Influence of cholesterol on the polar region of phosphatidylcholine and phosphatidylethanolamine bilayers

The structural changes in the polar head group region of unsonicated bilayer membranes of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine and 1,2-dipalmitoyl-sn-glycero-3-phosphoethanolamine produced by addition of cholesterol have been determined using deuterium and phosphorus-31 NMR. Incorportion of up to 50 mol percent cholesterol produces little change in the phosphorus-31 chemical shielding anisotropies, compared with the values in pure bilayers above the phase transition temperatures, while some of the deuterium quadrupole splittings are reduced by almost a factor of two. Adjustment of the head group torsion angles by only a few degrees accounts for the observed spectral changes. Addition of cholesterol therefore has opposite effects on the hydrocarbon and polar regions of membranes: although cholesterol makes the hydrocarbon region gel-like, with an increased probability of trans conformations, the conformation of the polar head groups is very similar to that found in the liquid crystalline phase of pure phospholipid bilayers.     

Studies on the anomalous thermotropic behavior of aqueous dispersions of dipalmitoylphosphatidylcholine-cholesterol mixtures

Examination of the thermotropic behavior of aqueous dispersions of dipalmitoylphosphatidylcholine-cholesterol mixtures by high-sensitivity scanning calorimetry has revealed that the phospholipid gel to liquid-crystalline phase transition consists of two components. One, a relatively sharp transition centered at 39.6-40.7 degrees C, exhibits a transition enthalpy change which decreases linearly with increasing cholesterol content, approaching zero at a cholesterol content of about 25 mol %. The other, a broad, lower intensity transition centered at approximately 41.5 degrees C for cholesterol concentrations of 20 mol %, displays an enthalpy change which is maximal at about 20-25 mol % cholesterol and which decreases as the cholesterol content decreases to zero or increases above 25 mol %. The origin of these two transitions is discussed in terms of a separation of these lipid mixtures into cholesterol-rich and cholesterol-poor domains.     

Phosphatidylcholine structure determines cholesterol solubility and lipid polymorphism

In the present work, we demonstrate that phosphatidylcholine with (16:1)9 acyl chains undergoes polymorphic rearrangements in mixtures with 0.6-0.8 mol fraction cholesterol. Studies were performed using differential scanning calorimetry, X-ray diffraction, cryo-electron microscopy, 31P NMR static powder patterns and 13C MAS/NMR. Mixtures of phosphatidylcholine with (16:1)9 acyl chains and 0.6 mol fraction cholesterol, after being heated to 100 degrees C, can form an ordered array with periodicity 14 nm which may be indicative of a cubic phase. Our results indicate that the formation of highly curved bilayer structures, such as those required for membrane fusion, can occur in mixtures of cholesterol with certain phosphatidylcholines that do not form non-lamellar structures in the absence of cholesterol. We also determine the polymorphic behavior of mixtures of symmetric phosphatidylcholines with cholesterol. Species of phosphatidylcholine with (20:1)11, (22:1)13 or (24:1)15 acyl chains in mixtures with 0.6-0.8 mol fraction cholesterol undergo a transition to the hexagonal phase at temperatures 70-80 degrees C. This is not the case for phosphatidylcholine with (18:1)6 acyl chains which remains in the lamellar phase up to 100 degrees C when mixed with as much as 0.8 mol fraction cholesterol. Thus, the polymorphic behavior of mixtures of phosphatidylcholine and cholesterol is not uncommon and is dependent on the intrinsic curvature of the phospholipid. Crystals of cholesterol can be detected in mixtures of all of these phosphatidylcholines at sufficiently high cholesterol mole fraction. What is unusual about the formation of these crystals in several cases is that cholesterol crystals are present in the monohydrate form in preference to the anhydrous form. Furthermore, after heating to 100 degrees C and recooling, the cholesterol crystals are again observed to be in the monohydrate form, although pure cholesterol crystals require many hours to rehydrate after being heated to 100 degrees C. Both the nature of the acyl chain as well as the mole fraction cholesterol determine whether cholesterol crystals in mixtures with the phospholipids will be in the monohydrate or in the anhydrous form.     

Phase equilibria of cholesterol/dipalmitoylphosphatidylcholine mixtures: 2H nuclear magnetic resonance and differential scanning calorimetry

Deuterium nuclear magnetic resonance spectroscopy and differential scanning calorimetry are used to map the phase boundaries of mixtures of cholesterol and chain-perdeuteriated 1,2-dipalmitoyl-sn-glycero-3-phosphocholine at concentrations from 0 to 25 mol % cholesterol. Three distinct phases can be identified: the L alpha or liquid-crystalline phase, the gel phase, and a high cholesterol concentration phase, which we call the beta phase. The liquid-crystalline phase is characterized by highly flexible phospholipid chains with rapid axially symmetric reorientation; the gel phase has much more rigid lipid chains, and the motions are no longer axially symmetric on the 2H NMR time scale; the beta phase is characterized by highly ordered (rigid) chains and rapid axially symmetric reorientation. In addition, we identify three regions of two-phase coexistence. The first of these is a narrow L alpha/gel-phase coexistence region lying between 0 and about 6 mol % cholesterol at temperatures just below the chain-melting transition of the pure phospholipid/water dispersions, at 37.75 degrees C. The dramatic changes in the 2H NMR line shape which occur on passing through the phase transition are used to map out the boundaries of this narrow two-phase region. The boundaries of the second two-phase region are determined by 2H NMR difference spectroscopy, one boundary lying near 7.5 mol % cholesterol and running from 37 down to at least 30 degrees C; the other boundary lies near 22 mol % cholesterol and covers the same temperature range. Within this region, the gel and beta phases coexist. As the temperature is lowered below about 30 degrees C, the phospholipid motions reach the intermediate time scale regime of 2H NMR so that spectral subtractions become difficult and unreliable. The third two-phase region lies above 37 degrees C, beginning at a eutectic point somewhere between 7.5 and 10 mol % cholesterol and ending at about 20 mol %. In this region, the L alpha and beta phases are in equilibrium. The boundaries for this region are inferred from differential scanning calorimetry traces, for the boundary between the L alpha- and the two-phase region, and from a dramatic sharpening of the NMR peaks on crossing the boundary between the two-phase region and the beta-phase region. In this region, the technique of difference spectroscopy fails, presumably because the diffusion rate in both the L alpha- and beta-phase domains is so rapid that phospholipid molecules exchange rapidly between domains on the experimental time scale.     

Influence of the physical state of the membrane on the enzymatic activity and energy of activation of protein kinase C alpha.

The activation of protein kinase C alpha was studied by using a lipid system consisting of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoserine (POPS) (molar ratio 4:1) and different proportions of 1-palmitoyl-2-oleoyl-sn-glycerol (POG). The phase behavior of the lipidic system was characterized by using differential scanning calorimetry and 31P NMR, and a phase diagram was elaborated. The results suggested the formation of two diacylglycerol/phospholipid complexes, one at 15 mol % of POG and the second at 30 mol % of POG. These two complexes would define the three regions of the phase diagram: in the first region (concentrations of POG lower than 15 mol %) there is gel-gel immiscibility at temperatures below that of the phase transition between C1 and pure phospholipid, and a fluid lamellar phase above of the phase transition. In the second region (between 15 and 30 mol % of POG), gel-gel immiscibility between C1 and C2 with fluid-fluid immiscibility was observed, while inverted hexagonal HII and isotropic phases were detected by 31P NMR. In the third region (concentrations of POG higher than 30 mol %), gel-gel immiscibility seemed to occur between C2 and pure POG along with fluid-fluid immiscibility, while an isotropic phase was detected by 31P NMR. When PKC alpha activity was measured, as a function of POG concentration, maximum activity was found at POG concentrations as low as 5-10 mol %; the activity slightly decreased as POG concentration was increased to 45 mol % at 32 degrees C (above Tc) whereas activity did not change with increasing concentrations of POG at 5 degrees C (below Tc). When the activity was studied as a function of temperature, at different POG concentrations, and depicted as Arrhenius plots, it was found that the activity increased with increasing temperatures, showing a discontinuity at a temperature very close to the phase transition of the system and a lower activation energy at the upper slope of the graph, indicating that the physical state of the membrane affected the interaction of PKC alpha with the membrane.     

Time-resolved fluorometric and differential scanning calorimetric investigation of dehydroergosterol in 1-stearoyl-2-caprylphosphatidylcholine bilayers

Thermal and dynamic properties of dehydroergosterol (DHE) in 1-stearoyl-2-capryl-sn-glycero-3-phosphocholine [C(18):C(10)PC] have been studied by differential scanning calorimetry (DSC) and multifrequency phase-modulation fluorometry. C(18):C(10)PC is an asymmetric mixed-chain phosphatidylcholine known to form highly ordered mixed interdigitated bilayers below the maximal transition temperature, Tm, and partially interdigitated bilayers above Tm. This lipid system is thus unique in assessing the interactions between sterols and interdigitated lipid bilayers. DHE is a fluorescent analogue of cholesterol shown in previous studies to behave like cholesterol in noninterdigitated symmetric diacylphosphatidylcholines. DSC data show that DHE exhibits similar characteristics to cholesterol [Chong & Choate (1989) Biophys. J. 55, 551-556] in C(18):C(10)PC bilayers. DHE abolishes the phase transition of C(18):C(10)PC at 27 mol % compared to 25 mol % for cholesterol and decreases Tm, the onset temperature (To), and the completion temperature (Tc), at a similar rate to cholesterol at about -0.25 degrees C per mole percent DHE. Fluorescence data show that the rotational motion of DHE can be described by a hindered anisotropic model. In the gel state of C(18):C(10)PC, the rotational correlation of DHE decreases monotonically with increasing DHE content up to 24 mol %, suggesting that DHE causes a disordering/spacing effect on the packing of mixed interdigitated C(18):C(10)PC bilayers. The rotational correlation time undergoes an abrupt increase from 24 to 27 mol % DHE. Abrupt changes in the DSC parameters were also observed in the neighborhood of 27 mol %, suggesting that major reorganization takes place around this concentration.(ABSTRACT TRUNCATED AT 250 WORDS)     

Direct Visualization of the Lateral Structure of Porcine Brain Cerebrosides/POPC Mixtures in Presence and Absence of Cholesterol

We studied the thermal behavior of membranes composed of mixtures of natural cerebrosides (from porcine brain) and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) with and without cholesterol, using differential scanning calorimetry, Fourier transform infrared spectroscopy, and confocal/multiphoton fluorescence microscopy. The POPC/cerebroside mixture display solid ordered/liquid disordered phase coexistence in a broad range of compositions and temperatures in agreement with previous results reported for POPC/(bovine brain)cerebrosides. The observed phase coexistence scenario consists of elongated, micrometer-sized cerebroside-rich solid ordered domains that span the bilayer, embedded in a POPC-rich liquid disordered phase. The data obtained from differential scanning calorimetry and Fourier transform infrared spectroscopy was in line with that obtained in the microscopy experiments for the binary mixture, except at very high cerebroside molar fractions (0.8-0.9) were some differences are observed. Cholesterol incorporation exerts strong changes on the lateral organization of POPC/porcine brain cerebroside membranes. At intermediate cholesterol concentrations (10-25 mol %) the solid ordered/liquid disordered phase coexistence scenario gradually transform to a solid ordered/liquid ordered one. Above 25 mol % of cholesterol two distinct regions with liquid ordered phase character are visualized in the membrane until a single liquid ordered phase forms at 40 mol % cholesterol. The observed cholesterol effect largely differs from that reported for POPC/porcine brain ceramide, reflecting the impact of the sphingolipids polar headgroup on the membrane lateral organization.     

Differential scanning calorimetry and 2H NMR studies of the phase behavior of gramicidin-phosphatidylcholine mixtures

The extents of two-phase coexistence in the phase diagrams of mixtures of gramicidin with 1,2-bis(perdeuteriopalmitoyl)-sn-glycero-3-phosphocholine (DPPC-d62) and with 1,2-bis(perdeuteriomyristoyl)-sn-glycero-3-phosphocholine (DMPC-d54) mixtures have been explored with differential scanning calorimetry (DSC) and deuterium nuclear magnetic resonance (2H NMR). For both systems, increased gramicidin content causes a decrease in transition enthalpy and a broadening of the peak in excess heat capacity at the transition. In DMPC-d54-based mixtures, the broadening is roughly symmetric about the pure lipid transition temperature. Addition of gramicidin to DPPC-d62 extends the excess heat capacity peak on the low-temperature side, resulting in a slightly asymmetric scan. Deuterium NMR spectra showing a superposition of gel and liquid-crystalline components, observed for both mixtures, indicate the presence of two-phase coexistence. For the DPPC-d62-based mixtures, two-phase coexistence is restricted to an approximately 2 degrees C temperature range below the pure transition temperature. For DMPC-d54-based mixtures, the region of two-phase coexistence is even narrower. For both mixtures, beyond a gramicidin mole fraction of 2%, distinct gel and liquid-crystal contributions to the spectra cannot be distinguished. Along with the broad featureless nature of the DSC scan in this region, this is taken to indicate that the transition has been replaced by a continuous phase change. These results are consistent with the existence of a closed two-phase region having a critical concentration of gramicidin below 2 mol%.     

A new high-temperature transition of crystalline cholesterol in mixtures with phosphatidylserine

Phosphatidylserine and cholesterol are two major components of the cytoplasmic leaflet of the plasma membrane. The arrangement of cholesterol is markedly affected by the presence of phosphatidylserine in model membranes. At relatively low mol fractions of cholesterol in phosphatidylserine, compared with other phospholipids, cholesterol crystallites are formed that exhibit both thermotropic phase transitions as well as diffraction of x-rays. In the present study we have observed and characterized a novel thermotropic transition occurring in mixtures of phosphatidylserine and cholesterol. This new transition is observed at 96 degrees C by differential scanning calorimetry (DSC), using a heating scan rate of 2 degrees C/min. Observation of the transition requires that the hydrated lipid mixture be incubated for several days, depending on the temperature of incubation. The rate of formation of the material exhibiting a transition at 96 degrees C is more rapid at higher incubation temperatures. At 37 degrees C the half-time of conversion is approximately 7 days. Concomitant with the appearance of the 96 degrees C peak the previously known transitions of cholesterol, occurring at approximately 38 degrees C and 75 degrees C on heating scans of freshly prepared suspensions, disappear. These two transitions correspond to the polymorphic transition of anhydrous cholesterol and to the dehydration of cholesterol monohydrate, respectively. The loss of the 75 degrees C peak takes a longer time than that of the 38 degrees C peak, indicating that anhydrous cholesterol first gets hydrated to the monohydrate form exhibiting a transition at 75 degrees C and subsequently is converted by additional time of incubation to an altered form of the monohydrate, showing a phase transition at 96 degrees C. After several weeks of incubation at 37 degrees C, only the form with a phase transition at 96 degrees C remains. If such a sample undergoes several successive heating and cooling cycles, the 96 degrees C peak disappears and the 38 degrees C transition reappears on heating. For samples of 1-palmitoyl-2-oleoyl phosphatidylserine or of 1-stearoyl-2-oleoyl phosphatidylserine having mol fractions of cholesterol between 0.4 and 0.7, the 38 degrees C transition that reappears after the melting of the 96 degrees C component generally has the same enthalpy as do freshly prepared samples. This demonstrates that, at least for these samples, the amount of anhydrous cholesterol crystallites formed is indeed a property of the lipid mixture. We have also examined variations in the method of preparation of the sample and find similar behavior in all cases, although there are quantitative differences. The 96 degrees C transition is partially reversible on cooling and reheating. This transition is also scan rate dependent, indicating that it is, at least in part, kinetically determined. The enthalpy of the 96 degrees C transition, after incubation of the sample for 3 weeks at 37 degrees C is dependent on the ratio of cholesterol to 1-palmitoyl-2-oleoyl phosphatidylserine or to 1-stearoyl-2-oleoyl phosphatidylserine, with the enthalpy per mole cholesterol increasing between cholesterol mol fractions of 0.2 and 0.5. Dimyristoyl phosphatidylserine at a 1:1 molar ratio with cholesterol, after incubation at 37 degrees C, exhibits a transition at 95 degrees C that reverses on cooling at 44 degrees C, instead of 60 degrees C, as observed with either 1-palmitoyl-2-oleoyl phosphatidylserine or 1-stearoyl-2-oleoyl phosphatidylserine. These findings along with the essential absence of the 96 degrees C transition in pure cholesterol or in cholesterol/phosphatidylcholine mixtures, indicates that the phospholipid affects the characteristics of the transition, and therefore the cholesterol crystallites must be in direct contact with the phospholipid and are not simply in the form of pure crystals of cholesterol. These observations are particularly important in view of recent observations of the presence of cholesterol crystals in biological systems.     

Cholesterol crystalline polymorphism and the solubility of cholesterol in phosphatidylserine

There is a marked hysteresis between the heating and cooling polymorphic phase transition of anhydrous cholesterol. At a scan rate of 0.05 degrees C/min the difference in transition temperatures between heating and cooling scans is approximately 10 degrees C. This phenomenon also occurs with mixtures of cholesterol with phosphatidylserine and can result in an underestimation of the amount of crystalline cholesterol in a sample that has not been cooled sufficiently. With 1-palmitoyl-2-oleoyl phosphatidylserine and 1-stearoyl-2-oleoyl phosphatidylserine the cholesterol crystallites form while the lipid remains in the L(alpha) phase. Sonication of dimyristoyl phosphatidylserine with a 0.4 mol fraction cholesterol results in the loss of cholesterol crystallite diffraction, but only a partial loss of the polymorphic transition detected by calorimetry. We therefore conclude that the thermal history of the sample can have profound effects on the appearance of the polymorphic phase transition of cholesterol by differential scanning calorimetry. Depending on the morphology of the vesicles, diffraction methods may underevaluate the amount of cholesterol crystallites present.     

Phospholipid Chain Interactions with Cholesterol Drive Domain Formation in Lipid Membranes

Cholesterol is a key component of eukaryotic membranes, but its role in cellular biology in general and in lipid rafts in particular remains controversial. Model membranes are used extensively to determine the phase behavior of ternary mixtures of cholesterol, a saturated lipid, and an unsaturated lipid with liquid-ordered and liquid-disordered phase coexistence. Despite many different experiments that determine lipid-phase diagrams, we lack an understanding of the molecular-level driving forces for liquid phase coexistence in bilayers with cholesterol. Here, we use atomistic molecular dynamics computer simulations to address the driving forces for phase coexistence in ternary lipid mixtures. Domain formation is directly observed in a long-timescale simulation of a mixture of 1,2-distearoyl-sn-glycero-3-phosphocholine, unsaturated 1,2-dilinoleoyl-sn-glycero-3-phosphocholine, and cholesterol. Free-energy calculations for the exchange of the saturated and unsaturated lipids between the ordered and disordered phases give insight into the mixing behavior. We show that a large energetic contribution to domain formation is favorable enthalpic interactions of the saturated lipid in the ordered phase. This favorable energy for forming an ordered, cholesterol-rich phase is opposed by a large unfavorable entropy. Martini coarse-grained simulations capture the unfavorable free energy of mixing but do not reproduce the entropic contribution because of the reduced representation of the phospholipid tails. Phospholipid tails and their degree of unsaturation are key energetic contributors to lipid phase separation.     

A calorimetric study of the thermotropic behavior of pure sphingomyelin diastereomers

The phase-transition properties of sphingomyelins were investigated in detail with totally synthetic, chemically and stereochemically pure (2S,3R)-(N-stearoylsphingosyl)-1-phosphocholine (D-erythro-C18-SPM) (1) and the corresponding 2S,3S isomer (L-threo-C18-SPM) (2). Heating scans of an unsonicated dispersion of 1 right after hydration showed a main transition (I) at 44.7 degrees C (delta H = 6.8 kcal/mol). Upon incubation at 20-25 degrees C a second transition (II) appeared at 36.0 degrees C (delta H = 5.7 kcal/mol). The two gel phases were designated as G alpha and G beta phases, respectively. The G beta phase was also metastable and relaxed to a third gel phase (G gamma) upon incubation below 10 degrees C. Conversion of the G gamma phase to the liquid-crystalline phase occurred via two new endotherms at 33.4 degrees C (2.6 kcal/mol) (III) and 43.6 degrees C (8.0 kcal/mol) (IV) as well as a main transition at 44.7 degrees C (9.5 kcal/mol). Possible interpretations have been proposed to account for the observed phase transitions. The L-threo isomer 2 showed similar thermotropic behavior to dipalmitoylphosphatidylcholine (DPPC): a "main transition" at 44.2 degrees C (6.0 kcal/mol), a "pretransition" at 43.1 degrees C (1.8 kcal/mol), and upon incubation at 7 degrees C for 2 weeks, a very broad "subtransition" at ca. 35 degrees C. The results are substantially different from previous studies of sphingomyelins using mixtures of stereoisomers. Mixing of 1 with 2, 1 with DPPC, and 2 with DPPC removed the metastability of the gel phase and resulted in a single transition.     

Structure and thermotropic properties of 1-stearoyl-2-acetyl-phosphatidylcholine bilayer membranes.

The structural and thermotropic properties of 1-stearoyl-2-acetyl-phosphatidylcholine (C(18):C(2)-PC) were studied as a function of hydration. A combination of differential scanning calorimetry and x-ray diffraction techniques have been used to investigate the phase behavior of C(18):C(2)-PC. At low hydration (e.g., 20% H2O), the differential scanning calorimetry heating curve shows a single reversible endothermic transition at 44.6 degrees C with transition enthalpy delta H = 6.4 kcal/mol. The x-ray diffraction pattern at -8 degrees C shows a lamellar structure with a small bilayer periodicity d = 46.3 A and two wide angle reflections at 4.3 and 3.95 A, characteristic of a tilted chain, L beta' bilayer gel structure. Above the main transition temperature, a liquid crystalline L alpha phase is observed with d = 53.3 A. Electron density profiles at 20% hydration suggest that C(18):C(2)-PC forms a fully interdigitated bilayer at -8 degrees C and a noninterdigitated, liquid crystalline phase above its transition temperature (T > Tm). Between 30 and 50% hydration, on heating C(18):C(2)-PC converts from a highly ordered, fully interdigitated gel phase (L beta') to a less ordered, interdigitated gel phase (L beta), which on further heating converts to a noninterdigitated liquid crystalline L alpha phase. However, the fully hydrated (> 60% H2O) C(18):C(2)-PC, after incubation at 0 degrees C, displays three endothermic transitions at 8.9 degrees C (transition I, delta H = 1.6 kcal/mol), 18.0 degrees C (transition II), and 20.1 degrees C (transition III, delta HII+III = 4.8 kcal/mol). X-ray diffraction at -8 degrees C again showed a lamellar gel phase (L beta') with a small periodicity d = 52.3 A. At 14 degrees C a less ordered, lamellar gel phase (L beta) is observed with d = 60.5 A. However, above the transition III, a broad, diffuse reflection is observed at approximately 39 A, consistent with the presence of a micellar phase. The following scheme is proposed for structural changes of fully hydrated C(18):C(2)-PC, occurring with temperature: L beta' (interdigitated)-->L beta (interdigitated)-->L alpha(noninterdigitated)-->Micelles. Thus, at low temperature C(18):C(2)-PC forms a bilayer gel phase (L beta') at all hydrations, whereas above the main transition temperature it forms a bilayer liquid crystalline phase L alpha at low hydrations and a micellar phase at high hydrations (> 60 wt% water).     

Fluid-phase chain unsaturation controlling domain microstructure and phase in ternary lipid bilayers containing GalCer and cholesterol

We report the microstructure and phase behavior of three ternary mixtures each containing a long-chain saturated glycosphingolipid, galactosylceramide (GalCer), and cholesterol at room temperature. The unsaturation level of the fluid-phase component was varied by lipid choice, i.e., saturated 1,2-dilauroyl-sn-glycero-3-phosphocholine (DLPC), singly unsaturated 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), or doubly unsaturated 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC). GalCer was used because of its biological significance, for example, as a ligand in the sexual transmission of HIV and stimulator of natural killer T-cells. Supported lipid bilayers of the ternary mixtures were imaged by atomic force microscopy and GalCer-rich domains were characterized by area/perimeter ratios (A/P). GalCer domain phase transitions from solid (S) to liquid (L) phase were verified by domain behavior in giant unilamellar vesicles, which displayed two-dimensional microstructure similar to that of supported lipid bilayers. As cholesterol concentration was increased, we observed approximately 2.5, approximately 10, and approximately 20-fold decreases in GalCer domain A/P for bilayers in L-S phase coexistence containing DOPC, POPC, and DLPC, respectively. The transition to L-L phase coexistence occurred at approximately 10 mol % cholesterol for bilayers containing DOPC or POPC and was accompanied by maintenance of a constant A/P. L-L phase coexistence did not occur for bilayers containing DLPC. We systematically relate our results to the impact of chain unsaturation on the interaction of the fluid-phase lipid and cholesterol. Physiologically, these observations may give insight into the interplay of fatty acid chain unsaturation, sterol concentration, and lipid hydrophobic mismatch in membrane phenomena.     

A calorimetric study of the thermotropic behavior of aqueous dispersions of natural and synthetic sphingomyelins.

A recently developed differential scanning calorimeter has been used to characterize the thermotropic behavior of aqueous dispersions of liposomes containing sphingomyelin. Liposomes derived from sheep brain sphingomyelin exhibit a broad gel-liquid crystalline phase transition in the temperature range of 20-45 degrees C. The transition is characterized by maxima in the heat capacity function at 31.2 and 37.1 degrees C and a total enthalpy change of 7.2 +/-0.4 kcal/mol. Beef brain sphingomyelin liposomes behave similarly but exhibit heat capacity maxima at 30, 32, and 38 degrees C and a total enthalpy change of 6.9 kcal/mol. The thermotropic behavior of four pure synthetic sphingomyelins is reminiscent of multilamellar lecithin liposomes in that a single, sharp, main transition is observed. Results obtained for liposomes containing mixtures of different sphingomyelins are complex. A colyophilized mixture of N-palmitoylsphingosinephosphorylcholine, N-stearoylsphingosinephosphorylcholine, and N-lignocerylsphingosinephosphorylcholine in a 1 : 1 : 1 mol ratio exhibits a single transition with a Tm below that observed for the individual components. On the other hand a 1 : 1 mixture of N-stearoylsphingosinephosphorylcholine and 1-palmitoyl-2-oleylphosphatidylcholine exhibits three maxima in the heat capacity function. It is clear from these results that the thermotropic behavior of sphingomyelin-containing liposomes is a complex function of the exact composition. Furthermore, it appears that the behavior of the liposomes derived from natural sphingomyelins cannot be explained in terms of phase separation of the individual components.     

Bilayer properties of totally synthetic C16:0-lactosyl-ceramide

Differential scanning calorimetry (DSC) and x-ray diffraction have been used to study the structural and thermal properties of totally synthetic D-erythro-N-palmitoyl-lactosyl-C(18)-sphingosine (C16:0-LacCer). Over the temperature range 0-90 degrees C, fully hydrated C16:0-LacCer shows complex thermal transitions characteristic of polymorphic behavior of exclusively bilayer phases. On heating at 5 degrees C/min, hydrated C16:0-LacCer undergoes a complex two-peak endothermic transition with maxima at 69 degrees C and 74 degrees C and a total enthalpy of 14.6 kcal/mol C16:0-LacCer. At a slower heating rate (1.5 degrees C/min), two endothermic transitions are observed at 66 degrees C and 78 degrees C. After cooling to 0 degrees C, the subsequent heating run shows three overlapping endothermic transitions at 66 degrees C, 69 degrees C, and 71.5 degrees C, followed by a chain-melting endothermic transition at 78 degrees C. Two thermal protocols were used to completely convert C16:0-LacCer to its stable, high melting temperature (78 degrees C) form. As revealed by x-ray diffraction, over the temperature range 20-78 degrees C this stable phase exhibits a bilayer structure, periodicity d approximately 65 A with an ordered chain packing mode. At the phase transition (78 degrees C) chain melting occurs, and C16:0-LacCer converts to a liquid crystalline bilayer (L(alpha)) phase of reduced periodicity d approximately 59 A. On cooling from the L(alpha) phase, C16:0-LacCer converts to metastable bilayer phases undergoing transitions at 66-72 degrees C. These studies allow comparisons to be made with the behavior of the corresponding C16:0-Cer (. J. Lipid Res. 36:1936-1944) and C16:0-GluCer and C16:0-GalCer (. J. Lipid Res. 40:839-849). Our systematic studies are aimed at understanding the role of oligosaccharide complexity in regulating glycosphingolipid structure and properties.     

Temperature dependence of the energy-linked monosaccharide transport across the cell membrane of Rhodotorula gracilis.

The temperature dependence of the active monosaccharide transport across the cell membrane of the yeast Rhodotorula gracilis has been studied between 0 and 55 degrees C with D-xylose as the transported substrate: (i) Between 0 and 10 degrees C there is virtually no transport. (ii) The initial velocity of transport increases exponentially from 15 to 30 degrees C (deltaE equal to 32 plus or minus 2 kcal/mol). (iii) At 30 degrees C a sharp "break" occurs in the Arrhenius plot and with increasing temperature the transport becomes inactivated, with a positive slope of the corresponding straight line ("deltaE equal to minus 15 kcal/mol"). (iv) In the temperature range of 50-55 degrees C, both the transport and the metabolic activity cease. In order to account for the abrupt changes of the membrane permeability, we attempted to ascribe them to phase transitions in the membrane structure: the first one, between 10 and 15 degrees C, to the crystalline: liquid-crystalline phase change; the second one, around 30 degrees C, to a change from highly ordered (low entropy) to less ordered (high entropy) membrane structure. Whereas the former phase transition is reversible, the latter appears to be irreversible. Arrhenius plots of the cell respiration exhibit a "break" at 30 degrees C, as well. However, at higher temperatures there is no thermal inactivation of the respiratory activity. The importance of a proper organization of the cell membrane constituents for the efficient transport function is discussed.     

Application of pressure perturbation calorimetry to lipid bilayers

Pressure perturbation calorimetry (PPC) is a new method that measures the heat consumed or released by a sample after a sudden pressure jump. The heat change can be used to derive the thermal volume expansion coefficient, alpha(V), as a function of temperature and, in the case of phase transitions, the volume change, DeltaV, occurring at the phase transition. Here we present the first report on the application of PPC to determine these quantities for lipid bilayers. We measure the volume changes of the pretransition and main transition of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC), and the thermal expansivity of the fluid phase of DMPC and of two unsaturated lipids, 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine and 1,2-dioleoyl-sn-glycero-3-phosphocholine. The high sensitivity of PPC instrumentation gives accurate data for alpha(V) and DeltaV even upon the application of relatively low pressures of approximately 5 bar.     

Interaction of cholesterol with galactocerebroside and galactocerebroside-phosphatidylcholine bilayer membranes

The interaction of the galactocerebroside, N-palmitoylgalactosylsphingosine (NPGS), with cholesterol has been studied by differential scanning calorimetry (DSC) and x-ray diffraction. Thermal and structural studies demonstrate complex behavior characterized by two endothermic transitions: transition I (TI approximately equal to 50-60 degrees C) corresponding to an NPGS-cholesterol bilayer gel----bilayer liquid crystal transition II (TII where TI less than TII less than TNPGS) corresponding to an NPGS bilayer crystal (stable E form)----bilayer liquid crystal transition. For mixtures containing from 6 to 80 mol % cholesterol, x-ray diffraction studies at 22 degrees C (T less than TI) indicate two separate lamellar phases; an NPGS crystal bilayer phase and a cholesterol monohydrate phase. For cholesterol concentrations less than 50 mol % at TI less than T less than TII, NPGS-cholesterol liquid crystal bilayer and excess NPGS crystal bilayer phases are observed. For greater than 50 mol % cholesterol concentrations at these temperatures, an excess cholesterol monohydrate phase coexists with the NPGS-cholesterol liquid crystal bilayers. At T greater than TII, complete NPGS-cholesterol miscibility is only observed for less than 50 mol % cholesterol concentrations, whereas at greater than 50 mol % cholesterol an excess cholesterol phase is present. The solid phase immiscibility of cerebroside and cholesterol at low temperatures is suggested to result from preferential NPGS-NPGS associations via hydrogen bonding. The unique thermal and structural behavior of NPGS-cholesterol dispersions is contrasted with the behavior of cholesterol-phosphatidycholine and cholesterol-sphingomyelin bilayers. Thermal and structural studies of NPGS in dipalmitoylphosphatidylcholine (DPPC)/cholesterol (1:1, molar ratio) bilayers have been performed. For dispersions containing less than 20 mol % NPGS at 22 degrees C there are no observable calorimetric transitions and x-ray diffraction studies indicate complete lipid miscibility. At greater than 20 mol % NPGS, a high temperature transition is observed that is shown by x-ray diffraction studies to be due to an excess NPGS crystal bilayer----liquid crystal bilayer transition. Complete miscibility of NPGS in DPPC/cholesterol bilayers is observed at T greater than TNPGS. The properties of NPGS/DPPC/cholesterol bilayers are discussed in terms of the lipid composition of the myelin sheath.     

An ordered metastable phase in hydrated phosphatidylethanolamine: the Y-transition

By using time-resolved X-ray diffraction, differential scanning calorimetry and scanning densitometry, we observed rapid formation at low temperature of a metastable ordered phase, termed LR1 phase, in fully hydrated dihexadecylphosphatidylethanolamine (DHPE). The LR1 phase has the same lamellar repeat period as the gel Lbeta phase but differs from the latter in its more ordered, orthorhombic hydrocarbon chain arrangement. It forms at about 12 degrees C upon cooling and manifests itself as splitting of the sharp, symmetric wide-angle X-ray peak of the DHPE gel phase into two reflections. This transition, designated the 'Y-transition', is readily reversible and proceeds with almost no hysteresis between cooling and heating scans. Calorimetrically, the LR1-->Lbeta transition is recorded as a low-enthalpy (0.2 kcal/mol) endothermic event. The formation of the LR1 phase from the gel phase is associated with a small, about 2 microl/g, decrease of the lipid partial specific volume recorded by scanning densitometry, in agreement with a volume calculation based on the X-ray data. The formation of the equilibrium Lc phase was found to take place from within the LR1 phase. This appears to be the only observable pathway for crystallisation of DHPE upon low-temperature incubation. Once formed, the Lc phase of this lipid converts directly into Lbeta phase at 50 degrees C, skipping the LR1 phase. Thus, the LR1 phase of DHPE can only be entered by cooling of the gel Lbeta phase. The data disclose certain similarities between the low-temperature polymorphism of DHPE and that of long-chain normal alkanes.