Fluorescence study on the interaction of a multiple antigenic peptide from hepatitis A virus with lipid vesicles

The interaction of the multiple antigenic peptide MAP4VP3 with lipid membranes has been studied by spectroscopic techniques. MAP4VP3 is a multimeric peptide that corresponds to four units of the sequence 110-121 of the capsid protein VP3 of hepatitis A virus. In order to evaluate the electrostatic and hydrophobic components on the lipid-peptide interaction, small unilamelar vesicles of different compositions, including zwitterionic dipalmitoylphosphatidylcholine (DPPC), anionic dipalmitoylphosphatidylcholine/phatidylinositol (DPPC:PI 9:1), and cationic dipalmitoylphosphatidylcholine/stearylamine (DPPC:SA 9.5:0.5), were used as membrane models. Intrinsic tryptophan fluorescence changes and energy transfer experiments show that MAP4VP3 binds to all three types of vesicles with the same stoichiometry, indicating that the electrostatic component of the interaction is not important for binding of this anionic peptide. Steady-state polarization experiments with vesicles labeled with 1,6-diphenyl-1,3,5-hexatriene or with 1-anilino-8-naphtalene sulphonic acid indicate that MAP4VP3 induces a change in the packing of the bilayers, with a decrease in the fluidity of the lipids and an increase in the temperature of phase transition in all the vesicles. The percentage of lipid exposed to the bulk aqueous phase is around 60% in intact vesicles, and it does not change upon binding of MAP4VP3 to DPPC vesicles, indicating that the peptide does not alter the permeability of the membrane. An increase in the amount of lipid exposed to the aqueous phase in cationic vesicles indicates either lipid flip-flop or disruption of the vesicles. Binding to DPPC vesicles occurs without leakage of entrapped carboxyfluorescein, even at high mol fractions of peptide. However, a time-dependent leakage is seen with cationic DPPC/SA and anionic DPPC/PI vesicles, indicating that the peptide induces membrane destabilization and not lipid flip-flop. Resonance energy transfer experiments show that MAP4VP3 leakage from cationic vesicles is due to membrane fusion, whereas leakage from anionic vesicles is not accompanied by lipid mixing. Results show that MAP4VP3 interacts strongly with the lipid components of the membrane, and although binding is not of electrostatic nature, the bound form of the peptide has different activity depending on the membrane net charge; thus, it is membrane disruptive in cationic and anionic vesicles, whereas no destabilizing effect is seen in DPPC vesicles.     

Fusion and phase separation monitored by lifetime changes of a fluorescent phospholipid probe

The sensitivity of the fluorescence lifetime of 1-palmitoyl-2-[[2-[4- (6-phenyl-trans-1,3,5-hexatrienyl)phenyl]ethyl]carbonyl]- 3-sn-phosphatidylcholine (DPHpPC) to its local concentration in lipid bilayers was used to monitor both lipid mixing and phase separation occurring during membrane vesicle fusion. Vesicles containing 2 mol % DPHpPC were mixed with a 10-fold excess of vesicles devoid of probe. Upon addition of a fusogen, mixing of bilayer lipids associated with fusion was followed as an increase in the fluorescence lifetime of DPHpPC. Ca2+-induced fusion of phosphatidylserine vesicles served to test the method and was shown to have an exponential half-time of 7 s. Phase separation (between the phosphatidylserine head groups of bulk lipid and the phosphatidylcholine head groups of the probe) was monitored by DPHpPC under the same conditions used to follow lipid mixing due to fusion. Phase separation was not significant until 10 min after Ca2+ addition and was completely reversible by disodium ethylenediaminetetraacetate addition. Vesicle aggregation induced by Ca2+ addition to mixed phosphatidylserine/phosphatidylcholine vesicles did not alter the DPHpPC lifetime, indicating that close association of vesicles did not promote intervesicular exchange of the probe. In addition, we have investigated the effects of CA2+ on the fluorescence properties of this probe and of the head-group-labeled fluorescent probes N-(4-nitro-2,1,3-benzoxadiazolyl)phosphatidylethanolamine and N-(lissamine Rhodamine B sulfonyl)dioleoyl-phosphatidylethanolamine, which are used in the fluorescence energy transfer assay of Struck et al.(ABSTRACT TRUNCATED AT 250 WORDS)     

Reconstituted P2/Myelin-Lipid Multilayers

A complex forms when bovine P2 protein is added to single-bilayer vesicles created by sonicating myelin lipids. The complex was studied by biochemical analysis, freeze-fracture (FF) and thin-section electron microscopy (EM), and by X-ray diffraction. Smaller amounts of P2 cause the vesicles to aggregate and fuse whereas larger amounts (greater than or equal to 4 wt%) cause multilayers to form. Binding saturates at 15 wt% P2. FF EM shows that large, flat multilayers form within 15 min of addition of P2. Only smooth fracture faces are seen, as expected for a peripheral membrane protein. X-ray diffraction shows a constant repeating distance in the multilayers: 86.0 +/- 0.7 A between the centers of bilayers in the range 4 wt% less than or equal to P2/(P2 + lipid) less than or equal to 15 wt%. Assuming a 53 A-thick bilayer, the space between bilayers is 33 A wide. This is a wider space than for myelin basic protein (MBP) (20-25 A wide). The respective widths are consistent with a compact, globular structure for P2 and a flattened shape for MBP. Calculated electron-density profiles of the lipids with and without P2 reveal the protein largely in the interbilayer spaces, with a small part possibly inserted into the lipid headgroup layers. The different proportions of P2 in the sciatic nerve of various species are tentatively correlated with the different average widths observed by X-ray diffraction for the cytoplasmic space (major period line) between bilayers in the respective sciatic myelins.     

Fusion of negatively charged liposomes with clathrin-uncoated vesicles

The interaction of lipid vesicles with uncoated vesicles from bovine brain has been studied by fluorescence energy transfer between fluorescent lipid analogs (NBD-PE, Rh-DOPE), by loss of fluorescence self-quenching (NBD-PE, carboxyfluorescein) and by freeze-fracture electron microscopy. The fluorescence techniques monitor the mixing of membranous lipids and the induced release of encapsulated material. The results demonstrate a mixing of the negatively charged lipid (PA, PS) vesicles with the uncoated vesicles. In parallel with the lipid mixing a release of intravesicularly encapsulated material takes place. Lipid vesicles composed of zwitterionic lipids (PC, DOPC, PC:PE) do not specifically interact with uncoated vesicles. The electron micrographs reveal single fusion events. Studies on the kinetics are consistent with a fusional mechanism of the negatively charged lipid vesicles with uncoated vesicles.     

Binding of phospholipids to beta-Lactoglobulin and their transfer to lipid bilayers

The bovine milk lipocalin, beta-Lactoglobulin (beta-LG), has been associated with the binding and transport of small hydrophobic and amphiphilic compounds, whereby it is proposed to increase their bioavailability. We have studied the binding of the fluorescent phospholipid-derivative, NBD-didecanoylphosphatidylethanolamine (NBD-diC10PE) to beta-LG by following the increase in amphiphile fluorescence upon binding to the protein using established methods. The equilibrium association constant, KB, was (1.2+/-0.2)x10(6) M(-1) at 25 degrees C, pH 7.4 and I=0.15 M. Dependence of KB on pH and on the monomer-dimer equilibrium of beta-LG gave insight on the nature of the binding site which is proposed to be the hydrophobic calyx formed by the beta-barrel in the protein. The monomer-dimer equilibrium of beta-LG was re-assessed using fluorescence anisotropy of Tryptophan. The equilibrium constant for dimerization, KD, was (7.0+/-1.5)x10(5) M(-1) at 25 degrees C, pH 7.4, and 0.15 M ionic strength. The exchange of NBD-diC10PE between beta-LG and POPC lipid bilayers was followed by the change in NBD fluorescence. beta-LG was shown to be a catalyst of phospholipid exchange between lipid bilayers, the mechanism possibly involving adsorption of the protein at the bilayer surface.     

Properties of ion channels formed by Staphylococcus aureus delta-toxin

The delta-toxin of Staphylococcus aureus has been investigated in terms of its potential to form ion channels in planar lipid bilayers formed at the tip of patch electrodes. Channel formation has been shown to occur for delta-toxin concentrations in the range 0.1 to 2.0 microM. In 0.5 M KCl, two major classes of channels were seen--'small' with conductances of 70-100 pS, and 'large' with a conductance of approx. 450 pS. Current-voltage relationships for lipid bilayers containing several delta-toxin channels revealed both voltage-dependent and independent components to channel gating. Reversal potential measurements showed the channels to be cation selective. In the presence of 3.0 M KCl, the channel gating kinetics were complex, with multiple open and closed states. The results are interpreted in terms of a model for the channel consisting of a hexameric cluster of alpha-helical delta-toxin molecules.     

Membrane interaction of a beta-structure-forming synthetic peptide comprising the 116-139th sequence region of the cytotoxic protein alpha-sarcin.

alpha-Sarcin is a cytotoxic protein that strongly interacts with acid phospholipid vesicles. This interaction exhibits a hydrophobic component although alpha-sarcin is a highly polar protein. A peptide comprising the amino acid sequence corresponding to the 116-139th segment of the alpha-sarcin cytotoxin has been synthesized by a standard fluoren-9-yl-methoxycarbonyl-based solid phase method. Its primary structure is: (116)-NPGPARVIYTYPNKVFCGIIAHTK-(139). Two beta-strands have been predicted in this region of alpha-sarcin, where the less polar stretches of the protein are found. The synthetic peptide interacts with negatively charged large unilamellar vesicles of either natural or synthetic phospholipids. An apparent fragmentation of the vesicles is produced by the peptide based on electron microscopy studies. The peptide promotes leakage of the intravesicular aqueous contents and lipid mixing of bilayers. The packing of the phospholipid molecules is greatly perturbed by the peptide, as deduced from the drastic changes induced by the peptide in cooperative properties associated with the phase transition of the bilayers. At saturating peptide/phospholipid ratios, the phase transition of dimyristoylphosphatidylglycerol vesicles is abolished. All of these effects are saturated at about 0.3 peptide/lipid molar ratio. The peptide adopts a mostly random structure in aqueous solution. A conformation composed of a high proportion of antiparallel beta-sheet is induced as a consequence of the interaction with the phospholipid vesicles in opposition to trifluoroethanol that promotes alpha-helical peptide structures, as deduced from circular dichroism measurements.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fatty acid-albumin complexes and the determination of the transport of long chain free fatty acids across membranes

Understanding the mechanism that governs the transport of long chain free fatty acids (FFA) across lipid bilayers is critical for understanding transport across cell membranes. Conflicting results have been reported for lipid vesicles; most investigators report that flip-flop occurs within the resolution time of the method (<5 ms) and that dissociation from the membrane is rate limiting, while other studies find that flip-flop is rate limiting and on the order of seconds. We have reinvestigated this problem and find that the methods used in studies reporting rapid flip-flop have not been interpreted correctly. We find that accurate information about transport of FFA across lipid vesicles requires that FFA be delivered to the vesicles as complexes with albumin (BSA). For example, we find that stopped-flow mixing of uncomplexed FFA with small unilamellar vesicles (SUV) containing pyranine yields the very fast influx rates reported previously (>100 s(-1)). However, these influx rates increase linearly with lipid vesicle concentration and can therefore not, as previously interpreted, represent flip-flop. In contrast, measurements of influx rates in SUV and giant unilamellar vesicles performed with oleate-BSA complexes reveal no dependence on vesicle concentration and yield influx rate constants of approximately 4 and approximately 0.5 s(-1), respectively. Rate constants for efflux and dissociation were determined from the transfer of oleate from vesicles to BSA and reveal similar influx and efflux but dissociation rate constants that are approximately 5-10-fold greater. We conclude that flip-flop is rate limiting for transport of FFA across lipid vesicles and slows with an increasing radius of curvature. These results, in contrast to those reporting that flip-flop is extremely fast, indicate that the lipid bilayer portion of biological membranes may present a significant barrier to transport of FFA across cell membranes.     

Aggregation, lipid exchange, and metastable phases of dimyristoylphosphatidylethanolamine vesicles

A new fluorescent lipid analogue, bimanephosphatidylcholine, has been synthesized for use in lipid bilayers. This probe is well suited as an energy-transfer donor with N-(7-nitro-2,1,3-benzoxadiazol-4-yl)phosphatidylethanolamine as the acceptor. Dimyristoylphosphatidylethanolamine vesicles are prepared by sonication at pH 9 and characterized by electron microscopy and other methods. Resonance energy transfer between separately labeled donor and acceptor vesicles is monitored during HCl-induced aggregation to determine the kinetics of lipid randomization. Light scattering is also monitored to measure the kinetics of aggregation. The light scattering shows a marked reversal with NaOH while the energy transfer does not, indicating lipid exchange during a reversibly aggregated state; the extent of energy transfer suggests that only lipids in the outer monolayers exchange. The gel to liquid-crystalline phase transition temperature in HCl-treated vesicles is found to be 47 degrees C with diphenylhexatriene. The initial sonicated dispersion does not show a sharp phase transition. In vesicles labeled with both donor and acceptor probes, a small, irreversible increase in energy transfer is obtained upon lowering and then restoring the pH. These results suggest a metastable phase in the sonicated vesicles containing a randomized distribution of lipid and probes within the bilayers; the thermodynamically favored phase, whose formation is triggered by the pH shock, contains domains within which the probe lipids are more highly concentrated.     

Bilayer curvature and certain amphipaths promote poly(ethylene glycol)-induced fusion of dipalmitoylphosphatidylcholine unilamellar vesicles.

Unilamellar vesicles of varying and reasonably uniform size were prepared from 1,2-dipalmitoyl-3-sn-phosphatidylcholine (DPPC) by the extrusion procedure and sonication. Quasi-elastic light scattering was used to show that different vesicle preparations had mean (Z-averaged) diameters of 1340, 900, 770, 630, and 358 A (sonicated). Bilayer-phase behavior as detected by differential scanning calorimetry was consistent with the existence of essentially uniform vesicle populations of different sizes. The response of these different vesicles to treatment with poly(ethylene glycol) (PEG) was monitored using fluorescence assays for lipid transfer, contents leakage, and contents mixing, as well as quasi-elastic light scattering. No fusion, as judged by vesicle contents mixing and change in vesicle size, was detected for vesicles of diameter greater than 770 A. The diameters of smaller vesicles increased dramatically when treated with high concentrations of PEG, although mixing of their contents could not be detected both because of their small trapped volumes and because of the extensive leakage induced in small vesicles by high concentrations of PEG. Lipid transfer was detected between vesicles of all sizes. We conclude the high bilayer curvature does encourage fusion of closely juxtaposed membrane bilayers but that highly curved vesicles appear also to rupture and form larger structures when diluted from high PEG concentration, a process that can be confused with fusion. Despite the failure of PEG to induce fusion of large, uncurved vesicles composed of a single phosphatidylcholine, these vesicles can be induced to fuse when they contain small amounts of certain amphiphathic compounds thought to play a role in cellular fusion processes. Thus, vesicles which contained 0.5 mol % L-alpha-lysopalmitoylphosphatidylcholine, 5 mol % platelet activating factor, or 0.5 mol % palmitic acid fused in the presence of 30%, 25%, and 20% (w/w) PEG, respectively. However, vesicles containing 1,2-dipalmitoyl-sn-glycerol, 1,2-dioleoyl-sn-glycerol, 1-oleoyl-2-acetyl-sn-glycerol, or monooleoyl-rac-glycerol at surface concentrations up to 5 mol % did not fuse in the presence or absence of PEG. There was no correlation between the abilities of these amphipaths to induce phase separation or nonlamellar phases and their abilities to support fusion of pure DPPC unilamellar vesicles in the presence of high concentrations of PEG. The results are discussed in terms of the type of disrupted lipid packing that could be expected to favor PEG-mediated fusion.     

Interaction of influenza M protein with viral lipid and phosphatidylcholine vesicles.

The M protein of influenza is the predominant structural component of the virus. The interactions of this protein with the viral lipid or with other proteins are not known. The ability of M to interact with viral or other lipids was investigated. Purified M was mixed with viral lipid or egg phosphatidylcholine and was incorporated into vesicles (i) by addition of sodium deoxycholate followed by dialysis or (ii) by sonication. Between 90 and 100% of the M became firmly associated with the lipid by either of these two methods, whereas nucleoprotein failed to associate with the vesicles. From association also occurred if M was mixed with performed vesicles. Most of the M attached to the vesicles could be hydrolyzed with proteolytic enzymes such as trypsin or thermolysin, except for a small fragment of about 5,000 daltons which remained associated with the lipid vesicles. The ability of fragments of M to interact with lipids was also investigated. Of 13 fragments produced by cleavage with cyanogen bromide, 3 specifically associated with lipid vesicles. The data indicate that a specific portion of the M molecule has a high affinity for lipid bilayers of various origins.     

Mechanism of poly(ethylene glycol)-induced lipid transfer between phosphatidylcholine large unilamellar vesicles: a fluorescent probe study

Experiments were performed to assess three possible mechanisms of poly(ethylene glycol) (PEG) induced rapid lipid transfer between large unilamellar vesicles composed of dioleoylphosphatidylcholine: (1) transfer between aggregated vesicles, (2) transfer through an aqueous medium of lowered dielectric constant, and (3) transfer via a PEG carrier. The results showed that close contact between vesicles as a result of PEG dehydration was largely responsible for the rapid lipid transfer observed in the presence of PEG. The rate and extent of lipid transfer were also examined at 10 wt % PEG and analyzed in terms of a two-state model especially developed to account for the initial rate of lipid transfer as followed by the fluorescence lifetime of DPHpPC as a fluorescent lipid probe. Analysis revealed that two rate processes were involved in DPHpPC transfer between bilayers, both in the absence and presence of PEG. Since the maximum extent of transfer was 50%, transbilayer diffusion of DPHpPC seemed not to contribute to either process. The fast process in the presence of PEG was identified as due to rapid interbilayer monomer diffusion between closely apposed vesicles, and, in the absence of PEG, as due to monomer diffusion through the aqueous phase. The origin of the slow process, in both cases, remains obscure. The Arrhenius activation energies (and entropies) for the initial rates at temperatures from 10 to 48 degrees C were 15.3 +/- 0.3 kcal/mol (-26.3 +/- 0.2 eu) and 10.6 +/- 0.5 kcal/mol (-16.1 +/- 0.3 eu) in the absence and presence of PEG, respectively. The slow process was invariant with temperature.(ABSTRACT TRUNCATED AT 250 WORDS)     

Formation of supported planar bilayers by fusion of vesicles to supported phospholipid monolayers.

A technique for the production of supported phospholipid bilayers by adsorption and fusion of small unilamellar vesicles to supported phospholipid monolayers on quartz is described. The physical properties of these supported bilayers are compared with those of supported bilayers which are prepared by Langmuir-Blodgett deposition or by direct vesicle fusion to plain quartz slides. The time courses of vesicle adsorption, fusion and desorption are followed by total internal reflection fluorescence microscopy and the lateral diffusion of the lipids in the adsorbed layers by fluorescence recovery after photobleaching. Complete supported bilayers can be formed with phosphatidylcholine vesicles at concentrations as low as 35 microM. However, the adsorption, fusion and desorption kinetics strongly depend on the used lipid, NaCl and Ca2+ concentrations. Asymmetric negatively charged supported bilayers can be produced by incubating a phosphatidylcholine monolayer with vesicles composed of 80% phosphatidylcholine and 20% phosphatidylglycerol. Adsorbed vesicles can be removed by washing with buffer. The measured fluorescence intensities after washing are consistent with single supported bilayers. The lateral diffusion experiments confirm that continuous extended bilayers are formed by the monolayer-fusion technique. The measured lateral diffusion coefficient of NBD-labeled phosphatidylethanolamine is (3.6 +/- 0.5) x 10(-8) cm2/s in supported phosphatidylcholine bilayers, independent of the method by which the bilayers were prepared.     

Characterization of the interaction of phospholipase A(2) with phosphatidylcholine-phosphatidylglycerol mixed lipids

The first requirement in the hydrolysis of phospholipid bilayers by phospholipase A(2) is the interaction of the enzyme with the bilayer surface. The catalytic ability of phospholipase A(2) has been shown to be extremely sensitive to the topology of the bilayer to which it binds and hydrolyzes. Phospholipid bilayer properties and composition such as unsaturation, charge, and the presence of reaction products are known regulators of the catalytic activity of phospholipase A(2) toward the phospholipids and influences the binding of enzyme to the membrane. We show in this paper that the effect of increased anionic lipid results in enhanced binding that can be described quantitatively in terms of a simple phenomenological model. However, the interaction with anionic lipid does not singularly dominate the thermodynamics of binding, nor can the lag phase observed in the time course of hydrolysis of large unilamellar vesicles simply be the result of limited interaction between the enzyme and the bilayer. Furthermore, we show that phospholipase A(2) from Akgistrodon piscivorus piscivorus can exist in at least two bilayer-bound states and that the absence of a fluorescence change upon mixing the enzyme with lipid bilayers does not necessarily indicate the absence of an interaction.     

Kinetics of lipid rearrangements during poly(ethylene glycol)-mediated fusion of highly curved unilamellar vesicles.

In an effort to increase our understanding of the molecular rearrangements that occur during lipid bilayer fusion, we have used different fluorescent probes to characterize the lipid rearrangements associated with poly(ethylene glycol) (PEG)-mediated fusion of DOPC:DL(18:3)PC (85:15) small, unilamellar vesicles (SUVs). Unlike in our previous studies of fusion kinetics [Lee, J., and Lentz, B. R., Biochemistry 36, 6251-6259], these vesicles have mean diameters of 20 nm compared to 45 nm. Surprisingly, we found significant inter-vesicle lipid mixing at 5 wt % PEG, well below the PEG concentration required (17.5 wt %) for vesicles fusion. Lipid movement rate between bilayers (or inter-leaflet movement) increased abruptly at 10 wt % PEG, and the rate of lipid mixing increased thereafter with increasing amounts of PEG. The characteristic time of lipid mixing between outer leaflets (tau approximately equal to 24 s) was comparable to that observed at and above PEG concentrations needed to induce fusion (17.5 wt %) of either 20 or 45 nm vesicles. We also found that slower lipid mixing (tau approximately equal to 267 s) between fusing vesicles occurred on the same time scale or slightly faster than vesicle contents mixing (tau approximately equal to 351 s). In addition, our measurements showed that lipids redistributed across the bilayer on a time scale just slightly faster than pore formation (tau approximately equal to 217 s). This is the first demonstration of trans-bilayer movement of lipids during fusion. We also found that water was excluded from the bilayer (tau approximately equal to 475 s) during product maturation. These observations suggest that fusion in smaller vesicles (approximately 20 nm) proceeds via a multistep mechanism similar to that we reported for somewhat larger vesicles, except that two intermediates are no longer clearly resolved.     

Phase properties of liquid-crystalline Phosphatidylcholine/Phosphatidylethanolamine bilayers revealed by fluorescent probes.

The mixing properties of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoethanolamine (POPE) and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) were examined in liquid-crystalline phase using fluorescent probes incorporated into lipid bilayers. The excimer to monomer (E/M) fluorescence ratio of 1-hexadecanoyl-2-(1-pyrenedecanoyl)-sn-glycero-3-phosphocholine (PPC) versus PPC concentration was higher for binary mixtures containing phosphatidylcholine (PC)/phosphatidylethanolamine (PE) (1:1) compared to PC matrix. When POPC was gradually replaced with POPE, the E/M ratio also increased suggesting the enhanced lateral mobility or the lateral enrichment of PPC into domains or both. Evidences for the PE-induced domain formation were further provided by resonance energy transfer between 2-(4, 4-difluoro-5-methyl-4-boro-3a, 4a-diaza-s-indacene-3-dodecanoyl)-1-hexadecanoyl-sn-glycero- 3-phospho choline and PPC, which was enhanced as a function of PE concentration, and by the polarization of 1,6-diphenyl-1,3, 5-hexatriene. In addition, PE reduced free volume and polarity of lipid bilayers as measured by the emission fluorescence of 1,2-bis PPC and 6-lauroyl-2-dimethylaminonaphthalene. When POPE analogs with a methylated head group instead of normal POPE were used, the diminished effect on the domain formation was shown in the order N-methyl PE > N,N-dimethyl PE. The results suggest that the mixing properties of POPE and POPC are not random but that lipid domains of phospholipids are formed.     

Osmotic and curvature stress affect PEG-induced fusion of lipid vesicles but not mixing of their lipids

Poly (ethylene glycol) (PEG) in the external environment of membrane vesicles creates osmotic imbalance that leads to mechanical stress in membranes and may induce local membrane curvature. To determine the relative importance of membrane stress and curvature in promoting fusion, we monitored contents mixing (CM) and lipid mixing (LM) between different sized vesicles under a variety of osmotic conditions. CM between highly curved vesicles (SUV, 26 nm diameter) was up to 10 times greater than between less curved vesicles (LUV, 120 nm diameter) after 5 min incubation at a low PEG concentration (<10 wt%), whereas LM was only approximately 30% higher. Cryo-electron microscopy showed that PEG at 10 wt% did not create high curvature contacts between membranes in LUV aggregates. A negative osmotic gradient (-300 mOs/kg, hypotonic inside) increased CM two- to threefold for both types of vesicles, but did not affect LM. A positive gradient (+220 mOs/kg, hypertonic inside) nearly eliminated CM and had no effect on LM. Hexadecane added to vesicles had no effect on LM but enhanced CM and reduced the inhibitory effect on CM of a positive osmotic gradient, but had little influence on results obtained under a negative osmotic gradient. We conclude that the ability of closely juxtaposed bilayers to form an initial intermediate ("stalk") as soon as they come into close contact was not influenced by osmotic stress or membrane curvature, although pore formation was critically dependent on these stresses. The results also suggest that hexadecane affects the same part of the fusion process as osmotic stress. We interpret this result to suggest that both a negative osmotic gradient and hexadecane reduce the unfavorable free energy of hydrophobic interstices associated with the intermediates of the fusion process.     

Membrane insertion and lateral diffusion of fluorescence-labelled cytochrome c oxidase subunit IV signal peptide in charged and uncharged phospholipid bilayers.

The synthetic 25-residue signal peptide of cytochrome c oxidase subunit IV was labelled with the fluorophor 7-nitrobenz-2-oxa-1,3-diazole (NBD) at its single cysteine residue. Addition of small unilamellar vesicles of 1-palmitoyl 2-oleoyl phosphatidylcholine (POPC) to the labelled peptide resulted in a shift of the NBD excitation and emission spectra to shorter wavelengths. Binding of the peptide to the vesicles was measured by the increase in the fluorescence emission yield. A surface partition constant of (3.9 +/- 0.5) x 10(3) M-1 was derived from these titrations. When the membrane contained, in addition to POPC, negatively charged 1-palmitoyl 2-oleoyl phosphatidylglycerol (POPG), the NBD fluorescence spectra were further shifted to shorter wavelengths and exhibited increased quantum yields. The apparent partition constants were increased to 10(4)-10(5) M-1 for vesicles with 20 or 100 mol% POPG. Lateral diffusion of the peptide was measured by fluorescence recovery after photobleaching in multibilayers of POPC, POPG, POPC/POPG (4:1) and 1,2-dimyristoyl phosphatidylcholine. The lateral diffusion coefficients of the peptide in bilayers of POPC (8 x 10(-8) cm2/s at 21 degrees C) were 1.5-1.6-fold greater than those of NBD-labelled phospholipids (5 x 10(-8) cm2/s at 21 degrees C), but 1.5-1.8-fold smaller (3 x 10(-8) cm2/s in 20% POPG and at 21 degrees C) than the lipid diffusion coefficients in the negatively charged bilayers. It is concluded that the signal peptide associates with phospholipid bilayers in two different forms, which depend on the lipid charge. The experiments with POPC bilayers are well explained by a model in which the peptide partitions into the region of the phospholipid head-groups and diffuses along the membrane/water interface. If POPG is present in the membrane, electrostatic attractions between the basic residues of the peptide and the acidic lipid head-groups result in a deeper penetration of the bilayer. For this case, two models that are both consistent with the experimental data are discussed, in which the peptide either forms an oligomer of three to six partially helical membrane-spanning monomers, or inserts into the bilayer with its amphiphilic helical segment aligned parallel to the plane of the membrane and located near the head-group and outer hydrocarbon region of the bilayer.     

Fusion of phospholipid vesicles produced by the anti-tumour protein alpha-sarcin.

The anti-tumour protein alpha-sarcin causes fusion of bilayers of phospholipid vesicles at neutral pH. This is demonstrated by measuring the decrease in the efficiency of the fluorescence energy transfer between N-(7-nitro-2-1,3-benzoxadiazol-4-yl)-dimyristoylphosphatidylethano lamine (NDB-PE) (donor) and N-(lissamine rhodamine B sulphonyl)-diacylphosphatidylethanolamine (Rh-PE) (acceptor) incorporated in dimyristoylphosphatidylcholine (DMPG) vesicles. The effect of alpha-sarcin is a maximum at 0.15 M ionic strength and is abolished at basic pH. alpha-Sarcin promotes fusion between 1,6-diphenylhexa-1,3,5-triene (DPH)-labelled DMPG and dipalmitoyl-PG (DPPG) vesicles, resulting in a single thermotropic transition for the population of fused phospholipid vesicles. Bilayers composed of DMPC and DMPG, at different molar ratios in the range 1:1 to 1:10 PC/PG, are also fused by alpha-sarcin. Freeze-fracture electron micrographs corroborate the occurrence of fusion induced by the protein. alpha-Sarcin also modifies the permeability of the bilayers, causing the leakage of calcein in dye-trapped PG vesicles. All of the observed effects reach saturation at a 50:1 phospholipid/protein molar ratio, which is coincident with the binding stoichiometry previously described.     

Functional reconstitution of the nicotinic acetylcholine receptor by CHAPS dialysis depends on the concentrations of salt, lipid, and protein.

The detergent CHAPS was found to be the preferable surfactant for the efficient purification and reconstitution of the Torpedo californica nicotinic acetylcholine receptor (AChR). The main result is that the incorporation of the AChR proteins into lipid vesicles by CHAPS dialysis was strongly dependent on the salt and protein concentrations. As monitored by sucrose gradients, by electron microscopy, and by agonist-induced lithium ion flux, the best reconstitution yields were obtained in 0.5 M NaCl at a protein concentration of 0.5 g/L and in 0.84 M NaCl at 0.15 g/L protein. Electron micrographs of receptor molecules, which were incorporated into vesicles, showed single, nonaggregated dimer (M(r) = 580,000) and monomer (M(r) = 290,000) species. CHAPS dialysis at NaCl concentrations less than 0.5 M largely reduced the receptor incorporation concomitant with protein aggregation. Electron micrographs of these preparations revealed large protein sheets or ribbons not incorporated into vesicles. The analysis of static and dynamic light scattering demonstrated that the detergent-solubilized AChR molecules aggregate at low lipid contents (less than or equal to 500 phospholipids/AChR dimer), independent of the salt concentration. AChR proteins eluted from an affinity column with a solution containing 8 mM CHAPS (but no added lipid) still contained 130 +/- 34 tightly bound phospholipids per dimer. The aggregates (about 10 dimers on the average) could be dissociated by readdition of lipid and, interestingly, also by increasing the CHAPS concentration up to 15 mM. This value is much higher than the CMC of CHAPS = 4.0 +/- 0.4 mM, which was determined by surface tension measurements. The data clearly suggest protein-micelle interactions in addition to the association of monomeric detergents with proteins. Furthermore, the concentration of the (free) monomeric CHAPS at the vesicle-micelle transformation in 0.5 M NaCl ([Dw]c = 3.65 mM) was higher than in 50 mM NaCl ([Dw]c = 2.8 mM). However, it is suggested that the main effect of high salt concentrations during the reconstitution process is an increase of the fusion (rate) of the ternary protein/lipid/CHAPS complexes with mixed micelles or with vesicular structures, similar to the salt-dependent fusion of vesicles.