Evidence for antiferromagnetic exchange coupling in the tetranuclear high potential iron-sulfur protein of Rhodopseudomonas gelatinosa

Investigation of the role of a surface patch in the self-association of Chromatium vinosum high potential iron-sulfur protein

The role of a flattened, relatively hydrophobic surface patch in the self-association of Chromatium vinosum HiPIP was assessed by substituting phenylalanine 48 with lysine. The reduction potential of the F48K variant was 26 mV higher than that of the wild-type (WT) recombinant (rc) HiPIP, consistent with the introduction of a positive charge close to the cluster. Nuclear magnetic resonance spectroscopy (NMR) revealed that the electronic structure of the oxidized cluster in these two proteins is very similar at 295 K. In contrast, the electron transfer self-exchange rate constant of F48K was at least 15-fold lower than that of the WT rcHiPIP, indicating that the introduction of a positive charge at position 48 diminishes self-association of the HiPIP in solution. Moreover, the substitution at position 48 abolished the fine structure in the g(z) region of the electron paramagnetic resonance (EPR) spectrum of oxidized C. vinosum rcHiPIP recorded in the presence of 1 M sodium chloride. These results support the hypothesis that the flattened, relatively hydrophobic patch mediates interaction between two molecules of HiPIP and that freezing-induced dimerization of the HiPIP mediated by this patch is responsible for the unusual fine structure observed in the EPR spectrum of the oxidized C. vinosum HiPIP.

Temperature dependence of the electronic spin-lattice relaxation time in a 2-iron-2-sulphur model complex

The complex [Fe2S2(S2-o-xylyl)2]2- in DMF (dimethylformamide), DMSO (dimethylsulphoxide) or a 1:1 DMF/DMSO mixture, a model for the chromophore in the 2Fe-2S proteins (ferredoxins), has been reduced and studied by conventional EPR over a temperature range. The low-field feature of the spectrum, Hz, has been computer simulated in order to analyse the lineshape in terms of a convolution product of Lorentzian and Gaussian distributions. The Gaussian contribution to the linewidth and a fixed part of the Lorentzian contribution, which is a function of the solvent and the way it freezes, were measured at a low temperature (less than or equal to 100 K) and subtracted from the linewidths in the higher-temperature range (130-200 K). The variable Lorentzian contribution thus obtained was related to spin-lattice relaxation times. The spin-lattice relaxation times of the sample having 1:1 DMSO/DMF solvent were measured in the range 6 to 11 K by the saturating pulse technique and in the range 10 to 65 K by continuous saturation methods. Up to 65 K the results follow the law 1/T1 alpha T4.5, a relationship which is not readily interpreted in terms of a simple Debye model. At higher temperatures the results may be interpreted in terms either of a dominant Orbach mechanism involving excited states at approx. 900 +/- 50 cm-1 (DMSO, DMF) or 770 +/- 50 cm-1 (1:1 DMSO/DMF), or of a Raman process in which 1/T1 alpha T7.5. The former is compatible with the two-phonon process already described in some ferredoxins, especially those with little anisotropy (gy - gx approximately 0.0) which have characteristically high [J] values.

The orientation of the magnetic axes of the membrane-bound iron-sulfur clusters of spinach chloroplasts

Spinach chloroplast membranes were oriented onto mylar sheets by partial dehydration, and the orientation of the magnetic axes of membrane-bound paramagnetic clusters determined by electron paramagnetic resonance (EPR) spectroscopy. Our results indicate that the reduced Rieske iron-sulfur cluster signal is of orthorhombic symmetry oriented with th gy = 1.90 axis orthogonal to the membrane plane and with the gz = 2.03 axis in the membrane plane; the gx-axis is undetectable, presumably due to its broadness. If the Rieske center is a two-iron iron-sulfur cluster, we conclude that the iron-iron axis lies in the plane of the membrane. Illumination reduces the two bound chloroplast iron-sulfur proteins known as Clusters A and B. Center A is oriented such that gx = 1.86 and gy = 1.94 lie at an angle of about 40, and gz = 2.05 is at approximately 25, to the membrane plane. There are two possible orientations of Cluster B depending on the set of g-values assigned to this cluster. For one set of g-values, gz = 2.04 and gx = 1.89 are oriented in the plane of the membrane while gy = 1.92 is orthogonal to the plane. Alternatively, gz = 2.07 and gy = 1.94 are oriented approximately 50 and 40 to the membrane plane respectively, and gx = 1.80 is in the plane of the membrane. An additional light-induced signal at g = 2.15 oriented orthogonal to the plane is currently unexplained, as are other membrane perpendicular signals seen at g = 2.3 and g = 1.73 in dark-adapted samples.

Exchange integral for a variety of tetranuclear ferredoxins

The temperature dependence of EPR spectra of oxidized [4Fe-4S](-1,-2) ferredoxins (previously designated HiPIP) and a reduced [4Fe-4S](-2,-3) ferredoxin have been analyzed so as to determine the energy of a low-lying excited electronic state. The values obtained were: Center S-3 from beef heart, 44 cm-1; Center S-3 from mung bean, 53 cm-1; the [4Fe-4S](-1,-2) ferredoxin from Thermus thermophilus, 78 cm-1; Center N-2 of NADH ubiquinone reductase, 83 cm-1. Increasing axial distortion in the EPR spectra of the [4Fe-4S](-1,-2), ferrodoxins was associated with higher energy differences. Center N-2, a [Fe-4S](-2,-3) iron-sulfur cluster does not fit this relationship.

The orientation of iron-sulfur clusters and a spin-coupled ubiquinone pair in the mitochondrial membrane

Oriented multilayers made from beef heart and yeast mitochondria and submitochondrial particles were studied using electron paramagnetic resonance. EPR signals from membrane-bound iron-sulfur clusters and from a spin-coupled ubiquinone pair are highly orientation dependent, implying that these redox centers are fixed in the membrane at definite angles relative to the membrane plane. Typically the iron-iron axis (gz) of the binuclear iron-sulfur clusters is in the membrane plane. This finding is discussed in terms of the protein structure. The tetranuclear iron-sulfur clusters can have their gz axis either perpendicular or parallel to the membrane plane, but intermediate orientation was not observed.