Structure and interactions of ether- and ester-linked phosphatidylethanolamines

The ether-linked phospholipid 1,2-dihexadecylphosphatidylethanolamine (DHPE) was studied as a function of hydration and in fully hydrated mixed phospholipid systems with its ester-linked analogue 1,2-dipalmitoylphosphatidylethanolamine (DPPE). A combination of differential scanning calorimetry (DSC) and X-ray diffraction was used to examine the phase behavior of these lipids. By DSC, from 0 to 10 wt % H2O, DHPE displayed a single reversible transition that decreased from 95.2 to 78.8 degrees C and which was shown by X-ray diffraction data to be a direct bilayer gel to inverted hexagonal conversion, L beta----HII. Above 15% H2O, two reversible transitions were observed which stabilized at 67.1 and 92.3 degrees C above 19% H2O. X-ray diffraction data of fully hydrated DHPE confirmed the lower temperature transition to be a bilayer gel to bilayer liquid-crystalline (L beta----L alpha) phase transition and the higher temperature transition to be a bilayer liquid-crystalline to inverted hexagonal (L alpha----HII) phase transition. The lamellar repeat distance of gel-state DHPE increased as a function of hydration to a limiting value of 62.5 A at 19% H2O (8.6 mol of water/mol of DHPE), which corresponds to the hydration at which the transition temperatures are seen to stabilize by DSC. Electron density profiles of DHPE, in addition to calculations of the lipid layer thickness, confirmed that DHPE in the gel state forms a noninterdigitated bilayer at all hydrations. Fully hydrated mixed phospholipid systems of DHPE and DPPE exhibited two reversible transitions by DSC.(ABSTRACT TRUNCATED AT 250 WORDS)     

Phase behavior and structure of aqueous dispersions of sphingomyelin

The phase behavior of bovine brain sphingomyelin in water has been determined by polarizing light microscopy, differential scanning calorimetry, and X-ray diffraction. Lamellar phases, in which water is intercalated between sheets of lipid molecules arranged in the classical bilayer fashion, are present over much of the phase diagram. An order-disorder transition separates the high temperature, liquid crystalline, lamellar phase from a more ordered lamellar phase at low temperatures. The hydration characteristics of sphingomyelin are similar to the structurally related lecithin in that only limited amounts of water are incorporated above and below the transition. Above the transition at 47 degrees C, a maximum of 35% by weight of water can be incorporated between the lipid bilayers, the total thickness at maximum hydration being 60.2 A, the lipid thickness 38 A, and the surface area per lipid molecule at the interface 60 A(2). Water in excess of 35% by weight is present as a separate phase. Below the phase transition, at 25 degrees C a maximum of 42% by weight of water may be incorporated between the lipid bilayers. On increasing the hydration, the lamellar repeat distance increases from 63.5 A to a limiting value of 76 A. Within this hydration range the calculated lipid thickness decreases from 63.5 to 42.5 A, and the surface area per lipid molecule increases from 36.1 to 53.6 A(2). Although these changes may be accounted for by a structure in which the hexagonally packed ordered hydrocarbon chains tilt progressively with respect to the normal to the bilayer plane on increasing hydration, it is possible that changes in other more complex lamellar structures may be responsible for these variations in lipid thickness and surface area.     

Experimental evidence for hydrophobic matching and membrane-mediated interactions in lipid bilayers containing gramicidin.

Hydrophobic matching, in which transmembrane proteins cause the surrounding lipid bilayer to adjust its hydrocarbon thickness to match the length of the hydrophobic surface of the protein, is a commonly accepted idea in membrane biophysics. To test this idea, gramicidin (gD) was embedded in 1, 2-dilauroyl-sn-glycero-3-phosphocholine (DLPC) and 1, 2-myristoyl-sn-glycero-3-phosphocholine (DMPC) bilayers at the peptide/lipid molar ratio of 1:10. Circular dichroism (CD) was measured to ensure that the gramicidin was in the beta6.3 helix form. The bilayer thickness (the phosphate-to-phosphate distance, or PtP) was measured by x-ray lamellar diffraction. In the Lalpha phase near full hydration, PtP is 30.8 A for pure DLPC, 32.1 A for the DLPC/gD mixture, 35.3 A for pure DMPC, and 32.7 A for the DMPC/gD mixture. Gramicidin apparently stretches DLPC and thins DMPC toward a common thickness as expected by hydrophobic matching. Concurrently, gramicidin-gramicidin correlations were measured by x-ray in-plane scattering. In the fluid phase, the gramicidin-gramicidin nearest-neighbor separation is 26.8 A in DLPC, but shortens to 23.3 A in DMPC. These experiments confirm the conjecture that when proteins are embedded in a membrane, hydrophobic matching creates a strain field in the lipid bilayer that in turn gives rise to a membrane-mediated attractive potential between proteins.     

Small-angle neutron scattering study of the lipid bilayer thickness in unilamellar dioleoylphosphatidylcholine vesicles prepared by the cholate dilution method: n-decane effect

Previous X-ray diffraction studies on fully hydrated fluid lamellar egg phosphatidylcholine phases indicated a approximately 10 A increase of bilayer thickness in the presence of excess n-decane [Biochim. Biophys. Acta 597 (1980) 455], while the small-angle neutron scattering (SANS) on unilamellar extruded dioleoylphosphatidylcholine (DOPC) vesicles detected substantially smaller 2.4+/-1.3 A bilayer thickness increase at n-decane/DOPC molar ratio of 1.2 [Biophys. Chem. 88 (2000) 165]. The purpose of the present study is to investigate the n-decane effect on the bilayer thickness in unilamellar DOPC vesicles prepared by the sodium cholate (NaChol) dilution method. Mixed DOPC+NaChol micelles at DOPC and NaChol concentrations of 0.1 mol/l were prepared in 2H(2)O containing 0.135 mol/l NaCl. This micellar solution was diluted in 0.135 mol/l NaCl in 2H(2)O to reach the final DOPC and NaChol concentrations of 0.008 mol/l. Thirty microliters of n-decane solution in methanol was added to 1 ml of this dispersion. After methanol evaporation, SANS was conducted on the dispersions. From the Kratky-Porod plot ln[I(Q)Q(2)] vs. Q(2) of SANS intensity I(Q) in the range of scattering vector values Q corresponding to interval 0.001 A(-2)相似文献   

Bilayer thickness and lipid interface area in unilamellar extruded 1,2-diacylphosphatidylcholine liposomes: a small-angle neutron scattering study

Small-angle neutron scattering (SANS) experiments have been performed on large unilamellar liposomes prepared from 1,2-dilauroylphosphatidylcholine (DLPC), 1,2-dimyristoyl-phosphatidylcholine (DMPC) and 1,2-distearoylphosphatidylcholine (DSPC) in heavy water by extrusion through polycarbonate filters with 500 A pores. The neutron scattering intensity I(Q) in the region of scattering vectors Q corresponding to 0.0015 A(-2) < or = Q(2) < or = 0.0115 A(-2) was fitted using a step function model of bilayer neutron scattering length density and supposing that the liposomes are spherical and have a Gaussian distribution of radii. Using the lipid volumetric data, and supposing that the thickness of bilayer polar region equals to d(H) = 9+/-1 A and the water molecular volume intercalated in the bilayer polar region is the same as in the aqueous bulk aqueous phase, the steric bilayer thickness d(L), the lipid surface area A(L) and the number of water molecules per lipid molecule N intercalated in the bilayer polar region were obtained: d(L) = 41.58+/-1.93 A, A(L) = 57.18+/-1.00 A(2) and N = 6.53+/-1.93 in DLPC at 20 degrees C, d(L) = 44.26+/-1.42 A, A(L) = 60.01+/-0.75 A(2) and N = 7.37+/-1.94 in DMPC at 36 degrees C, and d(L) = 49.77+/-1.52 A, A(L) = 64.78+/-0.46 A(2) and N = 8.67+/-1.97 in DSPC at 60 degrees C. After correcting for area thermal expansivity alpha approximately 0.00417 K(-1), the lipid surface area shows a decrease with the lipid acyl chain length at 60 degrees C: A(L) = 67.56+/-1.18 A(2) in DLPC, A(L) = 66.33+/-0.83 A(2) in DMPC and A(L) = 64.78+/-0.46 A(2) in DSPC. It is also shown that a joint evaluation of SANS and small-angle X-ray scattering on unilamellar liposomes can be used to obtain the value of d(H) and the distance of the lipid phosphate group from the bilayer hydrocarbon region d(H1).     

Phase equilibria and molecular packing in the N,N-dimethyldodecylamine oxide/gramicidin D/water system studied by 2H nuclear magnetic resonance spectroscopy.

A partial phase diagram of the system N,N-dimethyldodecylamine oxide (DDAO)/water/gramicidin D was determined by 2H-NMR. Both 2H2O and perdeuterated DDAO (DDAO-d31) were studied by solid state NMR techniques. Addition of gramicidin D to the micellar (L1), normal hexagonal (HI) and cubic (I) phases of DDAO induces phase separations, giving two-phase regions, which all contain a lamellar (L alpha) phase. The L alpha phase containing gramicidin is characterized by larger order parameters for DDAO-d31 compared with the corresponding order parameters in the L alpha and HI phases of DDAO-d31/H2O. The L alpha phase may stay in equilibrium with any other phase in the phase diagram. The DDAO exchange between the coexisting phases is slow on the NMR timescale, which is why the recorded NMR spectrum consists of superimposed spectra from the different phases occurring in the sample. Gramicidin D can be solubilized in appreciable quantities only in the lamellar phase of DDAO-d31. Increasing amounts of gramicidin in the liquid crystalline phases result in a continuous increase in the molecular ordering up to about 5 mol% gramicidin, where a plateau is reached. This is consistent with a recent theoretical model describing the influence on the ordering of lipids by a membrane protein with larger hydrophobic thickness than the lipid bilayer. The solvent used for dissolving gramicidin at the incorporation of the peptide in the lipid aggregates has no effect on the 2H-NMR lineshapes of DDAO-d31. It is concluded that gramicidin is solubilized in the L alpha phase and that it always adopts the channel conformation independent of a particular solvent. The channel conformation is also supported by CD studies. In some of the samples, macroscopic orientation of the lipid aggregates is observed. It is concluded that DDAO-d31 in the binary system favors an orientation with the long axis of the hydrocarbon chain perpendicular to the magnetic field, whereas when gramicidin D is present the hydrocarbon chain orients parallel to the magnetic field. This is explained by the fact that gramicidin aligns with its helical axis parallel to the magnetic field, thereby forcing also the DDAO-d31 molecules to obtain such an orientation.     

Importance of hydration for gramicidin-induced hexagonal HII phase formation in dioleoylphosphatidylcholine model membranes

The macroscopic organization, lipid head group conformation, and structural and dynamic properties of 2H2O were investigated in dioleoylphosphatidylcholine (DOPC) model systems of varying gramicidin and 2H2O (or H2O) content by means of small-angle X-ray diffraction and 31P and 2H NMR. At low stages of hydration, N less than 6 (N = 2H2O/DOPC molar ratio), a single lamellar phase is observed in which the gramicidin molecules become preferentially hydrated upon increasing N. For 6 less than N less than 12 phase separation occurs between a gramicidin-poor and a gramicidin-rich lamellar phase. This latter phase is characterized by a smaller repeat distance and decreased DOPC head group order. For N greater than 12, the gramicidin-rich lamellar phase converts to a hexagonal HII phase. Thus, hydration of gramicidin is a prerequisite for HII phase formation in the DOPC/gramicidin system. The HII phase is very rich in gramicidin and 2H2O (gramicidin:DOPC:H2O = 1:1.1:0.9 w/w/w). A model is proposed in which self-assembly of hydrated gramicidin molecules into domains of a specific structure plays a determinant role in the formation of the HII phase by gramicidin.     

The effect of cholesterol in small amounts on lipid-bilayer softness in the region of the main phase transition

The temperature dependence of the small-angle neutron scattering from aqueous multilammellar DMPC lipid bilayers, containing small amounts of cholesterol, is analyzed near the main phase transition by means of a simple geometric model which yields the lamellar repeat distance, the hydrophobic thickness of the bilayer, the interlamellar aqueous spacing, as well as fluctuation parameters. The observation of anomalous swelling behavior in the transition region is interpreted as an indication of bilayer softening and thermally reduced bending rigidity. Our results indicate that the effect of small amounts of cholesterol, ≲3 mole%, is a softening of the bilayers in the transition region, whereas cholesterol contents above this range lead to the well-known effect of rigidification. The possible biological relevance of this result is discussed. Received: 24 October 1996 / Accepted: 9 December 1996     

Thermodynamic and structural effects of propranolol on DPPC liposomes

Some thermodynamic and structural aspects of propranolol-DPPC liposomes interaction were investigated by DSC and X-ray diffraction: the lamellar arrangement of the lipid matrix remains intact even at high concentrations of the drug (until 1:1 drug/lipid molar ratio). However, the bilayer thickness increases significantly and the chains become perpendicular to the lamellar planes, for increasing drug content. At still higher propranolol concentrations a hexagonal phase occurs followed by a lamellar phase, in which the liposomes are destroyed. Moreover, the presence of propranolol has been found to impart fluidity to the lipid matrix.     

A conformation transition of lung surfactant lipids probably involved in respiration.

X-ray scattering and freeze-fracture electron microscopy of a lung surfactant extract show the existence of a complex lamellar phase, L gamma, over a wide range of concentrations and temperatures. This lamellar phase, which consists of two bilayer motifs comprised of monolayers with stiff chains alternating with monolayers with disordered chains, allows us to propose a structural model of a collapse phase at the alveolar pulmonary interface. This model accounts for the increase in surface pressure during the compression as well as the easy respreading upon expansion of the interface during the respiratory cycle.     

Structural,dynamic and mechanical properties of POPC at low cholesterol concentration studied in pressure/temperature space

We have studied the structural, dynamic and mechanical properties of 1-palmitoyl-2-oleoyl- sn-glycero-3-phosphatidylcholine (POPC)/cholesterol binary mixtures by small-angle X-ray scattering. Our investigations were concentrated on the biologically most relevant pressure-temperature-cholesterol regime, i.e. the liquid crystalline phase and its phase boundary to the lamellar gel phase within a cholesterol concentration up to 25 mol%. From the dependence of the transition pressure we derived a value of 19 kJ/mol for the transition enthalpy Delta H(m) of POPC in excess water. With increasing cholesterol concentration, Delta H(m) drops to about 7 kJ/mol at 20 mol% cholesterol. Time-resolved pressure-scan (p-scan) and temperature-jump (T-jump) experiments reveal that at low cholesterol content (<5-8 mol%) the fluidity and also the bilayer compressibility increase remarkably. In contrast, at concentrations between 5 and 25 mol% cholesterol the bilayer becomes again more rigid and the lipid bilayer spacing increases about 2 A. Theses changes are attributed to the onset of phase separation between liquid disordered and liquid ordered phases. The fluid-fluid miscibility gap for this mono-unsaturated lecithin species is strongly enlarged compared with saturated lecithins.     

Combined influence of cholesterol and synthetic amphiphillic peptides upon bilayer thickness in model membranes.

Deuterium (2H) NMR was used to study bilayer hydrophobic thickness and mechanical properties when cholesterol and/or synthetic amphiphillic polypeptides were added to deuterated POPC lipid bilayer membranes in the liquid-crystalline (fluid) phase. Smoothed acyl chain orientational order profiles were used to calculate bilayer hydrophobic thickness. Addition of 30 mol% cholesterol to POPC at 25 degrees C increased the bilayer thickness from 2.58 to 2.99 nm. The peptides were chosen to span the bilayers with more or less mismatch between the hydrophobic peptide length and membrane hydrophobic thickness. The average thickness of the pure lipid bilayers was significantly perturbed upon addition of peptide only in cases of large mismatch, being increased (decreased) when the peptide hydrophobic length was greater (less) than that of the pure bilayer, consistent with the "mattress" model of protein lipid interactions (Mouritsen, O.G., and M. Bloom. 1984. Biophys. J. 46:141-153). The experimental results were also used to examine the combined influence of the polypeptides and cholesterol on the orientational order profile and thickness expansivity of the membranes. A detailed model for the spatial distribution of POPC and cholesterol molecules in the bilayers was proposed to reconcile the general features of these measurements with micromechanical measurements of area expansivity in closely related systems. Experiments to test the model were proposed.     

Structural properties of a phosphatidylcholine-cholesterol system as studied by small-angle neutron scattering: ripple structure and phase diagram

Small-angle neutron scattering has been used to study structural features of lamellar bilayer membranes of dimyristoylphosphatidylcholine (DMPC) and DMPC mixed with various amount of cholesterol. The studies were recorded at a fixed hydration level of 17% 2H2O, i.e. just below saturation. Bragg reflections gives information on the ripple structure and on the bilayer periodicity. The crystalline Lc phase, which was stabilized after long time storage at low temperature, exhibits major small angle scattering when cholesterol is mixed into the membrane. The intermediate P beta' gel-phase, which is characteristic by the rippled structure, is dramatically stabilized by the introduction of cholesterol. The ripple structure depends significantly both on the cholesterol content and on the temperature. At high temperatures, T greater than 15 degrees C, the inverse ripple periodicity varies basically linearly with cholesterol content, and approach zero (i.e. periodicity goes to infinite) at 20 mol% cholesterol, approximately. At lower temperatures the correlation is more complex. The data indicate additional phase boundaries below 2 mol% and at approx. 8 mol%. Secondary rippled structures are observed in the low temperature L beta'-phase for cholesterol content below approx. 8 mol%. The data gives detailed insight into the phosphatidylcholine cholesterol phase diagram, which is discussed on the basis of a simple model in which the cholesterol complexes are fixed to the defect stripes of the rippled structure.     

Neutron scattering shows that cytochrome b5 penetrates deeply into the lipid bilayer

Cytochrome b5 was asymmetrically reconstituted into small lipid vesicles made of a highly deuterated phospholipid. Small-angle neutron diffraction patterns were collected in a series of H2O-D2O mixtures from vesicles consisting of lipid and native or trypsinized cytochrome b5. The second moment of the radial distribution of scattering density in the vesicles was derived from these data and was compared to values calculated from three proposed models, which differ by the degree that cytochrome b5 penetrates the lipid bilayer. The model in which the hydrophobic domain of the protein is distributed across the bilayer agreed most closely with the data.     

Structure of the crystalline bilayer in the subgel phase of dipalmitoylphosphatidylglycerol

The structure of the subgel phase of dipalmitoylphosphatidylglycerol (DPPG) has been analyzed by X-ray diffraction techniques. Diffraction recorded from highly oriented DPPG specimens in the subgel phase extends to 2-A resolution. There are sharp lamellar reflections on the meridian, and other reflections lie on a series of wide-angle lattice lines parallel to the meridian and crossing the equator in the range of 8-2 A. The wide-angle lattice lines consist of radially sharp reflections centered on the equator of the X-ray film and also a series of broader, off-equatorial maxima. The lattice lines indicate that the DPPG molecules in each bilayer crystallize in a two-dimensional oblique lattice with dimensions a = 5.50 A, b = 7.96 A, and gamma = 100.5 degrees. These oblique lattices are not regularly aligned from bilayer to bilayer. Analysis of the lamellar diffraction shows that the bilayer has about the same thickness in the subgel and gel (L beta') phases. In the direction normal to the hydrocarbon chains, the chains are significantly closer together in the subgel phase as compared to the normal L beta' gel phase but have about the same separation as the chains in polyethylene and the crystalline n-alkanes. The bilayer thickness, area per lipid molecule, and intensity distribution along the lattice lines all indicate that in the subgel phase the hydrocarbon chains are tilted between 30 and 35 degrees from the normal to the bilayer plane.(ABSTRACT TRUNCATED AT 250 WORDS)     

Temperature and compositional dependence of the structure of hydrated dimyristoyl lecithin.

Differential scanning calorimetry and x-ray diffraction techniques have been used to investigate the structure and phase behavior of hydrated dimyristoyl lecithin (DML) in the hydration range 7.5 to 60 weight % water and the temperature range -10 to +60 degrees C. Four different calorimetric transitions have been observed: T1, a low enthalpy transition (deltaH approximately equal to 1 kcal/mol of DML) at 0 degrees C between lamellar phases (L leads to Lbeta); T2, the low enthalpy "pretransition" at water contents greater than 20 weight % corresponding to the transition Lbeta leads to Pbeta; T3, the hydrocarbon chain order-disorder transition (deltaH = 6 to 7 kcal/mol of DML) representing the transition of the more ordered low temperature phases (Lbeta, Pbeta, or crystal C, depending on the water content) to the lamellar Lalpha phase; T4, a transition occurring at 25--27 degrees C at low water contents representing the transition from the lamellar Lbeta phase to a hydrated crystalline phase C. The structures of the Lbeta, Pbeta, C, and Lalpha phases have been examined as a function of temperature and water content. The Lbeta structure has a lamellar bilayer organization with the hydrocarbon chains fully extended and tilted with respect to the normal to the bilayer plane, but packed in a distorted quasihexagonal lattice. The Pbeta structure consists of lipid bilayer lamellae distorted by a periodic "ripple" in the plane of the lamellae; the hydrocarbon chains are tilted but appear to be packed in a regular hexagonal lattice. The diffraction pattern from the crystalline phase C indexes according to an orthorhombic cell with a = 53.8 A, b = 9.33 A, c = 8.82 A. In the lamellae bilayer Lalpha strucure, the hydrocarbon chains adopt a liquid-like conformation. Analysis of the hydration characteristics and bilayer parameters (lipid thickness, surface area/molecule) of synthetic lecithins permits an evaluation of the generalized hydration and structural behavior of this class of lipids.     

Small angle x-ray scattering studies of magnetically oriented lipid bilayers.

Magnetically oriented lipid/detergent bilayers are potentially useful for studies of membrane-associated molecules and complexes using x-ray scattering and nuclear magnetic resonance (NMR). To establish whether the system is a reasonable model of a phospholipid bilayer, we have studied the system using x-ray solution scattering to determine the bilayer thickness, interparticle spacing, and orientational parameters for magnetically oriented lipid bilayers. The magnetically orientable samples contain the phospholipid L-alpha-dilauroylphosphatidylcholine (DLPC) and the bile salt analog 3-[(3-cholamidopropyl)dimethylammonio]-2-hydroxy-1-propanesulfonate (CHAPSO) in a 3:1 molar ratio in 70% water (w/v) and are similar to magnetically orientable samples used as NMR media for structural studies of membrane-associated molecules. A bilayer thickness of 30 A was determined for the DLPC/CHAPSO particles, which is the same as the bilayer thickness of pure DLPC vesicles, suggesting that the CHAPSO is not greatly perturbing the lipid bilayer. These data, as well as NMR data on molecules incorporated in the oriented lipid particles, are consistent with the sample consisting of reasonably homogeneous and well dispersed lipid particles. Finally, the orientational energy of the sample suggests that the size of the cooperatively orienting unit in the samples is 2 x 10(7) phospholipid molecules.     

A synchrotron X-ray diffraction characterization of the structure of complexes formed between sphingomyelin and cerebroside

Specific lipid-lipid interactions are believed to be responsible for lateral domain formation in the lipid bilayer matrix of cell membranes. The miscibility of glucocerebroside and sphingomyelin extracted from biological tissues has been examined by synchrotron X-ray powder diffraction methods. Fully hydrated binary mixtures of egg-sphingomyelin codispersed with glucosylceramide rich in saturated C22 and C24 N-acyl fatty acids were subjected to heating scans between 20 and 90 °C at 2 °C·min(-1). X-ray scattering intensity profiles were recorded at 1 °C intervals simultaneously in both small-angle and wide-angle scattering regions. A gel phase characterized by a single symmetric peak in the wide-angle scattering region was transformed in all mixtures examined to a fluid phase at about 40 °C, similar to dispersions of pure egg-sphingomyelin. A coexisting lamellar structure was identified at temperatures up to about 75 °C which was characterized by a broad Bragg reflection. The scattering intensity of this structure increased relative to the structure assigned as bilayers of pure sphingomyelin with increasing proportions of glucosylceramide in the mixture. The relationship between the scattering intensities of the two peaks and the relative mass fractions of the two lipids showed that the bilayers assigned to a glucosylceramide-rich structure were composed of sphingomyelin and glucosylceramide in molar ratios of 1 : 1 and 2 : 1, respectively, at temperatures below and above the order-disorder phase transition temperature of the sphingomyelin (40 °C).     

Solubilization of ubiquinone-10 in the lamellar and bicontinuous cubic phases of aqueous monoolein

Using X-ray diffraction measurements and polarizing microscopy, the solubilization of ubiquinone-10 (UQ10) was investigated in the lamellar and reversed bicontinuous cubic phases of aqueous monoolein (MO, 86 wt% of monooleoylglycerol). At 25 degrees C and UQ10 content below 0.5 wt%, a partial phase diagram of the MO/UQ10/H2O system indicated the same sequence of hydration-induced phases as found in the MO/H2O system. This low amount of coenzyme had no effect on the MO bilayer thickness and swelling behavior of phases, but it promoted thermotropic Q230-->HII phase transition. We suggested that the effect was determined by the UQ10 partitioning into the HII phase regions where the MO chains must be stressed upon the phase transition. At UQ10 contents above 0.5 wt%, a solid 'UQ10-rich' phase appeared inside the initially homogeneous phases within a few days. It was proposed that this process was driven by the coenzyme lateral diffusion in the MO bilayer.     

The structure of lipid bilayers and the effects of general anaesthetics: An X-ray and neutron diffraction study

We have looked for the effects of three clinically used inhalational anaesthetics (nitrous oxide, halothane and cyclopropane) on the structure of lecithin/ cholesterol bilayers. The anaesthetics were delivered to the membranes in the gaseous phase, so that effects at clinical concentrations could be determined.High-resolution X-ray diffraction patterns were recorded out to 4 Å and analyzed using swelling experiments. Parallel neutron diffraction experiments were performed and analyzed using H₂O-²H₂O exchange. Methods were developed which enabled us to obtain confidence limits for the X-ray and neutron structure factors.The resultant X-ray and neutron scattering density profiles clearly define the positions of the principal molecular groups in the unperturbed bilayer. In particular, the high-resolution electron density profiles reveal features directly attributable to the cholesterol molecule. A comparison with the neutron scattering density profiles shows that cholesterol is anchored with its hydroxyl group at the water/hydrocarbon interface, aligned with the fatty acid ester groups of the lecithin molecule. We suggest that this positioning of the cholesterol molecule allows it to act as a thickness buffer for plasma membranes.In the presence of very high concentrations of general anaesthetics, the bilayers show increased disorder while maintaining constant membrane thickness. At surgical concentrations, however, there are no significant changes in bilayer structure at 95% confidence levels. We briefly review the literature previously used to support lipid bilayer hypotheses of general anaesthesia. We conclude that the lipid bilayer per se is not the primary site of action of general anaesthetics.