Exploration of molecular interactions in cholesterol superlattices: effect of multibody interactions

Experimental evidences have indicated that cholesterol may adapt highly regular lateral distributions (i.e., superlattices) in a phospholipid bilayer. We investigated the formations of superlattices at cholesterol mole fraction of 0.154, 0.25, 0.40, and 0.5 using Monte Carlo simulation. We found that in general, conventional pairwise-additive interactions cannot produce superlattices. Instead, a multibody (nonpairwise) interaction is required. Cholesterol superlattice formation reveals that although the overall interaction between cholesterol and phospholipids is favorable, it contains two large opposing components: an interaction favoring cholesterol-phospholipid mixing and an unfavorable acyl chain multibody interaction that increases nonlinearly with the number of cholesterol contacts. The magnitudes of interactions are in the order of kT. The physical origins of these interactions can be explained by our umbrella model. They most likely come from the requirement for polar phospholipid headgroups to cover the nonpolar cholesterol to avoid the exposure of cholesterol to water and from the sharp decreasing of acyl chain conformation entropy due to cholesterol contact. This study together with our previous work demonstrate that the driving force of cholesterol-phospholipid mixing is a hydrophobic interaction, and multibody interactions dominate others over a wide range of cholesterol concentration.     

Effect of free cholesterol on incorporation of triolein in phospholipid bilayers

Triacylglycerols are the major substrates for lipolytic enzymes that act at the surface of emulsion-like particles such as triglyceride-rich lipoproteins, chylomicrons, and intracellular lipid droplets. This study examines the effect of cholesterol on the solubility of a triacylglycerol, triolein, in phospholipid surfaces. Solubilities of [carbonyl-13C]triolein in phospholipid bilayer vesicles containing between 0 and 50 mol % free cholesterol, prepared by cosonication, were measured by 13C NMR. The carbonyl resonances from bilayer-incorporated triglyceride were shifted downfield in the 13C NMR spectra from those corresponding to excess, nonincorporated material. This enabled solubilities to be determined directly from carbonyl peak intensities at most cholesterol concentrations. The bilayer solubility of triolein was inversely proportional to the cholesterol/phospholipid mole ratio. In pure phospholipid vesicles the triolein solubility was 2.2 mol %. The triglyceride incorporation decreased to 1.1 mol % at a cholesterol/phospholipid mole ratio of 0.5, and at a mole ratio of 1.0 for the bilayer lipids, the triolein solubility was reduced to just 0.15 mol %. The effects of free cholesterol were more pronounced and progressive than observed previously on the bilayer solubility of cholesteryl oleate (Spooner, P. J. R., Hamilton, J. A., Gantz, D. L., & Small, D. M. (1986) Biochim. Biophys. Acta 860, 345-353]. As with cholesteryl oleate, we suggest that cholesterol also displaces solubilized triglyceride to deeper regions of the bilayer.     

Maximum solubility of cholesterol in phosphatidylcholine and phosphatidylethanolamine bilayers

In any lipid bilayer membrane, there is an upper limit on the cholesterol concentration that can be accommodated within the bilayer structure; excess cholesterol will precipitate as crystals of pure cholesterol monohydrate. This cholesterol solubility limit is a well-defined quantity. It is a first-order phase boundary in the phospholipid/cholesterol phase diagram. There are many different solubility limits in the literature, but no clear picture has emerged that can unify the disparate results. We have studied the effects that different sample preparation methods can have on the apparent experimental solubility limit. We find that artifactual demixing of cholesterol can occur during conventional sample preparation and that this demixed cholesterol may produce artifactual cholesterol crystals. Therefore, phospholipid/cholesterol suspensions which are prepared by conventional methods may manifest variable, falsely low cholesterol solubility limits. We have developed two novel preparative methods which are specifically designed to prevent demixing during sample preparation. For detection of the cholesterol crystals, X-ray diffraction has proven to be quantitative and highly sensitive. Experiments based on these methods yield reproducible and precise cholesterol solubility limits: 66 mol% for phosphatidylcholine (PC) bilayers and 51 mol% for phosphatidylethanolamine (PE) bilayers. We present evidence that these are true, equilibrium values. In contrast to the dramatic headgroup effect (PC vs. PE), acyl chain variations had no effect on the cholesterol solubility limit in four different PC/cholesterol mixtures.     

Ternary phase diagram of dipalmitoyl-PC/dilauroyl-PC/cholesterol: nanoscopic domain formation driven by cholesterol

A ternary phase diagram is proposed for the hydrated lamellar lipid mixture dipalmitoylphosphatidylcholine/dilauroylphosphatidylcholine/cholesterol (DPPC/DLPC/cholesterol) at room temperature. The entire composition space has been thoroughly mapped by complementary experimental techniques, revealing interesting phase behavior that has not been previously described. Confocal fluorescence microscopy shows a regime of coexisting DPPC-rich ordered and DLPC-rich fluid lamellar phases, having an upper boundary at apparently constant cholesterol mole fraction chi(chol) approximately 0.16. Fluorescence resonance energy transfer experiments confirm the identification and extent of this two-phase regime and, furthermore, reveal a 1-phase regime between chi(chol) approximately 0.16 and 0.25, consisting of ordered and fluid nanoscopic domains. Dipyrene-PC excimer/monomer measurements confirm the new regime between chi(chol) approximately 0.16 and 0.25 and also show that rigidly ordered phases seem to disappear around chi(chol) approximately 0.25. This study should be considered as a step toward a more complete understanding of lateral heterogeneity within biomembranes. Cholesterol may play a role in domain separation on the nanometer scale.     

Comparison of cholesterol-phospholipid interaction in bilayers of liposomes and the red cell membrane

The energetics of interactions of cholesterol with phospholipid in simple liposome bilayers were compared with those in the bilayer of the human erythrocyte membrane, by measuring cholesterol distribution between erythrocytes and liposomes prepared from their whole phospholipid extract. With liposomes of a range of initial cholesterol contents, the equilibrium value for $\text{r}$, the ratio of cholesterol/phospholipid in the liposomes to that in the cells, is in the range 1.1–1.2. The closeness of this value to 1.0 indicates that overall cholesterol-phospholipid interaction in the cell membrane is similar to that in liposomes. However, while the deviation from 1.0 is small, and could arise from average cholesterol-phospholipid interactions in the membrane being only 0.06 to 0.1 kcal · mol^?1 weaker than in liposomes, it could also result from 10 to 20% of the cell membrane phospholipid being unavailable to mix with cholesterol.     

The immiscible cholesterol bilayer domain exists as an integral part of phospholipid bilayer membranes

Electron paramagnetic resonance (EPR) spin-labeling methods were used to study the organization of cholesterol and phospholipids in membranes formed from Chol/POPS (cholesterol/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylserine) mixtures, with mixing ratios from 0 to 3. It was confirmed using the discrimination by oxygen transport and polar relaxation agent accessibility methods that the immiscible cholesterol bilayer domain (CBD) was present in all of the suspensions when the mixing ratio exceeded the cholesterol solubility threshold (CST) in the POPS membrane. The behavior of phospholipid molecules was monitored with phospholipid analogue spin labels (n-PCs), and the behavior of cholesterol was monitored with the cholesterol analogue spin labels CSL and ASL. Results indicated that phospholipid and cholesterol mixtures can form a membrane suspension up to a mixing ratio of ~2. Additionally, EPR spectra for n-PC, ASL, and CSL indicated that both phospholipids and cholesterol exist in these suspensions in the lipid-bilayer-like structures. EPR spectral characteristics of n-PCs (spin labels located in the phospholipid cholesterol bilayer, outside the CBD) change with increase in the cholesterol content up to and beyond the CST. These results present strong evidence that the CBD forms an integral part of the phospholipid bilayer when formed from a Chol/POPS mixture up to a mixing ratio of ~2. Interestingly, CSL in cholesterol alone (without phospholipids) when suspended in buffer does not detect formation of bilayer-like structures. A broad, single-line EPR signal is given, similar to that obtained for the dry film of cholesterol before addition of the buffer. This broad, single-line signal is also observed in suspensions formed for Chol/POPS mixtures (as a background signal) when the Chol/POPS ratio is much greater than 3. It is suggested that the EPR spin-labeling approach can discriminate and characterize the fraction of cholesterol that forms the CBD within the phospholipid bilayer.     

Lateral distribution of cholesterol in dioleoylphosphatidylcholine lipid bilayers: cholesterol-phospholipid interactions at high cholesterol limit

Lateral organization of cholesterol in dioleoyl-phosphatidylcholine (DOPC) lipid bilayers at high cholesterol concentration (>45 mol%) was investigated using steady-state fluorescence anisotropy and fluorescent resonance energy transfer techniques. The recently devised Low Temperature Trap method was used to prepare compositionally uniform cholesterol/DOPC liposomes to avoid the problem of lipid demixing. The fluorescence anisotropy of diphenylhexatrience chain-labeled phosphatidylcholine (DPH-PC) in these liposomes exhibited local maxima at cholesterol mol fractions of 0.50 and 0.57, and a sharp drop at 0.67. For the liposomes labeled with both dehydroergosterol and DPH-PC, the fluorescent resonance energy transfer efficiency from dehydroergosterol to DPH-PC displayed a steep jump at cholesterol mol fraction of 0.5, and dips at 0.57 and 0.68. These results indicate the presence of highly ordered cholesterol regular distribution domains at those observed critical compositions. The observed critical mol fraction at 0.67 agreed favorably with the solubility limit of cholesterol in DOPC bilayers as independently measured by light scattering and optical microscopy. The regular distribution at 0.57 was previously predicted from a Monte Carlo simulation based on the Umbrella model. The results strongly support the hypothesis that the primary requirement for cholesterol-phospholipid mixing is that the polar phospholipid headgroups need to cover the nonpolar body of cholesterol to avoid the exposure of cholesterol to water.     

Liposome fusion catalytically induced by phospholipase C

Large unilamellar vesicles composed of phosphatidylcholine/phosphatidylethanolamine/cholesterol (50:25:25 mole ratio) were treated with phospholipase C. The early stages of phospholipid cleavage are accompanied by mixing of bilayer lipids (monitored by dequenching of octadecylrhodamine fluorescence) and leakage-free mixing of vesicle contents [measured by using 8-aminonaphthalene-1,3,6-trisulfonic acid (ANTS) and p-xylylenebis(pyridinium bromide) (DPX)]. These results are interpreted in terms of vesicle fusion induced by the catalytic activity of phospholipase C. The use of sonicated unilamellar vesicles decreases the lag time, but does not modify the amplitude, of the fusion process. The presence of both phosphatidylethanolamine and cholesterol appears to be essential for measurable fusion effects to occur with low levels of phospholipid hydrolysis. Optimal fusion rates are observed with about 10-20 enzyme molecules per large unilamellar vesicle. This system of catalytically induced liposome fusion may be of relevance for the interpretation of physiological membrane fusion processes.     

Lipid-protein interactions of the human erythrocyte concanavalin a receptor in phospholipid bilayers

The interaction of the human erythrocyte concanavalin A receptor (a subpopulation of Band 3) with phospholipids has been investigated using differential scanning microcalorimetry of reconstituted vesicles prepared by detergent dialysis. The mean diameter of dialyzed phospholipid vesicles jumps dramatically on inclusion of the concanavalin A receptor and then increases linearly with the fraction of protein in the bilayer. The glycoprotein has a dramatic effect on the phospholipid gel to liquid-crystalline phase transition, and ΔH decreases linearly with increasing mole fraction of protein up to a protein/lipid mole ratio of around 1:1160. Extrapolation of this data indicates that each concanavalin A receptor is able to perturb about 685 molecules of dimyristoylphosphatidylcholine, withdrawing them from the main phase transition. The cooperativity of phospholipid melting is profoundly disrupted by small amounts of glycoprotein, with the cooperative unit dropping to less than half its initial values at a protein/lipid mole ratio of 1:3800. A break occurs in the ΔH curve as the protein/lipid mole ratio is increased above 1:1160, and ΔH then increases linearly with increasing amounts of concanavalin A receptor in the bilayer. This phenomenon may be interpreted in terms of protein-protein aggregation which occurs in the phospholipid bilayer above a certain critical mole fraction of concanavalin A receptor, resulting in perturbed phospholipids being returned to the phase transition. In addition, the hydrophilic domains of the glycoprotein may exist in two different conformations depending on the protein concentration in the bilayer, and these may differ in their ability to interact with phospholipid headgroups at the membrane surface.     

The effect of free cholesterol on the solubilization of cholesteryl oleate in phosphatidylcholine bilayers: A 13C-NMR study

The solubilization of cholesteryl oleate in sonicated phosphatidylcholine vesicles containing between 0 and 50 mol% cholesterol was studied by 13C-NMR using isotopically enriched [carbonyl-13C]cholesteryl oleate. The carbonyl-13C chemical shift from cholesteryl oleate in the phospholipid/cholesterol bilayer was significantly downfield from that for cholesteryl oleate in an oil phase and the peak area, relative to that of the phospholipid carbonyl, was used to determine bilayer solubility of the ester. The solubility (with respect to phospholipid) in the phospholipid bilayer without cholesterol (2.9 mol%) was only moderately reduced (to 2.3 mol%) at cholesterol levels up to 33 mol% but showed a more marked reduction to 1.4 mol% at 40 mol% cholesterol or 1.2 mol% at 50 mol% cholesterol. Since the vesicles containing 50 mol% cholesterol were larger (520 +/- 152 A diameter) than those with no cholesterol (291 +/- 97 A diameter), we measured the solubility of cholesteryl oleate in large vesicles with no cholesterol, prepared by extrusion through polycarbonate membrane filters, and found it similar to that in small, sonicated vesicles with no cholesterol. Therefore, the larger size of vesicles was not the factor responsible for the decreased cholesteryl oleate solubility at high cholesterol contents. A more direct effect of cholesterol is envisioned where the ester becomes displaced to deeper regions of the bilayer.     

Cholesterol modulation of lipid intermixing in phospholipid and glycosphingolipid mixtures. Evaluation using fluorescent lipid probes and brominated lipid quenchers.

Carbazole- and indole-labeled phospholipids have been used to monitor the homo- or heterogeneity of lipid mixing in several types of lipid bilayers combining a brominated and a nonbrominated lipid with varying amounts of cholesterol. Experimental quenching curves (relating the normalized probe fluorescence intensity to the mole fraction of brominated lipid) show a characteristic smooth, monophasic form for homogeneous liquid-crystalline lipid mixtures. However, for mixtures exhibiting lipid lateral segregation, such curves show marked perturbations in form over the region of composition where segregation occurs. Using this approach, it is found that high mole fractions of cholesterol (40-50 mol %) promote the formation of apparently homogeneous solutions in mixtures of disaturated and monounsaturated phosphatidylcholines (PCs) that exhibit extensive thermotropic phase separations in the absence of sterol. At only slightly lower levels of cholesterol, however, these systems exhibit inhomogeneous lipid mixing over a wide range of relative proportions of the two PC components. Mixtures of cerebroside and monounsaturated PCs, even at high bilayer cholesterol contents, exhibit significant inhomogeneity in lipid mixing over a wide range of cerebroside/PC ratios. Phase-separating PC/PC and PC/cerebroside mixtures can readily form long-lived metastable solutions when the level of the higher-melting component in the liquid-crystalline phase exceeds its equilibrium solubility by as much as 20-30 mol %; this tendency is significantly increased by cholesterol. Cholesterol shows no significant ability to enhance lipid intermixing in a third type of phase-separating lipid system, combining a monounsaturated PC with a monounsaturated phosphatidic acid--calcium complex. Experiments using cleavable phospholipid conjugates, linking a fluorescent lipid to a brominated lipid, suggest that each fluorescent molecule probes a local lipid domain comprising approximately less than 40-50 nearby acyl chains.     

Cholesterol-phospholipid interaction in membranes. 1. Cholestane spin-label studies of phase behavior of cholesterol-phospholipid liposomes

The effect of cholesterol concentration on the thermotropic phase behavior of aqueous phospholipid multi-bilayers was monitored by means of electron spin resonance spectroscopy (ESR) of a cholestane spin-label (CSL). The spin-label itself induces an additional transition in several different phospholipids, which is attributed to local melting around the spin probe. In contrast, cholesterol prevents its neighboring phospholipids from undergoing fluidization. Small additions of cholesterol affect the position of the probe-induced lipid mobilization curve. The phospholipid main gel-liquid-crystal transition, which is also observed as a separate change in probe mobilization, is not affected by low concentrations of cholesterol. These observations indicate the presence of two phases, a cholesterol-rich phase and a pure phospholipid phase, and indicate that CSL preferentially enters the cholesterol-rich phase. Addition of more than 20 mol % cholesterol abolishes the bulk phospholipid phase. This is evidenced by the disappearance of the gel-liquid-crystal transition as observed by ESR. However, the CSL-induced transition is present at all concentrations of cholesterol and CSL. The behavioral differences between the two sterols caution against using this probe as a direct substitute for cholesterol. However, it remains a useful tool for monitoring the phase behavior of cholesterol-phospholipid bilayer systems.     

Phosphorylation reverses the membrane association of peptides that correspond to the basic domains of MARCKS and neuromodulin.

Several groups have observed that phosphorylation causes the MARCKS (Myristoylated Alanine-Rich C Kinase Substrate) protein to move off cell membranes and phospholipid vesicles. Our working hypothesis is that significant membrane binding of MARCKS requires both hydrophobic insertion of the N-terminal myristate into the bilayer and electrostatic association of the single cluster of basic residues in the protein with acidic lipids and that phosphorylation reverses this electrostatic association. Membrane binding measurements with myristoylated peptides and phospholipid vesicles show this hydrophobic moiety could, at best, barely attach proteins to plasma membranes. We report here membrane binding measurements with basic peptides that correspond to the phosphorylation domains of MARCKS and neuromodulin. Binding of these peptides increases sigmoidally with the percent acidic lipid in the phospholipid vesicle and can be described by a Gouy-Chapman/mass action theory that explains how electrostatics and reduction of dimensionality produce apparent cooperativity. The electrostatic affinity of the MARCKS peptide for membranes containing 10% acidic phospholipids (10(4) M-1 = chi/[P], where chi is the mole ratio of peptide bound to the outer monolayer of the vesicles and [P] is the concentration of peptide in the aqueous phase) is the same as the hydrophobic affinity of the myristate moiety for bilayer membranes. Phosphorylation decreases the affinity of the MARCKS peptide for membranes containing 15% acidic lipid about 1000-fold and produces a rapid (t1/2 < 30 s) dissociation of the peptide from phospholipid vesicles.     

Modulation of the phase transition behavior of phosphatidylethanolamine by cholesterol and oxysterols

Cholesterol lowers the bilayer to hexagonal phase transition temperature of phosphatidylethanolamines up to a mole fraction of about 0.1. At cholesterol mole fractions above about 0.3, the effect of this sterol is to stabilize the bilayer phase. The relatively weak effects of cholesterol in altering the bilayer to hexagonal phase transition temperature can be explained on the basis of lateral phase separation. This is indicated by the horizontal liquidus line for the gel to liquid-crystalline transition in the phase diagram for mixtures of cholesterol with dielaidoylphosphatidylethanolamine (DEPE) as well as the fact that cholesterol does not greatly decrease the cooperativity of the bilayer to hexagonal phase transition. The enthalpy of this latter transition increased with increasing mole fractions of cholesterol. Two oxidation products of cholesterol are 5-cholesten-3 beta,7 alpha-diol and cholestan-3 beta,5 alpha,6 beta-triol. Compared with cholesterol, 5-cholesten-3 beta,7 alpha-diol had a greater effect in decreasing the bilayer to hexagonal phase transition temperature and broadening this transition. It is suggested that its effectiveness is due to its greater solubility in the DEPE. In contrast, cholestan-3 beta,5 alpha,6 beta-triol raises the bilayer to hexagonal phase transition temperature of DEPE. This is due to its larger and more hydrophilic head group. In addition, its length, being shorter than that of DEPE, would not allow it to pack efficiently in a hexagonal phase arrangement.We suggest that this same effect is responsible for cholesterol raising the bilayer to hexagonal phase transition temperature at higher mole fractions.     

Interaction of short-chain lecithin with long-chain phospholipids: characterization of vesicles that form spontaneously

Stable unilamellar vesicles formed spontaneously upon mixing aqueous suspensions of long-chain phospholipid (synthetic, saturated, and naturally occurring phosphatidylcholine, phosphatidylethanolamine, and sphingomyelin) with small amounts of short-chain lecithin (fatty acid chain lengths of 6-8 carbons) have been characterized by using NMR spectroscopy, negative staining electron microscopy, differential scanning calorimetry, and Fourier transform infrared (FTIR) spectroscopy. This method of vesicle preparation can produce bilayer vesicles spanning the size range 100 to greater than 1000 A. The combination of short-chain lecithin and long-chain lecithin in its gel state at room temperature produces relatively small unilamellar vesicles, while using long-chain lecithin in its liquid-crystalline state produces large unilamellar vesicles. The length of the short-chain lecithin does not affect the size distribution of the vesicles as much as the ratio of short-chain to long-chain components. In general, additional short-chain decreases the average vesicle size. Incorporation of cholesterol can affect vesicle size, with the solubility limit of cholesterol in short-chain lecithin micelles governing any size change. If the amount of cholesterol is below the solubility limit of micellar short-chain lecithin, then the addition of cholesterol to the vesicle bilayer has no effect on the vesicle size; if more cholesterol is added, particle growth is observed. Vesicles formed with a saturated long-chain lecithin and short-chain species exhibit similar phase transition behavior and enthalpy values to small unilamellar vesicles of the pure long-chain lecithin prepared by sonication. As the size of the short-chain/long-chain vesicles decreases, the phase transition temperature decreases to temperatures observed for sonicated unilamellar vesicles. FTIR spectroscopy confirms that the incorporation of the short-chain lipid in the vesicle bilayer does not drastically alter the gauche bond conformation of the long-chain lipids (i.e., their transness in the gel state and the presence of multiple gauche bonds in the liquid-crystalline state).     

Effects of replacement of the hydroxyl group of cholesterol and tocopherol on the thermotropic behavior of phospholipid membranes

The role of the hydroxyl groups of cholesterol and tocopherol in mediating their interaction with phospholipid bilayers has been a subject of considerable interest. We have examined this question by using derivatives of cholesterol and tocopherol in which the hydroxyl group is esterified to succinate. The hemisuccinate esters of cholesterol and alpha-tocopherol can be readily incorporated into phospholipid membranes and in fact can by themselves form closed membrane vesicles as demonstrated by the encapsulation of [3H]sucrose. The thermotropic behavior of mixtures containing each succinate ester and phospholipid was studied by differential scanning calorimetry. The effect of cholesteryl hemisuccinate on the thermotropic properties of dipalmitoylphosphatidylcholine and dimyristoylphosphatidylethanolamine is very similar to that of cholesterol. This indicates that the 3 beta-OH is not required for the formation of a cholesterol-phospholipid complex. In mixtures of tocopherol acid succinate and phospholipids the peak transition temperature is progressively shifted to lower temperatures as the mole fraction of alpha-tocopherol succinate is increased, while the enthalpy of the transition is only slightly affected. At a tocopherol succinate/phospholipid molar ratio of 9/1 a phase transition is still detectable. A comparison between tocopherol succinate and tocopherol indicates that the substitution of the hydroxyl group reduces the interaction of tocopherol with phospholipids to a small but measurable extent. Thus, the hydroxyl group of tocopherol is more important than the hydroxyl group of cholesterol in influencing their interactions with phospholipids.     

Phospholipid peroxidation as a factor in gallstone pathogenesis

Phospholipid peroxidation markedly reduces the stability of mixed micellar systems composed of cholate, phosphatidylcholine and supersaturating levels of cholesterol. This suggests that lipid peroxidation is likely to play a significant role in the precipitation of cholesterol from gallbladder bile, thus in the pathogenesis of cholesterol gallstones. This conclusion is supported by studies of the nucleation time of cholesterol in gallbladder biles, which was significantly reduced by exposure to a stream of oxygen. This effect of phospholipid peroxidation on cholesterol solubility may occur in other biological fluids as well. In view of the increased lipid peroxidation in the elderly, it may explain the effect of age on the frequency of various diseases related to cholesterol precipitation.     

Ceramide drives cholesterol out of the ordered lipid bilayer phase into the crystal phase in 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine/cholesterol/ceramide ternary mixtures

The effect of brain ceramide on the maximum solubility of cholesterol in ternary mixtures of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), cholesterol, and ceramide was investigated at 37 degrees C by a cholesterol oxidase (COD) reaction rate assay and by optical microscopy. The COD reaction rate assay showed a sharp increase in cholesterol chemical potential as the cholesterol mole fraction approaches the solubility limit. A decline in the COD reaction rate was found after the formation of cholesterol crystals. The maximum solubility of brain ceramide in POPC bilayers was determined to be 68 +/- 2 mol % by microscopy. We found that ceramide has a much higher affinity for the ordered bilayers than cholesterol, and the maximum solubility of cholesterol decreases with the increase in ceramide content. More significantly, the displacement of cholesterol by ceramide follows a 1:1 relation. At the cholesterol solubility limit, adding one more ceramide molecule to the lipid bilayer drives one cholesterol out of the bilayer into the cholesterol crystal phase, and cholesterol is incapable of displacing ceramide from the bilayer phase. On the basis of these findings, a ternary phase diagram of the POPC/cholesterol/ceramide mixture was constructed. The behaviors of ceramide and cholesterol can be explained by the umbrella model. Both ceramide and cholesterol have small polar headgroups and relatively large nonpolar bodies. In a PC bilayer, ceramide and cholesterol compete for the coverage of the headgroups of neighboring PC to prevent the exposure of their nonpolar bodies to water. This competition results in the 1:1 displacement as well as the displacement of cholesterol by ceramide from lipid raft domains.     

Effect of lipidic factors on membrane cholesterol topology--mode of binding of theta-toxin to cholesterol in liposomes.

We have previously suggested the existence of two distinct states for cholesterol in cell membranes as revealed by high- and low-affinity binding sites for theta-toxin of Clostridium perfringens. In liposomes, phospholipid and cholesterol compositions, but not membrane protein composition, have been shown to be major determinants for the topology of membrane cholesterol. The effects of lipidic factors on cholesterol topology were investigated in detail by analyzing toxin binding to large unilamellar liposomes composed of cholesterol and phospholipids (neutral phospholipids/phosphatidylglycerol = 82:18, mol/mol). The numbers of high- and low-affinity toxin-binding sites depend strictly on the cholesterol mole percentage in liposomes. High-affinity toxin-binding sites appear only in liposomes with high cholesterol contents. Liposomes whose cholesterol/phospholipid ratio is 0.4 or less have no high-affinity sites regardless of their phospholipid compositions, while low-affinity sites appear in liposomes with lower cholesterol contents. The threshold values for the cholesterol mole percentage above which high-affinity toxin-binding sites appear were examined. The values decrease in accordance with the increase in the mole fraction of 18-carbon hydrocarbon chains among the total 14-18 carbon-hydrocarbon chains of the liposomal phospholipids. Furthermore, both the partial replacement of phosphatidylcholine with phosphatidylethanolamine and the digestion of phospholipids with phospholipase C also affect the threshold values. Thus the cholesterol mole percentage, in combination with phospholipid chain length and other factors, determines the topology of membrane cholesterol providing distinctively different affinity sites for theta-toxin.     

The interaction of cholesterol and cholest-4-en-3-one with dipalmitoylphosphatidylcholine. Comparison based on the use of three fluorophores

This study compares cholesterol-phospholipid and cholest-4-en-3-one-phospholipid interactions by their effect on thermotropic behavior of dipalmitoylphosphatidylcholine bilayers. This was approached by determining the temperature-dependent steady-state fluorescence anisotropy of three fluorophores; diphenylhexatriene (DPH), hydroxy-coumarin (HC) and trans-parinaric acid (TPA). The fluorophores monitor different lateral and vertical locations of the lipid bilayers; DPH and HC average laterally the properties of the hydrophobic and headgroup regions of the bilayer, respectively, while TPA distribution is determined by the lateral organization of the bilayer. The data show that the two steroids have similar qualitative but different quantitative effects. Both diminish the pretransition and behave as 'averagers', broadening the main gel to liquid crystalline phase transition through ordering of the acyl chains in the liquid crystalline state and disordering of them in the gel state. However, the mechanisms by which the two molecules operate are different. Cholesterol is more effective particularly on the hydrophobic region of the bilayer, and its effect is not linear with its mole fraction. A sharp increase of the steady-state fluorescence anisotropy occurs around 20 mol% cholesterol. The effect of cholestenone is proportional to its mole fraction. The difference between the effects of the two steroids is explained by the dissimilarity in their lateral distribution. Cholesterol forms cholesterol-rich domains. The size of the boundary regions which surround the cholesterol-rich domains changes drastically at about 20 mol% cholesterol. Cholestenone, on the other hand, is randomly distributed in the bilayer plane and therefore it does not cause the formation of such defined boundary regions. This study as well as reports by others suggests that the important structural differences between the two steroids are the molecular packing parameter and the presence of small polar group at the 3-beta position of the steroid.