SpA蛋白与磷脂单分子膜相互作用的研究

利用石英表面沉积ＬＢ膜的紫外吸收特性与ＣＤ谱特性研究了磷脂单分子膜与ＳｐＡ的相互作用,实验结果表明,单分子膜的疏密状态,蛋白质与膜表面的电荷特性及亚相Ｃａ＾２＋离子浓度均对该蛋白质与磷脂的相互作用有显著的影响,蛋白质在磷膜中的镶嵌与吸附作用为生物膜的重组提供了新的途径。     

Relationship of membrane sidedness to the effects of the lipophosphoglycan of Leishmania donovani on the fusion of influenza virus.

Cells expressing the influenza hemagglutinin protein were fused to planar lipid bilayers containing the viral receptor GD1a at pH 5.0. An amphiphile known to alter membrane properties is lipophosphoglycan (LPG). This glycoconjugate was added from aqueous solution to either the cis or the trans monolayer to examine its effects on the fusion process. LPG markedly inhibited the formation of fusion pores when present in the cis monolayer but LPG in the trans monolayer had no effect on the parameters of pore formation or on the properties of the pores. The N-terminal segment of the HA2 subunit of the influenza hemagglutinin protein is important for membrane fusion. The effect of LPG on the conformation and membrane insertion of a synthetic 20-amino-acid peptide, corresponding to the influenza fusion peptide, was examined at pH 5.0 by attenuated total reflection Fourier transform infrared spectroscopy and by the fluorescence properties of the Trp residues of this peptide. It was found that cis LPG did not prevent insertion of the peptide into the membrane but it did alter the conformation of the membrane-inserted peptide from alpha-helix to beta-structure. The beta-structure was oriented along the bilayer normal. The effect of cis LPG on the conformation of the fusion peptide probably contributes to the observed inhibition of pore formation and lipid mixing. In contrast, trans LPG has no effect on the conformation or angle of membrane insertion of the peptide, nor does it affect pore formation by HA-expressing cells. The ineffectiveness of trans LPG, despite it having strong positive curvature-promoting properties, may be a consequence of the size of this amphiphile being too large to enter a fusion pore.     

Thermodynamics of the coil <==> beta-sheet transition in a membrane environment

Biologically important peptides such as the Alzheimer peptide Abeta(1-40) display a reversible random coil <==>beta-structure transition at anionic membrane surfaces. In contrast to the well-studied random coil left arrow over right arrow alpha-helix transition of amphipathic peptides, there is a dearth on information on the thermodynamic and kinetic parameters of the random coil left arrow over right arrow beta-structure transition. Here, we present a new method to quantitatively analyze the thermodynamic parameters of the membrane-induced beta-structure formation. We have used the model peptide (KIGAKI)(3) and eight analogues in which two adjacent amino acids were substituted by their d-enantiomers. The positions of the d,d pairs were shifted systematically along the three identical segments of the peptide chain. The beta-structure content of the peptides was measured in solution and when bound to anionic lipid membranes with circular dichroism spectroscopy. The thermodynamic binding parameters were determined with isothermal titration calorimetry and the binding isotherms were analysed by combining a surface partition equilibrium with the Gouy-Chapman theory. The thermodynamic parameters were found to be linearly correlated with the extent of beta-structure formation. beta-Structure formation at the membrane surface is characterized by an enthalpy change of DeltaH(beta)=-0.23 kcal/mol per residue, an entropy change of DeltaS(beta)=-0.24 cal/mol K residue and a free energy change of DeltaG(beta)=-0.15 kcal/mol residue. An increase in temperature induces an unfolding of beta-structure. The residual free energy of membrane-induced beta-structure formation is close to that of membrane-induced alpha-helix formation.     

Biophysical properties of a synthetic transit peptide from wheat chloroplast ribulose 1,5-bisphosphate carboxylase.

The surface properties of pure RuBisCo transit peptide (RTP) and its interaction with zwitterionic, anionic phospholipids and chloroplast lipids were studied by using the Langmuir monolayer technique. Pure RTP is able to form insoluble films and the observed surface parameters are compatible with an alpha-helix perpendicular to the interface. The alpha-helix structure tendency was also observed by using transmission FT-IR spectroscopy in bulk system of a membrane mimicking environment (SDS). On the other hand, RTP adopts an unordered structure in either aqueous free interface or in the presence of vesicles composed of a zwitterionic phospholipid (POPC). Monolayer studies show that in peptide/lipid mixed monolayers, RTP shows no interaction with zwitterionic phospholipids, regardless of their physical state. Also, with the anionic POPG at high peptide ratios RTP retains its individual surface properties and behaves as an immiscible component of the peptide/lipid mixed interface. This behaviour was also observed when the mixed films were composed by RTP and the typical chloroplast lipids MGDG or DGDG (mono- and di-galactosyldiacylglycerol). Conversely, RTP establishes a particular interaction with phosphatidylglycerol and cardiolipin at low peptide to lipid area covered relation. This interaction takes place with an increase in surface stability and a reduction in peptide molecular area (intermolecular interaction). Data suggest a dynamic membrane modulation by which the peptide fine-tunes its membrane orientation and its lateral stability, depending on the quality (lipid composition) of the interface.     

Secondary structure and lipid interactions of the N-terminal segment of pulmonary surfactant SP-C in Langmuir films: IR reflection-absorption spectroscopy and surface pressure studies

Pulmonary surfactant, a thin lipid/protein film lining mammalian lungs, functions in vivo to reduce the work of breathing and to prevent alveolar collapse. Analogues of two hydrophobic surfactant proteins, SP-B and SP-C, have been incorporated into therapeutic agents for respiratory distress syndrome, a pathological condition resulting from deficiency in surfactant. To facilitate rational design of therapeutic agents, a molecular level understanding of lipid interaction with surfactant proteins or their analogues in aqueous monolayer films is necessary. The current work uses infrared reflection-absorption spectroscopy (IRRAS) to determine peptide conformation and the effects of S-palmitoylation on the lipid interactions of a synthetic 13 residue N-terminal peptide [SP-C13(palm)(2)] of SP-C, in mixtures with 1,2-dipalmitoylphosphatidylcholine (DPPC) or 1,2-dipalmitoylphosphatidylglycerol (DPPG). Two Amide I' features, at approximately 1655 and approximately 1639 cm(-1) in the peptide IRRAS spectra, are assigned to alpha-helical peptide bonds in hydrophobic and aqueous environments, respectively. In binary DPPC/SP-C13(palm)(2) films, the proportion of hydrated/hydrophobic helix increases reversibly with surface pressure (pi), suggestive of the peptide being squeezed out from hydrophobic regions of the monolayer. No such effect was observed for DPPG/peptide monolayers, indicative of stronger, probably electrostatic, interactions. Depalmitoylation produced a weakened interaction with either phospholipid as deduced from IRRAS spectra and from pi-area isotherms. S-Palmitoylation may modulate peptide hydration and conformation in the N-terminal region of SP-C and may thus permit the peptide to remain in the film at the high surface pressures present during lung compression. The unique capability of IRRAS to detect the surface pressure dependence of protein or peptide structure/interactions in a physiologically relevant model for surfactant is clearly demonstrated.     

Lysis of chromaffin granules by phospholipase A2-treated plasma membranes. A cell-free model for exocytosis in adrenal medulla

The conformations of a synthetic peptide corresponding to the signal sequence of E. coli alkaline phosphatase, Lys-Gln-Ser-Thr-Ile-Ala-Leu-Ala-Leu-Leu-Pro-Leu-Leu-Phe-Thr-Pro-Val-Thr- Lys- Ala-OCH3, have been examined in different environments by circular dichroism spectroscopy. In trifluoroethanol, methanol and aqueous mixtures of these solvents, the signal peptide has largely random conformation (approximately 80%) with small amounts of alpha-helix and beta-structure. However, in micellar environment, there is a significant increase in ordered conformation with both alpha-helix and beta-structure being present, unlike in other signal sequences reported in the literature, where only the alpha-helical conformation has been observed. Hence, an alpha-helical conformation may not be as stringent a requirement as overall hydrophobicity for recognition of signal sequences by the cell's export machinery.     

Infrared reflection-absorption of melittin interaction with phospholipid monolayers at the air/water interface.

The interaction of melittin with monolayers of 1,2-dipalmitoylphosphatidylcholine and 1,2-dipalmitoylphosphatidylserine has been investigated with infrared external reflection-absorption spectroscopy. Improved instrumentation permits determination of acyl chain conformation and peptide secondary structure in situ at the air/water interface. The IR frequency of the 1,2-dipalmitoylphosphatidylcholine antisymmetric acyl chain CH2 stretching vibration decreases by 1.3 cm-1 upon melittin insertion, consistent with acyl chain ordering, whereas the same vibrational mode increases by 0.5 cm-1 upon peptide interaction with the 1,2-dipalmitoylphosphatidylserine monolayer, indicative of chain disordering. Thus the peptide interacts quite differently with zwitterionic compared with negatively charged monolayer surfaces. Melittin in the monolayer adopted a secondary structure with an amide l(l') frequency (1635 cm-1) dramatically different from the alpha-helical motif (amide l frequency 1656 cm-1 in a dry or H2O hydrated environment, amide l' frequency 1645 cm-1 in an H-->D exchanged alpha-helix) assumed in bilayer or multibilayer environments. This work represents the first direct in situ spectroscopic indication that peptide secondary structure in lipid monolayers may differ from that in bilayers.     

Antimicrobial properties of a lipid interactive alpha-helical peptide VP1 against Staphylococcus aureus bacteria

Theoretical analysis indicates that peptide VP1 forms a membrane interactive amphiphilic alpha-helix with antibacterial properties. Fourier transform infra-red based analyses showed VP1 to be alpha-helical (45%) in the presence of vesicle mimics of membranes from Staphylococcus aureus and to induce increases in the fluidity of these vesicles, as indicated by a rise in wavenumber of circa 0.5 to 1.0 cm(-1). The peptide induced surface pressure increases of 5 mN m(-1) in monolayer mimics of S. aureus membranes confirm the formation of a membrane interactive alpha-helix. These interactions appeared to involve significant hydrophobic and electrostatic contributions as VP1 induced comparable surface pressure changes in anionic (5.5 mN m(-1)) and zwitterionic (4 mN m(-1)) lipid monolayers. It is suggested that whilst efficacy requires further sequence specific information, the peptides generic structure provides the basis for its broad antimicrobial activity.     

Low-ultraviolet circular dichroism spectroscopy of sequential peptides 1-63, 64-95, 96-128, and 129-168 derived from myelin basic protein of rabbit

Four sequential peptides (sequences 1-63, 64-95, 96-128, and 129-168) derived from rabbit myelin basic protein by thrombic cleavage were examined by low-ultraviolet circular dichroism spectroscopy in 0.5 mM tris(hydroxymethyl)aminomethane hydrochloride (pH approximately 7.2) containing 0-92% trifluoroethanol (TFE). In the absence of the alcohol, all of the peptides contained a significant amount (17-29%) of beta-structure. In the presence of relatively low concentrations (up to 30%) of TFE, all of the peptides except 96-128 adopted considerable alpha-helix (16-33%). This involved a transition from the beta-structure in peptide 1-63 and transitions from the nonordered structure in peptides 1-63, 64-95, and 129-168. Furthermore, additional alpha-helix formed in peptide 1-63 between 30% and 92% TFE at the expense of nonordered structure, whereas the alpha-helix formation above 50% TFE in peptide 129-168 resulted largely from a beta-structure----alpha-helix transition. With the exception of the 129-168 peptide, approximately 65-100% of the maximum level of beta-structure persisted throughout the entire range of TFE concentration. In the case of peptide 129-168, however, most of the beta-structure was converted to alpha-helix and nonordered structure at 75% TFE. While the present results support our previous assignments of beta-structure- and alpha-helix-forming regions to specific amino acid sequences of the basic protein, they also demonstrate that the beta-structure----alpha-helix transitions evidenced at various concentrations of TFE were influenced to a considerable degree by the length of the peptide, presumably due to the presence or absence of interactions between noncontiguous portions of the myelin basic protein polypeptide chain.     

Deacylated pulmonary surfactant protein SP-C transforms from alpha-helical to amyloid fibril structure via a pH-dependent mechanism: an infrared structural investigation

Bovine pulmonary surfactant protein C (SP-C) is a hydrophobic, alpha-helical membrane-associated lipoprotein in which cysteines C4 and C5 are acylated with palmitoyl chains. Recently, it has been found that the alpha-helix form of SP-C is metastable, and under certain circumstances may transform from an alpha-helix to a beta-strand conformation that resembles amyloid fibrils. This transformation is accelerated when the protein is in its deacylated form (dSP-C). We have used infrared spectroscopy to study the structure of dSP-C in solution and at membrane interfaces. Our results show that dSP-C transforms from an alpha-helical to a beta-type amyloid fibril structure via a pH-dependent mechanism. In solution at low pH, dSP-C is alpha-helical in nature, but converts to an amyloid fibril structure composed of short beta-strands or beta-hairpins at neutral pH. The alpha-helix structure of dSP-C is fully recoverable from the amyloid beta-structure when the pH is once again lowered. Attenuated total reflectance infrared spectroscopy of lipid-protein monomolecular films showed that the fibril beta-form of dSP-C is not surface-associated at the air-water interface. In addition, the lipid-associated alpha-helix form of dSP-C is only retained at the surface at low surface pressures and dissociates from the membrane at higher surface pressures. In situ polarization modulation infrared spectroscopy of protein and lipid-protein monolayers at the air-water interface confirmed that the residual dSP-C helix conformation observed in the attenuated total reflectance infrared spectra of transferred films is randomly or isotropically oriented before exclusion from the membrane interface. This work identifies pH as one of the mechanistic causes of amyloid fibril formation for dSP-C, and a possible contributor to the pathogenesis of pulmonary alveolar proteinosis.     

Actin binding to lipid-inserted alpha-actinin.

The interaction of alpha-actinin with lipid films and actin filaments was investigated. First alpha-actinin was incorporated in lipid films at the air/water interface. Injection of alpha-actinin into the subphase of a lipid monolayer led to a significant increase of the surface pressure only for lipid films consisting of a mixture of a negatively charged lipid with a high proportion of diacylglycerol. These alpha-actinin-containing films were transferred onto silanized quartz slides. Photobleaching experiments in the evanescent field allowed quantification of the lateral number density of the lipid-bound alpha-actinin. In combination with the area increase from the monolayer experiments, the photobleaching measurements suggest that alpha-actinin is incorporated into the lipid film in such a way that actin binding sites are accessible from the bulk phase. Binding experiments confirmed that the alpha-actinin selectively binds actin filaments in this configuration. We also showed that, in contrast to actin filaments which are adsorbed directly onto planar surfaces, the alpha-actinin-bound actin filaments are recognized and cleaved by the actin-severing protein gelsolin. Thus we have constructed an in vitro system which opens new ways for investigations of membrane-associated actin-binding proteins and of the physical behavior of actin filaments in the close neighborhood to membranes.     

Effects of pH on the binding of hematoporphyrin derivative to monolayer and bilayer membranes.

The effects of pH on the binding of hematoporphyrin derivative (HpD) to monolayer and bilayer membranes have been studied. Absorption spectra of HpD bound to phosphatidylcholine (PC) liposomes indicate that there is greater binding of HpD to lipid films at acidic, tumoricidal pH conditions than at normal tissue pH. These results were found to correlate with surface pressure measurements of monolayer films formed under similar conditions. Surface potential measurements in conjunction with surface pressure measurements from monolayer films suggest that at low pH (i.e. less than or equal to 6.6) porphyrin intercalates within the lipid film to reach relatively high concentrations, while at higher pH (i.e. greater than or equal to 7.4) the porphyrin preferably adsorbs to the lipid film at the monolayer/water interface.     

Interaction of the acetylcholine (nicotinic) receptor protein from Torpedo marmorata electric organ with monolayers of pure lipids

Membrane fragments rich in cholinergic (nicotinic) receptor protein were purified from the electric organ of Torpedo marmorata. Their lipid composition is essentially characterized by the prominence of cholesterol, phosphatidylethanolamine and phosphatidylcholine, long-chain fatty acyl constituents, and the absence of sphingomyelin. Solubilised receptor was purified from these fragments and the concentration of sodium cholate lowered by dialysis to 0.01% (w/v). When this preparation was injected under a lipid monolayer, an increase of surface pressure developed, which was not observed with the detergent alone nor in the absence of lipid film. When covalently radiolabelled receptor preparations were injected at a constant surface pressure the radioactivity recovered with the film was proportional to the increase in area. It is concluded that the pressure or area increases are due to the penetration of the cholinergic receptor protein into the lipid film. Incorporation experiments into films formed from various pure lipids showed that the protein interacts more readily with cholesterol than with ergosterol, phosphatidylcholine, or other phospholipids. Its affinity is also higher for long-chain phosphatidylcholines than for short-chain ones. The degree of unsaturation and fluidity of the 3-sn-phosphatidylcholine (lecithin) films are of secondary importance. Parallel experiments with covalently and non-covalently labelled receptor preparations showed that part of the protein recovered with the film lost its alpha-toxin binding ability during the penetration. Similar data were obtained with the receptor purified from Electrophorus electricus electric organ.     

Conformational mapping of the N-terminal peptide of HIV-1 gp41 in membrane environments using (13)C-enhanced Fourier transform infrared spectroscopy

The N-terminal domain of HIV-1 glycoprotein 41000 (FP; residues 1--23; AVGIGALFLGFLGAAGSTMGARSCONH(2)) participates in fusion processes underlying virus--cell infection. Here, we use physical techniques to study the secondary conformation of synthetic FP in aqueous, structure-promoting, lipid and biomembrane environments. Circular dichroism and conventional, (12)C-Fourier transform infrared (FTIR) spectroscopy indicated the following alpha-helical levels for FP in 1-palmitoyl-2-oleoylphosphatidylglycerol (POPG) liposomes-hexafluoroisopropanol (HFIP)>trifluoroethanol (TFE)>phosphate-buffered saline (PBS). (12)C-FTIR spectra also showed disordered FP structures in these environments, along with substantial beta-structures for FP in TFE or PBS. In further experiments designed to map secondary conformations to specific residues, isotope-enhanced FTIR spectroscopy was performed using a suite of FP peptides labeled with (13)C-carbonyl at multiple sites. Combining these (13)C-enhanced FTIR results with molecular simulations indicated the following model for FP in HFIP: alpha-helix (residues 3-16) and random and beta-structures (residues 1-2 and residues 17-23). Additional (13)C-FTIR analysis indicated a similar conformation for FP in POPG at low peptide loading, except that the alpha-helix extends over residues 1-16. At low peptide loading in either human erythrocyte ghosts or lipid extracts from ghosts, (13)C-FTIR spectroscopy showed alpha-helical conformations for the central core of FP (residues 5-15); on the other hand, at high peptide loading in ghosts or lipid extracts, the central core of FP assumed an antiparallel beta-structure. FP at low loading in ghosts probably inserts deeply as an alpha-helix into the hydrophobic membrane bilayer, while at higher loading FP primarily associates with ghosts as an aqueous-accessible, beta-sheet. In future studies, (13)C-FTIR spectroscopy may yield residue-specific conformations for other membrane-bound proteins or peptides, which have been difficult to analyze with more standard methodologies.     

Kinetics of phospholipid insertion into monolayers containing the lung surfactant proteins SP-B or SP-C

The lung surfactant proteins SP-B and SP-C are pivotal for fast and reversible lipid insertion at the air/liquid interface, a prerequisite for functional lung activity. We used a model system consisting of a preformed monolayer at the air/liquid interface supplemented with surfactant protein SP-B or SP-C and unilamellar vesicles injected into the subphase of a film balance. The content of SP-B or SP-C was similar to that found in lung lavage. In order to elucidate distinct steps of lipid insertion, we measured the time-dependent pressure increase as a function of the initial surface pressure, the temperature and the phosphatidylglycerol content by means of surface tension measurements and scanning force microscopy (SFM). The results of the film balance study are indicative of a two-step mechanism in which initial adsorption of vesicles to the protein-containing monolayer is followed by rupture and integration of lipid material. Furthermore, we found that vesicle adsorption on a preformed monolayer supplemented with SP-B or SP-C is strongly enhanced by negatively charged lipids as provided by DPPG and the presence of Ca2+ ions in the subphase. Hence, long-range electrostatic interactions are thought to play an important role in attracting vesicles to the surface, being the initial step in replenishment of lipid material. While insertion into the monolayer is independent of the type of protein SP-B or SP-C, initial adsorption is faster in the presence of SP-B than SP-C. We propose that the preferential interaction between SP-B and negatively charged DPPG leads to accumulation of negative charges in particular regions, causing strong adhesion between DPPG-containing vesicles and the monolayer mediated by Ca2+ ions, which eventually causes flattening and rupture of attached liposomes as observed by in situ SFM.     

Interaction of a nonspecific wheat lipid transfer protein with phospholipid monolayers imaged by fluorescence microscopy and studied by infrared spectroscopy.

The interaction of a nonspecific wheat lipid transfer protein (LTP) with phospholipids has been studied using the monolayer technique as a simplified model of biological membranes. The molecular organization of the LTP-phospholipid monolayer has been determined by using polarized attenuated total internal reflectance infrared spectroscopy, and detailed information on the microstructure of the mixed films has been investigated by using epifluorescence microscopy. The results show that the incorporation of wheat LTP within the lipid monolayers is surface-pressure dependent. When LTP is injected into the subphase under a dipalmytoylphosphatidylglycerol monolayer at low surface pressure (< 20 mN/m), insertion of the protein within the lipid monolayer leads to an expansion of dipalmytoylphosphatidylglycerol surface area. This incorporation leads to a decrease in the conformational order of the lipid acyl chains and results in an increase in the size of the solid lipid domains, suggesting that LTP penetrates both expanded and solid domains. By contrast, when the protein is injected under the lipid at high surface pressure (> or = 20 mN/m) the presence of LTP leads neither to an increase of molecular area nor to a change of the lipid order, even though some protein molecules are bound to the surface of the monolayer, which leads to an increase of the exposure of the lipid ester groups to the aqueous environment. On the other hand, the conformation of LTP, as well as the orientation of alpha-helices, is surface-pressure dependent. At low surface pressure, the alpha-helices inserted into the monolayers are rather parallel to the monolayer plane. In contrast, at high surface pressure, the alpha-helices bound to the surface of the monolayers are neither parallel nor perpendicular to the interface but in an oblique orientation.     

Conformational study of poly(L-lysine) interacting with acidic phospholipid vesicles

Circular dichroism measurements were carried out on poly(L-lysine) in the presence of vesicles of the negatively charged phospholipids, phosphatidylserine (PS; from bovine brain), phosphatidic acid (PA; prepared from egg yolk lecithin) and dimyristoylphosphatidylglycerol (DMPG). PS vesicles induced a conformational change in poly(L-lysine) from random coil to alpha-helix structure in 5 mM Tes (pH 7.0), whereas PA vesicles gave rise to beta-structure in the same buffer. The fraction of alpha-helix, F alpha (or beta-structure, F beta), increased with increasing PS (or PA) concentration, reaching a saturation value of about 0.7 (or about 1). Mixed vesicles comprising PS and dilauroylphosphatidylcholine (DLPC) also induced alpha-helix conformation, however, the saturation value of F alpha diminished with decreasing PS content in mixed vesicles. On the other hand, the spectral patterns for poly(L-lysine) in DMPG vesicle suspensions exhibited the coexistence of alpha-helix and beta-structure. Both F alpha and F beta increased with DMPG concentration and reached saturation values of about 0.5. Mixed vesicles composed of DMPG and dimyristoylphosphatidylcholine (DMPC) led to a reduction in F beta, while F alpha remained almost constant. The diversity in ordered structure induced by different phospholipid vesicles suggests the participation of lipid head groups in determining the secondary structure of poly(L-lysine) adsorbed on the vesicular surface.     

Surface properties of membrane systems. Transport of staphylococcal delta-toxin from aqueous to membrane phase

Hemolytic delta-toxin from Staphylococcus aureus was soluble in either water, methanol or chloroform/methanol (2 : 1, v/v). The toxin spread readily from distilled water into films with pressures (pi) of 10 dynes/cm on water and 30 dynes/cm on 6 M urea; from chloroform/methanol it produced 40 dynes/cm pressure on distilled water. The toxin adsorbed barely from water (pi = 1 dyne/ cm) but it did rapidly from 6 M urea (pi = 35 dynes/cm). The protein films had unusually high surface potentials, which increased with the film pressure and decreased with increasing both pH and urea concentration in the aqueous phase. The fluorescence of 1-aniline 8-naphthalene sulfonate with delta-toxin was much greater than that with RNAase and dipalmitoyl phosphatidylcholine itself, indicating probably a marked lipid-binding character of the toxin. By circular dichroism the alpha-helix content of delta-toxin was 42% in water, 45% in methanol, 24% in 6 M urea. Infrared spectroscopy showed predominant alpha-helix in both 2H2O and deuterated chloroform/methanol as well as in films spread from either solvent on 2H2O. In spreading from 6 M [2H]urea, in which the major infrared absorption was that of [2H]urea with peaks at 1600 and 1480 cm(-1), the delta-toxin film showed prevalently non-alpha-helix structures with major peak intensities at 1633 cm(-1) > 1680 cm(-1), indicating the appearance of new beta-aggregated and beta-antiparallel pleated sheet structures in the film. The data prove that (1) high pressure protein films can consist of alpha-helix as well as non-alpha-helix structures and, differently from another cytolytic protein, melittin, delta-toxin does not resume the alpha-helix conformation in going into the film phase from the extended chain in 6 M urea; (2) conformational changes are important in the transport of proteins from aqueous to lipid or membrane phase; (3) delta-toxin is by far more versatile in structural dynamics and more surface active than alpha-toxin.     

In situ study by polarization modulated Fourier transform infrared spectroscopy of the structure and orientation of lipids and amphipathic peptides at the air-water interface.

Free amphipathic peptides and peptides bound to dimyristoylphosphatidylcholine (DMPC) were studied directly at the air/water interface using polarization modulation infrared reflection absorption spectroscopy (PMIRRAS). Such differential reflectivity measurements proved to be a sensitive and efficient technique to investigate in situ the respective conformations and orientations of lipid and peptide molecules in pure and mixed films. Data obtained for melittin, a natural hemolytic peptide, are compared to those of L15K7, an ideally amphipathic synthetic peptide constituted by only apolar Leu and polar Lys residues. For pure peptidic films, the intensity, shape, and position of the amide I and II bands indicate that the L15K7 peptide adopts a totally alpha-helical structure, whereas the structure of melittin is mainly alpha-helical and presents some unordered domains. The L15K7 alpha-helix axis is oriented essentially parallel to the air-water interface plane; it differs for melittin. When injected into the subphase, L15K7 and melittin insert into preformed expanded DMPC monolayers and can be detected by PMIRRAS, even at low peptide content (> 50 DMPC molecules per peptide). In such conditions, peptides have the same secondary structure and orientation as in pure peptidic films.     

Interaction of amyloid beta-(1-40) peptide with model membranes

The amyloid beta (1-40) peptide (A beta) is the main component of amyloid deposits found in the brain of patients afflicted with Alzheimer's disease. After treatment with hexafluoroisopropanol, commercial A beta is readily soluble in water and buffers at pH 7.4 and has an irregular secondary structure. The adsorption of A beta to the water-air interface and to the surface of the dipalmitoylphosphatidylethanolamine monolayer at a surface pressure pi close to zero leads to an increase in pressure up to 17 mN/m. When being adsorbed, the molecules of the peptide occupy a part of the monolayer surface, which leads to the compression of lipid molecules forming the monolayer. Further compression of the monolayer composed of the molecules of the lipid and peptide leads to the extrusion of the peptide from the monolayer. If the lipid monolayer is preliminarily (prior to the addition of the peptide to the liquid phase) compressed to pi = 30 mN/m, no adsorption of the peptide to the monolayer occurs. No changes in the structure of the dipalmitoylphosphatidylethanolamine monolayer were detected by the sliding X-ray diffraction method, indicating the absence of specific interactions. The method of reflection and absorption infrared spectroscopy makes it possible to determine the conformation of the adsorbed peptide and its orientation in the lipid monolayer. It was found that A beta has the conformation of a beta-fold oriented parallel to the interface, as it is the case with the adsorption of peptide molecules to the lipid monolayer at pi < 30 mN/m and upon adsorption to the interface that is not occupied by the lipid.