Asymmetric Phosphatidylcholine Research Articles

PS Membrane Asymmetry Influences the Folding and Insertion of a Transmembrane Helix

The plasma membrane (PM) has an asymmetric distribution of lipids between the inner and outer leaflets of its bilayer. A lipid of special interest in eukaryotic cells is the negatively charged phosphatidylserine (PS). In healthy cells, PS is actively sequestered to the inner leaflet of the PM but can redistribute to the outer leaflet when the cell is damaged or at the onset of apoptosis. However, membranes contain also proteins. Marginally hydrophobic membrane proteins contain acidic residues in their transmembrane sequence and can experience topological transitions after membrane association. The pH low insertion peptide (pHLIP), which undergoes a topological reorientation and inserts into the membrane at low pH, as its name implies, is a well-characterized model for studying these transitions. Although it is known that the inclusion of PS in symmetric vesicles affects the membrane insertion process of pHLIP by lowering the pH midpoint of insertion, it is unclear how PS asymmetry affects these topological transitions. Here, we studied pHLIP's topology using freely-floating asymmetric phosphatidylcholine (PC)/PS vesicles with PS enriched in the inner leaflet. We found that the protocol to create asymmetric vesicles had to be modified due to the inclusion of PS. We used Annexin V labeled with an Alexa 568 fluorophore as a new way of quantifying PS asymmetry. For pHLIP, membrane insertion was affected by the surface charge difference between bilayer leaflets because of the asymmetric distribution of charged lipids. We thus conclude that lipid asymmetry can have consequences for the behavior of membrane-associated proteins. A corollary is that model studies using symmetric bilayers to mimic the PM may fail to capture important details of protein-membrane interactions.

Membrane Lipid Asymmetry, a Key Property of the Mammalian Plasma Membrane, Alters the Insertion of the pHLIP Peptide

The plasma membrane has an asymmetric distribution of lipids between the inner and outer leaflets of the bilayer. Two types of phospholipid asymmetry can occur between the leaflets: head group asymmetry and acyl chain asymmetry. One lipid head group of interest is phosphatidylserine (PS), which carries a net negative charge. In healthy cells, PS is actively sequestered to the inner leaflet of the membrane but can redistribute to the outer leaflet in situations such as apoptosis and cancer. Not only do membranes contain lipids, they also contain proteins. Marginally hydrophobic membrane proteins can contain acidic residues in their transmembrane sequence and can have topological transitions after membrane association. What is unclear is how lipid asymmetry affects these topological transitions. Here, we propose to use the pH low insertion peptide (pHLIP) as a model to study topological transitions in relation to membrane head group asymmetry in free floating asymmetric phosphatidylcholine (PC)/PS vesicles. Based on environmental pH, pHLIP undergoes a topological reorientation and inserts into the membrane. The inclusion of PS in symmetric vesicles affects the insertion process by lowering the pH midpoint of insertio n. However, we do not know how PS asymmetry will affect insertion. We propose that having an asymmetric distribution of PS (more in the inner leaflet) will affect the insertion of pHLIP. Fluorescence spectroscopy data show that the pH midpoint of pHLIP insertion into asymmetr ic vesicles is higher compared to symmetric vesicles containing PS. Acrylamide quenching data show that the two tryptophans in pHLIP are more solvent exposed in the presence of asymmetry. We hypothesize that pHLIP insertion is affected by a change in the transmembrane potential induced by the asymmetric distribution of charged lipids between the leaflets.

Comparison of Ternary Bilayer Mixtures with Asymmetric or Symmetric Unsaturated Phosphatidylcholine Lipids by Coarse Grained Molecular Dynamics Simulations

We studied the phase behavior of various ternary bilayer mixtures composed of cholesterol, an unsaturated lipid, and a fully saturated lipid, by means of molecular dynamics simulations of the MARTINI coarse grain model. We aimed at comparing lateral organization and local properties of bilayers containing phosphatidylcholine (PC) lipids, either with two unsaturated tails (symmetric), or one unsaturated and one saturated tail (asymmetric), as the low-melting component of the mixture. The number of unsaturations per chain was systematically varied in both classes of unsaturated lipids, to account for its consequences in segregation. In the asymmetric unsaturated PCs, the saturated tail was kept identical to the hydrophobic chains of the fully saturated lipid component. Membranes with a symmetric or an asymmetric unsaturated lipid, with the same kind of unsaturated chain, show different phase behavior. Symmetric polyunsaturated PCs set the separation in two phases. Instead, the asymmetric polyunsaturated lipids induced nonideal mixing of components in single-phase bilayers. A significative drop of temperature, within the accessible temperature range, enhances the segregation in mixtures with the more unsaturated asymmetric PC, but still within a single phase. This different phase behavior between membranes with symmetric and asymmetric unsaturated PCs is also observed for lipids with the same total number of unsaturations. On the other hand, the degree of unsaturation per se enhances the segregation, by increasing the composition fluctuations in single-phase membranes with asymmetric PC lipids, and raising the line tension in the two-phase bilayer mixtures with symmetric polyunsaturated PCs. Dynamic clusters of unsaturated asymmetric lipids can be identified. The clusters show no correlation between leaflets, as observed for the phase domains in mixtures with the symmetric polyunsaturated PCs. Interestingly, we found that asymmetric PC lipids have a preferential orientation such that their saturated tails increase their density toward the periphery of the clusters, facing regions enriched in the fully saturated lipids and cholesterol. The degree of unsaturation increases the cluster size and also enhances the anisotropy of the orientation. The surface density of cholesterol follows a gradient that favors its interaction with the saturated tails. Such gradients in composition lead to gradients in order parameters, such as the conformational order and the area of the tails, which increases away from the unsaturated lipid clusters. We compared, in addition, differences in hydrophobic length mismatch between acyl chains of the low-melting and high-melting components, in mixtures containing either symmetric or asymmetric unsaturated lipids.

Pressure study on symmetric and asymmetric phospholipid bilayers: effect of vesicle size on Prodan fluorescence

The bilayer phase behavior of symmetric and asymmetric phosphatidylcholines (PCs), 1,2-diheptadecanoyl-PC (C17PC), 1-palmitoyl-2-stearoyl-PC (PSPC), and 1-stearoyl-2-palmitoyl-PC (SPPC), with different vesicle sizes were investigated by a high-pressure fluorescence method using the polarity-sensitive fluorescent probe Prodan. The second derivative of fluorescence spectra for all the PCs of small-sized vesicle showed four minima characteristic of four membrane states on the spectra irrespective of the acyl-chain symmetry, whereas those of large-sized vesicle had one more minimum originating from the most hydrophilic site at the membrane surface. These findings indicate that Prodan molecules can distribute into multiple sites in the bilayer and move around the head-group region depending on the vesicle size. The behavior of the spectra in the SPPC bilayer suggested that the interdigitated gel phase had a less polar "pocket" formed by a space between uneven terminal methyl ends of the sn-1 and sn-2 chains. It turned out that the curvature of vesicles affects the distribution of the Prodan molecules in all phases, more particularly in the interdigitated gel phase.

Empirical dependence of the main phase transition temperatures of highly asymmetric diacyl phosphatidylcholines with saturated acyl chains on the chain volumes

An empirical correlation equation is proposed relating the “gel—liquid crystal” main phase transition temperatures, Tm, of aqueous dispersions of highly asymmetric diacyl phosphatidyl-cholines with saturated acyl chains to the chain volumes. The equation permits the prediction of Tm values with an accuracy close to their experimental reproducibility. The sn-1 and sn-2 acyl chains affect the Tm values in different manner, whereas the excess chain fragments have an identical effect on the transition temperatures.

The Activity of the Amphipathic Peptide δ-Lysin Correlates with Phospholipid Acyl Chain Structure and Bilayer Elastic Properties

Release of lipid vesicle content induced by the amphipathic peptide δ-lysin was investigated as a function of lipid acyl chain length and degree of unsaturation for a series of phosphatidylcholines. Dye efflux and peptide binding were examined for three homologous lipid series: di-monounsaturated, di-polyunsaturated, and asymmetric phosphatidylcholines, with one saturated and one monounsaturated acyl chain. Except for the third series, peptide activity correlated with the first moment of the lateral pressure profile, which is a function of lipid acyl chain structure. In vesicles composed of asymmetric phosphatidylcholines, peptide binding and dye efflux are enhanced compared to symmetric, unsaturated lipids with similar pressure profiles. We attribute this to the entropically more favorable interaction of δ-lysin with partially saturated phospholipids. We find that lipid acyl chain structure has a major impact on the activity of δ-lysin and is likely to be an important factor contributing to the target specificity of amphipathic peptides.

Positional specificity of lysosomal phospholipase A2

Lysosomal phospholipase A(2) (Lpla2) is highly expressed in alveolar macrophages and may mediate the phospholipid metabolism of surfactant. Studies on the properties of this phospholipase are consistent with the presence of both phospholipase A(1) and phospholipase A(2) activities. These activities were studied through the production of O-acyl compounds, produced by the transacylase activity of Lpla2. Liposomes containing POPC and N-acetylsphingosine (NAS) were incubated with the soluble fraction obtained from MDCK cells stably transfected with the mouse Lpla2 gene. Two 1-O-acyl-NASs, 1-O-palmitoyl-NAS and 1-O-oleoyl-NAS, were produced by Lpla2. The formation rate of 1-O-oleoyl-NAS was 2.5-fold that of 1-O-palmitoyl-NAS. When 1-oleoyl-2-palmitoyl-sn-glycero-3-phosphocholine (OPPC) was used, the formation rate of 1-O-oleoyl-NAS was 5-fold higher than that of 1-O-palmitoyl-NAS. Thus, Lpla2 can act on acyl groups at both sn-1 and sn-2 positions of POPC and OPPC. When 1-palmitoyl-2-unsaturated acyl-sn-glycero-3-phosphocholines were used as acyl donors, the transacylation of the acyl group from the sn-2 position to NAS was preferred to that of the palmitoyl group from the sn-1 position. An exception was observed for 1-palmitoyl-2-arachidonoyl-sn-glycero-3-phosphocholine (PAPC), for which the formation rate of 1-O-palmitoyl-NAS from PAPC was 4-fold greater than that of 1-O-arachidonoyl-NAS. Thus, Lpla2 has broad positional specificity for the sn-1 and sn-2 acyl groups in phosphatidylcholine and phosphatidylethanolamine.

Barotropic Phase Transitions of 1-Palmitoyl-2-stearoylphosphatidylcholine Bilayer Membrane

Abstract The barotropic phase transitions of an asymmetric phosphatidylcholine, 1-palmitoyl-2-stearoylphosphatidylcholine (PSPC), bilayer membrane were observed by the methods of high-pressure light transmittance and differential scanning calorimetry. The temperature–pressure phase diagram and thermodynamic quantities of the phase transitions were compared with those of three kinds of symmetric phosphatidylcholines. The different transition properties of PSPC bilayer from those of symmetric phosphatidylcholines may be attributable to the enhanced cohesive interaction between acyl chains in the gel state of the bilayer membrane.

Alkyl Chain Ordering of Asymmetric Phosphatidylcholines Adsorbed at a Liquid−Liquid Interface

Vibrational spectroscopic investigations of hydrocarbon chain ordering in phosphatidylcholines (PCs) adsorbed from aqueous solution to a carbon tetrachloride−water interface presented here examine on a molecular level the organization pertinent to the surface characteristics displayed by these films. In a series of saturated symmetric and asymmetric chain PCs, both symmetric PCs with 16 or fewer carbons per acyl chain and highly asymmetric PCs produced relatively disordered films at the liquid−liquid interface. The longest chain PCs studied, 1,2-distearoyl-sn-glycero-3-PC (C18/C18), 1-stearoyl-2-palmitoyl-sn-glycero-3-PC (C18/C16) and 1-palmitoyl-2-stearoyl-sn-glycero-3-PC (C16/C18), formed well-ordered layers at room temperature. The results can be explained in terms of enhanced chain−chain interactions among the longer, nearly symmetric hydrocarbon chains. Properties of the neat liquid−liquid interface that may influence the formation of these well-ordered two-dimensional phases are discussed.

Effects of alcohols on the phase transition temperatures of mixed-chain phosphatidylcholines

The biphasic effect of ethanol on the main phase transition temperature (Tm) of identical-chain phosphatidyl-cholines (PCs) in excess H2O is now well known. This biphasic effect can be attributed to the transformation of the lipid bilayer, induced by high concentrations of ethanol, from the partially interdigitated L beta, phase to the fully interdigitated L beta I phase at T < Tm. The basic packing unit of the L beta I phase has been identified recently as a binary mixture of PC/ethanol at the molar ratio of 1:2. The ethanol effect on mixed-chain PCs, however, is not known. We have thus in this study investigated the alcohol effects on the Tm of mixed-chain PCs with different delta C values, where delta C is the effective acyl chain length difference between the sn-1 and sn-2 acyl chains. Initially, molecular mechanics (MM) simulations are employed to calculate the steric energies associated with a homologous series of mixed-chain PCs packed in the partially and the fully interdigitated L beta I motifs. Based on the energetics, the preference of each mixed-chain PC for packing between these two different motifs can be estimated. Guided by MM results, high-resolution differential scanning calorimetry is subsequently employed to determine the Tm values for aqueous lipid dispersions prepared individually from a series of mixed-chain PCs (delta C = 0.5-6.5 C-C bond lengths) in the presence of various concentrations of ethanol. Results indicate that aqueous dispersions prepared from mixed-chain PCs with a delta C value of less than 4 exhibit a biphasic profile in the plot of Tm versus ethanol concentration. In contrast, highly asymmetric PCs (delta C > 4) do not exhibit such biphasic behavior. In the presence of a longer chain n-alcohol, however, aqueous dispersions of highly asymmetric C(12):C(20)PC (delta C = 6.5) do show such biphasic behavior against ethanol. Our results suggest that the delta C region in a highly asymmetric PC packed in the L beta I phase is most likely the binding site for n-alcohol.

ATP-dependent phosphatidylcholine translocation in rat liver canalicular plasma membrane vesicles

Phosphatidylcholine (PC) translocation was studied in rat liver canalicular plasma membrane vesicles using a fluorescent PC analogue that permitted the quantitation of asymmetric PC distribution in the outer and inner leaflet of the vesicles. PC translocation to the outer leaflet of the canalicular membrane was stimulated by ATP and an ATP-regenerating system in a time and temperature-dependent manner resulting in 200 pmol PC translocated/mg protein per 30 min. A non-hydrolyzable ATP analogue did not support translocation. Translocating activity was observed with PC but not with phosphatidylethanolamine and was specific for inside-out oriented canalicular membrane vesicles. Addition of taurocholate (10 microM), a micelle-forming bile acid, enhanced ATP-dependent PC translocation 1.5 +/- 0.1-fold, whereas addition of taurodehydrocholate (10 microM), a non-micelle-forming bile acid, did not. These results indicate the presence of an ATP-dependent transporter that "flips" phosphatidylcholine from the inner to the outer leaflet of the rat bile canalicular plasma membrane from where it can become associated with bile acids in the canalicular lumen, thereby enhancing ATP-dependent flipping activity. Several lines of evidence suggest that the transporter is Mdr2 P-glycoprotein.

Interdigitation does not affect translational diffusion of lipids in liquid crystalline bilayers

Asymmetric phosphatidylcholine molecules with one acyl chain twice as long as the other, below their phase transition temperature, from a mixed interdigitated phase in which the longer acyl chain spans the entire bilayer. Experimental evidence in the literature suggests that, above their phase transition temperature, these molecules may still exhibit partial interdigitation, with the longer acyl chain extending partially into the opposite leaflet, and are packed more tightly than equivalent symmetric phosphatidylcholines. Using the fluorescence recovery after photobleaching technique, we have investigated the translational diffusion in multilayers of a liquid crystalline phase, asymmetric phosphatidylcholine, 1-stearoyl-2-capryl-phosphatidylcholine (C18C10PC). We used as a fluorescent probe either a phospholipid analog of the same acyl chain composition, NBD-C18C10PE, or the symmetric equivalent of the same molecular weight, N-(7-nitrobenzoxa-2,3-diazol-4-yl)-dimyristoyl-phosphatidyle thanolamine (NBD-DMPE). Translational diffusion coefficients were also determined by using both probes in multilayers of dimyristoyl-phosphatidylcholine (DMPC) and in the eutectic mixture DMPC/C18C10PC (40/60 mol). We found that in a given host lipid, NBD-C18C10PE and NBD-DMPE diffuse at the same rate, which suggests that their bilayer free area is almost identical. This result can be explained by considering that in the liquid crystalline state, the increase in molecular packing is compensated by an increase in acyl chain dynamics. This view, which is supported by literature data, clearly suggests that the acyl chain interdigitation occurring in the liquid crystalline phase is highly dynamic.

Phospholipids with a short acyl chain modulate phospholipase and acyltransferase activities

1-Acyl lysophosphatidylcholine prepared from egg yolk has been chemically reacylated to form decanoyl, dodecanoyl, myristoyl and palmitoyl derivatives of phosphatidylcholine. The liposomes formed by these semi-synthetic phospholipids have been characterized by calorimetry, X-ray diffraction and fluorescence probe methods. Asymmetric phosphatidylcholines tend to promote formation of excimers of a codispersed fluorescent phospholipid (1-palmitoyl- sn-2-(1-pyrenedecanoyl)- l-α-phosphatidic acid) (2 mol%). Excimer formation is correlated with the rate of hydrolysis of the fluorescent anionic phospholipid by Crotalus venom phospholipase A 2. Codispersion with the semi-synthetic phosphatidylcholine of cholesterol or unsaturated fluid lecithin modulated both excimer formation and the susceptibility of the fluorescent probe to hydrolysis by venom phospholipase A 2 at 22°C. Similar results were btained with hydrolysis of a radiolabelled substrate, 1-palmitoyl- sn-2-[1 14C linoleoylphosphatidylethanolamine, codispersed with the semi-synthetic phosphatidylcholine. Enrichment of rat hepatocyte plasma membranes with semi-synthetic asymmetric phosphatidylcholines was mediated by incubation of membranes with phospholipid dispersions in the presence of a phospholipid exchange protein. Enrichment of the membranes with semi-synthetic phosphatidylcholines of between 30 and 60% of the membrane phosphatidylcholine was achieved. The resulting alteration of the biomembrane is associated with a decreased activity of endogenous membrane phospholipase A 2 acting on extramembranous radiolabelled substrate vesicles. By contrast, the activity of acylCoAaysophospholipid acyltransferase is increased in membranes enriched with highly asymmetric phospholipids.

Bilayer packing characteristics of mixed chain phospholipid derivatives: Raman spectroscopic and differential scanning calorimetric studies of 1-stearoyl-2-capryl- sn-glycero-3-phosphocholine (C(18) : C(10)PC) and 1-stearoyl-2-capryl- sn-glycero-3-phospho- N-trimethylpropanolamine (C(18) : C(10)TMPC)

Raman spectroscopy and high-sensitivity differential scanning calorimetry (DSC) were used to compare the effects of headgroup conformation on the acyl chain packing arrangements in two highly asymmetric phosphatidylcholine (PC) analogues 1-stearoyl-2-capryl- sn-glycero-3-phosphocholine (C(18) : C(10)PC) and a polar headgroup derivative of C(18): C(10)PC, 1-stearoyl-2-capryl- sn-glycero-3-phospho- N-trimethylpropanolamine (C(18):C(10)TMPC), which contains an additional methylene group within the choline moiety; namely, PO(CH 2) 3N(CH 3) 3. The C(18): C(10)TMPC headgroup exhibits an extended trans conformation which is independent of bilayer phase. A comparison of gel phase spectral order parameters of the two lipid species indicates a mixed interdigitated state characteristic of three chains per headgroup for C(18):C(10)TMPC. A more intermolecularly ordered liquid crystalline phase is observed, however, for the C(18):C(10)TMPC bilayers. The phase transition cooperative unit size estimated for the C(18):C(10)PC bilayers (≈ 140 molecules per unit) is about 7-fold greater than that for the C(18):C(10)TMPC dispersions (≈ 20 molecules per unit). We suggest that the extended headgroup for C(18):C(10)TMPC induces a slight tilt in the gel phase packing arrangements for the acyl chains, which may persist in the partially interdigitated liquid crystalline phase bilayer. Macroscopically, tighter packed multilamellar dispersions of C(18):C(10)TMPC occur for systems prepared first in the presence of a higher ionic strength medium. The stacked bilayers may then be transferred to a lower ionic strength environment without loss of their more closely packed adjacent lamellae.

Thermodynamic, thermomechanical, and structural properties of a hydrated asymmetric phosphatidylcholine

1-Behenyl-2-lauryl-sn-glycero-3-phosphocholine (22/12 PC) belongs to a unique group of phospholipids in which the molecule has one acyl chain almost twice as long as the other. The temperature-composition phase diagram for this lipid in the range of 25-65 degrees C, and 0 to 84.3% (w/w) water has been constructed by using the isoplethal method in the heating direction and x-ray diffraction for phase identification and structure characterization. At water contents between 10.3 and 34% (w/w) and at temperatures below 43 degrees C, a single mixed interdigitated lamellar gel phase (Lm beta, [symbol: see text]) of the type described by Hui et al. (1984. Biochemistry. 23:5570-5577) and McIntosh et al. (1984. Biochemistry. 23:4038-4044) was found. A second phase consisting of bulk aqueous solution coexists with the Lm beta phase at hydration levels above 34% (w/w) water in the temperature range between 25 and 43 degrees C. Above 43 degrees C, a partially interdigitated lamellar liquid crystalline (Lp alpha) phase ([symbol: see text]) is seen in the water concentration range extending from 0 to 84.3% (w/w). The pure Lp alpha phase is found below 43% (w/w) water, while coexistence of the Lp alpha phase and the bulk aqueous solution is observed above this water concentration which marks the hydration boundary. Interestingly, the latter boundary for both Lm beta and Lp alpha phases is nearly vertical in the temperature range studied. Furthermore, the lamellar chain-melting transition temperature appears to be relatively insensitive to hydration in the range 0-85% (w/w) water. We have confirmed the identify of the Lm beta phase by constructing a 5.7-A resolution electron density profile on oriented samples by the swelling method. Temperature-induced chain melting effects an increase in lipid bilayer thickness suggesting that the Lp alpha phase has chains packed in the partially as opposed to the mixed interdigitated configuration. Unlike the symmetric phosphatidylcholines a ripple (P beta') phase was not found as an intermediate between the low and high temperature lamellar phases of 22/12 PC. The specific volume of 22/12 PC is 940 (+/- 1) microliter/g and 946 (+/- 1) microliter/g in the hydrated lamellar gel state at 28 (+/- 2) and 40 (+/- 2) degrees C, respectively, from neutral buoyancy experiments. Based on measurements of the temperature dependence of the various lattice parameters of the different phases encountered in this study the corresponding lattice thermal expansion coefficients have been measured. These are discussed and their dependence on lipid hydration is reported.

Thermotropic and mixing behavior of mixed-chain phosphatidylcholines with molecular weights identical with L-.alpha.-dipalmitoylphosphatidylcholine

The thermotropic phase behavior of 10 mixed-chain phosphatidylcholines, in excess water, has been examined and compared with that of identical-chain C(16):C(16)PC by using high-resolution differential scanning calorimetry (DSC). The molecular weights (MW) of these 11 molecular species are the same, but their delta C/CL values, or the normalized chain length differences, vary considerably, ranging from 0.035 to 0.540. The thermodynamic parameters (Tm, delta H, and delta S) associated with the main phase transitions for these lipid dispersions exhibit biphasic V-shaped curves, when plotted against delta C/CL. Similar characteristic curves have been reported previously for aqueous dispersions of mixed-chain phosphatidylcholines with MW identical with that of C(17):C(17)PC [Lin et al. (1990) Biochemistry 29, 7063-7072]. The initial decrease in Tm (delta H or delta S) with increasing values of delta C/CL is attributed to the progressive increase in the magnitude of the chain-terminal perturbations on the conformational statistics of the adjacent hydrocarbon chains and hence the lateral chain-chain interactions of these mixed-chain phosphatidylcholines in the gel-state bilayer. At delta C/CL approximately equal to 0.42, the chain-end perturbation is presumably at its maximum; beyond this point, the highly asymmetric phosphatidylcholines are proposed to pack, at T less than Tm, into the mixed interdigitated bilayer. In this new packing mode, the methyl ends of the longer acyl chains are relocated at the interfaces between the hydrocarbon core of the bilayer and the aqueous medium. This disposition of the bulky chain ends releases a certain degree of chain-chain packing disorders, leading to an increase in Tm (delta H or delta S) with increasing delta C/CL.(ABSTRACT TRUNCATED AT 250 WORDS)

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.

Structural aspects of pressure effects on infrared spectra of mixed-chain phosphatidylcholine assemblies in deuterium oxide

The barotropic behavior of D2O dispersions of 1-stearoyl-2-caproyl-sn-glycero-3-phosphocholine, C(18):C(10)PC, a highly asymmetric phospholipid in which the length of the fully extended acyl chain at the sn-1 position of the glycerol backbone is twice as long as that at the sn-2 position, has been investigated by high-pressure Fourier transform infrared spectroscopy. This asymmetric phosphatidylcholine bilayer at room temperature displays a pressure-induced phase transition corresponding to the liquid-crystalline----gel phase transition at 1.4 kbar. A conformational ordering of the lipid acyl chains is observed to take place abruptly at the transition pressure of 1.4 kbar. However, the lamellar lipid molecules and their acyl chains remain to be orientationally disordered in the gel phase until the applied pressure reaches 5.5 kbar. In the gel phase of fully hydrated C(18):C(10)PC, the asymmetric lipid molecules assemble into mixed interdigitated bilayers with perpendicular orientation of the zigzag planes among neighboring acyl chains. The role of excess water played in the interchain structure and the behavior of excess water and bound water under high pressure are also discussed.

Binary mixtures of asymmetric phosphatidylcholines with one acyl chain twice as long as the other.

High-resolution differential scanning calorimetry and 31P NMR spectroscopy have been used to study aqueous phosphatidylcholine (PC) dispersions prepared from colyophilized mixtures of C(10):C(22)PC/C(22):C(12)PC of various molar ratios. These two lipid species are highly asymmetric but have a common structural feature; namely, one acyl chain in the fully extended conformation is about twice as long as the other. Our experimental results support two conclusions: (1) These two component lipids are miscible in all proportions in both gel and liquid-crystalline states. This type of system behaves as a nearly ideal mixture. Its calorimetric parameters are those expected on the basis of the mole fraction weighted average of the corresponding parameters for the pure components. (2) The component lipids appear to self-assemble, at T less than Tm, into a mixed interdigitated bilayer in excess water. In a mixed interdigitated bilayer, the short acyl chain of one asymmetric phosphatidylcholine on one side of the bilayer leaflet is apposed with the short acyl chain of another lipid molecule on the other side of the bilayer leaflet, while the longer acyl chain from each of the two leaflets crosses the entire hydrocarbon width of the bilayer. The fundamental packing unit, as well as the dynamic unit describing the axial rotator motion about the bilayer normal for this mixed interdigitated bilayer, is thus a dimer, whereas the packing unit assigned for the noninterdigitated bilayer such as C(16):C(16)PC lamellae is a monomer.

Scanning calorimetric study of fully hydrated asymmetric phosphatidylcholines with one acyl chain twice as long as the other

The asymmetric C(18):C(10)PC molecules are known by X-ray diffraction to self-assemble, in excess water, into a lamellar structure known as the mixed interdigitated bilayer at T less than Tm. In this structure, the long C(18)-acyl chain is interdigitated fully across the entire hydrocarbon width of the bilayer, while the shorter C(10)-acyl chain, which is about half as long as the C(18)-acyl chain, packs end to end with a C(10)-acyl chain of another lipid molecule in the opposing bilayer leaflet. We have synthesized the following asymmetric phosphatidylcholines (PC's): C(16):C(9)PC, C(16):C(10)PC, C(18):C(10)PC, C(18):C(11)PC, C(20):C(11)PC, C(20):C(12)PC, C(22):C(12)PC, C(22):C(13)PC, C(8):C(18)PC, and C(10):C(22)PC. These 10 asymmetric phosphatidylcholines have a common characteristic; i.e., the length of the longer extended acyl chain is about twice as long as that of the shorter acyl chain. On the basis of the known lamellar structure of C(18):C(10)PC, we anticipate that these asymmetric phosphatidylcholines will also form mixed interdigitated bilayers. We have employed high-resolution differential scanning calorimetry (DSC) to investigate the thermotropic behavior of liposomes prepared from these asymmetric phosphatidylcholines. If our anticipation is correct, one would find that the thermodynamic data (Tm, delta H, or delta S) associated with the main thermal phase transitions of these asymmetric phosphatidylcholine dispersions will fit into a continuous curve as they are plotted as a function of the hydrocarbon width of the putative mixed interdigitated bilayer. Experimental data presented in this paper indeed bear this out. For comparison, a DSC study of multilamellar dispersions prepared from a series of saturated symmetric phosphatidylcholines has also been carried out.(ABSTRACT TRUNCATED AT 250 WORDS)