Table 4.
Protein | N a | RMS deviationsb [Hz] | ||||
---|---|---|---|---|---|---|
<3J> | 3Jna | 3JANN | <(3Jna+3JANN)/2> | 3JSearle | ||
Aβ(1–40) | 30 | 0.45 | 0.38 | 0.37 | 0.37 | 0.42 |
α‐synuclein | 111 | 0.39 | 0.29 | 0.29 | 0.29 | 0.50 |
Protease | 64 | 0.44 | 0.38 | 0.42 | 0.38 | 0.43 |
Integrase‐N | 44 | 0.47 | 0.41 | 0.36 | 0.37 | 0.58 |
Ubiquitinc | 65 | 0.45 | 0.41 | 0.38 | 0.38 | 0.42 |
GGXGGd | 18 | 0.43 | 0.43 | 0.28 | 0.31 | 0.37 |
All | 332 | 0.43 | 0.37 | 0.36 | 0.35 | 0.47 |
Number of experimental 3J HN‐Hα couplings for each test set; for N‐terminally acetylated α‐synuclein, the first six residues have partial helical character and were excluded; temperature correction48 was applied to experimental data if not measured at 20°C, including a +0.16 Hz correction for Aβ (measured at 4°C) and a −0.10 Hz correction for denatured ubiquitin data (measured at 30°C); pressure correction of +0.08 Hz/kbar49 is applied to the experimental data not acquired at 1 bar, including a +0.20 Hz correction for both pressure‐denatured HIV‐1 Protease and the N‐terminal DNA‐binding domain of HIV‐1 Integrase (both collected at 2500 bar).
RMSD between experimental and predicted 3J HN‐Hα coupling constants; <3J> is the difference relative to the average 3J HN–Hα value calculated using Eq. (2) for residues of type X in the newly generated coil library, 3Jna is calculated relative to <3J> plus the neighbor adjustments of Table 3; 3JANN is the RMSD relative to values predicted by the ANN‐based Eq. (4). 3JANN values for each of the 8000 triplets are also available at https://spin.niddk.nih.gov/bax/nmrserver/rc_3Jhnha/ann_results.txt; 3JSearle is the RMSD relative to the neighbor‐corrected coil values of Searle and co‐workers.15
From Peti et al.50
From Shi and Kallenbach.33