Table 2.
Ac-GAY-NMea | |||
---|---|---|---|
Yb | Δ(φ = −60; ψ = −40)c | Δ(φ = −60; ψ = −60)c | Δ(φ = −140; ψ = +140)c |
Thr | 1.0 | 1.7 | 0.6 |
Asp | 1.4 | 0.9 | −0.3 |
Val | 0.7 | 1.5 | 0.3 |
Met | 0.7 | 1.1 | 0.1 |
Trp | 0.4 | 0.7 | 0.1 |
Tyr | 0.2 | 0.2 | −0.2 (0.8)d |
Gln | −1.0 | −0.5 | −0.3 |
Pro | −2.3 | 1.1 | −1.1 |
Gly | 0.6 | 1.2 | −0.1 |
All the listed results, in terms of Δ, were obtained assuming that the backbone torsional angles (φ,ψ)Y of residue Y are fixed at a canonical α–helix conformation, namely φ = −60° and ψ = −40°. The Δ values were computed as: Δ = (13C′A − 13C′Y) where 13C′A is the isotropic shielding value of residue A (Ala) in the tripeptide Ac-GAA-NMe, and 13C′Y is the isotropic shielding value of residue A in the tripeptide Ac-GAY-NMe, with the identity of residue Y listed in column 1.
Identity (by using a three letter code) of residue Y in the tripeptide Ac-GAY-NMe.
The sub index of Δ represents the particular backbone (φ,ψ) torsional angles chosen for the residue A, among all possible ones from the Ramachandran map. Those values for which |Δ| > 0.5 ppm are highlighted in boldface and italics.
In parentheses, an alternative value for Δ, (0.8), was computed for a slightly-shifted set of backbone torsional angles, namely (φ = −40°; ψ = +20°) rather than (φ = −40°; ψ = +40°); this result illustrates that the same absolute value of |Δ| computed for Tyr (0.2), in each column of this Table, is just a coincidence, and that the nature of residue Y, matters.