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The major coat protein (gVIIIp) of bacteriophage M13 solubilized in sodium dodecyl sulfate (SDS) detergent micelles was used as a model system to study this protein in the lipid-bound form. In order to probe the position of gVIIIp relative to the SDS micelles, stearate was added, spin-labeled at the 5- or 16-position with a doxyl group containing a stable nitroxide radical. The average position of the spin-labels in the micelles was derived from the line broadening of the resonances in the 13C spectrum of SDS. Subsequently, we derived a model of the relative position of gVIIIp in the SDS micelle from the effect of the spin-labels on the gVIIIp resonances, monitored via 1H-15N HSQC and TOCSY experiments. The results are consistent with the structure of gVIIIp having two helical strands. One strand is a long hydrophobic helix that spans the micelle, and the other is a shorter amphipathic helix on the surface of the micelle. These results are in good agreement with the structure of gVIIIp in membranes proposed by McDonnell et al. on the basis of solid state NMR data [McDonnell, P. A., Shon, K., Kim, Y., & Opella, S. J. (1993) J. Mol. Biol. 233, 447-463]. This study indicates that high-resolution NMR on this membrane protein, solubilized in detergent micelles, is a very suitable technique for mimicking these proteins in their natural environment. Furthermore, the data indicate that the structure of the micelle near the C-terminus of the major coat protein is distorted.(ABSTRACT TRUNCATED AT 250 WORDS)

The hairpin formed by d(ATCCTATTTATAGGAT) was studied by means of two-dimensional NMR spectroscopy and conformational analysis. Almost all 'H resonances of the stem region could be assigned, while the 'H and 31P spectra of the loop region were interpreted completely; this includes the stereospecific assignment of the H5' and H5" resonances. The derivation of the detailed loop structure was carried out in a stepwise fashion including some improved and new methods for structure determination from NMR data. In the first step, the mononucleotide structures were examined. The conformational space available to the mononucleotide was scanned systematically by varying the glycosidic torsion angle and pseudorotational parameters. Each generated conformer was tested against the experimental J coupling constants and NOE parameters. In the following stage, the structures of dinucleotides and longer fragments were derived. Inter-residue distances between protons were calculated by means of a procedure in which the simulated NOEs, obtained via a relaxation-matrix approach, were fitted to the experimental NOEs without the introduction of a molecular model. In addition, the backbone torsion angles fl, y and c were deduced from homocoupling and heterocoupling constants. These data served as constraints in the next step, in which the loop sequence was subjected to a multi-conformer generation procedure. The resulting structures were tested against the mentioned constraints and disregarded if these constraints were violated. This yielded a family of structures for the loop region, confined to a relatively narrow conformational space. A representative conformation was subsequently docked on a B-type stem which fulfilled the structural constraints (derived from the NMR experiments for the stem region) to yield the hairpin structure. Results obtained from subsequent restrained-molecular-mechanics as well as free-molecular-mechanics calculations are in accordance with those obtained by means of the analysis described above.The structure of the hairpin loop is a compactly folded conformation and the first base of the central TTTA region forms a Hoogsteen T-A pair with the fourth base. This Hoogsteen base pair is stacked upon the sixth base pair of the B-type double-helical stem. The second base of the loop is folded into the minor groove, whereas the third base of the loop is partly stacked on the first and fourth bases. The phosphate backbone exhibits a sharp turn between the third and fourth nucleotides of the loop. The peculiar structure of this hairpin loop is discussed in relation to loop folding in DNA and RNA hairpins and in relation to a general model for loop folding.Loop structures in RNA and DNA hairpins have been the subject of numerous studies. We have been interested in these structures because they may serve as models for the folding which occurs in RNA and DNA molecules in the cell, and also because they may provide insight into the mechanism underlying the folding. Our initial studies were concerned with the hairpin fo...

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The backbone dynamics of the major coat protein (gVIIIp) of the filamentous bacteriophage M13, solubilized in detergent micelles, have been studied using 15N nuclear magnetic resonance spectroscopy at three frequencies. Motional parameters and overall and internal correlation times were derived with the model-free approach. It was also checked whether these parameters had to be modified due to anisotropic motion of the protein/micelle complex. Reduced spectral density mapping was used to calculate the spectral densities at J(O), J(omegaN), and [J(omegaH)]. The spectral densities were interpreted by mapping a linear or scaled linear combination of two Lorentzians onto a J(O)-J(omega) plot. The major coat protein of bacteriophage M13 consists of two alpha-helices, one of which is hydrophobic and located within the micelle, while the other is amphipathic and located on the surface of the micelle. Our results indicate that the motion of the hydrophobic helix is restricted such that it corresponds to the overall tumbling of the protein/micelle complex. The interpretation of the relaxation data of the amphipathic helix by means of the model-free approach and the reduced spectral density mapping indicate that in addition to the overall motion all residues in this helix are subject to motion on the fast nanosecond and picosecond time scales. The motions of the vectors in the low nanosecond range are characterized by similar values of the spectral densities and correlation times and represent the motion of the amphipathic helix on and away from the surface of the micelle. The relaxation data of the residues in the hinge region connecting the helices show that there is an abrupt change from highly restricted to less restricted motion. Both the C-terminal and N-terminal residues are very mobile.