Effects of polypeptide-phospholipid interactions on bilayer reorganizations Raman spectroscopic study of the binding of polymyxin B to dimyristoylphosphatidic acid and dimyristoylphosphatidylcholine dispersions

The interactions of the antibiotic polymixin B, a polycationic cyclic polypeptide containing a branched acyl side chain, with dimyristoylphosphatidylcholine (DMPC) and dimyristoylphosphatidic acid (DMPA) bilayers were investigated by Raman spectroscopy for a wide range of lipid/polypeptide mole fractions. Temperature profiles, constructed from peak height intensity ratios derived from the lipid methylene C-H stretching and acyl chain C-C stretching mode regions, reflected changes originating from lateral chain packing effects and intrachain trans / gauche rotamer formation, respectively. For DMPC/polymyxin B bilayers the temperature dependent curves indicate a broadening of the gel-liquid crystalline phase transition accompanied by an approx. 3 C deg. increase in the phase transition temperature from 22.8°C for the pure bilayer to 26°C for the polypeptide complex. For a 10:1 lipid/polypeptide mole ratio the temperature profile derived from the C-C mode spectral parameters displays a second order/disorder transition, at approx. 35.5°C, associated with the melting behavior of approximately three bilayer lipids immobilized by the antibiotic's charged cyclic headgroup and hydrophobic side chain. For the 10:1 mole ratio DMPA/polypeptide liposomes, the temperature profiles indicate three order/disorder transitions at 46, 36 and 24°C. Pure DMPA bilayers display a sharp lamellar-micellar phase transition at 51°C.     

Interaction of poly(l-lysines) with negatively charged membranes: an FT-IR and DSC study

The influence of the binding of poly(l-lysine) (PLL) to negatively charged membranes containing phosphatidylglycerols (PG) was studied by DSC and FT-IR spectroscopy. We found a general increase in the main transition temperature as well as increase in hydrophobic order of the membrane upon PLL binding. Furthermore we observed stronger binding of hydration water to the lipid head groups after PLL binding. The secondary structure of the PLL after binding was studied by FT-IR spectroscopy. We found that PLL binds in an α-helical conformation to negatively charged DPPG membranes or membranes with DPPG-rich domains. Moreover we proved that PLL binding induces domain formation in the gel state of mixed DPPC/DPPG or DMPC/DPPG membranes as well as lipid remixing in the liquid–crystalline state. We studied these effects as a function of PLL chain length and found a significant dependence of the secondary structure, phase transition temperature and domain formation capacity on PLL chain length and also a correlation between the peptide secondary structure and the phase transition temperature of the membrane. We present a system in which the membrane phase transition triggers a highly cooperative secondary structure transition of the membrane-bound peptide from α-helix to random coil. Dedicated to Prof. K. Arnold on the occasion of his 65th birthday.     

Comparative study on the interaction of cell-penetrating polycationic polymers with lipid membranes

Cell-penetrating peptides are arginine- and lysine-rich cationic peptides that can readily enter cells not only by themselves but also carrying other macromolecular cargos. In fact, we have reported that polycationic polymer such as poly-l-lysine (PLL) and poly-l-arginine (PLA) translocate through negatively charged phospholipid liposome membranes. In this work, we made a comparative study of the interaction of PLL or PLA with lipid membranes consisting of negatively charged phospholipids to understand the role of basic amino acid residue (i.e. arginine and lysine) in the membrane-penetrating activity of polypeptides. PLA and PLL translocated into giant unilamellar vesicle composed of soybean phospholipids. ζ-potential and turbidity measurements demonstrated the electrostatic binding of PLL and PLA to large unilamellar vesicle (LUV). Fluorescence studies using membrane probes revealed that the binding of PLA and PLL to LUV affects the hydration and packing of the membrane interface region, in which the membrane insertion of PLA appeared to be greater than PLL. Differential scanning calorimetry showed that the enthalpy of the gel to liquid-crystalline phase transition for dipalmitoyl phosphatidylglycerol vesicle was greatly reduced by binding of PLL and PLA, in which the reduction is much larger in PLA than in PLL. Circular dichroism measurements in 2,2,2-trifluoroethanol/water mixture or in the presence of LUV indicated that the propensity of PLA to form α-helical structure is greater than PLL. Consistently, attenuated total reflection-Fourier transform infrared spectroscopy revealed that there is greater α-helical structure in PLA bound to LUV compared to PLL, which has much less ordered structure. Furthermore, isothermal titration calorimetry measurements demonstrated that the contribution of enthalpy to the energetics of binding to LUV is two-fold larger in PLA than in PLL. These results suggest that the stronger interaction of arginine residue with negatively charged phospholipid membranes compared to lysine residue appears to facilitate the conformational change in cationic polypeptide and its insertion into lipid membrane interior.     

Interaction of lipopolysaccharide and phospholipid in mixed membranes: solid-state 31P-NMR spectroscopic and microscopic investigations

Lipopolysaccharide (LPS), which constitutes the outermost layer of Gram-negative bacterial cells as a typical component essential for their life, induces the first line defense system of innate immunity of higher animals. To understand the basic mode of interaction between bacterial LPS and phospholipid cell membranes, distribution patterns were studied by various physical methods of deep rough mutant LPS (ReLPS) of Escherichia coli incorporated in phospholipid bilayers as simple models of cell membranes. Solid-state ³¹P-NMR spectroscopic analysis suggested that a substantial part of ReLPS is incorporated into 1,2-dimyristoyl-sn-glycero-3-phosphocholine lipid bilayers when multilamellar vesicles were prepared from mixtures of these. In egg L-α-phosphatidylcholine (egg-PC)-rich membranes, ReLPS undergoes micellization. In phosphatidylethanolamine-rich membranes, however, micellization was not observed. We studied by microscopic techniques the location of ReLPS in membranes of ReLPS/egg-PC (1:10 M/M) and ReLPS/egg-PC/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG) (1:9:1 M/M/M). The influence of ReLPS on the physicochemical properties of the membranes was studied as well. Microscopic images of both giant unilamellar vesicles and supported planar lipid bilayers showed that LPS was uniformly incorporated in the egg-PC lipid bilayers. In the egg-PC/POPG (9:1 M/M) lipid bilayers, however, ReLPS is only partially incorporated and becomes a part of the membrane in a form of aggregates (or as mixed aggregates with the lipids) on the bilayer surface. The lipid lateral diffusion coefficient measurements at various molar ratios of ReLPS/egg-PC/POPG indicated that the incorporated ReLPS reduces the diffusion coefficients of the phospholipids in the membrane. The retardation of diffusion became more significant with increasing POPG concentrations in the membrane at high ReLPS/phospholipid ratios. This work demonstrated that the phospholipid composition has critical influence on the distribution of added ReLPS in the respective lipid membranes and also on the morphology and physicochemical property of the resulting membranes. A putative major factor causing these phenomena is reasoned to be the miscibility between ReLPS and individual phospholipid compositions.     

Calorimetric investigations of the structural stability and interactions of colicin B domains in aqueous solution and in the presence of phospholipid bilayers

The effects of pH and temperature on the stability of interdomain interactions of colicin B have been studied by differential-scanning calorimetry, circular dichroism, and fluorescence spectroscopy. The calorimetric properties were compared with those of the isolated pore-forming fragment. The unfolding profile of the full-length toxin is consistent with two endothermic transitions. Whereas peak A (T(m) = 55 degrees C) most likely corresponds to the receptor/translocation domain, peak B (T(m) = 59 degrees C) is associated with the pore-forming domain. By lowering the pH from 7 to 3.5, the transition temperature of peaks A and B are reduced by 25 and 18 degrees C, respectively, due to proton exchange upon denaturation. The isolated pore-forming fragment unfolds at much higher temperatures (T(m) = 65 degrees C) and is stable throughout a wide pH range, indicating that intramolecular interactions between the different colicin B domains result in a less stable protein conformation. In aqueous solution circular dichroism spectra have been used to estimate the content of helical secondary structure of colicin B ( approximately 40%) or its pore-forming fragment ( approximately 80%). Upon heating, the ellipticities at 222 nm strongly decrease at the transition temperature. In the presence of lipid vesicles the differential-scanning calorimetry profiles of the pore-forming fragment exhibit a low heat of transition multicomponent structure. The heat of transition of membrane-associated colicin B (T(m) = 54 degrees C at pH 3.5) is reduced and its secondary structure is conserved even at intermediate temperatures indicating incomplete unfolding due to strong protein-lipid interactions.     

Hisactophilin-mediated binding of actin to lipid lamellae: a neutron reflectivity study of protein membrane coupling.

The neutron reflectivity technique is applied to determine the adsorptive interaction of the 13.5-kDa actin-binding protein hisactophilin from Dictyostelium discoideum with lipid monolayers at a lateral pressure of 21 mN/m < or = pi < or = 25 mN/m at the air-water interface. We compare binding of natural hisactophilin exhibiting a myristic acid chain membrane anchor at the N-terminus (DIC-HIS) and a fatty acid-deficient genetic product expressed in Escherichia coli (EC-HIS). It is demonstrated that only the natural hisactophilin DIC-HIS is capable of mediating the strong binding of monomeric actin to the monolayer, where it forms a layer of about 40 A thickness corresponding to the average diameter of actin monomers. Monolayers composed of pure dimyristoyl phosphatidylcholine with fully deuterated hydrocarbon tails and headgroup (DMPC-d67) and 1:1 mixtures of this lipid with chain deuterated dimyristoyl phosphatidylglycerol (DMPG-d54) are studied on subphases consisting either of fully deuterated buffer (D2O) or of a 9:1 H2O/D2O buffer that matches the scattering length density of air (CMA buffer). The reflectivity data are analyzed in terms of layer models, consisting of one to three layers, depending on the contrast of the buffer and the system. We show that both protein species bind tightly to negatively charged 1:1 DMPC-d67/DMPG-d54 monolayers, thereby forming a thin and most probably monomolecular protein layer of 12-15 A thickness. We find that the natural protein (DIC-HIS) partially penetrates into the lipid monolayer, in contrast to chain-deficient species (EC-HIS), which forms only an adsorbed layer. The coverage of the monolayer with DIC-HIS strongly depends on the presence of anionic DMPG in the monolayer. At a bulk protein concentration of 1.5 micrograms/ml, the molar ratio of bound protein to lipid is about 1:45 for the 1:1 lipid mixture but only 1:420 for the pure DMPC.     

Study of the effect of poly(L-lysine) on phosphatidic acid and phosphatidylcholine/phosphatidic acid bilayers by raman spectroscopy

The effect of polylysine (PLL) on dimyristoylphosphatidic acid (DMPA), on dimyristoyl-phosphatidylcholine (DMPC), and on mixtures of these lipids was investigated by Raman spectroscopy. These results show that long polylysine (Mr approximately 200,000) increases the stability of the acyl chain matrix of DMPA to form a more closely packed structure with a stoichiometry of one lysine residue per PA molecule. On the other hand, short PLL (Mr 4000) destabilizes the PA bilayer, and the complex formed undergoes a gel to liquid-crystalline transition at a lower temperature than of the pure lipid. For both cases, we have observed that bound polylysine adopts a beta-sheet conformation as opposed to the alpha-helical structure previously found for dipalmitoylphosphatidylglycerol/long PLL complexes [Carrier, D., & Pézolet, M. (1984) Biophys. J. 46, 497-506]. The difference in the thermal behavior of complexes of DMPA with long and short polylysines is believed to be associated with the fact that in the complex the long polypeptide adopts the beta-sheet conformation over the whole range of temperatures investigated while the short one undergoes a change of conformation from beta-sheet of random coil upon heating. Therefore, the conformation of the lipid-bound polypeptides depends on the nature of the polar head group of the lipid, not only on its net charge, and it affects considerably the thermotropism of the lipid. On the other hand, both long and short polylysines show no affinity for phosphatidylcholine since the temperature profiles of DMPC and of DMPC/PLL complexes exhibit exactly the same behavior.(ABSTRACT TRUNCATED AT 250 WORDS)     

Phase behavior of membranes reconstituted from dipentadecanoylphosphatidylcholine and the Mg2+-dependent, Ca2+-stimulated adenosinetriphosphatase of sarcoplasmic reticulum: evidence for a disrupted lipid domain surrounding protein

A new method was used for reconstituting active sodium deoxycholate solubilized Ca2+-ATPase of rabbit skeletal muscle sarcoplasmic reticulum. Removal of the detergent by dialysis at the pretransition temperature of the pure lipid (22 degrees C) favored the formation of sheet-like structures with a lipid and protein content close to that of the detergent-solubilized sample. Freeze-fracture electron micrographs revealed the Ca2+-ATPase to be organized in rows corresponding to the typical banded pattern seen in low-temperature freeze-fracture micrographs of pure lipid bilayers. Incubation of the sheetlike structures at a temperature (38 degrees C) above the pure lipid main phase transition (33.5 degrees C) caused closure of the sheets into vesicles displaying homogeneous intramembranous particle distributions, at least for membranes containing less than 150 lipids per Ca2+-ATPase. However, in membranes of higher lipid content, free lipid patches were seen both above and below the lipid phase transition. By use of high-sensitivity differential scanning calorimetry, three classes of excess heat capacity peaks were observed in the vesiculated samples. A broadened "free lipid" peak occurred for samples containing between 550 and 200 lipids per protein (Tm = 33.5 degrees C, as for the order-disorder transition in pure lipid vesicles). Between 200 and 150 lipids per Ca2+-ATPase, a broad shoulder became apparent in the range of 29-32 degrees C. Below 150 lipids per Ca2+-ATPase, a peak at 26-28 degrees C became increasingly prominent with lower lipid content. At a lipid to protein ratio of about 30, no peaks in heat capacity were observed. The temperature dependence of diphenylhexatriene fluorescence anisotropy revealed a similar pattern of membrane phase behavior, except that a phase transition was detected at 33.5 degrees C in all membranes studied. On the basis of these observations, we propose that the Ca2+-ATPase is surrounded by a "lipid annulus" of motionally inhibited lipid molecules that do not contribute to a calorimetrically detectable phase transition. Beyond the annulus, "secondary domains" of disrupted lipid packing account for the peak at 26-28 degrees C and the 29-32 degrees C shoulders. At high lipid to protein ratios, the secondary domains coexist with protein-free, lipid-bilayer patches, which account for the peak at 33.5 degrees C.     

Poly-l-lysines and poly-l-arginines induce leakage of negatively charged phospholipid vesicles and translocate through the lipid bilayer upon electrostatic binding to the membrane

Poly-l-lysines (PLL) and poly-l-arginines (PLA) of different polymer chain lengths interact strongly with negatively charged phospholipid vesicles mainly due to their different electrical charges. 1-Palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG), 1,2-dipalmitoyl-sn-glycero-3-phosphoglycerol (DPPG) and their mixtures (1/1 mol/mol) with the respective phosphatidylcholines of equivalent chain length were chosen as model membrane systems that form at room temperature either the fluid L_α or the gel phase L_β lipid bilayer membranes, respectively. Leakage experiments revealed that the fluid POPG membranes are more perturbed compared to the gel phase DPPG membranes upon peptide binding. Furthermore, it was found that pure PG membranes are more prone to release the vesicle contents as a result of pore formation than the lipid mixtures POPG/POPC and DPPG/DPPC. For the longer polymers (≥ 44 amino acids) maximal dye-release was observed when the molar ratio of the concentrations of amino acid residues to charged lipid molecules reached a value of R_P = 0.5, i.e. when the outer membrane layer was theoretically entirely covered by the polymer. At ratios lower or higher than 0.5 leakage dropped significantly. Furthermore, PLL and PLA insertions and/or translocations through lipid membranes were analyzed by using FITC-labeled polymers by monitoring their fluorescence intensity upon membrane binding. Short PLL molecules and PLA molecules of all lengths seemed to translocate through both fluid and gel phase lipid bilayers. Comparison of the PLL and PLA fluorescence assay results showed that PLA interacts stronger with phospholipid membranes compared to PLL. Isothermal titration calorimetry (ITC) measurements were performed to give further insight into these mechanisms and to support the findings obtained by fluorescence assays. Cryo-transmission electron microscopy (cryo-TEM) was used to visualize changes in the vesicles' morphology after addition of the polypeptides.     

Coupled changes between lipid order and polypeptide conformation at the membrane surface. A 2H NMR and Raman study of polylysine-phosphatidic acid systems

Thermotropism and segmental chain order parameters of sn-2-perdeuteriated dimyristoyl-phosphatidic acid (DMPA)-water dispersions, with and without poly(L-lysine) (PLL) of different molecular weights, have been investigated by solid-state deuterium NMR spectroscopy. The segmental chain order parameter profile of this negatively charged lipid is similar to that already found for other lipids. Addition of long PLL (MW = 200,000) increases the temperature, Tc, of the lipid gel-to-fluid phase transition, whereas short PLL (MW = 4000) has practically no effect on Tc. In the fluid phase both varieties of PLL increase the "plateau" character of segmental order parameters up to carbon position 10. At the same reduced temperature, long PLL more significantly increases the segmental ordering, especially at the methyl terminal position. This leads to the conclusion that polar head-group capping and charge neutralization by PLL induce severe changes in lipid chain ordering, even down to the bilayer core. The structure of PLL bound to the lipid bilayer surface was monitored by Raman spectroscopy, following the amide I bands. Results show that the lipid gel-to-fluid phase transition triggers a conformational transition from ordered beta-sheet to random structure of short PLL, while it does not affect the strongly stabilized beta-sheet structure of long PLL. It is concluded that both short and long PLL can efficiently cap and neutralize lipid head groups, whatever their structure, and that peptide length is a key parameter in whether lipids or peptides are the driving force in conformationally coupled changes of both partners in the membrane.     

Apolipophorin III interaction with model membranes composed of phosphatidylcholine and sphingomyelin using differential scanning calorimetry

Apolipophorin III (apoLp-III) from Locusta migratoria was employed as a model apolipoprotein to gain insight into binding interactions with lipid vesicles. Differential scanning calorimetry (DSC) was used to measure the binding interaction of apoLp-III with liposomes composed of mixtures of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) and sphingomyelin (SM). Association of apoLp-III with multilamellar liposomes occurred over a temperature range around the liquid crystalline phase transition (L_α). Qualitative and quantitative data were obtained from changes in the lipid phase transition upon addition of apoLp-III. Eleven ratios of DMPC and SM were tested from pure DMPC to pure SM. Broadness of the phase transition (T_1/2), melting temperature of the phase transition (T_m) and enthalpy were used to determine the relative binding affinity to the liposomes. Multilamellar vesicles composed of 40% DMPC and 60% SM showed the greatest interaction with apoLp-III, indicated by large T_1/2 values. Pure DMPC showed the weakest interaction and liposomes with lower percentage of DMPC retained domains of pure DMPC, even upon apoLp-III binding indicating demixing of liposome lipids. Addition of apoLp-III to rehydrated liposomes was compared to codissolved trials, in which lipids were rehydrated in the presence of protein, forcing the protein to interact with the lipid system. Similar trends between the codissolved and non-codissolved trials were observed, indicating a similar binding affinity except for pure DMPC. These results suggested that surface defects due to non-ideal packing that occur at the phase transition temperature of the lipid mixtures are responsible for apolipoprotein-lipid interaction in DMPC/SM liposomes.     

Interactions of helical polypepetide segments which span the hydrocarbon region of lipid bilayers. Studies of the gramicidin A lipid-water system.

The polypeptide gramicidin A in a dimeric form is considered to form a helical structure which spans the hydrocarbon region of lipid bilayers. In the present investigation it is used as a model for the interactions of the polypeptide segments of transmembrane proteins within the hydrocarbon region of the lipid bilayers of biomembrane structures. A variety of physical techniques (X-ray diffraction, differential scanning calorimetry, optical and electron microscopy, Raman and electron spin resonance spectroscopy) are applied to a study of the interactions of this polypeptide within the phospholipid bilayers of dimyristoyl and dipalmitoyl lecithins in water, at temperatures both above and below the main endothermic phase transition of the pure lipids.Above the transition temperature of the lipid, the Raman studies show that the polypeptide perturbs the fluid lipid environment and causes a marked decrease in the number of gauche isomers of the lipid hydrocarbon chains, even at quite low relative molar concentrations of the polypeptide to lipid (1:150). At concentrations of phospholipid to polypeptide of less than 5:1, the electron spin resonance studies show the existence of two lipid regions within the bilayer. One region corresponds to the relatively fluid lipid region normally observed at these temperatures and the other to a relatively rigid lipid region. The latter is considered to arise from clusters of the polypeptide in which some of the lipid is entrapped.Below the lipid phase transition temperature, the pretransition endotherm observed with pure lipid-water systems is removed by small molar concentrations of the polypeptide (1:50) and the rippled appearance observed in freeze-fracture electron micrographs with pure dimyristoyl lecithin-water dispersions is replaced by a smooth appearance.The main lipid phase transition becomes broadened by the presence of increasing amounts of the polypeptide within the lipid bilayer as indicated by calorimetry, and electron spin resonance spectroscopy. The enthalpy of the lipid transition decreases linearly with increasing amounts of the polypeptide until, with dipalmitoyl lecithin, a concentration of approximately 20 lipids per polypeptide is reached. This is considered to correspond to the onset of an aggregation process which produces localised polypeptide-lipid clusters within the plane of the membrane.At concentrations of polypeptide less than five lipids per polypeptide, freezefracture electron microscopy shows the presence of liposomes with smooth fracture faces. At higher polypeptide concentrations, sheet-like structures are observed with smooth fracture faces.When a mixed lipid-water system (dilauroyl and dipalmitoyl lecithin) containing low concentrations of the polypeptide is slowly cooled, the calorimetric evidence shows that the polypeptide moves preferentially into the lower melting region of the bilayer, whereas at higher polypcptide eoncentrations a mixing of the two lipids takes place.The various results are discussed to provide insight pertinent to the organisation, interactions, aggregation properties, boundary layer and packing arrangements of helical polypeptides and proteins in reconstituted systems and natural biomembranes.     

Interaction between perdeuterated dimyristoylphosphatidylcholine and low molecular weight pulmonary surfactant protein SP-C

A low molecular weight hydrophobic protein was isolated from porcine lung lavage fluid using silicic acid and Sephadex LH-20 chromatography. The protein migrated with an apparent molecular weight of 5000-6000 on SDS-PAGE under reducing and nonreducing conditions. Gels run under reducing conditions also showed a minor band migrating with a molecular weight of 12,000. Amino acid compositional analysis and sequencing data suggest that this protein preparation contains intact surfactant protein SP-C and about 30% of truncated SP-C (N-terminal leucine absent). The surfactant protein was combined with perdeuterated dimyristoylphosphatidylcholine (DMPC-d54) in multilamellar vesicles. The protein enhanced the rate of adsorption of the lipid at air-water interfaces. The ability of the protein to alter normal lipid organization was examined by using high-sensitivity differential scanning calorimetry (DSC) and 2H nuclear magnetic resonance spectroscopy (2H NMR). The calorimetric measurements indicated that the protein caused a decrease in the temperature maximum (Tm) and a broadening of the phase transition. At a protein concentration of 8% (w/w), the enthalpy change of transition was reduced to 4.4 kcal/mol compared to 6.3 kcal/mol determined for the pure lipid. NMR spectral moment studies indicated that protein had no effect on lipid chain order in the liquid-crystal phase but reduced orientational order in the gel phase. Two-phase coexistence in the presence of protein was observed over a small temperature range below the pure lipid transition temperature. Spin-lattice relaxation times (T1) were not substantially affected by the protein. Transverse relaxation time (T2e) studies suggest that the protein influences slow lipid motions.     

Hybrid Bifunctional Protein Based on OmpF Porin and Highly Active Alkaline Phosphatase

To improve the diagnostics of pseudotuberculosis by ELISA, a genetically engineered hybrid bifunctional protein (CmAP/OmpF) was obtained based on the pore-forming protein of the outer membrane of human pathogenic bacterium Yersinia pseudotuberculosis (OmpF) and the highly active alkaline phosphatase of marine bacterium Cobetia amphilecti KMM 296 (CmAP). The OmpF module in the fusion protein retains the properties of the diagnostic antigen of the pseudotuberculosis pathogen, and the CmAP module is an enzyme label for detecting porin complexes with specific antibodies. The CmAP/OmpF activity was successfully confirmed by the binding of antibodies to OmpF porin in murine antisera, as well as in the sera of patients with pseudotuberculosis. The use of hybrid complex CmAP/OmpF for the diagnostics of pseudotuberculosis will eliminate the use of enzyme-labeled secondary antibodies, usually necessary for detecting specific antibodies in the blood serum of patients, and thus simplify the procedure and shorten the analysis time.     

Interaction of non-classical detergents with the mitochondrial porin. A new purification procedure and characterization of the pore-forming unit

The effect of different families of detergents on the solubilization and purification of the pore-forming protein (porin) of the mitochondrial outer membrane of bovine heart was investigated in detail. With Tritons, dimethylamine oxides and zwittergents, porin solubilization with respect to total mitochondrial membrane protein was more efficient with the more hydrophobic members of each series. With most detergents the protein eluted as protein-detergent micelles in the void volume of hydroxyapatite/celite columns. In contrast, the protein was bound to the column material and was eluted after the addition of salt to the elution buffer when the detergents octylglucoside, zwittergent Z-314 and lauryl(dimethyl)-amine oxide were used. The protein purified in the presence of the latter detergent had a higher pore-forming activity in lipid bilayer membranes compared to porin isolated in the presence of Triton X-100. The binding of porin to the hydroxyapatite/celite column was used to study the lipid content of the active pore-forming complex. The analysis revealed that the complex contained no phospholipid but rather five molecules of cholesterol/polypeptide chain.     

Size Influences the Effect of Hydrophobic Nanoparticles on Lung Surfactant Model Systems

The alveolar lung surfactant (LS) is a complex lipid protein mixture that forms an interfacial monolayer reducing the surface tension to near zero values and thus preventing the lungs from collapse. Due to the expanding field of nanotechnology and the corresponding unavoidable exposure of human beings from the air, it is crucial to study the potential effects of nanoparticles (NPs) on the structural organization of the lung surfactant system. In the present study, we investigated both, the domain structure in pure DPPC monolayers as well as in lung surfactant model systems. In the pure lipid system we found that two different sized hydrophobic polymeric nanoparticles with diameter of ∼12 nm and ∼136 nm have contrasting effect on the functional and structural behavior. The small nanoparticles inserted into fluid domains at the LE-LC phase transition are not visibly disturbing the phase transition but disrupting the domain morphology of the LE phase. The large nanoparticles led to an expanded isotherm and to a significant decrease in the line tension and thus to a drastic disruption of the domain structures at a much lower number of nanoparticles with respect to the lipid. The surface activity of the model LS films again showed drastic variations due to presence of different sized NPs illustrated by the film balance isotherms and the atomic force microscopy. AFM revealed laterally profuse multilayer protrusion formation on compression but only in the presence of 136 nm sized nanoparticles. Moreover we investigated the vesicle insertion process into a preformed monolayer. A severe inhibition was observed only in the presence of ∼136 nm NPs compared to minor effects in the presence of ∼12 nm NPs. Our study clearly shows that the size of the nanoparticles made of the same material determines the interaction with biological membranes.     

Colicin N binds to the periphery of its receptor and translocator, outer membrane protein F

Colicins kill Escherichia coli after translocation across the outer membrane. Colicin N displays an unusually simple translocation pathway, using the outer membrane protein F (OmpF) as both receptor and translocator. Studies of this binary complex may therefore reveal a significant component of the translocation pathway. Here we show that, in 2D crystals, colicin is found outside the porin trimer, suggesting that translocation may occur at the protein-lipid interface. The major lipid of the outer leaflet interface is lipopolysaccharide (LPS). It is further shown that colicin N binding displaces OmpF-bound LPS. The N-terminal helix of the pore-forming domain, which is not required for pore formation, rearranges and binds to OmpF. Colicin N also binds artificial OmpF dimers, indicating that trimeric symmetry plays no part in the interaction. The data indicate that colicin is closely associated with the OmpF-lipid interface, providing evidence that this peripheral pathway may play a role in colicin transmembrane transport.     

Influence of poly(l-lysine) on the structure of dipalmitoylphosphatidylglycerol/water dispersions studied by X-ray scattering

The interaction between the negatively charged phospholipid DPPG and positively charged poly(l-lysine) (PLL) of different lengths was studied by X-ray scattering in the SAXS and WAXS region. As a reference pure DPPG (Na salt) was investigated over a wide temperature range (−30 to 70°C). The phase behavior of DPPG in aqueous and in buffer/salt dispersions showed a metastable subgel phase at low temperatures and a recrystallization upon heating before reaching the liquid–crystalline phase. The presence of additional salt stabilizes the bilayer structure and decreases the recrystallization temperature. Large changes in the SAXS region are not connected with changes in chain packing. In DPPG/PLL samples, the PLL is inserted between adjacent headgroup layers and liberates counterions which give rise to a freezing point depression. In the complex with DPPG PLL form an α-helical secondary structure at pH 7 and temperatures below the gel to liquid–crystalline phase transition. This prevents DPPG from recrystallization and strongly increases the stacking order. The lamellar repeat distance is decreased and fixed by the helix conformation of PLL in the gel phase. PLL with n = 14 is too short to form helices and is squeezed out reversibly from the interbilayer space upon cooling by freezing of trapped water. In dispersions with longer PLLs (n > 400) at −20°C a 1D crystallization of PLL α-helices in the aqueous layer between the headgroups takes place. A structural model is presented for the lateral periodic complex, which is similar to the known cationic lipid/DNA complex. Dedicated to Prof. K. Arnold on the occasion of his 65th birthday.     

Fourier transform infrared spectroscopic identification of gel phase domains in reconstituted phospholipid vesicles containing Ca2+-ATPase

Ca2+-ATPase from rabbit sarcoplasmic reticulum has been isolated, purified, and reconstituted into lipid environments containing as primary components 1,2-dielaidoylphosphatidylcholine (DEPC) and acyl-chain perdeuterated 1,2-dimyristoylphosphatidylcholine (DMPC-d54). Differential scanning calorimetry (DSC) has been used to elucidate the phase behavior of this lipid pair while Fourier transform infrared spectroscopy (FT-IR) has been used to monitor the state of each lipid component in the presence of protein. The lipid mixture shows gel state miscibility over at least most of the composition range, a result in good accord with Van Dijck et al. (Biochim. Biophys. Acta 470, 58-69 (1977)), for the binary mixture with proteated DMPC. Acyl chain perdeuteration thus does not greatly alter the miscibility properties of the lipid pair. Reconstitution of Ca2+-ATPase with this lipid pair proceeds with moderate efficiency. Up to 80% of the endogenous lipid can be replaced depending on the lipid composition. Unusual composition-dependent protein-induced effects on lipid melting properties are noticed. At low levels of DMPC-d54, both the DEPC and DMPC-d54 components have their melting processes broadened and shifted to lower temperatures, compared with binary lipid mixtures of the same composition. This suggests that protein perturbs both lipids in similar fashion. At high levels of DMPC-d54, the DEPC component exhibits a highly cooperative melting process at temperatures close to that for pure DEPC. This strongly indicates that domains of DEPC are present (at least at low temperatures) in the bilayer, and that Ca2+-ATPase is excluded from these domains. The protein thus exhibits preferential interaction with the DMPC-d54 component. This work demonstrates the utility of FT-IR for identification of the molecular origin of particular domains in reasonably complex lipid mixtures. The relevance of this work to native membrane systems where lipid domains have been observed by several groups is discussed.     

Domain structure and molecular conformation in annexin V/1,2-dimyristoyl-sn-glycero-3-phosphate/Ca2+ aqueous monolayers: a Brewster angle microscopy/infrared reflection-absorption spectroscopy study.

Annexins comprise a family of proteins that exhibit a Ca2+-dependent binding to phospholipid membranes that is possibly relevant to their in vivo function. Although substantial structural information about the ternary (protein/lipid/Ca2+) interaction in bulk phases has been derived from a variety of techniques, little is known about the temporal and spatial organization of ternary monolayer films. The effect of Ca2+ on the interactions between annexin V (AxV) and anionic DMPA monolayers was therefore investigated using three complementary approaches: surface pressure measurements, infrared reflection-absorption spectroscopy (IRRAS), and Brewster angle microscopy (BAM). In the absence of Ca2+, the injection of AxV into an aqueous subphase beneath a DMPA monolayer initially in a liquid expanded phase produced BAM images revealing domains of protein presumably surrounded by liquid-expanded lipid. The protein-rich areas expanded with time, resulting in reduction of the area available to the DMPA and, eventually, in the formation of condensed lipid domains in spatial regions separate from the protein film. There was thus no evidence for a specific binary AxV/lipid interaction. In contrast, injection of AxV/Ca2+ at a total Ca2+ concentration of 10 microM beneath a DMPA monolayer revealed no pure protein domains, but rather the slow formation of pinhead structures. This was followed by slow (>2 h) rigidification of the whole film accompanied by an increase in surface pressure, and connection of solid domains to form a structure resembling strings of pearls. These changes were characteristic of this specific ternary interaction. Acyl chain conformational order of the DMPA, as measured by nu(sym)CH2 near 2850 cm(-1), was increased in both the AxV/DMPA and AxV/DMPA/Ca2+ monolayers compared to either DMPA monolayers alone or in the presence of Ca2+. The utility of the combined structural and temporal information derived from these three complementary techniques for the study of monolayers in situ at the air/water interface is evident from this work.