Tubular Membrane Formation of Binary Giant Unilamellar Vesicles Composed of Cylinder and Inverse-Cone-Shaped Lipids

We have succeeded in controlling tubular membrane formations in binary giant unilamellar vesicles (GUVs) using a simple temperature changing between the homogeneous one-phase region and the two-phase coexistence region. The binary GUV is composed of inverse-cone (bulky hydrocarbon chains and a small headgroup) and cylinder-shaped lipids. When the temperature was set in the two-phase coexistence region, the binary GUV had a spherical shape with solidlike domains. By increasing the temperature to the homogeneous one-phase region, the excess area created by the chain melting of the lipid produced tubes inside the GUV. The tubes had a radius on the micrometer scale and were stable in the one-phase region. When we again decreased the temperature to the two-phase coexisting region, the tubes regressed and the GUVs recovered their phase-separated spherical shape. We infer that the tubular formation was based on the mechanical balance of the vesicle membrane (spontaneous tension) coupled with the asymmetric distribution of the inverse-cone-shaped lipids between the inner and outer leaflets of the vesicle (lipid sorting).     

Tubular Membrane Formation of Binary Giant Unilamellar Vesicles Composed of Cylinder and Inverse-Cone-Shaped Lipids

We have succeeded in controlling tubular membrane formations in binary giant unilamellar vesicles (GUVs) using a simple temperature changing between the homogeneous one-phase region and the two-phase coexistence region. The binary GUV is composed of inverse-cone (bulky hydrocarbon chains and a small headgroup) and cylinder-shaped lipids. When the temperature was set in the two-phase coexistence region, the binary GUV had a spherical shape with solidlike domains. By increasing the temperature to the homogeneous one-phase region, the excess area created by the chain melting of the lipid produced tubes inside the GUV. The tubes had a radius on the micrometer scale and were stable in the one-phase region. When we again decreased the temperature to the two-phase coexisting region, the tubes regressed and the GUVs recovered their phase-separated spherical shape. We infer that the tubular formation was based on the mechanical balance of the vesicle membrane (spontaneous tension) coupled with the asymmetric distribution of the inverse-cone-shaped lipids between the inner and outer leaflets of the vesicle (lipid sorting).     

Molecular dynamics simulations of lipid vesicle fusion in atomic detail

The fusion of a membrane-bounded vesicle with a target membrane is a key step in intracellular trafficking, exocytosis, and drug delivery. Molecular dynamics simulations have been used to study the fusion of small unilamellar vesicles composed of a dipalmitoyl-phosphatidylcholine (DPPC)/palmitic acid 1:2 mixture in atomic detail. The simulations were performed at 350-370 K and mimicked the temperature- and pH-induced fusion of DPPC/palmitic acid vesicles from experiments by others. To make the calculations computationally feasible, a vesicle simulated at periodic boundary conditions was fused with its periodic image. Starting from a preformed stalk between the outer leaflets of the vesicle and its periodic image, a hemifused state formed within 2 ns. In one out of six simulations, a transient pore formed close to the stalk, resulting in the mixing of DPPC lipids between the outer and the inner leaflet. The hemifused state was (meta)stable on a timescale of up to 11 ns. Forcing a single lipid into the interior of the hemifusion diaphragm induced the formation and expansion of a fusion pore on a nanosecond timescale. This work opens the perspective to study a wide variety of mesoscopic biological processes in atomic detail.     

Accelerated interleaflet transport of phosphatidylcholine molecules in membranes under deformation.

Biological membranes are lamellar structures composed of two leaflets capable of supporting different mechanical stresses. Stress differences between leaflets were generated during micromechanical experiments in which long thin tubes of lipid (tethers) were formed from the surfaces of giant phospholipid vesicles. A recent dynamic analysis of this experiment predicts the relaxation of local differences in leaflet stress by lateral slip between the leaflets. Differential stress may also relax by interleaflet transport of lipid molecules ("flip-flop"). In this report, we extend the former analysis to include interleaflet lipid transport. We show that transmembrane lipid flux will evidence itself as a linear increase in tether length with time after a step reduction in membrane tension. Multiple measurements were performed on 24 different vesicles composed of stearoyl-oleoyl-phosphatidylcholine plus 3% dinitrophenol-linked di-oleoyl-phosphatidylethanolamine. These tethers all exhibited a linear phase of growth with a mean value of the rate of interlayer permeation, cp = 0.009 s-1. This corresponds to a half-time of approximately 8 min for mechanically driven interleaflet transport. This value is found to be consistent with longer times obtained for chemically driven transport if the lipids cross the membrane via transient, localized defects in the bilayer.     

Asymmetry of lipid organization in cholinergic synaptic vesicle membranes.

The lipid composition of purified Torpedo cholinergic synaptic vesicles was determined and their distribution between the inner and outer leaflets of the vesicular membrane was investigated. The vesicles contain cholesterol and phospholipids at a molar ratio of 0.63. The vesicular phospholipids are (mol% of total phospholipids): phosphatidylcholine (40.9); phosphatidylethanolamine (24.6); plasmenylethanolamine (11.5); sphingomyelin (12); phosphatidylserine (7.3); phosphatidylinositol (3.7). The asymmetry of the synaptic vesicle membranes was investigated by two independent approaches: (a) determining accessibility of the amino lipids to the chemical label trinitrobenzenesulphonic acid (TNBS); (b) determining accessibility of the vesicular glycerophospholipids to phospholipase C (Bacillus cereus). TNBS was found to render the vesicles leaky and thus cannot be used reliably to determine the asymmetry of Torpedo synaptic vesicle membranes. Incubation of the vesicles with phospholipase C (Bacillus cereus) results in biphasic hydrolysis of the vesicular glycerophospholipids. About 45% of the phospholipids are hydrolysed in less than 1 min, during which no vesicular acetylcholine is released. In the second phase, the hydrolysis of the phospholipids slows down markedly and is accompanied by loss of all the vesicular acetylcholine. These findings suggest that the lipids hydrolysed during the first phase are those comprising the outer leaflet. Analysis of the results thus obtained indicate that the vesicular membrane is asymmetric: all the phosphatidylinositol, 77% of the phosphatidylethanolamine, 47% of the plasmenylethanolamine and 58% of the phosphatidylcholine were found to reside in the outer leaflet. Since phosphatidylserine is a poor substrate for phospholipase C (B. cereus), its distribution between the two leaflets of the synaptic vesicle membrane is only suggestive.     

Pore Formation in a Binary Giant Vesicle Induced by Cone-Shaped Lipids

We have investigated shape deformations of binary giant unilamellar vesicles (GUVs) composed of cone- and cylinder-shaped lipids. By coupling the spontaneous curvature of lipids with the phase separation, we demonstrated pore opening and closing in GUVs. When the temperature was set below the chain melting transition temperature of the cylinder-shaped lipid, the GUVs burst and then formed a single large pore, where the cone shape lipids form a cap at the edge of the bilayer to stabilize the pore. The pore closed when we increased the temperature above the transition temperature. The pore showed three types of shapes depending on the cone-shaped lipid concentration: simple circular, rolled-rim, and wrinkled-rim pores. These pore shape changes indicate that the distribution of the cone- and cylinder-shaped lipids is asymmetric between the inner and outer leaflets in the bilayer. We have proposed a theoretical model for a two-component membrane with an edge of bilayer where lipids can transfer between two leaflets. Using this model, we have reproduced numerically the observed shape deformations at the rim of pore.     

Attachment of β2-glycoprotein I to negatively charged liposomes may prevent the release of daughter vesicles from the parent membrane

The temperature-induced budding of POPC-cardiolipin-cholesterol, POPC-POPS-cholesterol and POPC-POPG-cholesterol giant lipid vesicles in the presence of beta(2)-glycoprotein I (beta(2)-GPI) in the outer solution was studied experimentally and theoretically. The observed budding transition of vesicles was continuous which can be explained by taking into account the orientational ordering and direct interactions between oriented lipids. The attachment of positively charged beta(2)-GPI to the negatively charged outer surface of POPC-cardiolipin-cholesterol, POPC-POPS-cholesterol and POPC-POPG-cholesterol giant vesicles caused coalescence of the spheroidal membrane bud with the parent vesicle before the bud could detach from the parent vesicle, i.e. vesiculate. Theoretically, the protein-mediated attraction between the membrane of a bud and the parent membrane was described as an interaction between two electric double layers. It was shown that the specific spatial distribution of charge within beta(2)-GPI molecules attached to the negatively charged membrane surface may explain the observed attraction between like-charged membrane surfaces.     

Transmembrane asymmetry and lateral domains in biological membranes

It is generally assumed that rafts exist in both the external and internal leaflets of the membrane, and that they overlap so that they are coupled functionally and structurally. However, the two monolayers of the plasma membrane of eukaryotic cells have different chemical compositions. This out-of-equilibrium situation is maintained by the activity of lipid translocases, which compensate for the slow spontaneous transverse diffusion of lipids. Thus rafts in the outer leaflet, corresponding to domains enriched in sphingomyelin and cholesterol, cannot be mirrored in the inner cytoplasmic leaflet. The extent to which lipids contribute to raft properties can be conveniently studied in giant unilamellar vesicles. In these, cholesterol can be seen to condense with saturated sphingolipids or phosphatidylcholine to form μm scale domains. However, such rafts fail to model biological rafts because they are symmetric, and because their membranes lack the mechanism that establishes this asymmetry, namely proteins. Biological rafts are in general of nm scale, and almost certainly differ in size and stability in inner and outer monolayers. Any coupling between rafts in the two leaflets, should it occur, is probably transient and dependent not upon the properties of lipids, but on transmembrane proteins within the rafts.     

Improving our picture of the plasma membrane: Rafts induce ordered domains in a simplified model cytoplasmic leaflet

By study of asymmetric membranes, models of the cell plasma membrane (PM) have improved, with more realistic properties of the asymmetric lipid composition of the membrane being explored. We used hemifusion of symmetric giant unilamellar vesicles (GUVs) with a supported lipid bilayer (SLB) to engineer bilayer leaflets of different composition. During hemifusion, only the outer leaflets of GUV and SLB are connected, exchanging lipids by simple diffusion. aGUVs were detached from the SLB for study. In general these aGUVs are formed with one leaflet that phase-separates into Ld (liquid disordered) + Lo (liquid ordered) phases, and another leaflet with lipid composition that would form a single fluid phase in a symmetric bilayer. We observed that ordered phases of either Lo or Lβ (gel phase) induce an ordered domain in the apposed fluid leaflet that lacks high melting lipids. Results suggest both an inter-leaflet and an intra-leaflet redistribution of cholesterol. We used C-Laurdan spectral images to investigate the lipid packing/order of aGUVs, finding that cholesterol partitions into the induced ordered domains. We suggest this behavior to be commonplace, that when Ld + Lo phase separation occurs in a cell PM exoplasmic leaflet, an induced order domain forms in the cytoplasmic leaflet.     

Detection of motional heterogeneities in lipid bilayer membranes by dual probe fluorescence correlation spectroscopy

We report the detection of heterogeneities in the diffusion of lipid molecules for the three-component mixture dipalmitoyl-PC/dilauroyl-PC/cholesterol, a chemically simple lipid model for the mammalian plasma membrane outer leaflet. Two-color fluorescence correlation spectroscopy (FCS) was performed on giant unilamellar vesicles (GUVs) using fluorescent probes that have differential lipid phase partition behavior—DiO-C18:2 favors disordered fluid lipid phases, whereas DiI-C20:0 prefers spatially ordered lipid phases. Simultaneously-obtained fluorescence autocorrelation functions from the same excitation volume for each dye showed that, depending on the lipid composition of this ternary mixture, the two dyes exhibited different lateral mobilities in regions of the phase diagram with previously proposed submicroscopic two-phase coexistence. In one-phase regions, both dyes reported identical diffusion coefficients. Two-color FCS thus may be detecting local membrane heterogeneities at size scales below the optical resolution limit, either due to short-range order in a single phase or due to submicroscopic phase separation.     

Detection of motional heterogeneities in lipid bilayer membranes by dual probe fluorescence correlation spectroscopy

We report the detection of heterogeneities in the diffusion of lipid molecules for the three-component mixture dipalmitoyl-PC/dilauroyl-PC/cholesterol, a chemically simple lipid model for the mammalian plasma membrane outer leaflet. Two-color fluorescence correlation spectroscopy (FCS) was performed on giant unilamellar vesicles (GUVs) using fluorescent probes that have differential lipid phase partition behavior--DiO-C18:2 favors disordered fluid lipid phases, whereas DiI-C20:0 prefers spatially ordered lipid phases. Simultaneously-obtained fluorescence autocorrelation functions from the same excitation volume for each dye showed that, depending on the lipid composition of this ternary mixture, the two dyes exhibited different lateral mobilities in regions of the phase diagram with previously proposed submicroscopic two-phase coexistence. In one-phase regions, both dyes reported identical diffusion coefficients. Two-color FCS thus may be detecting local membrane heterogeneities at size scales below the optical resolution limit, either due to short-range order in a single phase or due to submicroscopic phase separation.     

Pardaxin Permeabilizes Vesicles More Efficiently by Pore Formation than by Disruption

Pardaxin is a 33-amino-acid neurotoxin from the Red Sea Moses sole Pardachirus marmoratus, whose mode of action shows remarkable sensitivity to lipid chain length and charge, although the effect of pH is unclear. Here we combine optical spectroscopy and dye release experiments with laser scanning confocal microscopy and natural abundance ¹³C solid-state nuclear magnetic resonance to provide a more complete picture of how pardaxin interacts with lipids. The kinetics and efficiency of release of entrapped calcein is highly sensitive to pH. In vesicles containing zwitterionic lipids (PC), release occurs most rapidly at low pH, whereas in vesicles containing 20% anionic lipid (PG), release occurs most rapidly at high pH. Pardaxin forms stable or transient pores in PC vesicles that allow release of contents without loss of vesicle integrity, whereas the inclusion of PG promotes total vesicle collapse. In agreement with this, solid-state nuclear magnetic resonance reveals that pardaxin takes up a trans-membrane orientation in 14-O-PC/6-O-PC bicelles, whereas the inclusion of 14-0-PG restricts it to contacts with lipid headgroups, promoting membrane lysis. Pore formation in zwitterionic vesicles is more efficient than lysis of anionic vesicles, suggesting that electrostatic interactions may trap pardaxin in several suboptimal interconverting conformations on the membrane surface.     

Interaction of wheat alpha-thionin with large unilamellar vesicles.

The interaction of the wheat antibacterial peptide alpha-thionin with large unilamellar vesicles has been investigated by means of fluorescence spectroscopy. Binding of the peptide to the vesicles is followed by the release of vesicle contents, vesicle aggregation, and lipid mixing. Vesicle fusion, i.e., mixing of the aqueous contents, was not observed. Peptide binding is governed by electrostatic interactions and shows no cooperativity. The amphipatic nature of wheat alpha-thionin seems to destabilize the membrane bilayer and trigger the aggregation of the vesicles and lipid mixing. The presence of distearoylphosphatidylethanolamine-poly(ethylene glycol 2000) (PEG-PE) within the membrane provides a steric barrier that inhibits vesicle aggregation and lipid mixing but does not prevent leakage. Vesicle leakage through discrete membrane channels is unlikely, because the release of encapsulated large fluorescent dextrans is very similar to that of 8-aminonaphthalene-1,3,6,trisulfonic acid (ANTS). A minimum number of 700 peptide molecules must bind to each vesicle to produce complete leakage, which suggests a mechanism in which the overall destabilization of the membrane is due to the formation of transient pores rather than discrete channels.     

Visualization of Membrane Loss during the Shrinkage of Giant Vesicles under Electropulsation

We study the effect of permeabilizing electric fields applied to two different types of giant unilamellar vesicles, the first formed from EggPC lipids and the second formed from DOPC lipids. Experiments on vesicles of both lipid types show a decrease in vesicle radius, which is interpreted as being due to lipid loss during the permeabilization process. We show that the decrease in size can be qualitatively explained as a loss of lipid area, which is proportional to the area of the vesicle that is permeabilized. Three possible modes of membrane loss were directly observed: pore formation, vesicle formation, and tubule formation.     

Divalent cation induced fusion and lipid lateral segregation in phosphatidylcholine-phosphatidic acid vesicles

The interactions of unilamellar vesicles containing phosphatidylcholine (PC) and phosphatidic acid (PA) in the presence of calcium and magnesium were examined by fluorometric assays of vesicle lipid mixing, contents mixing, and contents leakage and by spray-freezing freeze-fracture electron microscopy. These results were correlated with calorimetric and fluorometric measurements of divalent cation induced lateral segregation of lipids in these vesicles under comparable conditions. PA-PC vesicles in the presence of calcium show a rapid but limited intermixing of vesicle lipids and contents, the extent of which increases as the vesicle size decreases or the PA content increases. Calcium produces massive aggregation and efficient mixing of the contents of vesicles containing high proportions of dioleoyl-PA or egg PA, but vesicle coalescence in the latter case is followed rapidly by vesicle collapse and massive leakage of contents. The effects of magnesium are similar for vesicles of very high PA content. However, in the presence of magnesium, vesicles containing lower amounts of PA exhibit "hemifusion", a mode of interaction in which vesicles aggregate and mix approximately 50% of their lipids, apparently representing the lipids of the outer monolayer of each vesicle, without significant mixing of vesicle contents or collapse of the vesicles. Fluorometric measurements of lipid lateral segregation demonstrate that lateral redistribution of lipids in PA-PC vesicles begins at submillimolar concentrations of divalent cations and shows no abrupt change at the "threshold" divalent cation concentration, above which coalescence of vesicles is observed. By correlating calorimetric and fluorometric measurements of lipid lateral segregation and mixing of vesicle components, we can demonstrate that lipid segregation is at least strongly correlated with calcium-promoted coalescence of PA-PC vesicles and is essential to the magnesium-promoted interactions of vesicles of low PA contents.     

Rapid transbilayer movement of ceramides in phospholipid vesicles and in human erythrocytes

The transbilayer diffusion of unlabeled ceramides with different acyl chains (C6-Cer, C10-Cer, and C16-Cer) was investigated in giant unilamellar vesicles (GUVs) and in human erythrocytes. Incorporation of a very small percentage of ceramides (approximately 0.1% of total lipids) to the external leaflet of egg phosphatidylcholine GUVs suffices to trigger a shape change from prolate to pear shape vesicle. By observing the reversibility of this shape change the transmembrane diffusion of lipids was inferred. We found a half-time for unlabeled ceramide flip-flop below 1 min at 37 degrees C. The rapid diffusion of ceramides in a phosphatidylcholine bilayer was confirmed by flip-flop experiments with a spin-labeled ceramide analogue incorporated into large unilamellar vesicles. Shape change experiments were also carried out with human erythrocytes to determine the trans-membrane diffusion of unlabeled ceramides into a biological membrane. Addition of exogenous ceramides to the external leaflet of human erythrocytes did not trigger echinocyte formation immediately as one would anticipate from an asymmetrical accumulation of new amphiphiles in the outer leaflet but only after approximately 15 min of incubation at 20 degrees C in the presence of an excess of ceramide. We interpret these data as being indicative of a rapid ceramide equilibration between both erythrocyte leaflets as indicated also by electron spin resonance spectroscopy with a spin-labeled ceramide. The late appearance of echinocytes could reveal a progressive trapping of a fraction of the ceramide molecules in the outer erythrocytes leaflet. Thus, we cannot exclude the trapping of ceramides into plasma membrane domains.     

Cascades of transient pores in giant vesicles: line tension and transport

Under ordinary circumstances, the membrane tension of a giant unilamellar vesicle is essentially nil. Using visible light, we stretch the vesicles, increasing the membrane tension until the membrane responds by the sudden opening of a large pore (several micrometers in size). Only a single pore is observed at a time in a given vesicle. However, a cascade of transient pores appear, up to 30-40 in succession, in the same vesicle. These pores are transient: they reseal within a few seconds as the inner liquid leaks out. The membrane tension, which is the driving force for pore opening, is relaxed with the opening of a pore and the leakage of the inner liquid; the line tension of the pore's edge is then able to drive the closure of a pore. We use fluorescent membrane probes and real-time videomicroscopy to study the dynamics of the pores. These can be visualized only if the vesicles are prepared in a viscous solution to slow down the leakout of the internal liquid. From measurements of the closure velocity of the pores, we are able to infer the line tension,. We have studied the effect of the shape of inclusion molecules on. Cholesterol, which can be modeled as an inverted cone-shaped molecule, increases the line tension when incorporated into the bilayers. Conversely, addition of cone-shaped detergents reduces. The effect of some detergents can be dramatic, reducing by two orders of magnitude, and increasing pore lifetimes up to several minutes. We give some examples of transport through transient pores and present a rough measurement of the leakout velocity of the inner liquid through a pore. We discuss how our results can be extended to less viscous aqueous solutions which are more relevant for biological systems and biotechnological applications.     

Asymmetric pore distribution and loss of membrane lipid in electroporated DOPC vesicles.

An externally applied electric field across vesicles leads to transient perforation of the membrane. The distribution and lifetime of these pores was examined using 1,2-di-oleoyl-sn-glycero-3-phosphocholine (DOPC) phospholipid vesicles using a standard fluorescent microscope. The vesicle membrane was stained with a fluorescent membrane dye, and upon field application, a single membrane pore as large as approximately 7 microm in diameter was observed at the vesicle membrane facing the negative electrode. At the anode-facing hemisphere, large and visible pores are seldom found, but formation of many small pores is implicated by the data. Analysis of pre- and post-field fluorescent vesicle images, as well as images from negatively stained electron micrographs, indicate that pore formation is associated with a partial loss of the phospholipid bilayer from the vesicle membrane. Up to approximately 14% of the membrane surface could be lost due to pore formation. Interestingly, despite a clear difference in the size distribution of the pores observed, the effective porous areas at both hemispheres was approximately equal. Ca(2+) influx measurements into perforated vesicles further showed that pores are essentially resealed within approximately 165 ms after the pulse. The pore distribution found in this study is in line with an earlier hypothesis (E. Tekle, R. D. Astumian, and P. B. Chock, 1994, Proc. Natl. Acad. Sci. U.S.A. 91:11512--11516) of asymmetric pore distribution based on selective transport of various fluorescent markers across electroporated membranes.     

Effects of the pore-forming agent nystatin on giant phospholipid vesicles

The effects of the polyene pore-forming agent nystatin were investigated on individual giant unilamellar phospholipid vesicles (GUVs), made of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), in different methanol-water solutions using phase-contrast optical microscopy. Three characteristic effects were detected in three different nystatin concentration ranges: vesicle shape changes (between 150 and 250μM); transient, nonspecific, tension pores (between 250 and 400μM); and vesicle ruptures (above 400μM). Both the appearance of the transient tension pores and the vesicle ruptures were explained as being a consequence of the formation of size-selective nystatin channels, whose membrane area density increases with the increasing nystatin concentrations. Our results also show that nystatin is able to form pores in the absence of sterols. In addition, study of the cross-interactions between nystatin and methanol revealed mutually antagonizing effects on the vesicle behavior for methanol volume fractions higher than 10%.     

The response of giant phospholipid vesicles to pore-forming peptide melittin

The interaction between the pore-forming peptide melittin (MLT) and giant phospholipid vesicles was explored experimentally. Micromanipulation and direct optical observation of a vesicle (loaded with sucrose solution and suspended in isomolar glucose solution) enabled the monitoring of a single vesicle response to MLT. Time dependences of the vesicle size, shape and the composition of the inner solution were examined at each applied concentration of MLT (in the range from 1 to 60 μg/ml). The response varied with MLT concentration from slight perturbation of the membrane to disintegration of the vesicle. A model for MLT-vesicle interaction is proposed that explains the observed phenomena in the entire span of MLT concentrations and is consistent with deduced underlying mechanisms of MLT action: trans-membrane positioning and dimerization of MLT, the lipid flow from the outer to the inner membrane leaflet induced by MLT translocation, formation of pores and the consequent transport of small molecules through the membrane. The results of the theoretical analysis stress the role of dimers in the MLT-membrane interaction and demonstrate that the MLT-induced membrane permeability for sugar molecules in this experimental set-up depends on both MLT concentration and time.