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The binding of divalent copper ions to the full-length recombinant murine prion protein PrP23-231 at neutral pH was studied using vibrational Raman optical activity (ROA) and ultraviolet circular dichroism (UV CD). The effect of the Cu2+ ions on PrP structure depends on whether they are added after refolding of the protein in water or are present during the refolding process. In the first case ROA reveals that the hydrated alpha-helix is lost, with UV CD revealing a drop from approximately 25% to approximately 18% in the total alpha-helix content. The lost alpha-helix could be that comprising residues 145-156, located within the region associated with scrapie PrP formation. In the second case, ROA reveals the protein's structure to be almost completely disordered/irregular, with UV CD revealing a drop in total alpha-helix content to approximately 5%. Hence, although Cu2+ binding takes place exclusively within the unfolded/disordered N-terminal region, it can profoundly affect the structure of the folded/alpha-helical C-terminal region. This is supported by the finding that refolding in the presence of Cu2+ of a mutant in which the first six histidines associated with copper binding to the N-terminal region are replaced by alanine has a similar alpha-helix content to the metal-free protein. In contrast, when the protein is refolded in the presence of divalent manganese ions, ROA indicates the alpha-helix is reinforced, with UV CD revealing an increase in total alpha-helix content to approximately 30%. The very different influence of Cu2+ and Mn2+ ions on prion protein structure may originate in the different stability constants and geometries of their complexes.

Vibrational Raman optical activity (ROA) spectra of the wheat proteins alpha-gliadin (A-gliadin), omega-gliadin, and a 30 kDa peptide called T-A-1 from the high molecular weight glutenin subunit (HMW-GS) Dx5 were measured to obtain new information about their solution structures. The spectral data show that, under the conditions investigated, A-gliadin contains a considerable amount of hydrated alpha-helix, most of which probably lies within a relatively structured C-terminal domain. Smaller quantities of beta-structure and poly(l-proline) II (PPII) helix were also identified. Addition of methanol was found to increase the alpha-helix content at the expense of some of the beta and PPII structure. In comparison, omega-gliadin and the T-A-1 peptide were found to consist of large amounts of well-defined PPII structure with some turns but no alpha-helix. The results for the T-A-1 peptide are in agreement with a model in which HMW-GS are extended but not highly rigid. Application of a pattern recognition technique, based on principal component analysis (PCA), to the ROA spectra reinforces these conclusions.

Recent observations using the novel technique of Raman optical activity suggest that individual residues in unfolded proteins and in disordered loop regions of molten globule-like states cluster in the alpha-helix, beta-structure, and PPII-helix regions of the Ramachandran surface and that they "flicker" between these regions at rates approximately 10(12) s-1 at room temperature. It is proposed that these rapid motions, which occur on the same picosecond time scale as rearrangements of the hydrogen bond network in bulk water, are promoted by solvent water molecules via a repertoire of transient hydrated reverse turn conformations. Some implications of this proposal for protein folding and function are discussed.

Because of its ability to probe directly the chiral elements of the peptide backbone, together with the very short time scale of the scattering process, vibrational Raman optical activity (ROA) can provide new information on structure in non-native states of proteins. Here we report ROA studies of hen egg white lysozyme and bovine ribonuclease A in unfolded denatured states, prepared by reducing all the disulfide bonds. ROA spectra of unfolded lysozyme at 45, 20, and 2 degrees C, and of unfolded ribonuclease A at 35 and 20 degrees C, are presented and discussed. At 45 and 20 degrees C, unfolded lysozyme appears to contain very little extended secondary structure, but at 2 degrees C there could be roughly 20% of the native amount of alpha-helix present but little beta-sheet. Unfolded ribonuclease A, on the other hand, appears to contain roughly 50% of its native-like secondary structure, including both alpha-helix and beta-sheet, at 20 degrees C; similar secondary structure persists at 35 degrees C, but the amount is reduced. The most striking result is the observation of three sharp ROA bands in the extended amide III region, originating in coupled C alpha-H and N-H deformations, which might monitor directly the dominant intrinsic propensities for residues to adopt particular phi, psi angles, averaged over the different amino acids in the mobile heteropolypeptide. Specifically, positive bands at approximately 1300 and 1314 cm-1 appear to monitor propensities for alpha-helix and beta-structure, respectively, and a negative band at approximately 1237 cm-1 appears to monitor that for the poly(L-proline) II helix. These signals are generated by individual residues clustering in the most favorable regions of the Ramachandran plot and are present even in the absence of signals from the corresponding extended secondary structures. At 45 degrees C, the 1300 and 1314 cm-1 ROA bands of unfolded lysozyme coalesce into a single sharp band from which an analysis similar to that used for exchange effects in NMR suggests a rate of approximately 2.6 x 10(12) s-1 for interconversion between the individual residue conformations at this temperature.