Phase transitions of phospholipid vesicles under osmotic stress and in the presence of ethylene glycol.

The effects of poly(ethylene glycol) (PEG) on the phase transition of phospholipid multilamellar vesicles (MLVs) were investigated by using differential scanning calorimetry (DSC). Main transition temperature (Tm) and the pre-transition temperature (Tp) of neutral phospholipid-, DMPC-1, DPPC- and DSPC-MLVs increased with an increase in PEG concentration. The subtransition temperature of DPPC-MLV also increased with an increase in PEG concentration. These results could be qualitatively explained by enhancement of the lateral packing on the basis of the osmoelastic coupling theory. The pretransition temperature increased faster than the main transition temperature did with an increase in PEG concentration. The increment of Tm depended on the hydrocarbon chain length, the shorter the hydrocarbon chain length was, the larger the increment was. The transition width in the DSC peak was broadened with an increase in PEG concentration. These three above-mentioned effects are the main differences between the effects of the osmotic stress on the phase transition of MLVs and those of hydrostatic pressure. On the other hand, ethylene glycol (EG), which is the monomer of PEG, had a biphasic effect on transition temperature of DPPC-, DSPC-, and DMPC-MLV, reducing Tm and Tp at low concentrations, but increasing Tm and extinguishing pretransition at high concentrations. This is explained by the induction of an interdigitated gel phase at high concentrations of EG, which indicates that EG can easily penetrate into the head group region of the lipid, in contrast with PEG 6K, because EG is small. Temperature-EG concentration phase diagrams for the various PC-MLVs were determined.(ABSTRACT TRUNCATED AT 250 WORDS)     

Aliphatic chain transitions of phospholipid vesicles and phospholipid dispersions determined by polarization of fluoroscence

The polarization of fluorescence of dansyl phosphatidylethanolamine and 9-methylanthracene shows that these compounds are reliable indicators of the order-disorder transitions of the phospholipid aliphatic chains in bilayer systems. The transition is better defined in phospholipid dispersion than in vesicles. It is concluded that the two models are not identical as far as the structure near the melting temperature is concerned. Experiments in turbid solutions were performed with horizontal slits either in the incident or emitted beams, which eliminate the effect of light scattering. This improvement in experimental technique may facilitate the fluorescence polarization study of membrane suspensions.     

Phase transition in lipid multilayers induced by benzene. A Raman spectroscopic study

The interaction of increasing amount of benzene with dipalmitoyl lecithin multilayers has been investigated by Raman spectroscopy. It is shown that benzene is able to promote a gel→liquid crystalline phase transition.     

Phase transitions in phospholipid vesicles Fluorescence polarization and permeability measurements concerning the effect of temperature and cholesterol

We have studied the solid to liquid-crystalline phase transition of sonicated vesicles of dipalmitoylphosphatidylglycerol and dipalmitoylphosphatidylcholine. The transition was studied by both fluorescence polarization of perylene embedded in the vesicles, and by the efflux rate of trapped ²²Na⁺.Fluorescence polarization generally decreases with temperature, showing an inflection in the region 32–42°C with a mid-point of approximately 37.5 °C. On the other hand, the perylene fluorescence intensity increases abruptly in this region. To explain this result, we have proposed that, for $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ where $\text{T}{}_{\mathrm{<mtext>c</mtext>}}$ is the transition temperature, perylene is excluded from the hydrocarbon interior of the membranes, whereas, $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ this probe may be accommodated in the membrane interior to a large extent.The self-diffusion rates of ²²Na⁺ through dipalmitoylphosphatidylglycerol vesicles exhibit a complex dependence on temperature. There is an initial large increase in diffusion rates (approximately 100-fold) between 30 and 38 °C, followed by a decrease (approximately 4-fold) between 38 and 48 °C. A monotonic increase is then observed at temperatures higher than 48 °C. The local maximum of ²²Na⁺ self-diffusion rates at approximately 38 °C coincides with the mid-point of phase transition as detected by changes in fluorescence polarization of perylene with the same vesicles. Vesicles composed of dipalmitoylphosphatidylcholine show the same general behavior in terms of ²²Na⁺ self-diffusion rates at different temperatures, except that the local maximum occurs at approximately 42 °C.The temperature dependence of the permeability and the appearance of a local maximum at the phase transition region could be explained in terms of a domain structure within the plane of the membranes. This explanation is based on the possibility that boundary regions between liquid and solid domains would exhibit relatively high permeability to ²²Na⁺.Mixed vesicles composed of equimolar amounts of dipalmitoyl phospholipids and cholesterol show no abrupt changes in the temperature dependence of either perylene fluorescence polarization or ²²Na⁺ diffusion rate measurements. This is taken to indicate the absence of agross phase transition in the presence of cholesterol.     

Low frequency and diffusive motion in aligned phospholipid multilayers studied by pulsed NMR

Measurements of T₁, T_1?, T_1D and the FID are reported for protons in aligned stacks of Egg Yolk Lecithin (EYL)-D₂O multilayers. From the ω₁ dependence of T_1? and the ω₀ dependence of T₁ the two dispersive regions of the spectral density function were identified. The lower frequency region has a centre angular frequency of 2.2 × 10⁵ rad/s and the upper frequency region a centre angular frequency of 4 × 10⁷ rad/s.From the orientation dependence of T_1?, T_1D and the FID, the lower frequency dispersion is assigned to fluctuations in the packing density of the hydrocarbon chains in the plane of the bilayer, and the upper frequency region to the translational diffusion of the lipid molecules. Based on a similar approach to one previously described, a diffusion coefficient of 1.4 × 10^?8 cm²/s is calculated for the EYL molecules in the bilayers.     

Shape transitions and shape stability of giant phospholipid vesicles in pure water induced by area-to-volume changes.

Shape transformations of vesicles of dimyristoylphosphatidylcholine (= DMPC) and palmitoyloleylphosphatidylcholine (= POPC) in ion-free water were induced by changing the area-to-volume ratio via temperature variations. Depending on the pretreatment we find several types of shape changes for DMPC (in pure water) at increasing area-to-volume ratio: (a) budding transitions leading to the formation of a chain of vesicles at further increase of the area-to-volume ratio, (b) discocyte-stomatocyte transitions, (c) reentrant dumbbell-pear-dumbbell transitions, and (d) spontaneous blebbing and/or tether formation of spherical vesicles. Beside these transitions a more exotic dumbbell-discocyte transition (e) was found which proceeded via local instabilities. Pears, discocytes, and stomatocytes are stable with respect to small temperature variations unless the excess area is close to values corresponding to limiting shapes of budded vesicles where temperature variations of less than or equal to 0.1 degree C lead to spontaneous budding to the inside or the outside. For POPC we observed only budding transitions to the inside leading either to chains of vesicles or to distributions of equally sized daughter vesicles protruding to the inside of the vesicle. Preliminary experiments concerning the effect of solutes are also reported. The first three types of shape transitions can be explained in terms of the bilayer coupling model assuming small differences in thermal expansivities of the two monolayers. This does not hold for the observed instabilities close to the limiting shapes.     

Phase transitions and hydrogen bonding in a bipolar phosphocholine evidenced by calorimetry and vibrational spectroscopy.

As a model for natural archaebacterial bolalipids, we have synthesized omega-hydroxybehenylphosphocholine (HBPC, HO-(CH(2))(22)-OP(O(-)(2))O-(CH(2))(2)-N+(CH(3))(3)) and investigated it, by Fourier-transform infrared and Raman spectroscopy and differential scanning calorimetry, both as fully hydrated dispersions (varying temperature) and as aligned films (varying hydration) in terms of particular structural features predestining such bipolar lipids for their occurrence in extremophilic organisms. The phase behavior of HBPC in dispersions depends on sample pretreatment as it comprises metastabilities in annealed samples. However, main transition proceeds consistently near 81 degrees C. Some (extra) deal of headgroup (phosphate) hydration accompanying a gel-gel phase transition near 66 degrees C appears to precede chain melting. Studies with HBPC films revealed lamellar interdigitated-like solid phases with an extraordinarily strong omega-OH--OPO(-) omega-OH--OPO(-) omega-OH hydrogen-bond pattern formed along both sides of the resulting monolayers. The "clamping" effect inherent to such structures provides a clue to explain the relatively high main-transition temperature of HBPC assemblies.     

Aggregation of phospholipid vesicles by water-soluble polymers.

Water-soluble polymers such as dextran and polyethylene glycol are known to induce aggregation and size growth of phospholipid vesicles. The present study addresses the dependence of these processes on vesicle size and concentration, polymer molecular weight, temperature, and compartmentalization of the vesicles and polymers, using static and dynamic light scattering. Increasing the molecular weight of the polymers resulted in a reduction of the concentration of polymer needed for induction of aggregation of small unilamellar vesicles. The aggregation was fully reversible (by dilution), within a few seconds, up to a polymer concentration of at least 20 wt %. At relatively low phosphatidylcholine (PC) concentrations (up to approximately 1 mM), increasing the PC concentration resulted in faster kinetics of aggregation and reduced the threshold concentration of polymer required for rapid aggregation (CA). At higher PC concentrations, CA was only slightly dependent on the concentration of PC and was approximately equal to the overlapping concentration of the polymer (C*). The extent of aggregation was similar at 37 and 4 degrees C. Aggregation of large unilamellar vesicles required a lower polymer concentration, probably because aggregation occurs in a secondary minimum (without surface contact). In contrast to experiments in which the polymers were added directly to the vesicles, dialysis of the vesicles against polymer-containing solutions did not induce aggregation. Based on this result, it appears that exclusion of polymer from the hydration sphere of vesicles and the consequent depletion of polymer molecules from clusters of aggregated vesicles play the central role in the induction of reversible vesicle aggregation. The results of all the other experiments are consistent with this conclusion.     

Factors affecting leakage of trapped solutes from phospholipid vesicles during thermotropic phase transitions.

Liposomes are commonly used as models for chilling and freezing damage, with leakage of water-soluble contents from the aqueous interior as the most frequently used measurement of damage. In order to achieve an understanding of the mechanism of the leakage, we have conducted a study of the factors that influence the leakage from liposomes during phase transitions. While such investigations have appeared sporadically in the literature, a detailed study has not been undertaken previously, despite the fact that liposomes are widely used as models for stress injury. Thus, we suggest that these findings will be of general interest in the cryobiology community. We now report that the following variables affected leakage from liposomes during chilling: (i) increasing the rate of cooling and warming resulted in decreased leakage; (ii) maximal leakage occurred at the measured phase transition temperature; (iii) addition of defect-forming additives such as a second phospholipid or a surfactant increased leakage from the liposomes during the phase transition but not above or below that temperature; (iv) small unilamellar vesicles leaked much more rapidly than large unilamellar vesicles; and (v) increasing the pH of the external buffer decreased leakage of carboxyfluorescein, an effect that is probably particular to ionizable solutes.     

Effects of temperature and molecular interactions on the vibrational infrared spectra of phospholipid vesicles

Infrared spectra were obtained as a function of temperature for a variety of phospholipid/water bilayer assemblies (80% water by weight) in the 3000-950 cm^?1 region. Spectral band-maximum frequency parameters were defined for the 2900 cm^?1 hydrocarbon chain methylene symmetric and asymmetric stretching vibrations. Temperature shifts for these band-maximum frequencies provided convenient probes for monitoring the phase transition behavior of both multilamellar liposomes and small diameter single-shell vesiclesof dipalmitoyl phosphatidylcholine/water dispersions. As examples of the effects of bilayer lipid/cholesterol/water (3 : 1 mol ratio) and lipid/cholesterol/amphotericin B/water (3 : 1 : 0.1 mol ratios) vesicles were examined using the methylene stretching frequency indices. In comparison to the pure vesicle form, the transition width of the lipid/cholesterol system increased by nearly a factor of two (to 8°C) while the phase transition temperature remained approximately the same (41° C). For the lipid/cholesterol/amphotericin B system, the phase transition temperature increased by about 4.5° C (to 45.5°C) with the transition width increasing by nearly a factor of four ($\text{to}\text{≈ 15°}\text{C}$) above that of the pure vesicles. The lipid/cholesterol/amphotericin B data were interpreted as reflecting the formation below 38°C of a cholesterol/amphotericin B complex whose dissociation at higher temperature (38–60°C range) significantly broades the gel-liquid crystalline phase transition.     

Temperature dependence of the low frequency dynamics of myoglobin. Measurement of the vibrational frequency distribution by inelastic neutron scattering.

Inelastic neutron scattering spectra of myoglobin hydrated to 0.33 g water (D2O)/g protein have been measured in the low frequency range (1-150 cm-1) at various temperatures between 100 and 350 K. The spectra at low temperatures show a well-resolved maximum in the incoherent dynamic structure factor Sinc(q, omega) at approximately 25 cm-1 and no elastic broadening. This maximum becomes gradually less distinct above 180 K due to the increasing amplitude of quasielastic scattering which extends out to 30 cm-1. The vibrational frequency distribution derived independently at 100 and 180 K are very similar, suggesting harmonic behavior at these temperatures. This result has been used to separate the vibrational motion from the quasielastic motion at temperatures above 180 K. The form of the density of states of myoglobin is discussed in relation to that of other amorphous systems, to theoretical calculations of low frequency modes in proteins, and to previous observations by electron-spin relaxation of fractal-like spectral properties of proteins. The onset of quasielastic scattering above 180 K is indicative of a dynamic transition of the system and correlates with an anomalous increase in the atomic mean-squared displacements observed by M?ssbauer spectroscopy (Parak, F., E. W. Knapp, and D. Kucheida. 1982. J. Mol. Biol. 161: 177-194.) and inelastic neutron scattering (Doster, W., S. Cusack, and W. Petry, 1989. Nature [Lond.]. 337: 754-756.) Similar behavior is observed for a hydrated powder of lysozyme suggesting that the low frequency dynamics of globular proteins have common features.     

Penetration and fusion of phospholipid vesicles by lysozyme

The lysozyme-induced fusion of phosphatidylserine/phosphatidylethanolamine vesicles as studied at a wide range of pH is found to correlate well with the binding of this protein to the vesicles. An identical 6000 molecular weight segment of lysozyme at the N-terminal region is found to be protected from tryptic digestion when initially incubated with vesicles at several pH values. Only this segment is labeled by dansyl chloride, which is partitioned into the bilayer. These results suggest the penetration of one segment of lysozyme into the bilayer. Photoactivated labeling of the membrane-penetrating segment of lysozyme with 3-(trifluoromethyl)-3-([125I]iodophenyl)diazirine ([125I]TID) and subsequent identification of the labeled residues by Edman degradation and gamma-ray counting indicate that four amino acids from the N-terminal are located outside the hydrophobic core of the bilayer. Although treatment of the membrane-embedded segment with aminopeptidase failed to cleave any amino acids from the N-terminal, it appears that a loop of lysozyme segment near the N-terminal penetrates into the bilayer at acidic pH. A helical wheel diagram shows that the labeling is done mainly on one surface of the alpha-helix. The penetration kinetics as studied by time-dependent [125I]TID labeling coincide with the fusion kinetics, strongly suggesting that the penetration of the lysozyme segment into the vesicles is the cause of the fusion.     

Phase transitions of phospholipid bilayers from an unsaturated fatty acid auxotroph of Escherichia coli.

Total phospholipids were extracted from cells of temperature sensitive unsaturated fatty acid auxotrophs of Escherichia coli (K-12 UFAts) grown at 28degrees C (PL28), and at 42degrees C in the presence of 2% KCl as an osmotic stabilizer (PL42 (KCl)). From the analysis of fatty acids, it was shown that the content of unsaturated fatty acids of PL42 (KCl) is only 9% of the total fatty acids, while that of PL28 is 54%. The thermal phase transitions of the bilayers prepared from the phospholipid fractions were studied by proton magnetic resonance. The line widths of the methylene signals and the sums of the methylene and methyl signal intensities were plotted against reciprocal values of absolute temperature 1/T or temperature itself. From the plots phase transitions were detected at about 19degrees C for PL28 and at 43degrees C for PL42 (KCl). In spite of its complex composition of fatty acids a highly cooperative transition was observed in the case of PL42 (KCl). It was also suggested that the phospholipids bilayers in the biomembranes of this strain at the growth temperature (42 degrees C) are in the state where the gel and liquid crystalline phases coexist.     

Calorimetric and infrared spectroscopic studies of the interaction of alpha-tocopherol and alpha-tocopheryl acetate with phospholipid vesicles

The location of alpha-tocopherol and alpha-tocopheryl acetate in the membrane has been a subject of considerable interest, not only because of their relevant physiological function, but also for understanding their interaction with the phospholipids. We have examined this question by using reconstituted systems including dipalmitoyl-glycerophosphocholine multibilayer vesicles to which alpha-tocopherol and alpha-tocopheryl acetate were incorporated. Differential scanning microcalorimetry measurements showed that both compounds were capable of modifying the thermotropic properties of the pure phospholipid, so that the pretransition disappears at low concentrations of these terpenoid molecules. The enthalpy corresponding to the main transition decreases as the concentration of alpha-tocopherol increases and the transition peak is progressively shifted to lower temperatures. alpha-Tocopheryl acetate gave the same type of effect but less marked than in the case of alpha-tocopherol. Fourier-transform infrared spectroscopic measurements were also made on these systems and the temperature dependence of the infrared spectra was studied. A comparison of the spectroscopic data showed that, in agreement with the calorimetric results, alpha-tocopherol remarkably perturbs the thermotropic phase transition of dipalmitoylglycerophosphocholine. It was concluded from a study of the CH2 stretching bands that alpha-tocopherol induced changes in frequency and in bandwidth parameters. However, the changes in frequency and bandwidth with respect to temperature are not concerted; this is a consequence of the existence of more than one phase in the presence of alpha-tocopherol. From the study of the CH2 scissoring band, it was concluded that alpha-tocopherol disrupts the acyl chain packing present in pure dipalmitoylglycerophosphocholine below the onset temperature of the gel-to-liquid-crystal transition. The effect of alpha-tocopheryl acetate is of a similar type to that of alpha-tocopherol but weaker with respect to these stretching and scissoring CH2 bands. Spectral changes were also found in the C = O stretching mode of the phospholipid in the presence of alpha-tocopherol and these changes were attributed to perturbations in the C1-C2 bonds of sn-2-acyl chains of the phospholipid. These effects were much weaker in the case of alpha-tocopheryl acetate; it is suggested that this may be due to a specific interaction between alpha-tocopherol and the polar region of the phospholipid. This interaction seems to be absent in the systems containing alpha-tocopheryl acetate.(ABSTRACT TRUNCATED AT 400 WORDS)     

Fusion and fragmentation of phospholipid vesicles by apohemoglobin at low pH.

Human apohemoglobin in acidic media was found to induce fusion of phosphatidylcholine/phosphatidylserine (1:1) vesicles at low protein concentration but to fragment the same vesicles to form micellar complex at high protein concentration. The fusion was demonstrated by size increase, vesicle content mixing, lipid mixing, and electron microscopy. The micellization of phospholipid vesicles was observed by light scattering, gel filtration, and electron microscopy. The hydrophobic labeling of the apohemoglobin/vesicle complex followed by CNBr cleavage of apohemoglobin showed that an N-terminal segment of the beta subunit with a molecular weight of approximately 6,000 seems to be mainly involved in the fusion process, but the whole sequences of both alpha and beta chains participate in the micellization process.