Calorimetric studies of the effects of cholesterol on the phase transition of C(18):C(10) phosphatidylcholine.

Differential scanning calorimetry (DSC) has been employed to study the effects of cholesterol on the phase transition of C(18):C(10) phosphatidylcholine (C(18):C(10)PC). C(18):C(10)PC is an asymmetric mixed-chain phosphatidylcholine known to form mixed-interdigitated structures below the transition temperature and form partially interdigitated lipid bilayers above the transition. Three types of samples were used. The treated sample is the lipid dispersion that had undergone three freeze-thaw cycles and stored at 4 degrees C for more than 48 h. The untreated sample was made by vortexing the dry lipid in 50 mM KCl, without the above-mentioned pretreatment. The cold-treated sample was prepared by incubating the treated sample at -20 degrees C for 15 d. There is no apparent difference in the DSC curves between the treated and cold-treated samples. The data derived from the treated samples seem to be more reproducible. The DSC curves between the cholesterol/C(18):C(10)PC and cholesterol/symmetric diacylphosphatidylcholine mixtures are different in three aspects: overall appearance, the cholesterol dependence of delta H, and the effect of cholesterol on the maximal transition temperature Tm, the onset temperature To, and the completion temperature Tc. for both the treated and untreated samples, the total enthalpy change delta H of the phase transition of C(18):C(10)PC decreases with increasing cholesterol content, approaching zero at approximately 25 mol%. This level is lower than the total enthalpy changes reported previously for the cholesterol/symmetric diacylphosphatidylcholine mixtures. Both the heating and cooling thermograms show that Tm, To, and Tc decrease with increasing cholesterol content. The decreasing rates of these temperatures with cholesterol are in the neighborhood of -0.24 degree per mol% of cholesterol.(ABSTRACT TRUNCATED AT 250 WORDS)     

Binary mixtures of saturated and unsaturated mixed-chain phosphatidylcholine. A differential scanning calorimetry study

High-resolution differential scanning calorimetry (DSC) has been used to study the aqueous dispersions of mixed-chain phosphatidylcholines prepared from colyophilized mixtures of C(18):C(11:1 delta 10) PC/C(18):C(10)PC and C(18):C(11:1 delta 10) PC/C(18):C(11)PC of various molar ratios. These mixed-chain phospholipids are characterized by a marked disparity in their acyl-chain lengths; however, the sn-1 acyl chain in the fully extended conformation is about twice as long as the sn-2 acyl chain. Their thermotropic behavior was determined, and the phase diagrams of these two mixtures were constructed from the calorimetric data. Results indicate that C(18):C(11:1 delta 10)PC/C(18):C(10)PC and C(18):C-(11:1 delta 10)PC/C(18):C(11)PC are miscible in all proportions with a near-ideal behavior of mixing in the gel and liquid-crystalline phases. Equimolar mixtures of diC(14)PC/C(18):C(11:1 delta 10)PC, diC(14)PC/C(18):C(10)PC, and diC(14)PC/C(18):C(11)PC have also been studied by DSC. These phosphatidylcholines in the 1:1 mixture differ in Tm by less than 11 degrees C; however, they exhibit gel-phase immiscibility in the plane of the bilayer. Taken together, these studies suggest that C(18):C(11)PC and C(18):C(11:1 delta 10)PC are packed similarly to C(18):C(10)PC in excess water as mixed interdigitated bilayers, at T less than Tm, which transform into partially interdigitated bilayers when heated above Tm.     

Monte Carlo simulation of lipid mixtures: finding phase separation.

The nonideal mixing of phosphatidylserine (PS) and phosphatidylcholine (PC) binary lipid mixtures was studied by computer simulation based on a model wherein the excess energy of mixing is divided between an electrostatic term and one adjustable term delta Em that includes all other nonideal interactions. The lateral distribution of the lipids and the energy of the mixtures were obtained by using Kawasaki relaxation in a canonical ensemble. The Gibbs free energies were calculated by Kirkwood's coupling parameter method. The simulation results are strongly dependent on simulation size for sizes smaller than about 1000 lipids. Nonideal interaction between lipids can result in large scale separation of lipid phases of different composition at reasonable delta Em values as well as clustering of like lipids. In plots of total Gibbs free energy of mixing versus PS mole fraction in PS/PC, the boundaries of the two phase region could be accurately determined. The electrostatic interaction influences cluster size and shape, and also the composition of phases in the two-phase region.     

Molecular mechanics and calorimetric studies of phosphatidylethanols

Phosphatidylethanols (PEths) are negatively charged diacyl phospholipids that are ubiquitously present in humans under the condition of alcohol intoxication. These lipids, derived in vivo from other naturally occurring phospholipids such as phosphatidylcholines (PC) via transphosphatidylation reaction as catalyzed by phospholipase D in the presence of ethanol, are well known to affect many biochemical properties of the cell membranes in humans. In this communication, we applied the combined approach of molecular mechanics (MM) simulations and high-sensitivity differential scanning calorimetry (DSC) to investigate the structure and phase transition behavior of PEth. We first determined the energy-minimized structures of tetrameric C(15):C(15)PEth arranged in two types of packing motif by the MM approach. An inwardly bent orientation of the lipid headgroup was observed; specifically, the methyl terminus of PEth's headgroup was juxtaposed intramolecularly to the C(2) atom of the sn-2 acyl chain. Clearly, this headgroup conformation was rather unique among all naturally occurring phospholipids. Subsequently, the phase transition behavior of the fully hydrated lipid bilayers prepared individually from 11 species of saturated C(X):C(Y)PEth with the same MW was studied by DSC, and the resulting Tm values were codified in terms of the normalized acyl chain asymmetry (deltaC/CL). A V-shaped Tm profile was observed in the plot of Tm versus deltaC/CL for each subclass of these lipids, suggesting two types of packing motif for C(X):C(Y)PEth at T < Tm. Moreover, it was observed that within each packing motif these Tm values were, on average, 2.0 +/- 0.9 degrees C smaller than the Tm values of the corresponding saturated PC. However, based on the unique headgroup conformation of PEth, we were able to predict that monounsaturated PEth with a cis double bond near the H2O/hydrocarbon interface would exhibit a higher Tm than the corresponding PC. Most interestingly, this prediction was indeed borne out by DSC results obtained with C(18):C(20:1delta5)PC and C(18):C(20:1delta5)PEth.     

Differential scanning calorimetry study of mixed-chain phosphatidylcholines with a common molecular weight identical with diheptadecanoylphosphatidylcholine

To examine the thermotropic phase behavior of various mixed-chain phosphatidylcholines in excess water and to compare it with the known behavior of identical-chain phosphatidylcholines, we have carried out high-resolution differential scanning calorimetric (DSC) studies on aqueous dispersions of 10 different mixed-chain phosphatidylcholines. These lipids, C(16):C(18)PC, C(18):C(16)PC, C(15):C(19)PC, C(19):C(15)PC, C(14):C(20)PC, C(20):C(14)PC, C(13):C(21)PC, C(21):C(13)PC, C(12):C(22)PC, and C(22):C(12)PC, have a common molecular weight which is the same as that of C(17):C(17)PC, an identical-chain phosphatidylcholine with a molecular weight of 762.2. When the values of any of the thermodynamic parameters (Tm, delta H, and delta S) of the mixed-chain phosphatidylcholines and C(17):C(17)PC are plotted against the normalized chain-length difference (delta C/CL), a linear function with negative slope is obtained provided that the value of delta C/CL is within the range of 0.09-0.4. The linear relationship suggests that these mixed-chain phospholipids are packed in the gel-state bilayer similar to the bilayer structure of C(17):C(17)PC at T less than Tm; however, the negative slope suggests that the conformational statistics of the hydrocarbon chain and the lateral lipid-lipid interactions of these phosphatidylcholines in the gel-state bilayer are perturbed proportionally by a progressive increase in the chain-length inequivalence between the two acyl chains within each lipid molecule. When the value of delta C/CL for mixed-chain phosphatidylcholines reaches the range of 0.44-0.55, the thermotropic phase behavior deviates markedly from that of less asymmetric phosphatidylcholines, suggesting that these highly asymmetric lipids are packed into mixed interdigitated bilayers at T less than Tm. The heating and cooling pathways of aqueous dispersions prepared from the 10 mixed-chain phospholipids are also discussed.     

Phosphatidylcholine acyl unsaturation modulates the decrease in interfacial elasticity induced by cholesterol.

The effect of cholesterol on the interfacial elastic packing interactions of various molecular species of phosphatidylcholines (PCs) has been investigated by using a Langmuir-type film balance and analyzing the elastic area compressibility moduli (Cs(-1)) as a function of average cross-sectional molecular area. Emphasis was on the high surface pressure regions (pi > or = 30 mN/m) which are thought to mimic biomembrane conditions. Increasing levels of cholesterol generally caused the in-plane elasticity of the mixed monolayers to decrease. Yet, the magnitude of the cholesterol-induced changes was markedly dependent upon PC hydrocarbon structure. Among PC species with a saturated sn-1 chain but different sn-2 chain cis unsaturation levels [e.g., myristate (14:0), oleate (18:1delta9(c), linoleate (18:2delta9,12(c), arachidonate (20:4delta5,8,11,14(c), or docosahexenoate (22:6delta4,7,10,13,16,19(c)], the in-plane elasticity moduli of PC species with higher sn-2 unsaturation levels were less affected by high cholesterol mol fractions (e.g., >30 mol %) than were the more saturated PC species. The largest cholesterol-induced decreases in the in-plane elasticity were observed when both chains of PC were saturated (e.g., di-14:0 PC). When both acyl chains were identically unsaturated, the resulting PCs were 20-25% more elastic in the presence of cholesterol than when their sn-1 chains were long and saturated (e.g., palmitate). The mixing of cholesterol with PC was found to diminish the in-plane elasticity of the films beyond what was predicted from the additive behavior of the individual lipid components apportioned by mole and area fraction. Deviations from additivity were greatest for di-14:0 PC and were least for diarachidonoyl PC and didocosahexenoyl PC. In contrast to Cs(-1) analyses, sterol-induced area condensations were relatively unresponsive to subtle structural differences in the PCs at high surface pressures. Cs(-1) versus average area plots also indicated the presence of cholesterol concentration-dependent, low-pressure (<14 mN/m) phase boundaries that became more prominent as PC acyl chain unsaturation increased. Hence, area condensations measured at low surface pressures often do not accurately portray which lipid structural features are important in the lipid-sterol interactions that occur at high membrane-like surface pressures.     

Calorimetric studies on the influence of N-methylated headgroups on the mixing behavior of diheptadecanoyl phosphatidylcholine with 1-behenoyl-2-lauroylphosphatidylcholine.

Recent studies of five different phosphatidylcholine/phosphatidylcholine (PC/PC) systems indicate that binary mixtures of phosphatidylcholines in which one component has a normalized chain length difference (delta C/CL) in the range of 0.09-0.40 and the other a delta C/CL in the range of 0.42-0.57 exhibit the phase behavior of a eutectic system. Here, delta C is the effective chain-length difference between the two acyl chains, and CL is the effective length of the longer of the two acyl chains for the same lipid molecule in the gel state. In each mixture, gel phase immiscibility occurs over a wide compositional range due to the difference in the gel phase acyl chain packing properties of each component. Although the mixtures differ in the location of their eutectic horizontal, with respect to temperature, all have a similar eutectic point that occurs at a composition of approximately 40 mol percent of the component with the delta C/CL value in the range of 0.42-0.57. Here, we extend these studies by systematically modifying the headgroup of C(17):C(17)PC and then analyzing the mixing behavior of the modified lipid with C(22):C(12)PC using DSC. Progressive demethylation of the C(17):C(17)PC headgroup leads to an increase in gel phase immiscibility and a decrease in the amount of C(22):C(12)PC that comprises the eutectic composition. The temperature defining the location of the eutectic horizontal, however, remains virtually unchanged in all three phase diagrams. Our results suggest that the eutectic composition is influenced by changes in gel phase acyl chain packing that are dependent on headgroup-headgroup interactions. In contrast, the eutectic nature of the phase diagram and the location of its solidus line are properties of acyl chain interactions that are independent of phospholipid headgroup-headgroup interactions.     

Cholesterol interacts with all of the lipid in bilayer membranes. Implications for models.

The interaction of cholesterol with lipid membranes has been studied by differential scanning calorimetry on liposomes, a technique which involves only the natural lipids, with no exogeneous probes. The influence of cholesterol at different molar percent concentrations c on the enthalpy delta H of the main gel to liquid crystal phase transition of saturated phosphatidylcholines of acyl chain length n = 12-20 was well represented by delta H = -9.43 + 1.01n - 0.268c kcal/mol. The linear dependence of delta H simultaneously upon chain length n and upon cholesterol concentration c shows clearly that cholesterol interacts with the deeper part of the lipids, as well as the superficial parts. This observation is not accommodated in any of the current models of cholesterol-lipid interactions.     

Interdigitated bilayer packing motifs: Raman spectroscopic studies of the eutectic phase behavior of the 1-stearoyl-2-caprylphosphatidylcholine/dimyristoylphosphatidylcholine binary mixture.

The thermotropic properties and acyl chain packing characteristics of multilamellar dispersions of binary mixtures of 1-stearoyl-2-caprylphosphatidylcholine (C(18):C(10)PC), an asymmetric chain species, and dimyristoylphosphatidylcholine (C(14):C(14)PC), a symmetric chain lipid, were monitored by vibrational Raman spectroscopy. In order to examine each component of the binary mixture separately, the acyl chains of the symmetric chain species were perdeuterated. As shown by differential scanning calorimetry, the mismatch in the gel phase bilayer thickness between the two lipid components generates a lateral phase separation resulting in two distinct gel phases, G(I) and G(II), which coexist over much of the composition range. The Raman data demonstrate that the mixed interdigitated phase (three chains per headgroup), analogous to single component phase behavior, is retained when the C(18):C(10)PC component act as a host for the G(I) gel phase. In contrast, the C(18):C(10)PC molecules exhibit partial interdigitation (two chains per headgroup) when they are included as guests within the C(14):C(14)PC host matrix to form the G(II) gel phase. Compared to pure C(14):C(14)PC bilayers at equivalent reduced temperatures, the host G(II) gel phase C(14):C(14)PC molecules exhibit an increased acyl chain order, while for the host G(I) gel phase the C(14):C(14)PC lipid species show increased intrachain disorder.     

Analysis of membrane lipids by 500 MHz 1H NMR

A nondestructive method has been developed for rapid analysis of lipid content of membrane extracts based on high field proton NMR spectroscopy. Lipid extraction is done by stepwise sonication of purified membranes into chloroform:methanol:water mixtures, and 1H spectra are recorded at 35 degrees C on final preparations consisting of at least 1 mg dried lipid solubilized in 2:1 CD3OD:CDCl3. Spectral peaks of lipid mixtures are assigned to lipid classes using a data base of standard lipid characteristic resonances derived from purified single membrane lipids and known mixtures of them. Peak intensities of characteristic peaks yield ratios of various lipids such as cholesterol:phospholipid and phosphatidylcholine:phosphatidylethanolamine, degree of unsaturation, average acyl chain length, total glycerol lipid content, and presence or absence of particular lipids, such as glycolipids or lysolipids. This procedure of membrane lipid analysis has been verified using known mixtures of purified standard lipids.     

Differential scanning calorimetric study of a homologous series of fully hydrated saturated mixed-chain C(X):C(X + 6) phosphatidylcholines

The successive high-resolution differential scanning calorimetric (DSC) thermograms for aqueous dispersions of a homologous series of mixed-chain phosphatidylcholines, C(X):C(X + 6)PC, have been recorded and analyzed. In this series of saturated mixed-chain phosphatidylcholines, the total number of carbon atoms in the sn-1 acyl chain increases from 11 to 20, and the sn-2 acyl chain is always 6 methylene units longer than the sn-1 acyl chain. In the initial heating DSC thermograms, two prominent endothermic transitions are detected for all the samples prepared from the various C(X):C(X + 6)PCs except C(12):C(18)PC. In contrast, a single exothermic transition is observed on cooling for all the samples except C(13):C(19)PC. The temperature difference between the two endothermic transitions increases linearly as the acyl chain length of C(X):C(X + 6)PC becomes progressively longer. Interestingly, the main phase transition occurs before the subtransition for C(11):C(17)PC dispersions. Our DSC data further demonstrate that the thermodynamic parameters (Tm, delta H, and delta S) associated with the main phase transition for fully hydrated C(13):C(19)PC and other identical MW phosphatidylcholines are inversely related to the corresponding values of the chain-length inequivalence (delta C/CL) for these lipids. This linear relationship can be employed to map the Tm values for aqueous dispersions prepared from a large number of mixed-chain phosphatidylcholines whose values of delta C/CL are within the range of 0.1-0.4.     

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)     

The ripple phase of phosphatidylcholines: effect of chain length and cholesterol

Saturated phosphatidylcholine (PC) bilayers display a rippled surface in the temperature region between the pre- and main transitions. Ripple repeat distance was measured from freeze-fracture electron micrographs. All of the lipids examined (C13PC to C16PC; C14C16PC and equimolar C14PC/C16PC) showed a bimodal distribution of ripple repeat distances with the two dominant values being in the ratio of 1:2. Within this series, chain length was a weak determinant of the actual repeat distance. The introduction of increasing concentrations of cholesterol eliminated the bimodal distribution and led to the appearance of a single distribution of increasing repeat distance and decreasing amplitude. Ripples disappeared above a cholesterol concentration of 15 mol%. These observations are discussed within the framework of a model which links the genesis of the ripples (vertical displacement of lipid molecules) to the trans-gauche isomerization known to occur at the pre-transition.     

The transfer of lipids from protein-free lipoprotein models to human fibroblasts in culture

Lipid microemulsions were prepared by sonication of mixtures of cholesteryl ester, triacylglycerol, phosphatidylcholine and cholesterol in aqueous dispersions and were purified by gel filtration. The resulting emulsion particles were characterized by differential scanning calorimetry, electron microscopy and analytical gel filtration and were shown to have the size and general organization of low-density lipoprotein. The lipid microemulsions were used as protein-free plasma lipoprotein models for studies of the receptor-independent transfer of lipids to human fibroblasts in culture. The transfer rate of [3H]cholesterol increased with the donor concentration and with the molar ratio between cholesterol and phosphatidylcholine in the donor particles. A maximal transfer value of 1 nmol per mg protein per h was obtained for cholesterol/phosphatidylcholine 1:1 particles. There was a profound temperature effect on the cholesterol transfer. The effect of altering the core lipid of the emulsion particles on the [3H]cholesterol transfer rate was small giving a somewhat higher rate with cholesteryl oleate and cholesteryl stearate than with cholesteryl linoleate. Addition of trioleoylglycerol to the cholesteryl ester core had no effect on the transfer rate. The transfer rate of palmitoyl[14C]oleoylphosphatidylcholine was found to be about 1/5 of that obtained for [3H]cholesterol. About 50% of the cell-associated [14C]cholesteryl oleate was found in the trypsin-releasable pool, while 25% was internalized by the cells at a rate of 0.06 nmol X mg-1 X h-1. Trioleoylglycerol was internalized at the same rate as the cholesteryl ester. Our data suggest that the lipoprotein lipid composition may play a role in the receptor-independent cellular uptake of cholesterol.     

Reconstitution of the leucine transport system of Lactococcus lactis into liposomes composed of membrane-spanning lipids from Sulfolobus acidocaldarius.

The effect of bipolar tetraether lipids, extracted from the thermophilic archaebacterium Sulfolobus acidocaldarius, on the branched-chain amino acid transport system of the mesophilic bacterium Lactococcus lactis was investigated. Liposomes were prepared from mixtures of monolayer lipids and the bilayer lipid phosphatidylcholine (PC), analyzed on their miscibility, and fused with membrane vesicles from L. lactis. Freeze-fracture electron microscopy demonstrates that the bipolar lipids in the hybrid membranes adopted a monomolecular organization at high S. acidocaldarius lipid content. Leucine transport activity (i.e., delta mu H(+)-driven and counterflow uptake) increased with the content of S. acidocaldarius lipids and was optimal at a one-to-one (w/w) ratio of PC to S. acidocaldarius lipids. Membrane fluidity decreased with increasing S. acidocaldarius lipid content. These data suggest that transport proteins can be functionally reconstituted into membranes composed of membrane-spanning lipids provided that membrane viscosity is restricted.     

Mixing behavior of identical molecular weight phosphatidylcholines with various chain-length differences in two-component lamellae.

It has recently been suggested that mixed-chain phosphatidylcholines with normalized chain length differences (deltaC/CL) in the range of 0.10-0.40 undergo spontaneous self-assembly in excess water at T less than Tm into the partially interdigitated bilayer and those with delta C/CL values in the range of 0.44-0.57 form, in excess water, mixed interdigitated bilayers at T less than Tm. The mixing behavior of binary mixtures of C(22):C(12)PC/C(17):C(17)PC, C(22):C(12)/C(15):C(19)PC, and C(15):C(19)PC/C(13):C(21)PC reported in this work is used to support this view. The values of delta C/CL for C(17):C(17)PC, C(15):C(19)PC, C(13):C(21)PC, and C(22):C(12)PC are 0.10, 0.15, 0.35, and 0.55, respectively. The binary mixture of C(15):C(19)PC/C(13):C(21)PC exhibits a lens-shaped phase diagram, indicating that these two identical molecular weight (MW) lipids with delta C/CL values less than 0.4 are completely miscible over the entire compositional range in both gel and liquid-crystalline phases. In contrast, the phase diagrams of C(22):C(12)PC/C(17):C(17)PC and C(22):C(12)PC/C(15):C(19)PC are eutectic, indicating immiscibility of the component lipids over a wide compositional range in the gel phase. This immiscibility of identical MW lipids in the bilayer plane can be attributed to the different packing properties of the component lipids in the bilayer at T less than Tm.     

Energy-minimized structures and packing states of a homologous series of mixed-chain phosphatidylcholines: a molecular mechanics study on the diglyceride moieties.

Phosphatidylcholines or C(X):C(Y)PC, quantitatively the most abundant lipids in animal cell membranes, are structurally composed of two parts: a headgroup and a diglyceride. The diglyceride moiety consists of the glycerol backbone and two acyl chains. It is the wide diversity of the acyl chains, or the large variations in X and Y in C(X):C(Y)PC, that makes the family of phosphatidylcholines an extremely complex mixture of different molecular species. Since most of the physical properties of phospholipids with the same headgroup depend strongly on the structures of the lipid acyl chains, the energy-minimized structure and steric energy of each diglyceride moiety of a series of 14 molecular species of phosphatidylcholines with molecular weights identical to that of dimyristoylphosphatidylcholine without the headgroup are determined in this communication by molecular mechanics (MM) calculations. Results of two types of trans-bilayer dimer for each of the 14 molecular species of phosphatidylcholines are also presented; specifically, the dimeric structures are constructed initially based on the partially interdigitated and mixed interdigitated packing motifs followed subsequently by the energy-minimized refinement with MM calculations. Finally, tetramers with various structures to model the lateral lipid-lipid interactions in a lipid bilayer are considered. Results of laborious MM calculations show that saturated diacyl C(X):C(Y)PC with delta C/CL values greater than 0.41 prefer topologically to assemble into tetramers of the mixed interdigitated motif, and those with delta C/CL values less than 0.41 prefer to assemble into tetramers with a repertoire of the partially interdigitated motif. Here, delta C/CL, a lipid asymmetry parameter, is defined as the normalized acyl chain length difference between the sn-1 and sn-2 acyl chains for a C(X):C(Y)PC molecule; an increase in delta C/CL value is an indication of increasing asymmetry between the two lipid acyl chains. These computational results are in complete accord with the calorimetric data presented previously from this laboratory (H-n. Lin, Z-q. Wang, and C. Huang. 1991. Biochim. Biophys. Acta. 1067:17-28).     

Liquid-crystalline phases of cholesterol/lipid bilayers as revealed by the fluorescence of trans-parinaric acid.

The presence of two liquid-crystalline phases, alpha and beta, in mixed bilayers of dimyristoylphosphatidylcholine/cholesterol was detected by the changes in the distribution of the fluorescence lifetimes of t-PnA, as analyzed by the Maximum Entropy Method. The formation of the liquid-ordered beta-phase, in the 30-40 degrees C temperature range as a function of cholesterol concentration (0-40 mol%), could be related quantitatively to the relative amplitude of a long lifetime component of the probe (10-14 ns). Based on this evidence, the phase behavior of mixtures of the unsaturated lipid palmitoyloleoylphosphatidylcholine and cholesterol was determined using the same technique, for cholesterol concentrations in the 0-50 mol% range, between 10 and 40 degrees C. It was found that two liquid-crystalline phases are also formed in this system, with physical properties reminiscent of the alpha- and beta-phases formed with saturated lipids. However, in this case it was determined that, for temperatures in the physiological range, the alpha- and beta-phases coexist up to 40 mol% cholesterol. This finding may be of significant biological relevance, because it supports the long held notion that cholesterol is responsible for the lipid packing heterogeneity of several natural membranes rich in unsaturated lipid components.     

Calcium-induced phase separation phenomena in multicomponent unsaturated lipid mixtures

The ability of calcium to induce phase separation in multicomponent lipid mixtures containing various unsaturated species of acidic and neutral phospholipids has been investigated by 31P NMR, 3H NMR, and small-angle X-ray diffraction techniques. It is shown that, in unsaturated (dioleoyl-) phosphatidylglycerol (PG)/phosphatidylethanolamine (PE) (1:1) and phosphatidic acid (PA)/phosphatidylcholine (PC) (1:1) mixtures, calcium is unable to induce lateral phase separation of the acidic and neutral lipids and that all the lipids adopt a hexagonal (HII) phase in the presence of calcium. In multicomponent mixtures containing one or more acidic species the presence of cholesterol either facilitates calcium-induced lamellar to hexagonal (HII) transitions for all the lipid components or, in systems already in a hexagonal (HII) phase, mitigates against calcium-induced lateral phase separations. Further, cholesterol is shown to exhibit no preferential interaction on the NMR time scale with either PC, PE, or phosphatidylserine (PS) when the lipids are in the liquid-crystal state. The ability of cholesterol to directly induce HII phase formation in PC/PE mixtures is also shown to be common to various other sterols including ergosterol, stigmasterol, coprostanol, epicoprostanol, and androstanol.     

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.