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.     

Electron transfer induces side-chain conformational changes of glutamate-286 from cytochrome bo3

Heme-copper oxidases have two putative proton channels, the so-called K-channel and the membrane-spanning D-channel. The latter contains a number of polar groups with glutamate-286 located in its center, which could-together with bound water-contribute to a transmembrane hydrogen-bonded network. Protonation states of carboxyl groups from cytochrome bo3 of Escherichia coli were studied by redox Fourier transform infrared (FTIR) difference spectroscopy. A net absorbance increase in the carboxyl region was observed upon reduction. The band signature typically found in heme-copper oxidases comprises an absorbance decrease (reduced-minus-oxidized difference spectra) at 1745 cm-1 and increase at 1735 cm-1. No significant changes in the carboxyl region were found in the site-specific mutants D135E and D407N. The difference bands were lacking in redox spectra of mutants at position 286; they could clearly be related to Glu-286. In wild-type oxidase, the pK of Glu-286 appears to be higher than 9.8. Upon solvent isotope exchange from H2O to D2O, the band at 1745 cm-1 shifts more readily than the one at 1735 cm-1, indicating dissimilar accessibility of the carboxyl side chain to the hydrogen-bonded network in both redox states. The data are consistent with a redox-triggered conformational change of Glu-286, which attributes to the carboxyl group an orientation toward the interior of the D-channel for the oxidized form. The change of Glu-286 is retained in cyanide complexes of cytochrome bo3 and of cytochrome c oxidase; therefore it should be related to oxidoreduction of the heme b and/or CuB metal centers.     

Redox-linked conformational changes in proteins detected by a combination of infrared spectroscopy and protein electrochemistry. Evaluation of the technique with cytochrome c

We have developed a new technique for the study of redox-linked conformational changes in proteins, by the combination of two established techniques. Fourier-transform infrared spectroscopy has been used together with direct electrochemistry of the protein at a modified metal electrode surface. The technique has been evaluated with cytochrome c, because of its well-characterized electrochemistry and because the availability of X-ray crystallographic and NMR studies of both redox states of the protein provides a reference against which our data can be compared. In electrochemical control experiments, it was confirmed that the spectroelectrochemical cell design allows fast, accurate and reproducible control of the redox poise of the protein. The resulting reduced-minus-oxidized infrared difference spectra show the changes in the frequencies and intensities of molecular vibrations which arise from the redox-linked conformational change. In contrast to the absolute infrared spectra of proteins, such difference spectra can be sufficiently straightforward to allow interpretation at the level of individual bonds. A complete interpretation of the spectra is beyond the scope of the present paper: however, on the basis of the data presented, we are able to suggest assignments for all except one of the major bands between 1500 cm-1 and 1800 cm-1.     

External reflection FTIR of peptide monolayer films in situ at the air/water interface: experimental design, spectra-structure correlations, and effects of hydrogen-deuterium exchange.

A Fourier transform infrared spectrometer has been interfaced with a surface balance and a new external reflection infrared sampling accessory, which permits the acquisition of spectra from protein monolayers in situ at the air/water interface. The accessory, a sample shuttle that permits the collection of spectra in alternating fashion from sample and background troughs, reduces interference from water vapor rotation-vibration bands in the amide I and amide II regions of protein spectra (1520-1690 cm-1) by nearly an order of magnitude. Residual interference from water vapor absorbance ranges from 50 to 200 microabsorbance units. The performance of the device is demonstrated through spectra of synthetic peptides designed to adopt alpha-helical, antiparallel beta-sheet, mixed beta-sheet/beta-turn, and unordered conformations at the air/water interface. The extent of exchange on the surface can be monitored from the relative intensities of the amide II and amide I modes. Hydrogen-deuterium exchange may lower the amide I frequency by as much as 11-12 cm-1 for helical secondary structures. This shifts the vibrational mode into a region normally associated with unordered structures and leads to uncertainties in the application of algorithms commonly used for determination of secondary structure from amide I contours of proteins in D2O solution.     

CO and O2 complexes of soybean leghemoglobins: pH effects upon infrared and visible spectra. Comparisons with CO and O2 complexes of myoglobin and hemoglobin.

The effects of pH upon infrared spectra [CO stretching frequency (vco) region] and visible spectra of the CO complexes of soybean leghemoglobins a, c1, and c2, sperm whale myoglobin, and human hemoglobin A are reported. The vco for leghemoglobin--CO complexes was 1947.5 cm-1 at neutral pH. At acid pH myoglobin-- and hemoglobin--CO complexes developed vco bands at 1966--1968 cm-1, whereas leghemoglobin--CO complexes developed vco bands at approximately 1957 cm-1. All pKapp co values determined by pH-dependent variation of vco fell in the range 4.0--4.6. The pKapp co values determined from visible spectra were consistent with vco-determined values except for that of myoglobin--CO (visible pKapp co = 5.8). The pKapp co values in the 4.0--4.6 range appear to be pK values of the distal histidines, while the visible pKapp co of myoglobin--CO appears to be the pK of a group other than the distal and proximal histidines. The data are consistent with a model in which protonation of the distal histidine permits protein-free heme FeCO geometry in leghemoglobin--CO complexes but not in myoglobin-- or hemoglobin--CO complexes. Thus the heme pockets of leghemoglobins appear to be more flexible than the heme pockets of myoglobin and hemoglobin. The effects of pH upon visible spectra of the O2 complexes of soybean leghemoglobins a, c1, and c2, sperm whale myoglobin, and human hemoglobin A also are reported. pKapp o2 values of approximately 5.5 (leghemoglobins) and 4.4 (hemoglobin) are probably the pK values of the distal histidines. Comparisons of pKapp o2 values with pKapp co values indicate a more flexible heme pocket in leghemoglobins than in hemoglobin. The O2 complex of leghemoglobin c2 differed significantly from the O2 complexes of leghemoglobins a and c1 in visible spectra and titration behavior. These differences might be associated with the small structural differences in the region between the E and F helixes of leghemoglobins.     

Similarities and dissimilarities in the structure-function relation between the cytochrome c oxidase from bovine heart and from Paracoccus denitrificans as revealed by FT-IR difference spectroscopy.

The redox dependent changes in the cytochrome c oxidase from bovine heart were studied with a combined electrochemical and FT-IR spectroscopic approach. A direct comparison to the electrochemically induced FT-IR difference spectra of the cytochrome c oxidase from Paracoccus denitrificans reveals differences in the structure and intensity of vibrational modes. These differences are partially attributed to interactions of subunits influencing the heme and protein modes. In the spectral regions characteristic for v(C=O) and v(COO-)s/as modes of protonated and deprotonated Asp and Glu residues, additional signals at 1736, 1602 and 1588 cm-1 are observed. On this basis, the possible involvement of Asp-51, a residue specifically conserved in mammalian oxidase and previously proposed to show redox depended conformational changes in the respective X-ray structures, is critically discussed.     

Redox-induced conformational changes in plastocyanin: an infrared study.

The conformational changes associated with the redox transition of plastocyanin (PC) were investigated by absorption and reaction-induced infrared spectroscopy. In addition to spectral features readily ascribed to beta and turn protein secondary structures, the amide I band shows a major component band at 1647 cm(-1) in both redox states of the protein. The sensitivity of this component to deuteration and increasing temperature suggests that PC adopts an unusual secondary structure in solution, which differs from those described for other type I copper proteins, such as azurin and halocyanin. The conformations of oxidized and reduced PC are different, as evidenced (1) by analysis of their amide I band contour and the electrochemically induced oxidized-minus-reduced difference spectrum and (2) by their different thermal stability. The redox-induced difference spectrum exhibits a number of difference bands within the conformationally sensitive amide I band that could be assigned to peptide C=O modes, in light of their small shift upon deuteration, and to signals attributable to side chain vibrational modes of Tyr residues. Lowering the pH to 4.8 induces destabilization of both redox states of the protein, more pronounced for reduced PC, without significantly affecting their secondary structure. Besides the conformational differences obtained at neutral pH, the oxidized-minus-reduced difference spectrum shows two broad and strong negative bands at 1405 and 1571 cm(-1), assigned to COO(-) vibrations, and a broad positive band at 1710 cm(-1), attributed to the C=O vibration of a COOH group(s). These bands are indicative of a protonation of (an) Asp or Glu side chain(s) upon plastocyanin oxidation at acidic pH.     

Beware of proteins in DMSO

The effect on the secondary structure of representative alpha-helical, beta-sheet and disordered proteins by varying concentrations of dimethyl sulphoxide (DMSO) in 2H2O has been investigated by Fourier transform infrared spectroscopy. Significant perturbations of protein secondary structure are induced by DMSO and DMSO/2H2O mixtures. For highly structured proteins, such as myoglobin and concanavalin A, the infrared spectra point to a progressive destabilisation of the secondary structure until at moderate DMSO concentrations (around 0.33 mol fraction) intermolecular beta-sheet formation and aggregation are induced, as indicated by the appearance of a strong band at 1621 cm-1. This is a direct consequence of the disruption of intramolecular peptide group interactions by DMSO (partial unfolding). At higher DMSO concentrations (above 0.75 mol fraction), such aggregates are dissociated by disruption of the intermolecular C = O...2H-N deuterium bonds. The presence of a single amide I band at 1662 cm-1 corresponding to free amide C = O groups indicates that at high concentrations and in pure DMSO the proteins are completely unfolded, lacking any secondary structure. While low concentrations of DMSO showed no detectable effect upon the gross secondary structure of myoglobin and concanavalin A, the thermal stability of both proteins was markedly reduced. In alpha-casein, a highly unstructured protein, the situation is one of direct competition. The amide I maximum in 2H2O, at 1645 cm-1, is typical of unordered proteins with C = O groups deuterium-bonded predominantly to 2H2O. Addition of DMSO disrupts such interactions by competing with the peptide C = O group for the deuterium bond donor capacity of the 2H2O, and so progressively increases the amide I maximum until it stabilizes at 1663 cm-1, a position indicative of free C = O groups.     

ATP-Induced phosphorylation of the sarcoplasmic reticulum Ca2+ ATPase: molecular interpretation of infrared difference spectra.

Time-resolved infrared difference spectra of the ATP-induced phosphorylation of the sarcoplasmic reticulum Ca2+-ATPase have been recorded in H2O and 2H2O at pH 7.0 and 1 degrees C. The reaction was induced by ATP release from P3-1-(2-nitro)phenylethyladenosine 5'-triphosphate (caged ATP) and from [gamma-18O3]caged ATP. A band at 1546 cm-1, not observed with the deuterated enzyme, can be assigned to the amide II mode of the protein backbone and indicates that a conformational change associated with ATPase phosphorylation takes place after ATP binding. This is also indicated between 1700 and 1610 cm-1, where bandshifts of up to 10 cm-1 observed upon protein deuteration suggest that amide I modes of the protein backbone dominate the difference spectrum. From the band positions it is deduced that alpha-helical, beta-sheet, and probably beta-turn structures are affected in the phosphorylation reaction. Model spectra of acetyl phosphate, acetate, ATP, and ADP suggest the tentative assignment of some of the bands of the phosphorylation spectrum to the molecular groups of ATP and Asp351, which participate directly in the phosphate transfer reaction: a positive band at 1719 cm-1 to the C==O group of aspartyl phosphate, a negative band at 1239 cm-1 to the nuas(PO2-) modes of the bound ATP molecule, and a positive band at 1131 cm-1 to the nuas(PO32-) mode of the phosphoenzyme phosphate group, the latter assignment being supported by the band's sensitivity toward isotopic substitution in the gamma-phosphate of ATP. Band positions and shapes of these bands indicate that the alpha- and/or beta-phosphate(s) of the bound ATP molecule become partly dehydrated when ATP binds to the ATPase, that the phosphoenzyme phosphate group is unprotonated at pH 7.0, and that the C==O group of aspartyl phosphate does not interact with bulk water. The Ca2+ binding sites seem to be largely undisturbed by the phosphorylation reaction, and a functional role of the side chains of Asn, Gln, and Arg residues was not detected.     

Time-resolved FT-IR studies on the CO adduct of Paracoccus denitrificans cytochrome c oxidase: comparison of the fully reduced and the mixed valence form.

The rebinding of CO to cytochrome c oxidase from Paracoccus denitrificans in the fully reduced and in the half-reduced (mixed valence) form as a function of temperature was investigated using time-resolved rapid-scan FT-IR spectroscopy in the mid-IR (1200-2100 cm-1). For the fully reduced enzyme, rebinding was complete in approximately 2 s at 268 K and showed a biphasic reaction. At 84 K, nonreversible transfer of CO from heme a3 to CuB was observed. Both photolysis at 84 K and photolysis at 268 K result in FT-IR difference spectra which show similarities in the amide I, amide II, and heme modes. Both processes, however, differ in spectral features characteristic for amino acid side chain modes and may thus be indicative for the motional constraint of CO at low temperature. Rebinding of photodissociated CO for the mixed-valence enzyme at 268 K is also biphasic, but much slower as compared to the fully reduced enzyme. FT-IR difference spectra show band features similar to those for the fully reduced enzyme. Additional strong bands in the amide I and amide II range indicate local conformational changes induced by electron and coupled proton transfer. These signals disappear when the temperature is lowered to 84 K. At 268 K, a difference signal at 1746 cm-1 is observed which is shifted by 6 cm-1 to 1740 cm-1 in 2H2O. The absence of this signal for the mutant Glu 278 Gln allows assignment to the COOH stretching mode of Glu 278, and indicates changes of the conformation, proton position, or protonation of this residue upon electron transfer.     

Characterization of the CuA center in the cytochrome c oxidase from Thermus thermophilus for the spectral range 1800-500 cm-1 with a combined electrochemical and Fourier transform infrared spectroscopic setup

In this study we present the electrochemically induced Fourier transform infrared (FTIR) difference spectra of the Cu(A) center derived from the ba(3)-type cytochrome c oxidase of Thermus thermophilus in the spectral range from 1800 to 500 cm(-1). The mid infrared is dominated by the nu(C[double bond]O) vibrations of the amide I modes at 1688, 1660, and 1635 cm(-1), reflecting the redox-induced perturbation of the predominantly beta-sheet type structure. The corresponding amide II signal is found at 1528 cm(-1). In the lower frequency range below 800 cm(-1), modes from amino acids liganding the Cu(A) center are expected. On the basis of the absorbance spectrum of the isolated amino acids, methionine is identified as an important residue, displaying C-S vibrations at these frequencies. This spectral range was previously disregarded by protein IR spectroscopists, mainly due to the strong absorbance of the solvent, H(2)O. With an optimized setup, however, IR is found suitable for structure/function studies on proteins.     

Fourier transform infrared spectrometric analysis of protein conformation: effect of sampling method and stress factors.

Changes in the amide bands in Fourier transform infrared spectra of proteins are generally attributed to alterations in protein secondary structure. In this study spectra of five different globular proteins were compared in the solid and solution states recorded with several sampling techniques. Spectral differences for each protein were observed between the various sampling techniques and physical states, which could not all be explained by a change in protein secondary structure. For example, lyophilization in the absence of lyoprotectants caused spectral changes that could (partially) have been caused by the removal of hydrating water molecules rather than secondary structural changes. Moreover, attenuated total reflectance spectra of proteins in H2O were not directly comparable to transmission spectra due to the anomalous dispersion effect. Our study also revealed that the amide I, II, and III bands differ in their sensitivities to changes in protein conformation: For example, strong bands in the region 1620-1630 and 1685-1695 cm(-1) were seen in the amide I region of aggregated protein spectra. Surprisingly, absorbance of such magnitudes was not observed in the amide II and III region. It appears, therefore, that only the amide I can be used to distinguish between intra- and intermolecular beta-sheet formation. Considering the differing sensitivity of the different amide modes to structural changes, it is advisable to utilize not only the amide I band, but also the amide II and III bands, to determine changes in protein secondary structure. Finally, it is important to realize that changes in these bands may not always correspond to secondary structural changes of the proteins.     

Laser Raman investigations of intact single muscle fibers. Protein conformations

Raman spectra, in the frequency region of the protein vibrations, of intact single muscle fibers of the giant barnacle are presented. Strong bands at 1521 and 1156 cm-1 in the spectra are attributed to resonance-enhanced Raman bands of membrane-bound beta-carotene. Many bands of the myofibrillar proteins are also observed, and at least three spectral features confirm that these proteins adopt a predominantly alpha-helical structure: (1) the amide I band at 1648 cm-1, (2) the weak scattering in the amide III region, and (3) a strong skeletal C-C stretching band at 939 cm-1. Deuterated fibers have also been examined in order to find the exact shape of the amide III band. The presence in the fibers of paramyosin, which is only found in catch muscles, is also apparent from the spectra.     

Comparison of various molecular forms of bovine trypsin: correlation of infrared spectra with X-ray crystal structures

Fourier-transform infrared spectroscopy is a valuable method for the study of protein conformation in solution primarily because of the sensitivity to conformation of the amide I band (1700-1620 cm-1) which arises from the backbone C = O stretching vibration. Combined with resolution-enhancement techniques such as derivative spectroscopy and self-deconvolution, plus the application of iterative curve-fitting techniques, this method provides a wealth of information concerning protein secondary structure. Further extraction of conformational information from the amide I band is dependent upon discerning the correlations between specific conformational types and component bands in the amide I region. In this paper, we report spectra-structure correlations derived from conformational perturbations in bovine trypsin which arise from autolytic processing, zymogen activation, and active-site inhibition. IR spectra were collected for the single-chain (beta-trypsin) and once-cleaved, double-chain (alpha-trypsin) forms as well as at various times during the course of autolysis and also for zymogen, trypsinogen, and beta-trypsin inhibited with diisopropyl fluorophosphate. Spectral differences among the various molecular forms were interpreted in light of previous biochemical studies of autolysis and the known three-dimensional structures of the zymogen, the active enzyme, and the DIP-inhibited form. Our spectroscopic results from these proteins in D2O imply that certain loop structures may absorb in the region of 1655 cm-1. Previously, amide I' infrared bands near 1655 cm-1 have been interpreted as arising solely from alpha-helices. These new data suggest caution in interpreting this band. We have also proposed that regions of protein molecules which are known from crystallographic experiments to be disordered absorb in the 1645 cm-1 region and that type II beta-turns absorb in the region of 1672-1685 cm-1. Our results also corroborate assignment of the low-frequency component of extended strands to bands below 1636 cm-1. Additionally, the results of multiple measurements have allowed us to estimate the variability present in component band areas calculated by curve fitting the resolution-enhanced IR spectra. We estimate that this approach to data analysis and interpretation is sensitive to changes of 0.01 unit or less in the relative integrated intensities of component bands in spectra whose peaks are well resolved.     

Redox-dependent changes in beta-extended chain and turn structures of cytochrome c in water solution determined by second derivative amide I infrared spectra.

The redox-dependent changes in secondary structure of cytochromes c from horse, cow, and dog hearts in water at 20 degrees C have been determined by amide I infrared spectroscopy. Second derivative amide I spectra were obtained by use of a procedure that includes a convenient method for the effective subtraction of the spectrum of water vapor in the system. The band at 1657 cm-1 representing the helix structure was unaffected by a change in redox state whereas changes in bands due to turns at 1680, 1672, and 1666 cm-1, unordered structure at 1650 cm-1, and beta-structures at 1632 and 1627 cm-1 occurred. About one-fourth of the beta-extended chain spectral region and one-fifth of the beta-turn region (involving a total of approximately 9-13 residues) were sensitive to the oxidation state of heme iron. No significant changes in the secondary structure of either the reduced or oxidized protein due to changes in ionic strength were detected. The localized structural rearrangements triggered by the changes in oxidation state of heme iron are consistent with differences in the binding of heme iron to a histidine imidazole nitrogen and a methionine sulfur atom from the beta-extended chain. The demonstrated ability to obtain highly reproducible second derivative amide I infrared spectra confirms the unique utility of such spectral measurements for localization of subtle changes in secondary structure within a protein, especially for changes among the multiple turns and beta-structures.     

Electrochemically induced FTIR difference spectroscopy in the mid- to far infrared (200 microm) domain: a new setup for the analysis of metal-ligand interactions in redox proteins

We report the setup of an electrochemical cell with chemical-vapor deposition diamond windows and the use of a Bruker 66 SX FTIR spectrometer equipped with DTGS and Si-bolometer detectors and KBr and mylar beam splitters, to record on the same sample, FTIR difference spectra corresponding to the structural changes associated with the change in redox state of active sites in proteins in the whole 1800-50 cm(-1) region. With cytochrome c we show that reliable reduced-minus-oxidized FTIR difference spectra are obtained, which correspond to single molecular vibrations. Redox-sensitive IR modes of the cytochrome c are detected until 140 cm(-1) with a good signal to noise. This new setup is promising to analyze the infrared spectral region where metal-ligand vibrations are expected to contribute and to extend the analysis of vibrational properties to metal sites or redox states not accessible to (resonance) Raman spectroscopy.     

63/65Cu and 1/2H2O isotope shifts in the low-temperature resonance Raman spectrum of fungal laccase

Resonance Raman spectra are reported for the type 1 Cu site of fungal laccase at 295 and 77 K. The low-temperature spectra show enhanced resolution and reveal several weak bands not previously observed, as well as overtone and combination bands associated with the strong approximately equal to 400 cm-1 fundamentals. A novel low-temperature Raman difference technique has been used to obtain 63/65Cu and 1/2H2O isotope shifts. The strong band at 428 cm-1, and the moderate intensity bands at 408 and 387 cm-1 show small (under 0.6 cm-1 63/65Cu isotope shifts. The aggregate shift is substantially less than that expected for an isolated Cu-S(cys) stretch, implying a high degree of mixing of this coordinate with internal modes of the ligands. 1/2H2O shifts of 1.1 and approximately equal to 0.3 cm-1 are observed for the 387 and 428 cm-1 bands. The isotope shift patterns are quite similar for fungal and tree laccase, as are the frequencies of the dominant bands, indicating that the large differences in relative intensity are primarily associated with differences in the excited state potential. The frequency and isotope shift patterns are appreciably different, however, from those observed for azurin and stellacyanin. In contrast to the other 'blue' Cu proteins, fungal laccase shows no moderate intensity band near 270 cm-1 which can be associated with Cu-imidazole stretching; weak features are seen in this region, but the intensities are too low to determine their 1/2H2O sensitivity. The C-S stretching mode of fungal laccase is identified at 737 cm-1, shifting to 741 cm-1 at 77 K. It is about 10 cm-1 lower than for most 'blue' Cu proteins, and the difference is suggested to reflect smaller kinematic coupling between the C-S and Cu-S coordinates, associated with a smaller Cu-S-C angle. Combination modes of the approx. 400 cm-1 fundamentals are substantially stronger, relative to the overtones, than is predicted by first-order scattering theory, implying changes in the excited-state normal modes (Dushinsky effect) associated with force constant alterations.     

Infrared spectroscopy of a single cell--the human erythrocyte

Methods for obtaining the infrared spectrum of a single erythrocyte by infrared microscopy have been developed. The spectrum contains the amide I, II, and III bands characteristic of protein secondary structure near 1650, 1550, and 1300 cm-1, respectively. Bound carbon monoxide exhibits a readily measured band at 1951 cm-1 for 12C16O and 1907 cm-1 for 13C16O. Both amide and CO bands are similar to those found for purified hemoglobin A. Spectra can be obtained in H2O or D2O media under physiologically relevant conditions. Single cell infrared spectroscopy (SCIR) permits the qualitative and quantitative determination of differences among individual red cells. These results suggest many potential applications for SCIR for the measurements of properties of individual cells at the molecular level under physiologically relevant conditions.     

Effects of crystallization on the heme-carbon monoxide moiety of bovine heart cytochrome c oxidase carbonyl.

Cytochrome c oxidase isolated from bovine heart was crystallized in the fully reduced carbon monoxide (CO)-bound form. To evaluate the structure of the O2 reaction site in crystals and in solution, the bound C-O stretch infrared band in protein crystals was compared with the band for protein solution. In solution, the C-O stretch band could be deconvoluted into two extremely narrow bands, one at 1963.6 cm-1 with delta v1/2 = 3.4 cm-1 of 60% Gaussian/40% Lorentzian character represented 86% of the total band area and the other at 1960.3 cm-1 with delta v1/2 = 3.0 cm-1 of 47% Gaussian/53% Lorentzian character represented 14% of the total band area. The crystals exhibited two deconvoluted C-O infrared bands having very similar band parameters with those in solution. These findings support the presence of two structurally similar conformers in both crystals and solution. Thus crystallization of this enzyme does not affect the structure at the CO-binding site to as great extent as has been noted for myoglobin and hemoglobin carbonyls, indicating that the active (CO- or O2-binding) site of cytochrome c oxidase must be conformationally very stable and highly ordered compared to other hemoproteins such as hemoglobin.     

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

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