Resonance Raman studies of dioxygen and carbon monoxide binding to imidazole-appended hemes.

Resonance Raman spectroscopy has been employed to probe the effects of proximal base strain on the bonding of O2 and CO in three synthetic hemins with covalently linked imidazole ligands. The strain is introduced by varying the length of the imidazole-containing side chain and by restricting the side chain flexibility with a phenyl ring. These hemins are abbreviated as "long," "short," and "stiff" hemins, respectively. In the deoxy state, the iron-imidazole stretching frequencies [nu(Fe--N epsilon)] for long, short, and stiff hemins are detected at 200, 207, and 204 cm-1, respectively. The strain induced in the iron-imidazole bond by the short hemin results in a higher nu(Fe--N epsilon) frequency, in contrast to the strain induced by sterically hindered 2-methylimidazole or 1,2-dimethylimidazole complexes in which the Fe--N epsilon bond is tilted and lengthened, but the imidazole ring remains perpendicular to the heme plane. However, in the short hemin, the plane of the imidazole ring may not be perpendicular to the plane of the porphyrin, altering the amount of pi-interaction (hence the strength of Fe--N epsilon bond) and the nature of normal mode containing Fe--N epsilon bond stretching. Upon CO binding, we have observed the nu(Fe--CO) stretching frequencies at 497 (long), 499 (short), and 496 cm-1 (stiff), somewhat lower than those reported by Mitchell et al. (Inorg. Chem., 1985, 24:967) for the chelated-heme X CO complexes (i.e., 501-506 cm-1). This is the first report of an iron-oxygen-associated vibration observed in solution for an unprotected heme.(ABSTRACT TRUNCATED AT 250 WORDS)     

Vibrational modes of tyrosines in cytochrome c oxidase from Paracoccus denitrificans: FTIR and electrochemical studies on Tyr-D4-labeled and on Tyr280His and Tyr35Phe mutant enzymes

A combined electrochemical and FTIR spectroscopic approach was used to identify the vibrational modes of tyrosines in cytochrome c oxidase from Paracoccus denitrificans which change upon electron transfer and coupled proton transfer. Electrochemically induced FTIR difference spectra of the Tyr-D4-labeled cytochrome c oxidase reveal that only small contributions arise from the tyrosines. Contributions between 1600 and 1560 cm(-1) are attributed to nu8a/8b(CC) ring modes. The nu19(CC) ring mode for the protonated form of tyrosines is proposed to absorb with an uncommonly small signal at 1525-1518 cm(-1) and for the deprotonated form at 1496-1486 cm(-1), accompanied by the increase of the nu19(CC) ring mode of the Tyr-D(4)-labeled oxidase at approximately 1434 cm(-1). A signal at 1270 cm(-1) can be tentatively attributed to the nu7'a(CO) and delta(COH) mode of a protonated tyrosine. Uncommon absorptions, like the mode at 1524 cm(-1), indicate the involvement of Tyr280 in the spectra. Tyr280 is a crucial residue close to the binuclear center and is covalently bonded to His276. The possible changes of the spectral properties are discussed together with the absorbance spectra of tyrosine bound to histidine. The vibrational modes of Tyr280 are further analyzed in combination with the mutation to histidine, which is assumed to abolish the covalent bonding. The electrochemically induced FTIR difference spectra of the Tyr280His mutant point to a change in protonation state in the environment of the binuclear center. Together with an observed decrease of a signal at 1736 cm(-1), previously assigned to Glu278, a possible functional coupling is reflected. In direct comparison to the FTIR difference spectra of the D4-labeled compound and comparing the spectra at pH 7 and 4.8, the protonation state of Tyr280 is discussed. Furthermore, a detailed analysis of the mutant is presented, the FTIR spectra of the CO adduct revealing a partial loss of Cu(B). Electrochemical redox titrations reflect a downshift of the heme a3 midpoint potential by 95 +/- 10 mV. Another tyrosine identified to show redox dependent changes upon electron transfer is Tyr35, a residue in the proposed D-pathway of the cytochrome c oxidase.     

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.     

Simultaneous resonance Raman detection of the heme a3-Fe-CO and CuB-CO species in CO-bound ba3-cytochrome c oxidase from Thermus thermophilus. Evidence for a charge transfer CuB-CO transition

Understanding of the chemical nature of the dioxygen and nitric oxide moiety of ba3-cytochrome c oxidase from Thermus thermophilus is crucial for elucidation of its physiological function. In the present work, direct resonance Raman (RR) observation of the Fe-C-O stretching and bending modes and the C-O stretching mode of the CuB-CO complex unambiguously establishes the vibrational characteristics of the heme-copper moiety in ba3-oxidase. We assigned the bands at 507 and 568 cm(-1) to the Fe-CO stretching and Fe-C-O bending modes, respectively. The frequencies of these modes in conjunction with the C-O mode at 1973 cm(-1) showed, despite the extreme values of the Fe-CO and C-O stretching vibrations, the presence of the alpha-conformation in the catalytic center of the enzyme. These data, distinctly different from those observed for the caa3-oxidase, are discussed in terms of the proposed coupling of the alpha-and beta-conformations that occur in the binuclear center of heme-copper oxidases with enzymatic activity. The CuB-CO complex was identified by its nu(CO) at 2053 cm(-1) and was strongly enhanced with 413.1 nm excitation indicating the presence of a metal-to-ligand charge transfer transition state near 410 nm. These findings provide, for the first time, RR vibrational information on the EPR silent CuB(I) that is located at the O2 delivery channel and has been proposed to play a crucial role in both the catalytic and proton pumping mechanisms of heme-copper oxidases.     

N-Isotope effects on the Raman spectra of Fe2S2 ferredoxin and Rieske ferredoxin: evidence for structural rigidity of metal sites

The diiron ferredoxins have a common diamond-core structure with two bridging sulfides, but differ in the nature of their terminal ligands: either four cysteine thiolates in the Fe(2)S(2) ferredoxins or two cysteine thiolates and two histidine imidazoles in the Rieske ferredoxins. Contributions of the bridging (b) and terminal (t) ligands to the resonance Raman spectra of the Fe(2)S(2) ferredoxins have been distinguished previously by isotopic substitution of the bridging sulfides. We now find that uniform (15)N-labeling of Anabaena Fe(2)S(2) ferredoxin results in shifts of -1 cm(-1) in the Fe-S(t) stretching modes at 282, 340, and 357 cm(-1). The (15)N dependence is ascribed to kinematic coupling of the Fe-S(Cys) stretch with deformations of the cysteine backbone, including the amide nitrogen. No (15)N dependence occurs for the nu(Fe-S(b)) modes at 395 and 426 cm(-1). Similar effects are observed for the Rieske center in T4MOC ferredoxin from the toluene-4-monooxygenase system of Pseudomonas mendocina. Upon selective (15)N-labeling of the alpha-amino group of cysteine, the vibrational modes at 321, 332, 350, and 362 cm(-1) all undergo shifts of -1 to -2 cm(-1), thereby identifying them as combinations of nu(Fe-S(t)) and delta(Cys). These same four modes undergo similar isotope shifts when T4MOC ferredoxin is selectively labeled with (15)N-histidine ((15)N in either the alpha1,delta1 or delta1,epsilon2 positions). Thus, the Fe-S(Cys) stretch must also be undergoing kinematic coupling with vibrations of the Fe-His moiety. The extensive kinematic coupling of iron ligand vibrations observed in both the Fe(2)S(2) and Rieske ferredoxins presumably arises from the rigidity of the protein framework and is reminiscent of the behavior of cupredoxins. In both cases, the structural rigidity is likely to play a role in minimizing the reorganization energy for electron transfer.     

Mediation of a phase transition in hyaluronate films by the counterions Li, Cs, Mg and Ca as observed by infrared spectroscopy, optical microscopy and optical birefringence

Infrared (IR) spectroscopy and optical microscopy have been performed as a function of relative humidity (rh) on wet-spun oriented films of hyaluronate (HA) prepared with various counterions. Complete swelling measurements have been obtained through optical microscopy for films of Cs-, Mg-, and CaHA. IR spectroscopy of Cs-, Mg-, Ca-, and LiHA films was performed for skeletal vibrations (800-1000 cm(-1)) and for vibrational modes (1150-1300 cm(-1)) attributed to C-C and C-O stretching modes and C-C-H and C-O-H bending modes. These techniques reveal evidence of a counterion-dependent phase transition occuring at high relative humidities. Optical birefringence measurements on the polycrystalline samples showed order before and disorder after the transition from lower to higher humidity.     

Tyrosine Raman signatures of the filamentous virus Ff are diagnostic of non-hydrogen-bonded phenoxyls: demonstration by Raman and infrared spectroscopy of p-cresol vapor

p-Cresol is a simple molecular model for the para phenolic side chain of tyrosine. Previously, Siamwiza and co-workers [(1975) Biochemistry 14, 4870-4876] investigated p-cresol solutions to identify Raman spectroscopic signatures for different hydrogen-bonding states of the tyrosine phenoxyl group in proteins. They found that the phenolic moiety exhibits an intense Raman doublet in the spectral interval 820-860 cm(-1) and that the doublet intensity ratio (I2/I1, where I2 and I1 are Raman peak intensities of the higher- and lower-wavenumber members of the doublet) is diagnostic of specific donor and acceptor roles of the phenoxyl OH group. The range of the doublet intensity ratio in proteins (0.30 < I2/I1 < 2.5) was shown to be governed by Fermi coupling between the phenolic ring-stretching fundamental nu1 and the first overtone of the phenolic ring-deformation mode nu(16a), such that when the tyrosine phenoxyl proton is a strong hydrogen-bond donor, I2/I1 = 0.30, and when the tyrosine phenoxyl oxygen is a strong hydrogen-bond acceptor, I2/I1 = 2.5. Here, we interpret the Raman and infrared spectra of p-cresol vapor and extend the previous correlation to the non-hydrogen-bonded state of the tyrosine phenoxyl group. In the absence of hydrogen bonding, the Raman intensity of the higher-wavenumber component of the canonical Fermi doublet is greatly enhanced such that I2/I1 = 6.7. Thus, for the non-hydrogen-bonded phenoxyl, the lower-wavenumber member of the Fermi doublet loses most of its Raman intensity. This finding provides a basis for understanding the anomalous Raman singlet signature (approximately 854 cm(-1)) observed for tyrosine in coat protein subunits of filamentous viruses Ff and Pf1 [Overman, S. A., et al. (1994) Biochemistry 33, 1037-1042; Wen, Z. Q., et al. (1999) Biochemistry 38, 3148-3156]. The implications of the present results for Raman analysis of tyrosine hydrogen-bonding states in other proteins are considered.     

Structure of a histidine ligand in the photosynthetic oxygen-evolving complex as studied by light-induced fourier transform infrared difference spectroscopy.

Fourier transform infrared (FTIR) signals of a histidine side chain were identified in flash-induced S(2)/S(1) difference spectra of the oxygen-evolving complex (OEC) of photosystem II (PS II) using PS II membranes from globally (15)N-labeled spinach and PS II core complexes from Synechocystis cells in which both the imidazole nitrogens of histidine were selectively labeled with (15)N. A negative band at 1113-1114 cm(-1) was downshifted by 7 cm(-1) upon both global (15)N-labeling and selective [(15)N]His labeling, and assigned to the C-N stretching mode of the imidazole ring. This band was unaffected by H-D exchange in the PS II preparations. In addition, several peaks observed at 2500-2850 cm(-1) all downshifted upon global and selective (15)N-labeling. These were ascribed to Fermi resonance peaks on a hydrogen-bonding N-H stretching band of the histidine side chain. FTIR measurements of model compounds of the histidine side chain showed that the C-N stretching band around 1100 cm(-)(1) can be a useful IR marker of the protonation form of the imidazole ring. The band appeared with frequencies in the following order: Npi-protonated (>1100 cm(-1)) > imidazolate > imidazolium > Ntau-protonated (<1095 cm(-1)). The frequency shift upon N-deuteration was occurred in the following order: imidazolium (15-20 cm(-1)) > Ntau-protonated (5-10 cm(-1)) > Npi-protonated approximately imidazolate ( approximately 0 cm(-1)). On the basis of these findings together with the Fermi resonance peaks at >2500 cm(-1) as a marker of N-H hydrogen-bonding, we concluded that the histidine residue in the S(2)/S(1) spectrum is protonated at the Npi site and that this Npi-H is hydrogen bonded. This histidine side chain probably ligated the redox-active Mn ion at the Ntau site, and thus, oxidation of the Mn cluster upon S(2) formation perturbed the histidine vibrations, causing this histidine to appear in the S(2)/S(1) difference spectrum.     

Electrochemical, FT-IR and UV/VIS spectroscopic properties of the caa3 oxidase from T. thermophilus.

The caa3-oxidase from Thermus thermophilus has been studied with a combined electrochemical, UV/VIS and Fourier-transform infrared (FT-IR) spectroscopic approach. In this oxidase the electron donor, cytochrome c, is covalently bound to subunit II of the cytochrome c oxidase. Oxidative electrochemical redox titrations in the visible spectral range yielded a midpoint potential of -0.01 +/- 0.01 V (vs. Ag/AgCl/3m KCl, 0.218 V vs. SHE') for the heme c. This potential differs for about 50 mV from the midpoint potential of isolated cytochrome c, indicating the possible shifts of the cytochrome c potential when bound to cytochrome c oxidase. For the signals where the hemes a and a3 contribute, three potentials, = -0.075 V +/- 0.01 V, Em2 = 0.04 V +/- 0.01 V and Em3 = 0.17 V +/- 0.02 V (0.133, 0.248 and 0.378 V vs. SHE', respectively) could be obtained. Potential titrations after addition of the inhibitor cyanide yielded a midpoint potential of -0.22 V +/- 0.01 V for heme a3-CN- and of Em2 = 0.00 V +/- 0.02 V and Em3 = 0.17 V +/- 0.02 V for heme a (-0.012 V, 0.208 V and 0.378 V vs. SHE', respectively). The three phases of the potential-dependent development of the difference signals can be attributed to the cooperativity between the hemes a, a3 and the CuB center, showing typical behavior for cytochrome c oxidases. A stronger cooperativity of CuB is discussed to reflect the modulation of the enzyme to the different key residues involved in proton pumping. We thus studied the FT-IR spectroscopic properties of this enzyme to identify alternative protonatable sites. The vibrational modes of a protonated aspartic or glutamic acid at 1714 cm-1 concomitant with the reduced form of the protein can be identified, a mode which is not present for other cytochrome c oxidases. Furthermore modes at positions characteristic for tyrosine vibrations have been identified. Electrochemically induced FT-IR difference spectra after inhibition of the sample with cyanide allows assigning the formyl signals upon characteristic shifts of the nu(C=O) modes, which reflect the high degree of similarity of heme a3 to other typical heme copper oxidases. A comparison with previously studied cytochrome c oxidases is presented and on this basis the contributions of the reorganization of the polypeptide backbone, of individual amino acids and of the hemes c, a and a3 upon electron transfer to/from the redox active centers discussed.     

Structural and chemical changes of the P(M) intermediate of paracoccus denitrificans cytochrome c oxidase revealed by IR spectroscopy with labeled tyrosines and histidine

Structural and chemical changes in the P(M) intermediate of Paracoccus denitrificans cytochrome c oxidase have been investigated by attenuated total reflection-Fourier transform infrared spectroscopy. Prior studies of P(M) minus oxidized (O) IR difference spectra of unlabeled, universally (15)N-labeled and ring-d(4)-tyrosine-labeled proteins (Iwaki, M., Puustinen, A., Wikstr?m, M., and Rich, P. R. (2004) Biochemistry 43, 14370-14378). provided a basis for band assignments to changes in metal centers and the covalently linked His-Tyr ligand of Cu(B) and highlighted a structural alteration of the protonated Glu278 in the P(M) intermediate. This work has been extended to equivalent measurements on enzymes with (13)C(9)(15)N-labeled and ring-(13)C(6)-labeled tyrosine and with (13)C(6)(15)N(3)-labeled histidine. Histidine labeling allows the assignment of troughs at 1104 and 973 cm(-1) in reduced minus O spectra to histidine changes, whereas tyrosine labeling moves otherwise obscured tyrosine bandshifts to 1454-1437 and 1287-1284 cm(-1). P(M) minus O spectra reveal bands at 1506, 1311, and 1094 cm(-1) in the oxidized state that are replaced by a band at 1519 cm(-1) in P(M). These bands shift with both tyrosine- and histidine-labeling, providing evidence for their assignment to the covalent His-Tyr and for its chemical change in P(M). Comparisons of isotope effects on the amide I regions in P(M) minus O spectra demonstrate that amide carbonyl bonds of tyrosine and histidine are major contributors. This suggests a structural alteration in P(M) that is centered on the His276-Pro277-Glu278-Val279-Tyr280 pentapeptide formed by the His-Tyr covalent linkage. This structural change is proposed to mediate the perturbation of the IR band of the protonated Glu278 headgroup.     

Multiple active site conformers in the carbon monoxide complexes of trematode hemoglobins

Sequence alignment of hemoglobins of the trematodes Paramphistomum epiclitum and Gastrothylax crumenifer with myoglobin suggests the presence of an unusual active site structure in which two tyrosine residues occupy the E7 and B10 helical positions. In the crystal structure of P. epiclitum hemoglobin, such an E7-B10 tyrosine pair at the putative helical positions has been observed, although the E7 Tyr is displaced toward CD region of the polypeptide. Resonance Raman data on both P. epiclitum and G. crumenifer hemoglobins show that interactions of heme-bound ligands with neighboring amino acid residues are unusual. Multiple conformers in the CO complex, termed the C, O, and N conformers, are observed. The conformers are separated by a large difference (approximately 60 cm(-1)) in the frequencies of their Fe-CO stretching modes. In the C conformer the Fe-CO stretching frequency is very high, 539 and 535 cm(-1), for the P. epiclitum and G. crumenifer hemoglobins, respectively. The Fe-CO stretching of the N conformer appears at an unusually low frequency, 479 and 476 cm(-1), respectively, for the two globins. A population of an O conformer is seen in both hemoglobins, at 496 and 492 cm(-1), respectively. The C conformer is stabilized by a strong polar interaction of the CO with the distal B10 tyrosine residue. The O conformer is similar to the ones typically seen in mutant myoglobins in which there are no strong interactions between the CO and residues in the distal pocket. The N conformer possesses an unusual configuration in which a negatively charged group, assigned as the oxygen atom of the B10 Tyr side chain, interacts with the CO. In this conformer, the B10 Tyr assumes an alternative conformation consistent with one of the conformers seen the crystal structure. Implications of the multiple configurations on the ligand kinetics are discussed.     

Binding of NO and CO to the d(1) Heme of cd(1) nitrite reductase from Pseudomonas aeruginosa

The cd(1) nitrite reductase, a key enzyme in bacterial denitrification, catalyzes the one-electron reduction of nitrite to nitric oxide. The enzyme contains two redox centers, a c-type heme and a unique d(1) heme, which is a dioxoisobacteriochlorin. Nitric oxide, generated by this enzymatic pathway, if not removed from the medium, can bind to the ferrous d(1) cofactor with extremely high affinity and inhibit enzyme activity. In this paper, we report the resonance Raman investigation of the properties of nitric oxide and carbon monoxide binding to the d(1) site of the reduced enzyme. The Fe-ligand (Fe-NO and Fe-CO) stretching vibrational frequencies are unusually high in comparison to those of other ferrous heme complexes. The frequencies of the Fe-NO and N-O stretching modes appear at 585 and 1626 cm(-1), respectively, in the NO complex, while the frequencies of the Fe-CO and C-O stretching modes are at 563 and 1972 cm(-1), respectively, for the CO complex. Also, the widths (fwhm) of the Fe-CO and C-O stretching modes are smaller than those observed in the corresponding complexes of other heme proteins. The unusual spectroscopic characteristics of the d(1) cofactor are discussed in terms of both its unique electronic properties and the strongly polar distal environment around the iron-bound ligand. It is likely that the influence of a highly ruffled structure of heme d(1) on its electronic properties is the major factor causing anomalous Fe-ligand vibrational frequencies.     

Heme environment in aldoxime dehydratase involved in carbon-nitrogen triple bond synthesis

Resonance Raman spectra have been measured to characterize the heme environment in aldoxime dehydratase (OxdA), a novel hemoprotein, which catalyzes the dehydration of aldoxime into nitrile. The spectra showed that the ferric heme in the enzyme is six-coordinate low spin, whereas the ferrous heme is five-coordinate high spin. We assign a prominent vibration that occurs at 226 cm(-1) in the ferrous enzyme to the Fe-proximal histidine stretching vibration. In the CO-bound form of OxdA, the correlation between the Fe-CO stretching (512 cm(-1)) and C-O stretching (1950 cm(-1)) frequencies also supports our assignment of proximal histidine coordination.     

Orientations of Tyr 21 and Tyr 24 in the capsid of filamentous virus Ff determined by polarized Raman spectroscopy

The capsid of filamentous virus Ff is assembled from approximately 2750 copies of a 50-residue alpha-helical subunit, the two tyrosines of which (Tyr 21 and Tyr 24) are located within a hydrophobic sequence that constitutes the subunit interface. We have determined the side chain orientations of Tyr 21 and Tyr 24 by polarized Raman microspectroscopy of oriented Ff fibers, utilizing a novel experimental approach that combines site-specific mutation and residue-specific deuteration of capsid subunits. The polarized Raman signature of Tyr 21 was obtained by incorporating C(delta 1),C(delta 2),C(epsilon 1),C(epsilon 2)-tetradeuteriotyrosine at position 21 in an Ff mutant in which Tyr 24 is replaced with methionine. Similarly, the polarized Raman signature of Tyr 24 was obtained by incorporating C(delta 1),C(delta 2),C(epsilon 1),C(epsilon 2)-tetradeuteriotyrosine at position 24 in the analogous Tyr 21 --> Met mutant. Polarizations of the corresponding C-D stretching bands in the 2200-2400 cm(-1) interval of the Raman spectrum were measured and interpreted using tensors transferred from a polarized Raman analysis of L-tyrosine-2,3,5,6-d(4) single crystals. Polarized Raman analysis was extended to the bands of Ff near 642 and 855 cm(-1), which originate from vibrational modes of the tyrosine phenolic ring. The results indicate the following: (i) For both Tyr 21 and Tyr 24, the phenolic 2-fold axis (C(1)-C(4) line) is inclined at 41 +/- 5 degrees from the virion axis and the normal to the plane of the phenolic ring is inclined at 71 +/- 5 degrees from the virion axis; (ii) the mutation of Tyr 24, but not the mutation of Tyr 21, perturbs Raman markers of the subunit tryptophan (Trp 26), suggesting interdependence of Tyr 24 and Trp 26 orientations in native Ff; and (iii) polarization anisotropies observed for Raman markers of Ff DNA bases are unperturbed by mutation of either Tyr 21 or Tyr 24, indicating that nonrandom base orientations of packaged Ff DNA are independent of the mutation of either Tyr 21 or Tyr 24. A molecular model consistent with these findings is proposed.     

Characteristic changes of the S2/S1 difference FTIR spectrum induced by Ca2+ depletion and metal cation substitution in the photosynthetic oxygen-evolving complex

Effects of Ca2+ depletion and substitution with other metal cations on the structure of the protein matrices of the oxygen-evolving complex (OEC) and their corresponding changes upon the S1 to S2 transition were examined using Fourier transform infrared (FTIR) spectroscopy. Ca2+ depletion and further supplementation with Li+, Na+, Mg2+, Ca2+, or Sr2+ did not significantly affect the typical vibrational features in the double difference S2/S1 spectrum, including the symmetric [1365(+)/1404(-) cm(-1)] and the asymmetric [1587(+)/1566(-) cm(-1)] stretching modes of the carboxylate ligand and the amide I and II modes of the backbone polypeptides. On the other hand, supplementation with K+, Rb+, Cs+, or Ba2+ significantly modified the S2/S1 spectrum, in which the carboxylate modes disappeared and the amide I and II modes were modified. Results indicate that the binding of metal cations that have ionic radii larger than that of Ca2+ to the Ca2+ site induces perturbations in the protein matrices in the vicinity of the Mn cluster to interrupt the characteristic structural and/or conformational changes upon the oxidation of the Mn cluster accompanied with the S1 to S2 transition. The spectrum was also altered by the supplementation of Cd2+, which has an ionic radius comparable to that of Ca2+. A single-pulse-induced S2/S1 difference spectrum revealed that bands that have been assigned to the vibrational modes for the Y(Z) tyrosine and the histidine ligand for the Mn cluster were not induced in the K+-supplemented membranes, although the histidine band is likely to be preserved in the Ca2+-depleted membranes. The Y(Z) band was considerably small in the double difference S2/S1 spectrum in the Ca2+-depleted and the cation-substituted membranes but distinctively present in the Sr2+- or Ca2+-replenished membranes. Furthermore, cation supplementation induced several new bands that disappeared following the Ca2+ replenishment. These results suggest that the proper organization of the hydrogen bond network within OEC for the water oxidation chemistry requires the Ca2+ ion and indicate that the role of Ca2+ is not purely structurally defined by the physical properties of the ion, such as valence and ionic radius. On the basis of these and other findings, we propose that Ca2+ is necessary for the formation of the hydrogen bond network that is involved in the reaction step of water oxidation.     

Unique ligand-protein interactions in a new truncated hemoglobin from Mycobacterium tuberculosis

A new truncated hemoglobin (HbO) from Mycobacterium tuberculosis has been expressed and purified. Sequence alignment of HbO with other hemoglobins suggests that the proximal F8 residue is histidine and the distal E7 and the B10 positions are occupied by alanine and tyrosine, respectively. The highly conserved residue at the CD1 position, surprisingly, is tyrosine, making HbO the first exception in the hemoglobin family that does not contain phenylalanine at this position. Resonance Raman data suggest that a strong hydrogen bonding network, involving the B10 Tyr and the CD1 Tyr, stabilizes the heme-bound O2 and CO as evidenced by the relatively low frequency of the Fe-O2 stretching mode (559 cm(-1)) and the high frequency of the Fe-CO stretching mode (527 cm(-1)). The presence of this hydrogen bonding network is supported by mutagenesis studies with the B10 tyrosine or the CD1 tyrosine mutated to phenylalanine. Taken together, these data demonstrate a rigid and polar distal pocket in HbO, which is significantly different from that of HbN, the other hemoglobin from M. tuberculosis. The distinct features in the heme active site structures and the temporal expression patterns of HbO and HbN suggest that these two hemoglobins may have very different physiological functions.     

Origin of the anomalous Fe-CO stretching mode in the CO complex of Ascaris hemoglobin

We report an unusually high frequency (543 cm(-)(1)) for an Fe-CO stretching mode in the CO complex of Ascaris suum hemoglobin as compared to vertebrate hemoglobins in which the frequency of the Fe-CO mode is much lower. A second Fe-CO stretching mode in Ascaris hemoglobin is observed at 515 cm(-1). We propose that these two Fe-CO stretching modes arise from two protein conformers corresponding to interactions of the heme-bound CO with the B10-tyrosine or the E7-glutamine residues. This postulate is supported by spectra from the B10-Tyr --> Phe mutant in which the 543 cm(-1) line is absent. Thus, a strong polar interaction, such as hydrogen bonding, of the CO with the distal B10 tyrosine residue is the dominant factor that causes this anomalously high frequency. Strong hydrogen bonding between O(2) and distal residues in the oxy complex of Ascaris hemoglobin has been shown to result in a rigid structure, rendering an extremely low oxygen off rate [Gibson, Q. H., and Smith, M. H. (1965) Proc. R. Soc. London B 163, 206-214]. In contrast, the CO off rate in Ascaris hemoglobin is very similar to that in sperm whale myoglobin. The high CO off rate relative to that of O(2) in Ascaris hemoglobin is attributed to a rapid equilibrium between the two conformations of the protein in the CO adduct, with the off rate being determined by the conformer with the higher rate.     

Infrared spectroscopic analysis of tumor pathology

Infrared spectra of normal and malignant breast tissues were measured in the 600 cm(-1) to 4000 cm(-1) region. The measured spectroscopic features which are the spectroscopic fingerprints of the tissues contain the vital information about the malignant and normal tissues. Fourier Transform Infrared (FTIR) data on 25 cases of infiterating ductal carcinoma of breast with different grades of malignancy from patients of different age groups were analyzed. The samples were taken from the tumor sections of the tissue removed during surgery. Infrared spectra demonstrate significant spectral differences between the normal and the cancerous breast tissues. In particular changes in frequency and intensity in the spectra of protein, nucleic acid and glycogen vibrational modes as well as the band intensity ratios for lipid/proteins, protein/nucleic acids, protein/glycogen were observed. This allows to make a qualitative and semi quantitative evaluation of the changes in proliferation activity from normal to diseased tissue. It was evident that the sample to sample or patient to patient variations were small and the spectral differences between normal and diseased tissues were reproducible. The findings establish a framework for additional studies, which may enable us to establish a relation of the diseased state with its infrared spectra.     

Sensory mechanism of oxygen sensor FixL from Rhizobium meliloti: crystallographic, mutagenesis and resonance Raman spectroscopic studies

FixL of Rhizobium meliloti (RmFixL) is a sensor histidine kinase of the two-component system, which regulates the expression of the genes related to nitrogen fixation in the root nodule in response to the O(2) levels. The crystal structure of the sensor domain of FixL (RmFixLH), which contains a heme (Fe-porphyrin) as a sensing site, was determined at 1.4 A resolution. Based on the structural and spectroscopic analyses, we propose the O(2) sensing mechanism that differs from the case proposed in BjFixLH as follows; conformational changes in the F/G loop, which are induced by steric repulsion between the bent-bound O(2) and the Ile209 side-chain, would be transmitted to the histidine kinase domain. Interaction between the iron-bound O(2) and Ile209 was also observed in the resonance Raman spectra of RmFixLH as evidenced by the fact that the Fe-O(2) and Fe-CN stretching frequencies were shifted from 575 to 570 cm(-1) (Fe-O(2)), and 504 to 499 cm(-1), respectively, as the result of the replacement of Ile209 with an Ala residue. In the I209A mutant of RmFixL, the O(2) sensing activity was destroyed, thus confirming our proposed mechanism.     

Could the tyrosine-histidine ligand to Cu<Subscript>B</Subscript> in cytochrome<Emphasis Type="Italic"> c</Emphasis> oxidase be coordinatively labile? Implications from a quantum chemical model study of histidine substitutional lability and the effects of the covalent tyrosine-histidine cross-link

Density functional theory calculations have been used to evaluate the effects of inter-ring interactions within a covalently linked histidine-tyrosine cofactor such as that which is a ligand to the Cu(B) centre in cytochrome c oxidases and to investigate the energetics of histidine substitution at the Cu(B) centre. Small, but significant, perturbations of the redox potentials and/or p K(a) values of the histidine imidazole, the tyrosine phenol and the copper ion are found. The Cu(B)-N(cofactor) bond is estimated to be weaker than the Cu(B)-N(histidine coligand) bonds in the Cu(B)(I) state and in the Cu(B) (II) state when the cofactor is oxidized, by approximately 13 kJ/mol and approximately 23 kJ/mol, respectively. The calculations reveal that displacement of a histidine ligand from the Cu(B) centre, as is suggested in proposals of "histidine cycle" mechanisms for proton pumping in cytochrome c oxidases, is only energetically feasible if accompanied by protonation of the histidine imidazole and coupled to an endothermic process. It is proposed that the histidine-tyrosine cofactor ought to be considered as the substitutionally labile ligand to Cu(B) as the covalent crosslink would ensure displacement of the cofactor from Cu(B)-driven helix deformation. It is estimated that this process could store up to approximately 70 kJ/mol, which, based upon thermodynamic considerations, is sufficient for the pumping of two protons in the later steps (reductive phase) of the catalytic cycle. Ramifications of this proposition for the mechanism of proton pumping in cytochrome c oxidases are discussed.