Resonance Raman investigation of CO-ligated monomeric insect hemoglobins. Direct evidence for reciprocal changes in iron-axial ligand bonds induced by allosteric transitions

The resonance Raman spectra of the two affinity states of the CO-ligated monomeric insect hemoglobins, Chironomus thummi thummi (CTT) III ad IV, have been investigated. We have identified (via 54Fe/57Fe and 13C18O/12C16O isotope exchange) the Fe-N epsilon(His) stretching mode at approximately 317 cm-1. This stretching mode changes from 329 (pH 5.5) to 317 cm-1 (pH 9.5) reflecting the pH-induced t in equilibrium with r conformational transition. The Fe-CO stretching mode is also pH-sensitive changing from 483 (pH 5.2) to 485 cm-1 (pH 9.2) in 57Fe CTT III . 13C18O complex. However the C-O stretching mode is pH-insensitive. The nonallosteric monomeric insect hemoglobin CTT I does not exhibit a pH-dependence of these vibrational modes. pH-Induced effects were also observed for a vinyl bending mode at 379 cm-1 (pH 9.5) in CTT III deuterated at the beta-carbons of the vinyls in position 2 and 4. It shifts to 390 cm-1 at pH 5.5. The other vinyl vibration at 573 cm-1 exhibits intensity enhancement via through-space coupling with the Fe-C-O bending mode. Our resonance Raman data provide the first direct evidence that the trans-effect is operative as a trigger mechanism for ligand-binding in monomeric allosteric insect hemoglobins. In going from the low-affinity to the high-affinity state, the Fe-N epsilon(His) bond becomes weaker, whereas the Fe-CO bond becomes stronger.     

Resonance Raman assignment and evidence for noncoupling of individual 2- and 4-vinyl vibrational modes in a monomeric cyanomethemoglobin

We have investigated the resonance Raman spectra of monomeric insect cyanomethemoglobins (CTT III and CTT IV) reconstituted with (1) protohemes IX selectively deuterated at the 4-vinyl as well as the 2,4-divinyls, (2) monovinyl-truncated hemes such as pemptoheme (2-hydrogen, 4-vinyl) and isopemptoheme (2-vinyl, 4-hydrogen), (3) symmetric hemes such as protoheme III (with 2- and 3-vinyls) and protoheme XIII (with 1- and 4-vinyls), and (4) hemes without 2- and 4-vinyls such as mesoheme IX, deuteroheme IX, 2,4-dimethyldeuteroheme IX, and 2,4-dibromodeuteroheme IX. Evidence is presented that the highly localized vinyl C = C stretching vibrations at the 2- and 4-positions of the heme in these cyanomet CTT hemoglobins are noncoupled and inequivalent; i.e., the 1631- and 1624-cm-1 lines have been assigned to 2-vinyl and 4-vinyl, respectively. The elimination of the 2-vinyl (in pemptoheme) or the 4-vinyl (in isopemptoheme) does not affect the C = C stretching frequency of the remaining vinyl. Furthermore, two low-frequency vinyl bending modes at 412 and 591 cm-1 exhibit greatly different resonance Raman intensities between 2-vinyl and 4-vinyl. The observed intensity at 412 cm-1 is primarily derived from 4-vinyl, whereas the 591-cm-1 line results exclusively from the 2-vinyl. Again, there is no significant coupling between 2-vinyl and 4-vinyl for these two bending modes.     

Bohr effect in monomeric insect haemoglobins controlled by O2 off-rate and modulated by haem-rotational disorder

The monomeric insect (Chironomus thummi thummi) haemoglobins CTT III and CTT IV show an alkaline Bohr effect. The amplitude of the Bohr effect curve of CTT IV is about twice as large as that of CTT III. In particular, at low pH a time-dependent 'slow' decrease in p50 upon cyclic oxygenation/deoxygenation is observed which is larger if dithionite, instead of ascorbate, is the reducing agent. The decrease of p50 (increase in affinity) correlates with the ratio of haem-rotational components exhibiting an increase of the 'myoglobin-like' haem-rotational component with high O2 affinity and high stability of the globin-haem complex. The replacement of protohaem IX by mesohaem IX and deuterohaem IX, respectively, causes an increase in O2 affinity following the order: proto less than meso less than deutero CTT Hbs. The Bohr effect, however, seems not to be affected by these porphyrin side-group substitutions. The O2 affinity is modulated by steric effects due to the substituents in position 2 and 4 via variation of the protein-haem interactions which influence the O2 release. The replacement of iron by cobalt in proto and meso CTT IV leads to an increase of the p50 by two to three orders of magnitude. Neither central metal nor vinyl replacement affect the Bohr effect. The natural CTT Hbs III and IV analyzed for mono-componential kinetic systems exhibit pH-dependent O2 off-rate constants: 300 s-1 (at pH 5.6) and 125 s-1 (at pH 9.7) for CTT III, and 550 s-1 (at pH 5.4) and 100 s-1 (at pH 9.0) for CTT IV. Inflection points and amplitudes of the log koff/pH plots correspond to those obtained from the Bohr effect curves indicating again a larger Bohr effect for CTT IV than for CTT III. In contrast, the O2 on-rate constants are pH-independent (kon = 1.15-1.26 X 10(8) M-1 s-1). Thus, the Bohr effect is completely controlled by the off-rate constants. Analysis for bi-componential kinetic systems employing the eigenfunction expansion method clearly identifies two kinetic components for proto-IX and deutero-IX CTT Hbs which can be attributed to the two haem-rotational components x and y (x and y differ due to an 180 degree rotation of the haem group about the alpha,gamma-meso axis; y is the myoglobin-like haem-rotational component).(ABSTRACT TRUNCATED AT 400 WORDS)     

Iron-histidine stretching vibration in the deoxy state of insect hemoglobins with different O2 affinities and Bohr effects

Resonance Raman spectroscopy has been employed to detect the iron-proximal histidine stretching mode in deoxyhemoglobins from insect larvae of Chironomus thummi thummi (CTT). With the excitation of 413.1 nm, we observe a sharp and intense line in the 220-224 cm-1 region. The assignment of this line to the Fe-N epsilon (His) stretching mode was made on the basis of a 3-cm-1 shift upon 57Fe/54Fe isotope substitution. The Fe-N epsilon (His) vibration is used to monitor the possible changes in the Fe-N epsilon (His) bond strength (hence bone length) in the deoxy state of the monomeric (CTT I, III, and IV) and dimeric (CTT II) insect hemoglobins. As these hemoglobins differ in O2 affinity, off-rate and on-rate constants, and in the Bohr effect, they are excellent model systems for investigating the mechanism of protein control of the heme reactivity. Some of these hemoglobins (CTT III, IV, and II) are allosteric, exhibiting two interconvertible conformational states with high and low O2 affinity at high and low pH, respectively. The Fe-N epsilon (His) stretching frequency does not correlate with the O2 affinity, the on-rate and the off-rate constants for different hemoglobins, for different conformational states, and for modified hemoglobins with different heme peripheral groups. This vibrational mode is insensitive to deuteration of the heme vinyl groups. It is important to note that the Fe-N epsilon (His) bonds in the high pH (high-affinity) and the low pH (low-affinity) states are identical. This implies that the O2 molecule, prior to binding, "sees" identical binding sites. Thus, the difference in free energy changes upon O2 binding is manifested only in the oxy form.     

Geometries and electronic structures of cyanide adducts of the non-heme iron active site of superoxide reductases: vibrational and ENDOR studies

We have added cyanide to oxidized 1Fe and 2Fe superoxide reductase (SOR) as a surrogate for the putative ferric-(hydro)peroxo intermediate in the reaction of the enzymes with superoxide and have used vibrational and ENDOR spectroscopies to study the properties of the active site paramagnetic iron center. Addition of cyanide changes the active site iron center in oxidized SOR from rhombic high-spin ferric (S = 5/2) to axial-like low-spin ferric (S = 1/2). Low-temperature resonance Raman and ENDOR data show that the bound cyanide adopts three distinct conformations in Fe(III)-CN SOR. On the basis of 13CN, C15N, and 13C15N isotope shifts of the Fe-CN stretching/Fe-C-N bending modes, resonance Raman studies of 1Fe-SOR indicate one near-linear conformation (Fe-C-N angle approximately 175 degrees) and two distinct bent conformations (Fe-C-N angles <140 degrees). FTIR studies of 1Fe-SOR at ambient temperatures reveals three bound C-N stretching frequencies in the oxidized (ferric) state and one in the reduced (ferrous) state, indicating that the conformational heterogeneity in cyanide binding is a characteristic of the ferric state and is not caused by freezing-in of conformational substates at low temperature. 13C-ENDOR spectra for the 13CN-bound ferric active sites in both 1Fe- and 2Fe-SORs also show three well-resolved Fe-C-N conformations. Analysis of the 13C hyperfine tensors for the three substates of the 2Fe-SOR within a simple heuristic model for the Fe-C bonding gives values for the Fe-C-N angles in the three substates of ca. 123 degrees (C3) and 133 degrees (C2), taking a reference value from vibrational studies of 175 degrees (C1 species). Resonance Raman and ENDOR studies of SOR variants, in which the conserved glutamate and lysine residues in a flexible loop above the substrate binding pocket have been individually replaced by alanine, indicate that the side chains of these two residues are not involved in direct interaction with bound cyanide. The implications of these results for understanding the mechanism of SOR are discussed.     

Resonance Raman evidence for an unusually strong exogenous ligand-metal bond in a monomeric nitrosyl manganese hemoglobin

Resonance Raman spectroscopy has been employed to determine the vibrational modes of monomeric nitrosyl manganese Chironomus thummi thummi hemoglobin (CTT IV). This insect hemoglobin has no distal histidine. By applying various isotope-labeled nitric oxides (14N16O, 15N16O, 14N18O), we have identified the Mn11-NO stretching model at 628 cm-1, the Mn11-N-O bending mode at 574 cm-1 and the N-O stretching mode at 1735 cm-1. The results suggest a strong Mn11-NO bond and a weak N-O bond. The vinyl group substitution does not influence the nu (Mn11-NO), delta (Mn11-N-O) and nu (N-O) vibrations. The Mn11-NO stretching frequency is insensitive to distal histidine interactions with NO, whereas the N-O stretching frequency is sensitive. Nitric oxide also binds to Met manganese CTT IV to form an Mn111. NO complex which undergoes a slow but complete autoreduction resulting in the Mn11.NO species. In manganese meso-IX CTT IV, the Mn111. NO Mn11. NO conversion alters the intensities of the porphyrin ring modes at 342, 360, 1587 and 1598 cm-1, but shifts the frequencies at 1504 and 1633 cm-1 (in Mn111.NO) to 1497 and 1630 cm-1 (in Mn11. NO), respectively. The unshifted marker line at 1378 cm-1 reflects the fact that the pi electron densities of the porphyrin ring are the same in the two complexes.     

Resonance Raman evidence for the mechanism of the allosteric control of O2-binding in a cobalt-substituted monomeric insect hemoglobin.

The substitution of iron for cobalt in the monomeric insect hemoglobin CTT (Chironomus thummi thummi) III does not alter the Bohr effect for O2-binding. The cobalt substitution in this hemoglobin allows us to identify not only the O-O and Co-O2 stretching mode but also the Co-O-O bending mode by resonance Raman spectroscopy. The assignments were made via 16O2/18O2 isotope exchange. The modes associated with the Co-O-O moiety are pH-dependent. These pH-induced changes of the resonance Raman spectra are correlated with the t = r conformation transition. At high pH (high-affinity state) two unperturbed O-O stretching modes are observed at 1,068 cm-1 (major component) and 1,093 cm-1 (minor component) for the 18O2 complex. These frequencies correspond to split modes at 1,107 cm-1 and 1,136 cm-1 and an unperturbed mode at approximately 1,153 cm-1 for the 16O2 complex. At low pH (low-affinity state) the minor component becomes the major component and vice versa. The Co-O2 stretching frequency varies for approximately 520 cm-1 (pH 5.5) to 537 cm-1 (pH 9.5) indicating a stronger (hence shorter) Co-O2 bond in the high-affinity state. On the other hand, the O-O bond is weakened upon the conversion of the low- to the high-affinity state. The Co-O-O bending mode changes from 390 cm-1 (pH 9.5) to 374 cm-1 (pH 5.5). In the deoxy form the resonance Raman spectra are essentially pH-insensitive except for a vinyl mode at 414 cm-1 (pH 5.5), which is shifted to 416 cm-1 (pH 5.5).     

The cobalt-nitrosyl stretching vibration as a sensitive resonance Raman probe for distal histidine-nitrosyl interaction in monomeric hemoglobins

The Co-NO stretching vibration has been assigned in the resonance Raman spectra of various cobalt-substituted monomeric hemoglobins by employing isotope-labeling of nitrosyl (14N16O, 15N16O, 14N18O). Monomeric hemoglobins with a distal histidine (sperm whale myoglobin and leghemoglobin) exhibit this vibration at 573-575 cm-1, whereas hemoglobins without distal histidine (elephant myoglobin and insect hemoglobin from Chironomus thummi thummi, CTT III) show this vibration in the range of 553-558 cm-1. The Fe-NO stretching vibration which occurs in the range of 554-556 cm-1 does not reflect the distal histidine-ligand interaction. Therefore, the Co-NO moiety which is isoelectronic with the Fe-O2 moiety is a good monitor for distal effects on the exogenous ligand of hemoglobins, especially due to the fact that in hemoglobins with distal histidine the Fe-O2 stretching vibration (567-572 cm-1) is similar to the Co-NO stretching vibration.     

The resonance Raman frequencies of the Fe-CO stretching and bending modes in the CO complex of cytochrome P-450cam

Resonance Raman spectra of the ferrous CO complex of cytochrome P-450cam have been observed both in its camphor-bound and free states. Upon excitation at 457.9 nm, near the absorption maximum of the Soret band, the ferrous CO complex of the camphor-bound enzyme showed an anomalously intense Raman line at 481 cm-1 besides the strong Raman lines at 1366 and 674 cm-1 for the porphyrin vibrations. The Raman line at 481 cm-1 (of the 12C16O complex) shifted to 478 cm-1 upon the substitution by 13C16O and to 473 cm-1 by 12C18O without any detectable shift in porphyrin Raman lines. This shows that the line at 481 cm-1 is assignable to Fe-CO stretching vibration. By the excitation at 457.9 nm, a weak Raman line was also observed at 558 cm-1, which was assigned to the Fe-C-O bending vibration, because it was found to shift by -14 cm-1 on 13C16O substitution while only -3 cm-1 on 12C18O substitution. These stretching and bending vibrations of the Fe-CO bond were not detected with the excitation at 413.1 nm, though the porphyrin Raman lines at 1366 and 674 cm-1 were clearly observed. When the substrate, camphor, was removed from the enzyme, the Fe-CO stretching vibration was found to shift to 464 cm-1 from 481 cm-1, while no detectable changes were found in porphyrin Raman lines. This means that the bound substrate interacts predominantly with the Fe-CO portion of the enzyme molecule.     

Resonance Raman studies of sterically hindered cyanomet "strapped" hemes. Effects of ligand distortion and base tension on iron-carbon bond

We report resonance Raman studies of the iron-carbon bond stretching vibrations, nu(Fe-CN), in sterically hindered and unhindered heme (FeIII)-CN- complexes. The sterically hindred "strapped hemes" are equipped with a covalently linked 13-, 14-, or 15-atom hydrocarbon chain across one face of the heme; these are called FeSP-13, FeSP-14, and FeSP-15, respectively. These straps would presumably exert a sideway shearing strain to force the linear ligands (e.g., CN- and CO) to be tilted and/or bent. The shorter the chain length, the weaker the ligand binding affinity because of a greater steric hindrance. This study reveals that the nu(Fe-CN) frequency decreases as the chain length is decreased, in contrast with the CO complexes, where the nu(Fe-CO) frequency increases as the chain length is decreased. For the heme-CN- complexes (with N-methylimidazole as a base), the nu(Fe-CN) frequencies are: heme 5 (unhindered), 451 cm-1; FeSP-15, 447 cm-1; FeSP-14, 447 cm-1; FeSP-13, 445 cm-1. For the heme-CO complexes (with N-methylimidazole as a base), the nu(Fe-CO) frequencies are: heme 5, 495 cm-1; FeSP-15, 509 cm-1; FeSP-14, 512 cm-1; FeSP-13, 514 cm-1 (Yu, N.-T., E. A. Kerr, B. Ward, and C. K. Chang, 1983, Biochemistry, 22:4534-4540). We have also studied the cyanide complexes with three different bases (pyridine, N-methylimidazole and 1,2-dimethylimidazole), and found that the trans-effect of cyanide complex is different from that of CO complexes.(ABSTRACT TRUNCATED AT 250 WORDS)     

Mechanism of the control of dioxygen binding in a dimeric cobalt-substituted insect hemoglobin. Resonance Raman evidence for cobalt-axial-ligand bond changes

Resonance Raman spectroscopy has been used to investigate the allosteric control mechanism for O2 binding in a cobalt-substituted dimeric insect hemoglobin (CTT II), which exhibits a large Bohr effect due to a pH-induced transition between two ligand affinity states. Substitution of cobalt for iron in CTT II does not modify the Bohr effect, but permits the resonance enhancement (hence the detection) of Raman lines corresponding to the vibrations of the axial ligand-cobalt bonds. Using 16O2/18O2 isotope substitution the O-O and Co-O2 stretching and the Co-O-O bending mode have been assigned to the two affinity states of this hemoglobin: v (O-O) changes from 1152 cm-1 (pH 5.5; t conformation) to about 1125 cm-1 (pH 9.5, r conformation), v (Co-O2) from 512 cm-1 (pH 5.5) to 537 cm-1 (pH 9.5) and delta (Co-O-O) from 378 cm-1 (pH 5.5) to 390 cm-1 (pH 9.5). The Co-N epsilon (His) stretching mode has also been detected changing from 313 cm-1 (pH 5.5) to 307 cm-1 (pH 9.5). For the first time, reciprocal behaviour between the Co-N epsilon and Co-O2 bonds and between the Co-O2 and the O-O bonds in an allosteric hemoglobin are demonstrated. Furthermore, the pH sensitivity of a vinyl bending mode in the range of 411-415 cm-1 has been investigated and shown also to reflect the t in equilibrium with r conformation transition.     

Resonance Raman spectra of anionic semiquinoid form of a flavoenzyme, D-amino acid oxidase

Resonance Raman (RR) spectra of the complex of anionic semiquinoid D-amino acid oxidase (DAO) with picolinate in H2O and D2O were observed in the 300-1,750 cm-1 region. RR spectra were also measured for the complex of the semiquinoid enzyme reconstituted with isotopically labeled FAD's, i.e., [4a-13C]-, [4,10a-13C2]-, [2-13C]-, [5-15N]-, and [1,3-15N2]-FAD. On the basis of the isotope effects, tentative assignments of the observed bands of the anionic semiquinoid flavin were made. The spectra differ from those of oxidized, neutral semiquinoid, and anionic reduced flavins previously reported. The 1,602 cm-1 band was not shifted for any FAD labeled in ring II and/or ring III and was assigned to a ring I mode. The 1,516 cm-1 band underwent an isotopic shift upon [4a-13C]- or [4,10a-13C2]-labeling. The band was assigned to the mode containing C(4a)-C(10a) stretching. The 1,331 and 1,292 cm-1 bands shifted upon [4a-13C]- or [5-15N]-labeling and were assigned to the modes containing C(4a)-N(5) stretching. The 1,217 and 1,188 cm-1 bands were assigned to the skeletal vibrations of ring III coupled with the N(3)-H bending mode. The RR spectrum of the complex of anionic semiquinoid DAO with alpha-iminopropionate or N-methyl-alpha-iminopropionate was essentially identical with that of the complex with picolinate.     

Resonance Raman studies of Escherichia coli sulfite reductase hemoprotein. 3. Bound ligand vibrational modes

The vibrations of the bound diatomic heme ligands CO, CN-, and NO are investigated by resonance Raman spectroscopy in various redox states of Escherichia coli sulfite reductase hemoprotein, and assignments are generated by use of isotopically labeled ligands. For the fully reduced CO complex (ferrous siroheme, reduced Fe4S4 cluster) at room temperature, nu CO is observed at 1904 cm-1, shifting to 1920 cm-1 upon oxidation of the cluster. The corresponding delta FeCO modes are identified at 574 and 566 cm-1, respectively, by virtue of the zigzag pattern of their isotopic shifts. In frozen solution, two species are observed for the cluster-oxidized state, with nu CO at 1910 and 1936 cm-1 and nu FeC at 532 and 504 cm-1, respectively; nu FeC for the fully reduced species is identified at 526 cm-1 in the frozen state. For the ferrous siroheme-NO complex (cluster oxidized), nu NO is identified at 1555 cm-1 in frozen solution and a low-frequency mode is identified at 558 cm-1; this stretching mode is significantly lower than that observed in Mb-NO. For the ferric siroheme cyanide complexes evidence of two ligand-bonding forms is observed, with modes at 451/390 and 451/352 cm-1; they are distinguished by a reversal of the isotopic shift patterns of the upper and lower modes and could arise from a linear and a bent Fe-C unit, respectively. For the ferrous siroheme cyanide complex isotope-sensitive modes observed at 495 and 452 cm-1 are assigned to the FeCN- bending and FeC stretching vibrations, respectively.(ABSTRACT TRUNCATED AT 250 WORDS)     

Resonance Raman studies of Rieske-type proteins.

Resonance Raman (RR) spectra are reported for the [2Fe-2S] Rieske protein from Thermus thermophilus (TRP) and phthalate dioxygenase from Pseudomonas cepacia (PDO) as a function of pH and excitation wavelength. Depolarization ratio measurements are presented for the RR spectra of spinach ferredoxin (SFD), TRP, and PDO at 74 K. By comparison with previously published RR spectra of SFD, we suggest reasonable assignments for the spectra of TRP and PDO. The spectra of PDO exhibit virtually no pH dependence, while significant changes are observed in TRP spectra upon raising the pH from 7.3 to 10.1. One band near 270 cm-1, which consists of components at 266 cm-1 and 274 cm-1, is attributed to Fe(III)-N(His) stretching motions. We suggest that these two components arise from conformers having a protonated-hydrogen-bonded imidazole (266 cm-1) and deprotonated-hydrogen-bonded imidazolate (274 cm-1) coordinated to the Fe/S cluster and that the relative populations of the two species are pH-dependent; a simple structural model is proposed to account for this behavior in the respiratory-type Rieske proteins. In addition, we have identified RR peaks associated with the bridging and terminal sulfur atoms of the Fe-S-N cluster. The RR excitation profiles of peaks associated with these atoms are indistinguishable from each other in TRP (pH 7.3) and PDO and differ greatly from those of [2Fe-2S] ferrodoxins. The profiles are bimodal with maxima near 490 nm and > approx. 550 nm. By contrast, bands associated with the Fe-N stretch show a somewhat different enhancement profile. Upon reduction, RR peaks assigned to Fe-N vibrations are no longer observed, with the resulting spectrum being remarkably similar to that reported for reduced adrenodoxin. This indicates that only modes associated with Fe-S bonds are observed and supports the idea that the reducing electron resides on the iron atom coordinated to the two histidine residues. Taken as a whole, the data are consistent with an St2FeSb2Fe[N(His)]t2 structure for the Rieske-type cluster.     

Resonance Raman characterization of the mononuclear iron active-site vibrations and putative electron transport pathways in Pyrococcus furiosus superoxide reductase

The resonance Raman spectrum of oxidized wild-type P. furiosus SOR at pH 7.5 and 10.5 has been investigated using excitation wavelengths between 406 and 676 nm, and vibrational modes have been assigned on the basis of isotope shifts resulting from global replacements of (32)S with (34)S, (14)N with (15)N, (56)Fe with (54)Fe, and exchange into a H(2)(18)O buffer. The results are interpreted in terms of the crystallographically defined active-site structure involving a six-coordinate mononuclear Fe center with four equatorial histidine ligands and axial cysteine and monodentate glutamate ligands (Yeh, A. P., Hu, Y., Jenney, F. E., Adams, M. W. W., and Rees, D. C. (2000) Biochemistry 39, 2499-2508). Excitation into the intense (Cys)S(p(pi))-to-Fe(d(pi)) CT transition centered at 660 nm results in strong enhancement of modes at 298 cm(-1) and 323 cm(-1) that are assigned to extensively mixed cysteine S-C(beta)-C(alpha) bending and Fe-S(Cys) stretching modes, respectively. All other higher-energy vibrational modes are readily assigned to overtone or combination bands or to fundamentals corresponding to internal modes of the ligated cysteine. Weak enhancement of Fe-N(His) stretching modes is observed in the 200-250 cm(-1) region. The enhancement of internal cysteine modes and Fe-N(His) stretching modes are a consequence of a near-planar Fe-S-C(beta)-C(alpha)-N unit for the coordinated cysteine and significant (His)N(p(pi))-Fe(d(xy))-(Cys)S(p(pi)) orbital overlap, respectively, and have close parallels to type 1 copper proteins. By analogy with type 1 copper proteins, putative superexchange electron-transfer pathways to the mononuclear Fe active site are identified involving either the tyrosine and cysteine residues or the solvent-exposed deltaN histidine residue in a Y-C-X-X-H arrangement. Studies of wild-type at pH 10.5 and the E14A variant indicate that the resonance Raman spectrum is remarkably insensitive to changes in the ligand trans to cysteine and hence are inconclusive concerning the origin of the alkaline transition and the nature of sixth Fe ligand in the E14A variant.     

Resonance Raman interrogation of the consequences of heme rotational disorder in myoglobin and its ligated derivatives

Resonance Raman spectroscopy is employed to characterize heme site structural changes arising from conformational heterogeneity in deoxyMb and ligated derivatives, i.e., the ferrous CO (MbCO) and ferric cyanide (MbCN) complexes. The spectra for the reversed forms of these derivatives have been extracted from the spectra of reconstituted samples. Dramatic changes in the low-frequency spectra are observed, where newly observed RR modes of the reversed forms are assigned using protohemes that are selectively deuterated at the four methyl groups or at the four methine carbons. Interestingly, while substantial changes in the disposition of the peripheral vinyl and propionate groups can be inferred from the dramatic spectral shifts, the bonds to the internal histidyl imidazole ligand and those of the Fe-CO and Fe-CN fragments are not significantly affected by the heme rotation, as judged by lack of significant shifts in the nu(Fe-N(His)), nu(Fe-C), and nu(C-O) modes. In fact, the apparent lack of an effect on these key vibrational parameters of the Fe-N(His), Fe-CO, and Fe-CN fragments is entirely consistent with previously reported equilibrium and kinetic studies that document virtually identical functional properties for the native and reversed forms.     

Biomimetic approach to the oxygen evolving center: resonance Raman investigation of a manganese µ-oxo dimer in three oxidation states

A biologically relevant dinuclear manganese mono-mu-oxo complex with a bound phenolate ligand in three oxidation states, (III,III), (III,IV) and (IV,IV), was studied using resonance Raman spectroscopy. Depending upon the excitation frequency, phenolate vibrations or mu-oxo vibrations were enhanced, which allowed us to assign the UV-visible absorption spectra. In the case of the mixed valence species (III,IV), the mu-oxo vibration at 854 cm-1 has been assigned by isotopic substitution (H2(18)O) to nu as(Mn-O-Mn). This preferential enhancement of the asymmetric vibration stresses the asymmetric character of the bridge.     

Metal-ligand vibrations of cyanoferric myeloperoxidase and cyanoferric horseradish peroxidase: evidence for a constrained heme pocket in myeloperoxidase

The low-frequency FeCN vibrations of cyanoferric myeloperoxidase (MPO) and horseradish peroxidase (HRP) have been measured by resonance Raman spectroscopy. The ordering of the frequencies of the predominantly FeC stretching and FeCN bending normal vibrational modes in the two peroxidases differs. These normal mode vibrations are identified by their wavenumber shifts upon isotopic substitution of the cyanide ligand. For MPO, the stretching mode nu 1 (361 cm-1) occurs at a lower frequency than the bending mode delta 2 (454 cm-1). For HRP, the order is reversed as nu 1 (456 cm-1) is at a higher frequency than delta 2 (404 cm-1). Normal coordinate analyses and model complexes have been used to address the origin of this behavior. The nu 1 stretching frequencies in cyanide complexes of iron porphyrin and iron chlorin model compounds are similar to one another and to that of HRP. Thus, the inverted order and altered frequencies of the nu 1 and delta 2 vibrations in MPO, relative to those in HRP and the model compounds, are not inherent to the proposed iron chlorin prosthetic group in MPO but, rather, are attributed to distinct distal environmental effects in the MPO active site. The normal coordinate analyses for MPO and HRP showed that the nu 1 and delta 2 vibrational frequencies are not pure; the potential energy distributions for these modes respond not only to the geometry but also to the force constants of the nu(FeC) and delta(FeCN) internal coordinates.(ABSTRACT TRUNCATED AT 250 WORDS)     

The significance of the 2' OH group and the influence of cations on the secondary structure of the RNA backbone.

In the IR spectra, the coupling of vibrations leads to band splitting and/or bands shifting in opposite directions which provides information on the mutual orientation of groupings. From such band shifts in the range 1800 to 1500 cm-1 one can draw conclusions on the double helix formation of polynucleotides. These band shifts are caused either by vibrational coupling of stretching vibrations within pairs of base residues or by coupling of stretching vibrations with the bending (scissor) vibration of the -NH2 groups; the latter is indicated by band shifts after deuterium substitution within the amino groups. Couplings of phosphate and 1 ibose vibrations in the range 1300 to 1000 cm-1 provide information on the secondary structure of the backbone. In order to obtain information of the structure of the RNA backbone, the IR spectra of poly(ribonucleotides) were studied in neutral media in which they were single-stranded. The shift due to coupling of the band of the 2'OD bending vibration and that of the antisymmetric stretching vibration of the ether group of the ribose residue proves that ribose residues of the backbone are cross-linked via hydrogen bonds. These are formed between the 2'OD or 2'OH groups, respectively, and the O atoms of the ether group of the neighboring ribose residues. This is the reason for the difference between DNA and RNA as regards the 2'OH group. The structure formation caused by these hydrogen bonds results in a stiffening of the RNA backbone. The tendency to form these hydrogen bonds increases in the order poly (U), poly(C), poly (A). This order of secondary structure stabilization is due to an interplay between the influences of (1) the 2'OH hydrogen bonds and (2) the base residues' stacking. Furthermore, the coupling of the antisymmetric stretching vibration of the greater than PO2- groups with a vibration involving the 2'OH group can result in a doublet structure of the band at about 1240 cm-1 if cations with strong fields are present. This probably shows that these cations can turn the greater than PO2-groups-which are usually turned outward at the backbone, as shown by construction of molecular models- towards the basic residues. Thus they cause stiff monohelices which are right-handed screws.     

Resonance Raman studies on the blue-green-colored bovine adrenal tyrosine 3-monooxygenase (tyrosine hydroxylase). Evidence that the feedback inhibitors adrenaline and noradrenaline are coordinated to iron

Tyrosine 3-monooxygenase (tyrosine hydroxylase) is a non-heme iron, tetrahydropterin-dependent enzyme which catalyzes the rate-limiting step in the biosynthesis of catecholamines. The highly purified bovine adrenal enzyme contains an unusual blue-green chromophore with lambda max at around 700 nm (epsilon = 1.3 (mM subunit enzyme)-1 cm-1). On excitation at 605.2 nm, resonance-enhanced Raman vibrations are observed at 454, 494, 527, 604, 635, 835, 1130, 1271, 1320, 1426, and 1476 cm-1. The excitation profiles of the modes of 1276 and 1476 cm-1 (from 488 to 620 nm) follow the contour of the 700 nm absorption band. The vibrations observed strongly indicate the presence of a bidentate catecholamine-Fe(III) complex in the enzyme as isolated which gives rise to the characteristic charge-transfer transitions. This is further supported by the release of 0.11 +/- 0.04 mol of noradrenaline and 0.25 +/- 0.06 mol of adrenaline per mol of enzyme subunit on denaturation of the enzyme. The energies of the catecholate to Fe(III) charge-transfer transitions indicate a mixture of histidines and carboxylate(s) coordinated to the iron center in tyrosine hydroxylase. At neutral pH, the enzymatic activity was inhibited more than 50% by 10 microM dopamine, noradrenaline, and adrenaline. The high affinity of the catecholamines to the nonphosphorylated form of tyrosine hydroxylase may have significance in vivo since catecholamines are potent feedback inhibitors of the enzyme.