WEFT-NOESY and transfer WEFT-NOESY NMR spectra were used to determine the heme proton assignments for Rhodobacter capsulatus ferricytochrome c2 . The Fermi contact and pseudo-contact contributions to the paramagnetic effect of the unpaired electron in the oxidized state were evaluated for the heme and ligand protons. The chemical shift assignments for the 1H and 15N NMR spectra were obtained by a combination of 1H–1H and 1H–15N two-dimensional NMR spectroscopy. The short-range nuclear Overhauser effect (NOE) data are consistent with the view that the secondary structure for the oxidized state of this protein closely approximates that of the reduced form, but with redox-related conformational changes between the two redox states. To understand the decrease in stability of the oxidized state of this cytochrome c2 compared to the reduced form, the structural difference between the two redox states were analyzed by the differences in the NOE intensities, pseudo-contact shifts and the hydrogen–deuterium exchange rates of the amide protons. We find that the major difference between redox states, although subtle, involve heme protein interactions, orientation of the heme ligands, differences in hydrogen bond networks and, possible alterations in the position of some internal water molecules. Thus, it appears that the general destabilization of cytochrome c2, which occurs on oxidation, is consistent with the alteration of hydrogen bonds that result in changes in the internal dynamics of the protein.

Specific binding of antigenic peptides to major histocompatibility complex (MHC) class I molecules is a prerequisite for their recognition by cytotoxic T-cells. Prediction of MHC-binding peptides must therefore be incorporated in any predictive algorithm attempting to identify immunodominant T-cell epitopes, based on the amino acid sequence of the protein antigen. Development of predictive algorithms based on experimental binding data requires experimental testing of a very large number of peptides. A complementary approach relies on the structural conservation observed in crystallographically solved peptide-MHC complexes. By this approach, the peptide structure in the MHC groove is used as a template upon which peptide candidates are threaded, and their compatibility to bind is evaluated by statistical pairwise potentials. Our original algorithm based on this approach used the pairwise potential table of Miyazawa and Jernigan (Miyazawa S, Jernigan RL, 1996, J Mol Biol 256:623–644) and succeeded to correctly identify good binders only for MHC molecules with hydrophobic binding pockets, probably because of the high emphasis of hydrophobic interactions in this table. A recently developed pairwise potential table by Betancourt and Thirumalai (Betancourt MR, Thirumalai D, 1999, Protein Sci 8:361–369) that is based on the Miyazawa and Jernigan table describes the hydrophilic interactions more appropriately. In this paper, we demonstrate how the use of this table, together with a new definition of MHC contact residues by which only residues that contribute exclusively to sequence specific binding are included, allows the development of an improved algorithm that can be applied to a wide range of MHC class I alleles.

The streptococcal pyrogenic toxins A, B, and C (SPEA, SPEB, and SPEC) are responsible for the fever, rash, and other toxicities associated with scarlet fever and streptococcal toxic shock syndrome. This role, together with the ubiquity of diseases caused by Streptococcus pyogenes, have prompted structural analyses of SPEA by several groups. Papageorgiou et al. (1999) have recently reported the structure of SPEA crystallized in the absence of zinc. Zinc has been shown to be important in the ability of some staphylococcal and streptococcal toxins to stimulate proliferation of CD4+ T-cells. Since cadmium is more electron dense than zinc and typically binds interchangeably, we grew crystals in the presence of 10 mM CdCl2. Crystals have been obtained in three space groups, and the structure in the P212121 crystal form has been refined to 1.9 Å resolution. The structural analysis revealed an identical tetramer as well as a novel tetrahedral cluster of cadmium in all three crystal forms on a disulfide loop encompassing residues 87–98. No cadmium was bound at the site homologous to the zinc site in staphylococcal enterotoxins C (SECs) despite the high structural homology between SPEA and SECs. Subsequent soaking of crystals grown in the presence of cadmium in 10 mM ZnCl2 showed that zinc binds in this site (indicating it can discriminate between zinc and cadmium ions) using the three ligands (Asp77, His106, and His110) homologous to the SECs plus a fourth ligand (Glu33).

The importance of unsatisfied hydrogen bonding potential on protein–protein interaction was studied. Two alternate modes of dimerization (conventional and flipped form) of an immunoglobulin light chain variable domain (VL) were previously identified. In the flipped form, interface residue Gln89 would have an unsatisfied hydrogen bonding potential. Removal of this Gln should render the flipped dimer as the more favorable quaternary form. High resolution crystallographic studies of the Q89A and Q89L mutants show, as we predicted, that these proteins indeed form flipped dimers with very similar interfaces. A small cavity is present in the Q89A mutant that is reflected in the ∼100 times lower association constant than found for the Q89L mutant. The association constant of Q89A and Q89L proteins (4 × 106 M−1 and >108 M−1) are 10- and 1,000-fold higher than that of the wild-type protein that forms conventional dimers clearly showing the energetic reasons for the flipped dimer formation.