Melittin-Lipid interaction: A comparative study using liposomes, micelles and bilayerdisks

Comparison of melittin interaction with liposomes, bilayer disks and micelles showed that melittin binding to lipid aggregates is largely dictated by the amount of highly curved areas in the aggregates. The PEG-stabilised bilayer disks were characterised by a combination of small angle neutron scattering, cryo-transmission electron microscopy and dynamic light scattering. Importantly, the theoretically foreseen partial segregation of the lipid components, important for maintaining the structure of the bilayer disk, was confirmed. Steady state fluorescence spectroscopy indicated that melittin mainly resides at the rim of the bilayer disks. Results of the present study help increase the understanding of the mechanisms behind, and the physico-chemical factors affecting, melittin-lipid interaction. We suggest that bilayer disks, due to their stable structure, constitute interesting vehicles for transport of peptides that have high propensity to associate with lipid surfaces of high curvature.     

Real-time structural investigation of a lipid bilayer during its interaction with melittin using sum frequency generation vibrational spectroscopy

Interactions between membrane bilayers and peptides/proteins are ubiquitous throughout a cell. To determine the structure of membrane bilayers and the associated peptides/proteins, model systems such as supported lipid bilayers are often used. It has been difficult to directly investigate the interactions between a single membrane bilayer and peptides/proteins without exogenous labeling. In this work we demonstrate that sum frequency generation vibrational spectroscopy can be employed to study the interactions between peptides/proteins and a single lipid bilayer in real time, in situ, and without exogenous labeling. Using melittin and a dipalmitoyl phosphatidylglycerol bilayer as a model system, we monitored the C-H and C-D stretching signals from isotopically symmetric or asymmetric dipalmitoyl phosphatidylglycerol bilayers during their interaction with melittin. It has been found that the extent and kinetics of bilayer perturbation induced by melittin are very sensitive to melittin concentration. Such concentration dependence is correlated to melittin's mode of action. Melittin is found to function via the early and late stage of the carpet model at low and high concentrations, respectively, whereas the toroidal model is probable at intermediate concentrations. This research illustrates the potential of sum frequency generation as a biophysical technique to monitor individual leaflet structure of lipid bilayers in real time during their interactions with biomolecules.     

Melittin-induced changes of the macroscopic structure of phosphatidylethanolamines

The binding of melittin to phosphatidylethanolamine model systems and its influence on the supramolecular organization of the lipid were investigated with binding assays, differential scanning calorimetry, 31P NMR, freeze-fracture electron microscopy, and small-angle X-ray scattering. The results are compared with binding to an analogous phosphatidylcholine and structural consequences thereof. Melittin binds with similar affinity to both lipid types in the liquid-crystalline state; at gel-phase temperatures, in contrast, interaction with phosphatidylethanolamine is much weaker and does not lead to the bilayer fragmentation observed for phosphatidylcholines. With regard to phosphatidylethanolamine polymorphism, it is shown that melittin acts as an inhibitor of HII-phase formation and as a stabilizer of the bilayer organization. It is demonstrated that the remarkable variety of effects of melittin on the polymorphism of different membrane phospholipids can be understood in a relatively simple concept, taking into account the relative position and the shape of the interacting components.     

Morphological changes of phosphatidylcholine bilayers induced by melittin: vesicularization, fusion, discoidal particles

Morphological changes induced by the melittin tetramer on bilayers of egg phosphatidylcholine and dipalmitoylphosphatidylcholine have been studied by quasi-elastic light scattering, gel filtration and freeze-fracture electron microscopy. It is concluded that melittin similarly binds and changes the morphology of both single and multilamellar vesicles, provided that their hydrocarbon chains have a disordered conformation, i.e., at temperatures higher than that of the transition, Tm. When the hydrocarbon chains are ordered (gel phase), only small unilamellar vesicles are morphologically affected by melittin. However after incubation at T greater than Tm, major structural changes are detected in the gel phase, regardless of the initial morphology of the lipids. Results from all techniques agree on the following points. At low melittin content, phospholipid-to-peptide molar ratios, Ri greater than 30, heterogeneous systems are observed, the new structures coexisting with the original ones. For lipids in the fluid phase and Ri greater than 12, the complexes formed are large unilamellar vesicles of about 1300 +/- 300 A diameter and showing on freeze-fracture images rough fracture surfaces. For lipids in the gel phase, T less than Tm after passage above Tm, and for 5 less than Ri less than 50, disc-like complexes are observed and isolated. They have a diameter of 235 +/- 23 A and are about one bilayer thick; their composition corresponds to one melittin for about 20 +/- 2 lipid molecules. It is proposed that the discs are constituted by about 1500 lipid molecules arranged in a bilayer and surrounded by a belt of melittin in which the mellitin rods are perpendicular to the bilayer. For high amounts of melittin, Ri less than 2, much smaller and more spherical objects are observed. They are interpreted as corresponding to lipid-peptide co-micelles in which probably no more bilayer structure is left. It is concluded that melittin induces a reorganization of lipid assemblies which can involve different processes, depending on experimental conditions: vesicularization of multibilayers; fusion of small lipid vesicles; fragmentation into discs and micelles. Such processes are discussed in connexion with the mechanism of action of melittin: the lysis of biological membranes and the synergism between melittin and phospholipases.     

Binding and reorientation of melittin in a POPC bilayer: Computer simulations

We performed, using an all-atom force field, molecular dynamics computer simulations to study the binding of melittin to the POPC bilayer and its subsequent reorientation in this bilayer. The binding process involves a simultaneous folding and adsorption of the peptide to the bilayer, followed by the creation of a "U shaped" conformation. The reorientation of melittin from the parallel to the perpendicular conformation requires charged residues to cross the hydrophobic core of the bilayer. This is accomplished by a creation of defects in the bilayer that are filled out with water. The defects are caused by peptide charged residues dragging the lipid headgroup atoms along with them, as they reorient. With increased concentration of melittin water defects form stable pores; this makes it easier for the peptide N-terminus to reorient. Our results complement experimental and computational observations of the melittin/lipid bilayer interaction.     

Barrel-stave model or toroidal model? A case study on melittin pores

Transmembrane pores induced by amphiphilic peptides, including melittin, are often modeled with the barrel-stave model after the alamethicin pore. We examine this assumption on melittin by using two methods, oriented circular dichroism (OCD) for detecting the orientation of melittin helix and neutron scattering for detecting transmembrane pores. OCD spectra of melittin were systematically measured. Melittin can orient either perpendicularly or parallel to a lipid bilayer, depending on the physical condition and the composition of the bilayer. Transmembrane pores were detected when the helices oriented perpendicularly to the plane of the bilayers, not when the helices oriented parallel to the bilayers. The evidence that led to the barrel-stave model for alamethicin and that to the toroidal model for magainin were reviewed. The properties of melittin pores are closely similar to that of magainin but unlike that of alamethicin. We conclude that, among naturally produced peptides that we have investigated, only alamethicin conforms to the barrel-stave model. Other peptides, including magainins, melittin and protegrins, all appear to induce transmembrane pores that conform to the toroidal model in which the lipid monolayer bends continuously through the pore so that the water core is lined by both the peptides and the lipid headgroups.     

Incorporation of highly purified melittin into phosphatidylcholine bilayer vesicles

Melittin free of phospholipase A2 was prepared. In the absence of salt this highly pure protein starts to aggregate in solution at a protein concentration of Cp greater than 10(-3) M. In high salt solution (2 M) aggregation starts at Cp greater than 10(-6) M. This was determined from the blue shift of the intrinsic fluorescence of the protein. Reinvestigation of the quenching behaviour clearly shows that self-aggregation cannot be deduced from quenching experiments using nitrate or 2,2,6,6-tetramethylpiperidine-1-oxyl as quencher. The incorporation of melittin into phosphatidylcholine bilayer vesicles was studied by fluorescence quenching and by energy-transfer experiments using 2- and 6-anthroyloxypalmitic acid as acceptor and peptide tryptophan as donor. Incorporation of melittin into small unilamellar vesicles was found to be reduced below the lipid phase transition temperature, Tt, whereas it incorporates and distributes more randomly above Tt. Cooling the temperature below Tt after incubation at T greater than Tt leads to a deeper incorporation of the peptide into the lipid bilayer due to electrostatic interaction between the lipid phosphate groups and the positively charged amino acids. This stabilizing effect is lost above Tt and melittin is extruded to the polar phase. Quenching experiments support this finding. EPR measurements clearly demonstrate that even in the presence of high amounts of melittin up to 10 mol% with respect to the lipid broadening of the phase transition curves was only observed with fatty acid spin labels, where the doxyl group is localized near the bilayer surface. The order degree of the inner part of the bilayer remains almost unchanged even in the presence of high melittin content.     

Melittin-induced alterations in dynamic properties of human red blood cell membranes.

The interaction of bee venom melittin with erythrocyte membrane ghosts has been investigated by means of fluorescence quenching of membrane tryptophan residues, fluorescence polarization and ESR spectroscopy. It has been revealed that melittin induces the disorders in lipid-protein matrix both in the hydrophobic core of bilayer and at the polar/non-polar interface of melittin complexed with erythrocyte membranes. The peptide has been found to act most efficiently at the concentration of the order of 10(-10) mol/mg membrane protein. The apparent distance separating the membrane tryptophan and bound 1-anilino-8-naphthalenesulphonate (ANS) molecules is decreased upon melittin binding, which results in a significant increase of the maximum energy transfer efficiency. Significant changes in the fluorescence anisotropy of both 1,6-diphenyl-1,3,5-hexatriene and 1-anilino-8-naphthalenesulphonate bound to erythrocyte ghosts, which have been observed in the presence of melittin and crude venom, indicate membrane lipid bilayer rigidization. The effect of crude honey bee venom has been found to be of similar magnitude as the effect of pure melittin at the concentration of 10(-10) mol/mg membrane protein. Using two lipophilic spin labels, methyl 5-doxylpalmitate and 16-doxylstearic acid, we found that melittin at its increasing concentrations induces a well marked rigidization in the deeper regions of lipid bilayer, whereas the effect of rigidization near the membrane surface maximizes at the melittin concentration of 10(-10) mol/mg (10(-4) mol melittin per mole of membrane phospholipid). The decrease in the ratio hw/hs of maleimide and the rise in relative rotational correlation time (tau c) of iodacetamid spin label, indicate that melittin effectively immobilizes membrane proteins in the plane of the lipid bilayer. We conclude that melittin-induced rigidization of the lipid bilayer may induce a reorganization of lipid assemblies as well as the rearrangements in membrane protein pattern and consequently the alterations in lipid-protein interactions. Thus, the interaction of melittin with erythrocyte membranes is supposed to produce local conformational changes in membranes, which are discussed in the connection with their significance during the synergistic action of melittin and phospholipase of bee venom on red blood cells.     

Anthrylvinyl-labeled phospholipids as fluorescent membrane probes. The action of melittin on mulitlipid systems

The interaction of melittin with multicomponent lipid mixtures composed of phosphatidylcholine, sphingomyelin and phosphatidylserine or phosphatidylglycerol was investigated by measuring the intrinsic fluorescence of the peptide, steady state fluorescence anisotropy of, and Trp-fluorescence energy transfer to fluorescent analogs of the same phospholipids bearing the anthrylvinyl fluorophore in one of the aliphatic chains at various distances from the polar head group. Based on the finding that at high lipid/peptide ratio the peptide induces unequal changes in the fluorescence parameters of phospholipid probes differing structurally only in their polar head groups, it is concluded that melittin induces lipid demixing in its nearest environment. Comparison of the fluorescence energy transfer from Trp to different lipid probes indicates that the depth of penetration of melittin into the bilayer depends on the polar head group composition of the phospholipid matrix and that certain segments of the melittin chain display a specific affinity for a given lipid head group.     

A molecular dynamics study of the bee venom melittin in aqueous solution, in methanol, and inserted in a phospholipid bilayer

The structural properties of melittin, a small amphipathic peptide found in the bee venom, are investigated in three different environments by molecular dynamics simulation. Long simulations have been performed for monomeric melittin solvated in water, in methanol, and shorter ones for melittin inserted in a dimyristoylphosphatidylcholine bilayer. The resulting trajectories were analysed in terms of structural properties of the peptide and compared to the available NMR data. While in water and methanol solution melittin is observed to partly unfold, the peptide retains its structure when embedded in a lipid bilayer. The latter simulation shows good agreement with the experimentally derived ³J-coupling constants. Generally, it appears that higher the stability of the helical conformation of melittin, lower is the dielectric permittivity of the environment. In addition, peptide-lipid interactions were investigated showing that the C-terminus of the peptide provides an anchor to the lipid bilayer by forming hydrogen bonds with the lipid head groups.     

A high-sensitivity differential scanning calorimetric study of the interaction of melittin with dipalmitoylphosphatidylcholine fused unilamellar vesicles

High-sensitivity differential scanning calorimetry has been used to examine the interaction of bee venom melittin with dipalmitoylphosphatidylcholine fused unilamellar vesicles. Experiments were performed under conditions for which melittin in solution is either monomeric (in low salt) or tetrameric (in high salt). It was found that under both sets of conditions melittin abolishes the pretransition at a relatively high lipid-to-protein molar incubation ratio, Ri (about 200) and that at intermediate values of Ri it broadens the main transition profile and reduces the transition enthalpy. This provides evidence which suggests that melittin is at least partially inserted into the apolar region of the bilayer. Evident at low values of Ri are two peaks in the lipid thermal transition profiles, which may arise from a heterogeneous population of lipid vesicles formed through fusion induced by melittin, or by lipid phase separation. For those profiles which exhibited only one peak, transition enthalpies, normalized to those of the lipid in the absence of the protein, are plotted vs. the bound protein-to-lipid molar ratios for the experiments performed under the conditions which give monomeric and tetrameric melittin in solution. These plots yield straight lines, the slopes of which give the number of lipid molecules each protein molecule excludes from participating in the phase transition. These were found to be 9.9 +/- 0.7 and 4.1 +/- 0.5 for monomeric and tetrameric melittin, respectively. The results are discussed in terms of possible models for the binding of melittin to phospholipid vesicles. For simple hexagonal packing of lipid molecules, incorporation as an aggregate is favored when melittin is tetrameric in solution, whereas incorporation as a monomer is favored when melittin is monomeric in solution. For low-salt solutions, evidence is obtained for the contribution of free melittin to lipid fusion, perhaps by the formation of protein bridges between apposed vesicles.     

Architecture of bacterial lipid A in solution. A neutron small-angle scattering study

The phase structure of isolated bacterial lipid A, the lipid anchor of the lipopolysaccharides of the outer membrane of Gram-negative bacteria, has been investigated by neutron small-angle scattering. The shape of the scattering curves obtained at different H2O/2H2O ratios revealed a lamellar organisation of the lipid A at neutral pH both above and below its main phase temperature (approximately 40-45 degrees C). Analysis of the scattering curves and interpretation of the corresponding thickness distance distribution functions of the lamellar aggregates led to a model in which the lipid A molecules form a bilayer of about 5 nm in thickness. This value for the thickness of the bilayer, as well as the neutron-scattering density profile across the bilayer, can be explained by a molecular model which shows interdigitation of the fatty acid chains of the lipid A.     

Exploring the effect of cholesterol in lipid bilayer membrane on the melittin penetration mechanism

A vascular mimetic membrane system was used to investigate the effect of cholesterol content in lipid bilayer on the dynamics of the melittin-membrane penetration reaction with real-time monitoring by a piezoelectric sensor and the assessment morphology using atomic force microscopy (AFM). In the presence of 30% cholesterol in a noncharged phosphatidylcholine (PC) phospholipid membrane, KA1 (binding affinity constant) and KA2 (insertion affinity constant) derived from a two-step model decreased significantly. This result suggests that the high dose of cholesterol in phospholipid membrane inhibits both the binding and the insertion of melittin. Next, dynamic laser scattering and AFM were used to verify the structural changes of lipid bilayers in solutions and interfaces, respectively. The superstructures in both 0 and 10% cholesterol lipid bilayers were disrupted with penetration of melittin according to these verifications. However, kinetic analysis reveals that the different mechanisms are dependent on cholesterol, particularly for the insertion step.     

Conformation and dynamics of melittin bound to magnetically oriented lipid bilayers by solid-state (31)P and (13)C NMR spectroscopy

The conformation and dynamics of melittin bound to the dimyristoylphosphatidylcholine (DMPC) bilayer and the magnetic orientation in the lipid bilayer systems were investigated by solid-state (31)P and (13)C NMR spectroscopy. Using (31)P NMR, it was found that melittin-lipid bilayers form magnetically oriented elongated vesicles with the long axis parallel to the magnetic field above the liquid crystalline-gel phase transition temperature (T(m) = 24 degrees C). The conformation, orientation, and dynamics of melittin bound to the membrane were further determined by using this magnetically oriented lipid bilayer system. For this purpose, the (13)C NMR spectra of site-specifically (13)C-labeled melittin bound to the membrane in the static, fast magic angle spinning (MAS) and slow MAS conditions were measured. Subsequently, we analyzed the (13)C chemical shift tensors of carbonyl carbons in the peptide backbone under the conditions where they form an alpha-helix and reorient rapidly about the average helical axis. Finally, it was found that melittin adopts a transmembrane alpha-helix whose average axis is parallel to the bilayer normal. The kink angle between the N- and C-terminal helical rods of melittin in the lipid bilayer is approximately 140 degrees or approximately 160 degrees, which is larger than the value of 120 degrees determined by x-ray diffraction studies. Pore formation was clearly observed below the T(m) in the initial stage of lysis by microscope. This is considered to be caused by the association of melittin molecules in the lipid bilayer.     

Modulation of melittin-induced lysis by surface charge density of membranes.

Phosphorus NMR spectroscopy was used to characterize the importance of electrostatic interactions in the lytic activity of melittin, a cationic peptide. The micellization induced by melittin has been characterized for several lipid mixtures composed of saturated phosphatidylcholine (PC) and a limited amount of charged lipid. For these systems, the thermal polymorphism is similar to the one observed for pure PC: small comicelles are stable in the gel phase and extended bilayers are formed in the liquid crystalline phase. Vesicle surface charge density influences strongly the micellization. Our results show that the presence of negatively charged lipids (phospholipid or unprotonated fatty acid) reduces the proportion of lysed vesicles. Conversely, the presence of positively charged lipids leads to a promotion of the lytic activity of the peptide. The modulation of the lytic effect is proposed to originate from the electrostatic interactions between the peptide and the bilayer surface. Attractive interactions anchor the peptide at the surface and, as a consequence, inhibit its lytic activity. Conversely, repulsive interactions favor the redistribution of melittin into the bilayer, causing enhanced lysis. A quantitative analysis of the interaction between melittin and negatively charged bilayers suggests that electroneutrality is reached at the surface, before micellization. The surface charge density of the lipid layer appears to be a determining factor for the lipid/peptide stoichiometry of the comicelles; a decrease in the lipid/peptide stoichiometry in the presence of negatively charged lipids appears to be a general consequence of the higher affinity of melittin for these membranes.     

The interaction of bee melittin with lipid bilayer membranes

The influence of melittin and the related 8-26 peptide on the stability and electrical properties of bilayer lipid membranes is reported. Melittin, unlike the 8-26 peptide, has a dramatic influence on lipid membranes, causing rupture at dilute concentrations. The circular dichroism of melittin demonstrated that under physiological conditions, in water, melittin is in extended conformation, which is enhanced in aqueous ethanol. However in 'membrane-like' conditions it is essentially alpha-helical. Secondary structure predictions were used to locate possible alpha-helical nucleation centres and a model of melittin was built according to these predictions. It is postulated that melittin causes a wedge effect in membranes.     

Solid-phase synthesis of melittin: purification and functional characterization

The main component of the honey bee venom, melittin, is a cationic polypeptide containing 26 amino acids. Exposure of lipid bilayers to this peptide results in the formation of anion-selective channels with a variety of unit conductances. One of the possible causes for this heterogeneity in the conductance could be heterogeneity of the melittin preparation, and indeed, the existence of two prominent forms of naturally occurring melittin, differing only at the N-terminal amino group, has been documented. This paper describes the synthesis of the major form of melittin, using stepwise solid-phase methodology and the demonstration that the synthetic melittin, devoid of the minor component (N-formylmelittin) and other contaminants, interacts with lipid bilayers to form channels which are qualitatively indistinguishable from the ones formed by the naturally occurring toxin. This result indicates that the heterogeneity in the channels produced in bilayers by bee venom is not due to differences in the channel-forming properties of the formyl and non-formyl melittin but rather to differences in the number and orientation of melittin monomers of identical primary structure as they aggregate to form channels in the lipid bilayer.     

Interaction of melittin with model membranes: effect on the size and permeability of liposomes

The influence of melittin, a monomer devoid of the phospholipase activity, on the size and permeability of liposomes from egg lecithin (PC), dimyristoylphosphatidylcholine (DMPC) and dipalmitoylphosphatidylcholine (DPPC) has been investigated by the methods of fluorescence spectroscopy, quasi-elastic light scattering and freeze-fracture electron microscopy. While studying calcein release from liposomes under the influence of melittin it has been shown that binding of melittin with a bilayer is a fast process which depends on the concentration lipid: protein (Ri) ratio as well as on the phase state of the lipid. The lipids being in the liquid-crystalline forms (PC and DMPC) are characterized by a more rapid release of the dye-stuff from liposomes than DPPC vesicles being in gel state with the same Ri. Under the influence of different melittin concentrations heterogeneity of the system and its medium hydrodynamic size of particles at first increases (100 less than or equal to Ri less than 500) due to their fusion and then these parameters decrease to the initial values.     

Structure of the dimyristoylphosphatidylcholine vesicle and the complex formed by its interaction with apolipoprotein C-III: X-ray small-angle scattering studies.

Single bilayer vesicles of dimyristoylphosphatidylcholine have been investigated by small-angle X-ray scattering at 28 degrees C. The results indicate that these vesicles are hollow spherical shell structures with an outer radius of approximately 12 nm and a molecular weight of (3.2 +/- 0.5) X 10(6). The shell was found to be 4.4 +/- 0.2 nm thick with a cross-sectional electron-density profile characteristic for a single phospholipid bilayer. Upon interaction of these vesicles with apolipoprotein C-III from human very low density lipoproteins at a protein/lipid ratio greater than 0.08 (g/g), a complex containing 0.25 g of protein/g of lipid, with molecular weight of (3.9 +/- 0.4) X 10(5), is formed. The shape analysis indicates a highly asymmetric particle with an internal partition of low and high electron density resembling that produced by a bilayer structure. Model calculations and curve-fitting procedures show good agreement between the experimental scattering curve and that computed for an oblate ellipsoidal structure with dimensions of 17 X 17 X 5 nm and a 1 nm thick shell of high electron density surrounding the core of low electron density.     

Liposomes, disks, and spherical micelles: aggregate structure in mixtures of gel phase phosphatidylcholines and poly(ethylene glycol)-phospholipids

Poly(ethylene glycol) (PEG) decorated lipid bilayers are widely used in biomembrane and pharmaceutical research. The success of PEG-lipid stabilized liposomes in drug delivery is one of the key factors for the interest in these polymer/lipid systems. From a more fundamental point of view, it is essential to understand the effect of the surface grafted polymers on the physical-chemical properties of the lipid bilayer. Herein we have used cryo-transmission electron microscopy and dynamic light scattering to characterize the aggregate structure and phase behavior of mixtures of PEG-lipids and distearoylphosphatidylcholine or dipalmitoylphosphatidylcholine. The PEG-lipids contain PEG of molecular weight 2000 or 5000. We show that the transition from a dispersed lamellar phase (liposomes) to a micellar phase consisting of small spherical micelles occurs via the formation of small discoidal micelles. The onset of disk formation already takes place at low PEG-lipid concentrations (<5 mol %) and the size of the disks decreases as more PEG-lipid is added to the lipid mixture. We show that the results from cryo-transmission electron microscopy correlate well with those obtained from dynamic light scattering and that the disks are well described by an ideal disk model. Increasing the temperature, from 25 degrees C to above the gel-to-liquid crystalline phase transition temperature for the respective lipid mixtures, has a relatively small effect on the aggregate structure.