X-ray absorption edge fine structure spectroscopy of the active site haem of cytochrome c

Towards a black-box for biological EXAFS data analysis. II. Automatic BioXAS Refinement and Analysis (ABRA)

In biological systems, X-ray absorption spectroscopy (XAS) can determine structural details of metal binding sites with high resolution. Here a method enabling an automated analysis of the corresponding EXAFS data is presented, utilizing in addition to least-squares refinement the prior knowledge about structural details and important fit parameters. A metal binding motif is characterized by the type of donor atoms and their bond lengths. These fit results are compared by bond valance sum analysis and target distances with established structures of metal binding sites. Other parameters such as the Debye-Waller factor and shift of the Fermi energy provide further insights into the quality of a fit. The introduction of mathematical criteria, their combination and calibration allows an automated analysis of XAS data as demonstrated for a number of examples. This presents a starting point for future applications to all kinds of systems studied by XAS and allows the algorithm to be transferred to data analysis in other fields.

Detecting transient protein-protein interactions by X-ray absorption spectroscopy: The cytochromec6-photosystem I complex

Reliable analysis of the functionality of metalloproteins demands a highly accurate description of both the redox state and geometry of the metal centre, not only in the isolated metalloprotein but also in the transient complex with its target. Here, we demonstrate that the transient interaction between soluble cytochrome c(6) and membrane-embedded photosystem I involves subtle changes in the heme iron, as inferred by X-ray absorption spectroscopy (XAS). A slight shift to lower energies of the absorption edge of Fe2+ in cytochrome c6 is observed upon interaction with photosystem I. This work constitutes a novel application of XAS to the analysis of weak complexes in solution.

Unusual heme iron-lipid acyl chain coordination in Escherichia coli flavohemoglobin

Escherichia coli flavohemoglobin is endowed with the notable property of binding specifically unsaturated and/or cyclopropanated fatty acids both as free acids or incorporated into a phospholipid molecule. Unsaturated or cyclopropanated fatty acid binding to the ferric heme results in a spectral change observed in the visible absorption, resonance Raman, extended x-ray absorption fine spectroscopy (EXAFS), and x-ray absorption near edge spectroscopy (XANES) spectra. Resonance Raman spectra, measured on the flavohemoglobin heme domain, demonstrate that the lipid (linoleic acid or total lipid extracts)-induced spectral signals correspond to a transition from a five-coordinated (typical of the ligand-free protein) to a hexacoordinated, high spin heme iron. EXAFS and XANES measurements have been carried out both on the lipid-free and on the lipid-bound protein to assign the nature of ligand in the sixth coordination position of the ferric heme iron. EXAFS data analysis is consistent with the presence of a couple of atoms in the sixth coordination position at 2.7 A in the lipid-bound derivative (bonding interaction), whereas a contribution at 3.54 A (nonbonding interaction) can be singled out in the lipid-free protein. This last contribution is assigned to the CD1 carbon atoms of the distal LeuE11, in full agreement with crystallographic data on the lipid-free protein at 1.6 A resolution obtained in the present work. Thus, the contributions at 2.7 A distance from the heme iron are assigned to a couple of carbon atoms of the lipid acyl chain, possibly corresponding to the unsaturated carbons of the linoleic acid.

Redox-induced structural dynamics of Fe-heme ligand in myoglobin by X-ray absorption spectroscopy

The Fe(III) --> Fe(II) reduction of the heme iron in aquomet-myoglobin, induced by x-rays at cryogenics temperatures, produces a thermally trapped nonequilibrium state in which a water molecule is still bound to the iron. Water dissociates at T > 160 K, when the protein can relax toward its new equilibrium, deoxy form. Synchrotron radiation x-ray absorption spectroscopy provides information on both the redox state and the Fe-heme structure. Owing to the development of a novel method to analyze the low-energy region of x-ray absorption spectroscopy, we obtain structural pictures of this photo-inducible, irreversible process, with 0.02-0.06-A accuracy, on the protein in solution as well as in crystal. After photo-reduction, the iron-proximal histidine bond is shortened by 0.15 A, a reinforcement that should destabilize the iron in-plane position favoring water dissociation. Moreover, we are able to get the distance of the water molecule even after dissociation from the iron, with a 0.16-A statistical error.

pH-dependent local structure of ferricytochrome c studied by x-ray absorption spectroscopy

We have studied, using x-ray absorption spectroscopy by synchrotron radiation, the native state of the horse heart cytochrome c (N), the HCl denatured state (U(1) at pH 2), the NaOH denatured state (U(2) at pH 12), the intermediate HCl induced state (A(1) at pH 0.5), and the intermediate NaCl induced state (A(2) at pH 2). Although many results concerning the native and denatured states of this protein have been published, a site-specific structure analysis of the denatured and intermediate solvent induced states has never been attempted before. Model systems and myoglobin in different states of coordination are compared with cytochrome c spectra to have insight into the protein site structure in our experimental conditions. New features are evidenced by our results: 1) x-ray absorption near edge structure (XANES) of the HCl intermediate state (A(1)) presents typical structures of a pentacoordinate Fe(III) system, and 2) local site structures of the two intermediate states (A(1) and A(2)) are different.

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.

Redox-dependent structure change and hyperfine nuclear magnetic resonance shifts in cytochrome c

Proton nuclear magnetic resonance assignments for reduced and oxidized equine cytochrome c show that many individual protons exhibit different chemical shifts in the two protein forms, reflecting diamagnetic shift effects due to structure change, and in addition contact and pseudocontact shifts that occur only in the paramagnetic oxidized form. To evaluate the chemical shift differences (delta delta) for structure change, we removed the pseudocontact shift contribution by a calculation based on knowledge of the electron spin g tensor. The g-tensor parameters were determined from the delta delta values of a large set (64) of C alpha H protons at well-defined spatial positions in the oxidized horse protein. The g-tensor calculation, when repeated using only 12 available C alpha H proton resonances for cytochrome c from tuna, proved to be remarkably stable. The largest principal value of the g tensor (gz) falls precisely along the ligand bond between the heme iron and methionine-80 sulfur, while gx and gy closely match the natural heme axes defined by the pyrrole nitrogens. The derived g tensor was then used together with spatial coordinates for the oxidized form to calculate the pseudocontact shift contribution (delta pc) to proton resonances at 400 identifiable sites throughout the protein, so that the redox-dependent chemical shift discrepancy, delta delta-delta pc, could be evaluated. Large residual changes in chemical shift define the Fermi contact shifts, which are found as expected to be limited to the immediate covalent structure of the heme and its ligands and to be asymmetrically distributed over the heme. Smaller chemical shift discrepancies point to a concerted change, involving residues 39-43 and 50-60 (bottom of the protein), and to other changes in the immediate vicinity of the heme ligands. Also, the three internal water molecules are implicated in redox sensitivity. The residues found to change are in good but not perfect agreement with prior X-ray diffraction observations of subangstrom redox-related displacements in the tuna protein. The chemical shift discrepancies observed appear in the main to reflect structure-dependent diamagnetic shifts rather than hyperfine effects due to displacements in the pseudocontact shift field. Although 51 protons in 29 different residues exhibit significant chemical shift changes, the general impression is one of small structural adjustments to redox-dependent strain rather than sizeable structural displacements or rearrangements.

Effect of the hinge protein on the heme iron site of cytochrome c1

X-ray absorption spectroscopic (XAS) studies on cytochrome C1 from beef heart mitochondria were conducted to identify the effect of the hinge protein [Kim, C.H., & King, T.E. (1983) J. Biol. Chem. 258, 13543-13551] on the structure of the heme site in cytochrome c1. A comparison of XAS data of highly purified "one-band" and "two-band" cytochrome c1 [Kim, C.H., & King, T.E. (1987) Biochemistry 26, 1955-1961] demonstrates that the hinge protein exerts a rather pronounced effect on the heme environment of the cytochrome c1: a conformational change occurs within a radius of approximately 5 A from the heme iron in cytochrome c1 when the hinge protein is bound to cytochrome c1. This result may be correlated with the previous observations that the structure and reactivity of cytochrome c1 are affected by the hinge protein [Kim, C.H., & King, T.E. (1987) Biochemistry 26, 1955-1961; Kim, C.H., Balny, C., & King, T.E. (1987) J. Biol. Chem. 262, 8103-8108].

Increase in apparent compressibility of cytochrome c upon oxidation

The apparent molal adiabatic compressibilities of ferri- and ferrocytochrome c have been determined from measurements of density and sound velocity. The values found were +2.99 X 10(-8) and -2.40 X 10(-8) cm5 mol-1 dyne-1 for the ferri and ferro forms, respectively. Experiments were performed on identical solutions containing either the oxidized or reduced form of protein. Solutions of ferricytochrome c were found to have significantly greater adiabatic compressibility than equivalent solutions of ferrocytochrome c at 25 degrees C and pH 7.15. The remarkable similarity of the three-dimensional structures of the ferri and ferro proteins [Takano, T. & Dickerson, R.E. (1980) Proc. Natl. Acad. Sci. USA 77, 6371-6375] strongly suggests that this difference in compressibility is due to an increase in volume fluctuations within ferricytochrome c relative to the ferro form rather than a change in equilibrium structure or hydration. Such a difference in the dynamic properties of the structures is consistent with both the crystallographic thermal B factors and the observed increase in amide hydrogen exchange kinetics when ferrocytochrome c is oxidized. The relative magnitude of the root mean square volume fluctuations is approximated from an ideal solution treatment of the compressibility data and yields a ratio of delta Vrms (ferri cyt c)/ delta Vrms (ferro cyt c) = 1.3.

Time-resolved resonance Raman spectroscopy of cytochrome c reduced by pulse radiolysis

The first investigation of the dynamics of a redox transition of an electron-transfer enzyme by time-resolved resonance Raman spectroscopy in combination with pulse-radiolytic reduction is described by an application to cytochrome c. A long-lived transient state is observed upon reduction of the alkaline form of cytochrome c as a distinct frequency shift of one resonance Raman band. From the frequency in the stable oxidized state, 1567 cm(-1), this particular resonance Raman band shifts within less than 1 microsecond to 1533 cm(-1) in the transient reduced state, which has a lifetime longer than 20 ms but shorter than a few seconds. Finally, in the stable reduced state, this band is located at 1547 cm(-1). According to a previous normal coordinate analysis, this resonance Raman band can be assigned predominantly to a stretching mode of the outermost C-C bonds in the four pyrrole rings of porphyrin. This vibrational mode is influenced by the protein most directly through the covalent thioether linkages of two cysteines to porphyrin. We interpret the long lifetime of the transient state as due to the slow return of Met-80 as sixth ligand to the heme iron upon reduction of the alkaline form of cytochrome c.