Structural organization of DMPC lipid layers on chemically micropatterned self-assembled monolayers as biomimetic systems

The growth structure of DMPC lipid layers on hydrophobic and hydrophilic alkylsilane-based self-assembled monolayers adsorbed on silicon has been investigated by means of X-ray reflectometry and atomic force microscopy. Hydrophilic modification of hydrophobically terminated ODS-SAMs has been achieved by dose-controlled irradiation with DUV light. While island formation of small DMPC bilayer islands is observed on hydrophobic SAM surfaces, closed layers of DMPC monolayers are formed on hydrophilic SAM surfaces. Furthermore, DMPC adsorption on chemically micropatterned substrates with alternating hydrophobic/hydrophilic surface properties has been studied by imaging ellipsometry and photoemission microscopy. Indication for at least partial bridging of hydrophobic areas by an adsorbed DMPC monolayer has been found.     

Donnan potential and surface potential of a charged membrane.

A model is presented for the electrical potential distribution across a charged biological membrane that is in equilibrium with an electrolyte solution. We assume that a membrane has charged surface layers of thickness d on both surfaces of the membrane, where the fixed charges are distributed at a uniform density N within the layers, and that these charged layers are permeable to electrolyte ions. This model unites two different concepts, that is, the Donnan potential and the surface potential (or the Gouy-Chapman double-layer potential). Namely, the present model leads to the Donnan potential when d much greater than 1/k' (k' is the Debye-Hückel parameter of the surface charge layer) and to the surface potential as d----0, keeping the product Nd constant. The potential distribution depends significantly on the thickness d of the surface charge layer when d less than or approximately equal to 1/k'.     

Structure and activity of lipid membrane biosensor surfaces studied with atomic force microscopy and a resonant mirror.

Three variants of the liposome fusion (coalescence) method to produce supported lipid bilayers, containing the ganglioside GM1 on silicon nitride surfaces, were studied. The first procedure involved attachment and fusion of liposomes containing DMPC, GM1 and a small amount of biotinylated lipid (Biotin-LC-DPPE) to a streptavidin coated surface. Direct fusion of liposomes composed of a mixture of DPPC, DPPG, DPPE, GM1 and cholesterol to the surface were the second variant. The final method utilised the second type of liposomes, fused onto a streptavidin layer with a small amount of exposed hydrophobic tails. The methods produced similar lipid layers, but with different ways of attachment to the surface. The binding of cholera toxin B-subunit (CTB) towards these sensor surfaces was measured in a resonant mirror biosensor instrument and the activity and longer-term stability of the layers were examined. The prepared surfaces were also imaged by atomic force microscopy (AFM) in liquid to characterise the topography of the lipid layers. The binding efficiency of CTB towards these surfaces was discussed in terms of lipid fluidity and surface roughness.     

A comparison of DMPC- and DLPE-based lipid bilayers.

A 250 ps molecular dynamics simulation of the dimyristoylphosphatidylcholine (DMPC)-based lipid bilayer, including explicit water molecules, is reported. The solvent environment of the head groups and other structural properties of the bilayer have been analyzed and compared with experimental results as well as our previous simulation of the dilauroylphosphatidylethanolamine (DLPE)-based bilayer. From this comparison we find that the solvent structure around the DMPC head group (clathrate shell) is significantly different than that around the DLPE head group (typical hydrogen bonding interactions). We have modeled the probable relationship between the different solvent environments around the R-N(CH3)3+ (DMPC) and R-NH3+ (DLPE) head groups and the different interlammelar distances in these systems by performing potential of mean force (PMF) simulations on two N(CH3)4+ and NH4+ ions in water. From the PMF simulations it appears that the differences in the hydration of the DMPC and DLPE head groups is not responsible for the differences in the hydration force observed for these systems. We also find that the orientational polarization of DLPE and DMPC is similar, which suggests that solvent polarization is not responsible for the differences in the hydration repulsion behavior observed in these systems. We also examined the order parameters for DMPC and found them to be in reasonable agreement with experiment. Given the different characteristics of the DLPE and DMPC head groups, we suggest an explanation of the differences in the interlammellar spacings of bilayers composed of these like-charged lipids. From our DLPE simulations we find that the R-NH3+ head groups can interact with the nonesterified oxygens of the phosphate group in an intraleaflet or an interleaflet manner. For the latter a "cross link" between two leaflets can be formed, which causes a stabilization of the interlamellar spacings at fairly short distances. Moreover, due to the strong intraleaflet interaction we find that the DLPE interface is relatively "flat" (as opposed to DMPC-based bilayers), which results in a surface that has regions of positive and negative charge that reside in the same plane along the bilayer normal. Based on this we propose that the DLPE bilayer interface can correlate itself with another DLPE interface by alignment of the regions of positive (or negative) charge on one leaflet with the opposite charges on the opposing leaflet.     

Investigation of phospholipid area compression induced by calcium-mediated dextran sulfate interaction.

The association of anionic polyelectrolytes such as dextran sulfate (DS) to zwitterionic phospholipid surfaces via Ca(2+) bridges results in a perturbation of lipid packing at physiologically relevant Ca(2+) concentrations. Lipid area compression was investigated in 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) multilamellar bilayer dispersions by (2)H-NMR and in monolayer studies. Binding of DS to DMPC surfaces via Ca(2+) results in denser lipid packing, as indicated by higher lipid chain order. DMPC order parameters are homogeneously increased throughout the lipid bilayer. Higher order translates into more extended hydrocarbon chains and decreased average lipid area per molecule. Area compression is reported as a function of DS concentration and molecular weight. Altering the NaCl and Ca(2+) concentrations modified electrostatic interactions between DS and phospholipid. A maximal area reduction of DeltaA = 2.7 A(2) per DMPC molecule is observed. The lipid main-phase transition temperature increases upon formation of DMPC/Ca(2+)/DS-complexes. Lipid area compression after addition of DS and Ca(2+) to the subphase was also observed in monolayer experiments. A decrease in surface tension of up to 3.5 mN/m at constant molecular area was observed. DS binds to the lipid headgroups by formation of Ca(2+) bridges without penetrating the hydrophobic region. We suggest that area compression is the result of an attractive electrostatic interaction between neighboring lipid molecules induced by high local Ca(2+) concentration due to the presence of DS. X-ray diffraction experiments demonstrate that DS binding to apposing bilayers reduces bilayer separation. We speculate that DS binding alters the phase state of low-density lipoproteins that associate with polyelectrolytes of the arterial connective tissue in the early stages of arteriosclerosis.     

Reconstitution of transferrin receptor in mixed lipid vesicles. An example of the role of elastic and electrostatic forces for protein/lipid assembly

We studied the interaction of transferrin receptors (of cell line Molt-4) with mixed model membranes as a function of lipid chain length (phospholipids with C14:0 and C18:1 hydrocarbon chains) and of the surface charge of the membrane using mixtures of C14:0 lecithin (DMPC) with C14:0 phosphatidylglycerol (DMPG) and C14:0 phosphatidylserine (DMPS). Spontaneous self-assembly of receptors and lipids was achieved by freeze-thaw cycles of a codispersion of mixed vesicles and receptors in buffer and subsequent separation of receptor-loaded and receptor-free vesicles by density gradient centrifugation. Information on specific lipid/protein interaction mechanisms was obtained by evaluation of protein-induced shifts of phase boundaries of lipid mixtures by calorimetry and by FTIR spectroscopy of partially deuterated lipid mixtures. The important role (1) of minimizing the elastic forces caused by the mismatch of the lengths of hydrophobic cores of the protein (lp) and the bilayer (lL) and (2) of the electrostatic coupling of protein head groups with the charged membrane/water interface for the lipid/protein self-assembly is established. The electrostatic interaction energy per receptor is about 10(3) kBT (by coupling to about 1000 charged lipids) which is sufficient to overcompensate the elastic energy associated with a mismatch of lp - lL approximately 1.0 nm. The maximum receptor concentration incorporated was measured as a function of membrane surface charge and lipid chain length. The maximum receptor molar fraction varied from xpmax = 5 x 10(-5) for DMPC to xpmax = 4 x 10(-4) for 1:1 DMPC/DMPG; moreover xpmax is higher for DMPS than for DMPG as charged component. For the long-chain lipids, xpmax is higher for a 9:1 DEPE/DEPC mixture [(4.2-9) x 10(-4)] than for pure DEPC (ca. 3.5 x 10(-4)). By decomposition of reconstituted receptors with proteases, we demonstrated the homogeneous orientation of the receptor with its extracellular head group pointing to the convex side of the vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of Lipid Head Groups on Double-Layered Two-Dimensional Crystals Formed by Aquaporin-0

Aquaporin-0 (AQP0) is a lens-specific water channel that also forms membrane junctions. Reconstitution of AQP0 with dimyristoyl phosphatidylcholine (DMPC) and E. coli polar lipids (EPL) yielded well-ordered, double-layered two-dimensional (2D) crystals that allowed electron crystallographic structure determination of the AQP0-mediated membrane junction. The interacting tetramers in the two crystalline layers are exactly in register, resulting in crystals with p422 symmetry. The high-resolution density maps also allowed modeling of the annular lipids surrounding the tetramers. Comparison of the DMPC and EPL bilayers suggested that the lipid head groups do not play an important role in the interaction of annular lipids with AQP0. We now reconstituted AQP0 with the anionic lipid dimyristoyl phosphatidylglycerol (DMPG), which yielded a mixture of 2D crystals with different symmetries. The different crystal symmetries result from shifts between the two crystalline layers, suggesting that the negatively charged PG head group destabilizes the interaction between the extracellular AQP0 surfaces. Reconstitution of AQP0 with dimyristoyl phosphatidylserine (DMPS), another anionic lipid, yielded crystals that had the usual p422 symmetry, but the crystals showed a pH-dependent tendency to stack through their cytoplasmic surfaces. Finally, AQP0 failed to reconstitute into membranes that were composed of more than 40% dimyristoyl phosphatidic acid (DMPA). Hence, although DMPG, DMPS, and DMPA are all negatively charged lipids, they have very different effects on AQP0 2D crystals, illustrating the importance of the specific lipid head group chemistry beyond its mere charge.     

Gly6 of kalata B1 is critical for the selective binding to phosphatidylethanolamine membranes

The membrane interaction of the cyclotide kalata B1, an all-d-analogue and a single alanine substituted analogue (G6A), was studied by surface plasmon resonance (SPR) and atomic force microscopy (AFM). Kalata B1 showed a strong binding selectivity for dimyristoyl-phosphatidylethanolamine (DMPE) compared to dimyristoyl-phoshatidylcholine (DMPC)-containing lipids. However, when the interaction was visualized by AFM the peptide interacted with DMPC and DMPE in a similar manner. There was no apparent change in membrane morphology with either lipid, suggesting that kalata B1 does not act via a carpet-like disruption mechanism. The d-analogue showed similar binding by SPR and the same strong selectivity for DMPE, indicating that the membrane-interaction and lipid selectivity are not stereo-specific. SPR studies of the G6A analogue revealed that it interacted in a similar way to kalata B1 on the DMPC containing lipids, but showed no increased response on the DMPE containing lipids observed for kalata B1 and d-kalata B1. These results indicate that the Gly6 residue directly influences membrane binding as it is located near a putative membrane interacting hydrophobic patch. Overall, the data suggest that very small changes in amino acid composition (with no change in conformation) can influence specific self-association in combination with membrane binding and mediate the activity of kalata B1.     

Gly(6) of kalata B1 is critical for the selective binding to phosphatidylethanolamine membranes

The membrane interaction of the cyclotide kalata B1, an all-d-analogue and a single alanine substituted analogue (G6A), was studied by surface plasmon resonance (SPR) and atomic force microscopy (AFM). Kalata B1 showed a strong binding selectivity for dimyristoyl-phosphatidylethanolamine (DMPE) compared to dimyristoyl-phoshatidylcholine (DMPC)-containing lipids. However, when the interaction was visualized by AFM the peptide interacted with DMPC and DMPE in a similar manner. There was no apparent change in membrane morphology with either lipid, suggesting that kalata B1 does not act via a carpet-like disruption mechanism. The d-analogue showed similar binding by SPR and the same strong selectivity for DMPE, indicating that the membrane-interaction and lipid selectivity are not stereo-specific. SPR studies of the G6A analogue revealed that it interacted in a similar way to kalata B1 on the DMPC containing lipids, but showed no increased response on the DMPE containing lipids observed for kalata B1 and d-kalata B1. These results indicate that the Gly6 residue directly influences membrane binding as it is located near a putative membrane interacting hydrophobic patch. Overall, the data suggest that very small changes in amino acid composition (with no change in conformation) can influence specific self-association in combination with membrane binding and mediate the activity of kalata B1.     

Interfacial phenomena governing adhesion of chlorella to glass surfaces

Interfacial phenomena are directly involved in the adhesion of a strain of Chlorella, a unicellular alga, to glass surfaces in simple ionic solutions. The principal mechanisms governing the adhesion appear to be electrostatic interaction between electrical double layers and various specific surface interactions resulting from surface heterogeneity and ion adsorption. Under most conditions the algal cells and glass surfaces have negative zeta potentials, and adhesion to glass will not occur; but if, for example, FeCl₃ is added to an algal–glass system immersed in 0.05M NaCl, the algal and glass surfaces will possess very different zeta potentials, and adhesion will be strongest under those conditions which produce the greatest, difference in zeta poentials. Prior pretreatment and usage of glass apparatus greatly affect the glass zeta potentials and the adhesion of algal cells to glass. An apparatus for measuring a relative set of numbers representing the force of adhesion of algal cells is described.     

Effects of semiconductor substrate and glia-free culture on the development of voltage-dependent currents in rat striatal neurones

An essential requirement for successful long-term coupling between neuronal assemblies and semiconductor devices is that the neurones must be able to fully develop their electrogenic repertoire when growing on semiconductor (silicon) substrates. While it has for some time been known that neurones may be cultured on silicon wafers insulated with SiO2 and Si3N4, an electrophysiological characterisation of their development under such conditions is lacking. The development of voltage-dependent membrane currents, especially of the rapid sodium inward current underlying the action potential, is of particular importance because the conductance change during the action potential determines the quality of cell-semiconductor coupling. We have cultured rat striatal neurones on either glass coverslips or silicon wafers insulated with SiO2 and Si3N4 using both serum-containing and serum-free media. We here report evidence that not only serum-free culture media but also growth on semiconductor surfaces may negatively affect the development of voltage-dependent currents in neurones. Furthermore, using surface-charge measurements with the atomic force microscope, we demonstrate a reduced negativity of the semiconductor surface compared to glass. The reduced surface charge may affect cellular development through an effect on the binding and/or orientation of extracellular matrix proteins, such as laminin. Our findings therefore suggest that semiconductor substrates are not entirely equivalent to glass in terms of their effects on neuronal cell growth and differentiation.     

Electrostatic interaction between ion-penetrable multi-layered membranes

A theory of the double layer interaction regulated by the Donnan potential between two ion-penetrable membranes in an electrolyte solution developed previously by Ohshima and Kondo is extended to the case in which the membranes consist of many layers having different thickness and densities of membrane-fixed charges. The interaction force is found to be determined mainly by the contributions from layers located within the depth of 1/kappa (kappa, Debye-Hückel parameter) from the membrane surface. It is also predicted that the interaction force may alter its sign with changing electrolyte concentration.     

Effect of leucine to phenylalanine substitution on the nonpolar face of a class A amphipathic helical peptide on its interaction with lipid: high resolution solution NMR studies of 4F-dimyristoylphosphatidylcholine discoidal complex

Model class A amphipathic helical peptides mimic several properties of apolipoprotein A-I (apoA-I), the major protein component of high density lipoproteins. Previously, we reported the NMR structures of Ac-18A-NH(2) (renamed as 2F because of two phenylalanines), the base-line model class A amphipathic helical peptide in the presence of lipid ( Mishra, V. K., Anantharamaiah, G. M., Segrest, J. P., Palgunachari, M. N., Chaddha, M., Simon Sham, S. W., and Krishna, N. R. (2006) J Biol. Chem. 281, 6511-6519 ). Substitution of two Leu residues on the nonpolar face (Leu(3) and Leu(14)) with Phe residues produced the peptide 4F (so named because of four phenylalanines), which has been extensively studied for its anti-inflammatory and antiatherogenic properties. Like 2F, 4F also forms discoidal nascent high density lipoprotein-like particles with 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC). Since subtle structural changes in the peptide-lipid complexes have been shown to be responsible for their antiatherogenic properties, we undertook high resolution NMR studies to deduce detailed structure of 4F in 4F.DMPC discs. Like 2F, 4F adopts a well defined amphipathic alpha-helical structure in association with the lipid at a 1:1 peptide/lipid weight ratio. Nuclear Overhauser effect (NOE) spectroscopy revealed a number of intermolecular close contacts between the aromatic residues in the hydrophobic face of the helix and the lipid acyl chain protons. Similar to 2F, the pattern of observed peptide-lipid NOEs is consistent with a parallel orientation of the amphipathic alpha helix, with respect to the plane of the lipid bilayer, on the edge of the disc (the belt model). However, in contrast to 2F in 2F.DMPC, 4F in the 4F.DMPC complex is located closer to the lipid headgroup as evidenced by a number of NOEs between 4F and DMPC headgroup protons. These NOEs are absent in the 2F.DMPC complex. In addition, the conformation of the DMPC sn-3 chain in 4F.DMPC complex is different than in the 2F.DMPC complex as evidenced by the NOE between lipid 2.CH and betaCH(2) protons in 4F.DMPC, but not in 2F.DMPC, complex. Based on the results of this study, we infer that the antiatherogenic properties of 4F may result from its preferential interaction with lipid headgroups.     

Ion flux across lipid bilayer membranes with charged surfaces

Summary In this paper we derive expressions for the ion flux across lipid bilayer membranes with charged surfaces treating the membrane as a continuous phase interposed between two electrolyte solutions and calculating the ion flux with the Nernst-Planck equations. The theoretical results are compared with experiments of Seufert and Hashimoto on lipid bilayer membranes with charged surface active agents added to the membranes. If the charge of both membrane surfaces has the same sign the flux of the gegenions is greatly increased whereas the flux of the coions decreases to a small amount. For oppositely charged membrane surfaces the membrane behaves like a np semiconductor and typical rectification voltage-current characteristics are obtained.     

Mechanism of silicate binding to the bacterial cell wall in Bacillus subtilis.

To investigate the chemical mechanism of silicate binding to the surface of Bacillus subtilis, we chemically modified cell wall carboxylates to reverse their charge by the addition of an ethylenediamine ligand. For up to 9 weeks, mixtures of Si, Al-Fe-Si, and Al-Fe-Si plus toxic heavy metals were reacted with these cells for comparison with control cells and abiotic solutions. In general, more Si and less metal were bound to the chemically modified surfaces, thereby showing the importance of an electropositive charge in cell walls for fine-grain silicate mineral development. The predominant reaction for this development was the initial silicate-to-amine complexation in the peptidoglycan of ethylenediamine-modified and control cell walls, although metal ion bridging between electronegative sites and silicate had an additive effect. The binding of silicate to these bacterial surfaces can thus be described as outer sphere complex formation because it occurs through electrostatic interaction.     

Direct force measurements between cellulose surfaces and colloidal silica particles

The interaction of cellulose layers with colloidal silica particles was investigated by direct force measurements with the atomic force microscope (AFM). Upon approach, repulsive forces were found between the negatively charged silica particles and the cellulose surface. The forces were interpreted quantitatively in terms of electrostatic interactions due to overlap of diffuse layers originating from negatively charged carboxylic groups on the cellulose surface. The diffuse layer charge density of cellulose was estimated to be 0.80 mC/m2 at pH 9.5 and 0.21 mC/m2 at pH 4. The forces upon retraction are characterized by molecular adhesion events, whereby individual cellulose chains desorb from the probe surface. The retraction profiles are dominated by well-defined force plateaus, which correspond to single-chain desorption forces of 35-42 pN. We surmise that adsorption of cellulose to probe surfaces is dominated by nonelectrostatic forces, probably originating from hydrogen bonding. Electrostatic contributions to desorption force could be detected only at high pH, where the silica surface is highly charged.     

Response of the phosphatidylcholine headgroup to membrane surface charge in ternary mixtures of neutral, cationic, and anionic lipids: a deuterium NMR study.

Deuterium nuclear magnetic resonance (2H NMR) spectroscopy was used to investigate the response of the phosphatidylcholine headgroup of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) to changes in surface electrostatic charge in membranes consisting of ternary mixtures of lipids. DMPC was deuterated at the choline alpha- and beta-methylene segments. The membrane surface charge was manipulated by the simultaneous addition of cationic didodecyldimethylammonium bromide (DDAB) and anionic 1,2-dimyristoyl-sn-glycero-3-phosphoglycerol (DMPG) to neutral DMPC. Addition of increasing amounts of DDAB caused a progressive decrease (increase) in the 2H NMR quadrupole splitting from DMPC-alpha-d2 (DMPC-beta-d2). Addition of increasing amounts of DMPG caused a progressive increase (decrease) in the quadrupole splitting from DMPC-alpha-d2 (DMPC-beta-d2). Qualitatively, the 2H NMR quadrupole splitting charge response exhibited the same main features for ternary mixtures of DDAB/DMPG/DMPC and binary mixtures of DDAB/DMPC or DMPG/DMPC. Quantitatively, however, the 2H NMR quadrupole splittings obtained from ternary mixtures did not coincide with those obtained from binary mixtures of nominally identical surface charge densities. Hence, the quadrupole splitting did not respond directly to the net membrane surface charge. Instead, the quadrupole splitting measured for a given ternary lipid composition could be reproduced by summing the individual effects of the charged lipids in binary mixtures, weighted according to their appropriate mole fractions.     

Detection of DNA recognition events using multi-well field effect devices

We proposed the multi-well field effect device for detection of charged biomolecules and demonstrated the detection principle for DNA recognition events using quasi-static capacitance-voltage (QSCV) measurement. The multi-well field effect device is based on the electrostatic interaction between molecular charges induced by DNA recognition and surface electrons in silicon through the Si(3)N(4)/SiO(2) thin double-layer. Since DNA molecules and DNA binders such as Hoechst 33258 have intrinsic charges in aqueous solutions, respectively, the charge density changes due to DNA recognition events at the Si(3)N(4) surface were directly translated into electrical signal such as a flat band voltage change in the QSCV measurement. The average flat band shifts were 20.7 mV for hybridization and -13.5 mV for binding of Hoechst 33258. From the results of flat band voltage shifts due to hybridization and binding of Hoechst 33258, the immobilization density of oligonucleotide probes at the Si(3)N(4) surface was estimated to be 10(8) cm(-2). The platform based on the multi-well field effect device is suitable for a simple and arrayed detection system for DNA recognition events.     

Differential lipid binding of truncation mutants of Galleria mellonella apolipophorin III

Apolipophorin III (apoLp-III) is a prototype exchangeable apolipoprotein that is amenable to structure-function studies. The protein folds as a bundle of five amphipathic alpha-helices and undergoes a dramatic conformational change upon lipid binding. Recently, we have shown that a truncation mutant of Galleria mellonella apoLp-III comprising helices 1-3 is stable in solution and able to bind to lipid surfaces [Dettloff, M., Weers, P. M. M., Niere, M., Kay, C. M., Ryan, R. O., and Wiesner, A. (2001) Biochemistry 40, 3150-3157]. To investigate the role of the C-terminal helices in apoLp-III structure and function, two additional 3-helix mutants were designed: a core fragment comprising helix (H) 2-4, and a C-terminal fragment (H3-5). Each truncation mutant retained the ability to associate spontaneously with dimyristoylphosphatidylcholine (DMPC) vesicles, transforming them into discoidal complexes. The rate of apolipoprotein-dependent DMPC vesicle transformation decreased in the order H1-3 > H2-4 > H3-5. Truncation of two helices led to a significant decrease in alpha-helical content in buffer in each case, from 86% (wild-type) to 50% (H1-3), 28% (H2-4), and 24% alpha-helical content (H3-5). On the other hand, trifluoroethanol or complexation with DMPC induced the truncation mutants to adopt a high alpha-helical structure similar to that of wild-type protein (84-100% alpha-helical structure). ApoLp-III(H1-3) and apoLp-III(H2-4), but not apoLp-III(H3-5), were able to prevent phospholipase-C-induced low density lipoprotein aggregation, indicating that interaction of the C-terminal fragment with spherical lipoprotein surfaces was impaired. As lipoprotein binding is significantly affected and DMPC transformation rates are relatively slow upon removal of N-terminal helices, the data indicate that structural elements necessary for lipid interaction reside in the N-terminal part of the protein.     

Membrane topology of a 14-mer model amphipathic peptide: a solid-state NMR spectroscopy study

We have investigated the interaction between a synthetic amphipathic 14-mer peptide and model membranes by solid-state NMR. The 14-mer peptide is composed of leucines and phenylalanines modified by the addition of crown ethers and forms a helical amphipathic structure in solution and bound to lipid membranes. To shed light on its membrane topology, 31P, 2H, 15N solid-state NMR experiments have been performed on the 14-mer peptide in interaction with mechanically oriented bilayers of dilauroylphosphatidylcholine (DLPC), dimyristoylphosphatidylcholine (DMPC), and dipalmitoylphosphatidylcholine (DPPC). The 31P, 2H, and 15N NMR results indicate that the 14-mer peptide remains at the surface of the DLPC, DMPC, and DPPC bilayers stacked between glass plates and perturbs the lipid orientation relative to the magnetic field direction. Its membrane topology is similar in DLPC and DMPC bilayers, whereas the peptide seems to be more deeply inserted in DPPC bilayers, as revealed by the greater orientational and motional disorder of the DPPC lipid headgroup and acyl chains. 15N{31P} rotational echo double resonance experiments have also been used to measure the intermolecular dipole-dipole interaction between the 14-mer peptide and the phospholipid headgroup of DMPC multilamellar vesicles, and the results indicate that the 14-mer peptide is in contact with the polar region of the DMPC lipids. On the basis of these studies, the mechanism of membrane perturbation of the 14-mer peptide is associated to the induction of a positive curvature strain induced by the peptide lying on the bilayer surface and seems to be independent of the bilayer hydrophobic thickness.