Exchange and interactions between lipid layers at the surface of a liposome solution.

Lipid organization and lipid transport processes occurring at the air-water interface of a liposome (lipid vesicle) solution are studied by conventional surface pressure-area measurements and interpreted by an adequate theory. At the interface of a dioleoyl phosphatidylcholine vesicle solution, used for demonstration, a well defined two layer structure selfassembles: vesicles disintegrate at the interface forming a surface-adsorbed lipid monolayer, which prevents further disintegration beyond about 1 dyne/cm surface pressure. A layer of vesicles now assembles in close association with the monolayer. This layer is in vesicle diffusion exchange with the solution and in lipid exchange with the monolayer. The lipid exchange occurs exclusively between the monolayer and the outer lipid layer of the vesicles; it is absent between outer and inner vesicle layers. Equilibration of the lipid density in the monolayer with that in the vesicle outer layer provides a coherent and quantitative explanation of the observed hysteresis effects and equilibrium states. The correspondence between monolayer and vesicle outer layer is traced down to equilibrium constants and rate constants and their dependences on surface pressure, vesicle size and concentration. Other alternate realizations of surface structure and exchange, including induced lipid flip-flop within vesicles or vesicle monolayer adhesion or fusion are potential applications of the proposed analysis.     

Asymmetric exchange of vesicle phospholipids catalyzed by the phosphatidylcholine exhange protein. Measurement of inside--outside transitions.

Purified phosphatidylcholine exchange protein was used to exchange phosphatidylcholine between homogeneous single-walled phosphatidylcholine vesicles and human erythrocyte ghosts. When excess ghosts were present, it was found that only 70% of the vesicle phosphatidylcholine was available for exchange. This fraction corresponds closely to the amount of phosphatidycholine in the outer monolayer of these vesicles, indicating that only the outer surface of the vesicle is accessible to the exchange protein. Also, it was found that all phosphatidylcholine introduced into vesicles by the exchange protein was available for subsequent exchange. Using the exchange protein, asymmetrical vesicles were prepared in which the outer monolayer was either enriched or depleted in radioactive phosphatidylcholine as compared to the inner monolayer. Re-equilibration of the radioactivity between the two surfaces of the vesicle (flip-flop) could not be detected, even after 5 days at 37degrees. It is estimated that the half-time for flip-flop is in excess of 11 days at 37degrees. These results indicate that the properties of the exchange protein can be expolited to measure phosphatidylcholine flip-flop rates and possible phosphatidylcholine asymmetry in biological and model membranes, without altering the structure of the membrane.     

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.     

Kinetics of phospholipid insertion into monolayers containing the lung surfactant proteins SP-B or SP-C

The lung surfactant proteins SP-B and SP-C are pivotal for fast and reversible lipid insertion at the air/liquid interface, a prerequisite for functional lung activity. We used a model system consisting of a preformed monolayer at the air/liquid interface supplemented with surfactant protein SP-B or SP-C and unilamellar vesicles injected into the subphase of a film balance. The content of SP-B or SP-C was similar to that found in lung lavage. In order to elucidate distinct steps of lipid insertion, we measured the time-dependent pressure increase as a function of the initial surface pressure, the temperature and the phosphatidylglycerol content by means of surface tension measurements and scanning force microscopy (SFM). The results of the film balance study are indicative of a two-step mechanism in which initial adsorption of vesicles to the protein-containing monolayer is followed by rupture and integration of lipid material. Furthermore, we found that vesicle adsorption on a preformed monolayer supplemented with SP-B or SP-C is strongly enhanced by negatively charged lipids as provided by DPPG and the presence of Ca2+ ions in the subphase. Hence, long-range electrostatic interactions are thought to play an important role in attracting vesicles to the surface, being the initial step in replenishment of lipid material. While insertion into the monolayer is independent of the type of protein SP-B or SP-C, initial adsorption is faster in the presence of SP-B than SP-C. We propose that the preferential interaction between SP-B and negatively charged DPPG leads to accumulation of negative charges in particular regions, causing strong adhesion between DPPG-containing vesicles and the monolayer mediated by Ca2+ ions, which eventually causes flattening and rupture of attached liposomes as observed by in situ SFM.     

Exchange of phosphatidylcholine between small unilamellar liposomes and human plasma high-density lipoprotein involves exclusively the phospholipid in the outer monolayer of the liposomal membrane

By making use of the capacity of phospholipase A₂ to degrade selectively the phospholipid in the outer half of the lipid bilayer of small unilamellar phospholipid/cholesterol vesicles without affecting the retention of a vesicle-encapsulated solute, we demonstrated that the exchange of phosphatidylcholine between such vesicles and human high density lipoprotein involves exclusively the phosphatidylcholine present in the outer monolayer of the vesicle membrane.     

Lipid exchange between membranes.

The exchange of lipid molecules between vesicle bilayers in water and a monolayer forming at the water surface was investigated theoretically within the framework of thermodynamics. The total number of exchanged molecules was found to depend on the bilayer curvature as expressed by the vesicle radius and on the boundary condition for exchange, i.e., whether during exchange the radius or the packing density of the vesicles remains constant. The boundary condition is determined by the rate of flip-flop within the bilayer relative to the rate of exchange between bi- and monolayer. If flip-flop is fast, exchange is independent of the vesicle radius; if flip-flop is slow, exchange increases with the vesicle radius. Available experimental results agree with the detailed form of this dependence. When the theory was extended to exchange between two bilayers of different curvature, the direction of exchange was also determined by the curvatures and the boundary conditions for exchange. Due to the dependence of the boundary conditions on flip-flop and, consequently, on membrane fluidity, exchange between membranes may partially be regulated by membrane fluidity.     

Use of the fluorescent weak acid dansylglycine to measure transmembrane proton concentration gradients

The amphiphilic fluorescent dye N-[(5-dimethylamino)naphth-1-ylsulfonyl]glycine (dansylglycine) can be used to monitor the magnitude and stability of transmembrane proton gradients. Although freely soluble in aqueous media, the dye readily adsorbs to the surfaces of lipid vesicles. Because membrane-bound dye fluoresces at a higher frequency, and with greater efficiency, than dye in aqueous solution, it is easy to isolate the fluorescence emission from those dye molecules adsorbed to the lipid surface. When dansylglycine is mixed with phospholipid vesicles, the dye molecules attain a partition equilibrium between buffer and the outer, proximal surface of the vesicles. This is a rapid, diffusion-limited process that is indicated by a fast phase of fluorescence intensity increase monitored at 510 nm. In a second step, the inner, distal surface of each vesicle becomes populated with dye, a process that involves permeation through the lipid bilayer and that is generally much slower than the original adsorption step. Dansylglycine is a weak acid that permeates as an electrically neutral species; the flux of dye across the bilayer is thus strongly dependent on the degree of protonation of the dye's carboxylate moiety. When the external pH is lower than that of the vesicle lumen, the inward flux of dye is greater than that in the opposite direction, and dye accumulates in the lumen. This leads to a local elevation of dansylglycine concentration in the inner membrane monolayer, which in turn results in an elevated fluorescence intensity proportional to the membrane pH gradient.     

Characterization of lipid insertion into monomolecular layers mediated by lung surfactant proteins SP-B and SP-C

Pulmonary surfactant proteins, SP-B and SP-C, if present in preformed monolayers can induce lipid insertion from lipid vesicles into the monolayer after the addition of (divalent) cations [Oosterlaken-Dijksterhuis, M. A., Haagsman, H. P., van Golde, L. M. G., & Demel, R. A. (1991) Biochemistry 30, 8276-8287]. This model system was used to study the mechanisms by which SP-B and SP-C induce monolayer formation from vesicles. Lipid insertion proceeds irrespectively of the molecular class, and PG is not required for this process. In addition to lipids that are immediately inserted from vesicles into the monolayer, large amounts of vesicles are bound to the monolayer and their lipids eventually inserted when the surface area is expanded. SP-B and SP-C are directly responsible for the binding of vesicles to the monolayer. By weight, the vesicle binding capacity of SP-B is approximately 4 times that of SP-C. For vesicle binding and insertion, the formation of close contacts between monolayer and vesicles is essential. SP-B and SP-C show very similar surface properties. Both proteins form extremely stable monolayers (collapse pressures 36-37 mN/m) of alpha-helical structures oriented parallel to the interface. In monolayers consisting of DPPC and SP-B or SP-C, an increase in mean molecular area is observed, which is mainly attributed to the phospholipid. This will greatly enhance the insertion of new lipid material into the monolayer. The results of this study suggest that the surface properties and the hydrophobic nature of SP-B and SP-C are important for the protein-mediated monolayer formation.     

Novel inner monolayer fusion assays reveal differential monolayer mixing associated with cation-dependent membrane fusion

The ability to specifically monitor the behavior of the inner monolayer lipids of membranous vesicles during the membrane fusion process is useful technically and experimentally. In this study, we have identified N-NBD-phosphatidylserine as a reducible probe particularly suitable for inner monolayer fusion assays because of its low rate of membrane translocation after reduction of the outer monolayer probes by dithionite. Data are presented on translocation as a function of temperature, vesicle size, membrane composition, and serum protein concentration. Translocation as a result of the fusion event itself was also characterized. We further show here that a second membrane-localized probe, a long wavelength carbocyanine dye referred to a diI(5)C18ds, appears to form a membrane-bound resonance energy transfer pair with N-NBD-PS, and its outer monolayer fluorescence can also be eliminated by dithionite treatment. Lipid dilution of these probes upon fusion with unlabeled membranes leads to an increase in NBD donor fluorescence, and hence is a new type of inner monolayer fusion assay. These inner monolayer probe mixing assays were compared to random lipid labeling and aqueous contents mixing assays for cation-dependent fusion of liposomes composed of phosphatidylserine and phosphatidylethanolamine. The results showed that the inner monolayer fusion assay eliminates certain artifacts and reflects fairly closely the rate of non-leaky mixing of aqueous contents due to fusion, while outer monolayer mixing always precedes mixing of aqueous contents. In fact, vesicle aggregation and outer monolayer lipid mixing were found to occur over very long periods of time without inner monolayer mixing at low cation concentrations. Externally added lysophosphatidylcholine inhibited vesicle aggregation, outer monolayer mixing and any subsequent fusion. The state of vesicle aggregation and outer monolayer exchange that occurs below the fusion threshold may represent a metastable intermediate state that may be useful for further studies of the mechanism of membrane fusion.     

Structure of planar membrane formed from liposomes

Lipid vesicles with incorporated ion channels from polyene antibiotic amphotericin B were used to investigate structures of planar membranes formed by Shindler's techniques. A planar membrane assembled on the aperture in a lavsan film from two layers generated at the air-aqueous liposome suspension interface is not a simple bilayer but a bimolecular membrane containing numerous partly fused liposomes. A complete fusion of liposomal membranes with the planar bilayer is an unlikely event during membrane formation. A planar bimolecular lipid membrane without incorporated liposomes can be made by a method consisting of three stages: formation of a lipid layer on the air-water interface of a suspension containing liposomes, transfer of this layer along the surface of the solution into a chamber containing a solution without liposomes where a lipid monomolecular layer forms gradually (within about 20 min) at the air-water interface, assembling of the planar bilayer membrane from this monolayer. The knowledge of the planar membrane structure may be useful in experiments on incorporation of membrane proteins into a planar lipid bilayer.     

GsMTx4: Mechanism of Inhibiting Mechanosensitive Ion Channels

GsMTx4 is a spider venom peptide that inhibits cationic mechanosensitive channels (MSCs). It has six lysine residues that have been proposed to affect membrane binding. We synthesized six analogs with single lysine-to-glutamate substitutions and tested them against Piezo1 channels in outside-out patches and independently measured lipid binding. Four analogs had ～20% lower efficacy than the wild-type (WT) peptide. The equilibrium constants calculated from the rates of inhibition and washout did not correlate with the changes in inhibition. The lipid association strength of the WT GsMTx4 and the analogs was determined by tryptophan autofluorescence quenching and isothermal calorimetry with membrane vesicles and showed no significant differences in binding energy. Tryptophan fluorescence-quenching assays showed that both WT and analog peptides bound superficially near the lipid-water interface, although analogs penetrated deeper. Peptide-lipid association, as a function of lipid surface pressure, was investigated in Langmuir monolayers. The peptides occupied a large fraction of the expanded monolayer area, but that fraction was reduced by peptide expulsion as the pressure approached the monolayer-bilayer equivalence pressure. Analogs with compromised efficacy had pressure-area isotherms with steeper slopes in this region, suggesting tighter peptide association. The pressure-dependent redistribution of peptide between “deep” and “shallow” binding modes was supported by molecular dynamics (MD) simulations of the peptide-monolayer system under different area constraints. These data suggest a model placing GsMTx4 at the membrane surface, where it is stabilized by the lysines, and occupying a small fraction of the surface area in unstressed membranes. When applied tension reduces lateral pressure in the lipids, the peptides penetrate deeper acting as “area reservoirs” leading to partial relaxation of the outer monolayer, thereby reducing the effective magnitude of stimulus acting on the MSC gate.     

Spreading of liposomes at the air/water interface

Two types of film structure are formed when liposomes are spread at the air/water interface. At zero surface pressure, there is a slow transformation of the closed bilayered structure into a lipid monolayer. The internal content of the liposomes is released into the aqueous subphase. In contrast, when multilamellar liposomes are spread against a surface pressure, they retain their internal content at the air/water interface by forming multilayered structures. Among the liposomes which dipped through the interface an important fraction loses its internal content. During the spreading process at zero surface pressure, it seems that the outer layer of the liposome spreads with a better yield as compared with the inner layer. It is possible to use this spreading technique to determine the asymmetrical distribution of lipids across bilayers.     

Interaction of lipid vesicles with monomolecular layers containing lung surfactant proteins SP-B or SP-C

Pulmonary surfactant contains two families of hydrophobic proteins, SP-B and SP-C. Both proteins are thought to promote the formation of the phospholipid monolayer at the air-fluid interface of the lung. The Wilhelmy plate method was used to study the involvement of SP-B and SP-C in the formation of phospholipid monolayers. The proteins were either present in the phospholipid vesicles which were injected into the subphase or included in a preformed phospholipid monolayer. In agreement with earlier investigators, we found that SP-B and SP-C, present in phospholipid vesicles, were able to induce the formation of a monolayer, as became apparent by an increase in surface pressure. However, when the proteins were present in a preformed phospholipid monolayer (20 mN/m) at similar lipid to protein ratios, the rate of surface pressure increase after injection of pure phospholipid vesicles into the subphase at similar vesicle concentrations was 10 times higher. The process of phospholipid insertion from phospholipid vesicles into the protein-containing monolayers was dependent on (1) the presence of (divalent) cations, (2) the phospholipid concentration in the subphase, (3) the size of the phospholipid vesicles, (4) the protein concentration in the preformed monolayer, and (5) the initial surface pressure at which the monolayers were formed. Both in vesicles and in preformed monolayers, SP-C was less active than SP-B in promoting the formation of a phospholipid monolayer. The use of preformed monolayers containing controlled protein concentrations may allow more detailed studies on the mechanism by which the proteins enhance phospholipid monolayer formation from vesicles.     

In vitro interaction of zajdela ascites hepatoma cells with lipid vesicles

We studied the in vitro interaction between Zajdela ascites hepatoma cells and small unilamellar vesicles, consisting of ¹⁴C-labeled phosphatidylcholine, cholesterol, and phosphatidylserine (molar ratio 5: 4: 1), containing high intravesicular concentrations of carboxyfluorescein or fluorescein isothiocyanate tagged dextran.The entrapped markers were found to be associated with the cells to a lesser degree than the vesicle membrane marker. This discrepancy, which is slightly less pronounced for fluorescein isothiocyanate tagged dextran than for carboxyfluorescein, increases with incubation time and decreases with increasing vesicle lipid concentration in the incubation mixture. Vesicle-plasma membrane exchange of the vesicle lipid marker could not entirely explain the observed discrepancy. It is tentatively concluded that the gap mainly arises from a selective loss of entrapped dyes from vesicles actually interacting with the cell surface. Both spectrofluorimetric and fluorescence microscopic observations, as well as the relative insensitivity of vesicle uptake towards the presence of metabolic inhibitors, exclude a major contribution of endocytosis as a vesicle uptake route. We therefore conclude that vesicles are primarily internalized by a vesicle-cell fusion-like process. The observed discrepancy in uptake between entrapped materials and vesicle lipid is discussed in terms of a two-site vesicle cell surface interaction model.     

The interaction of liposomes containing intrinsic erythrocyte membrane proteins with lipid monolayers at air/water and oil/water interfaces

The main intrinsic membrane proteins of the human erythrocyte membrane, glycophorin and the anion transporter, were isolated by extraction with Triton X-100 and ion-exchange chromatography. After removal of detergent the extract consisted of proteolipid vesicles with a lipid:protein molar ratio in the range 50-60 and a diameter of the order of 200 nm. The interaction between these vesicles and dipalmitoylphosphatidylcholine (DPPC), cholesterol and cholesterol:DPPC (2:1 molar ratio) monolayers at air/water and n-decane/water interfaces has been studied. The vesicles interact with the monolayers, rapidly causing large increases in surface pressure. Limiting values of surface pressure, 39.4-43 mN . m-1 at air/water and 31.5-33.4 mN . m-1 at the n-decane/water interface, were reached at protein levels above 1 microgram . ml-1. At the air/water interface, and probably at the n-decane/water, surface pressure increases were limited by monolayer collapse. Compression isotherms and surface potential measurements indicated that material from the proteolipid vesicles entered the monolayer phase. In contrast to proteolipid vesicles, injection of protein-free liposomes beneath the monolayer resulted in smaller, slower increases in surface pressure. Thus, the presence of intrinsic membrane proteins in vesicles greatly facilitated the transfer of material into the lipid monolayer.     

Surface-active properties of the antitumour ether lipid 1-O-octadecyl-2-O-methyl-rac-glycero-3-phosphocholine (edelfosine)

The surface activity and interaction with lipid monolayers and bilayers of the antitumour ether lipid 1-O-octadecyl-2-O-methyl-rac-glycero-3-phosphocholine (edelfosine) have been studied. Edelfosine is a surface-active soluble amphiphile, with critical micellar concentrations at 3.5 μM and 19 μM in water. When the air-water interface is occupied by a phospholipid, edelfosine becomes inserted in the phospholipid monolayer, increasing surface pressure. This increase is dose-dependent, and reaches a plateau at ca. 2 μM edelfosine bulk concentration. The ether lipid can become inserted in phospholipid monolayers with initial surface pressures of up to 33 mN/m, which ensures its capacity to become inserted into cell membranes. Upon interaction with phospholipid vesicles, edelfosine exhibits a weak detergent activity, causing release of vesicle contents to a low extent (< 5%), and a small proportion of lipid solubilization. The weak detergent properties of edelfosine can be related to its very low critical micellar concentrations. Its high affinity for lipid monolayers combined with low lytic properties support the use of edelfosine as a clinical drug. The surface-active properties of edelfosine are similar to those of other “single-chain” lipids, e.g. lysophosphatidylcholine, palmitoylcarnitine, or N-acetylsphingosine.     

Secondary structure of spiralin in solution, at the air/water interface, and in interaction with lipid monolayers

The surface of spiroplasmas, helically shaped pathogenic bacteria related to the mycoplasmas, is crowded with the membrane-anchored lipoprotein spiralin whose structure and function are unknown. In this work, the secondary structure of spiralin under the form of detergent-free micelles (average Stokes radius, 87.5 A) in water and at the air/water interface, alone or in interaction with lipid monolayers was analyzed. FT-IR and circular dichroism (CD) spectroscopic data indicate that spiralin in solution contains about 25+/-3% of helices and 38+/-2% of beta sheets. These measurements are consistent with a consensus predictive analysis of the protein sequence suggesting about 28% of helices, 32% of beta sheets and 40% of irregular structure. Brewster angle microscopy (BAM) revealed that, in water, the micelles slowly disaggregate to form a stable and homogeneous layer at the air/water interface, exhibiting a surface pressure up to 10 mN/m. Polarization modulation infrared reflection absorption spectroscopy (PMIRRAS) spectra of interfacial spiralin display a complex amide I band characteristic of a mixture of beta sheets and alpha helices, and an intense amide II band. Spectral simulations indicate a flat orientation for the beta sheets and a vertical orientation for the alpha helices with respect to the interface. The combination of tensiometric and PMIRRAS measurements show that, when spiroplasma lipids are used to form a monolayer at the air/water interface, spiralin is adsorbed under this monolayer and its antiparallel beta sheets are mainly parallel to the polar-head layer of the lipids without deep perturbation of the fatty acid chains organization. Based upon these results, we propose a 'carpet model' for spiralin organization at the spiroplasma cell surface. In this model, spiralin molecules anchored into the outer leaflet of the lipid bilayer by their N-terminal lipid moiety are composed of two colinear domains (instead of a single globular domain) situated at the lipid/water interface. Owing to the very high amount of spiralin in the membrane, such carpets would cover most if not all the lipids present in the outer leaflet of the bilayer.     

Transmembrane movement and distribution of cholesterol in the membrane of vesicular stomatitis virus.

The transmembrane movement and distribution of cholesterol in the vesicular stomatitis virus membrane were studied by following the depletion of cholesterol from virions to interacting phospholipid vesicles and by exchange of radiolabeled cholesterol between virions and phospholipid-cholesterol vesicles. The kinetics of the cholesterol exchange or depletion reactions revealed the presence of two exponential rates: a rapid rate, dependent on the vesicle to virus ratio, and a slower rate, independent of the vesicle to virus ratio. The kinetics of cholesterol movement could be best interpreted by a model of the virion membrane considered as a two pool system in which approximately 30% of the cholesterol resides in the outer monolayer and approximately 70% in the inner monolayer. The half-time for equilibration of the two pools was calculated to be 4--6 h and was assumed to represent the time required for transmembrane movement of cholesterol across the bilayer. The initial rate of transfer of cholesterol from virus into vesicles increased when vesicle phospholipids contained more unsaturated and shorter chain fatty acids. Furthermore, the transfer of cholesterol appeared to occur by a collisional mechanism requiring membrane-membrane contact. Interaction with lipid vesicles did not significantly affect the integrity of the virion membrane as assessed by the relative inaccessibility of internal proteins to lactoperoxidase-catalyzed iodination and by the small loss of [3H]amino acid labeled protein from the virus.     

Biomembrane Fabrication by the Solvent-assisted Lipid Bilayer (SALB) Method

In order to mimic cell membranes, the supported lipid bilayer (SLB) is an attractive platform which enables in vitro investigation of membrane-related processes while conferring biocompatibility and biofunctionality to solid substrates. The spontaneous adsorption and rupture of phospholipid vesicles is the most commonly used method to form SLBs. However, under physiological conditions, vesicle fusion (VF) is limited to only a subset of lipid compositions and solid supports. Here, we describe a one-step general procedure called the solvent-assisted lipid bilayer (SALB) formation method in order to form SLBs which does not require vesicles. The SALB method involves the deposition of lipid molecules onto a solid surface in the presence of water-miscible organic solvents (e.g., isopropanol) and subsequent solvent-exchange with aqueous buffer solution in order to trigger SLB formation. The continuous solvent exchange step enables application of the method in a flow-through configuration suitable for monitoring bilayer formation and subsequent alterations using a wide range of surface-sensitive biosensors. The SALB method can be used to fabricate SLBs on a wide range of hydrophilic solid surfaces, including those which are intractable to vesicle fusion. In addition, it enables fabrication of SLBs composed of lipid compositions which cannot be prepared using the vesicle fusion method. Herein, we compare results obtained with the SALB and conventional vesicle fusion methods on two illustrative hydrophilic surfaces, silicon dioxide and gold. To optimize the experimental conditions for preparation of high quality bilayers prepared via the SALB method, the effect of various parameters, including the type of organic solvent in the deposition step, the rate of solvent exchange, and the lipid concentration is discussed along with troubleshooting tips. Formation of supported membranes containing high fractions of cholesterol is also demonstrated with the SALB method, highlighting the technical capabilities of the SALB technique for a wide range of membrane configurations.