pH- and thermal-dependent conformational transition of PGAIPG, a repeated hexapeptide sequence from tropoelastin

The secondary structure of PGAIPG (Pro-Gly-Ala-IIe-Pro-Gly), a repeated hexapeptide of tropoelastin, in buffer solution of different pH was determined by using attenuated total reflection-Fourier transform infrared (ATR-FTIR) spectroscopy. The thermal-dependent structural change of PGAIPG in aqueous solution or in solid state was also examined by thermal FTIR microspectroscopy. The conformation of PGAIPG in aqueous solution exhibited a pH-dependent structural characterization. A predominant peak at 1614 cm(-1) (aggregated beta-sheet) with a shoulder near 1560 cm(-1) (beta-sheet) appeared in pH 5.5-8.5 buffer solutions. A new broad shoulder at 1651 cm(-1) (random coil and/or alpha-helix) with 1614 cm(-1) was observed in the pH 4.5 buffer solution. However, the broad shoulder at 1651 cm(-1) was converted to a maximum peak at 1679 cm(-1) (beta-turn/antiparallel beta-sheet) when the pH shifted from 4.5 to 3.5, but the original pronounced peak at 1614 cm(-1) became a shoulder. Once the pH was lowered to 2.5, the IR spectrum of PGAIPG was dominated by major absorption at 1679 cm(-1) with a minor peak at 1552 cm(-1) (alpha-helix/random coil). The result indicates that the pH was a predominant factor to transform PGAIPG structure from aggregated beta-sheet (pH 8.5) to beta-turn/intermolecular antiparallel beta-sheet (pH 2.5). Moreover, a partial conformation of PGAIPG with minor alpha-helix/random coil structures was also explored in the lower pH buffer solution. There was no thermal-dependent structural change for solid-state PGAIPG. The thermal-induced formation of aggregated beta-sheet for PGAIPG in aqueous solution was found from 28 to 30 degrees C, however, which might be correlated with the formation of an opaque gel that turned from clear solution. The formation of aggregated beta-sheet structure for PGAIPG beyond 30 degrees C might be due to the intermolecular hydrogen bonded interaction between the hydrophobic PGAIPG fragments induced by coacervation.     

Resonance raman studies of oxo intermediates in the reaction of pulsed cytochrome bo with hydrogen peroxide

Cytochrome bo from Escherichia coli, a member of the heme-copper terminal oxidase superfamily, physiologically catalyzes reduction of O(2) by quinols and simultaneously translocates protons across the cytoplasmic membrane. The reaction of its ferric pulsed form with hydrogen peroxide was investigated with steady-state resonance Raman spectroscopy using a homemade microcirculating system. Three oxygen-isotope-sensitive Raman bands were observed at 805/X, 783/753, and (767)/730 cm(-)(1) for intermediates derived from H(2)(16)O(2)/H(2)(18)O(2). The experiments using H(2)(16)O(18)O yielded no new bands, indicating that all the bands arose from the Fe=O stretching (nu(Fe)(=)(O)) mode. Among them, the intensity of the 805/X cm(-)(1) pair increased at higher pH, and the species giving rise to this band seemed to correspond to the P intermediate of bovine cytochrome c oxidase (CcO) on the basis of the reported fact that the P intermediate of cytochrome bo appeared prior to the formation of the F species at higher pH. For this intermediate, a Raman band assignable to the C-O stretching mode of a tyrosyl radical was deduced at 1489 cm(-)(1) from difference spectra. This suggests that the P intermediate of cytochrome bo contains an Fe(IV)=O heme and a tyrosyl radical like compound I of prostaglandin H synthase. The 783/753 cm(-)(1) pair, which was dominant at neutral pH and close to the nu(Fe)(=)(O) frequency of the oxoferryl intermediate of CcO, presumably arises from the F intermediate. On the contrary, the (767)/730 cm(-)(1) species has no counterpart in CcO. Its presence may support the branched reaction scheme proposed previously for O(2) reduction by cytochrome bo.     

Pressure-induced transformation of alpha-helix to beta-sheet in the secondary structures of amyloid beta (1-40) peptide exacerbated by temperature

The effect of pressure on the conformational structure of amyloid beta (1-40) peptide (A beta(1-40)), exacerbated with or without temperature, was determined by Fourier transform infrared (FT-IR) microspectroscopy. The result indicates the shift of the maximum peak of amide I band of intact solid A beta(1-40) from 1655 cm(-1) (alpha-helix) to 1647-1643 cm(-1) (random coil) with the increase of the mechanical pressure. A new peak at 1634 cm(-1) assigned to beta-antiparallel sheet structure was also evident. Furthermore, the peak at 1540 cm(- 1) also shifted to 1527 (1529) cm(-1) in amide II band. The former was assigned to the combination of alpha-helix and random coil structures, and the latter was due to beta-sheet structure. Changes in the composition of each component in the deconvoluted and curve-fitted amide I band of the compressed A beta(1-40) samples were obtained from 33% to 22% for alpha-helix/random coil structures and from 47% to 57% for beta-sheet structure with the increase of pressure, respectively. This demonstrates that pressure might induce the conformational transition from alpha-helix to random coil and to beta- sheet structure. The structural transformation of the compressed A beta(1-40) samples was synergistically influenced by the combined effects of pressure and temperature. The thermal-induced formation of beta-sheet structure was significantly dependent on the pressures applied. The smaller the pressure applied the faster the beta-sheet structure transformed. The thermal-dependent transition temperatures of solid A beta(1-40) prepared by different pressures were near 55-60 degrees C.     

Conformational study of globulin from rice (Oryza sativa) seeds by Fourier-transform infrared spectroscopy

The conformation of rice globulin (10%, w/v, in deuterated phosphate buffer, pD 7.4) under the influence of pH, chaotropic salts, several protein structure perturbants and heat treatments was studied by Fourier-transform infrared (FTIR) spectroscopy. Rice globulin exhibited seven major bands in the region of 1700-1600 cm-1 and the spectrum suggests high alpha-helical content with large quantities of beta-sheet and beta-turn structures. Highly acidic and alkaline pH conditions induced changes in band intensity attributed to intermolecular beta-sheet structure (1681 and 1619 cm-1). Addition of chaotropic salts led to progressive changes in band intensity, following the lyotropic series of anions, whereas several protein structure perturbants caused shifts in band positions. Heating at increasing temperature led to progressive decreases in alpha-helical content and increases in random coil structures, suggesting protein denaturation. This was accompanied by intensity increases in the intermolecular beta-sheet transitions.     

Thermal-induced changes in the secondary conformation of superoxide dismutase containing different metal ions

The thermal stability of three superoxide dismutases (SODs) with different metal ions (Mn, Cu/Zn, Fe) in the solid state was studied by a Fourier transform infrared (FT-IR) microspectroscopy combined with thermal analyzer. The IR spectra showed a maximum peak at 1652 cm(-1) for all the native SODs in the amide I band, suggesting a predominant random coil with less alpha-helix structures. By heating each sample, a shoulder at 1631 cm(-1) in the amide I band gradually appeared from 45 degrees C for Fe SOD and from 50 degrees C for Mn SOD but another shoulder at 1639 cm(-1) appeared from 50 degrees C for Cu/Zn SOD. The peak at 1631 cm(-1) is due to the intermolecular beta-sheet structure, but the peak at 1639 cm(-1) corresponds to the major intramolecular beta-sheet with less random coil structure. This reveals that in the first heating process the transformation from random coil/alpha-helix structure to beta-sheet structure initiated from around 45-50 degrees C. There was about 16-22% compositional change resulting from that transformation. However, both additional shoulders stood there and did not restore to their original spectra even with cooling to room temperature, suggesting the denaturation and irreversible properties of the solid SODs after heating. The thermal-dependent denaturation and irreversibility of Mn SOD, Cu/Zn SOD and Fe SOD were clearly evidenced by the increase in intramolecular and intermolecular beta-sheet structure.     

Redox infrared markers of the heme and axial ligands in microperoxidase: bases for the analysis of c-type cytochromes

Structural changes accompanying the change in the redox state of microperoxidase-8 (MP8), the heme-octapeptide obtained from cytochrome c, and its complexes with (methyl)imidazole ligands were studied by electrochemically induced Fourier transform IR (FTIR) difference spectroscopy. To correlate with confidence IR modes with a specific electronic state of the iron, we used UV-vis and electron paramagnetic resonance spectroscopy to define precisely the heme spin state in the samples at the millimolar concentration of MP8 required for FTIR difference spectroscopy. We identified four intense redox-sensitive IR heme markers, nu38 at 1,569 cm(-1) (ox)/1,554 cm(-1) (red), nu42 at 1,264 cm(-1) (ox)/1,242 cm(-1) (red), nu43 at 1,146 cm(-1) (ox), and nu44 at 1,124-1,128 cm(-1) (ox). The intensity of nu42 and nu43 was clearly enhanced for low-spin imidazole-MP8 complexes, while that of nu44 increased for high-spin MP8. These modes can thus be used as IR markers of the iron spin state in MP8 and related c-type cytochromes. Moreover, one redox-sensitive band at 1,044 cm(-1) (red) is attributed to an IR marker specific of c-type hemes, possibly the delta(CbH3)(2,4) heme mode. Other redox-sensitive IR bands were assigned to the MP8 peptide backbone and to the fifth and sixth axial heme ligands. The distinct IR frequencies for imidazole (1,075 cm(-1)) and histidine (1,105 cm(-1)) side chains in the imidazole-MP8 complex allowed us to provide the first direct determination of their pKa at pH 9 and 12, respectively.     

Conformation transition kinetics of regenerated Bombyx mori silk fibroin membrane monitored by time-resolved FTIR spectroscopy

The ethanol-induced conformation transition of regenerated Bombyx mori silk fibroin membrane from a poorly defined to the well ordered state was monitored by time-resolved Fourier transform infrared spectroscopy (FTIR) for the first time. From the analysis of FTIR difference spectra, taken on time scales as short as 6 s and up to 1 h after addition of ethanol, intensity vs. time plots of an increasing band at 1618 cm(-1) were observed indicating formation of a beta-sheet coincident with the loss of intensity of a band at 1668 cm(-1) indicating decreases of random coil and/or silk I structure. Both infrared markers were fitted with identical biphasic exponential decay functions, however, there was a clear burst phase occurring prior to the onset of the observed transitions. The conformation transition process is indicated to either proceed sequentially through (at least) two intermediate states that contain different levels of beta-sheet structure or to have parallel pathways of initial beta-sheet formation followed by a slower 'perfection' phase. The first observed process forms in a burst phase a few seconds after mixing (or even faster), prior to the collection of the first spectrum at 6 s. The second observed process occurs with a time constant of approximately 0.5 min, the intermediate present at this stage then continues with a time constant of 5.5 min completing the observed formation of the beta-sheet. The conformation transition of this slower intermediate is not only indicated by an analysis of the kinetics of the random coil and beta-sheet-specific bands discussed above, it roughly coincides with the appearance of an additional infrared marker at 1695 cm(-1), which may be a marker for beta-sheet structure specific to the formation of the perfected structure. The conformation transition of this protein analyzed by infrared spectroscopy provides insight into a part of the fascinating process of cocoon formation in B. mori.     

Topology of sarcoplasmic reticulum Ca2+-ATPase: an infrared study of thermal denaturation and limited proteolysis.

Sarcoplasmic reticulum Ca2+-ATPase structure and organization in the membrane has been studied by infrared spectroscopy by decomposition of the amide I band. Besides the component bands assignable to secondary structure elements such as alpha-helix, beta-sheet, etc...., two unusual bands, one at 1,645 cm(-1) in H2O buffer and the other at 1,625 cm(-1) in D2O buffer are present. By perturbing the protein using temperature and limited proteolysis, the band at 1,645 cm(-1) is tentatively assigned to alpha-helical segments located in the cytoplasmic domain and coupled to beta-sheet structure, whereas the band at 1,625 cm(-1) arises probably from monomer-monomer contacts in the native oligomeric protein. The secondary structure obtained is 33% alpha-helical segments in the transmembrane plus stalk domain; 20% alpha-helix and 22% beta-sheet in the cytoplasmic domain plus 19% turns and 6% unordered structure. Thermal unfolding of Ca2+-ATPase is a complex process that cannot be described as a two-state denaturation. The results obtained are compatible with the idea that the protein is an oligomer at room temperature. The loss of the 1,625 cm(-1) band upon heating would be consistent with a disruption of the oligomers in a process that later gives rise to aggregates (appearance of the 1,618 cm(-1) band). This picture would also be compatible with early results suggesting that processes governing Ca2+ accumulation and ATPase activity are uncoupled at temperatures above 37 degrees C, so that while ATPase activity proceeds at high rates, Ca2+ accumulation is inhibited.     

Resonance Raman characterization of the P intermediate in the reaction of bovine cytochrome c oxidase

Reduced cytochrome c oxidase binds molecular oxygen, yielding an oxygenated intermediate first (Oxy) and then converts it to water via the reaction intermediates of P, F, and O in the order of appearance. We have determined the iron-oxygen stretching frequencies for all the intermediates by using time-resolved resonance Raman spectroscopy. The bound dioxygen in Oxy does not form a bridged structure with Cu(B) and the rate of the reaction from Oxy to P (P(R)) is slower at higher pH in the pH range between 6.8 and 8.0. It was established that the P intermediate has an oxo-heme and definitely not the Fe(a(3))-O-O-Cu(B) peroxy bridged structure. The Fe(a(3))=O stretching (nu(Fe=O)) frequency of the P(R) intermediate, 804/764 cm(-1) for (16)O/(18)O, is distinctly higher than that of F intermediate, 785/750 cm(-1). The rate of reaction from P to F in D(2)O solution is evidently slower than that in H(2)O solution, implicating the coupling of the electron transfer with vector proton transfer in this process. The P intermediate (607-nm form) generated in the reaction of oxidized enzyme with H(2)O(2) gave the nu(Fe=O) band at 803/769 cm(-1) for H(2)(16)O(2)/H(2)(18)O(2) and the simultaneously measured absorption spectrum exhibited the difference peak at 607 nm. Reaction of the mixed valence CO adduct with O(2) provided the P intermediate (P(M)) giving rise to an absorption peak at 607 nm and the nu(Fe=O) bands at 804/768 cm(-1). Thus, three kinds of P intermediates are considered to have the same oxo-heme a(3) structure. The nu(4) and nu(2) modes of heme a(3) of the P intermediate were identified at 1377 and 1591 cm(-1), respectively. The Raman excitation profiles of the nu(Fe=O) bands were different between P and F. These observations may mean the formation of a pi cation radical of porphyrin macrocycle in P.     

Structural changes due to the deprotonation of the proton release group in the M-photointermediate of bacteriorhodopsin as revealed by time-resolved FTIR spectroscopy

One of the steps in the proton pumping cycle of bacteriorhodopsin (BR) is the release of a proton from the proton-release group (PRG) on the extracellular side of the Schiff base. This proton release takes place shortly after deprotonation of the Schiff base (L-to-M transition) and results in an increase in the pKa of Asp85, which is a crucial mechanistic step for one-way proton transfer for the entire photocycle. Deprotonation of the PRG can also be brought about without photoactivation, by raising the pH of the enzyme (pKa of PRG; approximately 9). Thus, comparison of the FTIR difference spectrum for formation of the M intermediate (M minus initial unphotolyzed BR state) at pH 7 to the corresponding spectrum generated at pH 10 may reveal structural changes specifically associated with deprotonation of the PRG. Vibrational bands of BR that change upon M formation are distributed across a broad region between 2120 and 1685 cm(-1). This broad band is made up of two parts. The band above 1780 cm(-1), which is insensitive to C15-deuteration of the retinal, may be due to a proton delocalized in the PRG. The band between 1725 and 1685 cm(-1), on the lower frequency side of the broad band, is sensitive to C15-deuteration. This band may arise from transition dipole coupling of the vibrations of backbone carbonyl groups in helix G with the side chain of Tyr57 and with the C15H of the Schiff base. In M, these broad bands are abolished, and the 3657 cm(-1) band, which is due to the disruption of the hydrogen bonding of a water molecule, probably with Arg82, appears. Loss of the interaction of the backbone carbonyl groups in helix G with Tyr57 and the Schiff base, and separation of Tyr57 from Arg82, may be causes of these spectral changes, leading to the stabilization of the protonated Asp85 in M.     

A new approach for determining the stability of recombinant human epidermal growth factor by thermal Fourier transform infrared (FTIR) microspectroscopy

Based on Fourier transform infrared (FTIR) microspectroscopy, the conformation of rhEGF under the influence of pH, heat treatment, chaotropic salts, concentration of salt and protein structure perturbants was studied. The FTIR spectrum of rhEGF showed that major secondary structures from amide I bands composed of 40.6% beta-sheets, 25.0% reverse turns, 16.5% random coils, 13.0% loops and 4.9% side-chain structures. At extreme pH conditions (pH < 4 and pH > 8), there were changes in intensity of the bands attributed to loop (1658 cm(-1)) and random coil structures, and these bands shifted to lower wavenumbers, indicating changes in protein conformation. Thermal denaturation of rhEGF occurred at 40-76 degrees C and the formation of intermolecular beta-aggregates was revealed by the FTIR spectra. Thermal-irreversible property of rhEGF after second-heating treatment suggested that rhEGF has a poor thermal stability. While investigating the stability of rhEGF in the presence of chaotropic salts, anions induced protein unfolding of rhEGF more significantly than cations. The optimal stabilizing effect was found at the 2 M NaCl added to rhEGF, and expressed the structure of rhEGF more stable on the many components. The bands of loop structure (1654 cm(-1)), beta-sheet (1638 cm(-1)) and intermolecular antiparallel beta-aggregation formation (1694, 1619 and 1612 cm(-1)) seem to be "marked" to be more sensitive in determining environmental changes of rhEGF for FTIR microspectroscopy.     

Induced optical activity in poly-L-lysine-methyl orange system

The absorption and cicular dichroism spectra of the complex of poly-L -lysine (PLL) in the random coil form with methyl orange (MO) have been measured in aqueous solution. A new absorption band is observed at the shorter wavelength compared with that of the free dye. Although MO does not show a formation of dimer or aggregation with an increase in concentration, circular dichroism bands are observed at the wavelength corresponding to the wavelength of the new absorption band. These induced circular dichroism bands may arise from the dimeric MO molecules bound to PLL in the random coil form. The main contribution to the interaction between MO molecules is shown to be the electro static interaction. The observed circular dichroism spectra and the configuration of dimeric MO molecules bound to PLL can be explained by the dipole couping mechanism.     

Micro-Raman characterisation of the R to T state transition of haemoglobin within a single living erythrocyte

We present the first recorded Raman spectra of haemoglobin in both the R and T states from within a single living erythrocyte using 632.8 nm excitation. Bands characteristic of low spin haems are observed in oxygenated and carboxylated erythrocytes at approx. 1636 (nu(10)), 1562-1565 (nu(2)), 1250-1245 cm(-1) (nu(13)) and 1226-1224 cm(-1) (nu(5)+nu(8)). The spectra of deoxygenated and methaemoglobin erythrocytes have characteristic high spin bands at approx. 1610-1606 cm(-1) (nu(10)), 1582-1580 (nu(37)), 1547-1544 (nu(11)), 1230-1220 cm(-1) (nu(13)) and 1215-1210 cm(-1) (nu(5)+nu(8)). Bands at 1172 (nu(30)), 976 (nu(45)) and 672 (nu(7)) cm(-1) appear to be enhanced at 632.8 nm in low spin haems. The oxidation state marker band (nu(4)) at 1364-1366 cm(-1) appeared invariant within this domain in all single cells and conditions investigated contrary to other resonance Raman studies on haem isolates. The information gained by in vivo single erythrocyte molecular analysis has important ramifications to the understanding of fundamental physiological processes and may have applications in the diagnosis and treatment of red blood cell disorders.     

Phosphoenzyme conversion of the sarcoplasmic reticulum Ca(2+)-ATPase. Molecular interpretation of infrared difference spectra.

Time-resolved Fourier transform infrared difference spectra of the phosphoenzyme conversion and Ca(2+) release reaction (Ca(2)E(1)-P --> E(2)-P) of the sarcoplasmic reticulum Ca(2+)-ATPase were recorded at pH 7 and 1 degrees C in H(2)O and (2)H(2)O. In the amide I spectral region, the spectra indicate backbone conformational changes preserving conformational changes of the preceding phosphorylation step. beta-sheet or turn structures (band at 1685 cm(-1)) and alpha-helical structures (band at 1653 cm(-1)) seem to be involved. Spectra of the model compound EDTA for Ca(2+) chelation indicate the assignment of bands at 1570, 1554, 1411 and 1399 cm(-1) to Ca(2+) chelating Asp and Glu carboxylate groups partially shielded from the aqueous environment. In addition, an E(2)-P band at 1638 cm(-1) has been tentatively assigned to a carboxylate group in a special environment. A Tyr residue seems to be involved in the reaction (band at 1517 cm(-1) in H(2)O and 1515 cm(-1) in (2)H(2)O). A band at 1192 cm(-1) was shown by isotopic replacement in the gamma-phosphate of ATP to originate from the E(2)-P phosphate group. This is a clear indication that the immediate environment of the phosphoenzyme phosphate group changes in the conversion reaction, altering phosphate geometry and/or electron distribution.     

Carbonmonoxy horseradish peroxidase as a function of pH and substrate: influence of local electric fields on the optical and infrared spectra

Infrared and optical spectra of carbonmonoxy horseradish peroxidase were monitored as a function of pH and substrate binding. The analyses of experimental results together with semiempirical calculations show that the CO-porphyrin complex is sensitive to environmental changes. The electronic Q(0,0) band of the porphyrin and the CO stretching mode respond to external perturbations with different symmetry dependencies. In this way, the complex is nonisotropic, and the combined spectral analyses constitute a valuable tool for the investigation of structure. In the absence of substrate and at pH 6.0, the low-spin heme optical Q(0,0) absorption band is a single peak that narrows as the temperature decreases. Under these conditions, the CO vibrational stretch frequency is at 1903 cm(-1). Addition of the substrates benzohydroxamic acid or naphthohydroxamic acid produces a split of approximately 320 cm(-1) in the Q(0,0) absorption band that is clearly evident at < 100 K and shifts the CO absorption to 1916 cm(-1). Increasing the pH to 9.3 also causes a split in the Q(0,0) optical band and elicits a shift in nu(CO) to a higher frequency (1936 cm(-1)). The splitting of the Q(0,0) band and the shifts in the IR spectra are both consistent with changes in the local electric field produced by the proximity of the electronegative carbonyl of the substrate near the heme or the protonation and/or deprotonation of the distal histidine, although other effects are also considered. The larger effect on the Q(0,0) band with substrate at low pH and the shift of nu(CO) at high pH can be rationalized by the directionality of the field and the orientation dependence of dipolar interactions.     

Entrapping intermediates of thermal aggregation in alpha-helical proteins with low concentration of guanidine hydrochloride

Aggregation of proteins is a problem with serious medical implications and economic importance. To develop strategies for preventing aggregation, the mechanism(s) and pathways by which proteins aggregate must be characterized. In this study, the thermally induced aggregation processes of three alpha-helix proteins (myoglobin, cytochrome c, and lysozyme) in the presence and absence of 1.0 m guanidine hydrochloride (GdnHCl) were investigated by means of infrared spectroscopy. In the absence of GdnHCl, intensities of the alpha-helix bands (approximately 1656 cm(-1)) decrease as a function of temperature at above 50 degrees C. With myoglobin and cytochrome c, the loss of helix bands was accompanied by the appearance of two new bands at 1694 and 1623 cm(-1), indicative of the formation of intermolecular beta-sheet aggregates. For lysozyme, bands indicative of intermolecular beta-sheet aggregates did not appear in any significant intensity. In the presence of 1.0 m GdnHCl, two major intermediate states rich in 3(10)-helix (represented by the band at 1663 cm(-1)) and beta-turn structure (represented by the band at 1667 cm(-1)), respectively, were observed. These findings demonstrated that IR spectroscopic studies of protein aggregation using a combination of thermal and chemical denaturing factors could provide a means to populate and characterize aggregation intermediates.     

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.     

Inelastic neutron-scattering study of the proton transfer dynamics in polyglycine I at 20 K

Inelastic neutron-scattering (INS) spectra of three isotopic derivatives of polyglycine I (-COCH2NH-)n, (-COCD2NH-)n, and (-COCH2ND-)n at 20 K are presented from 30 to 4000 cm(-1). The band frequencies are compared to those observed in the infrared and Raman. Assignments in terms of group vibrations are proposed. These mostly resemble previous assignment schemes, except for the amide bands. The INS intensities reveal that the proton dynamics for the (N)H proton are totally different from those proposed previously. They are independent of the molecular frame and the valence bond approach is not consistent with observation. A phenomenological approach is proposed in terms of localized modes. The calculated intensities reveal that the (N)H stretching mode has two components at approximately 1377 and 1553 cm(-1). This is a dramatic change compared to all former assignments at approximately 3280 cm(-1) based on infrared and Raman data. These proton-dynamics are associated with a weakening of the NH bond due to the ionic character of the hydrogen bond (N(delta-)...H+...O(delta'-)) and proton transfer. The infrared and Raman spectra are re-examined and a new assignment scheme is proposed for the amide bands; the amide A and B bands are re-assigned to the overtones of the stretching modes. A symmetric double-minimum potential for the proton is consistent with all the observations.     

Two-dimensional vibrational correlation spectroscopy of in vitro hydroxyapatite maturation

Two-dimensional (2-D) Raman and 2-D IR correlation spectroscopy are applied to analyze changes in the nu(4) region of the IR spectrum and in the nu(1) region of the Raman spectrum during the maturation of hydroxyapatite (HA) following the solution-mediated conversion of amorphous calcium phosphate (ACP) to HA. The nu(1) region of the Raman spectrum exhibits a frequency shift and sharpening during the maturation. Comparison of the experimental and simulated 2-D plots for this process suggests that the shift of a single peak, rather than a change in the relative intensity of two overlapped bands, is responsible for the observed spectral changes. The nu(4) mode of the PO(3-)(4) ion (T(2) symmetry in the free species) splits into a triplet with components near 563, 575, and 603 cm(-1) in HA. In addition, broad features appear at 540 and 617 cm(-1). During the latest stages of the maturation, an OH(-) librational mode develops at approximately 632 cm(-1). Changes in the relative intensities of three components of the nu(4) mode are not all correlated with each other. The synchronous 2-D plots reveal that the 563 and 603 cm(-1) pair are positively correlated while the feature at 575 cm(-1) is absent. A 587 cm(-1) mode arising from ACP is negatively correlated with the 563 and 603 cm(-1) pair and is both synchronously (positively) and asynchronously correlated with the 540 cm(-1) feature during the early stages of the maturation but is absent from 2-D plots of the later stages of the maturation. Cross correlations between the nu(4) mode and the nu(1),nu(3) contour generally confirm and extend previous assignments for the latter spectral region. Finally, the suitability of the 2-D approach for analysis of IR spectral images is examined through studies of HA crystallinity in a human iliac crest biopsy sample. Trabecular bone contains a fraction of HA that is more crystalline and mature than could be achieved in vitro during the room temperature ACP --> HA interconversion.     

Spectroscopic characterization of carbon monoxide complexes generated for copper/topa quinone-containing amine oxidases

Carbon monoxide complexes have been generated for copper/topa quinone (TPQ)-containing amine oxidases from Arthrobactor globiformis (AGAO) and Aspergillus niger (AO-I) and characterized by various spectroscopic measurements. Addition of CO to AGAO anaerobically reduced with its substrate 2-phenylethylamine led to a slight increase of absorption bands at 440 and 470 nm derived from the semiquinone form (TPQ(sq)) of the TPQ cofactor, concomitantly giving rise to new CO-related absorption bands at 334 and 434 nm. The intensity of the TPQ(sq) radical EPR signal at g = 2.004 also increased in the presence of CO, while its hyperfine coupling structure was affected insignificantly. FT-IR measurements revealed C-O stretching bands (nu(CO)) at 2063 and 2079 cm(-1) for the CO complex of the substrate-reduced AGAO (at 2085 cm(-1) for AO-I), which shifted nearly 100 cm(-1) to lower frequencies upon using (13)C(18)O. Collectively, these results suggest that CO is bound to the Cu(I) ion in the Cu(I)/TPQ(sq) species formed in the reductive half-reaction of amine oxidation, thereby shifting the Cu(II)/aminoresorcinol right arrow over left arrow Cu(I)/semiquinone equilibrium toward the latter. When AGAO was reduced with dithionite, an intermediary form of the enzyme with Cu(II) reduced to Cu(I) but TPQ still in the oxidized state (TPQ(ox)) was produced. Dithionite reduction of AGAO in the presence of CO resulted in the immediate formation of FT-IR bands at 2064 and 2083 cm(-1), which were assigned to the nu(CO) bands of the CO bound to the TPQ(ox) enzyme. The intense 2083 cm(-1) band was then displaced by a new band at 2077 cm(-1), corresponding to the formation of the fully reduced topa. Significant variation of these nu(CO) frequencies indicates that vibrational properties of CO bound to copper amine oxidases are sensitively influenced by the coordination structure of the Cu(I) ion, which may be modulated by the chemical and redox states of the TPQ cofactor.