Protein lateral distribution in lipid bilayer membranes

We analyse recent ESR measurements on Ca²⁺ ATPase and Myelin proteolipid apoprotein reconstituted in phosphatidylcholine bilayer membranes. Our intention is to discover whether the measurements indicate significant protein-protein repulsive or attractive interactions. In order to do so we have studied a model of a lipid bilayer membrane containing transbilayer proteins. It represents the proteins by hexagons moving on a triangular lattice interacting via an energy E ₀ which can be attractive, repulsive or zero. The last-named represents the random case studied earlier. We find that all of the Ca²⁺ ATPase data is best described either by the random model or one in which there is always at least one layer of lipid chains between every pair of proteins. We find that all of the Myelin PLA data is best described by a random distribution of hexamers and not by an annulus model of hexamers. We suggest measurements that can be done in order to unambiguously settle the question of whether these systems are best described by a random-type model or an annulus-type model.Abbreviations PC phosphatidylcholine - DMPC dimyristoyl PC - DPPC dipalmitoyl PC - EYPC egg yolk PC - 14-PCSL 1-acyl-2-[14-(4,4-dimethyloxazolidine-N-oxyl)steroyl]-sn-glycero-3-phosphocholine - DPH 1,6-diphenyl-1,3,5-hexatriene - PLA proteolipid apoprotein - ESR electron spin resonance - T _c temperature of main lipid phase transition Work supported by NSERC of Canada     

Deducing the lateral distribution of proteins in lipid bilayer membranes

We consider four models of the lateral distribution of proteins in lipid bilayer membranes and study the fraction of lipids which are adjacent to at least one protein (adjacent lipids) and how this quantity depends upon protein concentration. The models are (i) hard hexagons free to move from one lattice site to another; (ii) hard disks moving on a continuum; (iii) a mixture of two sizes of nearly-hard disks moving on a continuum; (iv) a modification of (ii). The hexagons or disks represent proteins, while unocupied lattice sites or the remainder of the continuum represents lipids. In (iii) large disks represent proteins and small disks represent lipids. In (iv) some of the continuum between pairs of disks, where packing defects might occur, is not occupied by lipids. We find that an analytical expression for the adjacent lipids (Hoffmann et al. 1981), which is in excellent agreement with the results of the Hexagon model (i), breaks down at a packing density of f _A0.805, and we show by considering the hexagon pair correlation function, that this indicates the onset of random close packing, and that a transition to ordered close packing occurs at f _A=0.866. We thus obtain an operational definition for a random distribution of hexagons: distributions of packing densities0.805. We show that the Disk model (ii) gives results for adjacent lipids that are greater than the Hexagon model and compare these results to the Two Disk model (iii) which gives a result substantially less than the Hexagon model (Mountain et al. 1986). We show that the Modified Disk model (iv) gives results in essential agreement with the Hexagon model except for f _A0.77. Finally we discuss the general appearance of the motion restricted ESR spectrum and conclude that, of these four models, the Modified Disk or the Hexagon models best account for the data. We discuss why this is so with reference to the representation of a 3-dimensional membrane by a 2-dimensional plane.Abbreviations ESR Electron Spin Resonance     

Quantitative characterization of the lateral distribution of membrane proteins within the lipid bilayer.

The dependence of the lateral distribution of membrane proteins on the size, protein/lipoid molar ratio, and the magnitude of the interaction potentials has been investigated by computer modeling protein-lipid distributions with Monte Carlo calculations. These results have allowed us to develop a quantitative characterization of the distribution of membrane proteins and to correlate these distributions with experimental observables. The topological arrangement of protein domains, protein plus annular lipid domains, and free lipid domains is described in terms of radial distribution, pair connectedness, and cluster distribution functions. The radial distribution functions are used to measure the distribution of intermolecular distances between protein molecules, whereas the pair connectedness functions are used to estimate the physical extension of compositional domains. It is shown that, at characteristic protein/lipid molar ratios, previously isolated domains become connected, forming domain networks that extend over the entire membrane surface. These changes in the lateral connectivity of compositional domains are paralleled by changes in the calculated lateral diffusion coefficients and might have important implications for the regulation of diffusion controlled processes within the membrane.     

Electrical conductivity in lipid bilayer membranes induced by pentachlorophenol.

Electrical conductivity induced in thin lipid bilayer membranes by pentachlorophenol has been studied. The membranes were formed from phosphatidyl choline, phosphatidyl ethanolamine, or phosphatidyl glycerol and various amounts of cholesterol. The position and the magnitude of the maximum of the conductivity vs. pH curve depend on the type of lipids and cholesterol content. At low pentachlorophenol concentrations and low pH the concentration dependence of conductivity is quadratic and becomes linear at higher pH. Above 10(-5) M of pentachlorophenol the concentration dependence of the membrane conductivity tends to saturate. Presence of pentachlorophenol enhances membrane transport of nonactin-K+ complex. Increase of cholesterol content increases pentachlorophenol induced conductivity in all membranes and shifts the conductivity toward lower pH. For phosphatidyl choline the largest rate of change of membrane conductivity with cholesterol occurs at 1:1 phospholipid to cholesterol molar ratio. Pentachlorophenol is found to be a class II uncoupler and the experimental results are consistent with the hypothesis that the membrane permeable species are dimers formed by combination of neutral and dissociated pentachlorophenol molecules. Several schemes of membrane conduction, including dimer formation in the aqueous phase as well as at the membrane-water interface have been considered. Arguments are given in favor of the formation of dimers within the membrane surface.     

Quantification of lipid bilayer effective microviscosity and fluidity effect induced by propofol

Electron spin resonance (ESR) spectroscopy with nitroxide spin probes was used as a method to probe the liposome microenvironments. The effective microviscosities have been determined from the calibration of the ESR spectra of the probes in solvent mixtures of known viscosities. In the first time, by measuring ESR order parameter (S) and correlation time (tau(c)) of stearic spin probes, we have been able to quantify the value of effective microviscosity at different depths inside the liposome membrane. At room temperature, local microviscosities measured in dimyristoyl-l-alpha phosphatidylcholine (DMPC) liposome membrane at the different depths of 7.8, 16.95, and 27.7 A were 222.53, 64.09, and 62.56 cP, respectively. In the gel state (10 degrees C), those microviscosity values increased to 472.56, 370.61, and 243.37 cP. In a second time, we have applied this technique to determine the modifications in membrane microviscosity induced by 2,6-diisopropyl phenol (propofol; PPF), an anaesthetic agent extensively used in clinical practice. Propofol is characterized by a unique phenolic structure, absent in the other conventional anaesthetics. Indeed, given its lipophilic property, propofol is presumed to penetrate into and interact with membrane lipids and hence to induce changes in membrane fluidity. Incorporation of propofol into dimyristoyl-l-alpha phosphatidylcholine liposomes above the phase-transition temperature (23.9 degrees C) did not change microviscosity. At 10 degrees C, an increase of propofol concentration from 0 to 1.0 x 10(-2) M for a constant lipid concentration mainly induced a decrease in microviscosity. This fluidity effect of propofol has been qualitatively confirmed using merocyanine 540 (MC540) as lipid packing probe. Above 10(-2) M propofol, no further decrease in microviscosity was observed, and the microviscosity at the studied depths (7.8, 16.95, and 27.7 A) amounted 260.21, 123.87, and 102.27 cP, respectively. The concentration 10(-2) M was identified as the saturation limit of propofol in dimyristoyl-l-alpha phosphatidylcholine liposomes.     

Effects of uranyl ions on lipid bilayer membranes

Uranyl ions (UO₂²⁺) stabilize black lipid membranes (BLM's) as inferred from the doubling of the breakdown voltage and from a considerable increase in the lifetime of the BLM's. These effects are observed also in BLM's made of mono-olein and of oxidized cholesterol. The lytic effect of lysolecithin is significantly reduced in the presence of UO₂²⁺. Uranyl ions adsorb to the interface of BLM's made of phosphatidylcholine (PC) with a dissociation constant of about 3 : 10^?6 M and thereby charge the interface of the membrane and attain almost stoichiometric binding of one molecule of uranyl ion per one molecule of PC at 1 M ionic strength and 20 μM of UO₂²⁺. The membrane conductance induced by ionophores is considerably reduced by UO₂²⁺ and it is inferred by various tests that this is due to the charging of the interface and not to changes in membrane fluidity.     

Spontaneous lipid bilayer transmembrane electrical oscillations induced by concanavalin A-polysaccharide interaction

Potassium ion currents through bilayer lipid membranes were modified by the membrane-surface reaction of concanavalin A and the polysaccharides dextran and glycogen. Aggregative reaction with glycogen occasionally induced spontaneous periodic ion current fluctuations with cycle times of minutes and durations of over one hour. Different electrochemical characteristics were observed between large planar lipid membranes and filter paper supported membranes, providing an indication that the aqueous unstirred surface layer participates in the control of the surface aggregative event. Lipid chemical composition was implicated in the development of spontaneous oscillations.     

Ionic channels induced by surfactin in planar lipid bilayer membranes.

Surfactin is a lipopeptide produced by certain strains of Bacillus subtilis and has potent surface activity. Here, we present the first results showing that ion-conducting pores can be formed by surfactin in artificial lipid membranes. With a low aqueous concentration of surfactin (1 microM) and a restricted membrane area (5.10(-5) cm2) we observed conductance jumps that indicate the formation of individual ionic channels in the presence of K+, Rb+, Cs+, Na+ or Li+ chlorides. Although for every salt concentration (Ci), the distribution in amplitude of the conductance steps (lambda i) may be rather broad, there is always a step amplitude which is more frequent than the others. In addition, the channels corresponding to this most frequent step amplitude are the longest in duration. For Ci = 1 M, the cationic selectivity sequence deduced from these most frequent events is K+ greater than Rb+ greater than Na+ greater than Cs+ = Li+ with respective values for lambda Mi: 130, 110, 80 and 30 pS. In KCl solutions lambda MKCl increases as a function of Ci for low Ci, and shows a plateau for Ci greater than 0.5 M. When measured on larger area membranes (10(-2)cm2) with 1 M solutions of the monovalent salts KCl, NaCl, RbCl and CsCl or the divalent salt CaCl2, the macroscopic low voltage conductance (G0) increases with a slope of 2 on a log-log plot as a function of surfactin concentration. These results demonstrate that surfactin produces selective cationic channels in lipid bilayer membranes and suggest that at higher salt concentration, a dimer is involved in this functional channel-forming process.     

Pressure variation of the lateral diffusion in lipid bilayer membranes

A pressure-induced decrease of the lateral diffusion in pure and cholesterol containing phosphatidylcholine bilayer membranes has been determined by the excimer formation technique using pyrene as probe molecule. The experimental results at pressures up to 150 bars are described satisfactorily by the free volume theory of a molecular transport in liquids. A pressure increase of extrapolated 575 bars decreases the lateral diffusion of lipids by a factor of two in pure dipalmitoylphosphatidylcholine membranes. Higher pressures are necessary to induce the same effect in cholesterol containing membranes. This result is interpreted by the condensing effect of cholesterol in fluid bilayer membranes.     

Size distribution of barrel-stave aggregates of membrane peptides: influence of the bilayer lateral pressure profile

Some membrane peptides, such as Alamethicin, form barrel-stave aggregates with a broad probability distribution of size (number of peptides in the aggregate). This distribution has been shown to depend on the characteristics of the lipid bilayer. A mechanism for this influence is suggested, in analogy to earlier work on the effects of changes in bilayer composition on conformational equilibria in membrane proteins, that is based on coupling of shifts in the distribution of lateral pressures in the bilayer to depth-dependent changes in the lateral excluded area that accompanies the formation of an aggregate. Thermodynamic analysis is coupled with a simple geometric model of aggregates of kinked cylindrical peptides and with results of previously calculated lateral pressure distributions to predict the effects of changes in bilayer characteristics on aggregate size distributions, in qualitative agreement with experimental results.     

Electrically silent anion transport through bilayer lipid membrane induced by tributylin and triethyllead

Summary The method of the measurement of the nonelectrogenic fluxes of hydrogen (or hydroxyl) ions (J _H) based on the local proton gradients formation in the unstirred layers near a bilayer lipid membrane (BLM) is applied for recording the nonelectrogenic anion/OH^– exchange on BLM induced by tributyltin (TBT) and a novel carrier (Hager, A., Moser, I., & Berthold, W. 1987.Z. Naturforsch.,42C1116–1120), triethyllead (TEL). This method has been used previously for measuring the cation fluxes through BLM. TBT and TEL are shown to be equally efficient in the induction of Cl^–/OH^– exchange.J _H induced by TBT is constant at 4J _H decreases at pH<4 and pH>7. Both ionophores have a transport sequence: I^–> Br^–>Cl^–>F^–. The quatitative measurements reveal that TEL better discriminates these four anions than TBT. It is concluded that this method may prove helpful in a search and study of anion/OH^–-exchangers isolated from natural membranes.     

Study of conductance changes of bilayer lipid membrane induced by electric field

Changes in the bilayer lipid membrane (BLM) conductance induced by electric field were studied. BLMs were formed from diphytanoylphosphocholine (DPhPC) solution in squalene. Certain time after a constant voltage (200-500 mV) was applied to the BLM in the voltage-clamp mode, the BLM conductance started to grow up to approximately 10 nS until the BLM ruptured. The conductance often changed abruptly (with the front duration of less than 33 micros) and then stabilized for a relatively long time (up to 10; 300 ms on average) thus resembling the ion channel activity. The mean amplitude of conductance steps was 650 pS. However, in some cases a slow conductance drift was recorded. When N-methyl-D-glucamine/glutamate ions were used instead of KCl, the conductance changes became 5 times smaller. We suggest that formation in the BLM of single pores approximately 1 nm in diameter should result in the observed changes in BLM conductance. The BLM conductance growth was due to consecutive opening of several such pores. When the electric field amplitude was abruptly decreased (down to 50-100 mV), the conductance dropped rapidly to the background value. When we increased the voltage again, the BLM conductance right after the increase depended on the time BLM spent under "weak" electric field. If this time exceeded 500 ms, the conductance was at the background level, but when the time was diminished, the conductance reached the value recorded before the voltage decrease. These data imply that the closure of the pores should lead to the formation in BLM of small defects (prepores) that can be easily transformed into pores when the voltage is increased. The lifetimes of such prepores did not exceed 500 ms.     

The alterations of lipid bilayer fluidity induced by newly synthesized phenothiazine derivative

Using fluorescence spectroscopy, calorimetry and ESR the interactions of the phenothiazine derivative 2-trifluoromethyl-10-(4-[methylsulfonylamid]buthyl)-phenothiazine (FPhMS) with lipids were studied. Calorimetry showed biphasic effect of FPhMS on main phase transition of DPPC. At molar ratios up to 0.06 drug induced decrease of transition temperature and enthalpy, while at higher concentrations it caused subsequent increase of these parameters. For all concentrations studied we observed gradual broadening of transition peaks. Fluorescence polarization revealed that in FPhMS/lipid mixtures, order in bilayers is decreased in the gel state and increased in the liquid crystalline state. ESR experiment showed that at molar ratio of 0.06, FPhMS reduces the mobility of spin probes located in both polar and hydrophobic regions. Comparing observed effects with those reported for cholesterol/lipid mixtures, we conclude that at higher concentrations FPhMS presumably induces a new mode of bilayer packing. This structure is less co-operative than an unperturbed bilayer, but locally the mobility of lipid molecules is decreased.     

Phase transition kinetics of lipid bilayer membranes studied by time-resolved pressure perturbation calorimetry

The relaxation kinetics of aqueous lipid dispersions after a pressure jump (p-jump) was investigated using time-resolved pressure perturbation calorimetry (PPC). Analysis of the calorimetric response curves by deconvolution with the instrumental response function gives information about slow processes connected with the lipid phase transition. The lipid transition from the gel to the liquid-crystalline state was found to be a multi-step process with relaxation constants in the seconds range resolvable by time-resolved PPC and faster processes with relaxation times shorter than ca. 5 s that could not be resolved by the instrument. The faster processes comprise ca. 50% of the total heat uptake at the transition midpoint. This is the first calorimetric measurement showing the multi-step nature of the transition. The results are in good agreement with data obtained with other detection methods and with molecular modelling experiments describing the transition as a multi-step process with nucleation and growth steps.     

Strain, stress and energy in lipid bilayer induced by electrostatic/electrokinetic forces

Lipid bilayer was deformed by the electrostatic/electrokinetic forces induced by the fixed charges on the top monolayer-solution interface. The strains, stresses and energy were simulated using finite element method. The elastic moduli of the heads were four times greater than those of tails sections, but were individually isotropic. The physics of the situation was evaluated using a coupled system of linear elastic equations and electrostatic-electrokinetic (Poisson-Nernst-Planck) equations. The Coulomb force (due to fixed charges in the electric field), and the dielectric force (due to uneven electric field and the solution-membrane permittivity mismatch) bend the membrane, but unevenly. Whereas the bottom monolayer extends vertically (towards charged surface), the top monolayer compresses. In contrast the top monolayer extends horizontally, but the bottom monolayer compresses. The horizontal normal stress is higher in the heads than in the tails sections, but is similar in two monolayers, whereas the vertical normal stress is small. The horizontal normal stress is associated with horizontal normal strain, and vertical with both vertical and horizontal strain. Surprisingly, the shear stress (an indicator where the membrane will deform), is greater in the tails sections. Finally, the elastic energy (which is clearly greater in the heads sections) is dominated by its horizontal component and peaks in the middle of the membrane. The shear component dominates in the tails sections, and is minimal in the membrane center. Even spatially uniform external force thus leads to complex membrane deformation and generates complex profiles of stress and elastic energy.     

Globoside with spin-labelled fatty acid: bilayer lateral distribution and immune recognition

We have critically addressed the question of lateral distribution of glycolipids in bilayer membranes, and the effect of glycolipid fatty acid chain length upon such distribution. For this purpose we synthesised the complex neutral glycosphingolipid, globoside, with spin-labelled fatty acid. Base hydrolysis to remove the natural fatty acid was found to deacetylate the GalNAc residue concomitantly, necessitating application of the synthetic route described for gangliosides by Neuenhofer et al. (Biochemistry 24, 525-532 (1985)). Globosides were produced with 18-carbon and 24-carbon fatty acids bearing a spin label at the C-16 position. Spin-labelled globosides were incorporated at 2 and 10 mol% into rigid, highly cooperative bilayer matrices of 1,2-dipalmitoylglycerophosphocholine (DPPC) and also into semi-fluid, non-cooperative membranes of DPPC/cholesterol. Recorded electron paramagnetic resonance (EPR) spectra were analysed by comparison with a library of standards representing samples of known composition. Spectra were manipulated using a computer program which permitted linear combination of standards to stimulate coexistence of laterally separated domains of different composition. The most important conclusions were as follows: (1) at least 80% of the globoside was definitely not confined to domains highly enriched in glycolipid, although there was evidence of binary-phase separation in the rigid DPPC/globoside matrix; (2) the presence of 33 mol% cholesterol reduced the evidence of globoside phase separation; (3) there was remarkably little difference in results whether the globoside fatty acid chain length was similar to that of the phospholipid host matrix or eight carbons longer. Temperature profiles derived over the phase-transition region of DPPC using spin-labelled globoside or an unattached amphiphilic spin label were consistent with these findings. The same systems lent themselves to consideration of the role of glycolipid fatty acid chan length and cholesterol in determining glycolipid crypticity in membranes: (1) polyclonal anti-globoside IgG bound to globoside in DPPC liposomes without inducing agglutination. (2) The same antibodies did agglutinate DPPC/cholesterol liposomes bearing globoside. (3) The effect of cholesterol probably was upon glycolipid dynamics or attitude in the membrane, rather than upon distribution. (4) These observations were basically unaffected by the choice of 18-carbon vs. 24-carbon glycolipid fatty acids.(ABSTRACT TRUNCATED AT 400 WORDS)     

Structural rearrangements induced by glycerol increase the permeability of bilayer lipid membranes for amphotericin

It has been shown that structural rearrangements induced by glycerol in bilayer lipid membranes (BLM) containing cholesterol facilitate the transmembrane transport of amphotericin B molecules in the direction of glycerol gradient. The addition of amphotericin B to the same side with glycerol results in a change in bilayer selectivity from the cation to the anion one. Besides, the final conductivity is blocked by tetraethylammonium from the solution with no amphotericin B added. It testifies to the transport of amphotericin molecules to the opposite side of the membrane. The transport effect depends on the cholesterol content in bilayer, ionic strength of the medium and slightly depends on temperature. It is concluded that transport of amphotericin B in such conditions differs from the diffusive one and is due to the formation of intermediate lipid phases in the course of structural rearrangements of bilayers.     

Effects of membrane composition and lipid structure on the photopolymerization of lipid diacetylenes in bilayer membranes

Molecules analogous to biological and synthetic lipids have been prepared with conjugated diacetylene moieties in the long alkyl chain. These lipid diacetylenes form bilayer structures when suspended in aqueous buffers. Ultraviolet light (254 nm) exposure initiates the polymerization of the diacetylenes in the lipid bilayer to give a fully conjugated, highly colored product. The reaction is topotactic, and its efficiency depends on the correct alignment of the monomeric units. Thus, the lipid diacetylenes are photopolymerizable if the hydrocarbon chains are in a regular lattice found at temperatures below the lipid transition temperature; polymerization is inhibited above this transition. The photopolymerization of a diacetylenic glycerophosphocholine in lipid bilayer membranes was observed in two-component mixtures with a nonpolymerizable lipid, either dioleoylphosphatidylcholine or distearoylphosphatidylcholine. The photochemical and thermochemical characteristics suggest that the diacetylenic glycerophosphocholine exists largely in separate domains in the mixed bilayers. Lipid diacetylenes analogous to a dialkyldimethylammonium salt and to a dialkyl phosphate have a plane of symmetry, which suggests that both chains penetrate equally into the bilayer. The photopolymerization of these symmetrical synthetic species is more than 10³-times more efficient than that of the diacetylenic glycerophosphocholine. These differences are interpretable in terms of the expected conformational preference of the lipid molecules.     

Interactions between two sheets of a bilayer membrane and its internal lateral pressure

We have modelled a phospholipid bilayer as two monolayer sheets which interact with each other by a coupling which depends upon the states of the lipid hydrocarbon chains in each sheet. We make use of a model (Georgallas and Pink 1982a) and its parameters, already used to study monolayer phase changes at the LC-LE transition, in order to study the lipid main transition. Although the monolayer coexistence curve can be calculated exactly, we have made use of high-temperature series expansions to calculate the critical point of the bilayer. We also present the results of computer simulations on triangular lattices for the pressure-area isotherms. We find: (i) the interaction between the sheets of a DPPC bilayer is about 1.5–2% of the maximum interaction within the plane of each sheet; (ii) the internal lateral pressure of a DPPC bilayer is about 30.5 dyne/cm; (iii) the bilayer transition enthalpy depends sensitively upon the coupling between the sheets. Should this coupling vary from sample to sample (due, possibly, to its preparation) then very different values of transition enthalpy may be measured. (iv) We present a rough rule-of-thumb for estimating the internal lateral pressure of a bilayer from a knowledge of the corresponding monolayer pressure-area isotherms.Abbreviations LC-LE liquid condensed — liquid expanded - DPPC dipalmitoylphosphatidylcholine - Q transition enthalpy Work supported in part by the Natural Sciences and Engineering Research Council of Canada