The solution structure of the paramagnetic seven-iron ferredoxin from Bacillus schlegelii in its oxidized form has been determined by 1H NMR. The protein, which contains 77 amino acids, is thermostable. Seventy-two residues and 79% of all theoretically expected proton resonances have been assigned. The structure has been determined through torsion angle dynamics calculations with the program DYANA, using 966 meaningful NOEs (from a total of 1305), hydrogen bond constraints, and NMR derived dihedral angle constraints for the cluster ligating cysteines, and by using crystallographic information to build up the two clusters. Afterwards, restrained energy minimization and restrained molecular dynamics were applied to each conformer of the family. The final family of 20 structures has RMSD values from the mean structure of 0.68 A for the backbone atoms and of 1.16 A for all heavy atoms. The contributions to the thermal stability of the B. schlegelii ferredoxin are discussed by comparing the present structure to that of the less stable Azotobacter vinelandii ferredoxin I which is the only other available structure of a bacterial seven-iron ferredoxin. It is proposed that the hydrophobic interactions and the hydrogen bond network linking the N-terminus and the C-terminus together and a high number of salt bridges contribute to the stability.

Heteronuclear multidimensional NMR spectroscopy was used to investigate in detail the structural and dynamical properties of a partially unfolded intermediate of the reduced high-potential iron-sulfur protein (HiPIP) from Chromatium vinosum present in 4 M guanidinium chloride solution. After an extensive assignment of 15N and 1H resonances, NOE data, proton longitudinal relaxation times, and 3JHNHalpha coupling constants as well as 15N relaxation parameters (T1, T2, T1rho, and 1H-15N NOE) were obtained and used to build a structural model of the intermediate. The Fe4S4 cluster of the HiPIP plays a decisive role in determining the resulting structure, which is random in the N-terminal half of the protein and partially organized in the loops between the cysteines bound to the cluster. Consistent with the structural data, the backbone mobility is typical of folded proteins in the regions where there are elements of structure and increases with the structural indetermination.

A “merry‐go‐round” of iron valences is seen in an [Fe3S4]0 cluster with cysteine ligands. This phenomena is revealed by the observation of hyperfine‐shifted 1H NMR signals from the coordinated cysteine units, and the disappearance of these signals upon protonation of the cluster at low pH values. The proton binds to each of the three μ‐bridging sulfides for a fraction of time (see scheme). The protonation of one μ‐S causes the two iron atoms bridged by that μ‐S to form a mixed‐valence pair and the exchange of the proton from one μ‐S to another causes a change in the iron valences in the cluster.

15N T(1), T(2) and (1)H-(15)N NOE were measured for the thermophilic Fe(7)S(8) protein from Bacillus schlegelii and for the Fe(4)S(4) HiPIP protein from Chromatium vinosum, which is a mesophilic protein. The investigation was performed at 276, 300, and 330 K at 11.7 T for the former, whereas only the 298 K data at 14.1 T for the latter were acquired. The data were analyzed with the model-free protocol after correcting the measured parameters for the effect of paramagnetism, because both proteins are paramagnetic. Both thermophilic and mesophilic proteins are quite rigid, with an average value of the generalized order parameter S2at room temperature of 0.92 and 0.94 for Fe(7)S(8) and Fe(4)S(4) proteins, respectively. The analyzed nitrogens for the Fe(7)S(8) protein showed a significant decrease in S2with increasing temperature, and at the highest temperature >70% of the residues had an internal correlation time. This research shows that subnanosecond rigidity is not related to thermostability and provides an estimate of the effect of increasing temperature on this time scale.