Fusion and lipid exchange in vesicles containing lipophilic spin labels

Lipophilic non-electrolyte spin labels greatly accelerate the fusion of unilamellar vesicles of dipalmitoylphosphatidylcholine when the system is maintained below the lipid phase transition. Differential scanning calorimetry and centrifugation measurements show that the transformed vesicles are large and probably unilamellar. Differential scanning calorimetry and fluorescence depolarization measurements were also carried out on mixtures of labeled dipalmitoylphosphatidylcholine vesicles and of vesicles composed of pure dimyristoylphosphatidylcholine. A mixing of the membrane components is observed when the vesicles are incubated above the transition temperature of the two constituent lipids. However, the process does not involve a real fusion of the entire vesicles. An exchange of lipid and label monomers between the two lipid phases seems to occur. These observations are discussed in view of the molecular organization of the spin label within the dipalmitoylphosphatidylcholine matrix below and above the lipid transition temperature.     

Complexity of lipid domains and rafts in giant unilamellar vesicles revealed by combining imaging and microscopic and macroscopic time-resolved fluorescence

The application of fluorescence lifetime imaging microscopy to study gel/fluid and raftlike lipid domains in giant unilamellar vesicles (GUVs) is demonstrated here. Different regions of the ternary dipalmitoylphosphatidylcholine/dioleoylphosphatidylcholine/cholesterol phase diagram were studied. The head-labeled phospholipid Rhodamine-dioleoylphosphatidylethanolamine (Rhod-DOPE) was used as a fluorescent probe. Gel/fluid and liquid-ordered (l(o))/liquid-disordered (l(d)) phase separation were clearly visualized upon two-photon excitation. Fluorescence intensity decays in different regions of a GUV were also obtained with the microscope in fixed laser-beam configuration. The ensemble behavior of the system was studied by obtaining fluorescence intensity decays of Rhod-DOPE in nongiant vesicle suspensions. The fingerprints for gel/fluid coexistence and for the presence of l(o) raftlike phase, based on fluorescence lifetime imaging microscopy histograms and images, and on the fluorescence intensity decay parameters of Rhod-DOPE, are presented. The presence of three lipid phases in one single GUV is detected unequivocally. From the comparison of lifetime parameters, it can be concluded that the l(o) phase is formed in the binary dipalmitoylphosphatidylcholine/cholesterol but not in the dioleoylphosphatidylcholine/cholesterol mixture. The domains apparent in fluorescence intensity images have a more complex substructure revealed by analysis of the lifetime data. The potential applications of this combined imaging/microscopic/macroscopic methodology are discussed.     

Effects of alcohol-induced lipid interdigitation on proton permeability in L-alpha-dipalmitoylphosphatidylcholine vesicles.

6-Carboxyfluorescein was employed to examine the effect of alcohol-induced lipid interdigitation on proton permeability in L-alpha-dipalmitoylphosphatidylcholine (DPPC) large unilamellar vesicles. Proton permeability was measured by monitoring the decrease of 6-carboxyfluorescein fluorescence after a pH gradient from 3.5 (outside the vesicle) to 8.0 (inside the vesicle) was established. At 20 degrees C and below 1.2 M ethanol, the fluorescence decrease is best described by a single exponential function. Above 1.2 M ethanol, the intensity decrease is better described by a two-exponential decay law. Using the fitted rate constants and the vesicle radii determined from light-scattering measurements, the proton permeability coefficient, P, in DPPC vesicles was calculated as a function of ethanol concentration. At 20 degrees C, P increases monotonically with increasing ethanol content up to 1.0 M, followed by an abrupt increase at 1.2 M. The vesicle size also exhibits a sudden increase at around 1.2 M ethanol, which has been shown to result from vesicle aggregation rather than vesicle fusion. The abrupt increases in P and in vesicle size occur at the concentration region close to the critical ethanol concentration for the formation of the fully interdigitated gel state of DPPC. At 14 degrees C, the abrupt change in P shifts to 1.9-2.0 M ethanol, completely in accordance with the ethanol-temperature phase diagram of interdigitated DPPC. Effects of methanol and benzyl alcohol on lipid interdigitation have also been examined. At 20 degrees C, DPPC large unilamellar vesicles exhibit a dramatic change in P at 3 M methanol and at 40 mM benzyl alcohol. These concentrations come close to the critical methanol and benzyl alcohol concentrations for the formation of fully interdigitated DPPC structures determined previously by others. It can be concluded that proton permeability increases dramatically as DPPC is transformed from the noninterdigitated gel to the fully interdigitated gel state by high concentrations of alcohol. This marked increase in proton permeability can be attributed to the combined effect of the changes in membrane thickness and surface charge density, due to the ethanol-induced lipid interdigitation. The possible effects of the increased proton permeability caused by ingested ethanol on gastric mucosal membranes are discussed.     

Morphology and phase behavior of two types of unilamellar vesicles prepared from synthetic phosphatidylcholines studied by freeze-fracture electron microscopy and calorimetry

Differential scanning calorimetry and freeze-fracture electron microscopy have been used to characterize the phase behavior and morphology of two types of unilamellar vesicles composed of synthetic phosphatidylcholines. The first type displayed an average diameter of roughly 100 nm and was formed by slow dilution and dialysis of octylglucoside-solubilized lipid. These large, unilamellar vesicles were termed dialyzed, octylglucoside vesicles and could be obtained as a fairly well defined and uniform population of vesicles. The second vesicle type was prepared by a unique procedure involving dialysis of deoxycholate-solubilized lipid at its pre-transition temperature. This procedure produced a much more heterogeneous distribution of vesicle sizes (500 to 4000 nm in diameter) and left some dilamellar and oligolamellar species which could not be conveniently separated from the giant, unilamellar vesicles constituting the major portion of the sample. Both populations of vesicles displayed phase behavior similar, but not identical to that of large, multilamellar vesicles (LMV). Fracture-face morphology of the gel phase was also observed to differ between the two unilamellar and the multilamellar species. LMV have previously been shown to have clear undulated or banded fracture-faces in the P beta phase, while octylglucoside vesicles are shown here to have facetted fracture-faces. Giant, unilamellar vesicles displayed a faint banded morphology similar to but less distinct than that of the LMV P beta phase. These results have demonstrated that bilayer apposition is not required to support the banded fracture-face morphology characteristic of the P beta phase but that a limiting curvature is necessary.     

The temporal sequence of events in the activation of phospholipase A2 by lipid vesicles. Studies with the monomeric enzyme from Agkistrodon piscivorus piscivorus

The substrate dependence of the time courses of hydrolysis of both small and large unilamellar vesicles of dipalmitoylphosphatidylcholine (DPPC) by Agkistrodon piscivorus piscivorus monomeric phospholipase A2 is consistent with an activation process involving enzyme aggregation on the vesicle surface. The time course of hydrolysis of large unilamellar vesicles is particularly complex; a slow initial rate of hydrolysis is followed by an extremely abrupt increase in enzyme activity. The length of this slow phase is a minimum at the phase transition temperature of the vesicles. The intrinsic fluorescence intensity of the phospholipase A2 also abruptly increases (50-60%) after a latency period revealing a strong temporal correlation between enzyme activity and the increase in fluorescence intensity. The length of the latency period before the sudden increase in fluorescence intensity is directly proportional to substrate concentration at DPPC concentrations above 20-100 microM. At lower concentrations, the length of the latency period is inversely proportional to the DPPC concentration. Such biphasic substrate dependence is predicted by a previously proposed enzyme activation model involving dimerization on the surface vesicle. Simultaneous monitoring of the protein fluorescence and hydrolysis demonstrates that the magnitude of the fluorescence change and the rate of hydrolysis are in exact temporal correlation. Furthermore, simultaneous monitoring of the fluorescence of the protein and that of a lipid probe, trimethylammonium diphenylhexatriene, indicates a change in lipid vesicle structure prior to, or coincident with, the abrupt change in protein activation. These results are consistent with the hypothesis that the monomeric phospholipase A2 from A. piscivorus piscivorus initially possesses a low level of intrinsic activity toward large unilamellar DPPC vesicles and that the enzyme slowly becomes further activated on the vesicle surface via dimerization. Eventually, the vesicles undergo an abrupt transition in internal structure leading to sudden rapid activation of the enzyme.     

Effects of hemagglutinin fusion peptide on poly(ethylene glycol)-mediated fusion of phosphatidylcholine vesicles.

The effects of hemagglutinin (HA) fusion peptide (X-31) on poly(ethylene glycol)- (PEG-) mediated vesicle fusion in three different vesicle systems have been compared: dioleoylphosphatidylcholine (DOPC) small unilamellar vesicles (SUV) and large unilamellar vesicles (LUV) and palmitoyloleoylphosphatidylcholine (POPC) large unilamellar perturbed vesicles (pert. LUV). POPC LUVs were asymmetrically perturbed by hydrolyzing 2.5% of the outer leaflet lipid with phospholipase A(2) and removing hydrolysis products with BSA. The mixing of vesicle contents showed that these perturbed vesicles fused in the presence of PEG as did DOPC SUV, but unperturbed LUV did not. Fusion peptide had different effects on the fusion of these different types of vesicles: fusion was not induced in the absence of PEG or in unperturbed DOPC LUV even in the presence of PEG. Fusion was enhanced in DOPC SUV at low peptide surface occupancy but hindered at high surface occupancy. Finally, fusion was hindered in proportion to peptide concentration in perturbed POPC LUV. Contents leakage assays demonstrated that the peptide enhanced leakage in all vesicles. The peptide enhanced lipid transfer between both fusogenic and nonfusogenic vesicles. Peptide binding was detected in terms of enhanced tryptophan fluorescence or through transfer of tryptophan excited-state energy to membrane-bound diphenylhexatriene (DPH). The peptide had a higher affinity for vesicles with packing defects (SUV and perturbed LUV). Quasi-elastic light scattering (QELS) indicated that the peptide caused vesicles to aggregate. We conclude that binding of the fusion peptide to vesicle membranes has a significant effect on membrane properties but does not induce fusion. Indeed, the fusion peptide inhibited fusion of perturbed LUV. It can, however, enhance fusion between highly curved membranes that normally fuse when brought into close contact by PEG.     

The internal aqueous volume of small unilamellar vesicles changes at the phase transition temperature of the phospholipid

Changes in the fluorescence of partially self-quenched 5(6)-carboxyfluorescein trapped within the internal aqueous compartment of small unilamellar dipalmitoylphosphatidylcholine vesicles indicate that the trapped volume of these vesicles decreases when the phospholipid undergoes the liquid crystalline to gel state transition. This volume change is completely reversible and is not caused by vesicle-vesicle fusion. Furthermore, this decrease in volume of the internal aqueous compartment may be attributed to a change in vesicle shape upon undergoing the phase transition.     

Comparative study of an adenosine triphosphatase trigger-fused lipid vesicle and other vesicle forms of dimyristoylphosphatidylcholine

Several known forms of bilayer vesicles of dimyristoylphosphatidylcholine exhibit the gel to liquid-crystalline phase transition in the temperature range convenient for membrane enzyme reconstitution studies. This warrants a systematic investigation of their physical characteristics and their phase transition behaviors. We have employed electron microscopy, gel chromatography, 31P nuclear magnetic resonance, differential scanning microcalorimetry, and fluorescence spectroscopy to determine several physical parameters of the limiting size microvesicle (260 +/- 40 A), the larger vesicle form (900 +/- 100A) of Enoch and Strittmatter [Enoch, H. G., & Strittmatter, P. (1979) Proc. Natl. Acad. Sci. U.S.A. 76, 145], the multilamellar vesicle, and, in particular, an ATPase-trigger-fused macrovesicle (950 +/- 200 A). This latter vesicle form was produced by a spontaneous fusion of the complex of the plasma membrane ATPase of Schizosaccharomyces pombe and the lipid microvesicles at a low ratio of enzyme to vesicle concentrations, and at a low temperature (around 10 degrees C). The ATPase-trigger-fused vesicles are unilamellar and have an intact ionic permeation barrier at 30 degrees C and a gel to liquid-crystalline transition temperature at 24.4 degrees C with a transition heat of 5.64 kcal/mol. Thus, this vesicle form should be a valuable tool for studying possible proton-pumping activity of this ATPase. In contrast to data found in the literature, which show lack of the pretransition for unilamellar microvesicles, we have observed the pretransition around 15 degrees C for all the vesicle forms examined. Moreover, the transition widths of unilamellar vesicles are much broader than those of the multilamellar vesicles, suggesting that in the latter system interlayer interactions may contribute to the cooperativity of the transition.     

Effects of lipid headgroup and packing stress on poly(ethylene glycol)-induced phospholipid vesicle aggregation and fusion.

The effect of lipid headgroup and curvature-related acyl packing stress on PEG-induced phospholipid vesicle aggregation and fusion were studied by measuring vesicle and aggregate sizes using the quasi-elastic light scattering and fluorescence energy transfer techniques. The effect of the lipid headgroup was monitored by varying the relative phosphatidylcholine (PC) and phosphatidylethanolamine (PE) contents in the vesicles, and the influence of hydrocarbon chain packing stress was controlled either by the relative amount of PE and PC content in the vesicles, or by the degree of unsaturation of the acyl chains of a series of PEs, e.g., dilinoleoylphosphatidylethanolamine (dilin-PE), lysophosphatidylethanolamine (lyso-PE), and transacylated egg phosphatidylethanolamine (TPE). The PEG threshold for aggregation depends only weakly on the headgroup composition of vesicles. However, in addition to the lipid headgroup, the curvature stress of the monolayer that forms the vesicle walls plays a very important role in fusion. Highly stressed vesicles, i.e., vesicles containing PE with highly unsaturated chains, need less PEG to induce fusion. This finding applies to the fusion of both small unilamellar vesicles and large unilamellar vesicles. The effect of electrostatic charge on vesicle aggregation and fusion were studied by changing the pH of the vesicle suspension media. At pH 9, when PE headgroups are weakly charged, increasing electrostatic repulsion between headgroups on the same bilayer surface reduces curvature stress, whereas increasing electrostatic repulsion between apposing bilayer headgroups hinders intervesicle approach, both of which inhibit aggregation and fusion, as expected.     

Temperature-induced fusion of small unilamellar vesicles formed from saturated long-chain lecithins and diheptanoylphosphatidylcholine

Small unilamellar vesicles which form when gel-state long-chain phosphatidylcholines are mixed with micellar short-chain lecithins undergo an increase in size as the long-chain species melts to its liquid-crystalline form. Analysis of the vesicle population with quasi-elastic light scattering shows that the particle size increases from 90-A radius to greater than 5000-A radius. Resonance energy transfer experiments show total mixing of lipid probes with unlabeled vesicles only when the Tm of the long-chain phosphatidylcholine is exceeded. This implies that the large size change represents a fusion process. Aqueous compartments are also mixed during this transition. 31P NMR analysis of the vesicle mixtures above the phase transition shows a great degree of heterogeneity with large unilamellar particles coexisting with oligo- and multilamellar structures. Upon cooling the vesicles below the Tm, the original size distribution (e.g., small unilamellar vesicles) is obtained, as monitored by both quasi-elastic light scattering and 31P NMR spectroscopy. This temperature-induced fusion of unilamellar vesicles is concentration dependent and can be abolished at lower total phospholipid concentrations. It occurs over a wide range of long-chain to short-chain ratios and occurs with 1-palmitoyl-2-stearoylphosphatidylcholine and dimyristoylphosphatidylcholine as well. Characterization of this fusion event is used to understand the anomalous kinetics of water-soluble phospholipases toward these unusual vesicles.     

Gramicidin induced aggregation and size increase of phosphatidylcholine vesicles

To investigate the role of membrane proteins in the fusion process, linear hydrophobic polypeptide gramicidin was used as fusogenic agent in small unilamellar vesicles (SUV) constituted of saturated lecithins. It was found that gramicidin, externally added to a suspension of vesicles, induces a reversible vesicles aggregation. When incorporated into the bilayer, gramicidin induces increase in vesicle size. The vesicle size increase was monitored by column chromatography and transmission electron microscopy. The process of vesicle size increase occurs only when the lipid membrane is in the gel state. A maximum is observed in the kinetics at a temperature of approx. 25 degrees C lower than the phase transition temperature of lipids. Higher rates of vesicle size increase are obtained as the lipid chain length increases. The process is accompanied by a release of internal vesicle content and by membrane lipid mixing.     

Liposome fusion catalytically induced by phospholipase C

Large unilamellar vesicles composed of phosphatidylcholine/phosphatidylethanolamine/cholesterol (50:25:25 mole ratio) were treated with phospholipase C. The early stages of phospholipid cleavage are accompanied by mixing of bilayer lipids (monitored by dequenching of octadecylrhodamine fluorescence) and leakage-free mixing of vesicle contents [measured by using 8-aminonaphthalene-1,3,6-trisulfonic acid (ANTS) and p-xylylenebis(pyridinium bromide) (DPX)]. These results are interpreted in terms of vesicle fusion induced by the catalytic activity of phospholipase C. The use of sonicated unilamellar vesicles decreases the lag time, but does not modify the amplitude, of the fusion process. The presence of both phosphatidylethanolamine and cholesterol appears to be essential for measurable fusion effects to occur with low levels of phospholipid hydrolysis. Optimal fusion rates are observed with about 10-20 enzyme molecules per large unilamellar vesicle. This system of catalytically induced liposome fusion may be of relevance for the interpretation of physiological membrane fusion processes.     

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.     

Anthracenyl crown ethers and cryptands as fluorescent probes for solid-phase transitions of phosphatidylcholines: syntheses and phospholipid membrane studies

Three structurally related crown compounds and cryptands have been synthesized that differ by the number and linkage of coronand units and anthracene moieties. The interaction of the fluorescent dyes with sonicated dimyristoylphosphatidylcholine (DMPC) vesicles is characterized by the relative quantum yields, uptake kinetics, binding curves, lifetimes, fluorescence titrations with water- and lipid-soluble quenching agents, fluorescence anisotropy, and equilibrium cooling curves. The most lipophilic compound II, which displays a similar quantum yield as the parent fluorophore 9,10-dimethylanthracene, shows a nearly equal distribution between solid and fluid lipid and is located at the bilayer surface. The least lipophilic compound IV is excluded from the hydrocarbon phase. The anthracenophane cryptand III preferentially partitions into solid-phase lecithins with the highest affinity for the phases L epsilon and L beta. The binding constant to DMPC amounts to (5.4 +/- 1.3) X 10(2) M-1 at 0 degrees C. From fluorescence quenching titrations it is concluded that the average position of the anthracenoyl dye III discontinuously shifts during the gel to liquid crystalline transition from the glycerol backbone to the choline head group. Electron microscopy and NMR experiments revealed that the anthracenophane induces in the liquid crystalline phase the fusion of small unilamellar DMPC vesicles to unilamellar medium-sized vesicles and macrovesicles, which subsequently fuse at the transition temperature to large multilamellar coacervates. Due to its large change of fluorescence intensity, the anthracenophane cryptand is a very sensitive probe for the detection of the pretransition of symmetrically substituted and of the subtransition of asymmetrically substituted phosphatidylcholines.(ABSTRACT TRUNCATED AT 250 WORDS)     

Membrane elasticity in giant vesicles with fluid phase coexistence

Biological membranes are known to contain compositional heterogeneities, often termed rafts, with distinguishable composition and function, and these heterogeneities participate in vigorous transport processes. Membrane lipid phase coexistence is expected to modulate these processes through the differing mechanical properties of the bulk domains and line tension at phase boundaries. In this contribution, we compare the predictions from a shape theory derived for vesicles with fluid phase coexistence to the geometry of giant unilamellar vesicles with coexisting liquid-disordered (L(d)) and liquid-ordered (L(o)) phases. We find a bending modulus for the L(o) phase higher than that of the L(d) phase and a saddle-splay (Gauss) modulus difference with the Gauss modulus of the L(o) phase being more negative than the L(d) phase. The Gauss modulus critically influences membrane processes that change topology, such as vesicle fission or fusion, and could therefore be of significant biological relevance in heterogeneous membranes. Our observations of experimental vesicle geometries being modulated by Gaussian curvature moduli differences confirm the prediction by the theory of Juelicher and Lipowsky.     

Interaction of short-chain lecithin with long-chain phospholipids: characterization of vesicles that form spontaneously

Stable unilamellar vesicles formed spontaneously upon mixing aqueous suspensions of long-chain phospholipid (synthetic, saturated, and naturally occurring phosphatidylcholine, phosphatidylethanolamine, and sphingomyelin) with small amounts of short-chain lecithin (fatty acid chain lengths of 6-8 carbons) have been characterized by using NMR spectroscopy, negative staining electron microscopy, differential scanning calorimetry, and Fourier transform infrared (FTIR) spectroscopy. This method of vesicle preparation can produce bilayer vesicles spanning the size range 100 to greater than 1000 A. The combination of short-chain lecithin and long-chain lecithin in its gel state at room temperature produces relatively small unilamellar vesicles, while using long-chain lecithin in its liquid-crystalline state produces large unilamellar vesicles. The length of the short-chain lecithin does not affect the size distribution of the vesicles as much as the ratio of short-chain to long-chain components. In general, additional short-chain decreases the average vesicle size. Incorporation of cholesterol can affect vesicle size, with the solubility limit of cholesterol in short-chain lecithin micelles governing any size change. If the amount of cholesterol is below the solubility limit of micellar short-chain lecithin, then the addition of cholesterol to the vesicle bilayer has no effect on the vesicle size; if more cholesterol is added, particle growth is observed. Vesicles formed with a saturated long-chain lecithin and short-chain species exhibit similar phase transition behavior and enthalpy values to small unilamellar vesicles of the pure long-chain lecithin prepared by sonication. As the size of the short-chain/long-chain vesicles decreases, the phase transition temperature decreases to temperatures observed for sonicated unilamellar vesicles. FTIR spectroscopy confirms that the incorporation of the short-chain lipid in the vesicle bilayer does not drastically alter the gauche bond conformation of the long-chain lipids (i.e., their transness in the gel state and the presence of multiple gauche bonds in the liquid-crystalline state).     

Comparison of the enthalpy state of vesicles of different size by their interaction with alpha-lactalbumin

The characteristics of small unilamellar, large unilamellar and large multilamellar vesicles of dimyristoylphosphatidylcholine and their interaction with alpha-lactalbumin are compared at pH 4. (1) By differential scanning calorimetry and from steady-state fluorescence anisotropy data of the lipophilic probe 1,6-diphenyl-1,3,5-hexatriene it is shown that the transition characteristics of the phospholipids in the large unilamellar vesicles resemble more those of the multilamellar vesicles than of the small unilamellar vesicles. (2) The size and composition of the lipid-protein complex formed with alpha-lactalbumin around the transition temperature of the lipid are independent of the vesicle type used. Fluorescence anisotropy data indicate that in this complex the motions of the lipid molecules are strongly restricted in the presence of alpha-lactalbumin. (3) The previous data and a comparison of the enthalpy changes, delta H, of the interaction of the three vesicle types with alpha-lactalbumin allow us to derive that the enthalpy state of the small unilamellar vesicles just below 24 degrees C is about 24 kJ/mol lipid higher than the enthalpy state of both large vesicle types at the same temperature. The abrupt transition from endothermic to exothermic delta H values around 24 degrees C for large vesicles approximates the transition enthalpy of the pure phospholipid.     

Interaction of intestinal brush border membrane vesicles with small unilamellar phospholipid vesicles. Exchange of lipids between membranes is mediated by collisional contact

The kinetics of lipid transfer from small unilamellar vesicles as the donor to brush border vesicles as the acceptor have been investigated by following the transfer of radiolabeled or spin-labeled lipid molecules in the absence of exchange protein. The labeled lipid molecules studied were various radiolabeled and spin-labeled phosphatidylcholines, radiolabeled cholesteryl oleate, and a spin-labeled cholestane. At a given temperature and brush border vesicle concentration similar pseudo-first-order rate constants (half-lifetimes) were observed for different lipid labels used. The lipid transfer is shown to be an exchange reaction leading to an equal distribution of label in donor and acceptor vesicles at equilibrium (time t----infinity). The lipid exchange is a second-order reaction with rate constants being directly proportional to the brush border vesicle concentration. The results are only consistent with a collision-induced exchange of lipid molecules between small unilamellar phospholipid vesicles and brush border vesicles. Other mechanisms such as collision-induced fusion or diffusion of lipid monomers through the aqueous phase are negligible at least under our experimental conditions.     

Morphological changes induced by phospholipase C and by sphingomyelinase on large unilamellar vesicles: a cryo-transmission electron microscopy study of liposome fusion

Cryo-transmission electron microscopy has been applied to the study of the changes induced by phospholipase C on large unilamellar vesicles containing phosphatidylcholine, as well as to the action of sphingomyelinase on vesicles containing sphingomyelin. In both cases vesicle aggregation occurs as the earliest detectable phenomenon; later, each system behaves differently. Phospholipase C induces vesicle fusion through an intermediate consisting of aggregated and closely packed vesicles (the "honeycomb structure") that finally transforms into large spherical vesicles. The same honeycomb structure is also observed in the absence of enzyme when diacylglycerols are mixed with the other lipids in organic solution, before hydration. In this case the sample then evolves toward a cubic phase. The fact that the same honeycomb intermediate can lead to vesicle fusion (with enzyme-generated diacylglycerol) or to a cubic phase (when diacylglycerol is premixed with the lipids) is taken in support of the hypothesis according to which a highly curved lipid structure ("stalk") would act as a structural intermediate in membrane fusion. Sphingomyelinase produces complete leakage of vesicle aqueous contents and an increase in size of about one-third of the vesicles. A mechanism of vesicle opening and reassembling is proposed in this case.     

Aggregation and fusion of unilamellar vesicles by poly(ethylene glycol)

Various aspects of the interaction between the fusogen, poly(ethylene glycol) and phospholipids were examined. The aggregation and fusion of small unilamellar vesicles of egg phosphatidylcholine (PC), bovine brain phosphatidylserine (PS) and dimyristoylphosphatidylcholine (DMPC) were studied by dynamic light scattering, electron microscopy and NMR. The fusion efficiency of Dextran, glycerol, sucrose and poly(ethylene glycol) of different molecular weights were compared. Lower molecular weight poly(ethylene glycol) are less efficient with respect to both aggregation and fusion. The purity of poly(ethylene glycol) does not affect its fusion efficiency. Dehydrating agents, such as Dextran, glycerol and sucrose, do not induce fusion. 31P-NMR results revealed a restriction in the phospholipid motion by poly(ethylene glycol) greater than that by glycerol and Dextran of similar viscosity and dehydrating capacity. This may be associated with the binding of poly(ethylene glycol) to egg PC, with a binding capacity of 1 mol of poly(ethylene glycol) to 12 mol of lipid. Fusion is greatly enhanced below the phase transition for DMPC, with extensive fusion occurring below 6% poly(ethylene glycol). Fusion of PS small unilamellar vesicles depends critically on the presence of cations. Large unilamellar vesicles were found to fuse less readily than small unilamellar vesicles. The results suggest that defects in the bilayer plays an important role in membrane fusion, and the 'rigidization' of the phospholipid molecules facilitates fusion possibly through the creation of defects along domain boundaries. Vesicle aggregation caused by dehydration and surface charge neutralization is a necessary but not a sufficient condition for fusion.