Extended Data Fig. 3: In the absence of magnesium, the open/closed rate exchange rate is in the slow exchange regime, in agreement with earlier reports25.
From: Structure determination of high-energy states in a dynamic protein ensemble

(a) [1H, 15N]-HSQC spectra for Zn2+ and Co2+ samples with either 20 mM ADP or 20 mM Mg2+ADP. Residues that were broadened in the Mg2+ADP sample show reduced linewidths in the ADP sample, indicating a shift in exchange timescales from intermediate to slow exchange. Black lines trace the PCSs between diamagnetic and paramagnetic samples. For residue 38, the corresponding diamagnetic peaks are at 8.46 ppm (1H) and 123.5 ppm (15N) and are not shown for illustration purposes. (b) 1HN CPMG dispersion profiles for Co2+ Adk with 20 mM ADP and 0 mM Mg2+. Representative traces show slow exchange that is fit to the Tollinger equation75 (F-statistics were used to determine whether the description by a slow exchange model compared to a “no-exchange” model was justified at the 95% confidence interval; p>0.05). (c) Representative CPMG relaxation dispersion profiles for residues in the presence on 20 mM Mg2+ADP. Notably, the paramagnetic chemical shift differences in the absence and presence of magnesium are similar, whereas the timescale is significantly altered (kopen, ADP = 2.6 ± 0.3 s−1 vs kopen, ADP = 180 ± 36 s−1). Uncertainties (s.d.) in R2,eff are determined from the rmsd in the intensities of duplicate points (n = 3) according to the definition of pooled relative standard deviation. Uncertainties (s.d.) in chemical shift differences were calculated from the covariance matrix.