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.     

The Raman spectra of Bence-Jones proteins. Disulfide stretching frequencies and dependence of Raman intensity of tryptophan residues on their environments

The Raman spectra of Bence-Jones proteins (BJP) were measured for their native and denatured states. All of the native BJPs investigated gave amide I at 1670–1675 cm^?1 and amide III at 1242–1246 cm^?1. Although the amide I was shifted to 1667 cm^?1 upon the LiBr, acid, and thermal denaturation, as expected, the amide III frequency was unaltered, indicating that the antiparallel β- and disordered structures of BJP provide amide III at almost the same frequencies. The intensity of the 880-cm^?1 line of native BJP was relatively intense compared with that of amino acid mixed solution in which the mole ratios of Trp, Phe, and Tyr were adjusted to reproduce the corresponding ratios of BJP. However, the intensity was evidently reduced upon LiBr, acid, and thermal denaturation, approaching that of the amino acid mixture. Thus, the intensity of the 880-cm^?1 line is proposed as a practical probe for the environment of Trp residues. The pH dependence of the intensity of the 880-cm^?1 line suggests that one of two buried Trp residues is exposed between pH 4 and 3.2 and the other between pH 3.2 and 1.4. The variable fragment (V_L) of BJP (Tod) exhibited a S? S stretching Raman line at 525 cm^?1. Provided that the crystallographic data of the V_L of BJP is applicable to V_L of BJP (Tod), the 525 cm^?1 of the S? S stretching frequency should be assigned to a TGG conformation of linkage, but not to the AGT or AGG conformation. This supports Sugeta's model rather than Scheraga's model.     

Raman studies of the crystalline, solution, and alkaline-denatured states of beta-lactoglobulin.

The Raman spectra of β-lactoglobulin in the crystalline, freeze-dried, and solution states are compared. The spectra of the freeze-dried and crystalline proteins were practically identical. The conformationally sensitive amide III line appearing at 1242 cm^?1 increased in intensity 30% upon dissolution of the protein in water which is interpreted as a conformational change in the disordered chains of the protein. This result appears to be a phenomenon for globular proteins containing a large disordered chain fraction. The alkaline denaturation of β-lactoglobulin was studied. When the pH was increased from 6.0 to 11.0, the amide III line shifted from 1242 to 1246 cm^?1, broadened, and decreased in intensity. This is consistent with the conversion of β-sheet regions in β-lactoglobulin to the disordered conformation, as has been proposed by other investigators. At pH 13.5 the amide III shifts to 1257 cm^?1 characteristic of a completely disordered protein, indicating that any remaining “core” of β-sheet has been randomized. Several changes in the intensities of the tyrosine and tryptophan vibrations accompany the denaturation. As the pH is increased from 6.0 (native state) to 11.0 (denatured state) the intensity ratio of two tyrosine ring vibrations, I₈₅₅ cm^?1/I₈₃₀ cm^?1, decreases from 1.0:0.9 to 1.0:1.3. The same ratio for a copolymer consisting of 95% glutamic acid and 5% tyrosine at pH 7.0, where the polymer forms a random coil exposing the tyrosine to the aqueous environment, is 1.0:0.62. This ratio more closely resembles that corresponding to β-lactoglobulin at pH 6.0 (native state) than pH 11.0 (denatured state) suggesting that the average tyrosine in the denatured state may be in a more hydrophobic environment than in the native state. A time-dependent polymerization of the denatured protein reported by other investigators and observed by us may account for the change in the tyrosine environment. A tryptophan vibration appearing at 833 cm^?1 in the spectrum of the native state becomes weak as the pH is increased to 11.0. The intensity of this line may also reflect the local environment of the tryptophan residue.     

Raman scattering of collagen, gelatin, and elastin.

The Raman spectra of collagen, gelatin, and elastin are presented. The Raman lines in the latter two spectra are assigned by deuterating the amide N-H groups in gelatin and by studying the superposition spectra of the constituent amino acids. Two lines appear at 1271 and 1248 cm^?1 in the spectra of collagen and gelatin that can be assigned to the amide III mode. Possibly, the appearance of two amide III lines is related to the biphasic nature of the tropocollagen molecule, i.e., proline-rich (nonpolar) and proline-poor (polar) regions distributed along the chain. The melting, or collagen-to-gelatin transition, in water-soluble calf skin collagen is studied and the 1248-cm^?1 amide III line is assigned to the 3₁ helical regions of the tropocollagen molecule. Elastin is thought to be mostly random and the Raman spectrum confirms this assertion. Strong amide I and III lines appear at 1668 and 1254 cm^?1, respectively, and only weak scattering is observed at 938 cm^?1. These features have been shown to be characteristic of the disordered conformation in proteins.     

Effect of Mid-infrared Free-Electron Laser Irradiation on Refolding of Amyloid-Like Fibrils of Lysozyme into Native Form

Aggregation of lysozyme in an acidic solution generates inactive amyloid-like fibrils, with a broad infrared peak appearing at 1,610?C1,630?cm^?1, characteristic of a ??-sheet rich structure. We report here that spontaneous refolding of these fibrils in water could be promoted by mid-infrared free-electron laser (mid-IR FEL) irradiation targeting the amide bands. The Fourier transform infrared spectrum of the fibrils reflected a ??-sheet content that was as low as that of the native structure, following FEL irradiation at 1,620?cm^?1 (amide I band); both transmission-electron microscopy imaging and Congo Red assay results also demonstrated a reduced fibril structure, and the enzymatic activity of lysozyme fibrils recovered to 70?C90?% of the native form. Both irradiations at 1,535?cm^?1(amide II band) and 1,240?cm^?1 (amide III band) were also more effective for the refolding of the fibrils than mere heating in the absence of FEL. On the contrary, either irradiation at 1,100 or 2,000?cm^?1 afforded only about 60?% recovery of lysozyme activity. These results indicate that the specific FEL irradiation tuned to amide bands is efficient in refolding of lysozyme fibrils into native form.     

A resonance Raman study on the interaction of rifampicin with Escherichia coli RNA polymerase

The technique of resonance Raman spectroscopy has been used to investigate the interaction of the antibiotic rifampicin with Escherichia coli RNA polymerase. Spectra were analyzed by generating the first derivative of each recorded spectrum using the Savitsky-Golay algorithm. The only band that shifted significantly in the resonance Raman spectrum of rifampicin upon the formation of the drug-core polymerase complex was the amide III band. It underwent an 8 cm^?1 shift from 1306 cm^?1 in aqueous solution to 1314 cm^?1. A comparable shift was observed for the rifampicin-holoenzyme complex. Thus, the interaction of the sigma subunit with the core polymerase does not significantly alter the manner in which rifampicin interacts with RNA polymerase. The nature of this shift has been analyzed further by recording the resonance Raman spectrum of rifampicin in a variety of solvents with different hydrogen-bonding ability. In non-hydrogen-bonding solvents (benzene and carbon disulfide) the amide III band was observed at approximately 1220 cm^?1; in dimethyl sulfoxide, a weak hydrogen-bond acceptor, 1274 cm^?1; in water, a strong hydrogen-bonding solvent, 1306 cm^?1; and finally, in triethylamine, a stronger hydrogen-bonding solvent than water, it was observed at 1314 cm^?1. Thus, as the hydrogen-bonding ability of the solvent increased, the amide III band shifted to higher frequency. Based on these results, the rifampicin binding site in RNA polymerase provides a stronger hydrogen-bonding environment for the amidic proton of rifampicin than is encountered when rifampicin is free in aqueous solution.     

Raman spectroscopic study of mechanically deformed poly-L-alanine

Raman spectroscopy has been used in investigating the conformational transitions of poly-L -alanine (PLA) induced by mechanical deformation. We see evidence of the alpha-helical, antiparallel beta-sheet, and a disordered conformation in PLA. The disordered conformation has not been discussed in previous infrared and X-ray diffraction investigations and may have local order similar to the left-handed 3₁ poly glycine helix. The amide III mode in the Raman spectrum of PLA is more sensitive than the amide I and II modes to changes in secondary structure of the polypeptide chain. Several lines below 1200 cm^?1 are conformationally sensitive and may generally be useful in the analysis of Raman spectra of proteins. A line at 909 cm^?1 decreases in intensity after deformation of PLA. In general only weak scattering is observed around 900 cm^?1 in the Raman spectra of antiparallel beta-sheet polypeptides. The Raman spectra of the amide N–H deuterated PLA and poly-L -leucine (PLL) in the alpha-helical conformation and poly-L -valine (PLV) in the beta-sheet conformation are presented. Splitting is observed in the amide III mode of PLV and the components of this mode are assigned. The Raman spectrum of an alpha-helical random copolymer of L -leucine and L -glutamic acid is shown to be consistent with the spectra of other alphahelical polypeptides.     

Vibrational analysis of peptides,polypeptides, and proteins. VI. Assignment of β-turn modes in insulin and other proteins

The normal modes have been calculated for structures having the dihedral angles of the four β-turns of insulin. Frequencies are predicted in the amide I region near 1652 and 1680 cm^?1. The former overlaps the α-helix band at 1658 cm^?1 in the Raman spectrum, while the latter accounts for the hitherto unassignable band at 1681 cm^?1. Calculated amide III frequencies extend above 1300 cm^?1, providing a compelling assignment of the 1303-cm^?1 band in insulin and similar bands in other globular proteins.     

Raman spectroscopic study of the proteins of egg white

The Raman spectra of ovalbumin, ovomucoid, and conalbumin are reported. Spectral shifts in the conformationally sensitive amide I and amide III lines as a result of thermal denaturation indicate the formation of intermolecular β- sheets. A medium intensity line at 1260 cm^?1 in the spectra of ovomucoid and ribonuclease is demonstrated to contain a substantial contribution from tyrosine residues.     

Raman scattering of chymotrypsinogen A, ribonuclease, and ovalbumin in the aqueous solution and solid state

The Raman spectra of three globular proteins, beef pancreas chymotrypsinogen A, beef pancreas ribonuclease, and hen egg white ovalbumin have been obtained in the solid state and aqueous solution. X-ray diffraction and circular dichroism evidence have indicated that these proteins have a low α-helical content and a large fraction of the residues in the unordered and β-sheet conformation. The frequencies and intensities of the amide I and amide III lines are consistent with assignments based on the Raman spectra of polypeptides. The intense amide III lines observed in all the spectra would be expected for proteins with a low fraction of the residues in the α-helical conformation. Several spectra changes occur upon dissolution of the proteins in water and may be associated with further hydration of the proteins. The spectrum of thermally denatured chymotrypsinogen is presented. A 3 cm^–1 decrease in the frequency of the amide I line of the protein dissolved in D₂O upon heating was observed. This observation is consistent with a denaturation mechanism allowing only slight changes in the secondary structure but an increase in solvent penetration upon going from the native to the reversibly denatured state.     

Raman spectroscopic investigations of sarcoplasmic reticulum membranes

Raman spectra are presented for sarcoplasmic reticulum membranes. Interpretation of the 1000–1130 cm^?1 region of the spectrum indicates that the sarcoplasmic reticulum membrane may be more fluid than erythrocyte membranes that have been examined by the same technique. The fluidity of the membrane also manifests itself in the amide I portion of the membrane spectrum with a strong 1658 cm^?1 band characteristic of CC stretching in hydrocarbon side chains exhibiting cis conformation. This band is unaltered in intensity and position in H₂O and in ²H₂O thus obscuring amide I protein conformation. Of particular interest is the appearance of strong, resonantly enhanced bands at 1160 and 1527 cm^?1 attributable to membrane-associated carotenoids.     

Raman spectra of chemically modified lysozyme. Oxindole derivatives.

The Raman spectra of oxidation products of lysozyme have been investigated. The protein was oxidized by N-bromosuccinimide and dimethyl sulfoxide/HCl. Depending on the experimental conditions one to six tryptophan residues are oxidized to oxindole. The most prominent difference between the spectra of lysozyme and its oxindole derivatives is the strong band at 1017 cm^?1 which displaces the tryptophan peak at 1010 cm^?1. Other tryptophan bands are also weakened corresponding to the number of the tryptophan side chains destroyed. Shifts are observed in the amide I and in the amide III regions sensitive to conformational changes. These shifts indicate conformational differences in the higher oxidized species and in the native enzyme, although the amide III maxima overlap with a strong oxindole band. Similar effects are observed in the range of the C-C stretching vibrations of the peptide backbone. If more than one tryptophan side chain is oxidized changes have also been found in the S-S stretching range. The evaluation of this effect is difficult because of the strong oxindole vibration appearing in this region. In species oxidized by great excess of N-bromosuccinimide the tyrosine vibrations can no longer be detected, indicating the modification of this amino acid too.     

The structural analysis of three‐dimensional fibrous collagen hydrogels by raman microspectroscopy

To investigate molecular effects of 1‐Ethyl‐3‐(3‐dimethylaminopropyl) carbodiimide (EDC), EDC/N‐hydroxysuccinimide (NHS), glyceraldehyde cross‐linking as well as polymerization temperature and concentration on the three‐dimensional (3D) collagen hydrogels, we analyzed the structures in situ by Raman microspectroscopy. The increased intensity of the 814 and 936 cm^?1 Raman bands corresponding to the C—C stretch of a protein backbone and a shift in the amide III bands from 1241 cm^?1/1268 cm^?1 in controls to 1247 cm^?1/1283 cm^?1 in glyceraldehyde‐treated gels indicated changes to the alignment of the collagen molecules, fibrils/fibers and/or changes to the secondary structure on glyceraldehyde treatment. The increased intensity of 1450 cm^?1 band and the appearance of a strong peak at 1468 cm^?1 reflected a change in the motion of lysine/arginine CH₂ groups. For the EDC‐treated collagen hydrogels, the increased intensity of 823 cm^?1 peak corresponding to the C—C stretch of the protein backbone indicated that EDC also changed the packing of collagen molecules. The 23% decrease in the ratio of 1238 cm^?1 to 1271 cm^?1 amide III band intensities in the EDC‐modified samples compared with the controls indicated changes to the alignment of the collagen molecules/fibrils and/or the secondary structure. A change in the motion of lysine/arginine CH₂ groups was detected as well. The addition of NHS did not induce additional Raman shifts compared to the effect of EDC alone with the exception of a 1416 cm^?1 band corresponding to a COO^? stretch. Overall, the Raman spectra suggest that glyceraldehyde affects the collagen states within 3D hydrogels to a greater extent compared to EDC and the effects of temperature and concentration are minimal and/or not detectable. © 2012 Wiley Periodicals, Inc. Biopolymers 99: 349–356, 2013.     

Laser Raman scattering of cobramine B, a basic protein from cobra venom

Cobramine B, a small basic protein from cobra venom, is selected as a model for studying the scattering intensity of tyrosyl ring vibrations in the Raman spectra of proteins. All three tyrosines in this protein appear to be “buried” in the interior of the molecule and probably involved in interactions which are similar to those of the three “buried” tyrosines in RNase A when it is dissolved in water. Spectral evidence is presented and discussed. The Raman spectra in the 300–1800 cm^?1 region of cobramine B in the solid and solution are compared quantitatively. Several differences exist between the two spectra and may be interpreted in terms of difference in conformation. In the amide I region, a strong single line was observed at 1672 cm^?1 both in the solid and solution spectra, suggesting that this protein may contain a large fraction of antiparallel-β structure. This is supported by the presence of a line at 1235 cm^?1 in the amide III region, which is also characteristic of β-structure. The resolved peaks at 1254 and 1270 cm^?1 indicate the coexistence of some hydrogen-bonded random-coil and some α-helix with the β-structure.     

Raman spectroscopic study of poly (β-benzyl-L-aspartate) and sequential polypeptides

Poly-β-benzyl-L -aspartate (poly[Asp(OBzl)]) forms either a lefthanded α-helix, β-sheet, ω-helix, or random coil under appropriate conditions. In this paper the Raman spectra of the above poly[Asp(OBzl)] conformations are compared. The Raman active amide I line shifts from 1663 cm^?1 to 1679 cm^?1 upon thermal conversion of poly[Asp(OBzl)] from the α-helical to β-sheet conformation while an intense line appearing at 890 cm^?1 in the spectrum of the α-helix decreases in intensity. The 890 cm^?1 line also displays weak intensity when the polymer is dissolved in chloroform–dichloroacetic acid solution and therefore is converted to the random coil. This line probably arises from a skeletal vibration and is expected to be conformationally sensitive. Similar behavior in the intensity of skeletal vibrations is discussed for other polypeptides undergoing conformational transitions. The Raman spectra of two cross-β-sheet copolypeptides, poly(Ala-Gly) and poly(Ser-Gly), are examined. These sequential polypeptides are model compounds for the crystalline regions of Bombyx mori silk fibroin which forms an extensive β-sheet structure. The amide I, III, and skeletal vibrations appeared in the Raman spectra of these polypeptides at the frequencies and intensities associated with β-sheet homopolypeptides. Since the sequential copolypeptides are intermediate in complexity between the homopolypeptides and the proteins, these results indicate that Raman structure–frequency correlations obtained from homopolypeptide studies can now be applied to protein spectra with greater confidence. The perturbation scheme developed by Krimm and Abe for explaining the frequency splitting of the amide I vibrations in β-sheet polyglycine is applied to poly(L -valine), poly-(Ala-Gly), poly(Ser-Gly), and poly[Asp(OBzl)]. The value of the “unperturbed” frequency, V₀, for poly[Asp(OBzl)] was significantly greater than the corresponding values for the other polypeptides. A structural origin for this difference may be displacement of adjacent hydrogen-bonded chains relative to the standard β-sheet conformation.     

Comparison of protein structure in crystals and in solution by laser raman scattering. I. Lysozyme

The laser Raman-scattering technique was employed to examine the question of whether the structure of a globular protein is the same in crystals as in solution. Lysozyme was selected as a model system for this study. In the amide I and amide III regions we found a good agreement between the Raman spectra of lysozyme chloride crystals (in 100% relative humidity) and lysozyme solution (at pH 4.50), indicating that the main-chain conformation is the same between two phases. However, small but definite spectral differences were observed near 464, 622, 644, 934, 960, 978, 1032, 1129, and 1196 cm^?1. Some of these spectral differences may be interpreted in terms of side-chain conformational changes. Additionally, we present Raman spectrum of lysozyme in the lyophilized form and compare it to those of crystals and solution. It was concluded that lyophilization caused conformational changes appreciably, both in the main chain and side chain.     

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.     

Far-infrared spectra of some globular proteins

The far-infrared absorption spectrum (40–400 cm^?1) of solid pellets and films of several globular proteins (lysozyme, myoglobin, hemoglobin, serum albumin, ribonuclease, chymotrypsinogen, subtilisin) and of some representative polypeptides [nylon 66, poly (γ-benzyl L -glutamate)] have been investigated by using a Michelson interferometer. While polypeptides are known to present several peaks which can be assigned mostly to hydrogen-bond modes, all the investigated globular proteins display only one broad, intense baud in the 100–200 cm^?1 region. The origin of this band, which persists even after denaturation or partial digestion, is discussed.     

Laser Raman spectra of glucagon

Laser Raman spectroscopy study indicates that in concentrated fresh acidic solution (30 mg/ml), glucagon remains predominantly α-helix and not random-coil. The splitting of the amide III band into three components in the crystal at 1262, 1275, and 1295 cm^?1 is due to the α-conformation as expected. The presence of a small fraction of β-conformation is demonstrated by the appearance of the weak band at 1230 cm^?1 in the fresh solution. This study also established the frequencies of amide III′ bands for the α- and β-conformations of glucagon: 957 and 988 cm^?1 for α and β forms, respectively. The conformations of acidic and basic glucagon solutions are apparently different.     

The conformation of polycytidylic acid, polyguanylic acid, polyinosinic acid, and their helical complexes in aqueous solution from laser Raman scattering

The Raman spectra of the double helical complexes of poly C–poly G and poly I–poly C at neutral p^H are presented and compared with the spectra of the constituent homopolymers. When a completely double-helical structure is formed in solution a strong sharp band at 810–814 cm^?1 appears which has previously been shown to be due to the A-type conformation of the sugar–phosphate backbone chain. By taking the ratio of the intensity of the 810–814 cm^?1 band to the intensity of the 1090–1100 cm^?1 phosphate vibration, one can obtain an estimate of the fraction of the backbone chain in the A-type conformation for both double-stranded helices and self-stacked single chains. This type of information can apparently only be obtained by Raman spectroscopy. In addition, other significant changes in Raman intensities and frequencies have been observed and tabulated: (1) the Raman intensity of certain of the ring vibrations of guanine and hypoxanthine bases decrease as these bases become increasingly stacked (Raman hypochromism), (2) the Raman band at 1464 cm^?1 in poly I is asigned to the amide II band of the cis-amide group of the hypoxanthine base. It shifts in frequency upon base pairing to 1484 cm^?1, thus permitting the determination of the fraction of I–C pairs formed.