added to skins preincubated with bumetanide, the effect of papaverine on SCC and V _scc was unchanged. Therefore, the depolarization of V _scc, observed during the papaverine induced inhibition of the SCC, must be due to a reduction in the cellular K permeability.In conclusion, it is suggested that papaverine reduces the sodium permeability of the apical membrane and the potassium permeability of the basolateral membrane of the frog skin epithelium.     

Electrophysiologic changes associated with potassium depletion of frog skin

Summary Skins from the frogRana pipiens pipiens were studied under short-circuited conditions during the course of removing and replacing potassium in the inner bathing media in 14 experiments. The intracellular potential (V _SC), fractional resistance (FR), short-circuit current (I _SC) and total tissue conductance (g _T) were constantly monitored during impalements of the epithelial cells. The mean value (±se) forV _SC was –79 (±3) mV under baseline conditions. Removal of potassium from the inner bathing solution transiently stimulated the short-circuit current and hyperpolarized the basolateral membrane; with sufficiently long incubations, the basolateral membrane was eventually depolarized. Restoration of potassium to the inner solution within 43 min after initiating the perfusion with K⁺-free solution depolarized the basolateral membrane. However, restoration of potassium after at least 11/2 hr of incubation hyperpolarized the membrane. Ouabain consistently depolarized the basolateral membrane, even after extended periods of potassium depletion as long as 320 min. In the presence of ouabain, restoration of potassium depolarized the basolateral membrane. The data provide further evidence for the concept that the Na–K exchange pump of frog skin is rheogenic. Furthermore, the results suggest that the pump continues to be active even during prolonged periods of potassium depletion, reaccumulating potassium which has leaked out of the epithelial cells.     

Rheogenic transport in the renal proximal tubule

The electrophysiology of the renal Na-K ATPase was studied in isolated perfused amphibian proximal tubules during alterations in bath (serosal) potassium. Intracellular and extracellular ionic activity measurements permitted continuous evaluation of the Nernst potentials for Na+, K+, and Cl- across the basolateral membrane. The cell membrane and transepithelial potential differences and resistances were also determined. Return of K to the basal (serosal) solution after a 20-min incubation in K-free solution hyperpolarized the basolateral membrane to an electrical potential that was more negative than the Nernst potential for either Na, Cl, or K. This constitutes strong evidence that at least under stimulated conditions the Na-K ATPase located at the basolateral membrane of the renal proximal tubule mediates a rheogenic process which directly transfers net charge across the cell membrane. Interpretation of these data in terms of an electrical equivalent circuit permitted calculation of both the rheogenic current and the Na/K coupling ratio of the basolateral pump. During the period between 1 and 3 min after pump reactivation by return of bath K, the basolateral rheogenic current was directly proportional to the intracellular Na activity, and the pump stoichiometry transiently exceeded the coupling ratio of 3Na to 2K reported in other preparations.     

Basolateral membrane potassium conductance of A6 cells

Summary To study the properties of the basolateral membrane conductance of an amphibian epithelial cell line, we have adapted the technique of apical membrane selective permeabilization (Wills, N.K., Lewis, S.A., Eaton, D.C., 1979b, J. Membrane Biol. 45:81–108). Monolayers of A6 cells cultured on permeable supports were exposed to amphotericin B. The apical membrane was effectively permeabilized, while the high electrical resistance of the tight junctions and the ionic selectivity of the basolateral membrane were preserved. Thus the transepithelial current-voltage relation reflected mostly the properties of the basolateral membrane. Under basal conditions, the basolateral membrane conductance was inward rectifying, highly sensitive to barium but not to quinidine. After the induction of cell swelling either by adding chloride to the apical solution or by lowering the osmolarity of the basolateral solution, a large out-ward-rectifying K⁺ conductance was observed, and addition of barium or quinidine to the basolateral side inhibited, respectively, 82.4±1.9% and 90.9±1.0% of the transepithelial current at 0 mV. Barium block was voltage dependent; the half-inhibition constant (K _i) varied from 1499±97 m at 0 mV to 5.7±0.5 m at –120 mV.Cell swelling induces a large quinidine-sensitive K⁺ conductance, changing the inward-rectifying basolateral membrane conductance observed under basal conditions into a conductance with outward-rectifying properties.     

Distinct apical and basolateral membrane requirements for stretch-induced membrane traffic at the apical surface of bladder umbrella cells

Epithelial cells respond to mechanical stimuli by increasing exocytosis, endocytosis, and ion transport, but how these processes are initiated and coordinated and the mechanotransduction pathways involved are not well understood. We observed that in response to a dynamic mechanical environment, increased apical membrane tension, but not pressure, stimulated apical membrane exocytosis and ion transport in bladder umbrella cells. The exocytic response was independent of temperature but required the cytoskeleton and the activity of a nonselective cation channel and the epithelial sodium channel. The subsequent increase in basolateral membrane tension had the opposite effect and triggered the compensatory endocytosis of added apical membrane, which was modulated by opening of basolateral K⁺ channels. Our results indicate that during the dynamic processes of bladder filling and voiding apical membrane dynamics depend on sequential and coordinated mechanotransduction events at both membrane domains of the umbrella cell.     

Electrical properties of the cellular transepithelial pathway inNecturus gallbladder: III. Ionic permeability of the basolateral cell membrane

Summary The ionic permeability of the basolateral membrane ofNecturus gallbladder epithelium was studied with intracellular microelectrode techniques. After removal of most of the subepithelial tissue (to reduce unstirred layer thickness), impalements were performed from the serosal side, and ionic substitutions were made in the serosal solution while a microelectrode was kept in a cell. Thus, it was possible to obtain continuous (and reversible) records of transepithelial and cell membrane potentials and to measure intermittently the transepithelial resistance and the ratio of cell membrane resistances. From these data and the mean value of the equivalent resistance of the cell membranes in parallel (obtained from cable analysis in a different group of tissues), absolute cell membrane and shunt resistances and equivalent electromotive forces (emf's) were calculated. From the changes of basolateral membrane emf (E _b ) produced by the substitutions, the conductance (G) and permeability (P) of the membrane for K, Cl and Na were estimated. Potassium-for-sodium substitutions produced large reductions of both cell membrane potentials, ofE _b , and of the resistance of the basolateral membrane (R _b ), indicating highG _K andP _K . Chloride substitution with isethionate or sulfate resulted in smaller changes of cell membrane potentials andE _b and in no significant change ofR _b , indicating small but measurable values ofG _Cl andP _Cl . Sodium substitutions with N-methyl-d-glucamine (NMDG) resulted in cell potential changes entirely attributable to the biionic potential produced in the shunt pathway (P _Na >P _NMDG ), and in no significant changes ofP _b orE _b , indicating thatG _Na andP _Na are undetectable. The question of the mechanism of Cl transport across the basolateral membrane was addressed by comparing the mean rate of transepithelial Cl transport (J _Cl ^net ) and the predicted passive Cl flux across the basolateral membrane (from the membrane Cl conductance, potential, and Cl equilibrium potential). The conclusion is that only a very small fraction of the Cl flux across the basolateral membrane can be electrodiffusional. Since the paracellular Cl conductance is also too low to account forJ _Cl ^net , these results suggest the presence of a neutral mechanism of Cl extrusion from the cells. This could be a NaCl pump, a downhill KCl transport mechanism, or a Cl–HCO₃ exchange mechanism.     

Mechanism of inhibition of net ion transport across frog corneal epithelium by calcium channel antagonists

Summary In the isolated bullfrog cornea, three calcium channel antagonists had dose-dependent inhibitory effects on the Cl-originated short-circuit current (SCC). Their order of decreasing potency was bepridil, verapamil and diltiazem. One millimolar diltiazem inhibited the SCC by 98% and subsequent incubation with the calcium ionophore A23187 had no restorative effect. Increasing the bathing solution Ca concentration from 0.05 to 15mm, however, decreased diltiazem's inhibitory efficacy. This antagonist depolarized the intracellular potential differenceV _m from –54 to –18 mV (tear: reference) and the voltage divider ratioFR ₀ decreased from 0.58 to 0.30, suggesting an increase in basolateral membrane electrical resistance. Additional indication of a basolateral membrane effect by the drug was that preincubation with 10⁵ m amphotericin B in Cl-free Ringer's did not eliminate the inhibitory effect of the drug on the Na- and K-elicited SCC. In the absence of amphotericin B in Cl-free Ringer's (SCC=0), 1 ×10³ m diltiazem depolarized theV _m from –78 to –9 mV suggesting that the increase in basolateral membrane resistance was due to K channel blockade. Diltiazem (1×10³ m) significantly decreased cyclic AMP content; however, isoproterenol in the presence of the drug increased cyclic AMP fourfold without having any restorative effect on the inhibited SCC. Therefore, the inhibition of the Cl-originated SCC resulting from an increase in basolateral membrane K resistance is not caused by a decline in cyclic AMP content. In plasma membrane-enriched fractions prepared from broken cell preparations of bovine corneal epithelium, 1×10³ m diltiazem had no inhibitory effects on either Na,K-ATPase or Ca,Mg-ATPase activities. These latter effects further point to the selectivity of diltiazem as an inhibitor of K-channel activity, but do not preclude a Ca-channel blocker effect by the drug in the micromolar range.     

Voltage dependence of the basolateral membrane conductance in theAmphiuma collecting tubule

Summary The basolateral potassium conductance of cells of most epithelial cells plays an important role in the transcellular sodium transport inasmuch as the large negative equilibrium potential of potassium across this membrane contributes to the electrical driving force for Na⁺ across the apical membrane. In the present study, we have attempted to establish, theI-V curve of the basolateral membrane of theAmphiuma collecting tubule, a membrane shown to be K⁺ selective. TransepithelialI-V curves were obtained in short, isolated perfused collecting tubule segments. The shunt conductance was determined using amiloride to block the apical membrane Na⁺ conductance. In symmetrical solutions, the shuntI-V curve was linear (conductance: 2.2±0.3 mS·cm^–2). Transcellular current was calculated by subtracting the shunt current from the transepithelial current in the absence of amiloride. Using intracellular microelectrodes, it was then possible to measure the basolateral membrane potential simultaneously with the transcellular current. The basolateral conductance was found to be voltage dependent, being activated by hyperpolarization: conductance values at –30 and –80 mV were 3.6±1.0 and 6.6±1.0 mS·cm^–2, respectively. BasolateralI-V curves were thus clearly different from that predicted by the constant field model. These results indicate that the K⁺-selective basolateral conductance of an amphibian collecting tubule shows inward (anomalous) rectification. Considering the electrogenic nature basolateral Na–K-pump, this may account for coupling between pump-generated potential and basolateral K⁺ conductance.     

Active and passive Na+ fluxes across the basolateral membrane of rabbit urinary bladder

The apical membrane of rabbit urinary bladder can be functionally removed by application of nystatin at high concentration if the mucosal surface of the tissue is bathed in a saline which mimics intracellular ion concentrations. Under these conditions, the tissue is as far as the movement of univalent ions no more than a sheet of basolateral membrane with some tight junctional membrane in parallel. In this manner the Na+ concentration at the inner surface of the basolateral membrane can be varied by altering the concentration in the mucosal bulk solution. When this was done both mucosal-to-serosal 22Na flux and net change in basolateral current were measured. The flux and the current could be further divided into the components of each that were either blocked by ouabain or insensitive to ouabain. Ouabain-insensitive mucosal-to-serosal Na+ flux was a linear function of mucosal Na+ concentration. Ouabain-sensitive Na+ flux and ouabain-sensitive, Na+-induced current both display a saturating relationship which cannot be accounted for by the presence of unstirred layers. If the interaction of Na+ with the basolateral transport process is assumed to involve the interaction of some number of Na+ ions, n, with a maximal flux, MMAX, then the data can be fit by assuming 3.2 equivalent sites for interaction and a value for MMAX of 287.8 pM cm-2 sec-1 with an intracellular Na concentration of 2.0 mM Na+ at half-maximal saturation. By comparing these values with the ouabain-sensitive, Na+-induced current, we calculate a Na+ to K+ coupling ratio of 1.40 +/- 0.07 for the transport process.     

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.     

Separation of tonoplast and plasma membrane potential and resistance in cells of oat coleoptiles

Summary Membrane potential and resistance were recorded from parenchymal cells of oat (Avena) coleoptiles, using one and two intracellular electrodes. Membrane potential is largest (–100 mV) in impalements with low input resistance (2–4 M), and is less negative (–50 mV) in penetrations with high input resistance (> 20 m). The interpretation is that the electrode lodges in the vacuole which is positive to the cytoplasm (but still negative to the external solution), and that measurements of net membrane potential are compromised to varying degrees by leakage shunts introduced across the high resistance vacuolar membrane by the electrode. This conclusion is supported by several additional lines of evidence. (1) It is possible to convert large-R/small-V impalements into small-R/large-V penetrations by passing excess current through the electrode or by briefly ringing the capacitance neutralization circuit in the amplifier. The cells usually recover their resistance in a few minutes, with a concomitant decrease in the negativity of the membrane potential. (2) Changes in external [K] affect the measuree potential by an amount that is independent of the input resistance of the impalement. This is consistent with an effect of [K] _o on the potential of the plasma membrane and the occurrence of leakage shunts primarily at the tonoplast. (3) Quantitatively, the effects of a change in [K] _o on resistance indicate that nearly 90 percent of the input resistance of unshunted cells resides in the tonoplast. (4) The effects of metabolic inhibitors (DNP, CN^–) on potential are smaller in large-R than in small-R impalements. This observation suggests there are electrogenic pumps contributing to the membrane potential at both the plasmalemma and tonoplast. Finally, we conclude that with an electrode in the vacuole it is possible to record potentials that are dominated by the contribution of the plasma membrane, provided care is taken to select impalements combining both large, negative potential and low input resistance.     

Sodium transport effects on the basolateral membrane in toad urinary bladder

In toad urinary bladder epithelium, inhibition of Na transport with amiloride causes a decrease in the apical (Vmc) and basolateral (Vcs) membrane potentials. In addition to increasing apical membrane resistance (Ra), amiloride also causes an increase in basolateral membrane resistance (Rb), with a time course such that Ra/Rb does not change for 1-2 min. At longer times after amiloride (3-4 min), Ra/Rb rises from its control values to its amiloride steady state values through a secondary decrease in Rb. Analysis of an equivalent electrical circuit of the epithelium shows that the depolarization of Vcs is due to a decrease in basolateral electromotive force (Vb). To see of the changes in Vcs and Rb are correlated with a decrease in Na transport, external current (Ie) was used to clamp Vmc to zero, and the effects of amiloride on the portion of Ie that takes the transcellular pathway were determined. In these studies, Vcs also depolarized, which suggests that the decrease in Vb was due to a decrease in the current output of a rheogenic Na pump. Thus, the basolateral membrane does not behave like an ohmic resistor. In contrast, when transport is inhibited during basolateral membrane voltage clamping, the apical membrane voltage changes are those predicted for a simple, passive (i.e., ohmic) element.     

An Amiloride-sensitive Na+ conductance in the basolateral membrane of toad urinary bladder

Summary Exposing the apical membrane of toad urinary bladder to the ionophore nystatin lowers its resistance to less than 100 cm². The basolateral membrane can then be studied by means of transepithelial measurements. If the mucosal solution contains more than 5mm Na⁺, and serosal Na⁺ is substituted by K⁺, Cs⁺, or N-methyl-d-glucamine, the basolateral membrane expresses what appears to be a large Na⁺ conductance, passing strong currents out of the cell. This pathway is insensitive to ouabain or vanadate and does not require serosal or mucosal Ca²⁺. In Cl-free SO ₄ ^2– Ringer's solution it is the major conductive pathway in the basolateral membrane even though the serosal side has 60mm K⁺. This pathway can be blocked by serosal amiloride (K _i=13.1 m) or serosal Na⁺ ions (K _i 10 to 20mm). It also conducts Li⁺ and shows a voltage-dependent relaxation with characteristic rates of 10 to 20 rad sec^–1 at 0 mV.     

Changes in cellular membrane and paracellular conductances by amphotericin B in the epithelium of the bullfrog cornea.

In the isolated bullfrog cornea, measurements of DC electrical parameters in conjunction with AC impedance and ultrastructural analyses were used to determine the effects of 10(-5) M amphotericin B on epithelial cellular membrane and paracellular conductances. In NaCl Ringers, amphotericin B elicited a 3.5-fold increase in the specific apical membrane conductance (Ga/Ca); where Ga and Ca are the apical membrane conductance and capacitance, respectively. The basolateral membrane conductance (Gb) and the basolateral membrane capacitance (Cb) fell by 57% and 50%, respectively. In the paracellular pathway, the tight junctional complex (Gj) was unchanged whereas the lateral intercellular space resistance (Rp) decreased by 55%. The declines in Gb and Cb were suggestive of cell volume shrinkage because these changes were consistent with a previously described decline in intracellular K+ content and reduction in exposed basolateral membrane area to current flow. Ultrastructural analysis validated that amphotericin B caused cell volume shrinkage because there was: (1) increased folding of the basolateral membrane and waviness of the basal aspects- of the plasma membrane; (2) dilatation of the lateral intercellular spaces. This agreement suggests that intracellular activity decreased following exposure to amphotericin B which resulted in cell volume shrinkage and an impairment of Cl- uptake across the basolateral membrane.     

Chloride movement across the basolateral membrane of proximal tubule cells

Summary Electrophysiologic and tracer experiments have shown that Cl^– entersNecturus proximal tubule cells from the tubule lumen by a process coupled to the flow of Na⁺, and that Cl^– entry is electrically silent. The mechanism of Cl^– exit from the cell across the basolateral membrane has not been directly studied. To evaluate the importance of the movement of Cl^– ions across the basolateral membrane, the relative conductance of Cl^– to K⁺ was determined by a new method. Single-barrel ion-selective microelectrodes were used to measure intracellular Cl^– and K⁺ as a function of basolateral membrane PD as it varied normally from tubule to tubule. Basolateral membrane Cl^– conductance was about 10% of K⁺ conductance by this method. A second approach was to voltage clamp the basolateral PD to 20 mV above and below the spontaneous PD, while sensing intracellular Cl^– activity with the second barrel of a double-barrel microelectrode. An axial wire electrode in the tubule lumen was used to pass current across the tubular wall and thereby vary the basolateral membrane PD. Cell Cl^– activity was virtually unaffected by the PD changes. We conclude that Cl^– leavesNecturus proximal tubule cells by a neutral mechanism, possibly coupled to the efflux of Na⁺ or K⁺.     

Electrical properties of the rabbit urinary bladder assessed using gramicidin D

Summary Recently, antibiotics have enjoyed widespread usage as tools in studies of epithelial transport. In the present study we assess the usefulness of the pore-forming antibiotic gramicidin D as a means for probing the electrical properties of the tight epithelium rabbit urinary bladder. Addition of 50 M gramicidin to the mucosal bath (either a NaCl or KCl Ringer's solution) led to a large irreversible increase in the transepithelial conductance (G _T ) within 800 sec.G _T increased by approximately 1200% and 500% in KCl and NaCl Ringer's solutions, respectively. Microelectrode measurements of the resistance ration (the ration of apical membrane resitance to basolateral membrane resistance) showed that apical membrane resistance is dereased by the drug. Measurements of the basolateral membrane resistance (R _bl ) and tight junctional resistance (R _j ) using a new and independent method (based on the perturbation of basolateral membrane electrogenic Na⁺ pump) demonstrated thatR _bl andR _j were unaffected, suggesting that the effects of gramicidin are restricted to the apical membrane for periods of at least 2 hours after drug addition. The selectivity of the gramicidin-induced permeability in the apical membrane was calculated from measurements of the apical membrane potential after ion substitutions using a modified version of the constant field equation. The selectivity sequence for cations was Cs⁺>K⁺>Na⁺>Li⁺>choline. Unlike the commonly used polyene antibiotics nystatin and amphotericin B, gramicidin did not induce a significant Cl^– permeability. In addition, the dose-response curve had a slope of 1. A method is described for calculating membrane resistances directly from transepithelial measurements under some conditions of gramicidin use, without requiring the use of microlectrode measurements.     

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.