Lysozyme effect on oleic acid/oleate vesicles

We have analysed by means of turbidimetric, dynamic light scattering (DLS), and fluorimetric techniques the effect of lysozyme on negatively charged oleic acid/oleate vesicles. The addition of lysozyme brings about a decrease in optical density of the vesicle population, which finally results in a size distribution of oleate vesicles shifted toward smaller mean diameters. On the contrary, (a) when phosphatidylserine vesicles were used, lysozyme induces an increase of turbidity and a shift toward larger vesicle sizes; and (b) the addition of histone H1 or poly-L-lysine produces an aggregative behavior both in oleate and in phosphatidylserine vesicles. Experiments carried out with calcein-containing vesicles indicate that the observed changes in the lysozyme/oleate system occur with partial leakage of the vesicle content. All this is taken to suggest that the interaction between lysozyme and oleate vesicles is of quite specific nature, and certainly not just due to electrostatic interactions.     

Lysozyme Effect on Oleic Acid/Oleate Vesicles

We have analysed by means of turbidimetric, dynamic light scattering (DLS), and fluorimetric techniques the effect of lysozyme on negatively charged oleic acid/oleate vesicles. The addition of lysozyme brings about a decrease in optical density of the vesicle population, which finally results in a size distribution of oleate vesicles shifted toward smaller mean diameters. On the contrary, (a) when phosphatidylserine vesicles were used, lysozyme induces an increase of turbidity and a shift toward larger vesicle sizes; and (b) the addition of histone H1 or poly-L-lysine produces an aggregative behavior both in oleate and in phosphatidylserine vesicles. Experiments carried out with calcein-containing vesicles indicate that the observed changes in the lysozyme/oleate system occur with partial leakage of the vesicle content. All this is taken to suggest that the interaction between lysozyme and oleate vesicles is of quite specific nature, and certainly not just due to electrostatic interactions.     

Cooperativity of the phase transition in single- and multibilayer lipid vesicles.

The effect of membrane morphology on the cooperativity of the ordered-fluid, lipid phase transition has been investigated by comparing the transition widths in extended, multibilayer dispersons of dimyristoyl phosphatidyl-choline, and also of dipalmitoyl phosphatidylcholine, with those in the small, single-bilayer vesicles obtained by sonication. The electron spin resonance spectra of three different spin-labelled probes, 2,2,6,6-tetramethylpiperdine-N-oxyl, phosphatidylcholine and stearic acid, and also 90 degrees light scattering and optical turbidity measurements were used as indicators of the phase transition. In all cases the transition was broader in the single-bilayer vesicles than in the multibilayer dispersions, corresponding to a decreased cooperativity on going to the small vesicles. Comparison of the light scattering properties of centrifuged and uncentrifuged, sonicated vesicles suggests that these are particularly sensitive to the presence of intermediate-size particles, and thus the spin label measurements are likely to give a more reliable measure of the degree of cooperativity of the small, single-bilayer vesicles. Application of the Zimm and Bragg theory ((1959) J. Chem. Phys. 31, 526-535) of cooperative transitions to the two-dimensional bilayer system shows that the size of the cooperative unit, 1/square root sigma, is a measure of the mean number of molecules per perimeter molecule, in a given region of ordered or fluid lipid at the centre of the transition. From this result it is found that it is the vesicle size which limits the cooperativity of the transition in the small, single-bilayer vesicles. The implications for the effect of membrane structure and morphology on the cooperativity of phase transitions in biological membranes, and for the possibility of achieving lateral communication in the plane of the membrane, are discussed.     

Optical characterization of liposomes by right angle light scattering and turbidity measurement

Liposomes have frequently been used as models of biomembranes or vehicles for drug delivery. However, the systematic characterization of lipid vesicles by right angle light scattering and turbidity has not been carried out despite the usefulness of such studies for size estimation. In this study, liposomes of various sizes were prepared by sonication and extrusion. The mean cumulant radii of the vesicles were determined by dynamic light scattering. The lamellarities were estimated based on fluorescence quenching of N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)dipalmitoyl-L-alpha-phosph ati dylethanolamine by sodium dithionite. Right angle light scattering intensity and optical density at 436 nm per unit lipid concentration were measured as a function of vesicle radius. With a vesicle radius < or =100 nm, the optical parameters could be well explained by the Rayleigh-Gans-Debye theory in which the liposomes were modeled as homogeneous spheres with mean refractive indices determined by the volume fractions of lipids in vesicles.     

Light scattering and turbidity measurements on lipid vesicles.

The dynamic behaviour of model membranes in the form of sonicated liposomes in excess water was studied by means of 90 degrees C light scattering and turbidity measurements. Computer calculations based on the Rayleigh-Gans theory of light scattering were used to estimate the average size of lipid vesicles dispersed in water, taking into account the various structures of the vesicles. Normal reversible changes in the scattered light intensity and turbidity with temperature could be accounted for mainly by the changes in the refractive index of the lipid and irreversible anomalous changes were explained on the basis of fusion of smaller aggregated vesicles.     

Light scattering and turbidity measurements on lipid vesicles

The dynamic behaviour of model membranes in the form of sonicated liposomes in excess water was studied by means of 90 °C light scattering and turbidity measurements. Computer calculations based on the Rayleigh-Gans theory of light scattering were used to estimate the average size of lipid vesicles dispersed in water, taking into account the various structures of the vesicles. Normal reversible changes in the scattered light intensity and turbidity with temperature could be accounted for mainly by the change in the refractive index of the lipid and irreversible anomalous changes were explained on the basis of fusion of smaller aggregated vesicles.     

Large vesicle contamination in small,unilamellar vesicles

Small, unilamellar phospholipid vesicles have been prepared using a new, high-powdered cup sonifier that avoids contact of the sample with a titanium probe. These vesicles have been characterized by gel filtration chromatography both before and after fractionation by high-speed centrifugation. Plots of the turbidity of centrifuged vesicles between 300 and 650 nm against the reciprocal fourth power of the scattering wavelength were linear with zero intercepts (extrapolated to infinite wavelength). In the presence of minute quantities of large, multilamellar vesicles, these plots remained linear but had intercepts quantitatively proportional to the amount of contaminating large vesicles. Since this measurement requires only a standard spectrophotometer and very small quantities of lipid, this method is suggested as a useful assay for determining contamination of small vesicle preparations by large vesicles. Two applications of this method as well as a practical limitation are discussed.     

Size distribution measurement of vesicles by atomic force microscopy

Vesicles have been utilized as nanoscale vehicles for reagents including potential drug delivery systems. When used to deliver drugs, vesicle size and the size distribution are important factors in the determination of the dosage, cell specificity, and rate of clearance from the body. Current size measurement techniques for vesicles are electron microscopy and dynamic light scattering, but their results are not equal. Therefore atomic force microscopy was attempted as another size measurement technique. After adsorption of the vesicles from a low-concentration solution of vesicles on mica substrate, each vesicle is generally found as a flattened structure. The diameters of vesicles in these solutions and their distribution have been successfully estimated from the surface area of the flattened structure of each vesicle. At higher concentrations, we have found a monolayer crammed with dome-shaped vesicles on the substrate. The diameters of vesicles in these solutions have also been successfully estimated from the surface area of the dome-shaped structure of each vesicle. Diameters of vesicles in solution estimated from two different vesicle concentrations are not close to those reported by electron microscope studies but are close to those reported by dynamic light scattering studies.     

Effects of divalent cations,temperature, osmotic pressure gradient,and vesicle curvature on phosphatidylserine vesicle fusion

Summary Fusion of phosphatidylserine vesicles induced by divalent cations, temperature and osmotic pressure gradients across the membrane was studied with respect to variations in vesicle size. Vesicle fusion was followed by two different methods: 1) the Tb/DPA fusion assay, whereby the fluorescent intensity upon mixing of the internal aqueous contents of fused lipid vesicles was monitored, and 2) measurement of the changes in turbidity of the vesicle suspension due to vesicle fusion. It was found that the threshold concentration of divalent cations necessary to induce vesicle fusion depended on the size of vesicles; as the diameter of the vesicle increased, the threshold value increased and the extent of fusion became less. For the osmotic pressure-induced vesicle fusion, the larger the diameter of vesicles, the smaller was the osmotic pressure gradient required to induce membrane fusion. Divalent cations, temperature increase and vesicle membrane expansion by osmotic pressure gradient all resulted in increase in surface energy (tension) of the membrane. The degree of membrane fusion correlated with the corresponding surface energy changes of vesicle membranes due to the above fusion-inducing agents. The increase in surface energy of 9.5 dyn/cm from the reference state corresponded to the threshold point of phosphatidylserine membrane fusion. An attempt was made to explain the factors influencing fusion phenomena on the basis of a single unifying theory.     

Aggregation and hemi-fusion of anionic vesicles induced by the antimicrobial peptide cryptdin-4

We show that cryptdin-4 (Crp4), an antimicrobial peptide found in mice, induces the aggregation and hemi-fusion of charged phospholipid vesicles constructed of the anionic lipid POPG and the zwitterionic lipid POPC. Hemi-fusion is confirmed with positive total lipid-mixing assay results, negative inner monolayer lipid-mixing assay results, and negative results from contents-mixing assays. Aggregation, as quantified by absorbance and dynamic light scattering, is self-limiting, creating finite-sized vesicle assemblies. The rate limiting step in the formation process is the mixing of juxtaposed membrane leaflets, which is regulated by bound peptide concentration as well as vesicle radius (with larger vesicles less prone to hemi-fusion). Bound peptide concentration is readily controlled by total peptide concentration and the fraction of anionic lipid in the vesicles. As little as 1% PEGylated lipid significantly reduces aggregate size by providing a steric barrier for membrane apposition. Finally, as stable hemi-fusion is a rare occurrence, we compare properties of Crp4 to those of many peptides known to induce complete fusion and lend insight into conditions necessary for this unusual type of membrane merger.     

Aggregation and hemi-fusion of anionic vesicles induced by the antimicrobial peptide cryptdin-4

We show that cryptdin-4 (Crp4), an antimicrobial peptide found in mice, induces the aggregation and hemi-fusion of charged phospholipid vesicles constructed of the anionic lipid POPG and the zwitterionic lipid POPC. Hemi-fusion is confirmed with positive total lipid-mixing assay results, negative inner monolayer lipid-mixing assay results, and negative results from contents-mixing assays. Aggregation, as quantified by absorbance and dynamic light scattering, is self-limiting, creating finite-sized vesicle assemblies. The rate limiting step in the formation process is the mixing of juxtaposed membrane leaflets, which is regulated by bound peptide concentration as well as vesicle radius (with larger vesicles less prone to hemi-fusion). Bound peptide concentration is readily controlled by total peptide concentration and the fraction of anionic lipid in the vesicles. As little as 1% PEGylated lipid significantly reduces aggregate size by providing a steric barrier for membrane apposition. Finally, as stable hemi-fusion is a rare occurrence, we compare properties of Crp4 to those of many peptides known to induce complete fusion and lend insight into conditions necessary for this unusual type of membrane merger.     

Turbidity changes of lipid vesicles near the phase transition temperature as an indication of fusion

Sonicated liposomes of dipalmitoyl phosphatidylcholine show sharp turbidity changes on heating at two distinct temperatures. A decrease in turbidity at the lower temperature (approx. 37°C) is thought to be associated with the phase transition of small vesicles and a decrease at about 44°C with larger vesicles or multilayer. An increase of turbidity between 38 and 43°C is attributed to the fusion of small vesicles. The turbidity changes were studied under various modes of vesicle preparation to confirm the interpretation of the turbidity data. Alternate interpretations are discussed.     

Kinetics of the micelle-to-vesicle transition: aqueous lecithin-bile salt mixtures

Important routes to lipid vesicles (liposomes) are detergent removal techniques, such as dialysis or dilution. Although they are widely applied, there has been only limited understanding about the structural evolution during the formation of vesicles and the parameters that determine their properties. We use time-resolved static and dynamic light scattering to study vesicle formation in aqueous lecithin-bile salt mixtures. The kinetic rates and vesicle sizes are found to strongly depend on total amphiphile concentration and, even more pronounced, on ionic strength. The observed trends contradict equilibrium calculations, but are in agreement with a kinetic model that we present. This model identifies the key kinetic steps during vesicle formation: rapid formation of disk-like intermediate micelles, growth of these metastable micelles, and their closure to form vesicles once line tension dominates bending energy. A comparison of the rates of growth and closure provides a kinetic criterion for the critical size at which disks close and thus for the vesicle size. The model suggests that liposomes are nonequilibrium, kinetically trapped structures of very long lifetime. Their properties are hence controlled by kinetics rather than thermodynamics.     

Light scattering study of phosphatidylcholine vesicles at the pretransition

Laser light scattering has been used to investigate the thermal pretransition of dipalmitoylglycerophosphocholine vesicles with variable radius as obtained by the mild sonication method. Intensity changes in 90° scattered light are observed at the pretransition for larger vesicles and actually increase with increasing vesicle size, reaching a constant value.This constant value is in good agreement with the value calculated from the refractive index data.The intensity ratio of scattered light at temperatures of 30°C and 40°C (I₄₀/I₃₀) approaches unity at a radius of small single-bilayer vesicle. This result is interpreted as no pretransition for small vesicles in agreement with the calorimetric results. An expression of the particle scattering factor is also presented for multilayered shells composed of anisotropic elements. It is shown numerically, using this expression, that changes in the lipid layer thickness and the tilting angles at the pretransition have no effects on the scattering factor. Therefore it is concluded that the intensity changes in scattered light reflect the changes in the refractive index of the vesicle originating in the polar head groups.     

Complex carbohydrate-lectin interaction at the interface: a model for cellular adhesion. I. Effect of vesicle size on the kinetics of aggregation between a fatty acid conjugate of lectin and a liposomal asialoganglioside

Two types of phospholipid vesicles capable of mutual recognition have been tailor-made to serve as a model system for the study of carbohydrate-mediated cellular adhesion. One of the vesicles contained a fatty acid conjugate of a galactose specific lectin (lectin vesicle) and the other an asialoganglioside with a reactive terminal galactose residue (galactose vesicle). The kinetics of aggregation of these two types of vesicles was followed by monitoring time-dependent change in turbidity. A 10-100-fold enhancement in the forward rate constant (kf ranging from 7.1 x 10(5) to 4.5 x 10(7) M-1.s-1 at 27 degrees C) was observed when compared with that for the lectin-galactose system in solution (kf being 4.5 x 10(5) M-1.s-1), reported in the literature. A study of the influence of vesicle size on the rate of aggregation showed that enhancement depended on the curvature of the galactose vesicle rather than the density of asialoganglioside suggesting a possible diffusion in the plane of the membrane. The ratio, kf/kd is found to be approx. 10(10) M-1 indicating that the formation of multiple bonds plays a role for stable adhesion.     

Phospholipid exchange between bilayer membrane vesicles.

The turbidity of lipid vesicles, freshly prepared by sonicating purified dimyristoyllecithin (DML) in dilute KCl solutions, was measured as a function of time at various temperatures. A sharp maximum in the rate of increase of turbidity is found just above the crystal:liquid-crystal phase transition temperature (Tm). The initial rate of turbidity increase is first order with respect to DML concentration. Electron and light microscopy reveal large vesicles which are not present before incubation or after incubation at temperatures far from the Tm. When temperature, rather than time, is the independent variable, a sharp drop in turbidity is seen at the Tm. The magnitude of this drop and the temperature at which it occurs were used to measure the rate of lipid transfer between vesicles composed of different lipids. A mixture of DML vesicles and dipalmitoyllecithin (DPL) vesicles exhibits sharp drops in turbidity at 24 and 41 degrees, the corresponding Tm's. With time, the magnitude of the transition at 24 degrees decreases while that which was originally at 41 degrees moves to lower temperatures and increases in magnitude. At equilibrium there is a single transition at 32.5 degrees characteristic of vesicles composed of equimolar DPL and DML. The rate at which equilibrium is approached increases at around 24 degrees and again around 41 degrees. These observations indicate that vesicles are in equilibrium with monomolecular lipid, the concentration of the latter being higher the shorter the lipid acyl group or the smaller the vesicle. DML molecules are therefore lost from small vesicles to large vesicles (DML system) or lost from DML vesicles to DML-DPL vesicles (mixed system). When DML vesicles containing a few percent brain gangliosides were studied, different behavior was observed; the initial rate of increase of turbidity becomes second order in lipid concentration, and the rate constant increases with increasing concentrations of KCl. The kinetic order, coupled with the fact that electrolyte reduces intervesicle electrostatic repulsion, argues that in this situation the mechanism of vesicle growth requires vesicle collision.     

Interaction of Cryptococcus neoformans Extracellular Vesicles with the Cell Wall

Cryptococcus neoformans produces extracellular vesicles containing a variety of cargo, including virulence factors. To become extracellular, these vesicles not only must be released from the plasma membrane but also must pass through the dense matrix of the cell wall. The greatest unknown in the area of fungal vesicles is the mechanism by which these vesicles are released to the extracellular space given the presence of the fungal cell wall. Here we used electron microscopy techniques to image the interactions of vesicles with the cell wall. Our goal was to define the ultrastructural morphology of the process to gain insights into the mechanisms involved. We describe single and multiple vesicle-leaving events, which we hypothesized were due to plasma membrane and multivesicular body vesicle origins, respectively. We further utilized melanized cells to “trap” vesicles and visualize those passing through the cell wall. Vesicle size differed depending on whether vesicles left the cytoplasm in single versus multiple release events. Furthermore, we analyzed different vesicle populations for vesicle dimensions and protein composition. Proteomic analysis tripled the number of proteins known to be associated with vesicles. Despite separation of vesicles into batches differing in size, we did not identify major differences in protein composition. In summary, our results indicate that vesicles are generated by more than one mechanism, that vesicles exit the cell by traversing the cell wall, and that vesicle populations exist as a continuum with regard to size and protein composition.     

Osmotically induced shape changes of large unilamellar vesicles measured by dynamic light scattering

Static and dynamic light scattering measurements have been used to characterize the size, size distribution, and shape of extruded vesicles under isotonic conditions. Dynamic light scattering was then used to characterize osmotically induced shape changes by monitoring changes in the hydrodynamic radius (R(h)) of large unilamellar vesicles (LUVs). These changes are compared to those predicted for several shapes that appear in trajectories through the phase diagram of the area difference elasticity (ADE) model (. Phys. Rev. E. 52:6623-6634). Measurements were performed on dioleoylphosphatidylcholine (DOPC) vesicles using two membrane-impermeant osmolytes (NaCl and sucrose) and a membrane-permeant osmolyte (urea). For all conditions, we were able to produce low-polydispersity, nearly spherical vesicles, which are essential for resolving well-defined volume changes and consequent shape changes. Hyper-osmotic dilutions of DOPC vesicles in urea produced no change in R(h), whereas similar dilutions in NaCl or sucrose caused reductions in vesicle volume resulting in observable changes to R(h). Under conditions similar to those of this study, the ADE model predicts an evolution from spherical to prolate then oblate shapes on increasing volume reduction of LUVs. However, we found that DOPC vesicles became oblate at all applied volume reductions.     

Cooperativity of the phase transition in single- and multibilayer lipid vesicles

The effect of membrane morphology on the cooperativity of the ordered-fluid, lipid phase transition has been investigated by comparing the transition widths in extended, multibilayer dispersions of dimyristoyl phosphatidylcholine, and also of dipalmitoyl phosphatidylcholine, with those in the small, single-bilayer vesicles obtained by sonication. The electron spin resonance spectra of three different spin-labelled probes, $\text{2,2,6,6-}\text{tetramethylpiperdine}\text{-N-}\text{oxyl}$, phosphatidylcholine and stearic acid, and also 90° light scattering and optical turbidity measurements were used as indicators of the phase transition. In all cases the transition was broader in the single-bilayer vesicles than in the multibilayer dispersions, corresponding to a decreased cooperativity on going to the small vesicles. Comparison of the light scattering properties of centrifuged and uncentrifuged, sonicated vesicles suggests that these are particularly sensitive to the presence of intermediate-size particles, and thus the spin label measurements are likely to give a more reliable measure of the degree of cooperativity of the small, single-bilayer vesicles. Application of the Zimm and Bragg theory ((1959) J. Chem. Phys. 31, 526–535) of cooperative transitions to the two-dimensional bilayer system shows that the size of the cooperative unit, 1/?σ, is a measure of the mean number of molecules, per perimeter molecule, in a given region of ordered or fluid lipid at the centre of the transition. From this result it is found that it is the vesicle size which limits the cooperativity of the transition in the small, single-bilayer vesicles. The implications for the effect of membrane structure and morphology on the cooperativity of phase transitions in biological membranes, and for the possibility of achieving lateral communication in the plane of the membrane, are discussed.     

Aggregation of ligand-modified liposomes by specific interactions with proteins. I: Biotinylated liposomes and avidin

The aggregation of biotin-modified phospholipid vesicles (liposomes) induced by binding the protein avidin in solution is analyzed experimentally and theoretically. Avidin has four binding sites that can recognize biotin specifically, and is able to cross-link the liposomes to form large aggregates. The aggregation kinetics were followed using quasi-elastic light scattering (QLS) to measure the mean particle size, and by measuring the solution turbidity. The rate and extent of aggregation were determined as a function of vesicle concentration, protein concentration, and the biotin density on the surface of the liposomes. A model based on Smoluchowski kinetics, fractal concepts, and Rayleigh and Mie light scattering theory was developed to analyze the experimental observations. Small aggregates (<7800 A diameter) may be treated as globular; however, the fractal nature of larger particles must be taken into account. Parameters in the model are taken from molecular simulations, or fit to the experimental observations. The aggregation kinetics are primarily determined by the biotin density on the liposome surface, the stoichiometric ratio of avidin molecules to liposomes, and the liposome concentration. Good agreement is found between the model and the experimental results. (c) 1996 John Wiley & Sons, Inc.