Jean-François Tocanne

Lipid domains and lipid/protein interactions in biological membranes

In the fluid mosaic model of membranes, lipids are organized in the form of a bilayer supporting peripheral and integral proteins. This model considers the lipid bilayer as a two-dimensional fluid in which lipids and proteins are free to diffuse. As a direct consequence, both types of molecules would be expected to be randomly distributed within the membrane. In fact, evidences are accumulating to indicate the occurrence of both a transverse and lateral regionalization of membranes which can be described in terms of micro- and macrodomains, including the two leaflets of the lipid bilayer. The nature of the interactions responsible for the formation of domains, the way they develop and the time- and space-scale over which they exist represent today as many challenging problems in membranology. In this report, we will first consider some of the basic observations which point to the role of proteins in the transverse and lateral regionalization of membranes. Then, we will discuss some of the possible mechanisms which, in particular in terms of lipid/protein interactions, can explain lateral heterogenities in membranes and which have the merit of providing a thermodynamic support to the existence of lipid domains in membranes.

Lipid lateral diffusion and membrane organization

Phospholipid; Photobleaching; Lateral diffusion; Membrane organization; Macrodomain; Microdomain

Molecular sorting of lipids by bacteriorhodopsin in dilauroylphosphatidylcholine/distearoylphosphatidylcholine lipid bilayers

A combined experimental and theoretical study is performed on binary dilauroylphosphatidylcholine/distearoylphosphatidylcholine (DLPC/DSPC) lipid bilayer membranes incorporating bacteriorhodopsin (BR). The system is designed to investigate the possibility that BR, via a hydrophobic matching principle related to the difference in lipid bilayer hydrophobic thickness and protein hydrophobic length, can perform molecular sorting of the lipids at the lipid-protein interface, leading to lipid specificity/selectivity that is controlled solely by physical factors. The study takes advantage of the strongly nonideal mixing behavior of the DLPC/DSPC mixture and the fact that the average lipid acyl-chain length is strongly dependent on temperature, particularly in the main phase transition region. The experiments are based on fluorescence energy transfer techniques using specifically designed lipid analogs that can probe the lipid-protein interface. The theoretical calculations exploit a microscopic molecular interaction model that embodies the hydrophobic matching as a key parameter. At low temperatures, in the gel-gel coexistence region, experimental and theoretical data consistently indicate that BR is associated with the short-chain lipid DLPC. At moderate temperatures, in the fluid-gel coexistence region, BR remains in the fluid phase, which is mainly composed of short-chain lipid DLPC, but is enriched at the interface between the fluid and gel domains. At high temperatures, in the fluid phase, BR stays in the mixed lipid phase, and the theoretical data suggest a preference of the protein for the long-chain DSPC molecules at the expense of the short-chain DLPC molecules. The combined results of the experiments and the calculations provide evidence that a molecular sorting principle is active because of hydrophobic matching and that BR exhibits physical lipid selectivity. The results are discussed in the general context of membrane organization and compartmentalization and in terms of nanometer-scale lipid-domain formation.

Characterization of membrane domains by FRAP experiments at variable observation areas.

Abstract In this paper we show that FRAP experiments at variable beam radii provide an experimental approach for investigating membrane organization and dynamics, with great potential for identifying micrometer-sized domains and determining their size and the diffusion coefficient of the lipid and protein molecules they contain. Monte Carlo simulations of FRAP experiments at variable beam radii R on models of compartmentalized membranes have allowed us to establish the relationships (i) between the mobile fraction M of a diffusing particle and the size r of the domains, and (ii) between the apparent diffusion coefficient Dapp and the real diffusion coefficient D0 of this particle inside the domains. Furthermore, in its present stage of development, this approach allows us to specify whether these domains are strictly closed or not. This approach was first validated on an experimental model of a strictly compartmentalized membrane consisting of a monolayer of apposed spherical phospholipid bilayers supported by silica beads of known radius (0.83 μm). To prevent fusion between the spherical bilayers 5 mol% of a polymer-grafted phospholipid was added to the lipids. Analysis of the M versus R data yielded a radius r of 0.92±0.09 μm for the spherical bilayers, close to that of the supporting silica beads. When applied to the experimental data available for lipids and proteins in the plasma membrane of living cells, this approach suggests the existence of domains within these membranes with a radius of about 0.4 – 0.7 μm for the lipids and 0.25 μm for the proteins. These domains are not strictly closed and they are believed to be delineated by fluctuating barriers which are more or less permeable to lipid and protein molecules.

Polymyxin B-induced phase separation and acyl chain interdigitation in phosphatidylcholine/phosphatidylglycerol mixtures

Monolayers, fluorescence polarization, differential scanning calorimetry and X-ray diffraction experiments have been carried out to examine the effect of the polypeptide antibiotic polymyxin B on the phase behaviour of dipalmitoylphosphatidylglycerol (DPPG) either pure or mixed with dimyristoylphosphatidylcholine (DMPC) and dipalmitoylphosphatidylcholine (DPPC). It is shown that in both phosphatidylglycerol alone and phosphatidylglycerol/phosphatidylcholine mixtures, polymyxin B can induce either phase separation between lipid domains of various compositions or interdigitation of the acyl chains in the solid state, without segregation of the two lipids. Phase separation was observed by fluorescence and differential scanning calorimetry after addition of the antibiotic to vesicles composed of mixtures of DMPC and DPPG in conditions where polymyxin B did not saturate phosphatidylglycerol (DPPG to polymyxin B molar ratio, Ri, higher than 15). Phase separation was also observed in mixed monolayers of DPPC and of the 5:1 DPPG/polymyxin B complex, at high surface pressure. Acyl chain interdigitation was observed by X-ray diffraction in both 5:1 DPPG/polymyxin B mixtures and preformed 5:5:1 DMPC/DPPG/polymyxin B mixture, in which the antibiotic saturates phosphatidylglycerol (Ri 5). In both cases, raising the temperature gave rise to a complex double-peaked phase transition by differential scanning calorimetry, from the interdigitating phase to a normal L alpha lamellar phase. As it is known that polymyxin B does not interact with phosphatidylcholine, the data presented show that, when phosphatidylcholine and phosphatidylglycerol are mixed together, a phase perturbation such as acyl chain interdigitation, which normally affects only phosphatidylglycerol, is also felt by phosphatidylcholine.

Polymyxin B-phosphatidylglycerol interactions. A monolayer (π, ΔV) study

Abstract Through a monolayer investigation (π, ΔV ), it is shown that the cationic antibiotic polymyxin B (or E) strongly interacts with films of acidic lipids, namely the didodecanoyl- and dihexadecanoylphosphatidylglycerol. The zwitterionic dihexadecanoylphosphatidylcholine was an unsuitable substrate. Interactions occurred at and above a polymyxin B concentration in the subphase of 2.5 · 10 −7 M, bringing about a considerable increase of both π and ΔV . These interactions proceeded in two steps, as revealed by a biphasic change of ΔV with time. They were independent of the film molecular packing (fluid or gel states) and of the initial film pressure. Since it was possible to monitor the relative number of polymyxin B and didodecanoyl- or dihexadecanoylphosphatidylglycerol molecules in the monolayer, it is demonstrated that, at saturation, one polymyxin B molecule is bound to five phosphatidylglycerol molecules, a result which accounts for an exact neutralization of the charges. From competition experiments, it is shown that Na + is ineffective in removing polymyxin B from the interface. Ca 2+ appeared to be a stronger competitor but no complete antibiotic desorption was observed even at a Ca 2+ concentration of 100 mM. As a working hypothesis, the antibiotic/lipid ( 1 5 ) system was assumed to constitute by itself one molecular species. The mixing of the polymyxin B/didodecanoylphosphatidylglycerol ( 1 5 ) system with an excess of lipid molecules in the monolayer was found to be ideal both in terms of π and ΔV . With dihexadecanoylphosphatidylglycerol, a small condensing effect could be detected only at intermediate surface pressures, in a region where the lipid phase transition occurred. The molecular area of polymyxin B interacting with didodecanoylphosphatidylglycerol can be calculated to be 1.23 ± 0.05 nm 2 . It is proposed that the whole antibiotic molecule penetrates the film, the five bound lipid molecules being distributed around the peptide structure, at given positions imposed by the five 2,4-diaminobutyric acid residues.

Synthesis and physical properties of phosphatidylcholine labelled with 9-(2-anthryl)nonanoic acid, a new fluorescent probe

Abstract Synthesis and physical properties of a new anthracene fatty acid, 9-(2-anthryl)nonanoic acid, and the corresponding anthracene-phosphatidylcholines which were obtained by condensing the acid with sn -1-palmitoyl-lysophosphatidylcholine (PAPC) and with egg lysophosphatidylcholine (EAPC) are described. Differential scanning calorimetry experiments show that these lipids can undergo a liquid-crystal to gel phase transition at temperatures of 15°C and 18°C for EAPC and PAPC, respectively. In monolayers, PAPC exhibits a compression curve nearly superimposable to that of dipalmitoylphosphatidylcholine (DPPC), with a molecular area of 0.48 nm 2 at π = 30 mN m −1 . The data indicate that in these lipids, the anthracene group is only slightly more bulky than a normal acyl chain and that it does not significantly affect the regular phospholipid molecular packing. In ethanol solutions or when incorporated into egg phosphatidylcholine liposomes in a molar ratio of 1%, these lipids display UV absorption spectra and fluorescence emission spectra similar to those of 2-methyl anthracene. For EAPC liposomes, a broad and structureless fluorescence emission spectrum centered at around 450 nm, was recorded, suggesting the occurrence of anthracene excimers. As ascertained by UV spectrophotometry, differential scanning calorimetry, fluorescence polarization and anthracene photodimerization experiments, EAPC displays good miscibility properties with lipids in the liquid state (egg phosphatidylcholine) or in the gel state (distearoylphosphatidylcholine (DSPC)). The potential of these anthracene derivatives for studying the dynamics and the topological distribution of lipids in biomembranes is discussed.

The spatial distribution of phospholipids and glycolipids in the membrane of the bacterium Micrococcus luteus varies during the cell cycle.

Recently, we have developed a photocrosslinking approach which uses anthracene as a photoactivatable group and which allows us to determine the lateral distribution of lipids in membranes quantitatively. In synchronous cultures of the gram‐positive bacterium Micrococcus luteus, this approach shows that the spatial distribution of phosphatidylglycerol and diamnnosyldiacylglycerol, the two major lipids in the bacterial membrane, varies greatly during the cell cycle. Minimum heterogeneity was observed during cell growth while maximum heterogeneity was detected during cell division.

Binding of substance P to monolayers and vesicles made of phosphatidylcholine and/or phosphatidylserine

Analyses of interactions between substance P (SP) and phospholipids were performed by combined surface pressure and surface potential measurements in monolayers and by 13C-NMR experiments on liposomes. This study was carried out using synthetic SP molecules: [1-13C-Gly9]SP and [1-13C-Gly2]SP. Injection of SP into the aqueous subphase led to an expansion of phosphatidylcholine (PtdCho) or phosphatidylserine (PtdSer) monolayer surface area. An apparent association constant of SP for PtdSer was estimated to be around 10(6)-10(-7) M-1. The surface potential delta V/n varied linearly with the molecular area whereas the variation of surface pressure was biphasic, suggesting that at least two binding states contributed to the monolayer expansion. These two states Si (SP is inserted into the bilayer) and Ss (SP is stuck on the surface) were observed on vesicular membranes by 13C-NMR. The kinetic of interconversion between these two states can be estimated by NMR, the Ss state being the stablest one. No perpendicular insertion of SP into these vesicular preparations seemed to occur, as previously postulated. However, SP might form aggregates in contact with these model systems, leading to a loss of permeability of the lipid vesicles.

Interactions of amiodarone with model membranes and amiodarone-photoinduced peroxidation of lipids.

The potent antiarrhythmic drug, amiodarone (AMIO) exhibits phototoxicity, which is thought to be related to its interaction with biological membranes. We report here a spectroscopic study of the interactions of this drug with phosphatidylglycerol (PG) and phosphatidylcholine (PC) liposomes used as membrane model systems. A linear increase in absorbance at 300 nm was observed with increasing addition of AMIO to dimyristoyl-DL-PC (DMPC) liposomes over all the drugs-lipid molar ratio (Ri)s tested. In contrast, in the dimyristoyl-DL-PG (DMPG) liposomes, there was a dramatic increase in absorbance at values of Ri above unity. Light scattering by DMPG liposomes at 350 nm increased with increasing AMIO concentration up to a Ri = 1, and then decreased with increasing drug concentration. Such changes were not observed with the DMPC liposomes. Moreover, addition of AMIO changed the fluorescence polarization rate of 1,6-diphenyl 1,3,5-hexatriene embedded in these liposomes. It reduced the rate below the phase transition temperature (Tt) of the lipid, but increased it above this temperature. These effects on the lipidic phases observed at low Ri were more pronounced on the DMPG than on the DMPC liposomes. The strong interactions of AMIO with phospholipids, especially the acidic ones, were confirmed by liposome size determinations. All these data strongly suggest that the drug was incorporated in the core of the lipid bilayers. Such a penetration would favor a drug-photoinduced peroxidation of lipids. Indeed, UV irradiation of AMIO-DOPG mixtures led to the disappearance of the unsaturated fatty acids of phospholipids, checked by gas chromatography measurements, which was correlated with the amount of oxygen consumed. This showed that AMIO did photosensitize phospholipid peroxidation.