Effects of hydrostatic pressure on bilayer phase behavior and dynamics of dilauroylphosphatidylcholine

Formation of intermediate gel-liquid crystalline phase on medium-chain phosphatidylcholine bilayers: Phase transitions depending on the bilayer packing

The bilayer phase transitions of medium-chain phosphatidylcholines with linear saturated acyl chains (C_n = 12, 13 and 14) were measured by high-pressure light-transmittance measurements and differential scanning calorimetry to investigate the formation of intermediate gel-liquid crystalline phase called L_x phase. The constructed phase diagrams showed that there existed a distinct region of the L_x phase between ripple gel (P_β') and liquid crystalline (L_α) phase for multilamellar vesicle bilayers of C12PC and C13PC. The L_x phase of the C12PC bilayer was metastable at all pressures and disappeared at a higher pressure. In the C13PC bilayer, the L_x phase was stable and also disappeared at a higher pressure but its region markedly shrunk. By contrast, the L_x phase was not detected for the C14PC bilayer. Effects of other factors such as vesicle size and solvent substitution on the L_x phase of the C13PC bilayer were also examined. A decrease in vesicle size and solvent substitution from water to 50 wt% ethylene glycol solution promoted the L_x-phase formation as opposed to the effects of acyl-chain elongation and pressurization. The fluorescence data of the C13PC bilayer with different vesicle sizes showed that the L_x phase is caused by the difference of local packing in the bilayer. Considering these facts, we concluded that the L_x phase is an intermediate gel-L_α phase that has gel-phase monolayers with negative curvature and L_α-phase monolayers with positive curvature. The formation mechanism of the L_x-phase in stacked bilayers and dispersed vesicles is also explainable by this difference in packing state.

Effect of chain unsaturation on bilayer response to pressure

Using wide-line deuterium NMR, the effects of pressure on saturated-chain orientational order and gel-to-liquid-crystal phase transition temperature were observed in bilayers of 16:0-18:1 PC-d31 (POPC-d31) and 16:0-18:2 PC-d31 (PLPC-d31). Spectra were recorded for a range of pressures at selected temperatures and for a range of temperatures at selected pressures up to 193 MPa. For 16:0-18:1 PC-d31, the main transition temperature increased by approximately 0.18 K/MPa, a rate that is similar to what is found for bilayers of disaturated PC's. For 16:0-18:2 PC-d31, the increase in transition temperature with pressure was slightly smaller at approximately 0.13 K/MPa. To investigate the isothermal response of chain orientational order to pressure, spectra for each lipid were obtained for three pressures (ambient, 55 MPa, and 110 MPa) near room temperature (approximately 25 degrees C) and for three pressures (ambient, 110 MPa, and 193 MPa) at higher temperature (approximately 40 degrees C). These temperatures were chosen such that the difference between the higher observation temperature and the main transition of 16:0-18:1 PC-d31 would be similar to the difference between the lower observation temperature and the main transition of 16:0-18:2 PC-d31. Application of a given pressure was found to raise the orientational order for all methylene groups on the saturated chain of a particular lipid by roughly similar amounts. For comparable pressure differences, the pressure-induced ordering of the 16:0-18:1 PC-d31 saturated chain at approximately 40 degrees C was greater than that of the corresponding chain in 16:0-18:2 PC- d31 at approximately 25 degrees C. These observations suggest that increasing levels of chain unsaturation may reduce the sensitivity of bilayer order to variations in pressure at corresponding temperatures relative to their ambient pressure transitions.

Relationship between the unbinding and main transition temperatures of phospholipid bilayers under pressure

Using neutron diffraction and a specially constructed high pressure cell suitable for aligned multibilayer systems, we have studied, as a function of pressure, the much observed anomalous swelling regime in dimyristoyl- and dilauroyl-phosphatidylcholine bilayers, DMPC and DLPC, respectively. We have also reanalyzed data from a number of previously published experiments and have arrived at the following conclusions. (a). The power law behavior describing anomalous swelling is preserved in all PC bilayers up to a hydrostatic pressure of 240 MPa. (b). As a function of increasing pressure there is a concomitant decrease in the anomalous swelling of DMPC bilayers. (c). For PC lipids with hydrocarbon chains >or=13 carbons the theoretical unbinding transition temperature T small star, filled is coupled to the main gel-to-liquid crystalline transition temperature T(M). (d). DLPC is intrinsically different from the other lipids studied in that its T small star, filled is not coupled to T(M). (e). For DLPC bilayers we predict a hydrostatic pressure (>290 MPa) where unbinding may occur.

Pressure-induced ordering in mixed-lipid bilayers

Isothermal application of hydrostatic pressure to liquid crystalline phospholipid bilayers increases chain segment orientational order and thus chain extension. By using pressure to perturb chain order in single-component bilayers and bilayers comprising a binary mixture of lipids, it is possible to compare the relative influences of intrinsic lipid properties and collective bilayer properties on chain orientational order. Deuterium nuclear magnetic resonance was used to investigate the response of saturated chain orientational order to pressure in single-component and two-component liquid crystal bilayers of lipids having saturated chains of different lengths (dipalmitoyl phosphatidylcholine and dimyristoyl phosphatidylcholine) or having one saturated chain and one unsaturated chain (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine). For bilayers containing a single lipid species, the isothermal response of average chain orientational order to pressure decreased with increasing difference between measurement temperature and that lipid's ambient-pressure gel-to-liquid-crystalline phase transition temperature. For all of the lipids observed, the range of orientational order displayed by the saturated chain methylene groups was approximately conserved as pressure was applied. In binary mixtures, the difference between the average saturated chain orientational orders of the two bilayer components was approximately conserved as pressure was increased. These observations provide some insight into how the response of the bilayer to pressure is distributed over interacting components with different intrinsic properties and illustrate the sensitivity of the effective chain ordering potential in the bilayer interior to bilayer composition.

Effects of the eukaryotic pore-forming cytolysin Equinatoxin II on lipid membranes and the role of sphingomyelin

Equinatoxin II (EqtII), a protein toxin from the sea anemone Actinia equina, readily creates pores in sphingomyelin-containing lipid membranes. The perturbation by EqtII of model lipid membranes composed of dimyristoylphosphatidycholine and sphingomyelin (10 mol %) was investigated using wideline phosphorus-31 and deuterium NMR. The preferential interaction between EqtII (0.1 and 0.4 mol %) and the individual bilayer lipids was studied by (31)P magic angle spinning NMR, and toxin-induced changes in bilayer morphology were examined by freeze-fracture electron microscopy. Both NMR and EM showed the formation of an additional lipid phase in sphingomyelin-containing mixed lipid multilamellar suspensions with 0.4 mol % EqtII. The new toxin-induced phase consisted of small unilamellar vesicles 20-40 nm in diameter. Deuterium NMR showed that the new lipid phase contains both dimyristoylphosphatidycholine and sphingomyelin. Solid-state (31)P NMR showed an increase in spin-lattice and a decrease in spin-spin relaxation times in mixed-lipid model membranes in the presence of EqtII, consistent with an increase in the intensity of low frequency motions. The (2)H and (31)P spectral intensity distributions confirmed a change in lipid mobility and showed the creation of an isotropic lipid phase, which was identified as the small vesicle structures visible by electron microscopy in the EqtII-lipid suspensions. The toxin appears to enhance slow motions in the membrane lipids and destabilize the membrane. This effect was greatly enhanced in sphingomyelin-containing mixed lipid membranes compared with pure phosphatidylcholine bilayers, suggesting a preferential interaction between the toxin and bilayer sphingomyelin.

Condensed lamellar phase in ternary DNA-DLPC-cationic gemini surfactant system: a small-angle synchrotron X-ray diffraction study

We report on a small-angle synchrotron X-ray diffraction study of dilauroylphosphatidylcholine (DLPC) liposomes aggregated with high molecular DNA in the presence of 1,4-butanediammonium-N,N'-dilauryl-N,N,N',N'-tetramethyl gemini surfactant cations (C12GS). The aggregates prepared at the DLPC/C12GS/DNA phosphate group=2:1:1.6 molar ratio in 0.0015 mol x l(-1) NaCl aqueous solution exhibit Bragg reflections due to lamellar lipid bilayer stacking and the Bragg reflection typical of one-dimensional DNA lattice with parallel strands intercalated between lipid bilayers. In this condensed fluid lamellar L(alpha)(c) phase, the interactions between DNA and charged bilayers damp the thermally induced bilayer undulations. The diffraction data obtained with the mixture of DLPC liposomes and DNA (at DNA phosphate group/DLPC=0.8:1 molar ratio) indicate a DNA-lipid interaction in the absence of C12GS.

The effects of osmotic and hydrostatic pressures on macromolecular systems

Osmotic pressure and hydrostatic pressure can be used effectively to probe the behavior of biologically important macromolecules and their complexes. Using the two techniques requires a theoretical framework as well as knowledge of the more common pitfalls. Both are discussed in this review in the context of several examples.

Theory of the generalized dynamic structure factor of polyatomic molecular fluids measured by inelastic x-ray scattering

We describe a theory for the calculation of the generalized dynamic structure factor S(k,omega) as measured by an inelastic x-ray scattering (IXS) experiment on single-component molecular or polyatomic molecular fluids. IXS spectrum of a simple fluid is proportional to the dynamic structure factor of a single species of atom. In the case of a molecular fluid, however, IXS spectrum is a weighted sum of partial dynamic structure factors of pairs of atomic species. The weighting factors are products of the atomic form factors of the pairs. We call this weighted average dynamic structure factor the generalized dynamic structure factor. We extend the formalism of a three effective eigenmode theory (TEE) developed previously for simple fluids to derive an approximate evolution equation for the generalized dynamic structure factor, which can be considered as a generalized hydrodynamic equation for molecular fluids. As examples, we first study the contributions of the partial dynamic structure factor to the generalized dynamic structure factor computed from molecular dynamics simulation of SPC/E model water. We found that the generalized dynamic structure factor of water measured by IXS can be well approximated by the center of mass or the oxygen atom dynamic structure factors. The generalized TEE model was then employed to analyze IXS spectra of nearly fully hydrated dilauroylphosphatidylcholine. The theory is able to fit all of the spectra in the k range from 5 to 32 nm(-1) quantitatively and gives their deconvoluted generalized dynamic structure factors.

The Effect of Temperature on Sorbitan Surfactant Monolayers

The effect of temperature on four sorbitan ester (Span 20, sorbitan monolaurate; Span 40, sorbitan monopalmitate; Span 60, sorbitan monostearate; and Span 80, sorbitan monooleate) monolayers was analyzed. The covered temperature range was from 22 to 42 degrees C. Surface pressure-molecular area isotherms were measured with a Langmuir-type instrument. As the temperature was increased, the monolayers expanded more. This change can also be seen from the surface compressional modulus that was lowered as the temperature was increased. Also, the collapse pressure was lowered as the temperature was increased. Copyright 2001 Academic Press.

Organotin compounds alter the physical organization of phosphatidylcholine membranes

Organotin compounds have a broad range of biological activities and are ubiquitous contaminants in the environment. Their toxicity mainly lies in their action on the membrane. In this contribution we study the interaction of tributyltin and triphenyltin with model membranes composed of phosphatidylcholines of different acyl chain lengths using differential scanning calorimetry, (31)P-nuclear magnetic resonance, X-ray diffraction and infrared spectroscopy. Organotin compounds broaden the main gel to liquid-crystalline phase transition, shift the transition temperature to lower values and induce the appearance of a new peak below the main transition peak. These effects are more pronounced in the case of tributyltin and are quantitatively larger as the phosphatidylcholine acyl chain length decreases. Both tributyltin and triphenyltin increase the enthalpy change of the transition in all the phosphatidylcholine systems studied except in dilauroylphosphatidylcholine. Organotin compounds do not affect the macroscopic bilayer organization of the phospholipid but do affect the degree of hydration of its carbonyl moiety. The above evidence supports the idea that organotin compounds are located in the upper part of the phospholipid palisade near the lipid/water interface.

Collective dynamics in fully hydrated phospholipid bilayers studied by inelastic x-ray scattering

The short wavelength density fluctuation of DLPC (dilaurylphosphatidylcholine) bilayers close to full hydration has been studied by the inelastic x-ray scattering technique below and above the main transition temperature. The analysis based on a generalized three effective eigenmode theory allows us to construct the dispersion relation of the high frequency sound mode for the first time. The marked softening of the excitation near k = 14 nm(-1), corresponding to the lipid chain-chain correlation peak in the structure factor, in the L(alpha) phase implies prevalent occurrences of short-wavelength in-plane motions of lipid chains that might be of importance for transportation of small molecules across membranes.

Binding of nystatin and amphotericin B with sterol-free L-dilauroylphosphatidylcholine bilayers resulting in the formation of dichroic lipid superstructures

Interactions of multilamellar vesicles (MLV) of dilauroylphosphatidylcholine (DLPC) with the polyene antibiotics, amphotericin B (AmB) and nystatin (Ny), were followed by circular dichroism (CD). These interactions proceed with both antibiotics through a slow association with high [DLPC]/[antibiotic] stoichiometric molar ratios (> or = 130), at room temperature for which DLPC membranes are in a fluid state. Microscopic investigations of the spatial distributions of the antibiotic and the MLV in the mixtures revealed that MLV form clusters inside which the antibiotic is strongly concentrated and lipid superstructures appear. Concomitantly with the appearance of these superstructures a DLPC dichroic signal emerges. This observation indicates that the chiral properties of antibiotic oligomers can induce a chirality of the DLPC molecules which are bound to them. These results support the hypothesis of a recent molecular modeling of AmB oligomers which postulates that their chiral properties result from a chiral assemblage of antibiotic molecules (Millié et al., J. Phys. Chem. B, in press).

Influence of lipid/peptide hydrophobic mismatch on the thickness of diacylphosphatidylcholine bilayers. A 2H NMR and ESR study using designed transmembrane alpha-helical peptides and gramicidin A

We have investigated the effect of a series of hydrophobic polypeptides (WALP peptides) on the mean hydrophobic thickness of (chain-perdeuterated) phosphatidylcholines (PCs) with different acyl chain length, using 2H NMR and ESR techniques. The WALP peptides are uncharged and consist of a sequence with variable length of alternating leucine and alanine, flanked on both sides by two tryptophans, and with the N- and C-termini blocked, e.g., FmAW2(LA)nW2AEtn. 2H NMR measurements showed that the shortest peptide with a total length of 16 amino acids (WALP16) causes an increase of 0.6 A in bilayer thickness in di-C12-PC, a smaller increase in di-C14-PC, no effect in di-C16-PC, and a decrease of 0.4 A in di-C18-PC, which was the largest decrease observed in any of the peptide/lipid systems. The longest peptide, WALP19, in di-C12-PC caused the largest increase in thickness of the series (+1.4 A), which decreased again for longer lipids toward di-C18-PC, in which no effect was noticed. WALP17 displayed an influence intermediate between that of WALP16 and WALP19. Altogether, incorporation of the WALP peptides was found to result in small but very systematic changes in bilayer thickness and area per lipid molecule, depending on the difference in hydrophobic length between the peptide and the lipid bilayer in the liquid-crystalline phase. ESR measurements with spin-labeled lipid probes confirmed this result. Because thickness is expected to be influenced most at the lipids directly adjacent to the peptides, also the maximal adaptation of these first-shell lipids was estimated. The calculation was based on the assumption that there is little or no aggregation of the WALP peptides, as was supported by ESR, and that lipid exchange is rapid on the 2H NMR time scale. It was found that even the maximal possible changes in first-shell lipid length were relatively small and represented only a partial response to mismatch. The synthetic WALP peptides are structurally related to the gramicidin channel, which was therefore used for comparison. In most lipid systems, gramicidin proved to be a stronger perturber of bilayer thickness than WALP19, although its length should approximate that of the shorter WALP16. The effects of gramicidin and WALP peptides on bilayer thickness were evaluated with respect to previous 31P NMR studies on the effects of these peptides on macroscopic lipid phase behavior. Both approaches indicate that, in addition to the effective hydrophobic length, also the physical nature of the peptide surface is a modulator of lipid order.

DMSO produces a new subgel phase in DPPC: DSC and X-ray diffraction study

Equilibrium phases and the kinetics of subgel phase transformation of dipalmitoylphosphatidylcholine (DPPC) hydrated with mixtures of dimethylsulfoxide (DMSO)/water have been studied using differential scanning calorimetry (DSC) and X-ray diffraction (XRD). The rate of gel-to-subgel transformation is decreased with a small increase in X, the DMSO/water mole fraction, but then speeds up and becomes faster than in pure water by X = 0.16. The DSC scans show multiple subgel peaks, some of which can be attributed to impacted domain growth. For X greater than 0.10, XRD shows that there is a new, stable subgel phase, S, which also accounts for some of the multiplicity of DSC peaks. Our electron density profiles show that the thickness of the bilayer in the S phase is greater than in the usual C subgel phase. We suggest that the S subgel phase is characterized by different headgroup ordering and smaller chain tilt angle than in the C subgel phase. Electron density profiles show that increasing X decreases the water space between bilayers in all phases, subgel, gel and fluid (L alpha). For X = 0.20, a different gel phase is also observed that may be due to subtle changes in the orientation of chain tilt first observed in partially dehydrated DMPC. The dehydrating effect of DMSO explains the results of a previous study, confirmed in this study, that increasing the concentration of DMSO raises the main transition temperature and eliminates the ripple phase.

Association of polyene antibiotics with sterol-free lipid membranes. II. Hydrophobic binding of nystatin to dilauroylphosphatidylcholine bilayers

Interaction of nystatin A1 with multilamellar vesicles (MLV) of dilauroylphosphatidylcholine (DLPC), observed either by adding nystatin to preformed MLV (mixtures I) or by incorporating it during the formation of vesicles (mixtures II, inner lamellas of MLV in contact with nystatin) was investigated for 0.002 < or = nystatin/DLPC = R(A) < or = 0.20, by four complementary methods. The main results were: (i) Ultraviolet absorption and circular dichroism (CD) spectra of mixtures I revealed the occurrence of a saturable association with a stoichiometry (R(A) = 0.007 +/- 0.002) constant between 3 and 33 degrees C. (ii) By differential scanning calorimetry, thermograms of the two types of mixtures were similar only when water was in great excess. In the opposite (e.g., (H2O)/(DLPC) = R(W) < or = 300), mixture II thermograms displayed two features, upshifted by about 6.5 degrees C with respect to the sharp peak observed with mixture I, resembling those obtained for pure DLPC when the low-temperature phase was the subgel phase. For this R(W), the nystatin absolute concentrations were those for which nystatin form superaggregates as revealed by the nystatin CD spectra. It is proposed that these superaggregates are excluded from the interlamellar spacings of MLV and exert a pumping action on the interlamellar water. The subsequent dehydration of the inner lamellas is thought to convert them into the subgel state. (iii) 2H-NMR spectra of sn-2-perdeuterated DLPC MLV + nystatin mixtures II, confirmed such a temperature shift of the main transition. They showed, in addition, an ordering of the aliphatic chains immediately above the transition temperature, equivalent to a bilayer thickening of 2 A.