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).     

The influence of acyl chain-length asymmetry on the phase transition parameters of phosphatidylcholine dispersions

The influence of acyl chain-length asymmetry on the thermodynamic parameters (Tm, delta H, and delta S) associated with the reversible main phase transition of aqueous dispersions prepared from saturated diacyl phosphatidylcholines was studied by high-resolution differential scanning calorimetry. Two series of saturated diacyl phosphatidylcholines, grouped according to their molecular weights of 678 and 706, with a total number of 25 molecular species were examined. The normalized acyl chain-length difference between the sn-1 and sn-2 acyl chains for a given phospholipid molecule in the gel-state bilayer is expressed quantitatively by the structural parameter delta C/CL, and the values of delta C/CL for the two series of lipids under study vary considerably from 0.04 to 0.67. When the value of delta C/CL is within the range of 0.09-0.40, it was shown that the thermodynamic parameters are, to a first approximation, a linear function of delta C/CL with a negative slope. In addition, the experimental Tm values and the predicted Tm values put forward by Huang (Biochemistry (1991) 30, 26-30) are in very good agreement. Beyond the point of delta C/CL = 0.41, the influence of acyl chain-length asymmetry on the thermodynamic parameters deviates significantly from a linear function. In fact, within the range of delta C/CL values of 0.42-0.67, the thermodynamic parameters in the Tm (or delta H) vs. delta C/CL plot were shown to be bell-shaped with the maximal Tm (or delta H) at delta C/CL = 0.57. These results are discussed in terms of changes in the acyl chain packing modes of various phosphatidylcholine molecules within the gel-state bilayer in excess water.     

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.     

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.     

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.     

Polymorphic phase behavior of lysophosphatidylethanolamine dispersions. A thermodynamic and spectroscopic characterization.

We have investigated the phase behavior of aqueous dispersions of a series of synthetic lysophosphatidylethanolamines as a function of the acyl chain length. Lysophosphatidylethanolamines exhibit phase polymorphism encompassing a well-ordered crystalline phase which may arise either from a metastable interdigitated lamellar gel phase or a metastable micellar phase. The time course of interconversion between these various phases have been outlined by observing the low temperature incubation time dependence of the calorimetric thermograms. We have determined differences in structure of these phases by Raman spectroscopy and 31P nuclear magnetic resonance spectroscopy. It appears that a principal contribution to this polymorphic phase behavior lies in the nature of headgroup hydration and headgroup-headgroup interactions.     

Thermotropic and mixing behavior of mixed-chain phosphatidylcholines with molecular weights identical with that of 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)     

Empirical estimation of the gel to liquid-crystalline phase transition temperatures for fully hydrated saturated phosphatidylcholines

Phospholipids are a major component of biological membranes. In excess water, phospholipids may self-assemble into fully hydrated lamellae which, upon heating, may undergo the gel to liquid-crystalline phase transition at the characteristic temperature, Tm. Our present knowledge about the Tm values for various phospholipids is far from complete, although it is necessary to know the Tm value for preparing liposomes. In this study, we have derived empirically a general expression of Tm = 154.2 + 2.0(delta C) - 142.8(delta C/CL) - 1512.5(1/CL) in which two apparent structural parameters, delta C and CL, of a phosphatidylcholine molecule and their ratio, delta C/CL, are applied to estimate the Tm value of the phosphatidylcholine bilayer in excess water. The parameter delta C is the effective chain-length difference, in C-C bond lengths, between the two acyl chains for the phosphatidylcholine molecule in the gel-state bilayer, and CL is the effective length of the longer of the two acyl chains, also in C-C bond lengths. A figure containing 163 calculated Tm values is presented, and this information will be useful as a guide for designing experiments.     

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.     

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.     

Mixing behavior of symmetric chain length and mixed chain length phosphatidylcholines in two-component multilamellar bilayers: evidence for gel and liquid-crystalline phase immiscibility

The mixing behavior of symmetric chain length and mixed chain length phosphatidylcholines in two-component multilamellar bilayers has been investigated by high-sensitivity differential scanning calorimetry. Phase diagrams have been constructed for two-component bilayers composed of C(18)C(18)PC and either C(18)C(16)PC, C(18)C(14)PC, C(18)C(12)PC, or C(18)C(10)PC. It is found that C(18)C(18)PC-C(18)C(16)PC and C(18)C(18)PC-C(18)C(14)PC mixed bilayers exhibit complete miscibility of the components in both the gel and liquid-crystalline phases. Whereas this mixing is observed to be nearly ideal for the C(18)C(18)PC-C(18)C(16)PC binary system, the intermixing of the lipids is highly nonideal in the gel phase of the C(18)C(18)PC-C(18)C(14)PC binary mixture. The C(18)C(18)PC-C(18)C(12)PC and C(18)C(18)PC-C(18)C(10)PC mixed bilayers are characterized by partial immiscibility of the phosphatidylcholine components in the bilayer gel phase. Over a large compositional range, these bilayers appear to consist of phase-separated regions of interdigitated and noninterdigitated gel phases. In addition, the C(18)C(18)PC-C(18)C(10)PC two-component bilayer displays a limited region of liquid-liquid immiscibility in the liquid-crystalline bilayer phase. The phase separation of the mixed chain length phosphatidylcholines revealed in these mixed bilayers may represent a three-dimensional phase separation of the lipid components where the phosphatidylcholines are both laterally separated within the plane of the bilayer and conformationally coupled across the bilayer. Such phase-separated domains could have profound effects on membrane structure and function if they were to occur in biological membranes.     

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.     

On the modulation of a high-enthalpy pretransition in binary mixtures of DMPC and DMPG by polar headgroup interaction.

Employing high-sensitivity differential scanning calorimetry (DSC), we discovered a pretransition in binary mixtures of dimyristoyl phosphatidylcholine and dimyristoyl phosphatidylglycerol, the main feature of which is its extraordinarily high transition enthalpy of 6.3 Kcal/mol, nearly an order of magnitude higher than those values previously found for such transitions. Using DSC, deuterium nuclear magnetic resonance, and electron microscopy, it is shown that the energetic origin of this type of pretransition is caused by interactions between the phospholipids in their headgroup region. The most likely interaction involves the formation of a hydrogen bond between the headgroups of the two phospholipid species in the gel (L beta') phase which is disrupted at the transition to the "ripple" (P beta') phase. The finding that this large pretransition is unique for mixtures of phosphocholine and phosphoglycerol with myristoyl chains indicates a dependence of the headgroup long range order of such mixtures in the gel phase on the acyl chain length.     

Effect of physical constraints on the mechanisms of membrane fusion: bolaform lipid vesicles as model systems.

Monolayers of an enantiomeric and a racemic triple-chain phosphatidylcholine (PC) at the air/water interface are studied by film balance measurements and x-ray diffraction. Although the area per three tails exceeds that per head, we observe tail ordering dependent on headgroup chirality and chain tilt. This indicates lateral headgroup interactions. The influence of the chiral carbon is suppressed at higher lateral pressures, and a centered-rectangular unit cell with tails tilted into the nearest neighbor (NN) direction is observed for both the enantiomer and the racemate. The distortion of the lattice changes at medium pressures from NN to NNN (next-nearest neighbor direction) with decreasing temperature. The phase behavior of the racemate at 15 degrees C is compared with that of a triple-chain PC with a branched chain of reduced length. Whereas the PC with the longer branched chain exhibits only a NN tilted phase at all pressures, the PC with the shorter branched chain has a rich polymorphism (NNN-NN-upright hexagonal packing) under increased lateral pressure.     

Preferential interaction of alpha-tocopherol with phosphatidylcholines in mixed aqueous dispersions of phosphatidylcholine and phosphatidylethanolamine.

The effect of alpha-tocopherol on the structure and phase behaviour of mixed aqueous dispersions of phosphatidylcholine and phosphatidylethanolamine has been examined by synchrotron X-ray diffraction and freeze-fracture electron microscopy. Equimolar mixtures of fully saturated derivatives of phospholipids that show gel phase immiscibility were examined including dimyristoylglycerophosphocholine/dipalmitoylglycerophosphoethanolamin e and distearoylglycerophosphocholine/dilauroylglycerophosphoethanolamine++ +. Analysis of the X-ray scattering intensities recorded at wide angles during heating scans of mixed aqueous dispersions containing 2.5 or 5 mol% alpha-tocopherol showed that alpha-tocopherol disordered the acyl chain packing of the phosphatidylcholine to a greater extent than the phosphatidylethanolamine component of the mixture. This suggested that alpha-tocopherol preferentially interacts with phosphatidylcholine rather than phosphatidylethanolamine, irrespective of whether this was the high or low melting point component of the mixture. The presence of 20 mol% alpha-tocopherol in either phospholipid mixture prevented gel phase separation during the prior cooling scan and no conclusions could be drawn as to the distribution of alpha-tocopherol in these mixtures.     

Electron spin resonance characterization of liquid ordered phase of detergent-resistant membranes from RBL-2H3 cells.

The dynamic structure of detergent-resistant membranes (DRMs) isolated from RBL-2H3 cells was characterized using two different acyl chain spin-labeled phospholipids (5PC and 16PC), a headgroup labeled sphingomyelin (SM) analog (SD-Tempo) and a spin-labeled cholestane (CSL). It was shown, by comparison to dispersions of SM, dipalmitoylphosphatidylcholine (DPPC), and DPPC/cholesterol of molar ratio 1, that DRM contains a substantial amount of liquid ordered phase: 1) The rotational diffusion rates (R( perpendicular)) of 16PC in DRM between -5 degrees C and 45 degrees C are nearly the same as those in molar ratio DPPC/Chol = 1 dispersions, and they are substantially greater than R( perpendicular) in pure DPPC dispersions in the gel phase studied above 20 degrees C; 2) The order parameters (S) of 16PC in DRM at temperatures above 4 degrees C are comparable to those in DPPC/Chol = 1 dispersions, but are greater than those in DPPC dispersions in both the gel and liquid crystalline phases. 3) Similarly, R( perpendicular) for 5PC and CSL in DRM is greater than in pure SM dispersions in the gel phase, and S for these labels in DRM is greater than in the SM dispersions in both the gel and liquid crystalline phases. 4) R( perpendicular) of SD-Tempo in DRM is greater than in dispersions of SM in both gel and liquid phases, consistent with the liquid-like mobility in the acyl chain region in DRM. However, S of SD-Tempo in DRM is substantially less than that of this spin label in SM in gel and liquid crystalline phases (in absolute values), indicating that the headgroup region in DRMs is less ordered than in pure SM. These results support the hypothesis that plasma membranes contain DRM domains with a liquid ordered phase that may coexist with a liquid crystalline phase. There also appears to be a coexisting region in DRMs in which the chain labels 16PC and 5PC are found to cluster. We suggest that other biological membranes containing high concentrations of cholesterol also contain a liquid ordered phase.     

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.     

Magic-angle spinning NMR studies of molecular organization in multibilayers formed by 1-octadecanoyl-2-decanoyl-sn-glycero-3-phosphocholine.

Magic-angle spinning 1H and 13C nuclear magnetic resonance (NMR) have been employed to study 50%-by-weight aqueous dispersions of 1-octadecanoyl-2-decanoyl-sn-glycero-3-phosphocholine (C[18]:C[10]PC) and 1-octadecanoyl-2-d19-decanoyl-PC (C[18]:C[10]PC-d19), mixed-chain phospholipids which can form interdigitated multibilayers. The 1H NMR linewidth for methyl protons of the choline headgroup has been used to monitor the liquid crystalline-to-gel (LC-to-G) phase transition and confirm variations between freezing and melting temperatures. Both 1H and 13C spin-lattice relaxation times indicate unusual restrictions on segmental reorientation at megahertz frequencies for C(18):C(10)PC as compared with symmetric-chain species in the LC state; nevertheless each chemical moiety of the mixed-chain phospholipid exhibits motional behavior that may be classified as liquidlike. Two-dimensional nuclear Overhauser spectroscopy (NOESY) on C(18):C(10)PC and C(18):C(10)PC-d19 reveals cross-peaks between the omega-methyl protons of the C18 chain and the N-methyl protons of the phosphocholine headgroup, and several experimental and theoretical considerations argue against an interpretation based on spin diffusion. Using NMR relaxation times and NOESY connectivities along with a computational formalism for four-spin systems (Keepers, J. W., and T. L. James. 1984. J. Magn. Reson. 57:404-426), an estimate of 3.5 A is obtained for the average distance between the omega-methyl protons of the C18 chain and the N-methyl protons of the phosphocholine headgroup. This finding is consistent with a degree of interdigitation similar to that proposed for organized assemblies of gel-state phosphatidylcholine molecules with widely disparate acyl-chain lengths (Hui, S. W., and C.-H. Huang. 1986. Biochemistry. 25:1330-1335); however, acyl-chain bendback or other intermolecular interactions may also contribute to the NOESY results. For multibilayers of C(18):C(10)PC in the gel phase, 13C chemical-shift measurements indicate that trans conformers predominate along both acyl chains. 13C Spin-lattice relaxation times confirm the unusual motional restrictions noted in the LC state; nevertheless, 13C and 1H rotating-frame relaxation times indicate that the interdigitated arrangement enhances chain or bilayer motions which occur at mid-kilohertz frequencies.     

Determination of membrane cholesterol partition coefficient using a lipid vesicle-cyclodextrin binary system: effect of phospholipid acyl chain unsaturation and headgroup composition

Lateral domain or raft formation in biological membranes is often discussed in terms of cholesterol-lipid interactions. Preferential interactions of cholesterol with lipids, varying in headgroup and acyl chain unsaturation, were studied by measuring the partition coefficient for cholesterol in unilamellar vesicles. A novel vesicle-cyclodextrin system was used, which precludes the possibility of cross-contamination between donor-acceptor vesicles or the need to modify one of the vesicle populations. Variation in phospholipid headgroup resulted in cholesterol partitioning in the order of sphingomyelin (SM) > phosphatidylserine > phosphatidylcholine (PC) > phosphatidylenthanolamine (PE), spanning a range of partition DeltaG of -1181 cal/mol to +683 cal/mol for SM and PE, respectively. Among the acyl chains examined, the order of cholesterol partitioning was 18:0(stearic acid),18:1n-9(oleic acid) PC > di18:1n-9PC > di18:1n-12(petroselenic acid) PC > di18:2n-6(linoleic acid) PC > 16:0(palmitic acid),22:6n-3(DHA) PC > di18:3n-3(alpha-linolenic acid) PC > di22:6n-3PC with a range in partition DeltaG of 913 cal/mol. Our results suggest that the large differences observed in cholesterol-lipid interactions contribute to the forces responsible for lateral domain formation in plasma membranes. These differences may also be responsible for the heterogeneous cholesterol distribution in cellular membranes, where cholesterol is highly enriched in plasma membranes and relatively depleted in intracellular membranes.