Table 1.
K46 | K55 | K57 | K58 | |
---|---|---|---|---|
15N R1 (s−1) b) | 1.093 ± 0.013 | 0.637 ± 0.005 | 1.035 ± 0.004 | 0.363 ± 0.002 |
15N R1 (s−1) c) | 1.081 ± 0.023 | 0.617 ± 0.008 | 1.037 ± 0.008 | 0.364 ± 0.003 |
15N R2,ini (s−1) b) | 2.55 ± 0.10 | 1.76 ± 0.07 | 2.95 ± 0.04 | 1.20 ± 0.03 |
15N R2,ini (s−1) c) | 2.74 ± 0.20 | 2.05 ± 0.12 | 2.76 ± 0.06 | 1.14 ± 0.06 |
Heteronuclear NOE b) | −2.44 ± 0.12 | −2.83 ± 0.10 | −2.54 ± 0.05 | −2.71 ± 0.05 |
Heteronuclear NOE c) | −2.53 ± 0.18 | −2.75 ± 0.13 | −2.60 ± 0.08 | −2.65 ± 0.07 |
The experiments were conducted at 15 °C and the 1H frequency of 750 MHz. Uncertainties were estimated using the Monte Carlo approach based on the noise standard deviation of the spectra.
Measured with the current pulse sequences shown in Figure 1.
Measured with the previous pulse sequences [15].