Lipid phase transitions in membranes involving intrinsic periodic curvature

A conformation of the lipid bilayer of membranes is proposed, with periodic curvature corresponding to the minimal surface structure of cubic lipid phases. Evidence is given indicating that activities of lipid synthesis/modification enzymes embedded in the membrane are controlled by the lateral "packing-pressure", so that the lipid bilayer is close to a transition from the lamellar (L alpha) type of conformation to this periodically curved conformation. Such a phase transition mechanism is assumed to be involved in numerous cooperative membrane functions.     

Lipid phase transitions in cat oocytes supplemented with deuterated fatty acids

Cryopreservation of oocytes has already been used to preserve genetic resources, but this technology faces limitations when applied to the species whose oocytes contain large amounts of cytoplasmic lipid droplets. Although cryoinjuries in such oocytes are usually associated with the lipid phase transition in lipid droplets, this phenomenon is still poorly understood. We applied Raman spectroscopy of deuterium-labeled lipids to investigate the freezing of lipid droplets inside cat oocytes. Lipid phase separation was detected in oocytes cryopreserved by slow-freezing protocol. For oocytes supplemented with stearic acid, we found that saturated lipids form the ordered phase being distributed at the periphery of lipid droplets. When an oocyte is warmed to physiological temperatures after cooling, a fraction of saturated lipids may remain in the ordered conformational state. The fractions of monounsaturated and polyunsaturated lipids redistribute to the core of lipid droplets. Monounsaturated lipids undergo the transition to the ordered conformational state below −10°C. Using deuterated fatty acids with a different number of double bonds, we reveal how different lipid fractions are involved in the lipid phase transition of a cytoplasmic lipid droplet and how they can affect cell survival. Raman spectroscopy of deuterated lipids has proven to be a promising tool for studying the lipid phase transitions and lipid redistributions inside single organelles within living cells.     

Lipid phase transitions measured in intact cells with Fourier transform infrared spectroscopy

Lipid phase transitions in membranes are thought to be a major damaging event during cooling of cells prior to cryopreservation or during warming after freeze-thaw has been completed. Although there is abundant evidence that such transitions occur in isolated phospholipids, the evidence that they are found in membranes in intact cells is less clear, due largely to technical difficulties in detecting such transitions in the complex mixtures of lipids and proteins found in natural membranes. We show here that Fourier transform infrared spectroscopy provides a rapid, convenient method for detecting these transitions in intact cells. We have used intact pollen grains of cattail (Typha latifolia) as a primary experimental subject. Spectra taken of the intact pollen grains show most of the features commonly seen in natural membrane vesicles or pure phospholipids. Shifts in the vibrational frequency and width of the CH2 bands with temperature can be used to detect lipid phase transitions. Biochemical analysis, coupled with the spectroscopy, was used to assign transitions to nonpolar and polar lipids. Finally, although assignment of the melting lipid unambiguously in other cells has not yet been made, we show that the transitions can nevertheless be detected in other intact cells, including those of four plant species and sperm of three animals.     

Lipid phase transitions in cytoplasmic and outer membranes of Escherichia coli

The cytoplasmic and outer membranes containing either trans-Δ⁹-octadecenoate, trans-Δ⁹-hexadecenoate or cis-Δ⁹-octadecenoate as predominant unsaturated fatty acid residues in the phospholipids were prepared from a fatty acid auxotroph, Escherichia coli strain K1062. Order-disorder transitions of the phospholipids were revealed in both fractions of the cell envelope by fluorescent probing or wide angle X-ray diffraction. The mid-transition temperatures, $\text{T}\text{t}$, and the range of the transition, $\text{ΔT}$, are similar in the outer and cytoplasmic membrane. Relative to the corresponding extracted lipids, 60–80% of the hydrocarbon chains take part in the transition in the cytoplasmic membrane whereas in the outer membrane only 25–40% of the chains become ordered. The results suggest that in the outer membrane part of the lipids form fluid domains in the form of mono- and/or bilayers.     

Lipid phase transitions in fatty acid-homogeneous membranes of Acholeplasma laidlawii B

The thermotropic behaviour of fatty acid-homogeneous membranes of Acholeplasma laidlawii B was investigated by Fourier transform infrared spectroscopy. The organism was grown at 37°C in the presence of avidin, an inhibitor of fatty acid synthesis, in a medium supplemented with pentadecanoic acid-d₂₉; the enrichment of the membranes with this fatty acid was 95%. The temperature-dependent phase behaviour of the membranes was studied via the C–D stretching vibrational modes of the membrane lipids and was compared with that of the lipid extract. The high level of fatty acid homogeneity results in a sharp (for natural membranes) gel to liquid crystalline phase transition. The transition, in both the membranes and extracted lipids, is centered at about 6°C above the growth temperature. During the transition two principal liquid states are evident, one being more conformationally ordered than the other. The effect of proteins on the principal lipid phase transition is minimal. However, in the intact membranes there is evident a weaker, lower temperature transition, which is not evident in the extracted lipids.     

Lipid phase transitions in model biomembranes: The effect of ions on phosphatidylcholine bilayers

Differential scanning calorimetry has been used to study the endothermic phase behaviour of some model biomembranes (i.e. phosphatidylcholine-water systems) in the presence of a wide range of alkaline, alkaline earth and heavy metal salts. Studies and comparisons were made of both cation and anion effects. Shifts occur in the temperatures of both the pre-transition and main transition endotherms. The observed shifts are smaller than those which have been reported for charged lipids, and no evidence has been found for the formation of specific complexes. Electron microscopic studies on freeze-fractured dispersions of phosphatidylcholine-water-salt systems show that with some salts the typical rippled surface observed with l-α-dimyristoyl phosphatidylcholine, when in the gel state, is replaced by a smooth surface.     

Effect of inorganic cations on phase transitions.

The effect of protons and cations on the crystal (gel)-to-liquid crystal transition temperature Tm of isoelectric and negatively charged phospholipids are summarized. The general trends emerging are as follows: Tm depends on the state of ionization of the phospholipid in that Tm-vs-pH-curves parallel the titration curve of the phospholipid. Protonation of phospholipids causes Tm to increase, deprotonation or ionization has the opposite effect. The effects of cations on the Tm of phospholipids may be grouped into non-specific and specific effects. Unspecific effects of cations such as the screening of negative charges of the phospholipid polar group are qualitatively similar to protonation: Tm increases, in the order monovalent less than divalent less than trivalent cations and the effects on negatively charged phospholipids are larger than those on isoelectric phospholipids. Unspecific, electrostatic effects on Tm are reasonably well accounted for by the Gouy-Chapman theory. If, however, specific binding comes into play and/or electrostatic effects are accompanied by changes in phospholipid structure, simple, electrostatic theories fail to explain the observed changes in Tm. The crystal (gel)-to-liquid crystal transition is also a function of the degree of hydration: Tm generally decreases with increasing hydration reaching a plateau in excess H2O. In addition to screening of electric charges, ions may exert yet another non-specific effect: ions may affect Tm indirectly by competing with the phospholipid polar group for water of hydration. This indirect effect plays a role at high ionic strength and/or at low hydration of the phospholipid. Specific binding of cations to negatively charged phospholipids can lead to tight associations of the metal ion with the lipid polar group. Isothermal crystallization of the phospholipid bilayer is induced that is accompanied by a total or partial loss of water of hydration resulting in a marked increase in Tm. For instance, in crystalline Ca2(+)-phosphatidylserine complexes Tm is increased by more than 100 degrees C.     

Thermal phase transitions in deuterated lecithin bilayers.

Differential Thermal Analyses and Optical Density measurements show that perdeuteration of the fatty acid residues in phosphatidylcholines causes a 4–5°C decrease in the phase transition temperatures of bilayer dispersions prepared from these deuterated phospholipids. The implications of these findings on the use of deuterated phospholipids in membrane research will be briefly discussed.     

Lipid unsaturation determines the interaction of AFP type I with model membranes during thermotropic phase transitions

We have previously shown that antifreeze protein (AFP) type I from winter flounder interacts with the acyl chains of lipids in model membranes containing a mixture of dimyristoylphosphatidylcholine (DMPC) and the plant thylakoid lipid digalactosyldiacylglycerol (DGDG), most likely through hydrophobic interactions. By contrast, in studies with pure phospholipid membranes, no such interaction was seen. DGDG is a highly unsaturated lipid, which renders these studies quite different from the previous studies of AFP-membrane interaction where the lipids were saturated or trans-unsaturated. Therefore, it seemed possible that either the digalactose headgroups or the unsaturated DGDG acyl chains, or both, may be important for interactions of membranes with AFP type I. To distinguish between these possibilities, we catalytically hydrogenated the DGDG to obtain a galactolipid with completely saturated fatty acyl chains. The results with the hydrogenated DGDG were strikingly different from those obtained previously with the unsaturated DGDG; the clear binding of AFPs to the bilayer appeared to be lost. Nevertheless, the temperature-dependent folding of AFP type I was inhibited in the presence of liposomes containing either the unsaturated or the hydrogenated DGDG. The results indicate that the liposomes and protein still interact, even following hydrogenation of the acyl chains, perhaps at the membrane-solution interface.     

Isothermal lipid phase transitions

In liotropic lipid systems phase transitions can be induced isothermally by changing the solvent concentration or composition; alternatively, lipid composition can be modified by (bio)chemical means. The probability for isothermal phase transitions increases with the decreasing transition entropy; it is proportional to the magnitude of the transition temperature shift caused by transformation-inducing system variation. Manipulations causing large thermodynamic effects, such as lipid (de)hydration, binding of protons or divalent ions and macromolecular adsorption, but also close bilayer approach are, therefore, likely to cause structural lipid change(s) at a constant temperature. Net lipid charges enhance the membrane susceptibility to salt-induced isothermal phase transitions; a large proportion of this effect is due to the bilayer dehydration, however, rather than being a consequence of the decreased Coulombic electrostatic interactions. Membrane propensity for isothermal phase transitions, consequently, always increases with the hydrophilicity of the lipid heads, as well as with the desaturation and shortening of the lipid chains. Upon a phase change at a constant temperature, some of the interfacially bound solutes (e.g. protons or calcium) are released in the solution. Membrane permeability and fusogenicity simultaneously increase. In mixed systems, isothermal phase transitions, moreover, may result in lateral phase separation. All this opens up ways for the involvement of isothermal phase transitions in the regulation of biological processes.     

Cold-induced lipid phase transitions

The structural organization of biological membranes is largely determined by the weak interactions existing between their components and between these components and their aqueous environment. These interactions are particularly sensitive to changes in temperature and hydration. The factors influencing membrane lipid phase behaviour are briefly reviewed and used to develop a phase-separation model describing the response of biological membranes to stress. The factors affecting the interaction of cryoprotectants with membrane lipids are explored and their role in the stabilization of membrane organization at low temperatures discussed. It is suggested that the basis of their protective action lies in an ability to preserve the balance of interactions between membrane components at low temperatures at a level similar to that existing under physiological conditions.     

Lipid thermotropic transitions in Triatoma infestans lipophorin

The structure and lipid thermotropic transitions of highly purified lipophorin of Triatoma infestans were examined by several techniques: steady-state fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH), cis-parinaric acid (cis-PnA) and trans-parinaric acid (trans-PnA), light scattering fluorescence energy transfer between the lipophorin tryptophan residues and the bound chromophores, DPH, trans-parinaric acid cis-parinaric acid, gel electrophoresis, and gel filtration. Fluorescence polarization of PnAs and DPH revealed a reversible lipid thermotropic transition in intact lipophorin at about 20 degrees C and 18 degrees C, respectively. In lipophorin, lipid dispersion fluorescence polarization of DPH detected a lipid transition approximately at 20 degrees C, while trans-PnA showed a gel phase formation at a temperature below 30 degrees C. Similar experiments in which trans-PnA was incorporated into diacylglycerols and phospholipids extracted from the lipophorin revealed gel phase formation below 30 degrees C and 24 degrees C, respectively. Light scattering measurements showed that lipophorin particles aggregate irreversibly at 45 degrees C, increasing the molecular weight, as determined by gel filtration on Sephacryl S-300, from 740,000 to values larger than 1,500,000. The particle aggregation did not change the physical properties of the lipophorin studied by fluorescence polarization, indicating that the aggregation is apparently a non-denaturing process. Energy transfer between the lipophorin tryptophans and the bound chromophores cis-PnA, trans-PnA, and DPA revealed a different location of the fluorescent probes within the lipophorin. Temperature-dependence on the energy transfer efficiency for all probes confirmed a change in the ordering of the lipophorin lipids at 24 degrees C.     

Membrane phase transitions and the transport of chlortetracycline.

When chlortetracycline is added to a suspension of respiring Staphylococcus aureus cells, the active transport of the antibiotic may be monitored by its fluorescence enhancement as it moves from a polar aqueous environment into the apolar regions of the membrane. The initial rates of transport are temperature dependent with a maximal rate between 35 and 45 °C. Arrhenius plots of the initial rates are biphasic with a transition temperature of 27 °C for control cells. This transition temperature is sensitive to the fatty acid composition of the S. aureus cells. By culturing the cells in the presence of oleic acid or at 10 °C, the S. aureus cells incorporate a larger percentage of unsaturated and branched chain fatty acids into their membranes, resulting in transition temperatures 8–9 °C lower than the control cells. Studies of depolarization of fluorescence also indicate that the mobility of the bound chlortetracycline is temperature-dependent. Temperature transitions occur at the same temperatures as those measured by Arrhenius plots. The transition temperatures indicated by the Arrhenius plots and the polarization studies are believed to reflect order-disorder phase transitions associated with the melting of the phospholipids in the cell envelope.     

A theoretical model for lipid monolayer phase transitions.

We present a theoretical model for the liquid-expanded to liquid-condensed phase transition observed in many phospholipid monolayer films. The total two-dimensional pressure in the model is the sum of the hydrocarbon chain pressure and the surface pressure. The hydrocarbon chain pressure is calculated in an exteded version of a model published earlier. The surface pressure results from a lowering of the surface tension in the monolayer over that of pure water, thus producing a force on a Langmuir float. When these two contributions are added, pi/A isotherms are obtained which have slope discontinuities very similar to those observed experimentally. The results indicate that a successful model for lipid phase behavior must consider the interactions between head groups and water as well as cooperative hydrocarbon chain melting.     

Temperature- and cyclic nucleotide-induced phase transitions of Histoplasma capsulatum.

The transition from yeast to mycelia of Histoplasma capsulatum could be accomplished by shifting the temperature of incubation from 37 to 25 degrees C. It was accompanied by many changes in cellular metabolism, including changes in respiration, intracellular cyclic adenosine 3',5'-monophosphate (cAMP) levels, and activities of two enzymes specific for the yeast phase, cystine reductase (EC 1.6.4.1) and cysteine oxidase (EC 1.13.11.20). Even at 37 degrees C, the yeast to mycelial transition could be induced by cAMP and agents which raise the intracellular levels of cAMP (theophylline, acetylsalicylic acid, prostaglandin E1, and nerve growth factor). During this morphogenesis the same pattern of changes occurred as in the temperature-induced transition. Therefore, these changes were not simply dependent on a shift in temperature, but rather were part of the process of the phase transition.