The condensing effect of cholesterol in lipid bilayers

The condensing effect of cholesterol on phospholipid bilayers was systematically investigated for saturated and unsaturated chains, as a function of cholesterol concentration. X-ray lamellar diffraction was used to measure the phosphate-to-phosphate distances, PtP, across the bilayers. The measured PtP increases nonlinearly with the cholesterol concentration until it reaches a maximum. With further increase of cholesterol concentration, the PtP remains at the maximum level until the cholesterol content reaches the solubility limit. The data in all cases can be quantitatively explained with a simple model that cholesterol forms complexes with phospholipids in the bilayers. The phospholipid molecules complexed with cholesterol are lengthened and this lengthening effect extends into the uncomplexed phospholipids surrounding the cholesterol complexes. This long-range thickening effect is similar to the effect of gramicidin on the thickness of lipid bilayers due to hydrophobic matching.     

The effect of temperature on lipid-n-alkane interactions in lipid bilayers

The relationship between age-related alterations in the lipid composition of cultured rat-heart fibroblasts and several biochemical and biophysical parameters was investigated. Aged (14-15-day-old) cultures displayed higher mole ratios of sphingomyelin to phosphatidylcholine, as well as elevated cholesterol levels. A concomitant increase was observed in the total protein content of the cells and in the Vmax values of both membranal and cytoplasmic marker enzymes. Fluorescence photobleaching recovery was employed to study the lateral mobility of the lipid probe NBD-phosphatidylethanolamine and of membrane glycoproteins that bind succinylated concanavalin A. The mobile fractions of both probes were higher in aged cultures, while the lateral diffusion coefficients were lower. To further demonstrate the dependence of the above parameters on the cellular lipid composition, we have manipulated the lipid composition of old cultures by treatments with liposomes (small unilamellar vesicles) of specific compositions. Treatments which reversed the lipid composition towards that of young (5-6-day-old) cultures caused a concomitant reversal of the measured biochemical and biophysical parameters to the values observed in young cultures. These findings suggest that alterations in the organization and mobility of cell membrane constituents are involved in mediating changes in cellular functions. In view of our previous findings on cultures of rat-heart myocytes (Yechiel, E., Barenholz, Y. and Henis, Y.I. (1985) J. Biol. Chem. 260, 9132-9136), it appears that the modulation of cellular properties through the membrane lipid composition may be a general phenomenon in many cell types.     

The effect of lanthanum on alamethicin channels in black lipid bilayers

The properties of alamethicin channels in dioleyl phosphatidylcholine bilayers were studied in 1 M LaCl3 and were compared with those in 1 M NaCl. Single-channel recordings demonstrated that the mean single-channel life-time is about 0.25 s in NaCl but only about 17 ms in LaCl3. Whereas in NaCl the conductance levels 2 and 3 are mostly populated, in LaCl3 the levels 0 and 1 are preferentially adopted. The single-level conductance are slightly smaller in LaCl3 if the higher bulk solution conductivity of LaCl3 is taken into account. Multipore experiments confirmed earlier results (Boheim, G., Irmscher, G. and Jung, G. (1978) Biochim. Biophys. Acta 507, 485--506) that the bilayer conductance is less strongly dependent on voltage in LaCl3 than in NaCl solution. Current-fluctuation analysis showed that this effect can be explained by a less strong dependence on voltage of the pore-formation rate as well as of the mean channel life-time in LaCl3. The data can be interpreted as an increased lateral diffusion mobility of the alamethicin monomers in the bilayer. This can be the result of the binding of La3+ to the polar headgroups which can induce cluster formation of the phospholipids.     

Softening of lipid bilayers

The softening of wet lipid bilayer membranes during their gel-to-fluid first-order phase transition is studied by computer simulation of a family of two-dimensional microscopic interaction models. The models include a variable number, q, of lipid chain conformational states, where 2q10. Results are presented as functions of q and temperature for a number of bulk properties, such as internal energy, specific heat, and lateral compressibility. A quantitative account is given of the statistics of the lipid clusters which are found to form in the neighborhood of the transition. The occurrence of these clusters is related to the softening and the strong thermal density fluctuations which dominate the specific heat and the lateral compressibility for the high-q models. The cluster distributions and the fluctuations behave in a manner reminiscent of critical phenomena and percolation. The findings of long-lived metastable states and extremely slow relaxational behavior in the transition region are shown to be caused by the presence of intermediate lipid chain conformational states which kinetically stabilize the cluster distribution and the effective phase coexistence. This has as its macroscopic consequence that the first-order transition apperas as a continuous transition, as invariably observed in all experiments on uncharged lecithin bilayer membranes. The results also suggest an explanation of the non-horizontal isotherms of lipid monolayers. Possible implications of lipid bilayer softening and enhanced passive permeability for the functioning of biological membranes are discussed.Abbreviations PC phosphatidvlcholine - DMPC dimyristoyl PC - DPPC dipalmitoyl PC - ac alternating current - DSC differential scanning calorimetry - T _m lipid gel-to-fluid phase transition temperature - TEMPO 2,2,6,6-tetramethylpiperidine-N-oxyl Supported by the Danish Natural Science Research Council and A/S De Danske Spritfabrikkers JubilæumslegatSupported in part by the NSERC of Canada and Le FCAC du Quebec     

Structure of lipid bilayers

The quantitative experimental uncertainty in the structure of fully hydrated, biologically relevant, fluid (L(alpha)) phase lipid bilayers has been too large to provide a firm base for applications or for comparison with simulations. Many structural methods are reviewed including modern liquid crystallography of lipid bilayers that deals with the fully developed undulation fluctuations that occur in the L(alpha) phase. These fluctuations degrade the higher order diffraction data in a way that, if unrecognized, leads to erroneous conclusions regarding bilayer structure. Diffraction measurements at high instrumental resolution provide a measure of these fluctuations. In addition to providing better structural determination, this opens a new window on interactions between bilayers, so the experimental determination of interbilayer interaction parameters is reviewed briefly. We introduce a new structural correction based on fluctuations that has not been included in any previous studies. Updated measurements, such as for the area compressibility modulus, are used to provide adjustments to many of the literature values of structural quantities. Since the gel (L(beta)') phase is valuable as a stepping stone for obtaining fluid phase results, a brief review is given of the lower temperature phases. The uncertainty in structural results for lipid bilayers is being reduced and best current values are provided for bilayers of five lipids.     

A test of discreteness-of-charge effects in phospholipid vesicles: measurements using paramagnetic amphiphiles

A new series of negatively charged, paramagnetic alkylsulfonate probes was synthesized and can be used to measure both the internal and the external surface potentials of model membrane systems. We tested for discreteness-of-charge effects in lipid membranes by comparing the surface potentials, estimated by use of these negatively charged amphiphiles, with that of a series of positively charged alkylammonium nitroxides in charged membranes. From the partitioning of these probes, the membrane surface potential was estimated in phosphatidylcholine membranes containing either phosphatidylserine or didodecyldimethylammonium bromide. The surface potentials, estimated with either positive or negative probes, were identical, within experimental error, in either positive or negative membranes, and they were well accounted for by a simple Gouy-Chapman-Stern theory. This symmetry, with respect to the sign of the charge, indicates that discreteness-of-charge effects are not significant in determining the potential-sensitive phase partitioning of these probes in model membranes. Thus, despite the fact that charge on membranes is discrete, models that assume a uniform density of charge in the plane of the membrane adequately account for the potentials measured by these amphiphilic probes.     

Cholestryl-phosphoryl-choline in lipid bilayers.

Cholesteryl-phosphoryl-choline (CPC), a hybrid between cholesterol and lecithin, is incorporated into sonicated liposomes and erythrocyte membranes similarly to cholesterol. The effect of CPC on lipid microviscosity and degree of order is smaller, but not significantly than that of cholesterol. It is proposed that CPC may be employed as an efficient modulator of lipid dynamics.     

Under the influence of alcohol: the effect of ethanol and methanol on lipid bilayers

Extensive microscopic molecular dynamics simulations have been performed to study the effects of short-chain alcohols, methanol and ethanol, on two different fully hydrated lipid bilayer systems (POPC and DPPC) in the fluid phase at 323 K. It is found that ethanol has a stronger effect on the structural properties of the membranes. In particular, the bilayers become more fluid and permeable: ethanol molecules are able to penetrate through the membrane in typical timescales of approximately 200 ns, whereas for methanol that timescale is considerably longer, at least of the order of microseconds. A closer examination exposes a number of effects due to ethanol. Hydrogen-bonding analysis reveals that a large fraction of ethanols is involved in hydrogen bonds with lipids. This in turn is intimately coupled to the ordering of hydrocarbon chains: we find that binding to an ethanol decreases the order of the chains. We have also determined the dependence of lipid-chain ordering on ethanol concentration and found that to be nonmonotonous. Overall, we find good agreement with NMR and micropipette studies.     

Interaction of protegrin-1 with lipid bilayers: membrane thinning effect

Protegrins (PG) are important in defending host tissues, preventing infection via an attack on the membrane surface of invading microorganisms. Protegrins have powerful antibiotic abilities, but the molecular-level mechanisms underlying the interactions of their beta-sheet motifs with the membrane are not known. Protegrin-1 (PG-1) is composed of 18 amino acids with a high content of basic residues and two disulfide bonds. Here we focused on the stability of PG-1 at the amphipathic interface in lipid bilayers and on the details of the peptide-membrane interactions. We simulated all-atom models of the PG-1 monomer with explicit water and lipid bilayers composed of both homogeneous POPC (palmitoyl-oleyl-phosphatidylcholine) lipids and a mixture of POPC/POPG (palmitoyl-oleyl-phosphatidylglycerol) (4:1) lipids. We observed that local thinning of the lipid bilayers mediated by the peptide is enhanced in the lipid bilayer containing POPG, consistent with experimental results of selective membrane targeting. The beta-hairpin motif of PG-1 is conserved in both lipid settings, whereas it is highly bent in aqueous solution. The conformational dynamics of PG-1, especially the highly charged beta-hairpin turn region, are found to be mostly responsible for disturbing the membrane. Even though the eventual membrane disruption requires PG-1 oligomers, our simulations clearly show the first step of the monomeric effects. The thinning effects in the bilayer should relate to pore/channel formation in the lipid bilayer and thus be responsible for further defects in the membrane caused by oligomer.     

Permeability and the hidden area of lipid bilayers

The passive water permeability of a lipid vesicle membrane was studied, related to the hydrostatic (not osmotic) pressure difference between the inner and the outer side of the vesicle in a water environment without additives. Each pressure difference was created by sucking a vesicle into a micropipette at a given sucking pressure. The part of the membrane sucked into the micropipette (the projection length) was measured as a function of time. The time dependence can be divided into two intervals. We put forward the idea that smoothing of membrane defects, accompanied by an increase of the membrane area, takes place during the initial time interval, which results in a faster increase of the projection length. In the second time interval the volume of the vesicle decreases due to the permeability of its membrane and the increase of the projection length is slower. The hidden area and the water permeability of a typical lipid bilayer were estimated. The measured permeability, conjugated to the hydrostatic pressure difference, is an order of magnitude higher than the known value of the permeability, conjugated to the osmotic pressure difference. A hypothesis, based on pore formation, is proposed as an explanation of this experimental result.     

Structure determination of lipid bilayers

A method of determining the phases of X-ray reflections from oriented model membrane systems at low resolution is described. The method involves deconvolution and requires that d less than or equal to 2v where v is the width of the head group region within the bilayer and d is the thickness of the bilayer. The method can be used with a single set of X-ray data and applies to lipid bilayers which have a relatively constant density in the hydrocarbon region. Phases for the first five or six orders of phosphatidylethanolamine and lecithin are derived. A refined analysis based upon deconvolution but using information inherent in the Fourier profile is also described.     

The fusogenic effect of synthetic polycations on negatively charged lipid bilayers

The effect of synthetic polycations, polyallylamine, and polyethylenimine, on liposomes containing phosphatidylserine was investigated along with that of polylysine and divalent cations. The addition of polycations caused aggregation of sonicated vesicles composed of phosphatidylserine and phosphatidylcholine (molar ratio 1:4) as determined by measuring the turbidity changes. Liposomal turbidity increased 10 times compared with that of control liposomes at charge ratios of polymer/vesicle from 0.23 (polylysine) to 2.5 (linear polyethylenimine), while the turbidity was unchanged by the addition of Ca2+ or Mg2+ at charge ratios up to 500. These polycations also induced intermixing of liposomal membranes as indicated by resonance energy transfer between fluorescent lipids incorporated in lipid bilayers, without inducing drastic permeability changes as determined from the calcein release. Fifty percent intermixing of liposomes (0.05 mM as lipid concentration) was induced by these polycations at charge ratios of around 1.0. However, the highest resonance energy transfer was produced by the addition of polyallylamine, which caused multicycles of membrane intermixing between vesicles. Polycation-induced membrane intermixing and permeability changes of phosphatidylserine liposomes were also investigated. At charge ratios of around 1.0, these polymers caused resonance energy transfer of fluorescent lipids incorporated in separate vesicles; however, polyallylamine and branched polyethylenimine also caused permeability increases of liposomal membranes. Membrane intermixing and permeability changes of phosphatidylserine vesicles induced by polyallylamine were dependent on the polymer/vesicle charge ratio, and were different from those induced by Ca2+ since the latter caused half-maximal membrane intermixing or permeability change of phosphatidylserine vesicles at about 1 mM at the liposomal concentrations investigated.     

Initiation and dynamics of hemifusion in lipid bilayers

One approach to the understanding of fusion in cells and model membranes involves stalk formation and expansion of the hemifusion diaphragm. We predict theoretically the initiation of hemifusion by stalk expansion and the dynamics of mesoscopic hemifusion diaphragm expansion in the light of recent experiments and theory that suggested that hemifusion is driven by intramembrane tension far from the fusion zone. Our predictions include a square-root scaling of the hemifusion zone size on time as well as an estimate of the minimal tension for initiation of hemifusion. Whereas a minimal amount of pressure is evidently needed for stalk formation, it is not necessarily required for stalk expansion. The energy required for tension-induced fusion is much smaller than that required for pressure-driven fusion.     

Hydrocarbon chain dynamics in lipid bilayers

A model is proposed for hydrocarbon chain dynamics in lipid bilayers. In the upper and middle parts of the chain all motion occurs by concerted rotations around at least two carbon carbon bonds at a time, preserving a structural with kinks (that is gauche^±trans gauche^? conformations) as the only deviations from the all-trans chain. At the end, independent rotations around carboncarbon bonds play a larger and larger part. This gives a reasonable interpretation of deuterium NMR data.     

Diffusion in lipid bilayers containing barriers

In epithelial cells, a barrier or tight junction restricts the diffusion of lipid probes from the apical to the basolateral side of the outer membrane bilayer. This phenomenon is studied theoretically with the diffusion equation on planar and spherical surfaces. Two models for the tight junction are considered: a penetrable barrier embedded in a monolayer and an impenetrable obstacle in the outer membrane of a bilayer than must be bypassed by flip-flopping between inner and outer membranes. The rate of passing from one side of the cell to the other is calculated for each of these models under steady state conditions. The results are compared with recent fluorescent photobleaching recovery experiments. The theoretical interpretation indicates that it would be difficult to distinguish experimentally between the flip-flop case and the barrier crossing case. Assuming a flip-flop model, large differences in the magnitude of the flip-flop rates of probes are necessary to explain the experimental results as suggested by Dragsten et al. (Dragsten, P. R., R. Blumenthal, and J. S. Handler, 1981, Nature [Lond.], 294:718--722).     

Proton permeation of lipid bilayers

Proton permeation of the lipid bilayer barrier has two unique features. First, permeability coefficients measured at neutral pH ranges are six to seven orders of magnitude greater than expected from knowledge of other monovalent cations. Second, proton conductance across planar lipid bilayers varies at most by a factor of 10 when pH is varied from near 1 to near 11. Two mechanisms have been proposed to account for this anomalous behavior: proton conductance related to contaminants of lipid bilayers, and proton translocation along transient hydrogen-bonded chains (tHBC) of associated water molecules in the membrane. The weight of evidence suggests that trace contaminants may contribute to proton conductance across planar lipid membranes at certain pH ranges, but cannot account for the anomalous proton flux in liposome systems.Two new results will be reported here which were designed to test the tHBC model. These include measurements of relative proton/potassium permeability in the gramicidin channel, and plots of proton flux against the magnitude of pH gradients. (1) The relative permeabilities of protons and potassium through the gramicidin channel, which contains a single strand of hydrogenbonded water molecules, were found to differ by at least four orders of magnitude when measured at neutral pH ranges. This result demonstrates that a hydrogen-bonded chain of water molecules can provide substantial discrimination between protons and other cations. It was also possible to calculate that if approximately 7% of bilayer water was present in a transient configuration similar to that of the gramicidin channel, it could account for the measured proton flux. (2) The plot of proton conductance against pH gradient across liposome membranes was superlinear, a result that is consistent with one of three alternative tHBC models for proton conductance described by Nagle elsewhere in this volume.     

Helix-helix interactions in lipid bilayers.

Using a continuum model, we calculated the electrostatic interaction free energy between two alpha-helices in three environments: the aqueous phase, a low dielectric alkane phase, and a simple representation of a lipid bilayer. As was found in previous work, helix-helix interactions in the aqueous phase are quite weak, because of solvent screening, and slightly repulsive, because of desolvation effects that accompany helix assembly. In contrast, the interactions can be quite strong in a hypothetical alkane phase because desolvation effects are essentially nonexistent and because helix-helix interactions are not well screened. In this type of environment, the antiparallel helix orientation is strongly favored over the parallel orientation. In previous work we found that the free energy penalty associated with burying helix termini in a bilayer is quite high, which is why the termini tend to protrude into the solvent. Under these conditions the electrostatic interaction is strongly screened by solvent; indeed, it is sufficient for the termini to protrude a few angstroms from the two surfaces of the bilayer for their interaction to diminish almost completely. The effect is consistent with the classical model of the helix dipole in which the dipole moment is represented by point charges located at either terminus. Our results suggest, in agreement with previous models, that there is no significant nonspecific driving force for helix aggregation and, hence, that membrane protein folding must be driven by specific interactions such as close packing and salt-bridge and hydrogen bond formation.     

Polymer-cushioned lipid bilayers in porous alumina

Using small-angle neutron scattering (SANS) and cyclic voltammetry (CV), we show that model biological membranes can be deposited on a polymer cushion confined in highly regular porous alumina. The thicknesses of the dilute polymer cushion chemically bound to the alumina and of the supported bilayer are obtained for two polyethylene glycol cushions (PEG₅₀₀₀ and PEG₂₀₀₀₀) and for a cushion made of chains bearing a lipid anchor at their free end (DSPE-PEG₃₄₀₀). The bilayers are studied well below and well above the chain melting temperature of the lipid mixture (DMPC/DMPE: 80/20), using a coenzyme (Ubiquinone, UQ₁₀) as a redox probe for the voltammetry experiments. Analysis of the SANS form factor of the bilayers shows that the bilayer thickness can be extracted in this particular geometry. Using PEG chains grafted at a low surface density (D<2R_g), the thickness of the complete molecular construction is obtained by CV, which shows (after subtracting the bilayer thickness) that the polymer cushion thickness can be varied from 50 to 150 Å. The values obtained with three different chain lengths, are in perfect agreement with the radius derived from the Flory theory.