Interaction of ferricytochrome c with zwitterionic phospholipid bilayers: a Raman spectroscopic study

The vibrational Raman spectra of both pure L-alpha-dipalmitoylphosphatidylcholine (DPPC) liposomes and DPPC multilayers reconstituted with ferricytochrome c under varying conditions of pH and ionic strength are reported as a function of temperature. Total integrated band intensities and relative peak height intensity ratios, two spectral scattering parameters used to determine bilayer disorder, are invariant to changes in pH and ionic strength but exhibit a sensitivity to the bilayer concentration of the ferricytochrome c. Protein concentrations were estimated by comparing the 1636 cm-1 resonance Raman line of known ferricytochrome c solutions to intensity values for the reconstituted multilayer samples. Temperature-dependent profiles of the 3100-2800 cm-1 C-H stretching, 1150-1000 cm-1 C-C stretching, 1440 cm-1 CH2 deformation, and 1295 cm-1 CH2 twisting mode regions characteristic of acyl chain vibrations reflect bilayer perturbations due to the weak interactions of ferricytochrome c. The DPPC multilamellar gel to liquid-crystalline phase transition temperature, TM, defined by either the C-H stretching mode I2935/I2880 or the C-C stretching mode I1061/I1090 peak height intensity ratios, is decreased by approximately 4 degrees C for the approximately 10(-4) M ferricytochrome c reconstituted DPPC liposomes. Other spectral features, such as the increase in the 2935 cm-1 C-H stretching mode region and the enhancement of higher frequency CH2 twisting modes, which arise in bilayers containing approximately 10(-4) M protein, are interpreted in terms of protein penetration into the hydrophobic region of the bilayer.     

Evidence for acyl chain trans/gauche isomerization during the thermal pretransition of dipalmitoyl phosphatidylcholine bilayer dispersions

In order to clarify, in dipalmitoyl phosphatidylcholine multilayers, the effect of the 34 degrees C thermal pretransition on the acyl chain intramolecular disordering process, Raman spectra of dipalmitoyl phosphatidylcholine gels at 20 and 34 degrees C were compared in the 1000--1200 cm-1 skeletal C-C stretching region. In addition to an overall intensity decrease associated with a change in chain packing characteristics, the growth of intensity in the 1080--1090 and 1122 cm-1 regions in the 34--20 degrees C) difference spectrum clearly indicates that the thermal pretransition is accompanied by an increase in the population of hydrocarbon chain gauche rotamers toward the center of the bilayer.     

Raman spectroscopy of the thermal properties of reassembled high-density lipoprotein: apolipoprotein A-I complexes of dimyristoylphosphatidylcholine

Isolated complexes of apolipoprotein A-I (apoA-I), the major apoprotein of human plasma high-density lipoproteins, and dimyristoylphosphatidylcholine (DMPC) have been prepared and studied by differential scanning calorimetry (DSC) and Raman spectroscopy. DSC studies establish that complexes having lipid to protein ratios of 200, 100, and 50 to 1 each exhibit a broad reversible thermal transition at Tc = 27 degrees C. The enthalpy of lipid melting for each of the three complexes is about 3 kcal/mol of DMPC. Raman spectroscopy indicates that the physical state of lipid molecules in the complexes is different from that in DMPC multilamellar liposomes. Analysis of the C-H stretching region (2800-3000 cm-1) of the complexes and of the pure components in water suggests that below 24 degrees C (Tc for DMPC) there is considerably less lateral order among lipid acyl chains in the complexes than in DMPC liposomes. Above 24 degrees C, these types of interactions appear to contribute equally or slightly less to the complex structure than in pure DMPC. The temperature dependence of peaks in the C-C stretching region (1000-1180 cm-1) reveals a continuous increase in the number of lipid acyl chain C-C gauche isomers over a broad range with increasing temperature. Compared to liposomes, DMPC in the complexes has more acyl chain trans isomers at temperatures above 24 degrees C; at temperatures above ca. 30 degrees C, trans isomer content is about the same for complexes and liposomes. A large change was observed in a protein vibrational band at 1340 cm-1 for pure vs. complexed apoA-I, indicating that protein hydrocarbon side chains are immobilized by lipid binding. The Raman data indicate that the reduction in melting enthalpy for complexes DMPC (approximately 3 kcal/mol) compared to that for free DMPC (approximately 6 kcal/mol) is due to reduced van der Waals interactions in the low-temperature lipid phase.     

Low levels of irradiation modify lipid domains in model membranes: a laser Raman study

We have used Raman spectroscopy to study the effects of ionizing radiation on thermal transitions of dipalmitoyl lecithin + polyunsaturated fatty acid liposomes. Raman spectra in the CH (2800-3000 cm-1), C = C (1600-1680 cm-1), and C-C (1000-1150 cm-1) stretching regions are sensitive to ionizing radiation. The CH stretching of acyl chains yields three strong bands around 2850, 2880, and 2930 cm-1. The ratios of the relative intensities of 2880 and 2850 cm-1 bands, i.e., I2880/2850, when plotted against temperature show multiple infection points which correspond to multiple spectroscopic transitions. These are ascribed to a separate phase with distinctive proportions of lecithin and polyunsaturated fatty acids. We find these transitions sensitive to low levels of ionizing radiation. Doses as low as 5-15 rad after 48 h of 60Co gamma irradiation and 60 kVp X irradiation drastically broaden and shift the polyunsaturated rich phase which occurs at lower temperatures (-7 to +5 degrees C) than that of pure dipalmitoyl lecithin (39 degrees C). In addition a new transition around 46 degrees C also emerges upon irradiation (48 h postirradiation). These irradiation effects can be accelerated by the presence of catalytic amounts of Fe2+/EDTA +H2O2. The membrane transition modification is more sensitive to 60 kVp X rays in comparison to 60Co gamma rays owing to the high LET component of the former. The intensity of 1660 cm-1 band, assigned to C = C stretching in the cis-configuration, loses intensity upon irradiation. Concomitantly, a new band around 1675 cm-1, assigned to trans-configuration, emerges. Similarly the increase in the "order parameter" as calculated from the relative intensities of C--C stretching bands indicates rigidification of membrane. Various factors such as reduction in unsaturation, increase in trans-configuration, and the formation of multiple peroxidation products are invoked as lipid phase modifiers.     

Electric fields in active sites: substrate switching from null to strong fields in thiol- and selenol-subtilisins.

Although known to be important factors in promoting catalysis, electric field effects in enzyme active sites are difficult to characterize from an experimental standpoint. Among optical probes of electric fields, Raman spectroscopy has the advantage of being able to distinguish electronic ground-state and excited-state effects. Earlier Raman studies on acyl derivatives of cysteine proteases [Doran, J. D., and Carey, P. R. (1996) Biochemistry 35, 12495-502], where the acyl group has extensive pi-electron conjugation, showed that electric field effects in the active site manifest themselves by polarizing the pi-electrons of the acyl group. Polarization gives rise to large shifts in certain Raman bands, e.g. , the C=C stretching band of the alpha,beta-unsaturated acyl group, and a large red shift in the absorption maximum. It was postulated that a major source of polarization is the alpha-helix dipole that originates from the alpha-helix terminating at the active-site cysteine of the cysteine protease family. In contrast, using the acyl group 5-methylthiophene acryloyl (5-MTA) as an active-site Raman probe, acyl enzymes of thiol- or selenol-subtilisin exhibit no polarization even though the acylating amino acid is at the terminus of an alpha-helix. Quantum mechanical calculations on 5-MTA ethyl thiol and selenol ethyl esters allowed us to identify the conformational states of these molecules along with their corresponding vibrational signatures. The Raman spectra of 5-MTA thiol and selenol subtilisins both showed that the acyl group binds in a single conformation in the active site that is s-trans about the =C-C=O single bond. Moreover, the positions of the C=C stretching bands show that the acyl group is not experiencing polarization. However, the release of steric constraints in the active site by mutagenesis, by creating the N155G form of selenol-subtilisin and the P225A form of thiol-subtilisin, results in the appearance of a second conformer in the active sites that is s-cis about the =C-C=O bond. The Raman signature of this second conformer indicates that it is strongly polarized with a permanent dipole being set up through the acyl group's pi-electron chain. Molecular modeling for 5-MTA in the active sites of selenol-subtilisin and N155G selenol-subtilisin confirms the findings from Raman spectroscopic studies and identifies the active-site features that give rise to polarization. The determinants of polarization appear to be strong electron pull at the acyl carbonyl group by a combination of hydrogen bonds and the field at the N-terminus of the alpha-helix and electron push from a negatively charged group placed at the opposite end of the chromophore.     

Effect of melittin on thermotropic lipid state transitions in phosphatidylcholine liposomes.

We have examined the Raman scattering due to CH stretching vibrations, as well as to v(-C=C-) and v(=C-C=) of beta-carotene, of liposomes composed of phosphatidylcholine (egg, dimyristoyl, dipalmitoyl) +/- cholesterol, beta-carotene or melittin in the temperature range of -10 degrees C to 45 degrees C. (2) Plots vs. temperature of the intensities of the 2885 cm-1 and 2930 cm-1 CH stretching bands relative to the intensity of the thermally stable 2850 cm-1 band, i.e. the I2885/I2850 and I2930/I2850 ratios, reveal a sharp discontinuity in cholesterol-free phosphatidylcholine liposomes; this coincides with the gel leads to liquid-crystal transition temperature of the fatty acyl chains. In cholesterol/phosphatudylcholine liposomes the change in I2885/I2850 occurs over a very broad temperature range and I2930/I2850 remains stable. (3) I1527/I1158, i.e. the intensity of v(-C=C-) relative to that of v(=C-C-) in beta-carotene/phosphatidylcholine liposomes, changes discontinuously at the gel leads to liquid-crystal transition temperature. The values above the transition temperature approach those of the carotenoid in organic solution. (4) The transitions reported in I2885/I2850 for phosphatidylcholine/melittin liposomes (25-56; 1, M/M) are shifted to much higher temperatures than observed in phosphatidylcholine liposomes. In the case of dimyristoyl phosphatidylcholine/melittin the changes in I2930/I2850 also occurs at a higher temperature (28 degrees C) than without melittin (21 degrees C), but the temperature shift is less than the +13 degrees C observed for I2885/I2850. It appears that the apolar moiety of melittin organizes phospholipids adjacent to and more remote from the peptide moiety, to form complexes with an elevated lipid transition temperature. The effect of the peptide moiety is greater on the methylene segments (I2885/I2850) than on the methyl termini (I2930/I2850).     

Raman spectroscopy of selectively deuterated dimyristoylphosphatidylcholine: studies on dimyristoylphosphatidylcholine-cholesterol bilayers

Dimyristoylphosphatidylcholine (DMPC), selectively deuterated in the sn-2 chain at the 3, 6, and 10 positions is used to probe DMPC-cholesterol interactions in multilamellar dispersions. Using the Raman spectral linewidths of the 2100 cm-1 C2H2 stretching modes as an index of membrane disorder, we demonstrate that cholesterol tends to order, or increase the number of trans carbon-carbon bonds within the DMPC acyl chain near the headgroup region at all temperatures. At low temperatures, cholesterol disorders the acyl chains near the methyl termini by inducing gauche conformers; cholesterol orders the entire chain at higher temperatures. These determinations are qualitatively consistent with conclusions drawn from deuterium nuclear magnetic resonance studies, but specifically reflect acyl chain trans/gauche isomerization on the 10(-12)-10(-13) s vibrational time scale.     

Effect of ions on phospholipid layer structure as indicated by Raman spectroscopy.

Various anions and cations are found to induce changes in the layered structure of phosphatidylcholine-water systems as indicated by Raman Spectroscopy. From the ratio of Raman intensities, I1064/I1089, it is inferred that dipositive ions decrease the proportion of gauche character in the hydrocarbon chains, with the relative influence being: Ba2+ less than Mg2+ less than Ca2+ similar to Cd2+. Unipositive ions (Li+, K+ and Na+) produce no observed changes in the Raman spectrum of the lecithin dispersion. The proportion of gauche character of the hydrocarbon chains is found to be nearly independent of the anion for: Br-, Cl-, acetate-, I-, ClO4-, CNS- and SO42-. Dispersions prepared with a solution of KI+I2 produced Raman spectra in which the 1089cm-1 peak, which is characteristic of random lipid chains, was greatly intensified, presumably because of the presence of I3- which is known to penetrate the lipid lamellae. The observed trends are discussed.     

Raman spectroscopic studies of dimyristoylphosphatidic acid and its interactions with ferricytochrome c in cationic binary and ternary lipid-protein complexes.

The vibrational Raman spectra of both pure 1-alpha-dimyristoylphosphatidic acid (DMPA) liposomes and DMPA multilayers reconstituted with ferricytochrome c at pH 7 and pH 4, with either sodium or calcium as the cation, are reported as a function of temperature. Multilayers composed of a 1:1 mol ratio DMPA and dimyristoylphosphatidylcholine with perdeuterated acyl chains (DMPC-d54) have also been reconstituted with approximately 10(-4) M ferricytochrome c for Raman spectroscopic observation. Total integrated band intensities and relative peak height intensity ratios, two spectral Raman scattering parameters used to characterize bilayer properties, are sensitive to the presence of both ferricytochrome c and the cation in the reconstituted liposomes. Temperature profiles, derived from the various Raman intensity parameters for the 3,100-2,800 cm-1 lipid acyl chain C-H stretching mode region specifically reflect bilayer perturbations due to the interactions of ferricytochrome c. At pH 4 the calcium DMPA multilamellar gel to liquid crystalline phase transition temperatures Tm, defined by either the C-H stretching mode I2850/I2880 and I2935/I2880 peak height intensity ratios, are 58.5 +/- 0.5 degrees C and 60.0 +/- 0.3 degrees C, respectively. This difference in Tm's resolves the phase transition process into first an expansion of the lipid lattice and then a melting of the lipid acyl chains. At pH 7 the calcium DMPA liposomes show no distinct phase transition characteristics below 75 degrees C. For sodium DMPA liposomes reconstituted with ferricytochrome c at either pH 4.0 or pH 7.0, spontaneous Raman spectra show altered lipid structures at temperatures above 40 degrees C. Resonance Raman spectra indicate that ferricytochrome c reconstituted in either calcium or sodium DMPA liposomes changes irreversibly above Tm. For either the binary lipid or ternary lipid-protein systems reconstituted with DMPC-d54, linewidth parameters of the DMPC-d54 acyl chain CD2 symmetric stretching modes at 2,103 cm-1 provide a sensitive measure of the conformational and dynamic properties of the perdeuterated lipid component, while the 3,000 cm-1 C-H spectral region reflects the bilayer characteristics of the DMPA species in the complex. Although calcium clearly induces a lateral phase separation in the DMPA/DMPC-d54 system at pH 7.5 (Kouaouci, R., J.R. Silvius, I. Grah, and M. Pezolet. 1985. Biochemistry. 24:7132-7140), no distinct lateral segregation of the lipid components is observed in the mixed DMPA/DMPC-d54 lipid system in the presence of either ferricytochrome c or the sodium and calcium cations at pH 4.0.(ABSTRACT TRUNCATED AT 400 WORDS)     

A Raman spectroscopic study on the interaction of an ion-channel protein with a phospholipid in a model membrane system (gramicidin A/L-alpha-lysophosphatidylcholine)

The interaction of the ion channel polypeptide gramicidin A with the L-alpha-lysophosphatidylcholine micelles in a membrane state association (approximative molar ratio 1:9) was investigated by Raman spectroscopy. Studies were carried out over the spectral ranges of 700-1700 cm-1 and 2800-3100 cm-1 at 10 degrees C. The Raman spectrum of L-alpha-lysophosphatidylcholine micelles indicated a disordered structure of the lipid acyl chains by the high intensities of the gauche conformation vibrations. Changing from the micellar phase to the membrane state of association with gramicidin A, the intensities of all-trans stretching modes increased whereas the intensities of gauche conformation vibrations decreased, reflecting the emergence of ordered lipid chains. Hydrophobic interactions between the acyl chains and the polypeptide side chain residues were demonstrated. The absence of modifications in intensities of the very strong tryptophan vibrations in the complex spectrum indicated that, if the tryptophan-stacking interactions suggested by some authors exist, they are very weak ones.     

Effects of various numbers and positions of cis double bonds in the sn-2 acyl chain of phosphatidylethanolamine on the chain-melting temperature

In an attempt to investigate systematically the effects of various single and multiple cis carbon-carbon double bonds in the sn-2 acyl chains of natural phospholipids on membrane properties, we have de novo synthesized unsaturated C20 fatty acids comprised of single or multiple methylene-interrupted cis double bonds. Subsequently, 15 molecular species of phosphatidylethanolamine (PE) with sn-1 C20-saturated and sn-2 C20-unsaturated acyl chains were semi-synthesized by acylation of C20-lysophosphatidylcholine with unsaturated C20 fatty acids followed by phospholipase D-catalyzed base-exchange reaction in the presence of excess ethanolamine. The gel-to-liquid crystalline phase transitions of these 15 mixed-chain PE, in excess H2O, were investigated by high resolution differential scanning calorimetry. In addition, the energy-minimized structures of these sn-1 C20-saturated/sn-2 C20-unsaturated PE were simulated by molecular mechanics calculations. It is shown that the successive introduction of cis double bonds into the sn-2 acyl chain of C(20):C(20)PE can affect the gel-to-liquid crystalline phase transition temperature, Tm, of the lipid bilayer in some characteristic ways; moreover, the effect depends critically on the position of cis double bonds in the sn-2 acyl chain. Specifically, we have constructed a novel Tm diagram for the 15 species of unsaturated PE, from which the effects of the number and the position of cis double bonds on Tm can be examined simultaneously in a simple, direct, and unifying manner. Interestingly, the characteristic Tm profiles exhibited by different series of mixed-chain PE with increasing degree of unsaturation can be interpreted in terms of structural changes associated with acyl chain unsaturation.     

Conformation, orientation and dynamics of dodecylphosphocholine in micellar aggregate: a 3.2 ns molecular dynamics simulation study

A dodecylphosphocholine micelle of 86 monomers with 5776 water molecules has been simulated under NPT conditions for 3.2 ns using GROMACS2.0. The micelle was found to be very dynamic. Some of the C-C bonds, independent of their position in the DPC monomer, adopt gauche conformation and the trans <--> gauche transitions are quite frequent. An average of about 11% of the C-C bonds in the micelle are observed to be in the gauche conformation (i.e., |dihedral angle|< 120 degrees). The terminal methyl groups are randomly distributed all over the micelle whereas the nitrogen atom of phosphocholine headgroup atoms is restricted to the interface region. Some of the monomers were found to lie on the surface. The shape of micelle, influenced by the packing considerations, shows deviations from spherical shape. The phosphocholine headgroup is well solvated and there is no water penetration into the micelle core. The overall features of the micelle of 86 DPC monomers conforms to the lattice model of micelle proposed by Dill and Flory [Dill K A, Flory P J (1981) Proc Natl Acad Sci USA 78, 676-680] and is similar to DPC micelles of smaller aggregate sizes except for the positional preference of the C-C bonds for the gauche conformation and the trans<-->gauche transition times [Tieleman D P, van der Spoel D, Berendsen H J C (2000) J Phys Chem B 104, 6380-6388; Wymore T, Gao X F, Wong T C (1999) J Mol Struct (Theochem) 485-486, 195-210]. It appears that packing considerations play a predominant role in determining the shape and dynamics of the micelle.     

Effects of polypeptide-phospholipid interactions on bilayer reorganizations Raman spectroscopic study of the binding of polymyxin B to dimyristoylphosphatidic acid and dimyristoylphosphatidylcholine dispersions

The interactions of the antibiotic polymixin B, a polycationic cyclic polypeptide containing a branched acyl side chain, with dimyristoylphosphatidylcholine (DMPC) and dimyristoylphosphatidic acid (DMPA) bilayers were investigated by Raman spectroscopy for a wide range of lipid/polypeptide mole fractions. Temperature profiles, constructed from peak height intensity ratios derived from the lipid methylene C-H stretching and acyl chain C-C stretching mode regions, reflected changes originating from lateral chain packing effects and intrachain trans / gauche rotamer formation, respectively. For DMPC/polymyxin B bilayers the temperature dependent curves indicate a broadening of the gel-liquid crystalline phase transition accompanied by an approx. 3 C deg. increase in the phase transition temperature from 22.8°C for the pure bilayer to 26°C for the polypeptide complex. For a 10:1 lipid/polypeptide mole ratio the temperature profile derived from the C-C mode spectral parameters displays a second order/disorder transition, at approx. 35.5°C, associated with the melting behavior of approximately three bilayer lipids immobilized by the antibiotic's charged cyclic headgroup and hydrophobic side chain. For the 10:1 mole ratio DMPA/polypeptide liposomes, the temperature profiles indicate three order/disorder transitions at 46, 36 and 24°C. Pure DMPA bilayers display a sharp lamellar-micellar phase transition at 51°C.     

Effects of halothane on dipalmitoylphosphatidylcholine liposomes: a Raman spectroscopic study

Raman spectroscopy has been used to monitor the concentration of halothane (1-bromo-1-chloro-2,2,2-trifluoroethane) in 20% aqueous dispersions of dipalmitoylphosphatidylcholine (DPPC) as well as to follow changes in the acyl chain order within the hydrocarbon interior of the liposomes. Temperature profiles for the gel to liquid-crystalline phase transitions for the liposomes were constructed from changes in peak height intensity ratios in the C-H stretching mode and C-C stretching mode regions. Halothane present at the clinical level produces a change of -0.5 degrees C in the phase transition temperature. A limiting transition temperature of about 21 degrees C and saturation of the gel phase occur when the molar ratio of halothane to DPPC reaches about 1.25. At molar ratios above 2.1, the liquid-crystalline phase is also saturated with halothane. Calculations of the distribution of halothane between the various phases in the system are presented and used to interpret literature data as well as the present experiments. Ideal solution theory accounts rather well for the depression in the transition temperature over most of the mole ratio range, an outcome which implies that halothane is excluded from the hydrocarbon interior but not the head-group region in the gel phase. The role of halothane in the head-group region is discussed.     

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.     

The phase transition behavior of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) model membrane influenced by 2,4-dichlorophenol--an FT-Raman spectroscopy study

The effect of 2,4-dichlorophenol (DCP) on the structures and phase transitions of fully hydrated 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) liposomes was studied using FT-Raman spectroscopy. Whereas the Raman frequency shifts of the most frequently investigated bands of C-C and C-H stretching regions only indicate the main phase transition (P(beta')-L(alpha)) of the pure DPPC/water system, the Raman shift of C-H scissoring vibration at 1440 cm(-1) was found to be able to reveal the pretransition (L(beta')-P(beta')) as well. Analyzing the spectral parameters of the trans band at 1128 cm(-1), which does not overlap with DCP vibrational modes, a continuous decrease of trans conformations was found with increasing DCP concentration at 26 degrees C accompanying the phase transitions L(beta')-P(beta') and P(beta')-L(alpha). The intensity ratio of the symmetrical and asymmetrical methylene stretching bands (at 2850 cm(-1) and 2880 cm(-1)), defined as the disorder parameter by Levin [Levin, I.W., 1985. Two types of hydrocarbon chain interdigitation in sphingomielin bilayers. Biochemistry 24, 6282-6286], indicated that in the interdigitated phase (L(I)) the order is markedly high and comparable with that of L(beta). Both the phase transition P(beta')-L(alpha) in the DCP/DPPC molar ratio range of 10/100-50/100 and the phase transition L(I)-L(alpha) led to a significant increase of disordered chains and the presence of DCP molecules induced a more disordered chain region than that observed in the L(alpha) phase of DPPC. Nevertheless, it was found that the L(alpha) phase with DCP contains approximately the same amount of trans conformers than that without DCP.     

Raman spectroscopy of nerve fibers. A study of membrane lipids under steady state conditions.

The molecular structures of different nerve fibers kept in good physiological conditions were studied by laser Raman spectroscopy. For myelinated nerves like the rat sciatic nerve, the Raman spectrum is dominated by bands due to the lipid component of the myelin sheath. The temperature dependence of these bands does not reveal any thermotropic phase transition between 0 and 40 degrees C. There is, however, with temperature, a linear increase in the intermolecular disorder that is accompanied by an increase in the number of gauche bonds of the phospholipid acyl chains. For unmyelinated nerves such as the lobster leg nerve, the C-H stretching region of the Raman spectrum is covered by bands arising from the protein component of the axoplasm. However, for the garfish olfactory nerve that has a high density of excitable membranes, phospholipid bands are observed and can be used as intrinsic structural probes of the excitable membranes. The relative intensity of these bands is also temperature dependent.     

Raman spectroscopic study of polycrystalline mono- and polyunsaturated 1-eicosanoyl-d(39)-2-eicosenoyl-sn-glycero-3-phosphocholines: bilayer lipid clustering and acyl chain order and disorder characteristics

Polycrystalline lipid samples of a series of mono- and polyunsaturated, double bond positional isomers of 1-eicosanoyl-d(39)-2-eicosenoyl-sn-glycero-3-phosphocholines [C(20-d(39)):C(20:1 Delta(j))PC, with j = 5, 8, 11, or 13; C(20-d(39)):C(20:2 Delta(11,14))PC; and C(20-d(39)):C(20:3 Delta(11, 14,17))PC] were investigated using vibrational Raman spectroscopy to assess the acyl chain packing order-disorder characteristics and putative bilayer cluster formation of the isotopically differentiated acyl chains. Perdeuteration of specifically the saturated sn-1 acyl chains for these bilayer systems enables each chain's intra- and intermolecular conformational and organizational properties to be evaluated separately. Various saturated chain methylene CD(2) and carbon-carbon (C&bond;C) stretching mode peak height intensity ratios and line width parameters for the polycrystalline samples demonstrate a high degree of sn-1 chain order that is unaffected by either the double bond placement or number of unsaturated bonds within the sn-2 chain. In contrast, the unsaturated sn-2 chain spectral signatures reflect increasing acyl chain conformational disorder as either the cis double bond is generally repositioned toward the chain terminus or the number of double bonds increases from one to three. The lipid bilayer chain packing differences observed between the sn-1 and sn-2 chains of this series of monounsaturated and polyunsaturated 20 carbon chain lipids suggest the existence of laterally distributed microdomains predicated on the formation of highly ordered, saturated sn-1 chain clusters.     

Organic pesticides modify lipid-lipid and lipid-protein domains in model membranes. A laser Raman study.

The effect of hexachlorocyclohexane (all isomers) on the thermal transition properties of phospholipid liposomes was determined by Raman spectroscopy. Raman spectra of liposomes with and without the presence of hexachlorocyclohexanes were recorded in the C-H stretching region which shows three major bands around 2850, 2880 and 2930 cm-1. Thermal transition properties were estimated from plots of I2880/I2850 and or I2930/I2850 vs. temperature, where I represents the intensity of the respective band. Our data on phospholipid liposomes reveal that delta- and gamma-hexachlorocyclohexanes drastically reduce and broaden the main thermal transitions of phospholipids at toxic level concentrations. These effects are more pronounced in liposomes containing 18 or more carbon atom long acyl chains. Alpha- and beta-isomers at similar concentrations show a minimum effect on the thermal transition properties of phospholipids. Raman analysis of phospholipid liposomes containing melittin, interestingly, reveal that the delta-isomer unlike the gamma-isomer strongly alters the transition properties of boundary lipids. These data suggest that the effect of hexachlorocyclohexanes on the thermal transition properties of membranes is stereo specific and that the delta-isomer preferably disrupts the lipid-protein domains. Results are explained on the basis of the dynamic flexibility owing to the equatorial and axial chlorine atoms of various hexachlorocyclohexane isomers.