Table 1.
Unambiguous distance constraints calculated from paramagnetic line broadening effects and used in the structural determination
Atom | Iox/Ired | R2SP (Hz) | ra (Å) |
---|---|---|---|
E35 (NH) | N/Ab | N/Ab | 20 + 4Å |
I37 (NH) | N/Ab | N/Ab | 20 + 4Å |
Y24 (NH) | 0.209 | 80.8 | 22.4 ± 4Å |
Q44 (HE21) | 0.330 | 54.9 | 24.7 ± 4Å |
Q44 (HE22) | 0.330 | 54.9 | 24.7 ± 4Å |
N46 (HD21) | 0.330 | 54.9 | 24.7 ± 4Å |
N46 (HD22) | 0.330 | 54.9 | 24.7 ± 4Å |
A22 (NH) | 0.376 | 45.6 | 24.3 ± 4Å |
A86 (NH) | 0.504 | 30.4 | 25.4 ± 4Å |
W48 (NH) | 0.533 | 31.5 | 25.3 ± 4Å |
W69 (HE1) | 0.541 | 25.3 | 26.0 ± 4Å |
A85 (NH) | 0.574 | 26.2 | 25.9 ± 4Å |
T89 (NH) | 0.593 | 27.6 | 25.7 ± 4Å |
Notes: Distance constraints between the spin label and the amide or sidechain protons of individual residues.
The peaks in the oxidized spectrum are too broad to be observed. In these cases, the distance constraints were set with upper bounds 20 Å plus 4 Å and no lower bound was used. Details are described in the Materials and Methods section.