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The structure of the Ras-binding domain of human c-Raf-1 (residues 55-132) has been determined in solution by nuclear magnetic resonance (NMR) spectroscopy. Following complete assignment of the backbone and side-chain 1H, 15N, and 13C resonances, the structure was calculated using the program CHARMM. Over 1300 NOE-derived constraints were applied, resulting in a detailed structure. The fold of Raf55-132 consists of a five-stranded beta-sheet, a 12-residue alpha-helix, and an additional one-turn helix. It is similar to those of ubiquitin and the IgG-binding domain of protein G, although the three proteins share very little sequence identity. The surface of Raf55-132 that interacts with Ras has been identified by monitoring perturbation of line widths and chemical shifts of 15N-labeled Raf55-132 resonances during titration with unlabeled Ras-GMPPNP. The Ras-binding site is contained within a spatially contiguous patch comprised of the N-terminal beta-hairpin and the C-terminal end of the alpha-helix.

Raf-1 is a 74-kDa serine-threonine kinase which serves as the immediate downstream target of Ras in the cell growth signal transduction pathway. Recent genetic and biochemical experiments have demonstrated that (1) Ras interacts directly with the amino-terminal domain of Raf and (2) residues 51-131 of the Raf sequence are sufficient to mediate this interaction [Vojtek, A. B., Hollenberg, S. M., & Cooper, J. A. (1993) Cell 74, 205-214]. We have expressed a corresponding segment of the human Raf sequence (Raf55-132) in Escherichia coli as a fusion with maltose binding protein. The fusion protein was purified by affinity chromatography and cleaved at a pre-engineered site with factor Xa protease to liberate the 78-residue fragment of Raf. Raf55-132 bound to Ras with high affinity in a competition assay with GAP. An unlabeled version of Raf55-132 was studied by 2D homonuclear NMR, and uniformly 15N- and 13C/15N-labeled versions of Raf55-132 were studied by 2D and 3D heteronuclear NMR. Nearly complete sequence-specific assignments were made for the backbone HN, H alpha, 15N, and 13C alpha resonances. NOEs were used to determine regions of secondary structure and the overall folding topology. Raf55-132 is an independently folded domain composed of a five-stranded beta-sheet, a three-turn alpha-helix, and possibly an additional one-turn helix. Its structure resembles that of ubiquitin, even though there is no more than 11% sequence homology between the two proteins.

Steady-state nuclear Overhauser effects (NOE), two-dimensional (2D) nuclear Overhauser effect spectroscopy (NOESY), and 2D spin correlation spectroscopy (COSY) have been applied to the fully paramagnetic low-spin, cyanide-ligated complex of sperm whale ferric myoglobin to assign the majority of the heme pocket side-chain proton signals and the remainder of the heme signals. It is shown that the 2D NOESY map reveals essentially all dipolar connectivities observed in ordinary 1D NOE experiments and expected on the basis of crystal coordinates, albeit often more weakly than in a diamagnetic analogue. For extremely broad (approximately 600-Hz) and rapidly relaxing (Tf1 approximately 3 ms) signals which show no NEOSY peaks, we demonstrate that conventional steady-state NOEs obtained under very rapid pulsing conditions still allow detection of the critical dipoar connectivities that allow unambiguous assignments. The COSY map was found to be generally less useful for the hyperfine-shifted residues, with cross peaks detected only for protons greater than 6 A from the iron. Nevertheless, numerous critical COSY cross peaks between strongly hyperfine-shifted peaks were resolved and assigned. In all, 95% (53 of 56 signals) of the total proton sets within approximately 7.5 A of the iron, the region experiencing the strongest hyperfine shifts and paramagnetic relaxation, are now unambiguously assigned. Hence it is clear that the 2D methods can be profitably applied to paramagnetic proteins. The scope and limitations of such application are discussed. The resulting hyperfine shift pattern for the heme confirmed expectations based on model compounds. In contrast, while exhibiting fortuitous 1H NMR spectral similarities, a major discrepancy was uncovered between the hyperfine shift pattern of the axially bound (F8 histidyl) imidazole in the protein and that of the imidazole in a relevant model compound [Chacko, V.P., & La Mar, G. N. (1982) J. Am. Chem. Soc. 104, 7002-7007], providing direct evidence for a protein-based deformation of axial bonding in the protein.

The experimentally determined paramagnetic dipolar shifts for noncoordinated amino acid side-chain protons in the heme pocket of sperm whale cyanometmyoglobin [Emerson, S. d., & La Mar, G. N. (1990) Biochemistry (preceding paper in this issue]) were used to determine in solution the orientation of the principal axes for the paramagnetic susceptibility tensor relative to the heme iron molecular coordinates. The determination was made by a least-squares search for the unique Euler rotation angles which convert the geometric factors in the molecular (crystal) coordinates to ones that correctly predict each of 41 known dipolar shifts by using the magnetic anisotropies computed previously [Horrocks, W. D., Jr., & Greenberg, E. S. (973) Biochim. Biophys. Acta 322, 38-44]. An excellent fit to experimental shifts was obtained, which also provided predictions that allowed subsequent new assignments to be made. The magnetic axes are oriented so that the z axis is tipped approximately 15 degrees from the heme normal toward the hem delta-meso-H and coincides approximately with the characterized FeCO tilt axis in the isostructural MbCO complex [Kuriyan, J., Wilz, S., Karplus, M., & Petsko, G. A. (1986) J. Mol. Biol. 192, 133-154]. Since the FeCO and FeCN units are isostructural, we propose that the dominant protein constraints that tips the magnetic z axis from the heme normal is the tilt of the FeCN by steric interactions with the distal residues. The rhombic magnetic axes were found to align closely with the projection of the proximal His imidazole plane on the heme, confirming that the His-Fe bonding provides the protein constraints that orients the in-plane anisotrophy. The tipped magnetic z axis is shown to account quantitatively for the previously noted major discrepancy between the hyperfine shift patterns for the bound imidazole side chain in models and protein. Moreover, it is shown that the proximal His ring nolabile proton hyperfine shifts provide direct and exquisitely sensitive indicators of the degree of the z axis tilt that may serve as a valuable probe for characterizing variable steric interactions in the distal pocket of both point mutants and natural genetic variants of myoglobin.