Chloride flux in bilayer membranes: the electrically silent chloride flux in semispherical bilayers

Lipid Flip-Flop and Pore Nucleation on Zwitterionic Bilayers are Asymmetric under Ionic Imbalance

Lipid flip-flop and its associated transient pore formation are key thermodynamic properties of living cell membranes. However, there is a lack of understanding of whether ionic imbalance that exists ubiquitously across cell membranes affects lipid flip-flop and its associated functions. Potential of mean force calculations show that the free-energy barrier of lipid flip-flop on the extracellular leaflet reduces with the presence of ionic imbalance, whereas the barrier on the intracellular leaflet is generally not affected. The linear decrease of the activation energy of lipid flip-flop on the extracellular leaflet is consistent with the experimentally measured conductance-voltage relationship of zwitterionic lipid bilayers. This suggests: 1) lipid flip-flop has a directionality under physiological conditions and phospholipids accumulate at a rate on the order of 105 µm^-2 h^-1 on the cytoplasmic side of cell membranes; 2) ion permeation across a lipid membrane is moderated by lipid flip-flop; 3) the energy barrier of pore formation is aligned with the weaker leaflet that has a lower energy of lipid flip-flop. The asymmetry of lipid flip-flop and pore nucleation may have substantial implications for protein translocation, signaling, enzymatic activities, vesicle fusion, and transportation of biomolecules on cell membranes.

Hydrostatic pressure in small phospholipid vesicles

The internal solvent-filled cavity of a singlewalled spherical phospholipid vesicle must be at essentially the same pressure as the aqueous medium outside the vesicle. Whether or not the bilayer itself is under elevated pressure cannot at present be determined.

Effect of chloride on ferrous iron oxidation by a Leptospirillum ferriphilum-dominated chemostat culture

Biomining is the use of microorganisms to catalyze metal extraction from sulfide ores. However, the available water in some biomining environments has high chloride concentrations and therefore, chloride toxicity to ferrous oxidizing microorganisms has been investigated. Batch biooxidation of Fe(2+) by a Leptospirillum ferriphilum-dominated culture was completely inhibited by 12 g L(-1) chloride. In addition, the effects of chloride on oxidation kinetics in a Fe(2+) limited chemostat were studied. Results from the chemostat modeling suggest that the chloride toxicity was attributed to affects on the Fe(2+) oxidation system, pH homeostasis, and lowering of the proton motive force. Modeling showed a decrease in the maximum specific growth rate (micro(max)) and an increase in the substrate constant (K(s)) with increasing chloride concentrations, indicating an effect on the Fe(2+) oxidation system. The model proposes a lowered maintenance activity when the media was fed with 2-3 g L(-1) chloride with a concomitant drastic decrease in the true yield (Y(true)). This model helps to understand the influence of chloride on Fe(2+) biooxidation kinetics.

Chloride and bicarbonate transport in chick embryonic red blood cells

1. Unidirectional efflux of 36Cl- and H14CO3- from erythrocytes of 4- to 16-day-old chick embryos was measured under steady-state conditions at 37 degrees C and pH 7.7. The efflux rates were high, > 3 s-1, and were, therefore, measured by means of the continuous flow tube method. 2. At day 4 of development the range of permeability coefficients for bicarbonate and chloride (PHCO3 and PCl was 1-30 x 10(-4) cm s-1, with average values of respectively 10 x 10(-4) and 8 x 10(-4) cm s-1. However, the results can be divided into two groups, one with PHCO3 and PCl above 12 x 10(-4) cm s-1, and one with values below 5 x 10(-4) cm s-1. The same range of values was also obtained for day 6 erythrocytes, but the overlap is more conspicuous. At day 16, PHCO3 and PCl were respectively 9 x 10(-4) and 6 x 10(-4) cm s-1 (37 degrees C, pH 7.7). In adult chicken red blood cells PHCO3 and PCl were respectively 7 x 10(-4) and 4 x 10(-4) cm s-1, and in human red blood cells the respective values were 5.6 x 10(-4) and 4 x 10(-4) cm s-1. 3. Chloride self-exchange, measured at 0 degrees C, was almost completely inhibited by addition of 1 mM 4,4'-diisothiocyanostilbene-2,2'-disulphonate (DIDS) at both days 6 and 16 of embryonic development, supporting the finding that the embryonic chick erythrocytes also have a transmembrane anion exchanger similar to that of other red cells.(ABSTRACT TRUNCATED AT 250 WORDS)

Permeability and electrical properties of planar lipid membranes from thylakoid lipids

Electrical measurements were carried out on planar lipid membranes from thylakoid lipids. The specific capacitance of membranes formed from decane-containing monogalactosyldiacylglycerol (MGDG), which accounts for 57% of the total lipid content of thylakoids, showed that it adopted a bilayer structure. Solvent-free bilayers of MGDG were not formed, with very rare exceptions, indicating that decane is required to stabilize the planar conformation. However, this cone-shaped lipid produces bilayer structures in combination with other cylindrical thylakoid lipids even in the absence of organic solvent. We compared the properties of solvent-free and decane-containing bilayers from MGDG, soybean lecithin, and the quaternary mixture of lipids similar to that found in vivo. The conductance of decane-MGDG was 26 times higher than that of decane-lecithin. The flux through the decane-lecithin bilayer was found to be slightly dependent on pH, whereas the decane-MGDG membrane was not. The specific conductance of bilayers formed from the quaternary mixture of lipids was 5 to 10 times larger than lecithin (with alkane or not). Further experiments with bilayers made in the presence of a KCl gradient showed that decane-MGDG, decane-MGDG/DGDG/SQDG/PG, and solvent-free MGDG/DGDG/SQDG/PG were cation-selective. The permeability coefficient for potassium ranged from 4.9 to 8.3 x 10(-11) cm s-1. The permeability coefficient for protons in galactolipids, however, was determined to be about six orders of magnitude higher than the value for potassium ions. The HCl permeation mechanism through the lipid membranes was determined from diffusion potentials measured in HCl gradients. Our results suggest that HCl was not transported as neutral molecules. The data is discussed with regard to the function of galactolipids in the ion transport through thylakoid membranes.

NarK is a nitrite-extrusion system involved in anaerobic nitrate respiration by Escherichia coli

Escherichia coli can use nitrate as a terminal electron acceptor for anaerobic respiration. A polytopic membrane protein, termed NarK, has been implicated in nitrate uptake and nitrite excretion and is thought to function as a nitrate/nitrite antiporter. The longest-lived radioactive isotope of nitrogen, 13N-nitrate (half-life = 9.96 min) and the nitrite-sensitive fluorophore N-(ethoxycarbonylmethyl)-6-methoxyquinolinium bromide have now been used to define the function of NarK. At low concentrations of nitrate, NarK mediates the electrogenic excretion of nitrite rather than nitrate/nitrite exchange. This process prevents intracellular accumulation of toxic levels of nitrite and allows further detoxification in the periplasm through the action of nitrite reductase.

Diffusion of ionizable solutes across planar lipid bilayer membranes: boundary-layer pH gradients and the effect of buffers

The diffusion of weak acids or bases across planar lipid bilayer membranes results in aqueous boundary layer pH gradients. If not properly taken into account, such pH gradients will lead to errors in estimated membrane permeability coefficients, Pm. The role of the permeant concentration, the buffer capacity, and the physicochemical properties of both permeant and buffer on the magnitude and impact of such pH gradients have been explored. A theoretical model has been developed to describe the diffusion of both permeant and buffer species. Significant pH gradients develop depending on solution pH and the pKa's, concentrations, and Pm values of both permeant and buffer. The relative error in experimentally determined Pm values was calculated as the ratio, r, between apparent Pm values (obtained from flux measurements using an equation which neglected boundary layer pH gradients) and its true value. Simulated r values ranged from 1 (0% error) to < 0.01 (> 100% error) for weak acids, decreasing with decreasing buffer capacity and increasing solute flux. The buffer capacity required for an r > 0.95 was calculated versus pH for permeants varying in pKa and Pm. Membrane-permeable buffers significantly reduce boundary layer pH gradients through a feedback effect due to buffer cotransport. Apparent Pm values of p-hydroxymethyl benzoic acid across lecithin bilayer membranes at 25 degrees C were obtained as a function of permeant concentration in various buffers [glycolic, 2-(N-morpholino)ethane-sulfonic, and formic acids]. Predictions agreed closely with experimental fluxes.

Stable cupola-shaped bilayer lipid membranes with mobile Plateau-Gibbs border: expansion-shrinkage of membrane due to thermal transitions

Stable bilayer lipid membranes (BLM) with mobile Plateau-Gibbs border (PGB) have been formed. The precondition of the formation was the presence of a lipid coverage on the teflon surface near the hole, where the membrane has been formed. This allowed the movement of the PGB along the teflon surface after transformation of the planar bilayer into a cupola-shaped by bowing of the bilayer due to excess hydrostatic pressure. As a result the giant bilayers were obtained with an area up to two orders larger in magnitude compared with the initial area. Changes in lipid bilayer area depend on the temperature at the phase transition of the lipid. Cooling of the expanded bilayer was followed by a significant shrinkage of the bilayer at temperatures below the main phase transition.

The apparent permeability coefficient for proton flux through phosphatidylcholine vesicles is dependent on the direction of flux

A dioleoylphosphatidylcholine unilamellar vesicle model system was used to determine proton permeability. The fluorescence of the pH reporter group, pyranine, trapped within vesicles with a difference in pH across the bilayer, was digitized and analyzed with numerical integration. When H+ flux was initiated by the acidification of the external buffer (acid jump), the apparent H+ permeability was found to be a linear function of the reciprocal of the internal H+ concentration with the slope inversely proportional to the initial size of the H+ gradient. When flux was initiated by the alkalinization of the external buffer (base jump), the apparent permeability coefficient was constant for each external H+ concentration. However, the value of the apparent permeability was linearly dependent on the reciprocal of the external H+. The possibility that carbonates (carbon dioxide, carbonic acid, bicarbonate and carbonate) could be acting as proton carriers was tested by adding millimolar concentrations of bicarbonate to solutions greatly reduced in carbonates. The slopes of the graphs of apparent permeability coefficient vs. reciprocal H+ were linear functions of added bicarbonate concentration for both acid and base jump conditions. These observations were interpreted in terms of a model suggesting that carbonic acid or carbon dioxide together with bicarbonate was an efficient proton carrier across phospholipid bilayers.

Membrane electrostatics

In conclusion, charged membrane together with their adjacent electrolyte solution form a thermodynamic and physico-chemical entity. Their surfaces represent an exceptionally complicated interfacial system owing to intrinsic membrane complexity, as well as to the polarity and often large thickness of the interfacial region. Despite this, charged membranes can be described reasonably accurately within the framework of available theoretical models, provided that the latter are chosen on the basis of suitable criteria, which are briefly discussed in Section A. Interion correlations are likely to be important for the regular and/or rigid, thin membrane-solution interfaces. Lateral distribution of the structural membrane charge is seldom and charge distribution perpendicular to the membranes is nearly always electrostatically important. So is the interfacial hydration, which to a large extent determines the properties of the innermost part of the interfacial region, with a thickness of 2-3 nm. Fine structure of the ion double-layer and the interfacial smearing of the structural membrane charge decrease whilst the surface hydration increases the calculated value of the electrostatic membrane potential relative to the result of common Gouy-Chapman approximation. In some cases these effects partly cancel-out; simple electrostatic models are then fairly accurate. Notwithstanding this, it is at present difficult to draw detailed molecular conclusions from a large part of the published data, mainly owing to the lack of really stringent controls or calibrations. Ion binding to the membrane surface is a complicated process which involves charge-charge as well as charge-solvent interactions. Its efficiency normally increases with the ion valency and with the membrane charge density, but it is also strongly dependent on the physico-chemical and thermodynamic state of the membrane. Except in the case of the stereospecific ion binding to a membrane, the relatively easily accessible phosphate and carboxylic groups on lipids and integral membrane proteins are the main cation binding sites. Anions bind preferentially to the amine groups, even on zwitterionic molecules. Membrane structure is apt to change upon ion binding but not always in the same direction: membranes with bound ions can either expand or become more condensed, depending on the final hydrophilicity (polarity) of the membrane surface. The more polar membranes, as a rule, are less tightly packed and more fluid. Diffusive ion flow across a membrane depends on the transmembrane potential and concentration gradients, but also on the coulombic and hydration potentials at the membrane surface.(ABSTRACT TRUNCATED AT 400 WORDS)

Chloride transport pathways and their bioenergetic implications in the obligate acidophile Bacillus coagulans

The protonophore-mediated collapse of the large delta pH that acidophiles maintain across their cytoplasmic membranes was augmented by the presence of Cl-, and Cl- influx into the cells occurred evidently in response to the protonophore-induced increase in the inside-positive membrane potential (+ delta psi). In respiring cells, the addition of Cl- but not SO4(2-) salts caused a rapid and precipitous decrease in the + delta psi. A Nernstian relationship between the imposed transmembrane K+ gradient and the valinomycin-induced K+ diffusion potentials was observed when everted membrane vesicles were loaded with K2SO4 or KH2PO4 but not when loaded with KCl or KNO3. Thus, electrogenic Cl- transport occurred in Bacillus coagulans. In addition, a nonelectrogenic temperature-sensitive Cl- transport mechanism, with the net Cl- efflux coefficient (PCl-) ranging from 1.5 x 10(-4) to 6.1 x 10(-6) cm/s, accounted for the massive Cl- efflux from Cl(-)-loaded cells. Thus, B. coagulans, despite its dependence on the + delta psi and therefore the need to exclude anions, apparently possesses specific mechanisms for Cl- permeation. Active cells of B. coagulans prevented Cl- accumulation from attaining an electrochemical equilibrium, maintaining a delta micro Cl- of ca. -63 mV. B. coagulans therefore also possesses an energy-dependent mechanism for Cl- exclusion from the cells.

Characterization of H+/OH- currents in phospholipid vesicles

In pure phospholipid vesicles, the conductivity of H+/OH- ions exceeds that for other simple inorganic ions. Protons achieve electrochemical equilibrium across egg phosphatidylcholine vesicles within tens of minutes. When pH gradients are established across vesicles, transmembrane potentials develop. Conversely, the establishment of transmembrane potentials leads to the formation of pH gradients. When the phenomenological permeability of H+/OH- ions in vesicles is estimated, values are obtained that are much greater (six orders of magnitude larger) than those for Na+ or K+. A wide range in the values for this permeability has been reported; however, much of the discrepancy can be attributed to differences in the vesicle systems and experimental conditions. The H+/OH- current appears to be modulated by changes in membrane dielectric constant. However, the dependence of this current on the pH gradient and on the membrane voltage argues against simple diffusion mechanisms as the source of the H+/OH- current. In addition, in vesicle systems the H+/OH- current shows a surprising invariance to changes in the membrane dipole potential, an observation that argues against the role of simple carriers for H+ and OH- ions.

Electrogenic H+/OH- movement across phospholipid vesicles measured by spin-labeled hydrophobic ions

Transmembrane pH gradients created across phospholipid vesicles give rise to time-dependent potentials as determined from the EPR spectra of phosphonium ion spin labels in the system. From the time-dependent spectra, the transmembrane H+/OH- current is obtained and hence the current-voltage curve for the vesicle membrane is obtained. The current-voltage curve is linear with a membrane resistance of 3 +/- 2 X 10(9) omega cm2 corresponding to a membrane permeability of 5 +/- 2 X 10(-7) cm/s. This unusually high permeability is further increased by small amounts of lipid oxidation, CHCl3 or the general anesthetic halothane.

Hydroxyl ion permeability of lipid bilayer membranes

The OH- permeability of lipid bilayer (egg phosphatidylcholine-cholesterol) membranes was estimated from ionic transference numbers and membrane conductances at high pH. Membranes are slightly cation (Na+) selective over the pH range of 6--10. However, at pH greater than 11, Na+ and Cl- conductances decrease and OH- conductance increases so that the membrane becomes highly selective to OH-. From the OH- conductance we estimate the OH- permeability coefficient to be 1.8 . 10(-9) cm . s-1. The OH- selectivity of lipid bilayers may contribute to the observed H+/OH- selectivity of some biological membrane at high pH.

Comparison of chloride transport in mouse erythrocytes and Friend virus-transformed erythroleukemic cells

Friend erythroleukemic cells, which grow continuously in tissue culture, resemble in many respects early precursors of mouse erythrocytes. To determine whether or not the membranes of these cells exhibit the rapid and selective exchange of chloride, a specialized feature of the mature erythrocyte membrane, anion fluxes were compared in Friend cells and mouse erythrocytes. The chloride flux in Friend cells at 37 degrees C was about 800-fold lower than in mouse erythrocytes (extrapolated from data at lower temperatures). This difference could not be accounted for by the somewhat lower chloride concentration in Friend cells relative to erythrocytes. Comparison of chloride and sulfate fluxes revealed that the Friend cells had over a 1,000-fold lower selectivity for chloride versus sulphate than did the mouse red cells. The temperature dependence of chloride fluxes in Friend cells corresponded to an Arrhenius activation energy of 17.9 kcal/mol, in contrast to over 30 kcal/mol for mature red cells. The chloride flux in Friend cells was also 10-fold less sensitive to the inhibitor, furosemide, than was the flux in mature red cells. The selective chloride exchange system of the mature erythrocyte therefore does not seem to be functional at the stage represented by the Friend cell, and must appear at some later stage of erythroid maturation.

Some effects of trinitrocresolate and valinomycin on Na and K transport across thin lipid bilayer membranes: a steady-state analysis with simultaneous tracer and electrical measurements

This paper describes the effect of trinitrocresolate anions (TNC-) on the electrical conductance (Gm), and tracer-measured unidirectional Na and K fluxes (MNa and MK) across bilayers formed from sheep red cell lipids dissolved in decane. In the absence of TNC-, typical low conductances were observed, while the cation fluxes were too low to measure by our techniques (less than 10(-12) moles cm-2 sec-1). In the presence of TNC- (10(-2) M), Gm increased and TNC- was the main charge carrier in the system. The cationic fluxes were also much increased, but the membranes showed no significant selectivity between K and Na. Furthermore, the Na and K fluxes were at least two orders of magnitude larger than the ionic fluxes calculated from Gm. Thus, almost all of the K and Na transport across the membrane in the presence of TNC- is electrically silent and is probably carried out as KTNC and NaTNC ion pairs. In the presence of valinomycin (10(-6) M) and no TNC-, both the ion fluxes and Gm were 10(3) times larger in KCl than in NaCl, thus exhibiting the characteristic high selectivity of valinomycin for K over Na. In the presence of both valinomycin (10(-6) M) and TNC- (10(-2) M), this selectivity disappeared in that both Gm and MNa in the NaCl system were similar to the respective values in the KCl system. Even under these conditions, most of the Na is still transported by a process which does not carry charge. Both Gm and Mx increased alike and monotonically with increasing temperature over the range 7 to 30 degrees C. In the absence of TNC- the enthalpies of activation were invariably higher in KCl than in NaCl. Addition of TNC- produced equal enthalpies of activation for both Na and K containing systems suggesting a common, temperature-dependent, rate-determining step in charge transfer and the electrically silent cation fluxes.

Electrically silent anion transport through lipid bilayer membranes containing a long-chain secondary amine

The permeability properties of planar lipid bilayers made from egg lecithin, n-decane and a long-chain secondary amine (n-lauryl [trialkylmethyl]amine) are described. Membranes containing the secondary amine show halide selectivity and high conductance at pH less than 6, as estimated by measurements of zero-current potentials generated by NaBr activity gradients. In the absence of halide ions, the membranes show H+ selectivity, although the total membrane conductance is relatively low. In 0.1 M NaBr both the membrane conductance (Gm) and the Br- self-exchange flux (JBr) are proportional to H+ concentration over the pH range of 7 to 4, and both JBr and Gm saturate at pH less than 4. However, JBr is always more than 100 times the flux predicted from Gm and the transference number for Br-. Thus, greater than 99% of the observed (tracer) flux is electrically silent and is not a Br2 or HBrO flux because the reducing agent, S2O3=, has no effect on JBr. At pH 7, JBr is proportional to Br- concentration over the range of 1-340 mM, with no sign of saturation kinetics. Both urea and sulfate tracer permeabilities are low and are unaffected by pH. The results can be explained by a model in which the secondary amine behaves as a monovalent, titratable carrier which exists in three chemical forms (C, CH+, and CHBr). Br- crosses the membrane primarily as the neurtal complex (CHBr). The positively charged carrier (CH+) crosses the membrane slowly compared to CHBr, but CH+ is the principal charge carrier in the membrane. At neurtal pH greater than 99% of the amine is in the nonfunctional form (C), which can be converted to CH+ or CHBr by increasing the H+ or Br- concentrations. The permeability properties of these lipid bilayers resemble in many respects the permeability properties of red cell membranes.

Permeability of iodide in multilamellar liposomes modeled by two compartments and a reservoir

A previously published rate law for the diffusion of iodide from multilamellar egg phosphatidylcholine liposomes (Schullery, S.E. (1975) Chem. Phys. Lipids 14, 49-58) is fitted to the relatively simple mathematical model of two compartments in series with a reservoir. All of the inner liposome compartments are assumed to behave as effectively one compartment in series with the liposome's outermost compartment. Based on this model, reasonable values are calculated for the fraction of the total solution trapped by liposomes which is in the outermost liposome compartment, 17%, and the permeability coefficient of iodide against isotonic, mixed iodide-chloride solution, 2-10(-9) cm/s.

Nonelectrolyte diffusion across lipid bilayer systems

The permeability coefficients of a homologous series of amides from formamide through valeramide have been measured in spherical bilayers prepared by the method described by Jung. They do not depend directly on the water:ether partition coefficient which increases regularly with chain length. Instead there is a minimum at acetamide. This has been ascribed to the effect of steric hindrance on diffusion within the bilayer which increases with solute molar volume. This factor is of the same magnitude, though opposite in sign to the effect of lipid solubility, thus accounting for the minimum. The resistance to passage across the interface has been compared to the resistance to diffusion within the membrane. As the solute chain length increases the interface becomes more important, until for valeramide it comprises about 90% of the total resistance. Interface resistance is also important in urea permeation, causing urea to permeate much more slowly than an amide of comparable size, after allowance is made for the difference in the water:ether partition coefficient. Amide permeation coefficients have been compared with relative liposome permeation data measured by the rate of liposome swelling. The ratios of the two measures of permeation vary between 3 and 16 for the homologous amides. The apparent enthalpy of liposome permeation has been measured and found to be in the neighborhood of 12 kcal mol-1 essentially independent of chain length. Comparison of the bilayer permeability coefficients with those of red cells shows that red cell permeation by the lipophilic solutes resembles that of the bilayers, whereas permeation by the hydrophilic solutes differs significantly.