Lateral chain packing in lipids and membranes

The aliphatic chains of many biologically important lipids are heterogeneous and often related to the functions of the molecules. Certain phospholipids containing arachidonic acid may serve as precursors for prostaglandins, certain diglycerides may serve as second messengers for certain membrane-triggered reactions (43), and other phospholipids containing a very short chain in the two position may serve as vasoactive hormones (44). The packing of such molecules is of interest. The evidence is quite clear from both the conformation of saturated and unsaturated molecules and from mixing experiments in the solid state that long and short chains don't mix well, nor do unsaturated and saturated chains, even if they are of the same chain length. There is even some evidence to indicate that some degree of chain segregation occurs even in the liquid state. However, different chains are often associated through covalent bonds, e.g., in wax esters, diacylglycerols, triacylglycerols, and phospholipids. A variety of possibilities for chain segregation are present in the neat phases of wax esters, ceramides, diacylglycerols, and triacylglycerols. However, in the unique case of membrane lipids like phospholipids or sphingolipids, the two chains are forced to lie side by side by virtue of the interaction of the polar group with water, and thus interactions between different chains must occur. Most of the evidence suggests that, when a solid phase results in these systems, the nonspecific chain packing mode (hexagonal chain packing) is preferred. In fact, for all of the phospholipids studied thus far, clearcut evidence of specific chain-chain interaction in molecules having both unsaturated and saturated chains has never been observed. However, for mixed chain triacylglycerols, evidence of specific chain-chain interactions (beta' and even beta) has been found and some suggestions have been given as to how this might occur through chain segregation mechanisms in the neat state. The literature suggests that further work needs to be done on the interaction of different chains that are covalently linked to the same molecule. Such studies will lead to a better understanding of the structure of lipid bilayers, membranes, lipoproteins, and lipid deposits.     

Hydrocarbon chain packing and the effect of ethanol on the thermotropic phase behavior of mixed-chain phosphatidylglycerols

Previous studies in this laboratory have delineated the relationship between the acyl chain asymmetry of mixed-chain phosphatidylcholines and the effect of ethanol concentration ([EtOH]) on their melting behavior (Li et al., Biophys J., 70 (1996) 2784-2794). This present investigation extends these findings to another phospholipid family by using high-resolution differential scanning calorimetry (DSC) to characterize the effect of ethanol concentration on the main phase transition temperature (Tm) of five molecular species of mixed-chain phosphatidylglycerol (PG). For C(14):C(18)PG, C(15):C(17)PG, C(16):C(16)PG, and C(17):C(15)PG, a biphasic profile in the Tm versus [EtOH] plot was observed, and the minimum in the plot for each PG occurred at 33, 15, 19, and 36 mg/ml, respectively. This biphasic behavior is typical of phospholipids whose acyl chain asymmetry is fairly small. For C(18):C(14)PG, only a linear decrease in the Tm was observed as a function of ethanol concentration; this effect is characteristic of highly asymmetric phospholipids. Our DSC results obtained with mixed-chain PG in the presence of ethanol demonstrate that the acyl chain asymmetry of the five lipids studied can be ranked as follows: C(15):C(17)PG相似文献   

Lactosylceramide: effect of acyl chain structure on phase behavior and molecular packing

Lactosylceramide (LacCer) is a pivotal intermediate in the metabolism of higher gangliosides, localizes to sphingolipid-sterol "rafts," and has been implicated in cellular signaling. To provide a fundamental characterization of LacCer phase behavior and intermolecular packing, LacCer containing different saturated (16:0, 18:0, 24:0) or monounsaturated (18:1(Delta9), 24:1(Delta15)) acyl chains were synthesized and studied by differential scanning calorimetry and Langmuir film balance approaches. Compared to related sphingoid- and glycerol-based lipids, LacCers containing saturated acyl chains display relatively high thermotropic and pressure-induced transitions. LacCer monolayer films are less elastic in an in-plane sense than sphingomyelin films, but are somewhat more elastic than galactosylceramide films. Together, these findings indicate that the disaccharide headgroup only marginally disrupts gel phase packing and orients more perpendicular than parallel to the interface. This contrasts the reported behavior of digalactosyldiglycerides with saturated acyl chains. Introducing single cis double bonds into the LacCer acyl chains dramatically lowers the high thermotropic and pressure-induced transitions. Greater reductions occur when cis double bonds are located near the middle of the acyl chains. The results are discussed in terms of how an extended disaccharide headgroup can enhance interactions among naturally abundant LacCers with saturated acyl chains.     

Miscibility, chain packing, and hydration of 1-palmitoyl-2-oleoyl phosphatidylcholine and other lipids in surface phases.

The miscibility of 1-palmitoyl-2-oleoyl phosphatidylcholine with triolein, 1,2-diolein, 1,3-diolein, 1(3)-monoolein, oleyl alcohol, methyl oleate, oleic acid, and oleyl cyanide (18:1 lipids) was studied at the argon-water interface. The isothermal phase diagrams for the mixtures at 24 degrees were characterized by two compositional regions. At the limit of miscibility with lower mol fractions of 18:1 lipid, the surface pressure was composition-independent, but above a mixture-specific stoichiometry, surface pressure at the limit of miscibility was composition-dependent. From the two-dimensional phase rule, it was determined that at low mol fractions of 18:1 lipids, the surface consisted of phospholipid and a preferred packing array or complex of phospholipid and 18:1 lipid, whereas, above the stoichiometry of the complex, the surface phase consisted of complex and excess 18:1 lipids. In both regions of the phase diagram, mixing along the phase boundary was apparently ideal allowing application of an equation of state described earlier (J. M. Smaby and H. L. Brockman, 1984, Biochemistry, 23:3312-3316). From such analysis, apparent partial molecular areas and hydrations for phospholipid, complex, and 18:1 lipid were obtained. Comparison of these calculated parameters for the complexed and uncomplexed states shows that the aliphatic moieties behave independently of polar head group. The transition of each 18:1 chain to the complexed state involves the loss of about one interfacial water molecule and its corresponding area. For 18:1 lipids with more than one chain another two water molecules per additional chain are present in both states but contribute little to molecular area.(ABSTRACT TRUNCATED AT 250 WORDS)     

Lipid chain geometry of C14 glycerol-based lipids: effect on lipoplex structure and transfection

The effects have been determined of a systematic alteration of the alkyl chain geometry of a C14 analogue of DOTMA on the detailed molecular architecture of the resulting cationic vesicles formed both in the absence and presence of 50 mol% DOPE, and of the lipoplexes prepared from these vesicles using either calf thymus or plasmid DNA. The C14 DOTMA analogues studied involved cis- or trans-double bonds at positions Δ9 or Δ11, and a compound (ALK) featuring an alkyne at position C9. For all of these analogues, examination by light scattering and neutron scattering, zeta potential measurement, and negative staining electron microscopy showed that there were no significant differences in the structures or charges of the vesicles or of the resulting lipoplexes, regardless of the nature of the DNA incorporated. Differences were observed, however, between the complexes formed by the various lipids when examining the extent of complexation and release by gel electrophoresis, where the E-lipids appeared to complex the DNA more efficiently than all other lipids tested. Moreover, the lipoplexes prepared from the E-lipids were the most effective in transfection of MDA-MB-231 breast cancer cells. As indicated through confocal microscopy studies, the E-lipids also showed a higher internalisation capacity and a more diffuse cellular distribution, possibly indicating a greater degree of endosomal escape and/or nuclear import. These observations suggest that the extent of complexation is the most important factor in determining the transfection efficiency of the complexes tested. At present it is unclear why the E-lipids were more effective at complexing DNA, although it is thought that the effective area per molecule occupied by the cationic lipid and DOPE head groups, and therefore the density of positive charges on the surface of the bilayer most closely matches the negative charge density of the DNA molecule. From a consideration of the geometry of the cationic lipids it is anticipated that the head groups of the E-lipids would occupy a smaller area per molecule than the ALK or Z-lipids.     

A model for the packing of lipids in bilayer membranes

A number of known structural properties of mixed lipid bilayer membranes and monolayers are accounted for by a model in which lipids pack into bilayers and monolayers like building blocks, each characterized by a surface head group area and characteristic solid angle. In phospholipids above the melting transition the head group area (at a given temperature and degree of hydration) is fairly invariant while the hydrocarbon region may be liquid-like so long as the molecule is not compressed beyond its characteristic solid angle.Phosphotidylcholine and phosphotidylserine are tapered lipids, i.e. their surface head group areas are greater than their non-polar end areas; cholesterol is frayed, i.e. its polar end area is less than its non-polar end area; while phosphotidylethanolamine is almost cylindrical. The “condensing” effect of cholesterol in mixed phospholipid-cholesterol films is seen as a taper-fray accomodation. The lipid distribution in erythrocyte membranes is shown to be conductive to a stable strain-free membrane.     

Molecular dynamics simulation of packing and mobility of lipids in bilayer membranes

A model of DSPC lipid membrane in gel and liquid-crystalline states has been developed. The parameters have been determined that enable one to calculate the molecular dynamics of lipid bilayers in the full-atromic approximation. The parameters of packing and mobility of lipid molecules for the liquid crystalline state of the bilayer have been calculated. The values agree well with experimental data. Based on the model of the liquid crystalline state of the membrane, a system in the gel-like state has been constructed. The model of the gel-like state reproduces well the packing of lipids in real bilayers, whereas the mobility of molecules in the gel-like state was found to be overestimated.     

Conformation and packing properties of membrane lipids: the crystal structure of sodium dimyristoylphosphatidylglycerol

The conformation and molecular packing of sodium 1,2-dimyristoyl-sn-glycero-phospho-rac-glycerol (DMPG) have been determined by single crystal analysis (R = 0.098). The lipid crystallizes in the monoclinic spacegroup P2(1) with the unit cell dimensions a = 10.4, b = 8.5, c = 45.5 A and beta = 95.2 degrees. There are two independent molecules (A and B) in the asymmetric unit which with respect to configuration and conformation of their glycerol headgroup are mirror images. The molecules pack tail to tail in a bilayer structure. The phosphoglycerol headgroups have a layer-parallel orientation giving the molecules an L-shape. At the bilayer surface the (-) phosphoglycerol groups are arranged in rows which are separated by rows of (+) sodium ions. Laterally the polar groups interact by an extensive network of hydrogen, ionic and coordination bonds. The packing cross-section per molecule is 44.0 A2. The hydrocarbon chains are tilted (29 degrees) and have opposite inclination in the two bilayer halves. In the chain matrix the chain planes are arranged according to a so far unknown hybride packing mode which combines the features of T parallel and O perpendicular subcells. The two fatty acid substituted glycerol oxygens have mutually a - synclinal rather than the more common + synclinal conformation. The conformation of the diacylglycerol part of molecule A and B is distinguished by an axial displacement of the two hydrocarbon chains by four methylene units. This results in a reorientation of the glycerol back bone and a change in the conformation and stacking of the hydrocarbon chains. In molecule A the beta-chain is straight and the gamma-chain is bent while in molecule B the chain conformation is reversed.     

A model for the packing of lipids in bilayer membranes.

A number of known structural properties of mixed lipid bilayer membranes and monolayers are accounted for by a model in which lipids pack into bilayers and monolayers like building blocks, each characterized by a surface head group area and characteristic solid angle. In phospholipids above the melting transition the head group area (at a given temperature and degree of hydration) is fairly invariant while the hydrocarbon region may be liquid-like so long as the molecule is not compressed beyond its characteristic solid angle. Phosphatidylcholine and phosphatidylserine are tapered lipids, i.e. their surface head group areas are greater than their non-polar end areas; cholesterol is frayed, i.e. its polar end area is less than its non-polar end area; while phosphatidylethanolamine is almost cylindrical. The "condensing" effect of cholesterol in mixed phospholipid-cholesterol films is seen as a taper-fray accommodation. The lipid distribution in erythrocyte membrane is shown to be conducive to a stable strain-free membrane.     

Glycerol conformation and molecular packing of membrane lipids: The crystal structure of 2,3-dilauroyl-d-glycerol

The single-crystal structure of 2,3-dilauroyl-d-glycerol has been determined by Patterson rotation and translation methods and refined to R = 0.069. 2,3-dilauroyl-d-glycerol crystallizes in the monoclinic space group P2₁, with unit cell dimensions: $\text{a = 5.46}\text{A}\text{?}\text{, b = 7.59}\text{A}\text{?}\text{, c = 34.2}\text{A}\text{?}\text{and}\text{β = 93.1 °}$, and with two molecules per unit cell. The molecules have their hydrocarbon chains aligned parallel, and are arranged in a bilayer structure. The chain stacking is achieved by a bend in the fatty acid. The hydrocarbon chains pack according to the orthorhombic perpendicular chain packing mode, and are tilted 26.5 ° from the layer normal.The structural features of 2,3-dilauroyl-d-glycerol have been analysed with reference to the corresponding hydrophobic moieties in the crystal structures of different membrane lipids. The glycerol group in 2,3-dilauroyl-d-glycerol is oriented parallel to the layer plane, but changes to an approximately layer-perpendicular orientation when a polar group is attached. The molecular conformation of the glycerol-dicarboxylic ester group, however, is identical in both the absence and presence of a head group, indicating extensive conformational restrictions for this group due to both intrinsic properties and chain stacking. The gathered data provide detailed information on the structural properties of the hydrophobic moiety of membrane lipids.     

Polar group interaction and molecular packing of membrane lipids: The crystal structure of lysophosphatidylethanolamine

The conformation and molecular packing of 3-palmitoyl-dl-glycerol-1-phosphoryl-ethanolamine has been determined by a single crystal analysis (R = 0.115); it crystallizes in the monoclinic space group $\text{P2}{}_1\text{a}$ with a unit cell of $\text{a = 7.66}\text{A}\text{?}\text{, b = 9.08}\text{A}\text{?}\text{, c = 37.08}\text{A}\text{?}\text{and}\text{β = 90.2 °}$, with four molecules per unit cell. The molecules exist as configurational and conformational enantiomers and pack in a bilayer arrangement. The phosphorylethanolamine groups have an orientation parallel to the layer surface. The hydrocarbon chains are arranged according to the T∥ chain packing mode and adopt an extreme tilt of 57.5 ° with respect to the layer normal. The free glycerol hydroxyl group forms an intramolecular hydrogen bond with, a phosphate oxygen and thus affects the conformation and orientation of the head group. The phosphorylethanolamine dipoles are oriented parallel to each other in double rows, while they are antiparallel and form a continuous network in dilauroylphosphatidylethanolamine (Elder et al., 1977). The area per molecule in 3-palmitoyl-dl-glycerol-1-phosphorylethanolamine (34.8 Ų) is less than in diacylphosphatidylethanolamine (38.6 Ų), indicating that in the latter the hydrocarbon chains determine the molecular cross-section. The significance of the interaction and space requirement of the phosphorylethanolamine group for the phase behaviour of phosphatidylethanolamine is discussed.     

Functions of the flagellar modes of rotation in bacterial motility and chemotaxis

Bacteria swim by rotating their flagella, the rotation being due to a motor located at the base of each flagellum. In this paper the correlation between motor function and mode of swimming is reviewed, with special emphasis on recent data that indicate that the motor is a three-state device. Novel findings with regard to the motor function and bioenergetics are surveyed, and mechanisms are proposed to account for these findings.     

Hydrocarbon chain packing and molecular motion in phospholipid bilayers formed from unsaturated lecithins. Synthesis and properties of sixteen positional isomers of 1,2-dioctadecenoyl-sn-glycero-3-phosphorylcholine.

Isomers of cis-octadecenoic acid, with the double bond in each position in the hydrocarbon chain, were used to synthesize the corresponding 1,2-diacyl-sn-glycero-3phosphorylcholines (lecithins). Differential thermal analysis of the lecithins, as a function of water content, permitted evaluation of the limiting transition temperature (Tc) of each isomer. Values of Tc plotted against double bond position fell on a smooth curve with a minimum at minus 22 degrees for the dioctadec-9'-enoyl compound. The presence of a "pretransition" endotherm in differential thermal analysis of 1,2-dioctadec-15'-and 1,2-dioctadec-16'-enoyl-sn-glycero-3-phosphorylcholine implies the existence of two beta crystalline forms. This was not observed with any of the other lecithins. Enthalpy and entropy data were then obtained from differential scanning calorimetry measurements. Values of delta H were lower (7.6 plus or minus 0.1 kcal mol- minus 1) when the center of unsaturation was near the middle of the hydrocarbon chain than they were (9.6 kcal mol- minus 1) when the center of unsaturation was close to either end of the chain. However, values of delta S showed no consistent variation with double bond position. Four positional isomers of 1-octadec-cis-enoyl-2-octadecanoyl-sn-glycero-3-phosphorylcholine were synthesized. With the double bond near the middle of the chain or close to the terminal group, the Tc values of the mixed acid lecithins were higher than those of the corresponding dioctadecenoyl lecithins. 13-C nuclear magnetic resonance relaxation measurements were used to obtain information about chain motion of selected 1,2-dioctadec-cis-enoyl-sn-glycero-3-phosphorylcholines at a temperature (52 degrees) above the Tc values. Spin-lattice relaxation times of the resolved resonances indicated that location of double bonds near the middle, as compared to either end, of the hydrocarbon chain favors enhanced molecular motion along the length of the chins and especially at the terminal methyl end. In the gel state, the minimum interaction potential energy of hydrocarbon chains in bilayers formed from dioctadecenoyl lipids appears to be minimized by localization of the double bond near the middle of the chains. It is suggested that in the case of homogeneous chains the double bond primarily affects the cooperativity of interactions and has very little steric effect on van der Waals' contacts. By contrast, in bilayers of mixed lecithins, with heterogeneous chains, the steric effect may become dominant, depending on double bond position. These differences in chain packing in the gel state are promulgated beyond the phase transition to the liquid crystalline state as an enhancement of chain motion as the temperature rises above Tc.     

Molecular packing of high-density and low-density lipoprotein surface lipids and apolipoprotein A-I binding

The surface pressure (pi)-molecular area (A) isotherms for monolayers of human high-density lipoprotein (HDL3) and low-density lipoprotein (LDL) phospholipids and of mixed monolayers of these phospholipids with cholesterol spread at the air-water interface were used to deduce the likely molecular packing at the surfaces of HDL3 and LDL particles. LDL phospholipids form more condensed monolayers than HDL3 phospholipids; for example, the molecular areas of LDL and HDL3 phospholipids at pi = 10 dyn/cm are 88 and 75 A2/molecule, respectively. The closer packing in the LDL phospholipids monolayer can be attributed to the higher contents of saturated phosphatidylcholines and sphingomyelin relative to HDL3. Cholesterol condenses both HDL3 and LDL phospholipid monolayers but has a greater condensing effect on the LDL phospholipid monolayer. The pi-A isotherms for mixed monolayer of HDL3 phospholipid/cholesterol and LDL phospholipid/cholesterol at stoichiometries similar to those at the surfaces of lipoprotein particles suggest that the monolayer at the surface of the LDL particle is significantly more condensed than that at the surface of the HDL3 particle. The closer lateral packing in LDL is due to at least three factors: (1) the difference in phospholipid composition; (2) the higher unesterified cholesterol content in LDL; and (3) a stronger interaction between cholesterol and LDL phospholipids relative to HDL3 phospholipids. The influence of lipid molecular packing on the affinity of human apolipoprotein A-I (apo A-I) for HDL3 and LDL surface lipids was evaluated by monitoring the adsorption of 14C-methylated apo A-I to monolayers of these lipids spread at various initial surface pressures (pi i).(ABSTRACT TRUNCATED AT 250 WORDS)     

Optical rotation and helical polypeptide chain configuration in collagen and gelatin

The optical rotation phenomena exhibited by a citrate-extracted fraction of ichthyocol (from carp swim bladder), as well as by the parent gelatin derived therefrom, have been studied. Dispersion data for all cases follow a single-term Drude equation, but the variations with state are adequately expressed by simple reference to changes in [alpha](D) as follows:- 1. The native collagen fraction, dispersed in 0.15 M citrate buffer at pH 3.7 in the cold (11 degrees C.), yields a high negative specific rotation, [alpha](D), near -350 degrees . 2. During equilibration at 40 degrees C., which causes conversion to a monodisperse parent gelatin, the rotation drops to about -110 degrees . 3. Gelation at 2 degrees C. results in a partial regain of rotation to around -290 degrees . This mutarotation is reversible, depending on temperature. 4. In the range 0.02 to 0.28 per cent the native ichthyocol and the warm gelatin solutions show little concentration dependence, but with the cold gelatin solutions the specific rotation increases with concentration. Gelatin films formed by cold evaporation yield high specific rotation (ca. -620 degrees ), but those formed by hot evaporation retain low optical activity. 5. Since this same collagen-gelatin system has been investigated physicochemically, it is possible to relate molecular changes to the observed variations in optical rotation. Conclusions are similar to those of Robinson (1953), who studied other gelatins: high negative rotation is believed related to a native collagen polypeptide configuration, herein specified as helical (from x-ray diffraction considerations) and destroyed by heating. The possible roles of intermolecular interactions and of prevalent pyrrolidine constituents in influencing the helical configuration and optical activity are discussed.