Perspectives in inorganic structural biology: solution structures of metalloproteins

Modeling the backbone dynamics of reduced and oxidized solvated rat microsomal cytochrome b5

In this article, a description of the statistics and dynamics of cytochrome b(5) in both reduced and oxidized forms is given. Results of molecular dynamics computer simulations in the explicit solvent have been combined with mode-coupling diffusion models including and neglecting the molecule-solvent correlations. R(1) and R(1 rho) nuclear magnetic relaxation parameters of (15)N in the protein backbone have been calculated and compared with experiments. Slight changes in charge density in the heme upon oxidation produces a cascade of changes in charge distributions from heme propionates up to charged residues approximately 1.5 nm from Fe. These changes in charge distributions modify the molecular surface and the water shell surrounding the protein. The statistical changes upon oxidation can be included in diffusive models that physically explain the upper and lower limits of R(1 rho) relaxation parameters at high off-resonance fields.

Folding, Conformational Changes, and Dynamics of Cytochromes c Probed by NMR Spectroscopy

NMR spectroscopy has become a vital tool for studies of protein conformational changes and dynamics. Oxidized Fe(III)cytochromes c are a particularly attractive target for NMR analysis because their paramagnetism (S = (1)/(2)) leads to high (1)H chemical shift dispersion, even for unfolded or otherwise disordered states. In addition, analysis of shifts induced by the hyperfine interaction reveals details of the structure of the heme and its ligands for native and nonnative protein conformational states. The use of NMR spectroscopy to investigate the folding and dynamics of paramagnetic cytochromes c is reviewed here. Studies of nonnative conformations formed by denaturation and by anomalous in vivo maturation (heme attachment) are facilitated by the paramagnetic, low-spin nature of native and nonnative forms of cytochromes c. Investigation of the dynamics of folded cytochromes c also are aided by their paramagnetism. As an example of this analysis, the expression in Escherichia coli of cytochrome c(552) from Nitrosomonas europaea is reported here, along with analysis of its unusual heme hyperfine shifts. The results are suggestive of heme axial methionine fluxion in N. europaea ferricytochrome c(552). The application of NMR spectroscopy to investigate paramagnetic cytochrome c folding and dynamics has advanced our understanding of the structure and dynamics of both native and nonnative states of heme proteins.

Paramagnetic resonance of biological metal centers

The review deals with recent advances in magnetic resonance spectroscopy (hf EPR and NMR) of paramagnetic metal centers in biological macromolecules. In the first half of our chapter, we present an overview of recent technical developments in the NMR of paramagnetic bio-macromolecules. These are illustrated by a variety of examples deriving mainly from the spectroscopy of metalloproteins and their complexes. The second half focuses on recent developments in high-frequency EPR spectroscopy and the application of the technique to copper, iron, and manganese proteins. Special attention is given to the work on single crystals of copper proteins.

Molten-globule and other conformational forms of zinc cytochrome C. Effect of partial and complete unfolding of the protein on its electron-transfer reactivity

To test the effect of protein conformation on reactivity, we use laser flash photolysis to compare the electron-transfer properties of the triplet state of zinc-substituted cytochrome c, designated (3)Zncyt, in the folded forms at low (F(low)) and high (F(high)) ionic strength, molten-globule (MG) form, and the forms unfolded by acid (U(acid)) and urea (U(urea)) toward the following four oxidative quenchers: Fe(CN)(6)(3-), Co(acac)(3), Co(phen)(3)(3+), and iron(III) cytochrome c. We characterize the conformational forms of Zncyt on the basis of the far-UV circular dichroism, Soret absorption, and rate constant for natural decay of the triplet state. This rate constant in the absence of quencher increases in the order F(high) < F(low) < MG < U(acid) < U(urea) because the exposure of porphyrin to solvent increases as Zncyt unfolds. Bimolecular rate constants for the reaction of (3)Zncyt with the four quenchers show significant effects on reactivity of electrostatic interactions and porphyrin exposure to solvent. This rate constant at the ionic strength of 20 mM increases upon unfolding by urea and acid, respectively, as follows: 1340-fold and 466-fold when the quencher is Co(phen)(3)(3+) and 168-fold and 36-fold when the quencher is cyt(III). To compare reactivity of (3)Zncyt in the F(low), F(high), MG, U(acid), and U(urea) forms without complicating effects of electrostatic interactions, we used the electroneutral quencher Co(acac)(3). Indeed, reactivity of folded (3)Zncyt with Co(acac)(3) was independent of ionic strength. Reactivity of (3)Zncyt with Co(acac)(3) upon partial and complete unfolding increases 10-fold, 54-fold, and 64-fold in the molten-globule, urea-unfolded, and acid-unfolded forms.

Crystal structure of rat apo-heme oxygenase-1 (HO-1): mechanism of heme binding in HO-1 inferred from structural comparison of the apo and heme complex forms

Heme oxygenase (HO) catalyzes the oxidative cleavage of heme to biliverdin by utilizing O(2) and NADPH. HO (apoHO) was crystallized as twinned P3(2) with three molecules per asymmetric unit, and its crystal structure was determined at 2.55 A resolution. Structural comparison of apoHO and its complex with heme (HO-heme) showed three distinct differences. First, the A helix of the eight alpha-helices (A-H) in HO-heme, which includes the proximal ligand of heme (His25), is invisible in apoHO. In addition, the B helix, a portion of which builds the heme pocket, is shifted toward the heme pocket in apoHO. Second, Gln38 is shifted toward the position where the alpha-meso carbon of heme is located in HO-heme. Nepsilon of Gln38 is hydrogen-bonded to the carbonyl group of Glu29 located at the C-terminal side of the A helix in HO-heme, indicative that this hydrogen bond restrains the angle between the A and B helices in HO-heme. Third, the amide group of Gly143 in the F helix is directed outward from the heme pocket in apoHO, whereas it is directed toward the distal ligand of heme in HO-heme. This means that the F helix around Gly143 must change its conformation to accommodate heme binding. The apoHO structure has the characteristic that the helix on one side of the heme pocket fluctuates, whereas the rest of the structure is similar to that of HO-heme, as observed in such hemoproteins as myoglobin and cytochromes b(5) and b(562). These structural features of apoHO suggest that the orientation of the proximal helix and the position of His25 are fixed upon heme binding.

Control of cytochrome C redox potential: axial ligation and protein environment effects

Axial iron ligation and protein encapsulation of the heme cofactor have been investigated as effectors of the reduction potential (E degrees ') of cytochrome c through direct electrochemistry experiments. Our approach was that of partitioning the E degrees ' changes resulting from binding of imidazole, 2-methyl-imidazole, ammonia, and azide to both cytochrome c and microperoxidase-11 (MP11), into the enthalpic and entropic contributions. N-Acetylmethionine binding to MP11 was also investigated. These ligands replace Met80 and a water molecule axially coordinated to the heme iron in cytochrome c and MP11, respectively. This factorization was achieved through variable temperature E degrees ' measurements. In this way, we have found that (i) the decrease in E degrees ' of cytochrome c due to Met80 substitution by a nitrogen-donor ligand is almost totally enthalpic in origin, as a result of the stronger electron donor properties of the exogenous ligand which selectively stabilize the ferric state; (ii) on the contrary, the binding of the same ligands and N-acetylmethionine to MP11 results in an enthalpic stabilization of the reduced state, whereas the entropic effect invariably decreases E degrees ' (the former effect prevails for the methionine ligand and the latter for the nitrogenous ligands). A comparison of the reduction thermodynamics of cytochrome c and the MP11 adducts offers insight on the effect of changing axial heme ligation and heme insertion into the folded polypeptide chain. Principally, we have found that the overall E degrees ' increase of approximately 400 mV, comparing MP11 and native cytochrome c, consists of two opposite enthalpic and entropic terms of approximately +680 and -280 mV, respectively. The enthalpic term includes contributions from both axial methionine binding (+300 mV) and protein encapsulation of the heme (+380 mV), whereas the entropic term is almost entirely manifest at the stage of axial ligand binding. Both terms are dominated by the effects of water exclusion from the heme environment.

The solution structure of reduced dimeric copper zinc superoxide dismutase. The structural effects of dimerization

The solution structure of homodimeric Cu2Zn2 superoxide dismutase (SOD) of 306 aminoacids was determined on a 13C, 15N and 70% 2H labeled sample. Two-thousand eight-hundred and five meaningful NOEs were used, of which 96 intersubunit, and 115 dihedral angles provided a family of 30 conformers with an rmsd from the average of 0.78 +/- 0.11 and 1.15 +/- 0.09 A for the backbone and heavy atoms, respectively. When the rmsd is calculated for each subunit, the values drop to 0.65 +/- 0.09 and 1.08 +/- 0.11 A for the backbone and heavy atoms, respectively. The two subunits are identical on the NMR time scale, at variance with the X-ray structures that show structural differences between the two subunits as well as between different molecules in the unit cell. The elements of secondary structure, i.e. eight beta sheets, are the same as in the X-ray structures and are well defined. The odd loops (I, III and V) are well resolved as well as loop II located at the subunit interface. On the contrary, loops IV and VI show some disorder. The residues of the active cavity are well defined whereas within the various subunits of the X-ray structure some are disordered or display different orientation in different X-ray structure determinations. The copper(I) ion and its ligands are well defined. This structure thus represents a well defined model in solution relevant for structure-function analysis of the protein. The comparison between the solution structure of monomeric mutants and the present structure shows that the subunit-subunit interactions increase the order in loop II. This has the consequences of inducing the structural and dynamic properties that are optimal for the enzymatic function of the wild-type enzyme. The regions 37-43 and 89-95, constituting loops III and V and the initial part of the beta barrel and showing several mutations in familial amyotrophis lateral sclerosis (FALS)-related proteins have a quite extensive network of H-bonds that may account for their low mobility. Finally, the conformation of the key Arg143 residue is compared to that in the other dimeric and monomeric structures as well as in the recently reported structure of the CCS-superoxide dismutase (SOD) complex.