The effect of sonication on the hydrocarbon chain conformation in model membrane systems: A Raman spectroscopic study

Raman spectra are presented for egg lecithin above and below the gel-liquid crystal phase transition, and several regions of the Raman spectrum are shown to be sensitive to conformational changes in the hydrocarbon chains. These regions are used to investigate the effect of sonication on the structure of egg lecithin and dipalmitoyl lecithin vesicles.Sonication of both egg lecithin above T_m, and dipalmitoyl lecithin above and below T_m produces no change in the relative population of trans and gauche isomers in any of the systems studied. Sonication does however appear to effect interchain interactions, a possible consequence of imperfect packing towards the center of the bilayers in vesicle systems.     

Raman spectroscopic studies of biological membrane model systems: Dietherlecithins

Raman spectra are obtained for the multilayer dispersion of rac-1,2,dioctadec-9′-cis-enyl-glycero-3-phosphorylcholine (dietherlecithin) in excess water. The CH stretching region was studied as a function of temperature and indicates that the multilayer dispersions undergo a liquid crystal to the gel phase transition at ?21 ± 4°C.     

Raman spectroscopic study of semisynthetic species of cerebroside sulfate: two types of hydrocarbon chain interdigitation.

Raman spectroscopy was used to study the phase behavior of several semisynthetic species of the acidic glycosphingolipid cerebroside sulfate (CBS) which occur in myelin. The C-H stretching mode region at 2800-3100 cm-1 of C18:0-CBS, C24:0-CBS, and C26:0-CBS, and the alpha-hydroxy fatty acid species C18:0h-CBS, was studied in the presence of 2 M Li+ and 2 M K+. Earlier studies have shown that K+ shields the negative charge on the sulfate more effectively than Li+, thus promoting intermolecular hydrogen-bonding interactions between the lipid molecules. Indeed, a novel broad background feature was present in the Raman spectra from 2900 to 3200 cm-1, which was attributed to O-H stretch associated with intermolecular hydrogen bonding between lipid hydroxyl groups. After subtraction of this broad feature, the intensities of the lipid C-H stretching vibrational transitions could be determined. These indicated that in K+, the degree of order (intrachain conformation and lateral chain-chain interactions) of C18:0-CBS, whose hydrocarbon region is fairly symmetrical in chain length, is similar to that of the symmetric chain length glycerolipid dipalmitoylphosphatidylcholine, while the degree of order is lower in Li+, as a result of the increased lateral charge repulsion of the head groups in Li+. Two phase transitions were observed for the highly asymmetric species C24:0-CBS and C26:0-CBS in K+ but only one transition in Li+.(ABSTRACT TRUNCATED AT 250 WORDS)     

The solution conformation of poly(L-lysine). A Raman and infrared spectroscopic study.

The Raman and infrared spectra of poly(L -lysine) and poly(DL -lysine) in solution are reported and the effects of various salts are investigated. The results demonstrate that α-helix formation in solution is induced by specific salts and the spectral data support the hypothesis of regions of local order for poly(L -lysine) in aqueous solutions of low ionic strength.     

Effect of acyl chain unsaturation on the conformation of model diacylglycerols: a computer modeling study.

In a previous modeling study we identified an angle iron-shaped conformation of docosahexaenoic acid and showed that an sn-1-stearoyl diacylglycerol (DG) that contained an sn-2-docosahexaenoyl group in this conformation could adopt a highly regular shape. In the present study we compared the properties of this DG with those of sn-1-stearoyl DGs that contained other unsaturated fatty acyl groups in the sn-2 position. The major findings were that: 1) sn-1-stearoyl DGs that contain polyenoic fatty acids in the sn-2 position can assume regular shapes, and 2) these shapes differ depending on the location of the double bonds. sn-2-Polyenoic fatty acyl groups with a double bond sequence that begins close to the carboxyl ester bond are associated with one type of regular shape, while sn-2-polyenoic fatty acyl groups with a double bond sequence that begins toward the middle of the chain are associated with another. Such shapes would not have been predicted by current ideas relating membrane fluidity to unsaturation. In contrast, another finding of the present study, that sn-1-stearoyl-2-oleoyl DG can adopt, at best, only a highly irregular shape is in good agreement with the results of previous investigators.     

The effect of methylmercury (II) binding on the conformation of poly(L-glutamic acid) and poly(L-lysine: a Raman spectroscopic study

The binding of the methylmercury cation CH₃Hg⁺ by poly(L -glutamic acid) (PGA) and by poly(L -lysine) (PLL) has been investigated by Raman spectroscopy. Coordination on the side-chain COO^? and NH groups of these polypeptides gave characteristic ligand–Hg stretching modes at ca. 505 and 450 cm^?1, respectively. Precipitation generally occurred upon formation of the complexes and changes of conformation were common. The solid complex obtained from PGA at pH 4.6 was found to have a mostly disordered conformation, which differed from the respective α-helical and β-sheet structures of the dissolved and precipitated uncomplexed polypeptide in the same conditions. An α-helical structure was generally adopted by the complex formed with PLL, even in pH and temperature conditions where the free polypeptide normally exists in another conformation. The addition of a stronger complexing agent, glutathione, to the PLL/CH₃Hg⁺ complex caused a migration of the bound cations and a restoration of the polypeptide to its original state.     

Raman spectroscopic study on the conformation of 11 S form acetylcholinesterase from Torpedo californica

Vibrational Raman spectroscopy has been used to study the conformation of the 11 S form of acetylcholinesterase from Torpedo californica. Secondary structure analysis by the method of Williams [(1983) J. Mol. Biol. 166, 581-603] shows 49% alpha-helical structure, 23% beta-sheets, 11% turns and 15% undefined structure. Secondary structure estimates obtained for this enzyme by Raman spectroscopy and circular dichroism have been analyzed.     

The interactions of neuropeptides with membrane model systems: a case study.

The interactions between the positively charged neuropeptides substance P (SP), bradykinin (BK), and zwitterionic Met-enkephalin (ME) neuropeptides, and negatively charged SDS and zwitterionic lysophosphatidylcholine (LPC) membrane model systems, have been investigated using one- and two-dimensional nmr experiments. Proton longitudinal relaxation studies were used to characterize these interactions as intrinsic or extrinsic. An extrinsic interaction are similar to those observed for extrinsic membrane proteins. An intrinsic interaction are similar to those observed for intrinsic membrane proteins, and would require that the hydrophobic residues penetrate or insert into the hydrophobic core of the membrane. The interactions between both SP and BK and SDS, based on nmr results, may be characterized as intrinsic, and the interaction between ME and SDS may be characterized as extrinsic. Two-dimensional nuclear Overhauser enhancement spectroscopy experiments proved the insertion of the phenylalanine residues on both SP and BK into the hydrophobic core of SDS micelles. The interaction between SP and BK with LPC based on nmr results are characterized as extrinsic, with the interaction between ME and SDS characterized as weakly intrinsic.     

Deuterium nuclear magnetic resonance spectroscopic study of the fluorescent probe diphenylhexatriene in model membrane systems

We have investigated the deuterium (2H) nuclear magnetic resonance (NMR) spectra of two 2H-labeled fluorescence probes (trans,trans,trans-1,6-diphenylhexa-1,3,5-trienes, DPHs) incorporated into model lipid bilayer membrane systems at various temperatures. The membranes consisted of multilamellar bilayers of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) containing varying concentrations of cholesterol. The conventional one-order parameter approach often used in the analysis of the NMR data of lipid membranes does not explain the observed temperature variations of the spectral features. Consistent with the molecular symmetry, the results have thus been analyzed in terms of an ordering matrix with more than one independent element. The molecular order parameter (SNMR), the order along the long molecular axis, in the pure lipid system varies from 0.49 to 0.26 as the temperature is increased from 25 to 57 degrees C. These values are somewhat larger than the order parameters obtained from fluorescence depolarization (SFLU) on sonicated DMPC vesicles. Such discrepancies probably arise from the looser packing of the sonicated vesicles. Addition of cholesterol to the model membranes causes the order parameter of the probe molecules to increase. At 35 degrees C, SNMR increases from 0.38 (with no cholesterol) to 0.92 (in the presence of 50 mol % cholesterol). These values are about 10% larger than those obtained from fluorescence depolarization studies on sonicated vesicles. The SNMR for DPH are somewhat larger than those obtained in earlier NMR studies of 2H-labeled cholesterol. However, they compare well with those obtained for 2H-labeled DMPC.(ABSTRACT TRUNCATED AT 250 WORDS)     

Raman studies of conformational changes in model membrane systems

Laser Raman spectra of concentrated samples of phosphatidyl choline and phosphatidyl ethanolamine were taken at approximately 10° intervals over a temperature range of 90°–19°C. The spectral region from 30 to 3300 cm^?1 was investigated. Several new spectral features were discovered which are correlated to phospholipid liquid crystalline structure. It is shown that 1) frequency shifts occur in the $\text{PO}{}_2{}^{\mathrm{?}}$ symmetric stretch band which suggest a change in exposure of the PO₂ group to the solvent upon melting, 2) the frequency of the translational hydrocarbon mode around 150 cm^?1 appears to indicate the degree to which the hydrocarbon chain is extended, 3) the methyl and methylene stretch bands at 2890 and 2850 cm^?1 very clearly demonstrate hydrocarbon chain melting, and 4) the 720 cm^?1 band, previously assigned to the symmetric OPO diester stretch, appears to be due instead to the symmetric CN stretch of choline.     

Conformation and dynamic properties of a saturated hydrocarbon chain confined in a model membrane: a Brownian dynamics simulation

A Brownian dynamics simulation of a saturated hydrocarbon chain with simple mean-field potentials, namely anchorage, orientation and enclosing, reproducing a biological membrane environment is presented. The simulation was performed for a time equivalent to 1.4 micros thanks to the simplicity of our model. The results are compared with those obtained for a hydrocarbon chain simulated in the absence of the membrane potentials but with confinement. With the appropriate choice of parameters, equilibrium properties, such as deuterium order parameter, chain length, tilt angle and geometry, and dynamic properties, such as dihedral angle transition rate, rotational and translational diffusion, recovered from our simulations, correctly reproduced, are consistent with hydrocarbon-derived molecule experimental results and simulation results obtained from other more complex studies.     

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.     

Raman spectroscopic study of the structure of antibodies.

The Raman spectra of human IgG, IgM, and rabbit IgG in lyophilized form and solution are reported. The spectral results indicate that the predominant structure in these immunoglobulin proteins is the antiparallel β-sheet. The Raman spectra have also been obtained of rabbit anti-ovalbumin, and this antibody molecule precipitated with its respective antigen. The spectra reflect a conformational change on binding of antibody with antigen. The conformational change occurs in the direction of disordering.     

A Monte Carlo study of the excluded-volume effect on the amylosic chain conformation

A Monte Carlo procedure was used to determine the effect of excluded volume on the conformational dimensions of amylosic chains. The excluded volume was introduced into the model by assuming that hard spheres, which cannot overlap each other, exist at the center of mass of each glucose unit in the chain sequence. Monte Carlo chains, which were generated to be distributed consistent with the potential energy of nonbonded nearest-neighbor interactions, underwent self-intersections, and the attrition rate in the generation of self-avoiding chains was found to obey an exponential decay law with increasing chain length x. Thus, in order to generate effectively a large number of self-avoiding chains with long sequences, we used the Wall–Erpenbeck s-p method of chain enrichment [F. T. Wall and J. J. Erpenbeck (1959) J. Chem. Phys. 30 , 634–637]. By examination of the radial distribution of the end-to-end distance and the chain-length dependence of the quantity 〈r²〉/xl² (〈r²〉 is the mean square end-to-end distance and l is the virtual bond length), it was found that unperturbed amylosic chains change in overall conformation from a non-Gaussian chain having a helical character to Gaussian as x is increased, whereas perturbed chains do not show Gaussian behavior even at x = 500. For the perturbed chains, 〈r²〉 can be expressed by the equation 〈r²〉 = ax^b in the range of 100 ≤ x ≤ 500, where a and b > 1 are constants. From comparisons of the persistence vectors and perspective drawings of representative unperturbed and perturbed chains, we felt the local conformation of the amylosic chains, i.e., the local helical character, is also affected by the long-range excluded-volume interaction.     

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.     

A comparative Raman spectroscopic study of cholinesterases.

We report Raman spectra of various cholinesterases: lytic tetrameric forms (G4) obtained by tryptic digestion of asymmetric acetylcholinesterase (AChE) from Torpedo californica and Electrophorus electricus, a PI-PLC-treated dimeric form (G2) of AChE from T marmorata, and the soluble tetrameric form (G4) of butyrylcholinesterase (BuChE) from human plasma. The contribution of different types of secondary structure was estimated by analyzing the amide I band, using the method of Williams. The spectra of cholinesterases in 10 mM Tris-HCl (pH 7.0) indicate the presence of both alpha-helices (about 50%) and beta-sheets (about 25%), together with 15% turns and 10% undefined structures. In 20 mM phosphate buffer (pH 7.0), the spectra indicated a smaller contribution of alpha-helical structure (about 35%) and an increased beta-sheet content (from 25 to 35%). This shows that the ionic milieu profoundly affects either the conformation of the protein (AChE activity is known to be sensitive to ionic strength), or the evaluation of secondary structure, or both. In addition, we analyzed vibrations corresponding to the side chains of aromatic and aliphatic amino acids. In particular, the analyses of the tyrosine doublet (830-850 cm-1) and of the tryptophan vibration at 880 cm-1 indicated that these residues are predominantly 'exposed' on the surface of the molecules.     

FTIR spectroscopic studies of the conformation and amide hydrogen exchange of a peptide model of the hydrophobic transmembrane alpha-helices of membrane proteins.

The conformation and amide hydrogen exchangeability of the hydrophobic peptide Lys2-Gly-Leu24-Lys2-Ala-amide were studied by Fourier transform infrared spectroscopy. In these studies information on the secondary structure of the peptide was obtained from an examination of the contours of both the amide I and amide II absorption bands. The conformationally sensitive amide I and amide II regions of the infrared spectra suggest that the peptide is predominantly alpha-helical and that it contains some non-alpha-helical structures which are probably in an extended conformation. Studies of the exchangeability of the amide protons of the peptide indicate that there are two populations of amide protons which differ markedly with respect to their exchangeability with the bulk solvent phase, whether the peptide is dissolved in methanol or dispersed in hydrated lipid bilayers. One population of amide protons is very readily exchangeable, and our data suggest that it arises primarily but not exclusively from the extended regions of the peptide. The other population exchanges very slowly with the bulk solvent and appears to originate entirely from the alpha-helical domain of the peptide. This latter population is virtually unexchangeable when the peptide is dispersed in hydrated phosphatidylcholine bilayers but can be largely exchanged when the peptide is solubilized with methanol. We suggest that this slowly exchanging population of amide protons arises from the central part of the hydrophobic polyleucine core which forms a very stable alpha-helix that would be deeply buried in the hydrophobic domain of hydrated lipid bilayers.(ABSTRACT TRUNCATED AT 250 WORDS)     

Coupled changes between lipid order and polypeptide conformation at the membrane surface. A 2H NMR and Raman study of polylysine-phosphatidic acid systems

Thermotropism and segmental chain order parameters of sn-2-perdeuteriated dimyristoyl-phosphatidic acid (DMPA)-water dispersions, with and without poly(L-lysine) (PLL) of different molecular weights, have been investigated by solid-state deuterium NMR spectroscopy. The segmental chain order parameter profile of this negatively charged lipid is similar to that already found for other lipids. Addition of long PLL (MW = 200,000) increases the temperature, Tc, of the lipid gel-to-fluid phase transition, whereas short PLL (MW = 4000) has practically no effect on Tc. In the fluid phase both varieties of PLL increase the "plateau" character of segmental order parameters up to carbon position 10. At the same reduced temperature, long PLL more significantly increases the segmental ordering, especially at the methyl terminal position. This leads to the conclusion that polar head-group capping and charge neutralization by PLL induce severe changes in lipid chain ordering, even down to the bilayer core. The structure of PLL bound to the lipid bilayer surface was monitored by Raman spectroscopy, following the amide I bands. Results show that the lipid gel-to-fluid phase transition triggers a conformational transition from ordered beta-sheet to random structure of short PLL, while it does not affect the strongly stabilized beta-sheet structure of long PLL. It is concluded that both short and long PLL can efficiently cap and neutralize lipid head groups, whatever their structure, and that peptide length is a key parameter in whether lipids or peptides are the driving force in conformationally coupled changes of both partners in the membrane.