Topology of gel-phase domains and lipid mixing properties in phase-separated two-component phosphatidylcholine bilayers.

The influence of the lipid mixing properties on the lateral organization in a two-component, two-phase phosphatidylcholine bilayer was investigated using both an experimental (fluorescence recovery after photobleaching (FRAP)) and a simulated (Monte Carlo) approach. With the FRAP technique, we have examined binary mixtures of 1-stearoyl-2-capryl-phosphatidylcholine/1,2-distearoyl-phosphat idylcholine (C18C10PC/DSPC), and 1-stearoyl-2-capryl-phosphatidylcholine/1,2-dipalmitoyl-phospha tid ylcholine (C18C10PC/DPPC). Comparison with the 1,2-dimyristoyl-phosphatidylcholine/1,2-distearoyl-phosphatidylcholine (DMPC/DSPC) previously investigated by FRAP by Vaz and co-workers (Biophys. J., 1989, 56:869-876) shows that the gel phase domains become more effective in restricting the diffusion coefficient when the ideality of the mixture increases (i.e., in the order C18C10PC/DSPC-->C18C10PC/DPPC-->DMPC/DSPC). However, an increased lipid miscibility is accompanied by an increasing compositional dependence: the higher the proportion of the high-temperature melting component, the less efficient the gel phase is in compartmentalizing the diffusion plane, a trend that is best accounted for by a variation of the gel phase domain shape rather than size. Computer-simulated fluorescence recoveries obtained in a matrix obstructed with obstacle aggregates of various fractal dimension demonstrate that: 1) for a given obstacle size and area fraction, the relative diffusion coefficient increases linearly with the obstacle fractal dimension and 2) aggregates with a lower fractal dimension are more efficient in compartmentalizing the diffusion plane. Comparison of the simulated with the experimental mobile fractions strongly suggests that the fractal dimension of the gel phase domains increases with the proportion of high-temperature melting component in DMPC/DSPC and (slightly) in C18C10PC/DPPC.     

A correlation between lipid domain shape and binary phospholipid mixture composition in free standing bilayers: A two-photon fluorescence microscopy study

Giant unilamellar vesicles (GUVs) composed of different phospholipid binary mixtures were studied at different temperatures, by a method combining the sectioning capability of the two-photon excitation fluorescence microscope and the partition and spectral properties of 6-dodecanoyl-2-dimethylamino-naphthalene (Laurdan) and Lissamine rhodamine B 1,2-dihexadecanoyl-sn-glycero-3-phosphoethanolamine (N-Rh-DPPE). We analyzed and compared fluorescence images of GUVs composed of 1,2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-dipalmitoyl-sn-glycero-3-phosphocholine (DLPC/DPPC), 1, 2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-distearoyl-sn-glycero-3-phosphocholine (DLPC/DSPC), 1, 2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-diarachidoyl-sn-glycero-3-phosphocholine (DLPC/DAPC), 1, 2-dimyristoyl-sn-glycero-3-phosphocholine/1, 2-distearoyl-sn-glycero-3-phosphocholine (DMPC/DSPC) (1:1 mol/mol in all cases), and 1,2-dimyristoyl-sn-glycero-3-phosphoethanolamine/1, 2-dimyristoyl-sn-glycero-3-phosphocholine (DMPE/DMPC) (7:3 mol/mol) at temperatures corresponding to the fluid phase and the fluid-solid phase coexistence. In addition, we studied the solid-solid temperature regime for the DMPC/DSPC and DMPE/DMPC mixtures. From the Laurdan intensity images the generalized polarization function (GP) was calculated at different temperatures to characterize the phase state of the lipid domains. We found a homogeneous fluorescence distribution in the GUV images at temperatures corresponding to the fluid region for all of the lipid mixtures. At temperatures corresponding to phase coexistence we observed concurrent fluid and solid domains in the GUVs independent of the lipid mixture. In all cases the lipid solid domains expanded and migrated around the vesicle surface as we decreased the temperature. The migration of the solid domains decreased dramatically at temperatures close to the solid-fluid-->solid phase transition. For the DLPC-containing mixtures, the solid domains showed line, quasicircular, and dendritic shapes as the difference in the hydrophobic chain length between the components of the binary mixture increases. In addition, for the saturated PC-containing mixtures, we found a linear relationship between the GP values for the fluid and solid domains and the difference between the hydrophobic chain length of the binary mixture components. Specifically, at the phase coexistence temperature region the difference in the GP values, associated with the fluid and solid domains, increases as the difference in the chain length of the binary mixture component increases. This last finding suggests that in the solid-phase domains, the local concentration of the low melting temperature phospholipid component increases as the hydrophobic mismatch decreases. At the phase coexistence temperature regime and based on the Laurdan GP data, we observe that when the hydrophobic mismatch is 8 (DLPC/DAPC), the concentration of the low melting temperature phospholipid component in the solid domains is negligible. This last observation extends to the saturated PE/PC mixtures at the phase coexistence temperature range. For the DMPC/DSPC we found that the nonfluorescent solid regions gradually disappear in the solid temperature regime of the phase diagram, suggesting lipid miscibility. This last result is in contrast with that found for DMPE/DMPC mixtures, where the solid domains remain on the GUV surface at temperatures corresponding to that of the solid region. In all cases the solid domains span the inner and outer leaflets of the membrane, suggesting a strong coupling between the inner and outer monolayers of the lipid membrane. This last finding extends previous observations of GUVs composed of DPPE/DPPC and DLPC/DPPC mixtures (, Biophys. J. 78:290-305).     

Association of a fluorescent amphiphile with lipid bilayer vesicles in regions of solid-liquid-disordered phase coexistence

The effects of solid-fluid phase separations on the kinetics of association of a single-chain fluorescent amphiphile were investigated in two different systems: pure DMPC (dimyristoylphosphatidylcholine) and a 1:1 mixture of DMPC and DSPC (distearoylphosphatidylcholine). In pure DMPC vesicles, solid (s) and fluid (l(d)) phases coexist at the phase transition temperature, T(m), whereas a 1:1 mixture of DMPC and DSPC shows a stable s-l(d) phase separation over a large temperature interval. We found that in single-component bilayers, within the main phase transition, the experimental kinetics of association are clearly not single-exponential, the deviation from that function becoming maximal at the T(m). This observation can be accounted for by a rate of desorption that is slower than desorption from either fluid or solid phases, leaving the rates of insertion unchanged, but a treatment in terms of stable fluid and solid domains may not be adequate for the analysis of the association of an amphiphile with pure DMPC vesicles at the T(m). In DMPC/DSPC mixtures with solid-fluid phase coexistence, association occurs overall faster than expected based on phase composition. The observed kinetics can be described by an increase in the rate of insertion, leaving the desorption rates unchanged. The fast kinetics of insertion of the amphiphile into two-phase bilayers in two-component vesicles is attributed to a more rapid insertion into defect-rich regions, which are most likely phase boundaries between solid and fluid domains. A two-component mixture of lipids that shows a stable phase separation between l(d)-s phases over a large temperature interval thus behaves very differently from a single-component bilayer at the T(m), with respect to insertion of amphiphiles.     

Percolation and diffusion in three-component lipid bilayers: effect of cholesterol on an equimolar mixture of two phosphatidylcholines.

The lateral diffusion of a phospholipid probe is studied in bilayers of binary mixtures of dimyristoylphosphatidylcholine (DMPC)/cholesterol and distearoylphosphatidylcholine (DSPC)/cholesterol and in the ternary system DMPC/DSPC/cholesterol using fluorescence recovery after photobleaching. An approximate phase diagram for the ternary system, as a function of temperature and cholesterol concentration, was obtained using differential scanning calorimetry and the phase diagrams of the binary systems. This phase diagram is similar to those of the phospholipid/cholesterol binary mixtures. In bilayers where solid and liquid phases coexist, the diffusion results are interpreted in terms of phase percolation. The size of the liquid-phase domains is estimated using percolation theory. In the ternary system, addition of cholesterol up to approximately 20 mol% shifts the percolation threshold to lower area fractions of liquid, but the size of the liquid-phase domains does not change. Above approximately 20 mol% cholesterol, the liquid phase is always connected. The size of solid-phase domains clusters is estimated using a model recently developed (Almeida, P.F.F., W.L.C. Vaz, and T.E. Thompson. 1992. Biochemistry. 31:7198-7210). For cholesterol concentrations up to 20 mol%, the size of solid-phase domain units does not change. Beyond 20 mol%, cholesterol causes the size of the solid units to decrease.     

Phospholipase A(2) activity towards vesicles of DPPC and DMPC-DSPC containing small amounts of SMPC.

Phospholipase A(2) (PLA(2)) is an interfacially active enzyme whose hydrolytic activity is known to be enhanced in one-component phospholipid bilayer substrates exhibiting dynamic micro-heterogeneity. In this study the activity of PLA(2) towards large unilamellar vesicles composed of DPPC:SMPC and DMPC:DSPC:SMPC is investigated using fluorescence and HPLC techniques. Phase diagrams of the mixtures are established by differential scanning calorimetry and the PLA(2) activity, monitored by the lag time, is correlated with the phase behavior of the mixtures. In addition, the degree of lipid hydrolysis in the DMPC:DSPC:SMPC lipid mixtures is detected by HPLC. The PLA(2) activity is found to be significantly increased in the temperature range of the coexistence region where the lipid mixtures exhibit lateral gel-fluid phase separation. Furthermore, in the entire temperature range it is demonstrated that PLA(2) preferentially hydrolyzes the short chain DMPC lipid. This discriminative effect becomes less pronounced when the asymmetric lipid SMPC is present in the lipid substrate. Inclusion of SMPC into either DPPC or DMPC:DSPC vesicles prolongs the lag time. The results clearly show that the PLA(2) activity is significantly enhanced by lipid bilayer micro-heterogeneity in both one-component and multi-component lipid bilayer substrates. The PLA(2) activity measurements are discussed in terms of dynamic gel-fluid lipid domain formation due to density fluctuations and static lipid domain formation due to gel-fluid phase separation.     

A new method for determining the phase in the X-ray diffraction structure analysis of phosphatidylcholine/alcohol

A new method based on a sampling theorem is proposed for determining the phase in the X-ray diffraction analysis of the structure of phospholipid systems. The thickness of a lipid layer is changed by changing the length of hydrocarbon chains in order to rebuild the continuous transform from the scattering amplitudes. By employing this method, the phases were accurately determined in a structure analysis of nine phospholipid/alcohol systems at the interdigitated gel phase. The nine systems are dimyristoylphosphatidylcholine(DMPC)/propanol, DPPC/methanol, DPPC/ethanol, DPPC/propanol, DPPC/butanol, distearoylphosphatidylcholine(DSPC)/methanol, DSPC/ethanol, DSPC/propanol and DSPC butanol systems.     

Using micropatterned lipid bilayer arrays to measure the effect of membrane composition on merocyanine 540 binding

The lipophilic dye merocyanine 540 (MC540) was used to model small molecule-membrane interactions using micropatterned lipid bilayer arrays (MLBAs) prepared using a 3D Continuous Flow Microspotter (CFM). Fluorescence microscopy was used to monitor MC540 binding to fifteen different bilayer compositions simultaneously. MC540 fluorescence was two times greater for bilayers composed of liquid-crystalline (l.c.) phase lipids (1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC), 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC),1-stearoyl-2-oleoyl-sn-glycero-3-phosphocholine (SOPC), and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)) compared to bilayers in the gel phase (1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) and 1,2-distearoyl-sn-glycero-3-phosphocholine (DSPC)). The effect cholesterol (CHO) had on MC540 binding to the membrane was found to be dependent on the lipid component; cholesterol decreased MC540 binding in DMPC, DPPC and DSPC bilayers while having little to no effect on the remaining l.c. phase lipids. MC540 fluorescence was also lowered when 1,2-dioleoyl-sn-glycero-3-phospho-L-serine (sodium salt) (DOPS) was incorporated into DOPC bilayers. The increase in the surface charge density appears to decrease the occurrence of highly fluorescent monomers and increase the formation of weakly fluorescent dimers via electrostatic repulsion. This paper demonstrates that MLBAs are a useful tool for preparing high density reproducible bilayer arrays to study small molecule-membrane interactions in a high-throughput manner.     

Reorganization of lipid domain structure in membranes by a transmembrane peptide: an ESR spin label study on the effect of the Escherichia coli outer membrane protein A signal peptide on the fluid lipid domain connectivity in binary mixtures of dimyristoyl phosphatidylcholine and distearoyl phosphatidylcholine.

The effect of a transmembrane peptide on the domain structure of a two-component, two-phase lipid bilayer composed of dimyristoyl phosphatidylcholine (DMPC) and distearoyl phosphatidylcholine (DSPC) was examined by spin label electron spin resonance (ESR) spectroscopy. The peptide, pOmpA, is the hydrophobic, 25-residue signal sequence of the outer membrane protein A from Escherichia coli. Nitroxide derivatives of the phospholipid DSPC, 16-DSPCSL, and of the pOmpA signal peptide, pOmpA-IASL, were used as probes. The first-derivative lineshapes of the ESR spectra were analyzed using a normalized intensity ratio, R, that gives information on the average sizes of the disconnected fluid domains and their point of connectivity (Sankaram, M.B., D. Marsh, and T.E. Thompson. 1992. Biophys. J. 63:340-349). In the absence of the peptide, the number of fluid lipid domains does not vary with the fraction of lipid that is in the fluid phase, and phase conversion is accomplished solely by changes in the domain size. The phase boundaries of the lipid mixture remain largely unchanged by the presence of the peptide at mole fractions up to 0.02, but both the size and number of the fluid domains is changed, and the point at which they become connected is shifted to lower fractions of the fluid phase. In addition, the number of domains in the presence of the peptide no longer remains constant but increases from a domain density at low fractions of the fluid phase that is much lower than that in the absence of peptide to one that is comparable to the natural state in the absence of peptide at the point of domain connectivity. A simple model is presented for the process of domain fission, where the latter is determined by a balance between the effects of peptide concentration in the fluid domains, the line tension at the domain boundaries, and the distributional entropy of the domains.     

Ion permeation across the bilayer of annealed phosphatidylcholine vesicles at elevated temperatures. Concentration dependence and the micelle-bilayer dynamic equilibrium

The relative stability of the lipid bilayer toward ions above the crystalline to liquid-crystalline phase transition temperature has been studied under isotonic conditions for small annealed vesicles of dilauroyl (DLPC), dimyristoyl (DMPC), diplamitoyl (DPPC), and distearoyl (DSPC) phosphatidylcholine by using lanthanide ions as a probe. The bilayer stability increased as the chain length of the lipid fatty acid increased, and a rapid translocation of ions across the bilayer started at about 60, 70, and 80° C for DMPC, DPPC, and DSPC vesicles, respectively. The bilayer of DLPC vesicles is apparently permeable for the tested ions even at room temperature. Two other important phenomena concomitant with the observed translocation of ions were found. Firstly, the ion leakage occurred in an “an-or-none” fashion, i.e. as soon as the vesicles start to become permeable toward ions, the concentration of ions in the intra-and extravesicular media are equalized within a short time. Secondly, the rate of the relative number of inward facing lipid molecules which become exposed to extravesicularly added paramagnetic lanthanide is a function of the inverse phosphatidylcholine concentration. This feature explicitly excludes the possibilities that the observed ion leakage occurs through a diffusion, pore formation, or through the rupture of vesicle walls induced by vesicle-vesicle collisions. We instead propose as the most probable mechanism that a dynamic equilibrium between the various states of the phosphatidylcholine molecules in water, such as monomers, micelles, vesicles, and multilamellar liposomes, is in fact responsible for the observed phenomena.     

Membrane fluidity as affected by the organochlorine insecticide DDT

Fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH) was used to study the interaction of DDT with model and native membranes. DDT decreases the phase transition midpoint temperature (Tm) of liposomes reconstituted with dimyristoyl-, dipalmitoyl- and distearoylphosphatidylcholines (DMPC, DPPC and DSPC), and broadens the thermotropic profile of the transition. The effects of DDT are concentration dependent and are more pronounced in bilayers of short-chain lipids, e.g., DMPC. The insecticide fails to alter DPH polarization in the fluid phase of the above lipids. Similar effects were observed in binary mixtures of DMPC plus DPPC. Furthermore, DDT alters the single broad transition of the equimolar mixture of DMPC plus DSPC into a biphasic transition. The lower temperature component has a midpoint at 25 degrees C, i.e., a value close to the Tm of DMPC. DDT inhibits to some extent the cholesterol-induced ordering in DMPC bilayers and high cholesterol concentrations (greater than or equal to 30 mol%) do not prevent insecticide interaction, conversely to the effect observed for lindane (Antunes-Madeira, M.C. and Madeira, V.M.C. (1989) Biochim. Biophys. Acta 982, 161-166). Apparently, the bilayer order is not disturbed by DDT in fluid native membranes of mitochondria and sarcoplasmic reticulum, but moderate disordering effects are noticed in membranes enriched in cholesterol, namely, brain microsomes and erythrocytes.     

Permeability of dimyristoyl phosphatidylcholine/dipalmitoyl phosphatidylcholine bilayer membranes with coexisting gel and liquid-crystalline phases.

The passive permeation of glucose and a small zwitterionic molecule, methyl-phosphoethanolamine, across two-component phospholipid bilayers (dimyristoyl phosphatidylcholine (DMPC)/dipalmitoyl phosphatidylcholine (DPPC) mixtures) exhibit a maximum when gel domains and fluid domains coexist. The permeability data of the two-phase bilayers cannot be fitted to single-rate kinetics, but are consistent with a Gaussian distribution of rate constants. In pure DMPC and DPPC as well as in their mixtures, at the temperature of the maximum excess heat capacity, the logarithm of the average permeability rate constants are linearly correlated with the mole fraction of DPPC in the total system. In addition, in the 50:50 mixture, the excess heat capacity values as well as the apparent fractions of interfacial lipid correlate with the logarithm of the excess permeabilities in the two-phase region. These results suggest that small polar molecules can cross the membrane at the interface between gel and fluid domains at a much faster rate than through the homogeneous phases; the acyl chains located at the domain interface experience lateral density fluctuations that are inversely proportional to their average length, and large enough to allow rapid transmembrane diffusion of the solute molecules. The distribution of the permeability rate constants may reflect temporal and spatial fluctuations of the lipid composition at the phase boundaries.     

A differential scanning calorimetry study of the interaction of free fatty acids with phospholipid membranes

Mixtures of stearic, arachic, oleic and linoleic acids with dimyristoylphosphatidylcholine (DMPC) and distearylphosphatidylcholine (DSPC) have been studied by means of differential scanning calorimetry (DSC). The mixtures of stearic (SA) and arachic acids (AA) with DMPC and DSPC show phase diagrams of the peritectic type, with a region of solid phase immiscibility from 0 to 28.5 mol% of fatty acid. A pure component, with a stoichiometry fatty acid/phospholipid (2:1) seems to be formed except for the system AA/DSPC. The mixtures of oleic (OA) and linoleic acids (LA) show complex phase diagrams. In the case of OA, different regions where a phase separation exists can be observed and for the mixture of OA with DMPC, a pure component seems to be formed with a stoichiometry OA/DMPC (1:2). LA shows different behaviour in the mixtures with DMPC and with DSPC. For the mixture, LA/DMPC, a fluid phase immiscibility region is observed over the same range of concentration as for the mixture with OA, however, the mixture with DSPC shows a solid phase immiscibility for the samples containing 45 mol% or more of LA. The interaction of the different free fatty acids with equimolar mixtures of DMPC and DSPC, showing monotectic behaviour, has also been analyzed. From our results it can be clearly concluded that saturated fatty acids partition preferentially into solid-like domains, while cis-unsaturated fatty acids partition preferentially into fluid-like domains.     

The effects of bilirubin on the thermal properties of phosphatidylcholine bilayers.

The thermotropic properties of multilamellar vesicles of dimyristoylphosphatidylcholine (DMPC), dipalmitoylphosphatidylcholine (DPPC), and distearoylphosphatidylcholine (DSPC), as a function of the concentration of bilirubin in the range of 0.1 to 1 mol%, were measured. The exact effects of bilirubin depended on the chain length of the polymethylene chains. But the general effects of bilirubin were the same in all systems. At the lowest concentrations tested (0.1 mol bilirubin/100 mol phospholipid (0.1 mol%)), bilirubin broadened and shifted to higher temperatures the main phase transitions of all bilayers. For DPPC and DSPC, but not DMPC, this concentration of bilirubin was associated with a new transition at 25 degrees C (DPPC) or 34 degrees C (DSPC). Bilirubin at 0.2 mol% was required for the detection of a similar transition (at 13.7 degrees C) in DMPC. Higher concentrations of bilirubin (> 0.2 mol%) suppressed completely the main phase transitions in all bilayers but increased the enthalpy of the new transition. Maximal values of delta H for these transitions were reached at 0.5, 0.25, and 0.2 mol% bilirubin in DMPC, DPPC, and DSPC, respectively. Values of delta H and delta S for these transitions were far larger than for the corresponding gel-to-liquid crystal transitions in pure lipid bilayers but were equal to those expected for a transition between crystalline and liquid crystalline phases.     

Lateral organization and domain formation in a two-component lipid membrane system

The thermodynamic phase behavior and lateral lipid membrane organization of unilamellar vesicles made from mixtures of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) and 1,2 distearoyl-sn-glycero-3-phosphocholine (DSPC) were investigated by fluorescence resonance energy transfer (FRET) as a function of temperature and composition. This was done by incorporating a headgroup-labeled lipid donor (NBD-DPPE) and acceptor (N-Rh-DPPE) in low concentrations into the binary mixtures. Two instances of increased energy transfer efficiency were observed close to the phase lines in the DMPC/DSPC phase diagram. The increase in energy transfer efficiency was attributed to a differential preference of the probes for dynamic and fluctuating gel/fluid coexisting phases. This differential preference causes the probes to segregate (S. Pedersen, K. J?rgensen, T. R. Baekmark, and O. G. Mouritsen, 1996, Biophys. J. 71:554-560). The observed increases in energy transfer match with the boundaries of the DMPC/DSPC phase diagram, as measured by Fourier transform infrared spectroscopy (FTIR) and differential scanning calorimetry (DSC). We propose that the two instances of probe segregation are due to the presence of DMPC-rich and DSPC-rich domains, which form a dynamic structure of gel/fluid coexisting phases at two different temperatures. Monitoring the melting profile of each lipid component independently by FTIR shows that the domain structure is formed by DMPC-rich and DSPC-rich domains rather than by pure DMPC and DSPC domains.     

EPR spin label study of walnut oil effects on phosphatidylcholine membranes

Effects of walnut oil (WO) on dynamic and thermodynamic properties of 0–50 wt% cholesterol (CH) containing dimyristoylphosphatidylcholine (DMPC) and 10 wt% CH containing dipalmitoylphosphatidylcholine (DPPC) membrane dispersions were studied by electron paramagnetic resonance (EPR), using 5-doxyl stearic acid (5-DSA) and 16-doxyl stearic acid (16-DSA). Incorporation of 10 wt% WO alone decreased the phase transition temperature and created depth-dependent effects at the gel phase. The order increased close to the head region and decreased in the hydrocarbon core of the DMPC bilayer. For DPPC, the order decreased both close to head region and in the hydrocarbon core. Ten weight percent WO did not have considerable effect at the fluid phase for both DMPC and DPPC. Incorporation of 40 wt% WO into DMPC created an abrupt decrease in the maximum hyperfine splitting values after 305 K. The effect of 10 wt% WO in CH containing DMPC dispersions was dependent on the CH concentration. An increase and a decrease in the order were observed at low and high CH concentrations, respectively. Incorporation of WO created different effects on fluidity of 10 wt% CH containing DMPC and DPPC dispersions. Close to the head group region, the order in DMPC increased both in the gel and fluid phases; but for DPPC, an opposite effect was observed in both of the phases. In the hydrocarbon core of the bilayer, addition of 10 wt% WO into 10 wt% CH containing DMPC decreased the order in the gel phase and WO did not affect the order in the fluid phase. For DPPC, WO effects were observed to alter with temperature. In the studied temperature range, order parameters, diffusion constants and effective tilt angles were obtained from simulations of the spectra using Microscopic Order Macroscopic Disorder (MOMD) and Vary Anisotropic Reorientation (VAR) models. For 16-DSA, spectra were also simulated using two domains with EPRSIM.     

Phospholipid miscibility in ternary mixtures

The gel to liquid-crystalline phase transition of aqueous dispersions of phospholipid mixtures was investigated by means of the repartition of the spin label 2,2,6,6-tetramethylpiperidine-I-oxyl between aqueous space and lipid hydrocarbon region. The dimyristoylphosphatidylcholine (DMPC)/dibehenoylphosphatidylcholine (DBPC) and dipalmitoylphosphatidylcholine (DPPC)/DBPC phase diagrams indicate gel phase immiscibility, whereas the distearoylphosphatidylcholine (DSPC)/DBPC phase diagram indicates non-ideal gel phase miscibility at low DBPC molar fractions. Aqueous dispersions of DMPC/DPPC/DBPC ternary mixtures show two distinct phase transitions, the first associated with the melting of a DMPC/DPPC phase and the second with the melting of a DBPC phase. Aqueous dispersions of DMPC/DSPC/DBPC ternary mixtures show to phase transitions at low DSPC molar fractions; the first is probably associated with the melting of a DMPC/DSPC phase, and the second with the melting of a DBPC/DSPC phase. At high DSPC molar fractions, only one phase transition is observed; this suggests that all the lipids are mixed in gel state membranes.     

Two-dimensional diffusion of amphiphiles in phospholipid monolayers at the air-water interface.

Steady-state and time-resolved fluorescence spectroscopy has been used to examine lateral diffusion in dipalmitoyl-L-alpha-phosphatidylcholine (DPPC) and dimyristoyl-L-alpha-phosphatidylcholine (DMPC) monolayers at the air-water interface, by studying the fluorescence quenching of a pyrene-labeled phospholipid (pyrene-DPPE) by two amphiphilic quenchers. Steady-state fluorescence measurements revealed pyrene-DPPE to be homogeneously distributed in the DMPC lipid matrix for all measured surface pressures and only in the liquid-expanded (LE) phase of the DPPC monolayer. Time-resolved fluorescence decays for pyrene-DPPE in DMPC and DPPC (LE phase) in the absence of quencher were best described by a single-exponential function, also suggesting a homogeneous distribution of pyrene-DPPE within the monolayer films. Addition of quencher to the monolayer film produced nonexponential decay behavior, which is adequately described by the continuum theory of diffusion-controlled quenching in a two-dimensional environment. Steady-state fluorescence measurements yielded lateral diffusion coefficients significantly larger than those obtained from time-resolved data. The difference in these values was ascribed to the influence of static quenching in the case of the steady-state measurements. The lateral diffusion coefficients obtained in the DMPC monolayers were found to decrease with increasing surface pressure, reflecting a decrease in monolayer fluidity with compression.     

Properties of lipid-apolipoprotein association products. Complexes of human apo AI and binary phospholipid mixtures

The products resulting from the association of human apo A-I with binary phospholipid mixtures of dimyristoyl phosphatidylcholine (DMPC) and either dipalmitoyl (DPPC) or distearoyl (DSPC) phosphatidylcholine have been isolated and characterized. Effective lipid . protein complex formation was found to occur at the onset temperature for melting of the gel state, and equal incorporation of both lipid components of the binary mixture was observed. Two sizes of products were obtained, one containing 2 A-I molecules per complex and the other containing 3; the proportions of these two products depended upon the initial phospholipid/protein ratio employed. these two product species were found to be resolvable by density gradient centrifugation as well as gel filtration, reflecting substantial differences in composition as well as size. The ratio of DMPC to DPPC or DSPC was the same in the isolated complexes as in the initial mixture, suggesting that th protein does not associate preferentially with the fluid phase lipid, but with lipid domains in which the components are randomly distributed. Electron microscopy of recombinant particles containing a 2:1 ratio (w/w) of DSPC to DMPC revealed stacks of discs whose thickness was proportionately greater than for discs containing DMPC alone. Also of significance was the finding that recombinant discs containing 3 A-I molecules possessed a diameter approximately 1.5 times larger than recombinant discs containing 2 A-I molecules. These data are consistent with the model for the recombinant particles described by Tall et al. (Tall, A.R., Small, D.M., Deckelbau, R.J., and Shipley, G.G. (1977) J. Biol. Chem. 252; 4701-4711), in which the phospholipid is found as a circular bilayer, the thickness of which is dependent upon the length of the acyl chain, and around which the protein is distributed as an annulus.     

Differences in the physical properties of lipid monolayers and bilayers on a spherical solid support.

A monolayer of 1,2-dipalmitoyl-d62-glycero-3-phosphocholine (DPPC-d62) coated onto silanized silica beads (spherical supported monolayer: SSM) is studied by 2H-NMR and DSC. The results are compared with those obtained from a single bilayer on the same solid support (spherical supported vesicles: SSV) and from multilamellar vesicles (MLV). The phase transition temperature (Tm) of the SSMs is significantly higher than that of the bilayer systems and the extent of this difference depends on the lipid density in the monolayer that is determined during its preparation. 2H-NMR reveals a gel and fluid phase coexistence in the SSM transition region. A comparison of the 2H-NMR line shapes suggests the presence of highly curved structures for the fluid phase of the SSM samples. From a comparison of SSM and SSV transverse relaxation in the fluid phase we can conclude that the lateral diffusion coefficient D1 in supported monolayers is similar to that in bilayers.     

Modelling the phase equilibria in two-component membranes of phospholipids with different acyl-chain lengths

A phenomenological model is proposed to describe the membrane phase equilibria in binary mixtures of saturated phospholipids with different acyl-chain lengths. The model is formulated in terms of thermodynamic and thermomechanic properties of the pure lipid bilayers, specifically the chain-melting transition temperature and enthalpy, the hydrophobic bilayer thickness, and the lateral area compressibility modulus. The model is studied using a regular solution theory made up of a set of interaction parameters which directly identify that part of the lipid-lipid interaction which is due to hydrophobic mismatch of saturated chains of different lengths. It is then found that there is effectively a single universal interaction parameter which, in the full composition range, describes the phase equilibria in mixtures of DMPC/DPPC, DPPC/DSPC, DMPC/DSPC, and DLPC/DSPC, in excellent agreement with experimental measurements. The model is used to predict the variation with temperature and composition of the specific heat, as well as of the average membrane thickness and area in each of the phases. Given the value of the universal interaction parameter, the model is then used to predict the phase diagrams of binary mixtures of phospholipids with different polar head groups, e.g., DPPC/DPPE, DMPC/DPPE and DMPE/DSPC. By comparison with experimental results for these mixtures, it is shown that difference in acyl-chain lengths gives the major contribution to deviation from ideal mixing. Application of the model to mixtures with non-saturated lipids is also discussed.