Cholesterol-lipid interactions: An infrared and raman spectroscopic study of the carbonyl stretching mode region of 1,2-dipalmitoyl phosphatidylcholine bilayers

Infrared and Raman spectra were obtained for the 1690–1770 cm^?1 carbonyl stretching mode region for 1,2-dipalmitoyl phosphatidylcholine (DPPC) bilayers in the anhydrous, partially hydrated and completely hydrated states. Spectral features at approx. 1740 and 1721 cm^?1 are assigned to CO stretching modes associated with the 1- and 2-chain carbonyl groups, respectively. Splittings of the primary transitions at 1743, 1738, ～1731 and ～1721 cm^?1 are attributed to rotational isomers involving the entire chain. Hydrogen bond formation between the fatty acid carbonyl and 3βOH cholesterol groups was investigated for anhydrous DPPC bilayers. Examination of frequencies, intensities and half-widths of the carbonyl bands indicates that no hydrogen bonding occurs at either of the two carbonyl sites. However, the addition of cholesterol to completely hydrated DPPC dispersions reduces the conformational inequivalence between the two fatty acid carbonyl groups by specifically perturbing the 2-chain. For cholesterol containing systems the carbonyl stretching mode transitions were also used to monitor lattice effects within the interface region as water binds to the bilayer head groups. Specifically, the addition of approx. 2 molecules of water per lipid molecule orders the lipid lattice and increases the bilayer packing density, while the subsequent addition of 4 molecules of water per lipid molecule releases the packing constraints within the interface region and thereby decreases the packing density.     

Vibrational raman spectra of lipid systems containing amphotericin B

Resonance-enhanced and normal vibrational Raman spectra were observed for both multilamellar and single-wall vesicle assemblies of dimyristoyl phosphatidylcholine containing amphotericin B, a channel-forming polyene antibiotic, and cholesterol. The decrease in the frequency of the polyene antibiotic C  C stretching mode at 1556 cm^?1 and the increase in intensity of the CCH in-plane deformation mode at 1002 cm^?1 indicate that amphotericin B is ordered in a lipid-cholesterol medium similarly to the solid, but is surrounded by a slightly more polar environment. The intensity of the C  C stretching mode I₁₅₅₆ decreases 4-fold during the broadened gel to liquid crystalline phase transition (16–32°C) of dimyristoyl lecithin-cholesterol (4 : 1) multilayers. Other resonance-enhanced vibrations of amphotericin B exhibit similar behavior. For amphotericin B in pure dimyristoyl lecithin multilayer or vesicle systems, however, the vibrational intensity associated with the C  C stretching mode remains constant during the melting of lipid hydrocarbon chains. In addition, a third effect occurs in liquid crystalline egg lecithin-cholesterol (4 : 1, mol ratio) multilayers in which I₁₅₅₆ first increases by 25% between 3 and 25°C, in parallel with the loss of active channels, and then remains constant as the temperature increases from 25 to 42°C. This latter intensity pattern is masked in the dimyristoyl lecithin-cholesterol system by the overwhelming effect upon the C  C mode from changes in the lipid chain packing characteristics which occur during the phase transition.The broadened phase transition in 4 : 1 dimyristoyl lecithin-cholesterol multilayers (16–32°C), as followed by the ratio of intensities at 2880 and 2850 cm^?1 (asymmetric and symmetric methylene C-H stretching modes, respectively) is slightly narrowed by the addition of amphotericin B, and effect from which a binding stoichiometry at 24° of 1 : 1 amphotericin B : cholesterol is estimated. This stoichiometry was confirmed by differential calorimetric scans, which also show the presence of a peak proportional to cholesterol content.Raman I_2880/2850 peak height ratios in pure dimyristoyl lecithin bilayers were increased over the 14–38°C range by amphotericin B, a spectral effect which suggests an ordering of the lipid matrix perhaps as a consequence of the polyene binding to the bilayer surface. For bilayers containing cholesterol, the ratios of intensities of the 2935 cm^?1 feature, composed mainly of acyl chain terminal methyl and underlying methylene C-H stretching modes, to the 2850 cm^?1 feature are significantly increased by amphotericin B. This effect indicates that the antibiotic penetrates the bilayer in the lipid-sterol system.     

Vibrational spectroscopic analysis of LD-sequential, bacterial cell wall peptides: an IR and Raman study

The synthetic, zwitterionic bacterial cell wall peptides—D -Glu^γ-L-Lys, D -Glu^γ-L-Lys-D -Ala, D -Glu^γ-L-Lys-D -Ala-D -Ala, and L-Ala-D -Glu^γ-L-Lys-D -Ala-D -Ala—have been investigated in the crystalline and aqueous solution state applying ir and Raman spectroscopy. Additionally, aqueous solutions of the tetra- and pentapeptide have been investigated by CD spectroscopic techniques. Apart from the dipeptide, whose spectral features were dominated by end-group vibrations, the corresponding ir and Raman active bands of the crystalline peptides in the amide and skeletal regions were found at similar wave numbers, thus suggesting an analogous three-dimensional structure of these compounds. Dominant amide A, I, II, and III bands near 3275, 1630, 1540, and 1220–1250 cm^?1, respectively, in the ir are interpreted in favor of an intermolecularly hydrogen-bonded, β-like structure. The absence of any amide components near 1680–1690 cm^?1, together with the presence of strong amide bands near 1630 cm^?1, and weak bands near 1660 cm^?1 in the ir, which, conversely, were found in the Raman spectra as weak and strong bands, but at corresponding wave numbers, is taken as strong evidence for the presence of the unusual, parallel-arranged β-structure. On the basis of comparative theoretical considerations, a parallel-arranged, “β-type ring” conformation [P. De Santis, S. Morosetti, and R. Rizzo (1974) Macromolecules 7 , 52–58] is hypothesized. The solubilized peptides exhibited distinct similarities with their crystalline counterparts in respect to frequency values and relative intensities of the corresponding ir and Raman-active amide I/I′ components, and of some Raman bands in the skeletal region. This is interpreted in terms of residual short-range order, persisting even in aqueous solution. We concluded that the peptides show a strong propensity to form hydrated, strongly associated aggregates in water. On the basis of amide I/I′ band positions, stable, intramolecular interactions via the amide groups are discarded for the solubilized peptides. Complementarily, the CD data obtained suggest the presence of weakly bent, “open-turn”-like structures for the tetra- and pentapeptide in aqueous solution.     

Cationic amphiphiles and the solubilization of cholesterol crystallites in membrane bilayers

Cationic amphiphiles used for transfection can be incorporated into biological membranes. By differential scanning calorimetry (DSC), cholesterol solubilization in phospholipid membranes, in the absence and presence of cationic amphiphiles, was determined. Two different systems were studied: 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) + cholesterol (1:3, POPC:Chol, molar ratio) and 1-palmitoyl-2-oleoyl-sn-glycero-3-[phospho-l-serine] (POPS) + cholesterol (3:2, POPS:Chol, molar ratio), which contain cholesterol in crystallite form. For the zwitterionic lipid POPC, cationic amphiphiles were tested, up to 7 mol%, while for anionic POPS bilayers, which possibly incorporate more positive amphiphiles, the fractions used were higher, up to 23 mol%. 1,2-dioleoyl-3-trimethylammonium-propane (DOTAP) and DOTAP in methyl sulfate salt form (DOTAP^mss) were found to cause a small decrease on the enthalpy of the cholesterol transition of pure cholesterol aggregates, possibly indicating a slight increase on the cholesterol solubilization in POPC vesicles. With the anionic system POPS:Chol, the cationic amphiphiles dramatically change the cholesterol crystal thermal transition, indicating significant changes in the cholesterol aggregates. For structural studies, phospholipids spin labeled at the 5th or 16th carbon atoms were incorporated. In POPC, at the bilayer core, the cationic amphiphiles significantly increase the bilayer packing, decreasing the membrane polarity, with the cholesterol derivative 3β-[N-(N′,N′-dimethylaminoethane)-carbamoyl]-cholesterol (DC-chol) displaying a stronger effect. In POPS and POPS:Chol, DC-chol was also found to considerably increase the bilayer packing. Hence, exogenous cationic amphiphiles used to deliver nucleic acids to cells can change the bilayer packing of biological membranes and alter the structure of cholesterol crystals, which are believed to be the precursors to atherosclerotic lesions.     

Raman spectroscopic study of the valinomycin--KSCN complex

This paper reports the first Raman spectroscopic study of the potassium complex of the cation-specific antibiotic valinomycin. Complete Raman spectra (140 to 3600 cm^?1) of crystalline valinomycin-KSCN and its CCl₄, CHCl₃ and C₂H₅OH solutions are presented and used to probe the structure of the complex in these environments. In all cases a single, narrow peak is observed in the ester CO stretch region (1750 to 1775 cm^?1) which contrasts strongly with the broad bands observed in solutions of uncomplexed valinomycin. This is consistent with the presence of a single conformation in which all six ester CO groups co-ordinate an enclosed potassium ion. We find that although the ester CO stretch frequencies of the complex are similar in the solid state and in non-polar solution (~1770 cm^?1) they are considerably different in the presence of polar solvents (~1756 cm^?1); this may indicate that the complexed potassium ion is still free to interact with nearby solvent ions (and possibly its counterion) through gaps in the hydrophobic “shield” provided by the hydrocarbon residues of valinomycin. In contrast the amide CO frequencies of the complex (~1650 cm^?1) are solvent-independent. These groups are apparently strongly hydrogen-bonded to provide a rather rigid, compact framework for the complex conformation.     

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°C thermal pretransition on the acyl chain intramolecular disordering process, Raman spectra of dipalmitoyl phosphatidylcholine gels at 20 and 34°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°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.     

Phase transitions of phospholipid single-wall vesicles and multilayers. Measurement by vibrational raman spectroscopic frequency differences

Raman spectroscopic frequency differences between selected carbon-carbon stretching modes of lipid hydrocarbon chains were determined as a function of temperature for use in monitoring lipid phase transition behavior and acyl chain disorder in both multilamellar and single-wall vesicles. Transition temperatues detected by this procedure for pure dipalmitoyl phosphatidylcholine and dimyristoyl phosphatidylcholine multilayers were observed at $\text{39±1 °}\text{C}$ and $\text{23±1 °}\text{C}$, respectively. Although the phase transition for unilamellar vesicles of dipalmitoyl phosphatidylcholine occurred at nearly the same temperature as the multilayers, the crystal-liquid crystalline transition for the single-shell vesicles appeared to span a slightly broader temperature range, a characteristic consistent with irregularities in the packing arrangement of the hydrocarbon chains. Within the precision of the Raman spectroscopic method, however, the temperature behavior of both the multilamellar and the unilamellar dimyristoyl phosphatidylcholine assemblies appeared nearly identical. The temperature profile for the Raman frequency differences of an excess water sonicate of 25 mol percent cholesterol in dipalmitoyl phosphatidylcholine served as an example of the effect upon lipid phase transition characteristics of a bilayer component intercalated between the acyl chains. For this particular cholesterol-lipid system the phase transition was broadened over a 30 °C temperature range, in contrast to the narrow 5?4 °C range observed for pure multilayer and single-shell vesicle particles.     

Study of hydrogen bonds in cyrstalline monosaccharides the spectra of monosaccharides derivatives in the middle-and far-infrared regions

The spectra of a series of monosaccharide derivatives in the middle- and far-infrared region were investigated. An explanation is provided for the band shifts in the OH stretching region at 3100–3400 cm^?1 and in the region of hydrogen-bond vibrations at 180–120 cm^?1 under effect of low temperatures. A comparison of i.r., X-ray, and neutronographic data indicates the absence of intramolecular hydrogen-bonds in the crystalline monosaccharide derivatives investigated.     

Synthesis and characterization of bis[salicylideneaminato] palladium(II) complexes. Molecular structure of bis[N-(n-butyl)(3-benzyloxy)-2-salicylideneaminato]-palladium(II), pd(C18H20NO2)2]

Transition metal compounds having liquid crystalline properties can be interesting materials for practical applications. Attempting to correlate mesomorphic properties with molecular structure and crystal packing mode, we have investigated some complexes obtained from Schiff bases of long chain aliphatic amines and salicylaldehyde or 2,3-dihydroxybenzaldehyde derivatives. The X-ray structural analysis of bis[N-(n-butyl)(3-benzyloxy)-2-salicylideneaminato] palladium [II] is also reported.     

Characterization of the ternary mixture of sphingomyelin, POPC, and cholesterol: support for an inhomogeneous lipid distribution at high temperatures

A ternary lipid mixture of palmitoyl-oleoyl-phosphatidylcholine (POPC), palmitoyl-erythro-sphingosylphosphorylcholine (PSM), and cholesterol at a mixing ratio of 37.5:37.5:25 mol/mol/mol was characterized using fluorescence microscopy, ²H NMR, and electron paramagnetic resonance spectroscopy. The synthetic PSM provides an excellent molecule for studying the molecular properties of raft phases. It shows a narrow phase transition at a temperature of 311 K and is commercially available with a perdeuterated sn-2 chain. Fluorescence microscopy shows that large inhomogeneities in the mixed membranes are observed in the coexistence region of liquid-ordered and liquid-disordered lipid phases. Above 310 K, no optically detectable phase separation was shown. Upon decrease in temperature, a redistribution of the cholesterol into large liquid-ordered PSM/cholesterol domains and depletion of cholesterol from liquid-disordered POPC domains was observed by ²H NMR and electron paramagnetic resonance experiments. However, there is no complete segregation of the cholesterol into the liquid-ordered phase and also POPC-rich domains contain the sterol in the phase coexistence region. We further compared order parameters and packing properties of deuterated PSM or POPC in the raft mixture at 313 K, i.e., in the liquid crystalline phase state. PSM shows significantly larger ²H NMR order parameters in the raft phase than POPC. This can be explained by an inhomogeneous interaction of cholesterol between the lipid species and the mutual influence of the phospholipids on each other. These observations point toward an inhomogeneous distribution of the lipids also in the liquid crystalline phase at 313 K. From the prerequisite that order parameters are identical in a completely homogeneously mixed membrane, we can determine a minimal microdomain size of 45-70 nm in PSM/POPC/cholesterol mixtures above the main phase transition of all lipids.     

The effect of cholesterol on the structure of phosphatidylcholine bilayers

The effect of cholesterol on the structure of phosphatidylcholine bilayers was investigated by X-ray diffraction methods. Electron density profiles at 5 Å resolution along with chain tilt and chain packing parameters were obtained and compared for phosphatidylcholine/cholesterol bilayers and for pure phosphatidylcholine bilayers in both the gel and liquid crystalline states. The cholesterol in the bilayer was localized by noting the position of discrete elevations in the electron density profiles. Cholesterol can either increase or decrease the width of the bilayer depending on the physical state and chain length of the lipid before the introduction of cholesterol. For saturated phosphatidylcholines containing 12–16 carbons per chain, cholesterol increases the width of the bilayer as it removes the chain tilt from gel state lipids or increases the trans conformations of the chains for liquid crystalline lipids. However, cholesterol reduces the width of 18 carbon chain bilayers below the phase transition temperature as the long phospholipid chains must deform or kink to accomodate the significantly shorter cholesterol molecule. Although cholesterol has a marked effect on hydrocarbon chain organization, it was found that, within the resolution limits of the data, the phosphatidylcholine head group conformation is unchanged by the addition of cholesterol to the bilayer. The head group is oriented parallel to the plane of the bilayer for phosphatidylcholine in the gel and liquid crystalline states and this orientation is not changed by the addition of cholesterol.     

Raman spectroscopic study of tropomyosin denaturation

Raman spectra of the pH denaturation of tropomyosin are presented. In the native state tropomyosin has an alpha-helical content of nearly 90%, but this value drops rapidly as the pH is raised above 9.5. The Raman spectrum of the native state is characterized by a strong amide I line appearing at 1655 cm^?1, very weak scattering in the amide III region around 1250 cm^?1, and a medium-intensity line at 940 cm^?1. When the protein is pH-denatured, a strong amide III line appears at 1254 cm^?1 and the 940 cm^?1 line becomes weak. The intensities of the latter two lines are a sensitive measure of the alpha-helical and disordered chain content. These results are consistent with the helix-to-coil studies of the polypeptides. The Raman spectra of α-casein and prothrombin, proteins thought to have little or no ordered secondary structure, are investigated. The amide III regions of both spectra display strong lines at 1254 cm^?1 and only weak scattering is observed at 940 cm^?1, features characteristic of the denatured tropomyosin spectrum. The amide I mode of α-casein appears at 1668 cm^?1, in agreement with the previously reported spectra of disordered polypeptides, poly-L -glutamic acid and poly-L -lysine at pH 7.0 and mechanically deformed poly-L -alanine.     

Vibrational Raman optical activity of alanyl peptide oligomers: A new perspective on aqueous solution conformation

The vibrational Raman optical activity (ROA) spectra of di- and tri-L -alanine in the range 650–1750 cm^?1 have been measured in H₂O and D₂O solution at high, neutral, and low pH and pD. Corresponding ROA spectra for tetra- and penta-L -alanine have also been obtained, but over a more restricted set of pH and pD conditions. There are similarities with the ROA spectrum of L -alanine below ～ 1200 cm^?1, but the spectra are very different above this wavenumber due to the influence of the vibrational coordinates of the peptide group. The similar overall appearance of the di-, tri-, and tetrapeptide ROA under selected conditions of pH and pD, and of all four peptide ROA spectra in DCl and HCl solutions, in the backbone skeletal stretch region ～ 1050–1200 cm^?1 and the extended amide III region ～ 1250–1350 cm^?1, suggests that the backbone conformation is approximately the same in all four structures. One difference, however, is a shift of a large positive ROA band in H₂O at ～ 1341 cm^?1 in the dipeptide, assigned to C_α–H and in-plane N–H deformations, down to ～ 1331 cm ^?1 in the tripeptide and to ～ 1315 cm^?1 in the tetrapeptide and pentapeptide (the last in HCl due to insufficient solubility in H₂O), which indicates increasing delocalization of the corresponding normal mode with increasing chain length. Our results do not support the suggestion that stabilizing interactions of the zwitterionic end groups in tri-L -alanine at neutral pH leads to a different solution structure to that at high pH. © 1994 John Wiley & Sons, Inc.     

Electrostatically induced change of the conformational order of charged lipid membranes

Raman spectroscopy and X-ray diffraction are used to investigate the influence of surface charges on the structure of ionizable lipid membranes of dimyristoylmethylphosphatidic acid. The membrane surface charge density is regulated by varying the pH of the aqueous phase. Changes of the conformational order of the lipid chains are determined from the intensity of the CC stretch chain vibrations around 1100 cm^?1 in a lipid Raman spectrum. In going from an electrical neutral to a negatively charged membrane, the conformational order is reduced by 5% in the ordered and by 9% in the fluid membrane phase, corresponding to 0.6 and 0.8 CC bonds, respectively, which change from a trans to a gauche conformation. The electrostatically induced conformational change is mainly concentrated at the lipid chain ends as indicated by the spectral variations of the 890 cm^?1 CH₃ rocking band of the chain termini. The X-ray diffraction experiments show that increasing the surface charge density in the ordered membrane phase leads to a lateral expansion of the packing of the lipid polar groups, whereas the packing of the lipid chains in a plane perpendicular to the chain axes remains constant, indicating an increase of the tilt of the lipid chains from δ = 10° (pH 3) to δ = 27° (pH 9).     

Cationic amphiphiles and the solubilization of cholesterol crystallites in membrane bilayers

Cationic amphiphiles used for transfection can be incorporated into biological membranes. By differential scanning calorimetry (DSC), cholesterol solubilization in phospholipid membranes, in the absence and presence of cationic amphiphiles, was determined. Two different systems were studied: 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC)+cholesterol (1:3, POPC:Chol, molar ratio) and 1-palmitoyl-2-oleoyl-sn-glycero-3-[phospho-l-serine] (POPS)+cholesterol (3:2, POPS:Chol, molar ratio), which contain cholesterol in crystallite form. For the zwitterionic lipid POPC, cationic amphiphiles were tested, up to 7 mol%, while for anionic POPS bilayers, which possibly incorporate more positive amphiphiles, the fractions used were higher, up to 23 mol%. 1,2-dioleoyl-3-trimethylammonium-propane (DOTAP) and DOTAP in methyl sulfate salt form (DOTAPmss) were found to cause a small decrease on the enthalpy of the cholesterol transition of pure cholesterol aggregates, possibly indicating a slight increase on the cholesterol solubilization in POPC vesicles. With the anionic system POPS:Chol, the cationic amphiphiles dramatically change the cholesterol crystal thermal transition, indicating significant changes in the cholesterol aggregates. For structural studies, phospholipids spin labeled at the 5th or 16th carbon atoms were incorporated. In POPC, at the bilayer core, the cationic amphiphiles significantly increase the bilayer packing, decreasing the membrane polarity, with the cholesterol derivative 3 beta-[N-(N',N'-dimethylaminoethane)-carbamoyl]-cholesterol (DC-chol) displaying a stronger effect. In POPS and POPS:Chol, DC-chol was also found to considerably increase the bilayer packing. Hence, exogenous cationic amphiphiles used to deliver nucleic acids to cells can change the bilayer packing of biological membranes and alter the structure of cholesterol crystals, which are believed to be the precursors to atherosclerotic lesions.     

Development of a CP P NMR Broadline Simulation Methodology for Studying the Interactions of Antihypertensive AT1 Antagonist Losartan with Phospholipid Bilayers

A cross-polarization (CP) ³¹P NMR broadline simulation methodology was developed for studying the effects of drugs in phospholipids bilayers. Based on seven-parameter fittings, this methodology provided information concerning the conformational changes and dynamics effects of losartan in the polar region of the dipalmitoylphosphatidylcholine bilayers. The test molecule for this study was losartan, an antihypertensive drug known to exert its effect on AT₁ transmembrane receptors. The results were complemented and compared with those of differential scanning calorimetry, solid-state ¹³C NMR spectroscopy, Raman spectroscopy, and electron spin resonance. More specifically, these physical chemical methodologies indicated that the amphipathic losartan molecule interacts with the hydrophilic-head zone of the lipid bilayers. The CP ³¹P NMR broadline simulations showed that the lipid molecules in the bilayers containing losartan displayed greater collective tilt compared to the tilt displayed by the load-free bilayers, indicating improved packing. The Raman results displayed a decrease in the trans/gauche ratio and increased intermolecular interactions of the acyl chains in the liquid crystalline phase. Additional evidence, suggesting that losartan possibly anchors in the realm of the headgroup, was derived from upfield shift of the average chemical shift σ^iso of the ³¹P signal in the presence of losartan and from shift of the observed peak at 715 cm⁻¹ attributed to C-N stretching in the Raman spectra.     

Evidence for antiferromagnetic exchange coupling in the tetranuclear high potential iron-sulfur protein of Rhodopseudomonas gelatinosa.

EPR spectra of oxidized $\text{R. gelatinosa}$ HiPIP demonstrate two kinds of temperature dependent changes which can be analyzed in terms of an excited state at 142 ± 10cm^?1 and a second excited state at 490 ± 100cm^?1. These states represent further verification of antiferromagnetic exchange among the 4 irons in this tetranuclear cluster, with a value for the coupling constant of J = ?44cm^?1. Aside from resonance Raman spectroscopic results, this is the first report of a ladder of excited states predicted for exchange coupled ions.     

Interaction of cholesterol with synthetic sphingomyelin derivatives in mixed monolayers

To study the structural requirements of the molecular interactions between cholesterol and sphingomyelins in model membranes, sphingomyelin derivatives were synthesized in which (a) the 3-hydroxy group was replaced with a hydrogen atom or with a methoxy, ethoxy, or tetrahydropyranyloxy group, (b) the N-acyl chain length was varied, and (c) the N-acyl chain length contained an alpha-hydroxy group. The chemical syntheses of these derivatives from DL-erythro-sphingosine are reported. The properties of these sphingomyelin derivatives were examined in monolayer membranes at the air/water interface. The mean molecular area of the pure N-stearoylsphingomyelin derivatives was determined, and the effects of cholesterol on the condensation of sphingomyelin packing in the monolayer were recorded. It was observed that replacement of the 3-hydroxy group of sphingomyelin with a hydrogen atom or its substitution with a methoxy or ethoxy group did not affect the ability of cholesterol to condense the molecular packing in monolayers. Even when a bulky tetrahydropyranyloxy group was introduced at the 3-hydroxy position of egg sphingomyelin, cholesterol was still able to condense the molecular packing of this derivative. The condensing effect of cholesterol on derivatives of N-stearoyl-SPMs was significantly larger than the comparable effect observed with 1,2-distearoyl-sn-glycero-3-phosphocholine or 1,2-dipalmitoyl-sn-glycero-3-phosphocholine. Our results with 3-hydroxysphingomyelins having differing N-acyl chain lengths (i.e., N-stearoyl, N-myristoyl, and N-lauroyl), and with 3-hydroxy-N-(alpha-hydroxypalmitoyl)sphingomyelin also indicated that cholesterol was able to induce condensation of the molecular packing.(ABSTRACT TRUNCATED AT 250 WORDS)     

Low-frequency Raman spectra of lysozyme.

New techniques in laser Raman spectroscopy are used to obtain spectra of aqueous solutions of lysozylme for frequency shifts as small as 5 cm^?1. In addition, Raman measurements are made on two crystalline forms of hen egg white lysozyme. The spectra obtained from the solution and from the crystal are found to be similar for frequencies above 100 cm^?1. However, a low-frequency band at 25 cm^?1 observed in crystalline lysozyme is not found in the solution, indicating that this band cannot be attributed to an internal molecular vibration.