Structure of the recombinant full-length hamster prion protein PrP(29-231): the N terminus is highly flexible

The prion diseases seem to be caused by a conformational change of the prion protein (PrP) from the benign cellular form PrPC to the infectious scrapie form PrPSc; thus, detailed information about PrP structure may provide essential insights into the mechanism by which these diseases develop. In this study, the secondary structure of the recombinant Syrian hamster PrP of residues 29-231 [PrP(29-231)] is investigated by multidimensional heteronuclear NMR. Chemical shift index analysis and nuclear Overhauser effect data show that PrP(29-231) contains three helices and possibly one short beta-strand. Most striking is the random-coil nature of chemical shifts for residues 30-124 in the full-length PrP. Although the secondary structure elements are similar to those found in mouse PrP fragment PrP(121-231), the secondary structure boundaries of PrP(29-231) are different from those in mouse PrP(121-231) but similar to those found in the structure of Syrian hamster PrP(90-231). Comparison of resonance assignments of PrP(29-231) and PrP(90-231) indicates that there may be transient interactions between the additional residues and the structured core. Backbone dynamics studies done by using the heteronuclear [1H]-15N nuclear Overhauser effect indicate that almost half of PrP(29-231), residues 29-124, is highly flexible. This plastic region could feature in the conversion of PrPC to PrPSc by template-assisted formation of beta-structure.

Solution structure of a 142-residue recombinant prion protein corresponding to the infectious fragment of the scrapie isoform

The scrapie prion protein (PrPSc) is the major, and possibly the only, component of the infectious prion; it is generated from the cellular isoform (PrPC) by a conformational change. N-terminal truncation of PrPSc by limited proteolysis produces a protein of approximately 142 residues designated PrP 27-30, which retains infectivity. A recombinant protein (rPrP) corresponding to Syrian hamster PrP 27-30 was expressed in Escherichia coli and purified. After refolding rPrP into an alpha-helical form resembling PrPC, the structure was solved by multidimensional heteronuclear NMR, revealing many structural features of rPrP that were not found in two shorter PrP fragments studied previously. Extensive side-chain interactions for residues 113-125 characterize a hydrophobic cluster, which packs against an irregular beta-sheet, whereas residues 90-112 exhibit little defined structure. Although identifiable secondary structure is largely lacking in the N terminus of rPrP, paradoxically this N terminus increases the amount of secondary structure in the remainder of rPrP. The surface of a long helix (residues 200-227) and a structured loop (residues 165-171) form a discontinuous epitope for binding of a protein that facilitates PrPSc formation. Polymorphic residues within this epitope seem to modulate susceptibility of sheep and humans to prion disease. Conformational heterogeneity of rPrP at the N terminus may be key to the transformation of PrPC into PrPSc, whereas the discontinuous epitope near the C terminus controls this transition.

Local structural plasticity of the prion protein. Analysis of NMR relaxation dynamics

A template-assisted conformational change of the cellular prion protein (PrP(C)) from a predominantly helical structure to an amyloid-type structure with a higher proportion of beta-sheet is thought to be the causative factor in prion diseases. Since flexibility of the polypeptide is likely to contribute to the ability of PrP(C) to undergo the conformational change that leads to the infective state, we have undertaken a comprehensive examination of the dynamics of two recombinant Syrian hamster PrP fragments, PrP(29-231) and PrP(90-231), using (15)N NMR relaxation measurements. The molecular motions of these PrP fragments have been studied in solution using (15)N longitudinal (T(1)) and transverse relaxation (T(2)) measurements as well as [(1)H]-(15)N nuclear Overhauser effects (NOE). These data have been analyzed using both reduced spectral density mapping and the Lipari-Szabo model free formalism. The relaxation properties of the common regions of PrP(29-231) and PrP(90-231) are very similar; both have a relatively inflexible globular domain (residues 128-227) with a highly flexible and largely unstructured N-terminal domain. Residues 29-89 of PrP(29-231), which include the copper-binding octarepeat sequences, are also highly flexible. Analysis of the spectral densities at each residue indicates that even within the structured core of PrP(C), a markedly diverse range of motions is observed, consistent with the inherent plasticity of the protein. The central portions of helices B and C form a relatively rigid core, which is stabilized by the presence of an interhelix disulfide bond. Of the remainder of the globular domain, the parts that are not in direct contact with the rigid region, including helix A, are more flexible. Most significantly, slow conformational fluctuations on a millisecond to microsecond time scale are observed for the small beta-sheet. These results are consistent with the hypothesis that the infectious, scrapie form of the protein PrP(Sc) could contain a helical core consisting of helices B and C, similar in structure to the cellular form PrP(C). Our results indicate that residues 90-140, which are required for prion infectivity, are relatively flexible in PrP(C), consistent with a lowered thermodynamic barrier to a template-assisted conformational change to the infectious beta-sheet-rich scrapie isoform.

Hybrid-hybrid matrix structural refinement of a DNA three-way junction from 3D NOESY-NOESY

Homonuclear 3D NOESY-NOESY has shown great promise for the structural refinement of large biomolecules. A computationally efficient hybrid-hybrid relaxation matrix refinement methodology, using 3D NOESY-NOESY data, was used to refine the structure of a DNA three-way junction having two unpaired bases at the branch point of the junction. The NMR data and the relaxation matrix refinement confirm that the DNA three-way junction exists in a folded conformation with two of the helical stems stacked upon each other. The third unstacked stem extends away from the junction, forming an acute angle (approximately 60 degrees) with the stacked stems. The two unpaired bases are stacked upon each other and are exposed to the solvent. Helical parameters for the bases in all three strands show slight deviations from typical values expected for right-handed B-form DNA. Inter-nucleotide imino-imino NOEs between the bases at the branch point of the junction show that the junction region is well defined. The helical stems show mobility (+/- 20 degrees) indicating dynamic processes around the junction region. The unstacked helical stem adjacent to the unpaired bases shows greater mobility compared to the other two stems. The results from this study indicate that the 3D hybrid-hybrid matrix MORASS refinement methodology, by combining the spectral dispersion of 3D NOESY-NOESY and the computational efficiency of 2D refinement programs, provides an accurate and robust means for structure determination of large biomolecules. Our results also indicate that the 3D MORASS method gives higher quality structures compared to the 2D complete relaxation matrix refinement method.

Exact vs approximate methods for simulation of 3D NOE-NOE spectra

An exact full matrix analysis of 2D NOESY spectroscopy has been extended to 3D homonuclear NOE-NOE spectroscopy and applied to the simulation of NOE-NOE spectra of the Dickerson dodecamer d(CGCGAATTCGCG)2 and a tandem GA mismatched decamer deoxynucleotide duplex d(CCAAGATTGG)2. The exact method has been compared with the approximation method based on Taylor expansions. It has been found that the approximations using one or two terms in the Taylor expansion series are generally inadequate for simulations of 3D NOE-NOE volumes and fail at very short mixing times, depending on the motional properties of the biomolecule in question. Specifically, the first-order approximation fails at tau c tau m > or = 1.8 x 10(-10) s2 for both the dodecamer and the decamer if an RMS error in the volumes of < 50% is desired.