Raman spectral evidence for tyrosine coordination of iron in protocatechuate 3,4-dioxygenase.

The Raman spectrum of protocatechuate 3,4-dioxygenase [EC 1.13.11.3] shows four principal resonance-enhanced peaks at 1602, 1503, 1263 and 1171 cm^?1 with 514.5 nm laser excitation. These frequencies are associated with ringmode vibrations of one or more tyrosinate residues coordinated with the Fe(III) at the active site. These data provide the first direct evidence for the identity of a permanent iron ligand in this enzyme. The great similarity in the resonance Raman spectrum of protocatechuate 3,4-dioxygenase with those of iron-transferrins suggests the existence of a class of proteins characterized by Fe(III)-tyrosinate coordination.     

Raman spectrum of protocatechuate dioxygenase from Pseudomonas putida. New low frequency bands.

The Raman spectrum (441.6 nm excitation) of protocatechuate 3,4-dioxygenase (PCD) from Pseudomonas putida shows resonance enhanced bands at 1605, 1504, 1270, 858, and 830 cm^?1 which are due to the p-hydroxyphenyl group of tyrosine coordinated to iron. In addition, we observe strong resonance enhanced bands at 592 and 524 cm^?1 and weak (presumably iron-ligand) vibrations at 465, 423, and 371 cm^?1. Recent publications of the Raman spectrum of PCD from Pseudomonas aeruginosa (Tatsuno $\text{et al}$, J. Am. Chem. Soc. 100, 4614–4615 (1978) and Keyes $\text{et al}$, Biochem. Biophys. Res. Comm. 83, 941–945 (1978) using 488 and 514 nm excitation did not report these bands. Our 441.6 nm excitation Raman spectrum of human serum transferrin, another metalloprotein with an iron-tyrosine linkage, does not show the 592 and 524 cm^?1 bands and has only two very weak bands at about 423 and 364 cm^?1. We discuss several interpretations of these data.     

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.     

Raman spectroscopy characterization of antibody phases in serum

When administered in serum, an efficacious therapeutic antibody should be homogeneous to minimize immune reactions or injection site irritation during administration. Monoclonal antibody (mAb) phase separation is one type of inhomogeneity observed in serum, and thus screening potential phase separation of mAbs in serum could guide lead optimization. However, serum contains numerous components, making it difficult to resolve mAb/serum mixtures at a scale amenable to analysis in a discovery setting. To address these challenges, a miniaturized assay was developed that combined confocal microscopy with Raman spectroscopy. The method was examined using CNTO607, a poorly-soluble anti-interleukin-13 human mAb, and CNTO3930, a soluble anti-respiratory syncytial virus humanized mAb. When CNTO607 was diluted into serum above 4.5 mg/mL, phase separation occurred, resulting in droplet formation. Raman spectra of droplet phases in mixtures included bands at 1240 and 1670 cm^?1, which are typical of mAb β-sheets, and lacked bands at 1270 and 1655 cm^?1, which are typical of α-helices. The continuous phases included bands at 1270 and 1655 cm^?1 and lacked those at 1240 and 1670 cm^?1. Therefore, CNTO607 appeared to be sequestered within the droplets, while albumin and other α-helix-forming serum proteins remained within the continuous phases. In contrast, CNTO3930 formed only one phase, and its Raman spectra contained bands at 1240, 1670, 1270 and 1655 cm,^?1 demonstrating homogeneous distribution of components. Our results indicate that this plate-based method utilizing confocal Raman spectroscopy to probe liquid-liquid phases in mAb/serum mixtures can provide a screen for phase separation of mAb candidates in a discovery setting.     

Protocatechuate 3,4-dioxygenase. Resonance Raman studies of the oxygenated intermediate.

Resonance Raman spectra of protocatechuate 3,4-dioxygenase from Pseudomonas aeruginosa have been investigated during the reaction of the enzyme with substrate and oxygen. It is found that the spectrum of the turned-over enzyme is indistinguishable from that of the resting enzyme in the absence of substrate, and is characterized by resonance-enhanced tyrosinate ring vibrational modes at 1263 and 1174 cm^?1. In the ternary ESO₂ complex, however, the tyrosinate vibrational modes are shifted to 1252 and 1165 cm^?1, respectively. There is no evidence for any dioxygen vibrations in the spectra of ESO₂ complexes prepared with ¹⁶O₂, ¹⁸O₂, and ¹⁶O¹⁸O in the region between 1300 and 200 cm^?1. The results of this resonance Raman study are interpreted to indicate that molecular oxygen is attached only to the substrate (but not iron) in the stable intermediate, and that the concomitant rearrangement at C4 of the substrate induces a substantial change in geometry of the tyrosine residues associated with the iron complex. Furthermore, the optical spectrum of the ESO₂ complex (λ_max = 520 nm) is dominated by tyrosinate → Fe(III) charge transfer and contains little or no peroxide → Fe(III) charge transfer. These results invalidate the previously advanced analogy in spectral properties between this enzyme and the respiratory protein, oxyhemerythrin.     

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.     

Laser-excited raman spectroscopy of biomolecules. XII. Thermally induced conformational changes in poly(L-glutamic acid)

The α-helical from of poly(L -glutamic acid) [α-poly(Glu)] gives rise to the same amide I and III lines as α-poly(γ-benzyl-L -glutamate) at 1652 and 1296 cm^?1, respectively. The latter is a superposition of the amide III line near 1290 cm^?1 and a line deu to vibrational made of CH₂ groups of the side chain near 1300 cm^?1. A line at 924 cm^?1 is tentatively identified as characteristics of α-poly(Glu). Both the β₁- and β₂- forms of poly(Glu) give rise to characteristic of β-amide. III frequencies that are similar because of their similar backbone structures. Differences in the conformations of their side chains and in the environments of the backbone are reflected in the region 800–1200 cm^?1 and in the amide I. A line at 1042 cm^?1 and a pair at 1021 and 1059 cm^?1 are tentatively assigned as characteristic of β₁-poly(Glu) and β₂-poly(Glu), respectively. The α-β₂ transition in poly(L -Glu⁷⁸L -Val²²) is shown by the appearance of all the β₂-characteristic lines in the thermally transformed sample. The same features observed in poly(L -Glu⁹⁵L -Val⁵) also indicate that the α-β₂ transition of poly(Glu) is facilitated by the presence of L -valine and that the content of L -valine is not critical for this purpose. Investigation of the Raman spectra of the calcium, strontium, barium and sodium slats of poly(Glu) shows that these salts, under the conditions of preparation used, all the have random-coil conformations.     

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.     

Ribonucleotide reductase: A structural study of the dimeric iron site

The iron-containing B2 subunit of ribonucleotide reductase from Escherichia coli has been investigated by Raman spectroscopy. Both the tyrosyl radical-containing native protein and the radical-free protein exhibit a resonance-enhanced Raman band at 500 cm^?1. This band is assigned to an Fe-O vibrational mode arising from an oxygen-containing ligand. The failure to observe any tyrosinate ring modes makes it unlikely that ribonucleotide reductase is an iron-tyrosinate protein and rules out tyrosinate oxygen as a ligand. It is proposed that the 500 cm^?1 band in ribonucleotide reductase is analogous to the 510 cm^?1 Fe-O vibrational mode of methemerythrin and arises from an oxo- or carboxylate-bridge between the antiferromagnetically-coupled Fe(III) ions.     

Resonance Raman evidence for Fe(IV) in compound II of horseradish peroxidase

Resonance Raman spectra have been obtained for Compound II of horseradish peroxidase. Its prophyrin vibrational frequencies are consistent with a planar low-spin heme containing Fe(IV). The oxidation-state marker band is found at the unprecedentedly high value of 1382 cm^?1. This band was also observed in solutions of myoglobin and cytochrome c peroxidase to which H₂O₂ had been added. No evidence was found for an actual FeO double bond in Compound II.     

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.     

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.     

Structural investigation of poly d(BrU-A) by ultraviolet resonance raman spectroscopy

The resonance Raman spectra of a DNA containing bromodeoxy-uridine (BrdUrd), the poly d(BrU-A), are reported, using U.V. laser as a source of excitation. The conformational change from the ordered, base paired form of poly d(BrU-A) (at 25°C) to the melted form at high temperature (63°C) is reflected in a pronounced hyperchromism of Raman bands at 1627 cm^?1, 1352 cm^?1 and 1230 cm^?1. Particularly the band at 1627 cm^?1 assigned to the vibrations of C4 carbonyl which is hydrogen bonded to adenine increases strongly its intensity upon melting. This represents a new approach for a detection of base unpairing and of modifications in geometry of selective molecules (BrdUrd) in a DNA chain in dilute solutions (10^?4 M).     

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.     

The Combined Effects of Iron Excess in the Diet and Chromium(III) Supplementation on the Iron and Chromium Status in Female Rats

Inadequate iron supply has significant consequences to health. There are some relations between the metabolism of different trace elements, such as iron, zinc, copper and chromium. However, the direction of these interactions can be antagonistic or synergistic, and it depends on many factors. The aim of the study was to evaluate the combined effects of supplementary of chromium(III) propionate complex (Cr3) with iron excess on the Cr and Fe status in healthy female rats. The 36 healthy female Wistar rats were divided into six experimental groups (six animals in each) with different Fe levels—adequate (45 mg kg^?1—100% RDA) and high (excessive—180 mg kg^?1—400% RDA). At the same time, they were supplemented with Cr(III) at doses of 1, 50 and 500 mg kg^?1 of diet: C1—control (Fe 45 mg kg^?1, Cr 1 mg kg^?1); C50 (Fe 45 mg kg^?1, Cr 50 mg kg^?1); C500 (Fe 45 mg kg^?1, Cr 500 mg kg^?1); H1 (Fe 180 mg kg^?1, Cr 1 mg kg^?1); H50 (Fe 180 mg kg^?1, Cr 50 mg kg^?1); H500 (Fe 180 mg kg^?1, Cr 500 mg kg^?1). The serum iron level and total iron binding capacity (TIBC) were measured with colorimetric methods. The serum ferritin level was measured by means of electrochemiluminescence immunoassay. The serum transferrin level was measured with the ELISA method. Haematological measurements were made with an automated blood analyser. The Cr and Fe tissular levels were measured with the AAS method. The exposure to a high level of Fe(III) alone or in combination with Cr caused Fe accumulation in tissues, especially in the liver and kidneys, but there were no significant changes in the TIBC, transferrin, ferritin concentration in the serum and most haematological parameters. Moreover, the serum, hepatic and renal Cr concentrations decreased. The doses of supplementary Cr(III) given separately or in combination with high level of Fe(III) disturbed the Cr content in the liver and kidneys of healthy female rats. However, they did not change most of the parameters of Fe metabolism, except the Fe kidney concentration. Supplementary Cr3 decreased the renal Fe level in groups with adequate Fe content in the diet. However, the renal Fe levels increased along with a higher Cr level in the diet in groups with high Fe content. The findings proved a relationship between Fe(III) and Cr(III) metabolism in healthy female rats. However, the direction of change varied and depended on relative amounts of these elements in the diet.     

The vibrational spectra and structure of poly(rA-rU)-poly(rA-rU)

Infrared and Raman spectra of aqueous poly(rA-rU)·poly(rA-rU), the double-helical complex containing strands of alternating riboadenylate and ribouridylate residues, display significant differences from one another and from corresponding spectra of poly(rA)·poly(rU), the double-helical complex of riboadenylate and ribouridylate homopolymers. Parallel studies on the copolymer and homopolymer complexes by cesium sulfate density gradient centrifugation, ultraviolet absorption spectroscopy, hydrogenion titration, 1-N oxidation of adenine residues by monoperphthalic acid and X-ray diffraction reveal, however, that the geometry of base pairing between adenine and uracil is closely similar in each complex and apparently of the Watson-Crick type. Therefore the differences observed between vibrational spectra of poly (rA-rU)·poly (rA-rU) and poly(rA)·poly(rU) are not due to different base-pairing schemes but may be attributed to differences in vibrational coupling between vertically stacked bases. Vibrational coupling may also account for the differences between infrared and Raman spectra of the same complex. Thus, the present results indicate that infrared and Raman frequencies of RNA in the region 1750–1550 cm^?1 should be dependent on the base sequence.     

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.     

Quaternary structures and low frequency molecular vibrations of haems of deoxy and oxyhaemoglobin studied by resonance Raman scattering

The influence of quaternary structure on the low frequency molecular vibrations of the haem within deoxyhaemoglobin (deoxy Hb) and Oxyhaemoglobin (oxy Hb) was studied by resonance Raman scattering. The FeO₂ stretching frequency was essentially identical between the high affinity (R) state (Hb A) and low affinity (T) state (Hb Kansas and Hb M Milwaukee with inositol hexaphosphate). However in deoxy Hb, only one of the polarized lines showed an appreciable frequency shift upon switch of quaternary structure, i.e. 215 to 218 cm^?1 for the T state (Hb A, des-His(146β) Hb, and des-Arg(141α) Hb (pH 6.5)) and 220 to 221 cm^?1 for the R state (des-Arg(141α) Hb (pH 9.0), des-His(146β)-Arg(141α) Hb and NES des-Arg(141α) Hb). Based on the observed ⁵⁴Fe isotopic frequency shift of the corresponding Raman lines of deoxy Hb A (214 → 217 cm^?1), of deoxy NES des-Arg Hb (220 → 223 cm^?1), of the protoporphyrinato-Fe(II)-(2-methylimidazole) complex in the ferrous high spin state (207 → 211 cm^?1) and of deoxymyoglobin (220 → 222 cm^?1) (Kitagawa et al., 1979), and on substitution of perdeuterated for protonated 2-methylimidazole in the deoxygenated picket fence complex (T_pivPP)Fe²⁺ (2-MeIm) (209 → 206 cm^?1), and on the results of normal co-ordinates calculation carried out previously, we proposed that the 216 cm^?1 line of deoxy Hb is associated primarily with the FeN_ε(HisF8) stretching mode and accordingly that the FeN_ε(HisF8) bond is stretched in the T state due to a strain exerted by globin.     

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.     

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.