Exchange and flip-flop of dimyristoylphosphatidylcholine in liquid-crystalline, gel, and two-component, two-phase large unilamellar vesicles

The rate and extent of spontaneous exchange of dimyristoylphosphatidylcholine (DMPC) from large unilamellar vesicles (LUV) composed of either DMPC or mixtures of DMPC/distearoylphosphatidylcholine (DSPC) have been examined under equilibrium conditions. The phase state of the vesicles ranged from all-liquid-crystalline through mixed gel/liquid-crystalline to all-gel. The exchange rate of DMPC between liquid-crystalline DMPC LUV, measured between 25 and 55 degrees C, was found to have an Arrhenius activation energy of 24.9 +/- 1.4 kcal/mol. This activation energy and the exchange rates are very similar to those obtained for the exchange of DMPC between DMPC small unilamellar vesicles (SUV). The extent of exchange of DMPC in LUV was found to be approximately 90%. This is in direct contrast to the situation in DMPC SUV where only the lipid in the outer monolayer is available for exchange. Thus, transbilayer movement (flip-flop) is substantially faster in liquid-crystalline DMPC LUV than in SUV. Desorption from gel-phase LUV has a much lower rate than gel-phase SUV with an activation energy of 31.7 +/- 3.7 kcal/mol compared to 11.5 +/- 2 kcal/mol reported for SUV. A defect-mediated exchange in gel-phase SUV, which is not the major pathway for exchange in LUV, is proposed on the basis of the thermodynamic parameters of the activation process. Surprisingly, the rates of DMPC exchange between DMPC/DSPC two-component LUV, measured over a wide range of compositions and temperatures, were found to exhibit very little dependence on the composition or phase configuration of the vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Production of RNA by a polymerase protein encapsulated within phospholipid vesicles

Catalyzed polymerization reactions represent a primary anabolic activity of all cells. It can be assumed that early cells carried out such reactions, in which macromolecular catalysts were encapsulated within some type of boundary membrane. In the experiments described here, we show that a template-independent RNA polymerase (polynucleotide phosphorylase) can be encapsulated in dimyristoyl phosphatidylcholine vesicles without substrate. When the substrate adenosine diphosphate (ADP) was provided externally, long-chain RNA polymers were synthesized within the vesicles. Substrate flux was maximized by maintaining the vesicles at the phase transition temperature of the component lipid. A protease was introduced externally as an additional control. Free enzyme was inactivated under identical conditions. RNA products were visualized in situ by ethidium bromide fluorescence. The products were harvested from the liposomes, radiolabeled, and analyzed by polyacrylamide gel electrophoresis. Encapsulated catalysts represent a model for primitive cellular systems in which an RNA polymerase was entrapped within a protected microenvironment.Abbreviations ADP adenosine diphosphate - DMPC dimyristoyl phosphatidylcholine - EDTA ethylenediaminetetraacetic acid - LUV large unilamellar vesicle - MLV multilamellar vesicle - PAGE polyacrylamide gel electrophoresis - PNPase or PNP polynucleotide phosphorylase - SUV small unilamellar vesicle Correspondence to.: A.C. Chakrabarti     

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.     

The relationship between compositional phase separation and vesicle morphology: Implications for the regulation of phospholipase A2 by membrane structure

The action of phospholipase A₂ (PLA₂) on bilayer substrates causes the accumulation of reaction products, lyso-phospholipid and fatty acid. These reaction products and the phospholipid substrate generate compositional heterogeneities and then apparently phase separate when a critical mole fraction of reaction product accumulates in the membrane. This putative phase separation drives an abrupt morphologic rearrangement of the vesicle, which may be in turn responsible for modulating the activity of PLA₂. Here we examine the thermotropic properties of the phase-separated lipid system formed upon hydrating colyophilized reaction products (1:1 palmitic acid:1-palmitoyl-2-lyso-phosphatidylcholine) and substrate, dipalmitoylphosphatidylcholine. The mixture forms structures which are not canonical spherical vesicles and appear to be disks in the gel-state. The main gel-liquid transition of these structures is hysteretic. This hysteresis is apparent using several techniques, each selected for its sensitivity to different aspects of a lipid aggregate's structure. The thermotropic hysteresis reflects the coupling between phase separation and changes in vesicle morphology.     

Phospholipid exchange between bilayer membranes.

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 A) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains trans-delta 9-octadecenoate, the other type trans-delta 9-hexadecenoate as predominant acyl chain component. The vesicles show order in equilibrium disorder transitions at transition temperatures, Tt = 42 degrees C and Tt = 29 degrees C, respectively. A mixture of these vesicles is incubated at 45 degrees C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. trans-delta 9-hexadecenoate-containing lipid molecules appear more rapidly in the trans-delta 9-octadecenoate-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

Physicochemical characterization of large unilamellar phospholipid vesicles prepared by reverse-phase evaporation

Properties of large unilamellar vesicles (LUV), composed of phosphatidylcholine and prepared by reverse-phase evaporation and subsequent extrusion through Unipore polycarbonate membranes, have been investigated and compared with those of small unilamellar vesicles (SUV) and of multilamellar vesicles (MLV). The unilamellar nature of the LUV is shown by 1H-NMR using Pr3+ as a shift reagent. The gel to liquid-crystalline phase transition of LUV composed of dipalmitoylphosphatidylcholine (DPPC) monitored by differential scanning calorimetry, fluorescence polarization of diphenylhexatriene and 90 degrees light scattering, occurs at a slight lower temperature (40.8 degrees C) than that of MLV (42 degrees C) and is broadened by about 50%. The phase transition of SUV is shifted to considerably lower temperatures (mid-point, 38 degrees C) and extends over a wide temperature range. In LUV a well-defined pretransition is not observed. The permeability of LUV (DPPC) monitored by leakage of carboxyfluorescein, increases sharply at the phase transition temperature, and the extent of release is greater than that from MLV. Leakage from SUV occurs in a wide temperature range. Freeze-fracture electron microscopy of LUV (DPPC) reveals vesicles of 0.1-0.2 micron diameter with mostly smooth fracture faces. At temperatures below the phase transition, the larger vesicles in the population have angled faces, as do extruded MLV. A banded pattern, seen in MLV at temperatures between the pretransition and the main transition, is not observed in the smaller LUV, although the larger vesicles reveal a dimpled appearance.     

Membrane fusion and the lamellar-to-inverted-hexagonal phase transition in cardiolipin vesicle systems induced by divalent cations.

The polymorphic phase behavior of bovine heart cardiolipin (CL) in the presence of different divalent cations and the kinetics of CL vesicle fusion induced by these cations have been investigated. (31)P-NMR measurements of equilibrium cation-CL complexes showed the lamellar-to-hexagonal (L(alpha)-H(II)) transition temperature (T(H)) to be 20-25 degrees C for the Sr(2+) and Ba(2+) complexes, whereas in the presence of Ca(2+) or Mg(2+) the T(H) was below 0 degrees C. In the presence of Sr(2+) or Ba(2+), CL large unilamellar vesicles (LUVs) (0.1 microm diameter) showed kinetics of destabilization, as assessed by determination of the release of an aqueous fluorescent dye, which strongly correlated with the L(alpha)-H(II) transition of the final complex: at temperatures above the T(H), fast and extensive leakage, mediated by vesicle-vesicle contact, was observed. On the other hand, mixing of vesicle contents was limited and of a highly transient nature. A different behavior was observed with Ca(2+) or Mg(2+): in the temperature range of 0-50 degrees C, where the H(II) configuration is the thermodynamically favored phase, relatively nonleaky fusion of the vesicles occurred. Furthermore, with increasing temperature the rate and extent of leakage decreased, with a concomitant increase in fusion. Fluorescence measurements, involving incorporation of N-NBD-phosphatidylethanolamine in the vesicle bilayer, demonstrated a relative delay in the L(alpha)-H(II) phase transition of the CL vesicle system in the presence of Ca(2+). Freeze-fracture electron microscopy of CL LUV interaction products revealed the exclusive formation of H(II) tubes in the case of Sr(2+), whereas with Ca(2+) large fused vesicles next to H(II) tubes were seen. The extent of binding of Ca(2+) to CL in the lamellar phase, saturating at a binding ratio of 0.35 Ca(2+) per CL, was close to that observed for Sr(2+) and Ba(2+). It is concluded that CL LUVs in the presence of Ca(2+) undergo a transition that favors nonleaky fusion of the vesicles over rapid collapse into H(II) structures, despite the fact that the equilibrium Ca(2+)-CL complex is in the H(II) phase. On the other hand, in the presence of Sr(2+) or Ba(2+) at temperatures above the T(H) of the respective cation-CL complexes, CL LUVs rapidly convert to H(II) structures with a concomitant loss of vesicular integrity. This suggests that the nature of the final cation-lipid complex does not primarily determine whether CL vesicles exposed to the cation will initially undergo a nonleaky fusion event or collapse into nonvesicular structures.     

Modulation of membrane fusion by membrane fluidity: temperature dependence of divalent cation induced fusion of phosphatidylserine vesicles

We have investigated the temperature dependence of the fusion of phospholipid vesicles composed of pure bovine brain phosphatidylserine (PS) induced by Ca2+ or Mg2+. Aggregation of the vesicles was monitored by 90 degrees light-scattering measurements, fusion by the terbium/dipicolinic acid assay for mixing of internal aqueous volumes, and release of vesicle contents by carboxyfluorescein fluorescence. Membrane fluidity was determined by diphenylhexatriene fluorescence polarization measurements. Small unilamellar vesicles (SUV, diameter 250 A) or large unilamellar vesicles (LUV, diameter 1000 A) were used, and the measurements were done in 0.1 M NaCl at pH 7.4. The following results were obtained: (1) At temperatures (0-5 degrees C) below the phase transition temperature (Tc) of the lipid, LUV (PS) show very little fusion in the presence of Ca2+, although vesicle aggregation is rapid and extensive. With increasing temperature, the initial rate of fusion increases dramatically. Leakage of contents at the higher temperatures remains limited initially, but subsequently complete release occurs as a result of collapse of the internal aqueous space of the fusion products. (2) SUV (PS) are still in the fluid state down to 0 degree C, due to the effect of bilayer curvature, and fuse rapidly in the entire temperature range from 0 to 35 degrees C in the presence of Ca2+. The initial rate of leakage is low relative to the rate of fusion. At higher temperatures (15 degrees C and above), subsequent collapse of the vesicles' internal space causes complete release.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of the phase transition on the transbilayer movement of dimyristoyl phosphatidylcholine in unilamellar vesicles

Dimyristoyl phosphatidylcholine rapidly exchanges between vesicles at 37°C without vesicle fusion.The rate of the transbilayer movement of dimyristoyl phosphatidylcholine in sonicated vesicles has been measured employing ¹³C NMR using N-¹³CH_3? labeled lipids which are introduced into the outer monolayer of non-labeled vesicles by a phosphatidylcholine exchange protein. The rate of transbilayer movement of dimyristoyl phosphatidylcholine shows a distinct maximum (halftime 4 h) in the temperature range at which the hydrocarbon phase transition occurs.The activation energy of the flip-flop rate above the phase transition is 23.7 ± 2.0 kcal/mol.     

The effect of loperamide on the thermal behavior of dimyristoylphosphatidylcholine large unilamellar vesicles

The effect of loperamide, a drug belonging to the opiate family, on dimyristoyl phosphatidylcholine large unilamellar vesicles (DMPC LUV) was investigated by quasielastic light scattering (QLS) and Fourier transform infrared spectroscopy (FT-IR). Both techniques show that, in the presence of loperamide, DMPC LUV undergoes a two step transition in cooling: one step around the transition point of pure lipid vesicles, the other at a lower temperature. The temperature of the latter step transition is different for the head and tail regions of the drug-containing vesicles: FT-IR spectra demonstrate that the hydrophobic acyl chains transition starts at a temperature well above that of the interfacial region whereas the transition of the entire vesicle, explored by QLS, is broad and covers both temperature ranges. These transitions are thermally reversible in the FT-IR which measures local order but aggregation effects prevent the thermal reversibility of the QLS results. The nature of the drug-lipid interaction is also discussed.     

Exchange and aggregation in dispersions of dimyristoyl phosphatidylcholine vesicles containing myristic acid

Processes occurring in dispersions of dimyristoyl phosphatidylcholine containing myristic acid have been studied by light scattering of dilute dispersions (concn. ≤ 1 mg/ml) at temperatures above and below the phase transition temperatures of these dispersions. The transition temperatures increase with increasing mol fraction of myristic acid. Above these temperatures, vesicles with different mol fractions of myristic acid exchange lipid molecules. The exchange process leads to vesicles having phase transition temperatures and radii, which are both intermediate between the initial transitions and radii, respectively. In contrast with the observations above the phase transitions, it was found that when dimyristoyl phosphatidylcholine/myristic acid vesicles were cooled to a few degrees below the phase transition, larger particles were formed. These observations are consistent with a mechanism consisting of vesicle aggregation followed by fusion of the aggregated vesicles. The aggregation process is of second order in the vesicle concentration, and its rate increases with increasing mol fraction of myristic acid.     

Studies on membrane fusion. 1. Interactions of pure phospholipid membranes and the effect of myristic acid,lysolecithin, proteins and dimethylsulfoxide

The interaction and mixing of membrane components in sonicated unilamellar vesicles and also non-sonicated multilamellar vesicles prepared from highly purified phospholipids suspended in NaCl solutions has been examined. Electron microscopy and differential scanning calorimetry were used to characterize the extent and kinetics of mixing of membrane components between different vesicle populations. No appreciable fusion was detected between populations of non-sonicated phospholipid vesicles incubated in aqueous salt (NaCl) solutions. Mixing of vesicle membrane components via diffusion of phospholipid molecules between vesicles was observed in populations of negatively charged phosphatidylglycerol vesicles but similar exchange diffusion was not detected in populations of neutral phosphatidylcholine vesicles. Incubation of sonicated vesicle populations at temperatures close to or above the phospholipid transition temperature resulted in an increase in vesicle size and mixing of vesicle membrane components as determined by a gradual change in the thermotropic properties of the mixed vesicle population. The interaction of purified phospholipid vesicles was also examined in the presence of myristic acid and lysolecithin. Our results indicate that while these agents enhance mixing of vesicle membrane components, in most cases mixing probably proceeds via diffusion of phospholipid molecules rather than by fusion of entire vesicles. Increased mixing of vesicle membrane components was also produced when vesicles were prepared containing a purified hydrophobic protein (myelin proteolipid apoprotein) or were incubated in the presence of dimethylsulfoxide. In these two systems, however, the evidence suggests that mixing of membrane components results from the fusion of entire vesicles.     

Hydrolysis of dipalmitoylphosphatidylcholine large unilamellar vesicles by porcine pancreatic phospholipase A2

The interaction between dipalmitoylphosphatidylcholine large unilamellar vesicles and porcine pancreatic phospholipase A2 has been studied under a variety of conditions. It was found that the presence of large unilamellar vesicles inhibits the hydrolysis of small unilamellar vesicles at room temperature, and reaction calorimetric experiments showed that protein-lipid interactions in the absence of Ca2+ occur in the gel state with a stoichiometry of about 40 phospho-lipid molecules/protein-binding site. However, hydrolysis can be induced in the gel state under conditions of osmotic shock. On the other hand, hydrolysis is usually observed within the lipid transition temperature range, but then it occurs only after a latency phase during which the hydrolysis is very slow. The duration of this latency phase reaches a minimum near the phase transition temperature. However, if the enzyme-substrate mixture is heated from low temperatures (continuously or by a temperature jump) to a temperature within the phase transition region, hydrolysis occurs instantaneously. These results are in accordance with the conclusions of the preceding paper (Menashe, M., Romero, G., Biltonen, R. L., and Lichtenberg, D. (1986) J. Biol. Chem. 261, 5328-5333) that effective binding of the enzyme to lipid vesicles occurs relatively rapidly in the gel state and that activation of the enzyme-substrate complex requires the existence of structural irregularities in the lipid bilayer. Although hydrolysis products may have a pronounced effect on the time course of the reaction in the transition range, instantaneous hydrolysis can be induced in the phase transition region in the absence of reaction products by appropriate manipulation of the experimental conditions during which no reaction products are produced. Thus reaction products are not essential for activation of porcine pancreatic phospholipase A2. Furthermore, it is shown that the fraction of lipid hydrolyzed during the latency period is a function of the initial substrate concentration in a manner inconsistent with the proposition that the accumulation of a constant critical fraction of reaction products is the basis for activation. Comparison of the results of this study with those of the preceding paper strongly support the previously proposed reaction scheme.     

Hydrolysis of phosphatidylcholine in phosphatidylcholine-cholate mixtures by porcine pancreatic phospholipase A2

Pancreatic phospholipase A2 (PLA2)-catalyzed hydrolysis of egg yolk phosphatidylcholine (PC) in mixed PC-cholate systems depends upon composition, structure, and size of the mixed aggregates. The hydrolysis of PC-cholate-mixed micelles made of an equal number of PC and cholate molecules is consistent with a Km of about 1 mM and a turnover number of about 120 s-1. Increasing the cholate/PC ratio in the micelles results in a decreased initial velocity. Hydrolysis of cholate-containing unilamellar vesicles is very sensitive to the ratio of cholate to PC in the vesicles. The hydrolysis of vesicles with an effective cholate/PC ratio greater than 0.27 is similar to that of the mixed micelles. The time course of hydrolysis of vesicles with lower effective ratios is similar to that exhibited by pure dipalmitoyl-phosphatidylcholine (DPPC) large unilamellar vesicles in the thermotropic phase transition region. In the latter two cases, the rate of hydrolysis increases with time until substrate depletion becomes significant. The reaction can be divided phenomenologically into two phases: a latency phase where the amount of product formed is a square function of time (P(t) = At2) and a phase distinguished by a sudden increase in activity. The parameter A, which describes the activation rate of the enzyme during the initial phase in a quantitative fashion, increases with increasing [PLA2], decreasing [PC], decreasing vesicle size, and increasing relative cholate content of the vesicles. The effect of [PLA2] and [PC] on the hydrolysis reaction is similar to that found with pure DPPC unilamellar vesicles in their thermotropic phase transition region. The effect of cholate on the hydrolysis reaction is similar to that of temperature variation within the phase transition of temperature variation within the phase transition of DPPC. These results are consistent with our previously proposed model, which postulates that activation of PLA2 involves dimerization of the enzyme on the substrate surface and that the rate of activation is directly proportional to the magnitude of lipid structural fluctuations. It is suggested that large structural fluctuations, which exist in the pure lipid system in the phase transition range, are introduced into liquid crystalline vesicles by the presence of cholate and thus promote activation of the enzyme.     

Inverted micellar intermediates and the transitions between lamellar, cubic, and inverted hexagonal lipid phases. II. Implications for membrane-membrane interactions and membrane fusion.

Results of a kinetic model of thermotropic L alpha----HII phase transitions are used to predict the types and order-of-magnitude rates of interactions between unilamellar vesicles that can occur by intermediates in the L alpha----HII phase transition. These interactions are: outer monolayer lipid exchange between vesicles; vesicle leakage subsequent to aggregation; and (only in systems with ratios of L alpha and HII phase structural dimensions in a certain range or with unusually large bilayer lateral compressibilities) vesicle fusion with retention of contents. It was previously proposed that inverted micellar structures mediate membrane fusion. These inverted micellar structures are thought to form in all systems with such transitions. However, I show that membrane fusion probably occurs via structures that form from these inverted micellar intermediates, and that fusion should occur in only a sub-set of lipid systems that can adopt the HII phase. For single-component phosphatidylethanolamine (PE) systems with thermotropic L alpha----HII transitions, lipid exchange should be observed starting at temperatures several degrees below TH and at all higher temperatures, where TH is the L alpha----HII transition temperature. At temperatures above TH, the HII phase forms between apposed vesicles, and eventually ruptures them (leakage). In most single-component PE systems, fusion via L alpha----HII transition intermediates should not occur. This is the behavior observed by Bentz, Ellens, Lai, Szoka, et al. in PE vesicle systems. Fusion is likely to occur under circumstances in which multilamellar samples of lipid form the so-called "inverted cubic" or "isotropic" phase. This is as observed in the mono-methyl DOPE system (Ellens, H., J. Bentz, and F. C. Szoka. 1986. Fusion of phosphatidylethanolamine containing liposomes and the mechanism of the L alpha-HII phase transition. Biochemistry. In press.) In lipid systems with L alpha----HII transitions driven by cation binding (e.g., Ca2+-cardiolipin), fusion should be more frequent than in thermotropic systems.     

Preparation and characterization of long chain amino acid and peptide vesicle membranes

Four amino acid dicarboxylic amphiphiles which contain cysteine or homocysteine were synthesized. Each forms synthetic bilayer membranes upon hydration. Extensive sonication above the lipid phase transition temperature, 61 to 82 degrees C, produced 1000 A diameter vesicles. Treatment of the vesicles with water-soluble carbodiimides during and after sonication induced oligopeptide formation at the vesicle surface with retention of vesicle size and shape. Size exclusion chromatography indicates the products are predominantly di- to decapeptides. The permeability characteristics of the amino acid and peptide vesicles to [3H]glucose and 6-carboxyfluorescein are reported. The amino acid vesicles are among the least permeable nonpolymerized bilayer vesicles described in the literature to date. Formation of the peptide vesicles increases the membrane permeability, whereas in other polymerizable lipid vesicles the permeability decreases upon polymerization. The amino acid vesicles can be immobilized on Sephadex beads by reaction with carbodiimide. The impermeability, biodegradability, and ease of immobilization make this class of vesicles attractive materials for the encapsulation of reagents.     

Cryo-responses of two types of large unilamellar vesicles in the presence of non-permeable or permeable cryoprotecting agents

Cryo-responses of two types of large unilamellar vesicles (LUV) that were made from either egg yolk l-α-phosphatidylcholine (EPC) or 1,2-dipalmitoyl-rac-glycero-3-phosphocholine (DPPC), in the presence of non-permeable or permeable cryoprotective agents (CPA) was investigated. Partial ternary phase diagrams of CPA–salt–water with specific CPA to salt ratio (R), were constructed to estimate the phase volume of ice and unfrozen matrix of the LUV dispersion, which could aid in understanding the mechanistic actions of CPA. Leakage of both EPC and DPPC LUV was reduced if the sugar concentrations are above 10% (w/w) for disaccharides and 5% (w/w) for monosaccharides. Above these sugar concentrations, non-permeable CPA were more effective in preventing leakage of DPPC LUV than in EPC LUV. Below these sugar concentrations, EPC and DPPC LUV with limited mobility in the remaining unfrozen matrix were more likely to approach and interact with one and another, which were not anticipated when the LUV were completely embedded in the ice matrix. In the presence of Me₂SO or EG, EPC LUV that had been subjected to freezing and thawing processes were protected from leakage. At room temperature, Me₂SO and EG were detrimental to the DPPC LUV. This study suggests that the choice of CPA for cell cryopreservation depends on the type of phospholipids in plasma membranes, which vary in their acyl chain length and gel–liquid crystal phase transition temperature.     

Interrogating the role of liposome size in mediating the dynamics of a chromophore in the acyl chain region of a phospholipid bilayer

We have examined the temperature-dependent reorientation dynamics of perylene imbedded in bilayers of 1,2-dimyristoyl-sn-phosphatidylcholine (DMPC), where the bilayers exist in the form of unilamellar vesicles. Previous work using 100-nm diameter DMPC vesicles has shown that the phase transition from the gel phase to the fluid phase can be detected using the reorientation dynamics of perylene. In this work we explore the vesicle size dependence of the perylene reorientation dynamics in DMPC vesicles. The size of the vesicles is determined by extrusion and the reorientation dynamics of perylene are measured as a function of vesicle size between 100-nm and 5-microm diameter. We find that, while the phase transition for DMPC is seen in smaller vesicles, perylene becomes insensitive to the phase transition for vesicles larger than ca. 800-nm diameter. We also find a discontinuous change in perylene reorientation dynamics with increasing vesicle size, and we consider this result in the context of the location of perylene within the bilayer.     

Oxidation of cytochromes c and c2 by bacterial photosynthetic reaction centers in phospholipid vesicles. 1. Studies with neutral membranes

The oxidation of cytochrome c2 by photosynthetic reaction center isolated from Rhodopseudomonas sphaeroides and incorporated into unilamellar phosphatidylcholine vesicles was found to be kinetically similar to that observed earlier for reaction centers in low detergent solution [Overfield, R.E., Wraight, C.A., & DeVault, D. (1979) FEBS Lett. 105, 137-142]. At low ionic strength the kinetics were biphasic. The fast phase indicated the formation of a cytochrome-reaction center complex with an apparent binding constant, KB, of about 10(5) M-1. However, KB decreased dramatically with increasing salt concentration, and no fast oxidation was detectable in 0.1 M NaCl. The slow cytochrome oxidation was first order in both cytochrome and reaction centers and, thus, second order overall. Deviations from theoretical second-order behavior were observed when the rate of the first-order back reaction of the primary photoproducts was significant compared to the cytochrome oxidation. This can cause serious overestimation of the second-order rate constant. The slow oxidation of cytochrome c2 by reaction centers in phosphatidylcholine vesicles exhibited a 40% lower encounter frequency than with the solubilized reaction center. This was attributed to the much lower diffusion coefficient of the reaction center in the vesicle membrane than in solution. No effects of diminished dimensionality were detected with neutral vesicles. An activation energy of 8.0 +/- 0.4 kcal x mol-1 was determined for the slow phase of cytochrome c2 oxidation by reaction centers in solution and in vesicles of several different phosphatidylcholines, including dimyristoylphosphatidylcholine above and below its phase transition temperature. Thus, the physical state of the lipid did not appear to affect any rate-limiting steps leading to cytochrome oxidation. The ionic strength dependence of the slow kinetics of oxidation of cytochromes c and c2 confirmed the electrostatic nature of the cytochrome-reaction center interaction, and the pH dependence indicated the titration of a group or groups, important to this interaction, at pH 9.5.