Surface potential of mycoplasma membranes

Abstract The outer membrane surfaces of several mycoplasma species carry a dense layer of anionic charges, i.e., lipid phosphate groups. They induce a negative surface potential ψ at the membrane-aqueous phase interface. This surface potential strongly affects the distribution of ions including protons. Accordingly, the pH at the interface differs from the bulk pH. By using the fluorescent lipoid pH indicator 4-heptadecyl-7-hydroxycoumarin the pH at the membrane surface was determined. From the difference of the bulk and the interfacial pH the membrane surface potential of Mycoplasma mycoides subsp. capri was calculated to be ψ = −68 mV.     

Fusion of Spiroplasma floricola cells with small unilamellar vesicles is dependent on the age of the culture.

Small unilamellar vesicles were labeled with the fluorescent probe octadecylrhodamine B chloride and mixed with intact Spiroplasma floricola cells. The increase in fluorescence observed was interpreted as a result of the dilution of the probe in the unlabeled S. floricola membranes because of lipid mixing upon fusion. The progression of S. floricola cultures to the stationary phase of growth was accompanied by a sharp decrease in the ability of the cells to fuse with small unilamellar vesicles. Low fusogenic activity was also detected in cells from cultures that were aged in a growth medium maintained at pH 7.5 throughout the growth cycle. Chemical analysis of the cell membrane preparations isolated from cells harvested at the various phases of growth revealed that the phospholipid content and composition and the cholesterol/phospholipid molar ratio were changed very little upon aging of the cultures. Likewise, no changes in the fatty acid composition of membrane lipids were detected, with palmitic and oleic acids predominating throughout the cycle. Nonetheless, upon aging of S. floricola cultures, a pronounced increase in the levels of both cholesteryl esters, incorporated from the growth medium, and organic peroxides was observed. A decrease in both fluorescence anisotropy of diphenylhexatriene and merocyanine 540 binding to membranes of aged cells was also detected. The possible influence of these changes on the fusogenic activity of the cells is discussed.     

Surface pH controls purple-to-blue transition of bacteriorhodopsin. A theoretical model of purple membrane surface.

We have developed a surface model of purple membrane and applied it in an analysis of the purple-to-blue color change of bacteriorhodopsin which is induced by acidification or deionization. The model is based on dissociation and double layer theory and the known membrane structure. We calculated surface pH, ion concentrations, charge density, and potential as a function of bulk pH and concentration of mono- and divalent cations. At low salt concentrations, the surface pH is significantly lower than the bulk pH and it becomes independent of bulk pH in the deionized membrane suspension. Using an experimental acid titration curve for neutral, lipid-depleted membrane, we converted surface pH into absorption values. The calculated bacteriohodopsin color changes for acidification of purple, and titrations of deionized blue membrane with cations or base agree well with experimental results. No chemical binding is required to reproduce the experimental curves. Surface charge and potential changes in acid, base and cation titrations are calculated and their relation to the color change is discussed. Consistent with structural data, 10 primary phosphate and two basic surface groups per bacteriorhodopsin are sufficient to obtain good agreement between all calculated and experimental curves. The results provide a theoretical basis for our earlier conclusion that the purple-to-blue transition must be attributed to surface phenomena and not to cation binding at specific sites in the protein.     

Transmembrane proton-motive potential of Spiroplasma floricola

In Spiroplasma floricola, the transmembrane proton-motive potential delta p was studied. It is composed of a transmembrane electric potential difference, delta psi, and a transmembrane proton gradient, delta pH, according to delta p = delta psi - (Z.delta pH). Using a potential-sensitive carbocyanine dye and 5,5'-dimethyl[2-14C]oxazolidine-2,4-dione as probes, delta psi and delta pH were measured at different [H+] of the medium, and delta p was calculated to be remarkably constant at -123 mV +/- 16% over a wide range of external pH values. Inhibition experiments indicated that it is generated by a membrane-bound, electrogenic, proton-translocating ATPase.     

Interfacial pH modulation of membrane protein function in vivo. Effect of anionic phospholipids.

In yeast cells, the magnitude of the membrane surface potential (phi) is determined to a large extent by the relative amount of anionic phospholipids (Cerbón and Calderón (1990) Biochim. Biophys. Acta 1028, 261-267). When a significant surface potential exists, the pH at the membrane surface (interfacial pH) will be different to that in the bulk suspending medium. We now report that: (1) In cells with higher phi (phosphatidylinositol-rich cells (PI-rich) and phosphatidylserine-rich cells (PS-rich) a 10-times lower proton concentration in the bulk was enough to achieve the maximum transport activity of H(+)-linked transport systems when compared to normal cells. (2) When the phi was reduced by increasing the concentration of cations in the medium, more protons were required to achieve maximum transport, that is, the pH activity curves shifted downwards to a more acidic pH. (3) The magnitude of the downward pH shift was around 2.5-times higher for the more charged membranes. (4) Around 10-times more KCl than MgCl2 was necessary to give an equivalent pH shift, in agreement with their capacity to reduce the phi of artificial bilayers. The interfacial pH calculated from the values of phi indicates that it was 0.4 pH units lower in the anionic phospholipid rich cells as compared to normal cells. The results indicate that membrane surface potential may explain the complex relationship between pH, ionic strength and membrane protein function. Maximum transport activities were found for glutamate at interfacial pH of 4.2-4.8 and were inhibited at interfacial pH = 3.2-3.4, suggesting that surface groups of the carrier proteins with pK values in the region 3.8-4.2 (aspartyl and glutamyl) are involved in binding and/or release of charged substrates.     

Effects of surface potential and membrane potential on the midpoint potential of cytochrome c-555 bound to the chromatophore membrane of Chromatium vinosum

The values of midpoint potential (Em) of cytochrome c-555 bound to the chromatophore membranes of a photosynthetic bacterium Chromatium vinosum was determined under various pH and salt conditions. After a long incubation at high ionic concentrations in the presence of carbonylcyanide m-chlorophenylhydrazone, which was added to abolish electrical potential difference between the inner and outer bulk phases of chromatophore, the Em value was almost constant at pH values between 4.0 and 8.4. With the decrease of salt concentration, the pH dependence of the Em value became more marked. Under low ionic conditions, Em became more positive with the decrease of pH. Addition of salt made the value more positive or negative at pH values higher or lower than 4.5, respectively. Divalent cation salts were more effective than monovalent cation salts in producing the positive shift of Em at pH 7.8. The Em value became more positive when the electrical potential of the inner side of the chromatophore was made more positive by the diffusion potential induced by the K+ concentration gradient in the presence of valinomycin. These results were explained by a change of redox potential at the inner surface of the chromatophore membrane, at which the cytochrome is assumed to be situated, due to the electrical potential difference with respect to the outer solution induced by the surface potential or membrane potential change. The values for the surface potential and the net surface charge density of the inner surface of the chromatophore membrane were estimated using the Gouy-Chapman diffuse double layer theory.     

Phosphorylation alters the pH-dependent active state equilibrium of rhodopsin by modulating the membrane surface potential.

Phosphorylation reduces the lifetime and activity of activated G protein-coupled receptors, yet paradoxically shifts the metarhodopsin I-II (MI-MII) equilibrium (K(eq)) of light-activated rhodopsin toward MII, the conformation that activates G protein. In this report, we show that phosphorylation increases the apparent pK for MII formation in proportion to phosphorylation stoichiometry. Decreasing ionic strength enhances this effect. Gouy-Chapman theory shows that the change in pK is quantitatively explained by the membrane surface potential, which becomes more negative with increasing phosphorylation stoichiometry and decreasing ionic strength. This lowers the membrane surface pH compared to the bulk pH, increasing K(eq) and the rate of MII formation (k(1)) while decreasing the back rate constant (k(-)(1)) of the MI-MII relaxation. MII formation has been observed to depend on bulk pH with a fractional stoichiometry of 0.6-0.7 H(+)/MII. We find that the apparent fractional H(+) dependence is an artifact of altering the membrane surface charge during a titration, resulting in a fractional change in membrane surface pH compared to bulk pH. Gouy-Chapman calculations of membrane pH at various phosphorylation levels and ionic strengths suggest MII formation behavior consistent with titration of a single H(+) binding site with 1:1 stoichiometry and an intrinsic pK of 6.3 at 0.5 degrees C. We show evidence that suggests this same site has an intrinsic pK of 5.0 prior to light activation and its protonation before activation greatly enhances the rate of MII formation.     

Proton-induced phase separation in phosphatidylserine/phosphatidylcholine membranes

Effects of ph and ionic strength on phosphatidylserine/phosphatidylcholine mixed membranes prepared on Millipore filter pore surfaces have been studied using spin-labeled phosphatidylcholine. Lowering pH at constant ionic strength and lowering ionic strength at constant pH caused a lateral reorganization of the membrane. The trigger was protonation of the serine carboxyl group which caused solidification of phosphatidylserine molecules in the membrane, leaving a fluid phase consisting mainly of phosphatidylcholine. The appearent pK for the proton-induced phase separation was measured in a wide range of salt concentrations. The ionic strength dependence was satisfactorily explained based on the electrostatic free energy of proton in the field of membrane surface potential. The Gouy-Chapman theory gave a good approximation for the surface potential. The surface pK of phosphatidylserine and phosphatidic acid vesicles was directly measured in various salt concentrations by 31P-NMR and the results confirmed validity of the Gouy-Chapman-type analysis. The lateral reorganization was triggered by electrostatic interaction but the bulk of the stabilization energy for the structural changes would be the gains in intermolecular van der Waals energy due to closer packing of phosphatidylserine on solidification.     

Mechanisms of generation of local ΔpH in mitochondria and bacteria

The concepts of global and local coupling between proton generators, the enzymes of the respiratory chain, and the consumer, the ATP synthase, coexist in the theory of oxidative phosphorylation. Global coupling is trivial proton transport via the aqueous medium, whereas local coupling implies that the protons pumped are consumed before they escape to the bulk phase. In this work, the conditions for the occurrence of local coupling are explored. It is supposed that the membrane retains protons near its surface and that the proton current generated by the proton pumps rapidly decreases with increasing proton motive force (pmf). It is shown that the competition between the processes of proton translocation across the membrane and their dissipation from the surface to the bulk can result in transient generation of a local ΔpH in reply to a sharp change in pmf; the appearance of local ΔpH, in turn, leads to rapid recovery of the pmf, and hence, it provides for stabilization of the potential at the membrane. Two mechanisms of such kind are discussed: 1) pH changes in the surface area due to proton pumping develop faster than those due to proton escape to the bulk; 2) the former does not take place, but the protons leaving the surface do not equilibrate with the bulk immediately; rather, they give rise to a non-equilibrium concentration near the surface and, as a result, to a back proton flow to the surface. The first mechanism is more efficient, but it does not occur in mitochondria and neutrophilic bacteria, whereas the second can produce ΔpH on the order of unity. In the absence of proton retardation at the surface, local ΔpH does not arise, whereas the formation of global ΔpH is possible only at buffer concentration of less than 10 mM. The role of the mechanisms proposed in transitions between States 3 and 4 of the respiratory chain is discussed. The main conclusion is that surface protons, under conditions where they play a role, support stabilization of the membrane pmf and rapid communication between proton generators and consumers, while their contribution to the energetics is not significant.     

The effect of the lipid bilayer state on fluorescence intensity of fluorescein-PE in a saturated lipid bilayer

Fluorescein-PE is a fluorescence probe that is used as a membrane label or a sensor of surface associated processes. Fluorescein-PE fluorescence intensity depends not only on bulk pH, but also on the local electrostatic potential, which affects the local membrane interface proton concentration. The pH sensitivity and hydrophilic character of the fluorescein moiety was used to detect conformational changes at the lipid bilayer surface. When located in the dipalmitoylphosphatidylcholine (DPPC) bilayer, probe fluorescence depends on conformational changes that occur during phase transitions. Relative fluorescence intensity changes more at pretransition than at the main phase transition temperature, indicating that interface conformation affects the condition in the vicinity of the membrane. Local electrostatic potential depends on surface charge density, the local dielectric constant, salt concentration and water organisation. Initial increase in fluorescence intensity at temperatures preceding that of pretransition can be explained by the decreased value of the dielectric constant in the lipid polar headgroups region related in turn to decreased water organisation within the membrane interface. The abrupt decrease in fluorescence intensity at temperatures between 25 degrees C and 35 degrees C (DPPC pretransition) is likely to be caused by an increased value of the electrostatic potential, induced by an elevated value of the dielectric constant within the phosphate group region. Further increase in the fluorescence intensity at temperatures above that of the gel-liquid phase transition correlates with the calculated decreased surface electrostatic potential. Above the main phase transition temperature, fluorescence intensity increase at a salt concentration of 140 mM is larger than with 14 mM. This results from a sharp decline of the electrostatic potential induced by the phosphocholine dipole as a function of distance from the membrane surface.     

Effect of surface potential on the intramembrane electrical field measured with carotenoid spectral shift in chromatophores from Rhodopseudomonas sphaeroides

Changes in the surface potential, the electrical potential difference between the membrane surface and the bulk aqueous phase were measured with the carotenoid spectral shift which indicates the change of electrical field in the membrane. Chromatophores were prepared from a non-sulfur purple bacterium, Rhodopseudomonas sphaeroides, in a low-salt buffer. Surface potential was changed by addition of salt or by pH jump as predicted by the Gouy-Chapman diffuse double layer theory.When a salt was added at neutral pH, the shift of carotenoid spectrum to shorter wavelength, corresponding to an increase in electrical potential at the outside surface, was observed. The salts of divalent cations (MgSO₄, MgCl₂, CaCl₂) were effective at concentrations lower than those of monovalent cation salts (NaCl, KCl, Na₂SO₄) by a factor of about 50. Among the salts of monoor divalent cation used, little ionic species-dependent difference was observed in the low-concentration range except that due to the valence of cations. The pH dependence of the salt-induced carotenoid change was explained in terms of the change in surface charge density, which was about 0 at pH 5–5.5 and had negative values at higher pH values. The dependence of the pH jump-induced absorbance change on the salt concentration was also consistent with the change in the charge density. The surface potential change by the salt addition, which was calibrated by H⁺ diffusion potential, was about 90 mV at the maximum. From the difference between the effective concentrations with salts of mono- and divalent cations at pH 7.8, the surface charge density of (?1.9 ± 0.5) · 10^?3 elementary charge per Ų, and the surface potential of about ?100 mV in the presence of about 0.1 mM divalent cation or 5 mM monovalent cation were calculated.     

Salt-induced pH changes in spinach chloroplast suspension. Changes in surface potential and surface pH of thylakoid membranes

A pH decrease in chloroplast suspension in media of low salt concentration was observed when a salt was added at pH values higher than 4.4, while at lower pH values a pH increase was observed. The salt-induced pH changes depended on the valence and concentration of cations of added salts at neutral pH values (higher than 4.4) and on those of anions at acidic pH values (lower than 4.4). The order of effectiveness was trivalent > divalent > monovalent. The pH value change by salt addition was affected by the presence of ionic detergents depending on the sign of their charges. These characteristics agreed with those expected from the Gouy-Chapman theory on diffuse electrical double layers. The results were interpreted in terms of the changes in surface potential, surface pH and the ionization of surface groups which result in the release (or binding) of H⁺ to (or from) the outer medium.The analysis of the data of KCl-induced pH change suggests that the change in the surface charge density of thylakoid membranes depends mainly on the ionization of carboxyl groups, which is determined by the surface pH. When the carboxyl groups are fully dissociated, the surface charge density reaches ?1.0 ± 0.1 · 10^?3 elementary charge/square Å.Dependence of the estimated surface potential on the bulk pH was similar to that of electrophoretic mobility of thylakoid membrane vesicles.     

Electrostatic state of the membrane surface and the reactivity between ferricyanide and electron transport components inside chloroplast membranes

The relationship between the electrostatic state of the thylakoidmembrane and the photoreduction rate of ferricyanide were studiedin intact and sonically treated chloroplasts. In sonicated chloroplasts, reduction of ferricyanide by photosystemII required a high concentration of ferricyanide. for full activity,the apparent low affinity of the reduction site for ferricyanidesuggests that permeation of ferricyanide to the site is therate-limiting factor. The affinity was increased by additionof salts or a cationic detergent, but not by anionic or nonionicdetergent at neutral pH. It was also increased by decreasingpH or by adding lipophilic electron mediators such as naphthoquinonesor p-phenylenediamine. In intact chloroplasts similar characteristics of the systemII reducing site were also observed in the presence of dibromothymoquinone,an antagonist of plastoquinone. It is suggested from these results that the site of ferricyanidereduction in system II exists inside the membrane with negativesurface charges, which hinder the access of ferricyanide tothe site by electrostatic repulsion. The charges were probablyscreened by salts or decreased by protonation at low pH. Studywith the fluorescent probe, 8-anilinonaphthalene-1-sulfonate,in sonicated chloroplasts also showed the pH- or salt-inducedchanges and confirmed the interpretation above. From the rate constant for ferricyanide reduction, electricalpotential difference of the membrane surface with respect tothe bulk aqueous phase was estimated by assuming potential-inducedchanges in the ferricyanide concentration at the membrane surface.A potential of –25––30 mV and a surface densityof 1 negative charge per 12–22 chlorophylls were estimatedat pH 7.5 under low salt conditions. This potential was reducedby salt addition and changed the sign to positive at low pH(+17 mV at pH 4.9). The effect of the surface potential in photosynthetic energyconversion is discussed. (Received September 5, 1977; )     

Low dielectric permittivity of water at the membrane interface: effect on the energy coupling mechanism in biological membranes

Protonmotive force (the transmembrane difference in electrochemical potential of protons, ) drives ATP synthesis in bacteria, mitochondria, and chloroplasts. It has remained unsettled whether the entropic (chemical) component of relates to the difference in the proton activity between two bulk water phases (deltapH(B)) or between two membrane surfaces (deltapH(S)). To scrutinize whether deltapH(S) can deviate from deltapH(B), we modeled the behavior of protons at the membrane/water interface. We made use of the surprisingly low dielectric permittivity of interfacial water as determined by O. Teschke, G. Ceotto, and E. F. de Souza (O. Teschke, G. Ceotto, and E. F. de Sousa, 2001, PHYS: Rev. E. 64:011605). Electrostatic calculations revealed a potential barrier in the water phase some 0.5-1 nm away from the membrane surface. The barrier was higher for monovalent anions moving toward the surface (0.2-0.3 eV) than for monovalent cations (0.1-0.15 eV). By solving the Smoluchowski equation for protons spreading away from proton "pumps" at the surface, we found that the barrier could cause an elevation of the proton concentration at the interface. Taking typical values for the density of proton pumps and for their turnover rate, we calculated that a potential barrier of 0.12 eV yielded a steady-state pH(S) of approximately 6.0; the value of pH(S) was independent of pH in the bulk water phase under neutral and alkaline conditions. These results provide a rationale to solve the long-lasting problem of the seemingly insufficient protonmotive force in mesophilic and alkaliphilic bacteria.     

Some physicochemical properties of plasma membrane vesicles.

The plasma membranes of many animal cells can be disrupted into small sealed vesicles that can be purified centrifugally and utilized for studies on membrane transport. The vesicles behave as micro-osmometers. However, the presence of charges fixed at the internal and external surfaces of the membrane walls produce pH levels at these surfaces that deviate considerably from bulk pH. Transverse symmetry of charge distribution further leads to transverse asymmetry of surface pH. Finally, charges fixed at the internal membrane surface produced significant Donnan osmotic effects that depend upon membrane composition and ionic environment.     

Physical determinants of β-barrel membrane protein folding in lipid vesicles

The spontaneous folding of two Neisseria outer membrane proteins, opacity-associated (Opa)(60) and Opa(50) into lipid vesicles was investigated by systematically varying bulk and membrane properties. Centrifugal fractionation coupled with sodium dodecyl sulfate polyacrylamide gel electrophoresis mobility assays enabled the discrimination of aggregate, unfolded membrane-associated, and folded membrane-inserted protein states as well as the influence of pH, ionic strength, membrane surface potential, lipid saturation, and urea on each. Protein aggregation was reduced with increasing lipid chain length, basic pH, low salt, the incorporation of negatively charged guest lipids, or by the addition of urea to the folding reaction. Insertion from the membrane-associated form was improved in shorter chain lipids, with more basic pH and low ionic strength; it is hindered by unsaturated or ether-linked lipids. The isolation of the physical determinants of insertion suggests that the membrane surface and dipole potentials are driving forces for outer membrane protein insertion and folding into lipid bilayers.     

A model for the stimulation of taste receptor cells by salt.

A taste cell mucosal surface is regarded as a planar region containing bound anionic sites and openings to ionic channels. It is assumed that the bulk aqueous properties of the exterior phase are not continuous with the surface but terminate at a plane near the surface. The region between the (Stern) plane and the membrane is regarded as having a lower dielectric constant than bulk water. This fact admits the possibility of ion pair formation between fixed sites and mobile cations. Mobile ion pairs entering the region may also bind to a fixed anionic site. Thus, it is assumed that mobile cations and ion pairs are potential determining species at the surface. Binding cations neutralizes surface charges, whereas binding mobile ion pairs does not. This competition accounts for the observed anion effect on stimulation of tast receptors by sodium salts. The potential profile is constructed by superimposing the phase boundary potentials with an ionic diffusion potential across the membrane. The model accounts for the anion effect on receptor potential, pH effects, the reversal of polarity when cells are treated with FeCl3, and the so-called "water reponse," depolarization of the taste cell upon dilution of the stimulant solution below a critical lower limit. The proposed model does not require both bound cationic and anionic receptors, and further suggests that limited access to a Stern-like region continuous with membrane channels may generally serve to control transport of ions.     

Spiroplasma membrane lipids.

Membranes of six spiroplasma strains belonging to different Spiroplasma species and subgroups were isolated by a combination of osmotic lysis and sonication in the presence of EDTA to block endogenous phospholipase activity. Analysis of membrane lipids showed that in addition to free and esterified cholesterol the spiroplasmas incorporated exogenous phospholipids from the growth medium. Sphingomyelin was preferentially incorporated from phosphatidylcholine-sphingomyelin vesicles or from the serum used to supplement the growth medium. Palmitate was incorporated better than oleate into membrane lipids synthesized by the organisms during growth. The major phospholipid synthesized by the spiroplasmas was phosphatidylglycerol. The positional distribution of the fatty acids in phosphatidylglycerol of Spiroplasma floricola resembled that found in Mycoplasma species, in which the saturated fatty acids prefer position 2 in the glycerol backbone and not position 1 as found in Acholeplasma species and elsewhere in nature. Electron paramagnetic resonance analysis of spin-labeled fatty acids incorporated into S. floricola membranes exhibited homogeneous single-component spectra without immobilized regions. The S. floricola membranes were more rigid than those of Acholeplasma laidlawii and less rigid than those of Mycoplasma gallisepticum.     

Proton transfer dynamics at the membrane/water interface: dependence on the fixed and mobile pH buffers, on the size and form of membrane particles, and on the interfacial potential barrier

Crossing the membrane/water interface is an indispensable step in the transmembrane proton transfer. Elsewhere we have shown that the low dielectric permittivity of the surface water gives rise to a potential barrier for ions, so that the surface pH can deviate from that in the bulk water at steady operation of proton pumps. Here we addressed the retardation in the pulsed proton transfer across the interface as observed when light-triggered membrane proton pumps ejected or captured protons. By solving the system of diffusion equations we analyzed how the proton relaxation depends on the concentration of mobile pH buffers, on the surface buffer capacity, on the form and size of membrane particles, and on the height of the potential barrier. The fit of experimental data on proton relaxation in chromatophore vesicles from phototropic bacteria and in bacteriorhodopsin-containing membranes yielded estimates for the interfacial potential barrier for H(+)/OH(-) ions of approximately 120 meV. We analyzed published data on the acceleration of proton equilibration by anionic pH buffers and found that the height of the interfacial barrier correlated with their electric charge ranging from 90 to 120 meV for the singly charged species to >360 meV for the tetra-charged pyranine.