Spatial variation in the molecular tilt orientational order within the solid domains of phase-separated, mixed dialkylphosphatidylcholine monolayers

The miscibility of the solid-phase-forming distearoylphosphatidylcholine (DSPC) and the fluid-phase-forming dilauroylphosphatidylcholine (DLPC) at the air/water interface was investigated by the Langmuir film balance. Surface pressure-area isotherms suggest that mixtures containing 25.0-62.5-mol% DLPC (range of composition investigated) are phase-separated. The lateral structure of the DSPC/DLPC monolayers was imaged by Brewster angle microscopy (BAM) as a function of the surface pressure. Quasi-circular condensed domains appeared at pressures between 0 and 0.5mN m(-1), and these structures were already fully developed at approximately 1mN m(-1). Further compression of the monolayers above 1mN m(-1) merely brought the domains closer together. The mixed monolayers consisted of solid domains of DSPC, approximately 3-20 micro in size, in a fluid matrix of DLPC. BAM and the phase contrast mode of intermittent-contact atomic force microscopy (AFM) revealed that the quasi-circular DSPC domains are divided into segments of different reflectivities (BAM) or phase shift (AFM) that arise from abrupt changes in the long-range orientational order of the tilted hydrocarbon chains. The DSPC domains in DSPC/DLPC internally exhibited star and cardioid textures that were heretofore only reported for single-component lipid monolayers in the phase coexistence region.     

Interfacial properties of amphipathic beta strand consensus peptides of apolipoprotein B at oil/water interfaces

The region between residues 968 and 1882 of apolipoprotein B (apoB-21 to apoB-41) is rich in amphipathic beta strands (AbetaSs) and promotes the assembly of primordial triacylglyceride (TAG)-rich lipoproteins. To understand the importance of AbetaS in recruiting TAG, the interfacial properties of two AbetaS consensus peptides, P12 and P27, were studied at dodecane/water (DD/W) and triolein/water (TO/W) interfaces. P12 (acetyl-LSLSLNADLRLK-amide) and P27 (acetyl-LSLSLNADLRLKNGNLSLSLNADLRLK-amide), when added into the aqueous phase surrounding a suspended oil drop (dodecane or triolein), decreased the interfacial tension (gamma) in a concentration-dependent manner. At the DD/W interface, 1 x 10(-5) M P12 decreased gamma to approximately 20 mN/m and 6.6 x 10(-6) M P27 decreased gamma to approximately 13 mN/m. At the TO/W interface, 1.5 x 10(-5) M P12 decreased gamma to approximately 14 mN/m and 9.0 x 10(-6) M P27 decreased gamma to approximately 12 mN/m. The surface area of both peptides was between 11.2 and 15.1 angstroms2 per residue, consistent with beta sheets lying flat on DD/W and TO/W interfaces. P12 and P27 are almost purely elastic on DD/W, TO/W, and air/water interfaces. When P12 and P27 were compressed beyond the equilibrium gamma to as low as 4 mN/m, they could not be readily desorbed from either interface. These properties probably help in assembling nascent TAG-rich lipoproteins, and AbetaS may anchor apoB to beta lipoproteins.     

The interfacial properties of ApoA-I and an amphipathic alpha-helix consensus peptide of exchangeable apolipoproteins at the triolein/water interface

Apolipoprotein A-I (apoA-I) is the major protein in high density lipoprotein (HDL). During lipid metabolism, apoA-I moves among HDL and triacylglycerol-rich lipoproteins. The main structure and the major lipid binding motif of apoA-I is the amphipathic alpha-helix. To understand how apoA-I behaves at hydrophobic lipoprotein interfaces, the interfacial properties of apoA-I and an amphipathic alpha-helical consensus sequence peptide (CSP) were studied at the triolein/water (TO/W) interface. CSP ((PLAEELRARLRAQLEELRERLG)2-NH2) contains two 22-residue tandem repeat sequences that form amphipathic alpha-helices modeling the central part of apoA-I. ApoA-I or CSP added into the aqueous phase surrounding a triolein drop lowered the interfacial tension (gamma) of TO/W in a concentration- and time-dependent fashion. The gamma(TO/W) was lowered approximately 16 millinewtons (mN)/m by apoA-I at 1.4 x 10(-6) m and approximately 15 mN/m by CSP at 2.6 x 10(-6) m. At equilibrium gamma, both apoA-I and CSP desorbed from the interface when compressed and readsorbed when expanded. The maximum surface pressure CSP could withstand without being ejected (PiMAX) was 16 mN/m. The PiMAX) of apoA-I was only 14.8 mN/m, but re-adsorption kinetics suggested that only part of the apoA-I desorbed at Pi between 14.8 and 19 mN/m. However, above approximately 19 mN/m (PiOFF) the entire apoA-I molecule desorbed into the water. ApoA-I was more flexible at the TO/W interface than CSP and showed more elasticity at oscillation periods 4-128 s even at high compression, whereas CSP was elastic only at faster periods (4 and 8 s) and moderate compression. Flexibility and surface pressure-mediated desorption and re-adsorption of apoA-I probably provides lipoprotein stability during metabolic-remodeling reactions in plasma.     

Palmitoylation of a pulmonary surfactant protein C analogue affects the surface associated lipid reservoir and film stability

Surfactant protein C (SP-C) is a lipopeptide that contains two thioester-linked palmitoyl groups and is considered to be important for formation of the alveolar surface active lipid film. Here, a non- or dipalmitoylated SP-C analogue (SP-C(Leu)), in which all helical Val residues were replaced with Leu and Cys-5 and Cys-6 were replaced with Ser, was tested for surface activity in a captive bubble system (CBS). SP-C(Leu), either palmitoylated at Ser-5 and Ser-6 or non-palmitoylated, was added to mixtures of 1, 2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC)/phosphatidyl glycerol (PG)/palmitic acid (PA), 68:22:9, (by mass) at a concentration of 2 and 5%. With 2% peptide, surface film formation was rapid, reaching a surface tension below 25 mN/m within 5 s, but the samples with 5% SP-C(Leu) required more than 20 s to reach values below 25 mN/m. Minimum surface tension for the samples with dipalmitoylated SP-C(Leu) was below 1.5 mN/m and very stable, as the surface tension increased by less than 0.5 mN/m within 10 min at constant bubble volume. Minimum surface tension for the non-palmitoylated SP-C(Leu) was approximately 2 and 5 mN/m for 2 and 5% peptide, respectively, but the films were less stable as seen by frequent bubble clicking at low surface tensions. Films with dipalmitoylated SP-C(Leu) that were dynamically cycled at 20-30 cycles/min were substantially less compressible at a surface tension of 20 mN/m (0.007 m/mN) than those that contained the non-palmitoylated peptide (0.02 m/mN). After subphase depletion, the incorporation of lipids into the surface active film during initial bubble expansion occurred at a relatively low surface tension (about 35 mN/m) for the samples with dipalmitoylated SP-C(Leu) compared to approximately 45 mN/m for those containing the non-palmitoylated peptide. Furthermore, for samples that contained non-palmitoylated SP-C(Leu), the ability to reach near zero stable surface tension was lost after a few adsorption steps, whereas with the dipalmitoylated peptide the film quality did not deteriorate even after more than 10 expansion steps and the incorporation of reservoir material equivalent to more than two monolayers. It appears that the covalently linked palmitoyl groups of the SP-C analogue studied are important for the mechanical stability of the lipid film, for the capacity to incorporate material from the reservoir into the surface active film upon area expansion, and for the low film compressibility of dynamically cycled films.     

Surface properties of rat pulmonary surfactant studied with the captive bubble method: adsorption, hysteresis, stability.

Surface tension-area relations from pulmonary surfactant were obtained with a new apparatus that contains a leak free captive bubble of controllable size. Rat pulmonary surfactant was studied at phospholipid concentrations of 50, 200 and 400 micrograms/ml. At the highest concentration, adsorption was rapid, reaching surface tensions below 30 mN/m within 1 s, while at the lowest concentration, approximately 3 min were required. Upon a first quasi static or dynamic compression, stable surface tensions below 1 mN/m could be obtained by a film area reduction of approximately 50%. After three to four cycles the surface tension-area relations became stationary, and the tension fell from 25-30 to approximately 1 mN/m for a film area reduction of less than 20%. Hysteresis became negligible, provided the films were not collapsed by further area reduction. Under these conditions, the films could be cycled for more than 20 min without any noticeable loss in surface activity. After only three to four consecutive cycles, surfactant films exhibited the low surface tensions, collapse rates and compressibilities characteristic of alveolar surfaces in situ. Remarkably, surface tension and area are interrelated in the captive bubble which may promote low and stable surface tensions. If the surface tension of the captive bubble suddenly increases ('click') because of mechanical vibration or unstable surfactant, the bubble shape changes from flat to more spherical. The associated isovolumetric decrease in surface area prevents the surface tension from rising as much as it would have in a constant-area situation. This feedback mechanism may also have a favorable effect in stabilizing alveolar surface tension at low lung volumes.     

The detrimental effect of serum albumin on the re-spreading of a dipalmitoyl phosphatidylcholine Langmuir monolayer is counteracted by a fluorocarbon gas

We have recently reported that fluorocarbon gases exhibit an effective fluidizing effect on Langmuir monolayers of dipalmitoyl phosphatidylcholine (DPPC), preventing them from crystallizing up to surface pressures of approximately 40 mN m(-1), i.e. well above the DPPC's equilibrium surface pressure. We now report that gaseous perfluorooctyl bromide (gPFOB) promotes the re-spreading of DPPC Langmuir monolayers compressed on a bovine serum albumin (BSA)-containing sub-phase. The latter protein is known to maintain a concentration-dependent surface pressure that can exceed the re-spreading pressure of collapsed monolayers. This phenomenon was proposed to be responsible for lung surfactant inactivation. Compression/expansion isotherms and fluorescence microscopy experiments were carried out to assess the monolayers' physical state. We have found that, during expansion under gPFOB-containing air, the surface pressure of a DPPC monolayer on a BSA-containing sub-phase decreased to much lower values than when the DPPC monolayer was expanded in the presence of BSA under air ( approximately 0 mN m(-1) vs. approximately 7.5 mN m(-1) at 120 A(2), respectively). Moreover, fluorescence images showed that, during expansion, the BSA-coupled DPPC monolayers, in contact with gPFOB, remained in the liquid-expanded state for surface pressures lower than 10 mN m(-1), whereas they were in a liquid-condensed semi-crystalline state, even at large molecular areas (120 A(2)), when expanded under air. The re-incorporation of the PFOB molecules in the DPPC monolayer during expansion thus competes with the re-incorporation of BSA, thus preventing the latter from penetrating into the DPPC monolayer. We suggest that combinations of DPPC and a fluorocarbon gas may be useful in the treatment of lung conditions resulting from a deterioration of the native lung surfactant function due to plasma proteins, such as in the acute respiratory distress syndrome.     

Investigations into the membrane interactions of m-calpain domain V

m-calpain is a calcium-dependent heterodimeric protease implicated in a number of pathological conditions. The activation of m-calpain appears to be modulated by membrane interaction, which has been predicted to involve oblique-orientated alpha-helix formation by a GTAMRILGGVI segment located in domain V of the protein's small subunit. Here, we have investigated this prediction. Fourier transform infrared conformational analysis showed that VP1, a peptide homolog of this segment, exhibited alpha-helicity of approximately 45% in the presence of dimyristoylphosphatidylcholine/dimyristoylphosphatidylserine (DMPS) vesicles. The level of helicity was unaffected over a 1- to 8-mM concentration range and did not alter when the anionic lipid composition of these vesicles was varied between 1% and 10% DMPS. Similar levels of alpha-helicity were observed in trifluoroethanol and the peptide appeared to adopt alpha-helical structure at an air/water interface with a molecular area of 164 A(2) at the monolayer collapse pressure. VP1 was found to penetrate dimyristoylphosphatidylcholine/DMPS monolayers, and at an initial surface pressure of 30 mN m(-1), the peptide induced surface pressure changes in these monolayers that correlated strongly with their anionic lipid content (maximal at 4 mN m(-1) in the presence of 10% DMPS). Neutron diffraction studies showed VP1 to be localized at the hydrophobic core of model palmitoyloleylphosphatidylcholine/palmitoyloleylphosphatidylserine (10:1 molar ratio) bilayer structures and, in combination, these results are consistent with the oblique membrane penetration predicted for the peptide. It would also appear that although not needed for structural stabilization anionic lipid was required for membrane penetration.     

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.     

The N-terminal (1-44) and C-terminal (198-243) peptides of apolipoprotein A-I behave differently at the triolein/water interface

Apolipoprotein A-I (apoA-I), the major protein of high-density lipoprotein (HDL), moves between HDL and triacylglycerol-rich lipoproteins during metabolism. We reported that apoA-I is conformationally flexible at the triolein/water (TO/W) interface, partially desorbing at low surface pressure (Pi) but totally desorbing at Pi > 19 mN/m. We now report the different behavior of the N- and C-terminal peptides of apoA-I ([1-44]apoA-I and [198-243]apoA-I) at the TO/W interface. While both peptides are surface active, [198-243]apoA-I is more stable at the TO/W interface. At equilibrium interfacial tension both peptides desorb from the interface when compressed, but [1-44]apoA-I is pushed off at 13 mN/m while [198-243]apoA-I can withstand Pi = 16 mN/m. Neither peptide is very elastic or flexible at the interface. Only at small changes of area (<8%), fast oscillations (4 and 8 s periods), and relatively low concentrations (2 x 10(-7) M) do these peptides show elastic behavior but with a relatively small modulus compared to that of apoA-I. When mixed together, they appear not to interact on the surface. [1-44]ApoA-I binds more rapidly but is replaced by [198-243]apoA-I within minutes. We suggest that when apoA-I partially desorbs from lipoprotein surfaces during lipid metabolism, the N-terminal is the first to detach while the C-terminal remains on the interface and only desorbs at higher pressures. Thus, the observations that different domains of apoA-I adsorb or desorb with small variations in surface pressure make apoA-I a very flexible protein with multiple functions, one of which is to stabilize surface pressure during lipoprotein metabolism as lipids move in and out of the lipoprotein surface.     

Formation of three-dimensional protein-lipid aggregates in monolayer films induced by surfactant protein B

This study focuses on the structural organization of surfactant protein B (SP-B) containing lipid monolayers. The artificial system is composed of the saturated phospholipids dipalmitoylphosphatidylcholine (DPPC) and dipalmitoylphosphatidylglycerol (DPPG) in a molar ratio of 4:1 with 0.2 mol% SP-B. The different "squeeze-out" structures of SP-B were visualized by scanning probe microscopy and compared with structures formed by SP-C. Particularly, the morphology and material properties of mixed monolayers containing 0.2 mol% SP-B in a wide pressure range of 10 to 54 mN/m were investigated revealing that filamentous domain boundaries occur at intermediate surface pressure (15-30 mN/m), while disc-like protrusions prevail at elevated pressure (50-54 mN/m). In contrast, SP-C containing lipid monolayers exhibit large flat protrusions composed of stacked bilayers in the plateau region (app. 52 mN/m) of the pressure-area isotherm. By using different scanning probe techniques (lateral force microscopy, force modulation, phase imaging) it was shown that SP-B is dissolved in the liquid expanded rather than in the liquid condensed phase of the monolayer. Although artificial, the investigation of this system contributes to further understanding of the function of lung surfactant in the alveolus.     

Quantitative Brewster angle microscopy of the surface film of human broncho-alveolar lavage fluid

The morphology, thickness and surface pressure of the surfactant film of broncho-alveoalar lavage (BAL) fluid from patients with sarcoidosis were investigated during spontaneous adsorption of the BAL's surface active material at the air/aqueous buffer interface at 37 degrees C. The biochemical parameters of the BAL fluid determined were protein (Lowry), total phospholipids (from phosphate after ashing) and the individual phospholipids (HPLC). During the spontaneous adsorption of the pulmonary surfactant the surface pressure increased from initially 26 mN/m to 44 mN/m in the equilibrium state. Simultaneously to the increase of the surface pressure, a continuous increase of the reflectivity signal was observed by quantitative Brewster angle microscopy (BAM). The film thickness is calculated from the reflectivity values using an optical model. The effect of the uncertainty of the refractive index, which has to be estimated, is discussed. The BAM images show the inhomogeneous nature of the surfactant film with three distinct phases of different reflectivity, even at relatively low surface pressures. For the brightest phase, the thickness amounts to approximately 12 nm in the equilibrium state of adsorption. This suggests a multilamellar structure. Additionally, we found visual evidence for an adsorption mechanism involving the spreading of vesicles at the interface, in agreement with published results. Differences in the morphology and thickness of the pulmonary surfactant film reported in the literature are obviously due to the varying experimental conditions and materials. We think that the experimental conditions chosen in our study provide a more realistic view of the structure in the lungs in vivo.     

Lateral phase separation in interfacial films of pulmonary surfactant.

To determine if lateral phase separation occurs in films of pulmonary surfactant, we used epifluorescence microscopy and Brewster angle microscopy (BAM) to study spread films of calf lung surfactant extract (CLSE). Both microscopic methods demonstrated that compression produced domains of liquid-condensed lipids surrounded by a liquid-expanded film. The temperature dependence of the pressure at which domains first emerged for CLSE paralleled the behavior of its most prevalent component, dipalmitoyl phosphatidylcholine (DPPC), although the domains appeared at pressures 8-10 mN/m higher than for DPPC over the range of 20-37 degrees C. The total area occupied by the domains at room temperature increased to a maximum value at 35 mN/m during compression. The area of domains reached 25 +/- 5% of the interface, which corresponds to the predicted area of DPPC in the monolayer. At pressures above 35 mN/m, however, both epifluorescence and BAM showed that the area of the domains decreased dramatically. These studies therefore demonstrate a pressure-dependent gap in the miscibility of surfactant constituents. The monolayers separate into two phases during compression but remain largely miscible at higher and lower surface pressures.     

Discrepancy between phase behavior of lung surfactant phospholipids and the classical model of surfactant function

The studies reported here used fluorescence microscopy and Brewster angle microscopy to test the classical model of how pulmonary surfactant forms films that are metastable at high surface pressures in the lungs. The model predicts that the functional film is liquid-condensed (LC) and greatly enriched in dipalmitoyl phosphatidylcholine (DPPC). Both microscopic methods show that, in monolayers containing the complete set of phospholipids from calf surfactant, an expanded phase persists in coexistence with condensed domains at surface pressures approaching 70 mN/m. Constituents collapsed from the interface above 45 mN/m, but the relative area of the two phases changed little, and the LC phase never occupied more than 30% of the interface. Calculations based on these findings and on isotherms obtained on the continuous interface of a captive bubble estimated that collapse of other constituents increased the mol fraction of DPPC to no higher than 0.37. We conclude that monolayers containing the complete set of phospholipids achieve high surface pressures without forming a homogeneous LC film and with a mixed composition that falls far short of the nearly pure DPPC predicted previously. These findings contradict the classical model.     

Mitochondrial creatine kinase interaction with heterogeneous monolayers: Effect on lipid lateral organization

Our study highlights the tight relationship between protein binding to monolayers and the phase-state of the phospholipids. Interaction of mitochondrial creatine kinase with phospholipidic membranes was analysed using a two-phase monolayer system containing anionic phospholipids under chain mismatch conditions. Monolayers were made up of mixtures of DMPC/DPPG or DPPC/DMPG containing 40% negatively charged phospholipids which is approximately the negative charge content of the mitochondrial inner membrane. Langmuir isotherms of these monolayers showed that they underwent a phase transition from a liquid expanded state to a liquid-condensed phase at about 2 mN/m and 5 mN/m respectively. Interface morphology modifications caused by injection of mtCK under these monolayers at low or high surface pressure were monitored by Brewster angle microscopy. This work provides evidence that the presence at the air/water interface of discrete domains with increased charge density, may lead to difference in partition of soluble proteins such as mtCK, interacting with the lipid monolayer. Conversely these proteins may help to organize charged phospholipid domains in a membrane.     

Binding of a neuropeptide, substance P, to neutral and negatively charged lipids

The binding of substance P (SP), a positively charged neurotransmitter peptide, to neutral and to negatively charged phospholipids has been investigated by means of a monolayer technique. Monolayers formed at room temperature from 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG) or 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), or mixtures of the two, were maintained throughout the course of a binding experiment at a constant surface pressure while the monolayer surface area was monitored. Injection of SP into the aqueous subphase (154 mM NaCl, 10 mM Tris adjusted to pH 7.4) led to an expansion of the monolayer surface area that was attributed to a spontaneous insertion of SP between the lipid molecules. A quantitative evaluation of the area increase at constant pressure yielded SP insertion isotherms that showed that levels of SP insertion increased directly with the monolayer POPG content and decreased to negligible levels at surface pressures above 35 +/- 1 mN/m. If electrostatic effects were ignored, these data showed biphasic behavior in Scatchard plots. The apparent binding constants ranged, at 20 mN/m, from (3.2 +/- 0.3) X 10(4) M-1 for 100% POPG monolayers to (2.0 +/- 0.05) X 10(3) M-1 for 25% POPG/75% POPC monolayers. At 32 mN/m, a monolayer surface pressure that mimics bilayer conditions, the apparent binding constant for a 100% POPG monolayer was measured to be (1.1 +/- 0.05) X 10(3) M-1. However, for a monolayer containing only 25% charged lipids, corresponding to a natural membrane composition, K app at 32 mN/m was estimated to be at most 41 M-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Equivalent Aqueous Phase Modulation of Domain Segregation in Myelin Monolayers and Bilayer Vesicles

Purified myelin can be spread as monomolecular films at the air/aqueous interface. These films were visualized by fluorescence and Brewster angle microscopy, showing phase coexistence at low and medium surface pressures (<20-30 mN/m). Beyond this threshold, the film becomes homogeneous or not, depending on the aqueous subphase composition. Pure water as well as sucrose, glycerol, dimethylsulfoxide, and dimethylformamide solutions (20% in water) produced monolayers that become homogeneous at high surface pressures; on the other hand, the presence of salts (NaCl, CaCl₂) in Ringer's and physiological solution leads to phase domain microheterogeneity over the whole compression isotherm. These results show that surface heterogeneity is favored by the ionic milieu. The modulation of the phase-mixing behavior in monolayers is paralleled by the behavior of multilamellar vesicles as determined by small-angle and wide-angle x-ray scattering. The correspondence of the behavior of monolayers and multilayers is achieved only at high surface pressures near the equilibrium adsorption surface pressure; at lower surface pressures, the correspondence breaks down. The equilibrium surface tension on all subphases corresponds to that of the air/alkane interface (27 mN/m), independently on the surface tension of the clean subphase.     

Polarization-modulated FTIR spectroscopy of lipid/gramicidin monolayers at the air/water interface

Monolayers of gramicidin A, pure and in mixtures with dimyristoylphosphatidylcholine (DMPC), were studied in situ at the air/H2O and air/D2O interfaces by polarization-modulated infrared reflection absorption spectroscopy (PM-IRRAS). Simulations of the entire set of amide I absorption modes were also performed, using complete parameter sets for different conformations based on published normal mode calculations. The structure of gramicidin A in the DMPC monolayer could clearly be assigned to a beta6.3 helix. Quantitative analysis of the amide I bands revealed that film pressures of up to 25-30 mN/m the helix tilt angle from the vertical in the pure gramicidin A layer exceeded 60 degrees. A marked dependence of the peptide orientation on the applied surface pressure was observed for the mixed lipid-peptide monolayers. At low pressure the helix lay flat on the surface, whereas at high pressures the helix was oriented almost parallel to the surface normal.     

Kinetic properties of turkey pancreatic lipase: a comparative study with emulsified tributyrin and monomolecular dicaprin

Using the classical emulsified system and the monomolecular film technique, we compared several interfacial properties of turkey pancreatic lipase (TPL) and human pancreatic lipase (HPL). TPL, like HPL, presented the interfacial activation phenomenon when vinyl ester was used as substrate. In the absence of colipase and bile salts, using tributyrin emulsion or monomolecular films of dicaprin at low surface pressure, TPL, unlike HPL, hydrolyzes pure tributyrin emulsion as well as dicaprin films maintained at low surface pressures. TPL was also able to hydrolyze triolein emulsion in the absence of any additive and despite the accumulation of long-chain free fatty acids at the interface. The difference of behaviors between TPL and HPL can be explained by the penetration power of each enzyme. The enzyme that presents the maximal pi(c) (TPL) interacts more efficiently with interfaces, and it is not denaturated at high interfacial energy. Turkey pancreatic lipase is more active on rac-dicaprin than HPL; a maximal ratio of 9 was found between the catalytic activities of the two lipases measured at their surface pressure optima (20 mN m(-1)). A kinetic study on the surface pressure dependency, stereospecificity, and regioselectivity of TPL was performed using enantiopure diglyceride (1,2-sn-dicaprin and 2,3-sn-dicaprin) and a prochiral isomer (1,3-dicaprin) that were spread as monomolecular films at the air-water interface. At low surface pressure (15 mN m(-1)), TPL acts preferentially on primary carboxylic ester groups of the diglyceride isomers (1,3-dicaprin), but at high surface pressure (23 mN m(-1)), this enzyme prefers both adjacent ester groups of the diglyceride isomers (1,2-sn-dicaprin and 2,3-sn-dicaprin). HPL prefers adjacent ester groups of the diglyceride isomers (1,2-sn-dicaprin and 2,3-sn-dicaprin). Furthermore, TPL was found to be markedly stereospecific for the sn-1 position of the 1,2-sn-enantiomer of dicaprin at low surface pressure (15 mN m(-1)), while at high surface pressure (23 mN m(-1)), this lipase presents a stereopreference for the sn-3 position of the 2,3-sn-enantiomer of dicaprin. HPL is stereospecific for the sn-1 position of the 1,2-sn-enantiomer of dicaprin both at 15 and 23 mN m(-1).     

Effect of calcium and temperature on mixed lipid-valinomycin monolayers. A comparison of glycosphingolipids (ganglioside GT1b, sulphatides) and phosphatidylcholine

The influence of calcium and temperature on pure lipid (bovine brain PC, sulphatides, ganglioside GT1b), valinomycin and mixed lipid-valinomycin monolayers at the air/water interface was studied. In mixed films, evidence was found that the two components were miscible. On the other hand, at higher surface pressures, phase separation occurs in the cases of PC and sulphatides. Measuring the area requirement and the collapse pressure the stability of both lipid and the peptide was increased in particular due to ganglioside-valinomycin interaction. The addition of 10(-5) M calcium into the subphase at 20 and 37 degrees C and surface pressures of 10 and 20 mN/m led to a condensing effect in ganglioside mixtures, with formation of aggregates as indicated also by the nearly ideal behaviour of two component monolayers.     

Secondary structure of spiralin in solution, at the air/water interface, and in interaction with lipid monolayers

The surface of spiroplasmas, helically shaped pathogenic bacteria related to the mycoplasmas, is crowded with the membrane-anchored lipoprotein spiralin whose structure and function are unknown. In this work, the secondary structure of spiralin under the form of detergent-free micelles (average Stokes radius, 87.5 A) in water and at the air/water interface, alone or in interaction with lipid monolayers was analyzed. FT-IR and circular dichroism (CD) spectroscopic data indicate that spiralin in solution contains about 25+/-3% of helices and 38+/-2% of beta sheets. These measurements are consistent with a consensus predictive analysis of the protein sequence suggesting about 28% of helices, 32% of beta sheets and 40% of irregular structure. Brewster angle microscopy (BAM) revealed that, in water, the micelles slowly disaggregate to form a stable and homogeneous layer at the air/water interface, exhibiting a surface pressure up to 10 mN/m. Polarization modulation infrared reflection absorption spectroscopy (PMIRRAS) spectra of interfacial spiralin display a complex amide I band characteristic of a mixture of beta sheets and alpha helices, and an intense amide II band. Spectral simulations indicate a flat orientation for the beta sheets and a vertical orientation for the alpha helices with respect to the interface. The combination of tensiometric and PMIRRAS measurements show that, when spiroplasma lipids are used to form a monolayer at the air/water interface, spiralin is adsorbed under this monolayer and its antiparallel beta sheets are mainly parallel to the polar-head layer of the lipids without deep perturbation of the fatty acid chains organization. Based upon these results, we propose a 'carpet model' for spiralin organization at the spiroplasma cell surface. In this model, spiralin molecules anchored into the outer leaflet of the lipid bilayer by their N-terminal lipid moiety are composed of two colinear domains (instead of a single globular domain) situated at the lipid/water interface. Owing to the very high amount of spiralin in the membrane, such carpets would cover most if not all the lipids present in the outer leaflet of the bilayer.