Phase transition kinetics of phosphatidic acid bilayers A stopped-flow study of the electrostatically induced transition

The kinetics of the electrostatically induced phase transition of dimyristoyl phosphatidic acid bilayers was followed using the stopped-flow technique. The phase transition was triggered by a fast change in the pH or the magnesium ion concentration and followed by recording the time dependence of the absorbance. When the phase transition was induced by a pH jump the time course of the absorbance could be described by two exponentials, their time constants displaying the for cooperative processes characteristic maximum at the transition midpoint. The time constants are in the 10 and 100 ms range for the H⁺ triggered transition from the fluid to the ordered state. A third slower process shows no appreciable temperature dependence and is probably caused by vesicle aggregation. For the OH^--induced transition fron the ordered to the fluid state the time constants are in the 100 and 1000 ms range. The fluid-ordered transition could also be triggered by addition of magnesium ions. Of the several observed processes only the fastest in the 10–100 ms time range could definitely be assigned to the fluid-ordered transition while the others are due to aggregation phenomena. The experimental data were compared with results obtained from pressure jump experiments and could be interpreted on the basis of theories for non-equilibrium relaxation.     

The influence of charge on phosphatidic acid bilayer membranes.

A complete titration of phosphatidic acid bilayer membranes was possible for the first time by the introduction of a new anaologue, 1,2-dihexadecyl-sn-glycerol-3-phosphoric acid, which has the advantage of a high chemical stability at extreme pH values. The synthesis of the phosphatidic acid is described and the phase transition behaviour in aqueous dispersions is compared with that of three ester phosphatidic acids; 1,2-dimyristoyl-sn-glycerol-3-phosphoric acid, 1,3-dimyristoylglycerol-2-phosphoric acid and 1,2-dipalmitoyl-sn-glycerol-3-phosphoric acid. The phase transition temperatures (Tt) of aqueous phosphatidic acid dispersions at different degrees of dissociation were measured using fluorescence spectroscopy and 90 degrees light scattering. The Tt values are comparable to the melting points of the solid phosphatidic acids in the fully protonated states, but large differences exist for the charged states. The Tt vs. pH diagrams of the four phosphatidic acids are quite similar and of a characteristic shape. Increasing ionisation results in a maximum value for the transition temperatures at pH 3.5 (pK1). The regions between the first and the second pK of the phosphatidic acids are characterised by only small variations in the transition temperatures (extended plateau) in spite of the large changes occurring in the surface charge of the membranes. The slope of the plateau is very shallow with increasing ionisation. A further decrease in the H+ concentration results in an abrupt change of the transition temperature. The slope of the Tt vs. pH diagram beyond pK2 becomes very steep. This is the result of reduced hydrocarbon interaction energy, which was demonstrated by differential scanning calorimetry (Blume, A. and Eibl, H., unpublished data).     

Effect of the lipid phase transition on the kinetics of H+/OH− diffusion across phosphatidic acid bilayers

The kinetics of H⁺/OH^? diffusion across dimyristoyl phosphatidic acid bilayer membranes was measured by following the absorbance of the pH-sensitive indicator Cresol red ($\text{o-}\text{cresolsulfonphthalein}$) entrapped in single lamellar vesicles after rapidly changing the external pH in a stopped-flow apparatus. The H⁺/OH^?-permeability coefficient was found to be in the 10^?5 to 10^?3 cm·s^?1 range. The lipid phase transition has a strong influence on the permeation kinetics as the permeability coefficients in the liquid-crystalline phase are drastically higher. The permeability shows no maximum at the phase transition temperature as is the case for other ions, but displays a similar temperature dependence as water permeation. This is also reflected in the high activation energy of approx. 20 kcal/mol and supports the hypothesis (Nichols, J.W. and Deamer, D.W. (1980) Proc. Natl. Acad. Sci. U.S.A. 77, 2038–2042) of H⁺/OH^? permeation via hydrogen bonded water molecules. A second slower kinetic phase is also observed, where the permeation is obviously controlled by counterion diffusion. The temperature dependence of this slow process displays the for ion diffusion characteristic maximum in the permeability at the phase-transition temperature.     

The influence of charge on bilayer membranes. Calorimetric investigations of phosphatidic acid bilayers.

The pH-dependence of the phase transition of dimyristoyl phosphatidic acid and dihexadecyl phosphatidic acid has been investigated using differential scanning calorimetry. Varying the pH induces different degrees of ionization of the polar head group. The changes in transition temperature with pH as observed by calorimetry are in good agreement with those obtained by measuring the changes in light scattering, whereas the transition temperatures reported by the fluorescent probe N-phenylnaphthylamine do not always coincide with those determined from calorimetry [1]. The observed maximum of the transition temperature at pH 3.5 corresponds to a minimum in the transition enthalpy vs. pH diagram. At this pH a particular stable bilayer phase is formed. Full protonation of phosphatidic acids leads to suspensions of mycrocrystals. The transition enthalpy approaches the value of the melting enthalpy of crystalline anhydrous phosphatidic acid. The decrease in the transition enthalpy at high pH values is due to a change in the hydrocarbon chain interactions induced by the doubly charged head groups. The cooperativity of the transition varies with the degree of ionization of the head group, being lower for doubly charged phosphatidic acids.     

Asymmetric antagonistic effects of an inhalation anesthetic and high pressure on the phase transition temperature of dipalmitoyl phosphatidic acid bilayers

The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>t</mtext>}}$) of dipalmitoyl phosphatidic acid multilamellar liposomes is depressed 10°C by the inhalation anesthetic methoxyflurane at a concentration of 100 mmol/mol lipid. Application of 100 atm of helium pressure to pure phosphatidic acid liposomes increased $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C. However, application of 100 atm helium pressure to dipalmitoyl phosphatidic acid lipsomes containing 100 mmol methoxyflurane/mol lipid almost completely antagonized the effect of the anesthetic. A nonlinear pressure effect is observed. In a previous study, a concentration of 60 mmol methoxyflurane/mol dipalmitoyl phosphatidylcholine depressed $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C, exhibiting a linear pressure effect. The completely different behavior in the charged membrane is best explained by extrusion of the anesthetic from the lipid phase.     

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.     

Properties of bilayer membranes in the phase transition or phase separation region

The increase in passive permeability of bilayer membranes near the phase transition temperature is usually explained as caused by either the increase in the amount of ‘boundary lipid’ present in the membrane, or by the increase in lateral compressibility of the membrane. Since both the amount of ‘boundary lipid’ and the lateral compressibility show a similar anomaly near the transition temperature, it is difficult to distinguish experimentally between the two proposed mechanisms.We have examined some details of both of the proposed pictures. The fluid-solid boundary energy, neglected in previous work, has been computed as a function of the domain size. For a single component uncharged lipid bilayer, the results rule out the existence of even loosely defined solid domains in a fluid phase, or vice versa. Thermodynamic fluctuations, which are responsible for anomalous behaviour near the phase transition temperature, are not intense enough to approximate the formation of a domain of the opposite phase.Turning next to lateral compressibility of bilayer membranes we have considered two-component mixtures in the phase separation region. We present the first calculation of lateral compressibility for such systems. The behaviour shows interesting anomalies, which should correlate with existing and future data on transport across membranes.     

Influence of pH on phosphatidic acid multilayers a rippled structure at high pH values

The influence of pH on the structure of 1,2-(ditetradecyl)-phosphatidic acid was investigated by differential scanning calorimetry and freeze-fracture electron microscopy. At pH 13.5–14 (2.6 M K⁺), where phosphatidic acid has two negative charges, calorimetric scans show a small transition (pretransition) below the main phase transition temperature. Freeze-fracture studies of the same dispersions reveal regular band patterns (so-called ripples) in the plane of the bilayers, when the lipid is quenched from below the main phase transition temperature. This rippled structure is similar to the well-known rippled structure of phosphatidylcholines.     

Electrostatic interactions at charged lipid membranes Kinetics of the electrostatically triggered phase transition

Charged lipid membranes of dimyristoylmethylphosphatidic acid were mixed rapidly in a stopped-flow cell with protons or Ca²⁺ to compensate the charges and thereby trigger the ordered-fluid phase transition. The kinetics of the transition was studied by following the time development of the fluorescence anisotropy of diphenylhexatriene. A relaxation process was observed with a characteristic time in the range 10–200 ms. By comparison with existing theories of non-equilibrium relaxation it was concluded that the relaxation process is governed by a nucleation step.     

The rippled structure in bilayer membranes of phosphatidylcholine and binary mixtures of phosphatidylcholine and cholesterol

Freeze-fracture electron microscopy is used to study the rippled texture in pure dimyristoyl and dipalmitoyl phosphatidylcholine membranes and in mixtures of dimyristoyl phosphatidylcholine and cholesterol. Evidence is presented that the apparent phase transition properties of multilamellar liposomes may be dependent on the manner in which liposomes are prepared. Under certain conditions the ripple structures as visualized by freeze-fracture electron microscopy for the pure phosphatidylcholines are observed to be temperature dependent in the vicinity of the pretransition. Thus the transition can sometimes appear to be a gradual transition rather than a sharp, first-order phase transition. In mixtures of dimyristoyl phosphatidylcholine and cholesterol, the ripple repeat distance is found to increase as the cholesterol concentration is increased between 0 and 20 mol%. Above 20 mol%, no rippling is observed. A simple theory is presented for the dependence of ripple repeat spacing on cholesterol concentration in the range 0–20 mol%. This theory accounts for the otherwise inexplicable abrupt increase in the lateral diffusion coefficients of fluorescent lipids in binary mixtures of phosphatidylcholine and cholesterol when the cholesterol concentration is increased above 20 mol%.     

Pressure-induced changes in the molecular organization of a lipid-peptide complex. Polymyxin binding to phosphatidic acid membranes

The effect of 100 atm pressure on the organization of the lipid-peptide complex formed between polymyxin and dipalmitoyl phosphatidic acid has been investigated. Phase transition curves were obtained by electron paramagnetic resonance by measuring the partition coefficient of the spin label, 2, 2, 5, $\text{5-}\text{tetramethylpiperidine}\text{-N-}\text{oxyl}$. The three-step phase transition curve previously obtained with fluorescence polarization measurements was confirmed, demonstrating three distinct phosphatidic acid domains in the bilayer. Pressure increases binding of polymyxin to phosphatidic acid bilayers and alters the proportions of the two domains that differ in the mode of binding between phosphatidic acid and polymyxin. The binding curves of polymyxin to phosphatidic acid bilayers were determined and it was shown that application of pressure reduces the cooperativity of the binding curve.     

The effect of calcium on the bilayer stability of lipids from bovine rod outer segment disk membranes

The phase behavior of bovine rod outer segment disk lipids has been investigated using freeze-fracture and ³¹P nuclear magnetic resonance (NMR) techniques. ³¹P-NMR spectra of isolated disk membranes were taken as a function of temperature between 25°C and 45°C. The ³¹P-NMR spectrum characteristic of phospholipid bilayers was observed at all temperatures both in the absence of Ca²⁺ and in the presence of 10 mM and 50 mM Ca²⁺. A similar study was performed on lipids isolated from the disk membranes. In the absence of Ca²⁺ only lamellar phase behavior was observed. In the presence of less than 10 mM Ca²⁺, however, there was a change in morphology to non-lamellar structures. Removal of the Ca²⁺ caused the system to reassume the lamellar form.     

The effect of surface curvature on the head-group structure and phase transition properties of phospholipid bilayer vesicles

Proton nuclear magnetic resonance spectra at 360 MHz of small sonicated distearoyl phosphatidylcholine vesicles show easily distinguishable resonances due to choline N-methyl head-group protons located in the inner and outer bilayer halves. A study of the chemical shift of these resonances as a function of temperature reveals that the splitting between them increases below the phase transition. This occurs as a result of an upfield shift of the inner layer resonance at the phase transition. Consideration of the possible causes of this effect results in the conclusion that, at the phase transition, there is a change in the organization of the inner layer head-groups which does not occur for the outer layer head-groups.     

The adsorption of divalent cations to phosphatidylglycerol bilayer membranes

The ability of the Stern equation to describe the adsorption of divalent cations to phosphatidylglycerol membranes was tested by combining ³¹P-NMR and electrophoretic mobility measurements. In 0.1 M sodium chloride both the ³¹P-NMR and the zeta potential data are well described by the Stern equation. ³¹P-NMR and ¹³C-NMR results indicate that cobalt forms inner-sphere complexes only with the phosphate group of phosphatidylglycerol molecules and that a substantial fraction of the adsorbed cobalt ions form outer-sphere complexes. Evidence is presented that suggests the alkaline earth cations also bind to phospholipids mainly by forming outer sphere complexes. Electrophoretic mobility measurements were performed with several different divalent cations. In all cases the zeta potentials in 0.1 M sodium chloride were well described by the Stern equation. The intrinsic 1 : 1 association constants (M^?1) for the phosphatidylglycerol complexes decreased in the sequence: Mn²⁺, 11.5; Ca²⁺, 8.5; Ni²⁺, 7.5; Co²⁺, 6.5; Mg²⁺, 6.0; Ba²⁺, 5.5 and Sr²⁺, 5.0.     

A calorimetric study of the thermotropic behaviour of 1,2-dipentadecylmethylidene phospholipids

Differential scanning calorimetry was used to study the thermotropic behaviour of 1,2-dipentadecylmethylidene phospholipids with various head groups. The structural variation in the glycerol backbone region leads to a strong restriction of conformational freedom for the first two methylene segments of the chains, so that dipentadecylmethylidene phospholipids show lower transition temperatures, lower enthalpies and lower cooperativity of the transition from the gel to the liquid crystalline phase. The extreme chemical stability of these lipids in the alkaline pH region enables investigations of phosphatidylethanolamine and phosphatidic acid dispersions at high pH values. Both phospholipids show a decrease in the transition temperature and in the transition enthalpy as they become singly and doubly charged, respectively. A complex behaviour of the transition enthalpy of doubly charged 1,2-dipentadecylmethylidene phosphatidic acid was observed when the NaCl concentration of the dispersion was increased.     

The influence of different membrane components on the electrical stability of bilayer lipid membranes

A good understanding of cell membrane properties is crucial for better controlled and reproducible experiments, particularly for cell electroporation where the mechanism of pore formation is not fully elucidated. In this article we study the influence on that process of several constituents found in natural membranes using bilayer lipid membranes. This is achieved by measuring the electroporation threshold (V_th) defined as the potential at which pores appear in the membrane. We start from highly stable 1,2-diphytanoyl-sn-glycero-3-phosphocholine (DPhPC) membranes (V_th ∼ 200 mV), and subsequently add therein other phospholipids, cholesterol and a channel protein. While the phospholipid composition has a slight effect (100 mV ≤ V_th ≤ 290 mV), cholesterol gives a concentration-dependent effect: a slight stabilization until 5% weight (V_th ∼ 250 mV) followed by a noticeable destabilization (V_th ∼ 100 mV at 20%). Interestingly, the presence of a model protein, α-hemolysin, dramatically disfavours membrane poration and V_th shows a 4-fold increase (∼ 800 mV) from a protein density in the membrane of 24 × 10^− 3 proteins/μm². In general, we find that pore formation is affected by the molecular organization (packing and ordering) in the membrane and by its thickness. We correlate the resulting changes in molecular interactions to theories on pore formation.     

Membrane binding of oligomeric alpha-synuclein depends on bilayer charge and packing

Membrane disruption by oligomeric α-synuclein (αS) is considered a likely mechanism of cytotoxicity in Parkinson’s disease (PD). However, the mechanism of oligomer binding and the relation between binding and membrane disruption is not known. We have visualized αS oligomer-lipid binding by fluorescence microscopy and have measured membrane disruption using a dye release assay. The data reveal that oligomeric αS selectively binds to membranes containing anionic lipids and preferentially accumulates into liquid disordered (Ld) domains. Furthermore, we show that binding of oligomers to the membrane and disruption of the membrane require different lipid properties. Thus membrane-bound oligomeric αS does not always cause bilayer disruption.     

Phospholipid interactions with cytochrome P-450 in reconstituted vesicles Preference for negatively-charged phosphatidic acid

Cytochrome $\text{P-450}$ LM2 was reconstituted by the cholate-dialysis method into vesicles containing a mixture of either phosphatidylcholine or phosphatidylethanolamine with up to 50 mol% of phosphatidic acid. Phase transition curves in the presence or absence of cytochrome $\text{P-450}$ were obtained from electron paramagnetic resonance experiments by measuring the partitioning of 2,2,6,6-tetramethylpiperidine-1-oxyl. Protein-free phospholipid vesicles exhibit a phase separation into domains of gel phase enriched in phosphatidic acid in a surrounding fluid matrix containing mainly phosphatidylcholine. The phase transition of the phosphatidic acid domains disappeared following incorporation of cytochrome $\text{P-450}$ into the bilayers. In contrast, in vesicles containing mixtures of egg-phosphatidic acid and dimyristoyl phosphatidylcholine, the phase transition of the domains enriched in dimyristoyl phosphatidylcholine was less sharp than in the corresponding vesicles containing cytochrome $\text{P-450}$. The results of both of these experiments could be explained by a redistribution of the mol fraction of the two phospholipids in the gel phase due to preferential binding of the egg-phosphatidic acid to the cytochrome $\text{P-450}$. For comparison, incorporation of cytochrome $\text{P-450}$ into uncharged vesicles of dimyristoyl phosphatidylcholine and egg-phosphatidylethanolamine did not alter the     

The incorporation of cholesterol into inner mitochondrial membranes and its effect on lipid phase transition

Incubations of rat liver inner mitochondrial membranes with liposomes prepared from $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycero}\text{-3-}\text{phosphocholine}$ (DPPC) and cholesterol resulted in a considerable enrichment of the cholesterol composition of these membranes. This enrichment is not accompanied by an alteration in the membrane phospholipid content or fatty acid composition. The exogenous cholesterol appears to be integrated into the membrane structure because it has effects consistent with the known properties of this sterol in other natural and artificial membrane systems.Differential scanning calorimetry on both intact membranes and extracted lipids showed that as the ratio of cholesterol to phospholipid was increased, the endotherm corresponding to the lipid phase transition was reduced. Freeze-fracture electron microscopy of the native membranes showed that intramembranous particles are randomly distributed above the phase transition temperature. Below this temperature large smooth areas, believed to correspond to lipid in the gel state from which proteins have been excluded, can be observed. In the presence of high concentrations of cholesterol the fracture faces observed below the lipid transition temperature show no regions of phase segregation, an observation consistent with previous studies using pure lipids where cholesterol was observed to prevent the lipid undergoing a cooperative phase transition.The results are discussed in terms of the observed low concentrations of cholesteorl in normal liver inner mitochondrial membranes and the distribution of cholesterol within the liver cells.     

Polyunsaturated fatty acyl residues of galactolipids are involved in the control of bilayer/non-bilayer lipid transitions in higher plant chloroplasts

Total polar lipid extracts of chloroplasts isolated from broad beans (Vicia faba) tend to form non-bilayer structures when dispersed in dilute salt solutions. Monoglactosyldiacylglycerol is shown to play a dominant role in this process. The tendency of this lipid to form non-bilayer structures when dispersed alone in water was found to depend upon the degree of unsaturation of its associated fatty acyl chains. Highly unsaturated lipids (average number of double bonds per lipid molecule greater than about 5.0) form inverted hexagonal (Hex_II) structures in water at 20°C, whilst more saturated lipids (average number of double bonds per lipid molecule less than about 4.5) form lamellar sheets. Wide-angle X-ray diffraction and differential scanning calorimetry measurements indicate that these lamellae consist of gel-phase lipid that can adopt either of two structures depending on the thermal history of the sample. Freeze-fracture studies performed on total polar lipid extracts that have been hydrogenated using Adams' catalyst, and reconstituted extracts in which monogalactosyldiacylglycerol has been selectively hydrogenated, show that the degree of unsaturation of this lipid is a key factor in determining whether or not non-bilayer structures are formed in such extracts. Increasing the extent of saturation of the acyl residues of monogalactosyldiacylglycerol reduces the tendency to form non-bilayer structures. Similar effects are observed on lowering the temperature of the dispersions. Fluorescence polarisation measurements using 1,6-diphenyl-1,3,5-hexatriene indicate that the disappearance of non-bilayer structures is accompanied by a marked decrease in the fluidity of the lipid matrix. The possible significance of these observations is discussed in terms of the thermal adaptation and chilling sensitivity of plant membranes.