Interaction of plasma lipoproteins and apolipoproteins with lipid bilayer membranes

It was shown that the interaction of lipoproteins (LP) with bilayer lipid membranes (BLM) resulted in some changes in the physical-chemical properties of the membranes. Adsorption of very low and low density lipoproteins (VLDL and LDL) at concentrations of 5-8 g protein/ml increased the surface potential difference and decreased transversal elasticity module of the bilayer. LP concentrations higher than the mentioned ones increased BLM conductance and caused instability and disruption of the membranes. The same effects were revealed for high density lipoproteins (HDL) at higher concentrations--15-20 micrograms protein/ml. The effect of apolipoproteins in the interaction of LP with BLM was investigated. It is proposed that apolipoproteins and especially apo B are the main factor which affects the nonreceptor interactions of LP with the membranes.     

Interaction of glucagon with artificial lipid bilayer membranes.

The enhancement of fluorescence emission from the tryptophan residue of glucagon, the quenching of that emission with acrylamide and with 5-doxyl and 16-doxyl stearic acid, circular dichroism spectra, the release of 6-carboxyfluorescein, and polarized infrared attenuated total reflection (IR-ATR) spectra were used to study the interaction of glucagon with intact lipid vesicles and flat bilayers. Dimyristoylphosphatidylcholine bound the peptide only below the main transition temperature, thus confirming earlier results of Epand et al. (1977). However, the peptide is also bound by vesicles of unsaturated lipids above their transition temperature, suggesting an influence of lipid area on the binding process. Circular dichroism showed that binding to such vesicles also increases the helix content of glucagon. The IR-ATR study and a comparison with dynorphin-A-(1-13)-tridecapeptide revealed profound differences in orientation of the two peptides. The dichroic ratios and the derived order parameters indicated an isotropic orientation of the helical segments of glucagon, but did not exclude a principal orientation of the molecules lying flat on the membrane surface. In contrast, the axis of the dynorphin helix is clearly oriented normal to the interface. The two peptides also differ in their rates of 6-carboxyfluorescein release, suggesting a deeper penetration of the primary amphiphilic helix of dynorphin A-(1-13) than of the secondary amphiphilic helix of glucagon.     

The lipid charge density at the bilayer surface modulates the effects of melittin on membranes

The influence of melittin on two DMPA membrane systems at pH 4.2 and 8.2 has been investigated by solid-state 31P and 2H NMR, as a function of temperature and peptide concentration. Melittin promotes greater morphological changes for both systems in the fluid phase, the effect being larger at pH 4.2. Close inspection of fatty acyl chain dynamics suggests that some parallels can be drawn between the DMPA/melittin at pH 8.2 and PC/melittin systems. In addition, at pH 8.2 a direct neutralization at the interface of one of the lipid negative charges by a positive charge of the peptide occurs, as can be monitored by 31P NMR at the molecular level. For the system at pH 4.2 and at high temperature, a lipid-to-peptide molar ratio of 30 is sufficient to transform the whole system into an isotropic phase, proposed to be inverted micelles. When the system is cooled down towards the gel phase one observes an intermediate hexagonal phase in a narrow range of temperature.     

Phospholipid surface bilayers at the air-water interface. III. Relation between surface bilayer formation and lipid bilayer assembly in cell membranes.

Lipid bilayer assembly in cell membranes has been simulated with total lipid extracts from human red blood cells and from mesophilic and thermophilic bacteria grown at several temperatures. Aqueous dispersions of these natural lipid mixtures form surface bilayers, a single bimolecular lipid state, but only at the growth temperature of the source organism. Thus, a single isolated bilayer state forms spontaneously in vitro from lipids that are available in vivo at the growth temperature of the cell. Surface bilayers form at a specific temperature that is a function of hydrocarbon chain length and degree of fatty acid unsaturation of the phospholipids; this property is proposed as an essential element in the control of membrane lipid composition.     

Interaction between bending and tension forces in bilayer membranes.

A theoretical analysis is presented of the bending mechanics of a membrane consisting of two tightly-coupled leaflets, each of which shears and bends readily but strongly resists area changes. Structures of this type have been proposed to model biological membranes such as red blood cell membrane. It is shown that when such a membrane is bent, anisotropic components of resultant membrane tension (shear stresses) are induced, even when the tension in each leaflet is isotropic. The induced shear stresses increase as the square of the membrane curvature, and become significant for moderate curvatures (when the radius of curvature is much larger than the distance between the leaflets). This effect has implications for the analysis of shape and deformation of freely suspended and flowing red blood cells.     

Interaction of lipoproteins with isolated ovary plasma membranes

Plasma membranes of ovarian luteal and adrenal cortical cells from "microvillar channels," a unique extracellular compartment formed by the close apposition of flattened microvillar surfaces. Microvillar channels have unusual affinity for cholesterol-rich lipoproteins, and, in vivo, may provide an increased surface area for these particles. In this research, we have isolated a plasma membrane-enriched fraction from rat luteinized ovaries, in which closely apposed membrane (i.e. microvillar channels) comprise about 30% of the preparation. Following in vitro incubations (approximately 1 h) of this plasma membrane fraction with different plasma lipoproteins, the closely apposed plasma membrane surfaces widen and become filled with lipoprotein particles (up to about 30 nm), whereas other membranes of the fraction show little binding. Competition experiments show that rat high density lipoproteins have the highest affinity for binding to the plasma membrane fraction. Radiolabeled plasma lipoprotein and the tissue-specific hormone, human chorionic gonadotropin, showed specific and saturable binding to the plasma membrane fraction, whereas other macromolecules used as controls did not. Radioautographic analyses of 125I-labeled lipoproteins and human chorionic gonadotropin indicate that binding occurs predominantly to the closely apposed plasma membranes (i.e. microvillar channels of the fraction). These studies show that microvillar channels of steroid-secreting cells entrap large numbers of plasma lipoproteins, particularly high density lipoproteins particles, presumably functioning in the delivery of cholesterol to these cells.     

Interaction between surface shape and intra-surface viscous flow on lipid membranes

The theory of intra-surface viscous flow on lipid bilayers is developed by combining the equations for flow on a curved surface with those that describe the elastic resistance of the bilayer to flexure. The model is derived directly from balance laws and augments an alternative formulation based on a variational principle. Conditions holding along an edge of the membrane are emphasized, and the coupling between flow and membrane shape is simulated numerically.     

Interaction of botulinum and tetanus toxins with the lipid bilayer surface.

The interaction of botulinum neurotoxins serotypes A, B and E (from Clostridium botulinum) and of tetanus neurotoxin (from Clostridium tetani) with the surface of liposomes made of different lipid compositions was studied by photolabelling with a radioiodinated photoactive phosphatidylethanolamine analogue [125I-dipalmitoyl (3,4-azidosalicylamido)phosphatidylethanolamine]. When the vesicles were made of negatively charged lipids (asolectin), each of these neurotoxic proteins was radioiodinated, thus providing evidence for their attachment to the membrane surface. The presence of gangliosides on liposome membranes enhanced fixation of the neurotoxic proteins to the lipid vesicle surface. Both the heavy and light chains of the clostridial neurotoxins were involved in the attachment to the lipid bilayer surface. Each of the toxins tested here attached poorly to liposomes made of zwitterionic lipids (egg phosphatidylcholine), even when polysialogangliosides were present. The data suggest that the binding of botulinum and tetanus neurotoxins to their target neuronal cells involves negatively charged lipids and polysialogangliosides on the cell membrane.     

Intermonolayer friction and surface shear viscosity of lipid bilayer membranes

The flow behavior of lipid bilayer membranes is characterized by a surface viscosity for in-plane shear deformations, and an intermonolayer friction coefficient for slip between the two leaflets of the bilayer. Both properties have been studied for a variety of coarse-grained double-tailed model lipids, using equilibrium and nonequilibrium molecular dynamics simulations. For lipids with two identical tails, the surface shear viscosity rises rapidly with tail length, while the intermonolayer friction coefficient is less sensitive to the tail length. Interdigitation of lipid tails across the bilayer midsurface, as observed for lipids with two distinct tails, strongly enhances the intermonolayer friction coefficient, but hardly affects the surface shear viscosity. The simulation results are compared against the available experimental data.     

The structure of melittin in lipid bilayer membranes.

0.15 M inorganic phosphate dramatically increased the alpha-helix content of melittin in aqueous solution. When melittin interacted with egg yolk phosphatidylcholine liposomes in the absence of inorganic phosphate, it was converted to an alpha-helix rich form, as postulated by Dawson et al. (Dawson, C.R., Drake, A.F. Helliwell, J. and Hider, R.C. (1978) Biochim. Biophys. Acta 510, 75--86).     

The relationship between permeant size and permeability in lipid bilayer membranes

Permeability coefficients (P _m ) across planar egg lecithin/decane bilayers and bulk hydrocarbon/water partition coefficients (K _whc) have been measured for 24 solutes with molecular volumes, V, varying by a factor of 22 and P _m values varying by a factor of 10⁷ to explore the chemical nature of the bilayer barrier and the effects of permeant size on permeability. A proper bulk solvent which correctly mimics the microenvironment of the barrier domain was sought. Changes in P _m /K_whc were then ascribed to size-dependent partitioning and/or size-dependent diffusivity. The diffusion coefficient-size dependency was described by D _barrier = D ₀ /V ⁿ . When n-decane was used as a reference solvent, the correlation between log P _m /K _whc and log V was poor (r = 0.56) with most of the lipophilic (hydrophilic) permeants lying below (above) the regression line. Correlations improved significantly (r = 0.87 and 0.90, respectively) with more polarizable solvents, 1-hexadecene and 1,9-decadiene. Values of the size selectivity parameter n were sensitive to the reference solvent (n = 0.8 ± 0.3, 1.2 ± 0.1 and 1.4 ± 0.2, respectively, for decane, hexadecene, and decadiene). Decadiene was selected as the most suitable reference solvent. The value for n in bilayer transport is higher than that for bulk diffusion in decane (n = 0.74±0.10), confirming the steep dependence of bilayer permeability on molecular size. Statistical mechanical theory recently developed by the authors suggests that a component of this steep size dependence may reside in size-dependent solute partitioning into the ordered chain region of bilayers. This theory, combined with the above diffusion model, yielded the relationship, P _m /K _Whc=D ₀ exp(V)V ⁿ . A fit of the experimental data to this model gave the best fit (r=0.93) with = 0.0053±0.0021 and n=0.8 ± 0.3, suggesting that both diffusion and partitioning mechanisms may play a role in determining the size dependence of lipid bilayer permeabilities.This work was supported by a research grant from Glaxo, Inc. Instrumentation support was provided by a Biomedical Research Support Grant from the College of Pharmacy, University of Utah, and by a Faculty Research Grant from the University of Utah. The technical assistance of Barbara L. Hoesterey, who determined some of the partition coefficients, is gratefully acknowledged.     

The influence of charge on phosphatidic acid bilayer membranes.

A complete titration of phosphatidic acid bilayer membranes was possible for the first time by the introduction of a new anaologue, 1,2-dihexadecyl-sn-glycerol-3-phosphoric acid, which has the advantage of a high chemical stability at extreme pH values. The synthesis of the phosphatidic acid is described and the phase transition behaviour in aqueous dispersions is compared with that of three ester phosphatidic acids; 1,2-dimyristoyl-sn-glycerol-3-phosphoric acid, 1,3-dimyristoylglycerol-2-phosphoric acid and 1,2-dipalmitoyl-sn-glycerol-3-phosphoric acid. The phase transition temperatures (Tt) of aqueous phosphatidic acid dispersions at different degrees of dissociation were measured using fluorescence spectroscopy and 90 degrees light scattering. The Tt values are comparable to the melting points of the solid phosphatidic acids in the fully protonated states, but large differences exist for the charged states. The Tt vs. pH diagrams of the four phosphatidic acids are quite similar and of a characteristic shape. Increasing ionisation results in a maximum value for the transition temperatures at pH 3.5 (pK1). The regions between the first and the second pK of the phosphatidic acids are characterised by only small variations in the transition temperatures (extended plateau) in spite of the large changes occurring in the surface charge of the membranes. The slope of the plateau is very shallow with increasing ionisation. A further decrease in the H+ concentration results in an abrupt change of the transition temperature. The slope of the Tt vs. pH diagram beyond pK2 becomes very steep. This is the result of reduced hydrocarbon interaction energy, which was demonstrated by differential scanning calorimetry (Blume, A. and Eibl, H., unpublished data).     

Interaction of smooth muscle plasma membranes with flat lipid membranes

The method of implantation of smooth muscle cells from plasma membranes (PM) of the rabbit intestine into flat lipid membranes (FLM) is described. The method is based on the pretreatment of PM vesicles with asolectin liposomes in the ratio that provides the activation of membrane ATPases. Thus modified FLM possesses channel conductivity.     

Ionic transport in lipid bilayer membranes.

The current-voltage relationships of model bilayer membranes have been measured in various phospholipid systems, under the influence of both a gradient of potential and an ionic concentration, in order to describe the ion translocation through hydrated transient defects (water channels) across the bilayer formed because of lipid structure fluctuations and induced by temperature. The results have been analyzed in the light of a statistical rate theory for the transport process across a lipid bilayer, recently proposed by Skinner et al. (1993). In order to take into account the observed I-V curves and in particular the deviation from an ohmic behavior observed at high potential values, the original model has been modified, and a new version has been proposed by introducing an additional kinetic process. In this way, a very good agreement with the experimental values has been obtained for all of the systems we have investigated (dimyristoylphosphatidyl ethanolamine bilayers and mixed systems composed by dimyristoylphosphatidyl ethanolamine/dimyristoylphosphatidylcholine mixtures and dimyristoylphosphatidyl ethanolamine/phosphatidic acid dipalmitoyl mixtures). The rate constants governing the reactions at the bilayer interfaces have been evaluated for K+ and Cl- ions, as a function of temperature, from 5 to 35 degrees C and bulk ionic concentrations from 0.02 to 0.2 M. Finally, a comparison between the original model of Skinner and the modified version is presented, and the advantages of this new formulation are briefly discussed.     

Non-electrolyte permeability through black lipid membranes with different surface charge.

The permeability coefficients of some non-electrolytes has been measured across black lipid membranes of different composition. Large discrepancies between permeability coefficients and oil-water partition coefficients has been observed. The discrepancy level seems to be related to the degree of organization of the membrane.     

The movement of ion pairs across bilayer lipid membranes.

If a polyhalide concentration gradient exists across a bilayer lipid membrane (BLM), ion pair movement occurs. The term ion pair indicates a lipid soluble complex of cation and anion with stoichiometry dictated by the respective charges. In a mixture of metal halide (MX_n, X = I, Cl, Br) and iodine, the ion pair is of the form M(I₂X)_n. The flux of ion pairs was monitored by measuring the flow of metal ions or polyhalide ions across the BLM. The flux of ion pairs across the BLM depended on cation crystal radius, fluidity of the membrane, strength of the ion pair complex and on the osmotic gradient (i.e., there exists a coupling between water and ion pair fluxes). The relationship between ion pairing and the electrical conductivity of BLM is briefly discussed.