Resonance Raman spectroscopy of ribonucleotide reductase. Evidence for a deprotonated tyrosyl radical and photochemistry of the binuclear iron center

Native ribonucleotide reductase from Escherichia coli exhibits a resonance-enhanced Raman mode at 1498 cm-1 that is characteristic of a tyrosyl radical. The Raman frequency as well as the absorption maximum at 410 nm identifies the radical as being in a deprotonated state. The B2 subunit of ribonucleotide reductase shows an additional resonance Raman mode at 493 cm-1 that has been assigned to the symmetric stretch of an Fe-O-Fe moiety. When samples of active B2 or metB2 are exposed to a tightly focused laser beam at 406.7 nm, there is a loss of intensity at 493 cm-1 and the appearance of a new peak at 595 cm-1. Although the 595-cm-1 feature was previously assigned to an Fe-OH vibration on the basis of its 23-cm-1 shift to lower energy in H2(18)O and the apparent dependence of its intensity on pH [Sj?berg, B. M., Loehr, T. M., & Sanders-Loehr, J. (1987) Biochemistry 26, 4242], the present studies indicate that the intensity of this mode is dependent primarily on input laser power. The peak at 595 cm-1 is more plausibly assigned to a new vs(Fe-O-Fe) mode in view of its lack of the deuterium isotope dependence expected for an Fe-OH mode and its resonant scattering cross section which is comparable to that of the 493-cm-1 mode. This new species has a calculated Fe-O-Fe angle of approximately 113 degrees compared to approximately 138 degrees calculated for the Fe-O-Fe unit in unmodified protein B2. One possible explanation for the photoinduced vibrational mode is that a bridging solvent molecule has been inserted in place of a bridging carboxylate.     

Raman and infrared spectroscopy of the oxo-bridged iron(III) complex, [Cl3Fe-O-FeCl3]-2 as a spectroscopic model for the oxo bridge in hemerythrin and ribonucleotide reductase

Vibrational spectroscopic data were collected on the salt [C5H6N]2[Cl3FeOFeCl3] . C5H5N, which has previously been structurally characterized by X-ray crystallography. The modes associated with the oxo bridge were identified by experiments on the 18O-containing species. Spectra for the mu-16O complex contain Raman bands at 870, 458, and 203 cm-1 that shift to 826, 440, and 198 cm-1 in the mu-18O complex. These are respectively assigned to the asymmetric, symmetric, and angle deformations of the bent Fe-O-Fe moiety. A normal mode vibration analysis based on a simple valence force field for the Fe-O-Fe portion of the molecule provides surprisingly good agreement with these experimental frequencies and their assignments. The vibrational data for this simple inorganic complex confirm the assignment of a resonance Raman band around 500 cm-1 in the oxygen-carrying protein hemerythrin and enzyme ribonucleotide reductase as the symmetric stretch of an oxo bridge between two iron(III) centers.     

A comparison of the resonance Raman properties of the fast and slow forms of cytochrome oxidase

Resonance Raman (RR) spectra of the "rapid" and "slow" forms (Baker et al., 1987) of resting cytochrome oxidase obtained with Soret excitation at 413.1 nm are reported. There are a number of conspicuous differences between the two forms in the high-frequency region of the RR spectrum which involve changes in Raman intensity arising from a blue shift in the Soret maximum of cytochrome a3 upon conversion to the slow form. In the low-frequency region a peak present at 223 cm-1 in the rapid form shifts to 220 cm-1 in the slow form; this peak is assigned as the cytochrome a3 Fe(III)-N(His-Im) stretch. The slow form of the enzyme possesses greater intensity in RR peaks near 1620 cm-1 which have been previously attributed by others to partial photoreduction of the enzyme. We have quantitated the amount of laser-induced photoreduction in these RR spectra by comparison with the spectra of mixed-valence derivatives of the enzyme and find that these 1620-cm-1 features are unreliable indicators of photoreduction. The spectra of the fast- and slow-reacting species in H2O and D2O have been compared. The fast-reacting form exhibits a 4-cm-1 shift, from 223 to 219 cm-1, upon transferring to D2O in a peak which we assign as the cytochrome a3 Fe(III)-N(His-Im) stretch. There is a parallel shift in the feature at 1651 cm-1 due to the C = O stretch of the formyl group of cytochrome a. These deuterium shifts are not observed in the slow form.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydroxide ion binding to methemerythrin. An investigation by resonance Raman and difference spectroscopy

The pH dependence for the interconversion of the acid and base forms of methemerythrin from Themiste dyscritum was investigated by difference spectroscopy. A new technique was designed to be able to study mixtures without knowledge of extinction coefficients or exact protein concentrations. The resultant pKa value of 8.4 proved that T. dyscritum hemerythrin crystals used for previous X-ray crystallographic studies at pH less than or equal to 6.5 were in the acid form. Since this material contains a 5-coordinate iron atom with no evidence of a ligated water molecule, it is more appropriately referred to as methemerythrin than aquomethemerythrin. The presence of an iron-bound hydroxide in the base form of methemerythrin was verified by resonance Raman spectroscopy for both T. dyscritum and Phascolopsis gouldii. At pH greater than 9, the protein from either species exhibited a new feature at 490 cm-1 that shifted to 518 cm-1 in D2O and was assigned to a coupled Fe-OH stretching and O-H bending vibration. Thus, hydroxomethemerythrin is the correct designation for the base form of the protein. The other resonance-enhanced vibration, the Fe-O-Fe symmetric stretch, was observed at 506 cm-1 in hydroxomethemerythrin and at 511 cm-1 in methemerythrin and was unaffected by deuteration. Addition of perchlorate to methemerythrin had no effect on the Raman spectrum, despite its known role in stabilizing the met form relative to the hydroxomet form.     

Observation of an isotope-sensitive low-frequency Raman band specific to metmyoglobin

A resonance Raman band involving significantly the iron(III)-histidine stretching (upsilonFe-His) character is identified for metmyoglobin (metMb) through isotope sensitivity of its low-frequency resonance Raman bands, but the identification was not successful for methemoglobin (metHb) and its isolated alpha and beta subunits. A band at 218 cm-1 of natural abundance metMb exhibited a low-frequency shift for 15N-His-labeled metMb (-1.4 cm-1 shift), while the strong porphyrin bands at 248 and 271 cm-1 did not shift significantly. The frequency of the 218-cm-1 band of metMb decreased by 1.6 cm-1 in D2O, probably due to Ndelta-deuteration of the proximal His, in a similar manner to that of the upsilonFe-His band of deoxyMb in D2O. This 218-cm-1 band shifted slightly to a lower frequency in H2(18)O, whereas it did little upon 54Fe isotopic substitution (<0.3 cm-1), presumably because of the six-coordinate structure. The lack of the 54Fe-isotope shift shows that the 218-cm-1 band is specific to metMb and not due to the deoxy species. The intensity of this band decreased for hydroxymetMb and was indiscernible for cyanometMb. For metHb and its alpha and beta subunits, however, the frequencies of the band around 220 cm-1 were not D2O sensitive. These results suggest an assignment of the band around 220 cm-1 to a pyrrole tilting mode, which significantly contains the Fe-His stretching character for metMb but scarcely for metHb and its subunits. The differences in the isotope sensitivity of this band in different proteins are considered to reflect the heme distortion from the planarity and the Fe-His geometry specific to individual proteins.     

Determination of the exchange integral in binuclear iron-sulfur clusters in proteins of varying complexity.

The coupling constants J between the iron atoms in ferredoxin type iron-sulfur proteins containing binuclear clusters were evaluated by two parallel methods. The temperature dependence of the EPR linewidths and integrated abosrption intensities are both related to the energy of the first excited state. The values of J obtained were: center S-1 in succinate dehydrogenase, 90 cm-1; Rieske's iron-sulfur center, 65 cm-1; adrenodoxin, 270 cm-1. The behavior of iron-sulfur center N-1a in NADH:UQ reductase was also examined; its similarity to that of center S-1 indicates that center N-1a is also a binuclear iron-sulfur center, with J = 90 cm-1. Greater rhombic distortion present in the EPR spectrum of a binuclear cluster was associated with smaller values of J.     

Structure of the retinal chromophore in 7,9-dicis-rhodopsin

Bovine rhodopsin was bleached and regenerated with 7,9-dicis-retinal to form 7,9-dicis-rhodopsin, which was purified on a concanavalin A affinity column. The absorption maximum of the 7,9-dicis pigment is 453 nm, giving an opsin shift of 1600 cm-1 compared to 2500 cm-1 for 11-cis-rhodopsin and 2400 cm-1 for 9-cis-rhodopsin. Rapid-flow resonance Raman spectra have been obtained of 7,9-dicis-rhodopsin in H2O and D2O at room temperature. The shift of the 1654-cm-1 C = N stretch to 1627 cm-1 in D2O demonstrates that the Schiff base nitrogen is protonated. The absence of any shift in the 1201-cm-1 mode, which is assigned as the C14-C15 stretch, or of any other C-C stretching modes in D2O indicates that the Schiff base C = N configuration is trans (anti). Assuming that the cyclohexenyl ring binds with the same orientation in 7,9-dicis-, 9-cis-, and 11-cis-rhodopsins, the presence of two cis bonds requires that the N-H bond of the 7,9-dicis chromophore points in the opposite direction from that in the 9-cis or 11-cis pigment. However, the Schiff base C = NH+ stretching frequency and its D2O shift in 7,9-dicis-rhodopsin are very similar to those in 11-cis- and 9-cis-rhodopsin, indicating that the Schiff base electrostatic/hydrogen-bonding environments are effectively the same. The C = N trans (anti) Schiff base geometry of 7,9-dicis-rhodopsin and the insensitivity of its Schiff base vibrational properties to orientation are rationalized by examining the binding site specificity with molecular modeling.     

Paramagnetically shifted resonances in 1H NMR spectra of ribonucleotide reductase from Escherichia coli

The 400-MHz 1H NMR spectra of the subunit B2 of ribonucleotide reductase from Escherichia coli show paramagnetically shifted resonances at 24 ppm (exchangeable protons) and at 19 ppm (nonexchangeable protons). The protein contains an antiferromagnetically coupled dimeric iron center and a tyrosyl free radical. The paramagnetically shifted resonances must be due to the iron center, since they remain essentially unchanged in protein B2 with and without free radical. In analogy with recently published results for hemerythrin from Phascolopsis gouldii, which has a similar iron center, the 24-ppm resonance is suggested to arise from histidine ligands to the iron ions.     

Resonance Raman examination of axial ligand bonding and spin-state equilibria in metmyoglobin hydroxide and other heme derivatives

Resonance Raman spectra and excitation profiles have been obtained within the 5700-6300-A absorption band of purified sperm whale metmyoglobin hydroxide (MbIIIOH) solutions. A large enhancement occurs for a Raman peak at 490 cm-1 which is shown by isotopic substitution of 18O for 16O to be almost purely an Fe-O stretch. The Fe-O vibration in MbIIIOH occurs 5 cm-1 to lower energy than the corresponding vibration at 495 cm-1 in human methemoglobin hydroxide (HbIIIOH) [Asher, S., Vickery, L., Schuster, T., & Sauer, K. (1977) Biochemistry 16, 5849], reflecting differences in ligand bonding between Mb(III) and Hb(III). A larger frequency difference (10 cm-1) exists between MbIIIF and HbIIIF for the Fe-F stretch. We do not observe separate Fe-O or Fe-F stretches from the alpha and beta chains of either HbIIIOH or HbIIIF. Excitation profile measurements for MbIIOH indicate that the 5700-6300-A absorption band is composed of two separate absorption bands which result from a high- and a low-spin form of MbIIIOH. The spin-state-sensitive Raman band at 1608 cm-1 reflects the high-spin species and has an excitation profile maximum at about 6000 A while the low-spin Raman band occurs at 1644 cm-1 and shows an excitation profile maximum at 5800 A. The Fe-O stretch at 490 cm-1 has an excitation profile maximum at about 6000 A. The differences in frequency and Raman cross section between the Fe-X vibrations in MbIIIX and HbIIIX (X = OH-, F-) can be related to increases in the out-of-plane iron distance for the high-spin species of MbIIIX. The shift in the 1644-cm-1 MbIIIOH low-spin state Raman band indicative of the heme core size to 1636 cm-1 in HbIIIOH indicates a larger heme core size in HbIIIOH. Raman frequency shifts are used to estimate differences in bond strain energies between MbIIIX and HbIIIX (X = OH-, F-). Previous resonance Raman excitation profile data can be interpreted in terms of separate contributions from different spin-state species.     

Structures of met and azidomet hemerythrin at 1.66 A resolution

The crystallographic refinement of met and azidomet hemerythrin has been carried out at 1.66 A resolution in an attempt to characterize precisely the binuclear iron center in this protein. Restrained least-squares refinement has produced molecular models giving R-values of 18.9% for met (65,683 reflections from 10 A to 1.66 A) and 17.6% for azidomet hemerythrin (68,747 reflections from 10.0 A to 1.66 A). The protein structure in each derivative is very similar to that of myohemerythrin. The mu-oxo bridged iron center differs between the two forms. The complex in met hemerythrin is asymmetric with the bridging oxygen closer to one of the iron atoms while the complex in azidomet hemerythrin is symmetric. After investigations of the effects of correlation in the refinement, we believe this difference between the two complexes is associated with chemical differences and is not a refinement artefact.     

Structure of DNA hydration shells studied by Raman spectroscopy

We have used Raman scattering to study the water O-H stretching modes at approximately 3450 and approximately 3220 cm-1 in DNA films as a function of relative humidity (r.h.). The intensity of the 3220-cm-1 band vanishes as the r.h. is decreased from 98% to around 80%, which indicates that the hydrogen-bond network of water is disrupted in the primary hydration shell (which therefore cannot have an "ice-like" structure). The number of water molecules in the primary hydration shell was determined from the intensity of the approximately 3200-cm-1 band as about 30 water molecules per nucleotide pair. The approximately 3400-cm-1 O-H stretch band was used for determining the total water content, and this band persists at 0% r.h., implying that 5-6 tightly bound water molecules per nucleotide pair remain. The frequency of the approximately 3400-cm-1 O-H stretch mode is lower by 30 to 45 cm-1 in the primary hydration shell compared to free water. The water content as a function of r.h. obtained from these experiments agrees with gravimetric measurements. The disappearance of the approximately 3200-cm-1 band and the shift of the approximately 3400-cm-1 O-H stretch band provide a reliable way of measuring the hydration number of DNA.     

Resonance Raman studies of the stoichiometric catalytic turnover of a substrate-stearoyl-acyl carrier protein delta(9) desaturase complex

Resonance Raman spectroscopy has been used to study the effects of substrate binding (stearoyl-acyl carrier protein, 18:0-ACP) on the diferric centers of Ricinus communis 18:0-ACP Delta(9) desaturase. These studies show that complex formation produces changes in the frequencies of nu(s)(Fe-O-Fe) and nu(as)(Fe-O-Fe) consistent with a decrease in the Fe-O-Fe angle from approximately 123 degrees in the oxo-bridged diferric centers of the as-isolated enzyme to approximately 120 degrees in oxo-bridged diferric centers of the complex. Analysis of the shifts in nu(s)(Fe-O-Fe) and nu(as)(Fe-O-Fe) as a function of 18:0-ACP concentration also suggests that 4e(-)-reduced Delta9D containing two diferrous centers has a higher affinity for 18:0-ACP than resting Delta9D containing two diferric centers. Catalytic turnover of a stoichiometric complex of 18:0-ACP and Delta9D was used to investigate whether an O-atom from O(2) would be incorporated into a bridging position of the resultant mu-oxo-bridged diferric centers during the desaturation reaction. Upon formation of approximately 70% yield of 18:1-ACP product in the presence of (18)O(2), no incorporation of an (18)O atom into the mu-oxo bridge position was detected. The result with 18:0-ACP Delta(9) desaturase differs from that obtained during the tyrosyl radical formation reaction of the diiron enzyme ribonucleotide reductase R2 component, which proceeds with incorporation of an O-atom from O(2) into the mu-oxo bridge of the resting diferric site. The possible implications of these results for the O-O bond cleavage reaction and the nature of intermediates formed during Delta9D catalysis are discussed.     

Carbonmonoxy dopamine beta-hydroxylase. Structural characterization by Fourier transform infrared, fluorescence, and x-ray absorption spectroscopy

The carbon monoxide complex of ascorbate-reduced dopamine beta-hydroxylase has been prepared and characterized by Fourier transform infrared, fluorescence, and x-ray absorption spectroscopies. CO has previously been shown to be a competitive inhibitor with respect to O2, and binds to only one of the two copper atoms/active site (Blackburn, N. J., Pettingill, T. M., Seagraves, K. S., and Shigeta, R. T. (1990) J. Biol. Chem. 265, 15383-15386). Thus, it acts as an excellent probe of the O2-binding site. A single C-O infrared absorption band is observed at 2089 cm-1, shifting by 46 cm-1 to lower energy on substitution with either 13C16O or 12C18O. The 13C isotope shift is reversed to the position expected for 12CO upon vacuum flushing with 12CO gas, indicating that formation of the CO adduct is a fully reversible process. Binding of the substrate tyramine does not eliminate the infrared peak but causes a 3-cm-1 shift to lower energy. On the other hand, binding of a bifunctional inhibitor which cross-links the substrate and O2-binding site does eliminate the CO peak. These data, in conjunction with the competitive nature of CO binding with respect to O2, identify the CO-binding site as the O2-binding site, and place it in close proximity to the substrate-binding site. CO-dopamine beta-hydroxylase exhibits no luminescence in the visible region, suggesting a structure different from carbonmonoxy hemocyanin, and in all probability mononuclear. Analysis of extended x-ray absorption spectroscopy data is most consistent with an average coordination per Cu of 2-3 histidines, 0.5 CO, and 0.5 S atoms as ligands, and absorption edge comparisons indicates pseudo-4 coordination as the most likely geometry at each Cu(I) center. The results can be interpreted by a model involving inequivalent 4-coordination at each Cu(I) center in the CO adduct with CuAHis3S...CuBHis2CO-X as the coordination most consistent with all of the data.     

Half-site reactivity of the tyrosyl radical of ribonucleotide reductase from Escherichia coli

A C-terminally truncated form of protein B2, the homodimeric small subunit of ribonucleotide reductase from Escherichia coli, was found as the result of an apparently specific proteolysis. Truncated homodimers contain an intact binuclear iron center and a normal tyrosyl radical but have no binding capacity for the other ribonucleotide reductase subunit, protein B1, and are consequently enzymatically inactive. Heterodimers, consisting of one full-length and one truncated polypeptide, formed spontaneously during a chelation-reconstitution cycle and were easily separated from the two homodimeric variants. The heterodimeric form of B2 shows a weak interaction with the B1 subunit resulting in low enzyme activity. Using heterodimers containing deuterated tyrosine on the full-length side and protonated tyrosine on the truncated side, we could demonstrate that the tyrosyl radical was randomly generated in one or the other of the two polypeptide chains of the heterodimeric B2 subunit. The small subunit of ribonucleotide reductase thus conforms to a half-site reactivity.     

The role of herpes simplex virus ribonucleotide reductase small subunit carboxyl terminus in subunit interaction and formation of iron-tyrosyl center structure.

Herpes simplex virus ribonucleotide reductase consists of two nonidentical subunits, proteins R1 and R2, which are required together for activity. Active R2 protein contains a tyrosyl free radical and a binuclear iron center. A truncated form of the R2 subunit, lacking 7 amino acid residues in the carboxyl terminus, was constructed, overexpressed in Escherichia coli and purified to homogeneity. In the presence of ferrous iron and oxygen, the truncated protein readily generated similar amounts of tyrosyl free radical as the intact protein. However, the radical showed differences in EPR characteristics in the truncated protein compared with the normal one, indicating an altered structural arrangement of the radical relative to the iron center. The truncated R2* protein was completely devoid of binding affinity to the R1 protein, demonstrating that the subunit interaction is totally dependent on the 7 outermost carboxyl-terminal amino acids of protein R2.     

Oxygen infrared spectra of oxyhemoglobins and oxymyoglobins. Evidence of two major liganded O2 structures

The dioxygen stretch bands in infrared spectra for solutions of oxy species of human hemoglobin A and its separated subunits, human mutant hemoglobin Zurich (beta 63His to Arg), rabbit hemoglobin, lamprey hemoglobin, sperm whale myoglobin, bovine myoglobin, and a sea worm chlorocruorin are examined. Each protein exhibits multiple isotope-sensitive bands between 1160 and 1060 cm-1 for liganded 16O2, 17O2, and 18O2. The O-O stretch bands for each of the mammalian myoglobins and hemoglobins are similar, with frequencies that differ between proteins by only 3-5 cm-1. The spectra for the lamprey and sea worm hemoglobins exhibit greater diversity. For all proteins an O-O stretch band expected to occur near 1125 cm-1 for 16O2 and 17O2, but not 18O2, appears split by approximately 25 cm-1 due to an unidentified perturbation. The spectrum for each dioxygen isotope, if unperturbed, would contain two strong bands for the mammalian myoglobins (1150 and 1120 cm-1) and hemoglobins (1155 and 1125 cm-1). Two strong bands separated by approximately 30 cm-1 for each oxy heme protein subunit indicate that two major protein conformations (structures) that differ substantially in O2 bonding are present. The two dioxygen structures can result from a combination of dynamic distal and proximal effects upon the O2 ligand bound in a bent-end-on stereochemistry.     

Infrared spectroscopic studies of carbonyl horseradish peroxidases.

Infrared difference spectra, FeIIICO vs. FeIII of horseradish peroxidase isoenzymes A2 and C were recorded from 2000 to 1800 cm-1. Under alkaline conditions, pH 9, both isoenzymes exhibit two CO stretching bands, at 1938 and 1925 cm-1 for A2 and at 1933 and 1929 cm-1 for C. As the pH is lowered the low-frequency band for each isoenzyme decreases in intensity with a concommitant appearance and increase in intensity of a band at 1906 and 1905 cm-1 for the A2 and C isoenzymes, respectively. These changes conform to pK values of 6.7 for the A2 and 8.8 for the C isoenzymes of horseradish peroxidase. The interpretation of the infrared results was simplified by the observation that a linear relationship exists between the redox potential, Em7, for the FeIII/FeII system vs. the infrared CO stretching frequency, vCO, for cytochrome a3, hemoglobin, myoglobin, and cytochrome P-450 cam with substrate. This relationship suggests that the primary force altering vCO in these heme proteins is a variation in electron density at the heme iron and not direct protein interactions with the CO ligand. The horseradish peroxidase infrared bands in the 1930-cm-1 region correlate well with this relationship. The large deviation of the 1905-cm-1 band from the linear relationship and its dependence upon hydrogen ion concentration are consistent with horseradish peroxidase having a single CO binding site which can hold in two geometries, one of which contains an amino acid moiety capable of forming a hydrogen bond to the carbonyl oxygen.     

Characterization of the tryptophan-derived quinone cofactor of methylamine dehydrogenase by resonance Raman spectroscopy

The resonance Raman (RR) spectrum of oxidized methylamine dehydrogenase (MADHOX) exhibits a set of C-H, C-C, C = C, and C = O vibrational modes between 900 and 1700 cm-1 that are characteristic of the quinone moiety of the tryptophan tryptophlyquinone (TTQ) cofactor. The close similarity of the RR spectra for MADHs from Paracoccus denitrificans (Pd), Thiobacillus versutus (Tv), and bacterium W3A1 proves that the same cofactor is present in all three proteins. The MADHs from Pd and Tv have a v(C = O) mode at approximately 1625 cm-1 that shifts approximately 20 cm-1 upon 18O substitution of one of the carbonyl oxygens and is assigned to the in-phase symmetric stretch of the two C = O groups. The semiquinone form of Pd MADH has its own characteristic RR spectrum with altered peak frequencies and intensities as well as a decrease in the total number of peaks. The hydroxide and ammonia adducts of MADHOX produce RR spectra similar to that of the semiquinone. The spectral changes in all three cases are interpreted as being due to reduced conjugation of the cofactor. The ammonia adduct is formulated as a carbinolamine, a likely intermediate in the enzymatic mechanism. In contrast, formation of the electron-transfer complex between amicyanin and MADHOX has no effect on the vibrational frequencies (and, hence, structure) of either the MADH quinone or the amicyanin blue copper site. The behavior of the TTQ cofactors of Pd and Tv MADHs are very similar to one another and somewhat different from W3A1 MADH, particularly with regard to adduct formation and ability to undergo isotope exchange with solvent. These differences are ascribed to the cofactor environments within the proteins rather than to the structure of the cofactor itself.     

Ionic strength dependence of cytochrome c structure and Trp-59 H/D exchange from ultraviolet resonance Raman spectroscopy

Ultraviolet resonance Raman spectra are reported for cytochrome c (cyt c) in FeII and FeIII oxidation states at low (0.005 M) and high (0.9-1.5 M) ionic strength. With 200-nm excitation the amide band intensities are shown to remain constant, establishing that redox state and ionic strength have no influence on the alpha-helical content. The tyrosine 830/850-cm-1 doublet, however, shows a loss in 830-cm-1 intensity at I = 0.005 M for the FeIII protein, suggesting a weakening or a loss of H-bonding from an internal tyrosine, probably Tyr-48, which is H-bonded to a heme propionate group in cyt c crystals. Excitation profiles of tryptophan peak at approximately 229 nm for both FeII and FeIII forms of cyt c, but at approximately 218 nm for aqueous tryptophan. The approximately 2200-cm-1 red shift of the resonant electronic transition is attributed to the Trp-59 residue being buried and H-bonded. Consistent with this Trp environment, the H-bond-sensitive 877-cm-1 Trp band is strong and sharp, and the 1357/1341-cm-1 doublet has a large intensity ratio, approximately 1.5, for both FeII and FeIII cyt c. The 877-cm-1-band frequency shifts to 860 cm-1 when the Trp indole proton is replaced by a deuteron. This band was used to show that Trp H/D exchange in D2O is much faster for FeIII than FeII cyt c. The half-time for exchange at room temperature is estimated to be approximately 30 and approximately 5 h, respectively, for FeII and FeIII when examined at I = 0.005.(ABSTRACT TRUNCATED AT 250 WORDS)     

The 1.9 Å crystal structure of the “as isolated” rubrerythrin from <Emphasis Type="Italic">Desulfovibrio vulgaris</Emphasis>: some surprising results

Rubrerythrin is a non-heme iron dimeric protein isolated from the sulfate-reducing bacterium Desulfovibrio vulgaris. Each monomer has one mononuclear iron center similar to rubredoxin and one dinuclear metal center similar to hemerythrin or ribonucleotide reductase. The 1.88 A X-ray structure of the "as isolated" molecule and a uranyl heavy atom derivative have been solved by molecular replacement techniques. The resulting model of the native "as isolated" molecule, including 164 water molecules, has been refined giving a final R factor of 0.197 (R(free) = 0.255). The structure has the same general protein fold, domain structure, and dimeric interactions as previously found for rubrerythrin [1, 2], but it also has some interesting undetected differences at the metal centers. The refined model of the protein structure has a cis peptide between residues 78 and 79. The Fe-Cys4 center has a previously undetected strong seventh N-H...S hydrogen bond in addition to the six N-H...S bonds usually found in rubredoxin. The dinuclear metal center has a hexacoordinate Fe atom and a tetracoordinate Zn atom. Each metal is coordinated by a GluXXHis polypeptide chain segment. The Zn atom binds at a site distinctly different from that found in the structure of a diiron rubrerythrin. Difference electron density for the uranyl derivative shows an extremely large peak adjacent to and replacing the Zn atom, indicating that this particular site is capable of binding other atoms. This feature/ability may give rise to some of the confusing activities ascribed to this molecule.