Phase behavior and nanoscale structure of phospholipid membranes incorporated with acylated C14-peptides

The thermotropic phase behavior and lateral structure of dipalmitoylphosphatidylcholine (DPPC) lipid bilayers containing an acylated peptide has been characterized by differential scanning calorimetry (DSC) on vesicles and atomic force microscopy (AFM) on mica-supported bilayers. The acylated peptide, which is a synthetic decapeptide N-terminally linked to a C14 acyl chain (C14-peptide), is incorporated into DPPC bilayers in amounts ranging from 0-20 mol %. The calorimetric scans of the two-component system demonstrate a distinct influence of the C14-peptide on the lipid bilayer thermodynamics. This is manifested as a concentration-dependent downshift of both the main phase transition and the pretransition. In addition, the main phase transition peak is significantly broadened, indicating phase coexistence. In the AFM imaging scans we found that the C14-peptide, when added to supported gel phase DPPC bilayers, inserts preferentially into preexisting defect regions and has a noticeable influence on the organization of the surrounding lipids. The presence of the C14-peptide gives rise to a laterally heterogeneous bilayer structure with coexisting lipid domains characterized by a 10 A height difference. The AFM images also show that the appearance of the ripple phase of the DPPC lipid bilayers is unaffected by the C14-peptide. The experimental results are supported by molecular dynamics simulations, which show that the C14-peptide has a disordering effect on the lipid acyl chains and causes a lateral expansion of the lipid bilayer. These effects are most pronounced for gel-like bilayer structures and support the observed downshift in the phase-transition temperature. Moreover, the molecular dynamics data indicate a tendency of a tryptophan residue in the peptide sequence to position itself in the bilayer headgroup region.     

Preferential accumulation of Abeta(1-42) on gel phase domains of lipid bilayers: an AFM and fluorescence study

Peptide-membrane interactions have been implicated in both the toxicity and aggregation of beta-amyloid (Abeta) peptides. Recent studies have provided evidence for the involvement of liquid-ordered membrane domains known as lipid rafts in the formation and aggregation of Abeta. As a model, we have examined the interaction of Abeta(1-42) with phase separated DOPC/DPPC lipid bilayers using a combination of atomic force microscopy (AFM) and total internal reflection fluorescence microscopy (TIRF). AFM images show that addition of Abeta to preformed supported bilayers leads to accumulation of small peptide aggregates exclusively on the gel phase DPPC domains. Initial aggregates are observed approximately 90 min after peptide addition and increase in diameter to 45-150 nm within 24 h. TIRF studies with a mixture of Abeta and Abeta-Fl demonstrate that accumulation of the peptide on the gel phase domains occurs as early as 15 min after Abeta addition and is maintained for over 24 h. By contrast, Abeta is randomly distributed throughout both fluid and gel phases when the peptide is reconstituted into DOPC/DPPC vesicles prior to formation of a supported bilayer. The preferential accumulation of Abeta on DPPC domains suggests that rigid domains may act as platforms to concentrate peptide and enhance its aggregation and may be relevant to the postulated involvement of lipid rafts in modulating Abeta activity in vivo.     

Effects of diacylglycerols on the structure of phosphatidylcholine bilayers: a 2H and 31P NMR study

The interaction of four diacylglycerols (DAGs) with multilamellar phospholipid bilayers consisting either of dipalmitoylphosphatidylcholine (DPPC) or of a mixture of DPPC and bovine liver phosphatidylcholine (BL-PC) extracts was investigated by a combination of 31P and 2H NMR spectrometry. We found that saturated and unsaturated long-chain DAGs induce different types of perturbations into the bilayer structure. The saturated DAGs dipalmitin and distearin induce lateral phase separation of the lipids into (i) DAG-enriched gellike domains and (ii) relatively DAG-free regions in the liquid-crystalline phase. In the latter regions, the order parameters along the fatty acyl chains of DPPC are practically identical with the control. This phase separation effect was observed in both model systems studied, and its extent is dependent upon DAG concentration and temperature. Only bilayer phases were present upon addition of dipalmitin or distearin at all concentrations and temperatures studied. The unsaturated DAGs diolein and DAG derived from egg PC (egg-DAG) affect PC bilayers in the following two ways: (i) by increasing the order parameters of the side chains, as observed for both DPPC and BL-PC model systems; (ii) by inducing nonbilayer lipid phases, as observed for BL-PC, but not DPPC. At a concentration of 25 mol % of an unsaturated DAG in mixed PC bilayers, a peak corresponding to isotropic lipid conformation appeared and increased in intensity with increase in temperature, while at 32 mol % hexagonal and bilayer phases coexisted.(ABSTRACT TRUNCATED AT 250 WORDS)     

Preferential accumulation of Aβ(1−42) on gel phase domains of lipid bilayers: An AFM and fluorescence study

Peptide-membrane interactions have been implicated in both the toxicity and aggregation of β-amyloid (Aβ) peptides. Recent studies have provided evidence for the involvement of liquid-ordered membrane domains known as lipid rafts in the formation and aggregation of Aβ. As a model, we have examined the interaction of Aβ(1−42) with phase separated DOPC/DPPC lipid bilayers using a combination of atomic force microscopy (AFM) and total internal reflection fluorescence microscopy (TIRF). AFM images show that addition of Aβ to preformed supported bilayers leads to accumulation of small peptide aggregates exclusively on the gel phase DPPC domains. Initial aggregates are observed approximately 90 min after peptide addition and increase in diameter to 45-150 nm within 24 h. TIRF studies with a mixture of Aβ and Aβ-Fl demonstrate that accumulation of the peptide on the gel phase domains occurs as early as 15 min after Aβ addition and is maintained for over 24 h. By contrast, Aβ is randomly distributed throughout both fluid and gel phases when the peptide is reconstituted into DOPC/DPPC vesicles prior to formation of a supported bilayer. The preferential accumulation of Aβ on DPPC domains suggests that rigid domains may act as platforms to concentrate peptide and enhance its aggregation and may be relevant to the postulated involvement of lipid rafts in modulating Aβ activity in vivo.     

Correlation between the ripple phase and stripe domains in membranes

We investigate the relationship between stripe domains and the ripple phase in membranes. These have previously been observed separately without being linked explicitly. Past results have demonstrated that solid and ripple phases exhibit rich textural patterns related to the orientational order of tilted lipids and the orientation of ripple corrugations. Here we reveal a highly complex network pattern of ripple and solid domains in DLPC, DPPC bilayers with structures covering length scales from 10 nm to 100 μm. Using spincoated double supported membranes we investigate domains by correlated AFM and fluorescence microscopy. Cooling experiments demonstrate the mode of nucleation and growth of stripe domains enriched in the fluorescent probe. Concurrent AFM imaging reveals that these stripe domains have a one-to-one correspondence with a rippled morphology running parallel to the stripe direction. Both thin and thick stripe domains are observed having ripple periods of 13.5±0.2 nm and 27.4±0.6 nm respectively. These are equivalent to previously observed asymmetric/equilibrium and symmetric/metastable ripple phases, respectively. Thin stripes grow from small solid domains and grow predominantly in length with a speed of ~3 times that of the thick stripes. Thick stripes grow by templating on the sides of thinner stripes or can emerge directly from the fluid phase. Bending and branching angles of stripes are in accordance with an underlying six fold lattice. We discuss mechanisms for the nucleation and growth of ripples and discuss a generic phase diagram that may partly rationalize the coexistence of metastable and stable phases.     

Ripples and the formation of anisotropic lipid domains: imaging two-component supported double bilayers by atomic force microscopy

Direct visualization of the fluid-phase/ordered-phase domain structure in mica-supported bilayers composed of 1,2-dimyristoyl-sn-glycero-3-phosphocholine/1,2-distearoyl-sn-glycero-3-phosphocholine mixtures is performed with atomic force microscopy. The system studied is a double bilayer supported on a mica surface in which the top bilayer (which is not in direct contact with the mica) is visualized as a function of temperature. Because the top bilayer is not as restricted by the interactions with the surface as single supported bilayers, its behavior is more similar to a free-standing bilayer. Intriguing straight-edged anisotropic fluid-phase domains were observed in the fluid-phase/ordered-phase coexistence temperature range, which resemble the fluid-phase/ordered-phase domain patterns observed in giant unilamellar vesicles composed of such phospholipid mixtures. With the high resolution provided by atomic force microscopy, we investigated the origin of these anisotropic lipid domain patterns, and found that ripple phase formation is directly responsible for the anisotropic nature of these domains. The nucleation and growth of fluid-phase domains are found to be directed by the presence of ripples. In particular, the fluid-phase domains elongate parallel to the ripples. The results show that ripple phase formation may have implications for domain formation in biological systems.     

Galactocerebroside-phospholipid interactions in bilayer membranes.

Differential scanning calorimetry (DSC) and x-ray diffraction have been used to study the interaction of hydrated N-palmitoylgalactosylsphingosine (NPGS) and dipalmitoylphosphatidylcholine (DPPC). For mixtures containing less than 23 mol% NPGS, complete miscibility of NPGS into hydrated DPPC bilayers is observed in both the bilayer gel and liquid-crystal phases. X-ray diffraction data demonstrate insignificant differences in the DPPC-bilayer gel-phase parameters on incorporation of up to 23 mol% NPGS. At greater than 23 mol% NPGS, additional high-temperature transitions occur, indicating phase separation of cerebroside. For these cerebroside concentrations, at 20 degrees C, x-ray diffraction shows two lamellar phases, hydrated DPPC-NPGS gel bilayers (d = 64 A) containing 23 mol% NPGS, and NPGS "crystal" bilayers (d = 55 A). On heating to temperatures greater than 45 degrees C, the mixed DPPC-NPGS bilayer phase undergoes chain melting, and on further increasing the temperature progressively more NPGS is incorporated into the liquid-crystal DPPC-NPGS bilayer phase. At temperatures greater than 82 degrees C (the transition temperature of hydrated NPGS), complete lipid miscibility is observed at all DPPC/NPGS molar ratios.     

Thermotropic and barotropic phase transitions of N-methylated dipalmitoylphosphatidylethanolamine bilayers

In order to understand the effect of polar head group modification on the thermotropic and barotropic phase behavior of phospholipid bilayer membranes, the phase transitions of dipalmitoylphosphatidylethanolamine (DPPE), dipalmitoylphosphatidyl-N-methylethanolamine (DPMePE), dipalmitoylphosphatidyl-N,N-dimethylethanolamine (DPMe2PE) and dipalmitoylphosphatidylcholine (DPPC) bilayer membranes were observed by differential scanning calorimetry and high-pressure optical methods. The temperatures of the so-called main transition from the gel (L(beta)) or ripple gel (P(beta)') phase to the liquid crystalline (L(alpha)) phase were almost linearly elevated by applying pressure. The slope of the temperature-pressure boundary, dT/dp, was in the range of 0.220-0.264 K MPa(-1) depending on the number of methyl groups in the head group of lipids. The main-transition temperatures of N-methylated DPPEs decreased with increasing size of head group by stepwise N-methylation. On the other hand, there was no significant difference in thermodynamic quantities of the main transition between the phospholipids. With respect to the transition from the subgel (L(c)) phase to the lamellar gel (L(beta) or L(beta)') phase, the transition temperatures were also elevated by applying pressure. In the case of DPPE bilayer the L(c)/L(beta) transition appeared at a pressure higher than 21.8 MPa. At a pressure below 21.8 MPa the L(c)/L(alpha) transition was observed at a temperature higher than the main-transition temperature. The main (L(beta)/L(alpha)) transition can be recognized as the transformation between metastable phases in the range from ambient pressure to 21.8 MPa. Polymorphism in the gel phase is characteristic of DPPC bilayer membrane unlike other lipid bilayers used in this study: the L(beta)', P(beta)' and pressure-induced interdigitated gel (L(beta)I) phases were observed only in the DPPC bilayer. Regarding the bilayers of DPPE, DPMePE and DPMe2PE, the interdigitation of acyl chain did not appear even at pressures as high as 200 MPa.     

Temperature dependence of the surface topography in dimyristoylphosphatidylcholine/distearoylphosphatidylcholine multibilayers

Simple lipid binary systems are intensively used to understand the formation of domains in biological membranes. The size of individual domains present in the gel/fluid coexistence region of single supported bilayers, determined by atomic force microscopy (AFM), generally exceeds by two to three orders of magnitude that estimated from multibilayers membranes by indirect spectroscopic methods. In this article, the topography of equimolar dimyristoylphosphatidylcholine/distearoylphosphatidylcholine (DMPC/DSPC) multibilayers, made of two superimposed bilayers supported on mica surface, was studied by AFM in a temperature range from room temperature to 45 degrees C. In the gel/fluid phase coexistence region the size of domains, between approximately 100 nm and a few micrometers, was of the same order for the first bilayer facing the mica and the top bilayer facing the buffer. The gel to fluid phase separation temperature of the first bilayer, however, could be increased by up to 8 degrees C, most likely as a function of the buffer layer thickness that separated it from the mica. Topography of the top bilayer revealed the presence of lipids in ripple phase up to 38-40 degrees C. Above this temperature, a pattern characteristic of the coexistence of fluid and gel domains was observed. These data show that difference in the size of lipid domains given by AFM and spectroscopy can hardly be attributed to the use of multibilayers models in spectroscopy experiments. They also provide a direct evidence for metastable ripple phase transformation into a gel/fluid phase separated structure upon heating.     

Interaction of cholesterol with galactocerebroside and galactocerebroside-phosphatidylcholine bilayer membranes

The interaction of the galactocerebroside, N-palmitoylgalactosylsphingosine (NPGS), with cholesterol has been studied by differential scanning calorimetry (DSC) and x-ray diffraction. Thermal and structural studies demonstrate complex behavior characterized by two endothermic transitions: transition I (TI approximately equal to 50-60 degrees C) corresponding to an NPGS-cholesterol bilayer gel----bilayer liquid crystal transition II (TII where TI less than TII less than TNPGS) corresponding to an NPGS bilayer crystal (stable E form)----bilayer liquid crystal transition. For mixtures containing from 6 to 80 mol % cholesterol, x-ray diffraction studies at 22 degrees C (T less than TI) indicate two separate lamellar phases; an NPGS crystal bilayer phase and a cholesterol monohydrate phase. For cholesterol concentrations less than 50 mol % at TI less than T less than TII, NPGS-cholesterol liquid crystal bilayer and excess NPGS crystal bilayer phases are observed. For greater than 50 mol % cholesterol concentrations at these temperatures, an excess cholesterol monohydrate phase coexists with the NPGS-cholesterol liquid crystal bilayers. At T greater than TII, complete NPGS-cholesterol miscibility is only observed for less than 50 mol % cholesterol concentrations, whereas at greater than 50 mol % cholesterol an excess cholesterol phase is present. The solid phase immiscibility of cerebroside and cholesterol at low temperatures is suggested to result from preferential NPGS-NPGS associations via hydrogen bonding. The unique thermal and structural behavior of NPGS-cholesterol dispersions is contrasted with the behavior of cholesterol-phosphatidycholine and cholesterol-sphingomyelin bilayers. Thermal and structural studies of NPGS in dipalmitoylphosphatidylcholine (DPPC)/cholesterol (1:1, molar ratio) bilayers have been performed. For dispersions containing less than 20 mol % NPGS at 22 degrees C there are no observable calorimetric transitions and x-ray diffraction studies indicate complete lipid miscibility. At greater than 20 mol % NPGS, a high temperature transition is observed that is shown by x-ray diffraction studies to be due to an excess NPGS crystal bilayer----liquid crystal bilayer transition. Complete miscibility of NPGS in DPPC/cholesterol bilayers is observed at T greater than TNPGS. The properties of NPGS/DPPC/cholesterol bilayers are discussed in terms of the lipid composition of the myelin sheath.     

Thiocyanate and bromide ions influence the bilayer structural parameters of phosphatidylcholine bilayers

The influence of monovalent cations and anions on the structural parameters of dipalmitoylphosphatidylcholine (DPPC) bilayers was examined at 25 degrees C using X-ray diffraction. It was shown that monovalent salts, in general, have little effect on lipid packing within the bilayer. However, fully hydrated DPPC bilayers in 1 M KSCN pack in an interdigitated acyl chain phase. This is the first observation of an ion-induced interdigitated bilayer phase in a zwitterionic lipid. In addition, gel state DPPC bilayers in 1 M KBr imbibe approx. 10 A more solvent than bilayers in water. The influence of these same salts on the phase transitions of DPPC bilayers was also examined using high-resolution differential scanning calorimetry. These results are discussed in terms of ion-induced changes in solvent and solvent/bilayer structure.     

Persistence at low temperature of the P beta' ripple in dipalmitoylphosphatidylcholine multilamellar vesicles containing either glycosphingolipids or cholesterol

The disappearance and reappearance of the P beta' ripple in multilamellar liposomes of dipalmitoylphosphatidylcholine (DPPC) has been examined by freeze-etch electron microscopy. The presence of less than 10 mol% of various glycosphingolipids or cholesterol in the liposomes markedly increases the time required for ripple disappearance when the vesicles are cooled from 38 degrees C to 30 degrees C, as compared to the pure phospholipid. Once the ripples have begun to disappear in the two-component vesicles, they do not uniformly reappear until the system is heated above the main transition of DPPC and allowed to cool into the pretransition region. These results suggest that the long time for ripple disappearance in the two-component systems reflects a slow molecular reorganization process which occurs when the systems are forced to change from the P beta' gel to the L beta' gel by a temperature downshift.     

Differing modes of interaction between monomeric Aβ(1-40) peptides and model lipid membranes: an AFM study

Membrane interactions with β-amyloid peptides are implicated in the pathology of Alzheimer's disease and cholesterol has been shown to be key modulator of this interaction, yet little is known about the mechanism of this interaction. Using atomic force microscopy, we investigated the interaction of monomeric Aβ(1-40) peptides with planar mica-supported bilayers composed of DOPC and DPPC containing varying concentrations of cholesterol. We show that below the bilayer melting temperature, Aβ monomers adsorb to, and assemble on, the surface of DPPC bilayers to form layers that grow laterally and normal to the bilayer plane. Above the bilayer melting temperature, we observe protofibril formation. In contrast, in DOPC bilayers, Aβ monomers exhibit a detergent-like action, forming defects in the bilayer structure. The kinetics of both modes of interaction significantly increases with increasing membrane cholesterol content. We conclude that the mode and rate of the interaction of Aβ monomers with lipid bilayers are strongly dependent on lipid composition, phase state and cholesterol content.     

Coexisting stripe- and patch-shaped domains in giant unilamellar vesicles

We report a new type of gel-liquid phase segregation in giant unilamellar vesicles (GUVs) of mixed lipids. Coexisting patch- and stripe-shaped gel domains in GUV bilayers composed of DOPC/DPPC or DLPC/DPPC are observed by confocal fluorescence microscopy. The lipids in stripe domains are shown to be tilted according to the DiIC18 fluorescence intensity dependence on the excitation polarization. The patch domains are found to be mainly composed of DPPC-d62 according to the coherent anti-Stokes Raman scattering (CARS) images of DOPC/DPPC-d62 bilayers. When cooling GUVs from above the miscibility temperature, the patch domains start to appear between the chain melting and the pretransition temperature of DPPC. In GUVs containing a high molar percentage of DPPC, the stripe domains form below the pretransition temperature. Our observations suggest that the patch and stripe domains are in the Pbeta' and Lbeta' gel phases, respectively. According to the thermoelastic properties of GUVs described by Needham and Evans [(1988) Biochemistry 27, 8261-8269], the Pbeta' and Lbeta' phases are formed at relatively low and high membrane tensions, respectively. GUVs with high DPPC percentage have high membrane surface tension and thus mainly exhibit Lbeta' domains, while GUVs with low DPPC percentage have low membrane surface tension and form Pbeta' domains accordingly. Adding negatively charged lipid to the lipid mixtures or applying an osmotic pressure to GUVs using sucrose solutions releases the surface tension and leads to the disappearance of the Lbeta' gel phase. The relationship between the observed domains in free-standing GUV bilayers and those in supported bilayers is discussed.     

Evolution of a rippled membrane during phospholipase A2 hydrolysis studied by time-resolved AFM

The sensitivity of phospholipase A(2) (PLA(2)) for lipid membrane curvature is explored by monitoring, through time-resolved atomic force microscopy, the hydrolysis of supported double bilayers in the ripple phase. The ripple phase presents a corrugated morphology. PLA(2) is shown to have higher activity toward the ripple phase compared to the gel phase in 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) membranes, indicating its preference for this highly curved membrane morphology. Hydrolysis of the stable and metastable ripple structures is monitored for equimolar DMPC/1,2-distearoyl-sn-glycero-3-phosphocholine (DSPC)-supported double bilayers. As shown by high-performance liquid chromatography results, DSPC is resistant to hydrolysis at this temperature, resulting in a more gradual hydrolysis of the surface that leads to a change in membrane morphology without loss of membrane integrity. This is reflected in an increase in ripple spacing, followed by a sudden flattening of the lipid membrane during hydrolysis. Hydrolysis of the ripple phase results in anisotropic holes running parallel to the ripples, suggesting that the ripple phase has strip regions of higher sensitivity to enzymatic attack. Bulk high-performance liquid chromatography measurements indicate that PLA(2) preferentially hydrolyzes DMPC in the DMPC/DSPC ripples. We suggest that this leads to the formation of a flat gel-phase lipid membrane due to enrichment in DSPC. The results point to the ability of PLA(2) for inducing a compositional phase transition in multicomponent membranes through preferential hydrolysis while preserving membrane integrity.     

Blistering of supported lipid membranes induced by Phospholipase D, as observed by real-time atomic force microscopy

Phospholipase D from Streptomyces chromofuscus (PLDSc) is a soluble enzyme known to be activated by the phosphatidic acid (PA)-calcium complexes. Despite the vast body of literature that has accumulated on this enzyme, the exact mechanism of activation remains poorly understood. In this work, we report the first observation of PLDSc activity in real time and at nanometer resolution using atomic force microscopy (AFM). AFM images of continuous and patchy dipalmitoylphosphatidylcholine (DPPC) bilayers were recorded, prior and after incubation with PLDSc. For continuous bilayers, the enzyme induced important morphological alterations; holes corresponding to the bilayer thickness were created, while an additional elevated phase, about 2.5 nm high, was observed. This bilayer blistering is believed to be due to the production of the negatively charged lipid PA that would cause localized repulsions between the bilayer and the underlying mica surface. By contrast, these elevated domains were not seen on patchy bilayers incubated with the enzyme. Instead, the shapes of DPPC patches were strongly deformed by enzyme activity and evolved into melted morphologies. These results point to the importance of lipid packing on PLD activity and illustrate the potential of AFM for visualizing remodeling enzymatic activities.     

Controlling association of vesicle embedded peptides by alteration of the physical state of the lipid matrix

We report here the reversible association of a designed peptide embedded in a lipid membrane through a stimulus-sensitive trigger that changes the physical state of the bilayer matrix. A peptide designed with the classical 4-3 heptad repeat of coiled coils, equipped with leucine residues at all canonical interface positions, TH1, was rendered membrane soluble by replacement of all exterior residues with randomly selected hydrophobic amino acids. Insertion of TH1 into large unilamellar phosphatidylcholine vesicles was followed by monitoring tryptophan fluorescence. Peptide insertion was observed when the lipids were in the liquid-crystalline state [1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)] but not when they were in the crystalline phase [1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC)]. Formation of a trimeric alpha-helical bundle in lipid bilayers was followed by fluorescence resonance energy transfer. Global fit analysis revealed a monomer--trimer equilibrium with a dissociation constant of around 10(-5) [corrected] MF(2). A lipid mixture composed of DPPC and POPC exhibiting a phase transition at 34 degrees C between a crystalline/liquid-crystalline coexistence region and a completely miscible liquid-crystalline phase was used to control the formation of the trimeric peptide bundle. TH1 is phase excluded in crystalline DPPC domains below 34 degrees C, leading to a larger number of trimers. However, when the DPPC domains are dispersed at temperatures above 34 degrees C, the number of trimers is reduced.     

Blistering of supported lipid membranes induced by Phospholipase D, as observed by real-time atomic force microscopy

Phospholipase D from Streptomyces chromofuscus (PLDSc) is a soluble enzyme known to be activated by the phosphatidic acid (PA)-calcium complexes. Despite the vast body of literature that has accumulated on this enzyme, the exact mechanism of activation remains poorly understood. In this work, we report the first observation of PLDSc activity in real time and at nanometer resolution using atomic force microscopy (AFM). AFM images of continuous and patchy dipalmitoylphosphatidylcholine (DPPC) bilayers were recorded, prior and after incubation with PLDSc. For continuous bilayers, the enzyme induced important morphological alterations; holes corresponding to the bilayer thickness were created, while an additional elevated phase, about 2.5 nm high, was observed. This bilayer blistering is believed to be due to the production of the negatively charged lipid PA that would cause localized repulsions between the bilayer and the underlying mica surface. By contrast, these elevated domains were not seen on patchy bilayers incubated with the enzyme. Instead, the shapes of DPPC patches were strongly deformed by enzyme activity and evolved into melted morphologies. These results point to the importance of lipid packing on PLD activity and illustrate the potential of AFM for visualizing remodeling enzymatic activities.     

Submicron structure in L-alpha-dipalmitoylphosphatidylcholine monolayers and bilayers probed with confocal, atomic force, and near-field microscopy.

Langmuir-Blodgett (LB) monolayers and bilayers of L-alpha-dipalmitoylphosphatidylcholine (DPPC), fluorescently doped with 1,1'-dioctadecyl-3,3,3',3'-tetramethylindocarbocyanine perchlorate (diIC18), are studied by confocal microscopy, atomic force microscopy (AFM), and near-field scanning optical microscopy (NSOM). Beyond the resolution limit of confocal microscopy, both AFM and NSOM measurements of mica-supported lipid monolayers reveal small domains on the submicron scale. In the NSOM studies, simultaneous high-resolution fluorescence and topography measurements of these structures confirm that they arise from coexisting liquid condensed (LC) and liquid expanded (LE) lipid phases, and not defects in the monolayer. AFM studies of bilayers formed by a combination of LB dipping and Langmuir-Schaefer monolayer transfer exhibit complex surface topographies that reflect a convolution of the phase structure present in each of the individual monolayers. NSOM fluorescence measurements, however, are able to resolve the underlying lipid domains from each side of the bilayer and show that they are qualitatively similar to those observed in the monolayers. The observation of the small lipid domains in these bilayers is beyond the spatial resolving power of confocal microscopy and is complicated in the topography measurements taken with AFM, illustrating the utility of NSOM for these types of studies. The data suggest that the small LC and LE lipid domains are formed after lipid transfer to the substrate through a dewetting mechanism. The possible extension of these measurements to probing for lipid phase domains in natural biomembranes is discussed.     

The effect of cholesterol on measured interaction and compressibility of dipalmitoylphosphatidylcholine bilayers

We have examined the phase diagram of dipalmitoylphosphatidylcholine (DPPC)--cholesterol-water mixtures at low cholesterol content, and report phase separation between 3 and 10 mol% cholesterol. The two lamellar phases at equilibrium in this region appear to be pure DPPC and 11 mol% cholesterol in DPPC. For these two lamellar phases, which are made up of alternating layers of water and bimolecular lipid leaflets, we have measured the forces of interaction between leaflets and the lateral pressure and compressibility of the leaflets. Both bilayers experience a strong repulsive force when forced together only a few ?ngstr?ms (1 A = 0.1 nm) closer than their maximum separation in excess water. However, the presence of 11 mol% cholesterol causes the bilayers to move apart of 35-A separation from the 19-A characteristic of pure DPPC in excess water. This swelling may result from a decrease in van der Waals attraction between bilayers or from an increase in bilayer repulsion. Differences in bilayer interaction can be a cause for phase separation. More importantly these differences can cause changes in the composition of regions of membranes approaching contact. At 11 mol%, cholesterol substantially increases the lateral compressibility of DPPC bilayers leading to higher lateral density fluctuations and potentially higher bilayer permeability.