Position dependence of the 13C chemical shifts of alpha-helical model peptides. Fingerprint of the 20 naturally occurring amino acids

Effects of side-chain orientation on the 13C chemical shifts of antiparallel beta-sheet model peptides

The dependence of the (13)C chemical shift on side-chain orientation was investigated at the density functional level for a two-strand antiparallel beta-sheet model peptide represented by the amino acid sequence Ac-(Ala)(3)-X-(Ala)(12)-NH(2) where X represents any of the 17 naturally occurring amino acids, i.e., not including alanine, glycine and proline. The dihedral angles adopted for the backbone were taken from, and fixed at, observed experimental values of an antiparallel beta-sheet. We carried out a cluster analysis of the ensembles of conformations generated by considering the side-chain dihedral angles for each residue X as variables, and use them to compute the (13)C chemical shifts at the density functional theory level. It is shown that the adoption of the locally-dense basis set approach for the quantum chemical calculations enabled us to reduce the length of the chemical-shift calculations while maintaining good accuracy of the results. For the 17 naturally occurring amino acids in an antiparallel beta-sheet, there is (i) good agreement between computed and observed (13)C(alpha) and (13)C(beta) chemical shifts, with correlation coefficients of 0.95 and 0.99, respectively; (ii) significant variability of the computed (13)C(alpha) and (13)C(beta) chemical shifts as a function of chi(1) for all amino acid residues except Ser; and (iii) a smaller, although significant, dependence of the computed (13)C(alpha) chemical shifts on chi(xi) (with xi > or = 2) compared to chi(1) for eleven out of seventeen residues. Our results suggest that predicted (13)C(alpha) and (13)C(beta) chemical shifts, based only on backbone (phi,psi) dihedral angles from high-resolution X-ray structure data or from NMR-derived models, may differ significantly from those observed in solution if the dihedral-angle preferences for the side chains are not taken into account.

Energetic characterization of short helical polyalanine peptides in water: analysis of 13C=O chemical shift data

Measured at 2 degrees C in water, NMR chemical shifts of (13)C=O labeled central alanine residues of peptides W-Lys(5)-(t)L(3)-Ala(n)-(t)L(3)-Lys(5)NH(2), n = 9, 11, 13, 15, 19 and W-Lys(5)-(t)L(3)-a-Ala(n)-A-Inp-(t)L(2)-Lys(5)NH(2) (a = D-Ala; (t)L = tert-leucine; Inp = 4-carboxypiperidine) are used to assign jt(L) and ct(L), the N- and C-terminal (t)L capping parameters and length-dependent values for w(Ala)(n), the alanine helical propensity for Ala(n) peptides. These parameters allow Lifson-Roig characterization of the stabilities of Ala(n)() helices in water. To facilitate chemical shift characterization, different (13)C/(12)C ratios are incorporated into specific Ala sites to code up to six residue sites per peptide. Large left/right chemical shift anisotropies are intrinsic to helical polyalanines, and a correcting L-R-based model is introduced. Capping parameters jt(L) = ct(L) lie in the range of 0.3 to 0.5; the (t)L residues are thus moderately helix-destabilizing. For helical conformations of lengths shorter than eight residues, assigned values for w(Ala) approach 1.0 but increase monotonically with length to a value of 1.59 for w(Ala)(19).