A two-dimensional solid-state NMR technique is presented that can be used to determine the 15 N chemical shift and 1 H− 15 N dipolar coupling tensors in powder samples of polypeptides containing 15 N isotopes at multiple sites. By combining the magic-angle rf decoupling in one time period and the magic-angle turning pulse sequence in another time period of a 2D experiment, we obtain 2D spectra in which the convoluted chemical shift anisotropy (CSA) and dipolar coupling line shapes appear along one axis and the normal MAS spectrum appears along the other axis. The magnitudes of the principal elements of the 15 N CSA tensors and their orientations in the molecular frame for n -acetyl- 15 N- l -Val- 15 N- l -Leu (NAVL) and n -acetyl- 15 N- d, l -Val (NAV) powder samples are determined using this method. The magnitudes of the 15 N CSA tensors are 60.2 ± 1, 87.1 ± 1, and 230.1 ± 1 ppm for the Val residue in NAVL; 58.7 ± 1, 93.7 ± 1, and 232.8 ± 1 ppm for the Leu residue in NAVL; 59.6 ± 1, 80.5 ± 1, and 235.3 ± 1 ppm for site I in NAV; and 57.5 ± 2, 81.0 ± 2, and 227.0 ± 2 ppm for site II in NAV. The experimental results also suggest that the most-shielded axis, σ 11N, and the σ 22N axis of the 15 N CSA tensor are significantly tilted away from the peptide plane and the normal to the peptide plane, respectively. The tilt angles (α N ) are 34 ± 12° for Val and 36 ± 11° for Leu in NAVL, whereas it is 5 ± 22° in NAV. The angles (β N ) between the least-shielded axis of the 15 N CSA tensor, σ 33N, in the peptide plane and the N−H bond are determined to be 20 ± 2° for Val and 18 ± 2° for Leu in NAVL and 21 ± 2° for NAV. The values are in good agreement with some of the recent solid-state NMR experimental studies on peptides. The values for the β N angle reported in this study are also in agreement with the solution NMR studies on water-soluble proteins.
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Lee et al. (2001) studied this question.
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