Thermal transitions of DMPG bilayers in aqueous solution: SAXS structural studies

Dimyristoylphosphatidylglycerol (DMPG) has been extensively studied as a model for biological membranes, since phosphatidylglycerol is the most abundant anionic phospholipid in prokaryotic cells. At low ionic strengths, this lipid presents a peculiar thermal behavior, with two sharp changes in the light scattering profile, at temperatures named here T(on)(m) and T(off)(m). Structural changes involved in the DMPG thermal transitions are here investigated by small angle X-ray scattering (SAXS), and compared to the results yielded by differential scanning calorimetry (DSC) and electron spin resonance (ESR). The SAXS results show a broad peak, indicating that DMPG is organized in single bilayers, for the range of temperature studied (10-45 degrees C). SAXS intensity shows an unusual effect, starting to decrease at T(on)(m), and presenting a sharp increase at T(off)(m). The bilayer electron density profiles, obtained from modeling the SAXS curves, show a gradual decrease in electron density contrast (attributed to separation between charged head groups) and in bilayer thickness between T(on)(m) and T(off)(m). Results yielded by SAXS, DSC and ESR indicate that a chain melting process starts at T(on)(m), but a complete fluid phase exists only for temperatures above T(off)(m), with structural changes occurring at the bilayer level in the intermediate region.     

Preparation and structural studies of cholesterol bilayers

Bilayers consisting, in their hydrophobic core, entirely of cholesterol can be constructed if a hydrophilic molecular anchor is supplied. $\text{O-}\text{Methoxyethoxyethoxyethylcholesterol}$ and cholesterol sulfate form multilayered liposomes in water. With equimolar cholesterol added, cholesterol sulfate, cholesterolphosphocholine, and $\text{O-}\text{methoxyethoxyethoxyethylcholesterol}$ form small unilamellar liposomes on prolonged sonication. The dimensions of cholesterol-cholesterolphosphocholine vesicles are comparable to those of phospholipid vesicles. ¹³C-NMR spectra suggest that the centers of the bilayers are liquid. The permeability of the cholesterol-cholesterolphosphocholine bilayer against glycerol is lower than that of dipalmitoylphosphatidylcholine-cholesterol bilayer; the activation energy of permeation is two times larger, an indication of a higher degree of structural organization in the ‘hydrogen belts’ of the cholesterol-cholesterolphosphocholine bilayer.     

Interaction of small peptides with lipid bilayers.

Molecular dynamics simulations of the tripeptide Ala-Phe-Ala-O-tert-butyl interacting with dimyristoylphosphatidylcholine lipid bilayers have been carried out. The lipid and aqueous environments of the peptide, the alkyl chain order, and the lipid and peptide dynamics have been investigated with use of density profiles, radial distribution functions, alkyl chain order parameter profiles, and time correlation functions. It appears that the alkyl chain region accommodates the peptides in the bilayer with minimal perturbation to this region. The peptide dynamics in the bilayer bound form has been compared with that of the free peptide in water. The peptide structure does not vary on the simulation time scale (of the order of hundreds of picoseconds) compared with the solution structure in which a random structure is observed.     

Interaction of vasopressin with phosphatidylserine bilayers

Vasopressin causes a decrease in electrical resistance of phosphatidylserine bilayers. The magnitude of the decrease is a function of vasopressin and salt concentrations. The conducting channel is produced probably by aggregation of 4–5 molecules of the hormone.     

Interaction of bilayers with basic polypeptides

Summary The interaction of bilayers formed from glyceryl monooleate+oleic acid with basic polypeptides was studied. Copolymers of lysine with different amino acids interact with the bilayers reducing their resistance and increasing their capacitance.The largest effect was observed with the copolymerl-lysine/l-phenylalanine (1.41) which decreases the specific resistance by more than 3 orders of magnitude. The smallest effects on the resistance were obtained with the very hydrophilic copolymer ofl-lysine/l-serine (1.11). The contribution of the double-layer potential to the measured transmembrane potentials of the charged bilayers is considered and calculated for the case of the membrane containing dissociable components in the absence of interacting copolymers.     

Interaction of phosphatidylserine synthase from E. coli with lipid bilayers: coupled plasmon-waveguide resonance spectroscopy studies

The interaction of phosphatidylserine (PS) synthase from Escherichia coli with lipid membranes was studied with a recently developed variant of the surface plasmon resonance technique, referred to as coupled plasmon-waveguide resonance spectroscopy. The features of the new technique are increased sensitivity and spectral resolution, and a unique ability to directly measure the structural anisotropy of lipid and proteolipid films. Solid-supported lipid bilayers with the following compositions were used: 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC); POPC-1-palmitoyl-2-oleoyl-sn-glycero-3-phosphate (POPA) (80:20, mol/mol); POPC-POPA (60:40, mol/mol); and POPC-1-palmitoyl-2-oleoyl-sn-glycero-3-[phospho-rac-(1-glycerol)] (POPG) (75:25, mol/mol). Addition of either POPA or POPG to a POPC bilayer causes a considerable increase of both the bilayer thickness and its optical anisotropy. PS synthase exhibits a biphasic interaction with the bilayers. The first phase, occurring at low protein concentrations, involves both electrostatic and hydrophobic interactions, although it is dominated by the latter, and the enzyme causes a local decrease of the ordering of the lipid molecules. The second phase, occurring at high protein concentrations, is predominantly controlled by electrostatic interactions, and results in a cooperative binding of the enzyme to the membrane surface. Addition of the anionic lipids to a POPC bilayer causes a 5- to 15-fold decrease in the protein concentration at which the first binding phase occurs. The results reported herein lend experimental support to a previously suggested mechanism for the regulation of the polar head group composition in E. coli membranes.     

Interaction of fatty acids with lipid bilayers

We present a method by which it is possible to describe the binding of fatty acids to phospholipid bilayers. Binding constants for oleic acid and a number of fatty acids used as spectroscopic probes are deduced from electrophoresis measurements. There is a large shift in $\text{p}\text{K}$ value for the fatty acids on binding to the phospholipid bilayers, consistent with stronger binding of the uncharged form of the fatty acid. For dansylundecanoic acid, fluorescence titrations are consistent with the binding constants derived from the electrophoresis experiments. For 12-(9-anthroyloxy)stearic acid, fluorescence and electrophoresis data are inconsistent, and we attribute this to quenching of fluorescence at high molar ratios of 12-anthroylstearic acid to phospholipid in the bilayer.     

Interaction of fluorescently labeled pardaxin and its analogues with lipid bilayers.

Fluorescence measurements were used to monitor the interaction of the neurotoxin pardaxin and its analogues with membranes. Eight peptides were selectively labeled with the fluorophore 7-nitrobenz-2-oxa-1,3-diazole-4-yl, either at their N-terminal or at their C-terminal. No detectable changes in membrane permeability or hemolytic activity were observed upon modification. Upon the titration of solutions containing the different peptides with small unilamellar vesicles, the fluorescent emission spectra of 7-nitrobenz-2-oxa-1,3-diazole-4-yl-labeled pardaxin and its analogues, but not those of control peptides, displayed blue shifts in addition to enhanced intensities upon relocation of the probe to a more apolar environment. The results revealed that the N terminus of pardaxin is buried within the lipid bilayer while the C terminus is located at the bilayer's surface. Binding isotherms were obtained from the observed increases in the fluorescence emission yields, from which surface partition constants, in the range of 10(4) M-1, were in turn derived. The existence of an aggregation process was suggested by the shape of the binding isotherms. Furthermore, the results show good correlation between the incidence of aggregation and the ability of the different analogues to induce the release of relatively large molecules from vesicles. As such, our results suggest that the mechanism of pore formation employed by pardaxin and its analogues could be described by the "barrel stave" model.     

Interaction of lysophosphatidylcholine with phosphatidylcholine bilayers. A photo-physical and NMR study

Several photo-physical methods together with ³¹P-NMR have been used to investigate the effect of lysophosphatidylcholine on phosphatidylcholine bilayers. ³¹P-NMR shows that the permeability of the vesicle to Eu³⁺ increases sharply above approx. 40% lysophosphatidylcholine: fluorescence-quenching studies also show this type of behavior. Similar sharp changes in vesicle properties are observed via the photo-physical technique at this lysophosphatidylcholine/phosphatidylcholine composition. Fluorescence spectra of pyrene and pyrene carboxaldehyde show that increasing lysophosphatidylcholine composition increases the polarity of the environments of these probes up to 40% lysocompound. Above this composition the photo-physical properties of the probes slowly revert to those characteristic of the micellar lyso-compound. The pyrene fluorescence lifetime, the fine structure of the fluorescence, and the case of formation of pyrene excimer in these bilayer mixtures suggest that pyrene complexes weakly with the charged nitrogen of the choline group of the phosphatidylcholine and that the physical state of the system has a striking effect on this complexation process. Similar experiments with simple quaternary compounds lend strong support to this suggestion. The studies monitor in several ways the effect of bilayer composition on movement of molecules in these systems. The degree or site of solubilization of carcinogens is also uniquely affected by composition.     

Interaction of lysophospholipid/taurodeoxycholate submicellar aggregates with phospholipid bilayers.

The equilibrium partitioning and the rate of transfer of monoacylphosphatidylethanolamines (lysoPEs) between phospholipid bilayers and lysoPE/taurodeoxycholate submicellar aggregates (SMAs) were examined with a series of environment-sensitive fluorescent-labeled N-(7-nitro-2,1,3-benzoxadiazol-4-yl)-1-monoacylphosphatidyletha nolamine (N-NBD-lysoPE) probes of differing acyl chain length. Our previous work has demonstrated the formation of SMAs between bile salts and lysophospholipids [Shoemaker & Nichols (1990) Biochemistry 29, 5837-5842]. The experiments in the current work demonstrate that SMAs can coexist with phospholipid vesicles and can function as shuttle carriers for the transfer of lysophospholipids between membranes. The formation of submicellar aggregates of N-NBD-lysoPE and taurodeoxycholate (TDC) in equilibrium with 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) vesicles was determined from the increase in fluorescence generated upon addition of TDC to POPC vesicles containing 3 mol% N-NBD-lysoPE and 3 mol% N-(lissamine rhodamine B sulfonyl)dioleoylphosphatidylethanolamine (N-Rh-PE) as a nonextractable fluorescence energy-transfer quencher. The fraction of lysolipid extracted increased as a function of decreasing acyl chain length of the N-NBD-lysoPE molecule. The half-time for equilibration was independent of acyl chain length and averaged 44 ms at 10 degrees C. The delivery of N-NBD-lysoPE from preformed N-NBD-lysoPE/TDC SMAs into POPC vesicles containing the energy-transfer quencher N-Rh-PE was measured by the rate of fluorescence decline. The initial rate of insertion increased with decreasing acyl chain length of the N-NBD-lysoPE molecule and as a function of vesicle concentration.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interaction of dolichol and dolichyl phosphate with phospholipid bilayers

The thermotropic phase transition of dipalmitoylphosphatidylcholine vesicles reconstituted with dolichol or dolichyl phosphate was investigated as a function of the lipid-to-polyisoprenoid ratio by means of differential scanning calorimetry and fluorescence depolarization of the embedded probe 1,6-diphenyl-1,3,5-hexatriene. At the concentrations studied, dolichol and dolichyl phosphate lowered and broadened the transition temperature of dipalmitoylphosphatidylcholine bilayers. Dolichol was found to increase the motional freedom of the bilayer both below and above the transition temperature as determined by fluorescence depolarization. In contrast, low concentrations of dolichyl phosphate decreased the bilayer motional freedom below the transition temperature while high concentrations increased the motional freedom. Above the transition temperature, dolichyl phosphate decreased bilayer 'fluidity' at all concentrations. The data suggest that these polyisoprenoids perturb the bilayer lattice, with the neutral species dolichol increasing membrane 'fluidity', while dolichyl phosphate acts to 'stiffen' the membrane.     

Interaction of salt with ether- and ester-linked phospholipid bilayers

A distinguishing feature of Archaeal plasma membranes is that their phospholipids contain ether-links, as opposed to bacterial and eukaryotic plasma membranes where phospholipids primarily contain ester-links. Experiments show that this chemical difference in headgroup-tail linkage does produce distinct differences in model bilayer properties. Here we examine the effects of salt on bilayer structure in the case of an ether-linked lipid bilayer. We use molecular dynamics simulations and compare equilibrium properties of two model lipid bilayers in NaCl salt solution – POPC and its ether-linked analog that we refer to as HOPC. We make the following key observations. The headgroup region of HOPC “adsorbs” fewer ions compared to the headgroup region of POPC. Consistent with this, we note that the Debye screening length in the HOPC system is ∼ 10% shorter than that in the POPC system. Herein, we introduce a protocol to identify the lipid-water interfacial boundary that reproduces the bulk salt distribution consistent with Gouy-Chapman theory. We also note that the HOPC bilayer has excess solvent in the headgroup region when compared to POPC, coinciding with a trough in the electrostatic potential. Waters in this region have longer autocorrelation times and smaller lateral diffusion rates compared to the corresponding region in the POPC bilayer, suggesting that the waters in HOPC are more strongly coordinated to the lipid headgroups. Furthermore, we note that it is this region of tightly coordinated waters in the HOPC system that has a lower density of Na⁺ ions. Based on these observations we conclude that an ether-linked lipid bilayer has a lower binding affinity for Na⁺ compared to an ester-linked lipid bilayer.     

riDOM,a cell penetrating peptide. Interaction with phospholipid bilayers

Melittin is an amphipathic peptide which has received much attention as a model peptide for peptide–membrane interactions. It is however not suited as a transfection agent due to its cytolytic and toxicological effects. Retro-inverso-melittin, when covalently linked to the lipid 1,2-dioleoyl-sn-glycero-3-phosphoethanolamine (riDOM), eliminates these shortcomings. The interaction of riDOM with phospholipid membranes was investigated with circular dichroism (CD) spectroscopy, dynamic light scattering, ζ-potential measurements, and high-sensitivity isothermal titration calorimetry. riDOM forms cationic nanoparticles with a diameter of ~ 13 nm which are well soluble in water and bind with high affinity to DNA and lipid membranes. When dissolved in bilayer membranes, riDOM nanoparticles dissociate and form transient pores. riDOM-induced membrane leakiness is however much reduced compared to that of authentic melittin. The secondary structure of the ri-melittin is not changed when riDOM is transferred from water to the membrane and displays a large fraction of β-structure. The ³¹P NMR spectrum of the nanoparticle is however transformed into a typical bilayer spectrum. The Gibbs free energy of riDOM binding to bilayer membranes is − 8.0 to − 10.0 kcal/mol which corresponds to the partition energy of just one fatty acyl chain. Half of the hydrophobic surface of the riDOM lipid extension with its 2 oleic acyl chains is therefore involved in a lipid–peptide interaction. This packing arrangement guarantees a good solubility of riDOM both in the aqueous and in the membrane phase. The membrane binding enthalpy is small and riDOM binding is thus entropy-driven.     

X-ray diffraction studies of lecithin bilayers.

Counting the individuals in a population before and after an annual period of environmental stress allows the proportion s of the initial population surviving the period to be computed. A series of such observations over n annual periods gives a sequence s₁, s₂, …, s_n. A statistical model is formulated from axioms describing the survival process, and it is concluded that these observed values may usefully be regarded as realizations of a random variable that arises from the normal generated distribution (n.g.d.). Equations for estimating the n.g.d. parameters ζ and τ² from observed survival proportions by the method of moments and maximum likelihood are given. The distributions of parameter estimates ζ and τ² are obtained and discussed in the context of testing hypotheses comparing survival among different populations. Finally, the dependence of the n.g.d. upon parameters ζ and τ² is examined in terms of altering survival, either by population self-regulation mechanisms or man-induced controls. The intent is to provide insight into the relationship between the n.g.d. and its supporting axioms and, more generally, basic knowledge of population processes.     

Structural studies of polymer-cushioned lipid bilayers.

The structure of softly supported polymer-cushioned lipid bilayers, prepared in two different ways at the quartz-solution interface, were determined using neutron reflectometry. The polymer cushion consisted of a thin layer of branched, cationic polyethyleneimine (PEI), and the bilayers were formed by adsorption of small unilamellar dimyristoylphosphatidylcholine (DMPC) vesicles. When vesicles were first allowed to adsorb to a bare quartz substrate, an almost perfect bilayer formed. When the polymer was then added to the aqueous solution, it appeared to diffuse beneath this bilayer, effectively lifting it from the substrate. In contrast, if the polymer layer is adsorbed first to the bare quartz substrate followed by addition of vesicles to the solution, there is very little interaction of the vesicles with the polymer layer, and the result is a complex structure most likely consisting of patchy multilayers or adsorbed vesicles.     

Thermal, dynamic and structural properties of drug AT1 antagonist olmesartan in lipid bilayers

It is proposed that AT1 antagonists (ARBs) exert their biological action by inserting into the lipid membrane and then diffuse to the active site of AT1 receptor. Thus, lipid bilayers are expected to be actively involved and play a critical role in drug action. For this reason, the thermal, dynamic and structural effects of olmesartan alone and together with cholesterol were studied using differential scanning calorimetry (DSC), 13C magic-angle spinning (MAS) nuclear magnetic resonance (NMR), cross-polarization (CP) MAS NMR, and Raman spectroscopy as well as small- and wide angle X-ray scattering (SAXS and WAXS) on dipalmitoyl-phosphatidylcholine (DPPC) multilamellar vesicles. 13C CP/MAS spectra provided direct evidence for the incorporation of olmesartan and cholesterol in lipid bilayers. Raman and X-ray data revealed how both molecules modify the bilayer's properties. Olmesartan locates itself at the head-group region and upper segment of the lipid bilayers as 13C CP/MAS spectra show that its presence causes significant chemical shift changes mainly in the A ring of the steroidal part of cholesterol. The influence of olmesartan on DPPC/cholesterol bilayers is less pronounced. Although, olmesartan and cholesterol are residing at the same region of the lipid bilayers, due to their different sizes, display distinct impacts on the bilayer's properties. Cholesterol broadens significantly the main transition, abolishes the pre-transition, and decreases the membrane fluidity above the main transition. Olmesartan is the only so far studied ARB that increases the gauche:trans ratio in the liquid crystalline phase. These significant differences of olmesartan may in part explain its distinct pharmacological profile.