Table 1.
RDCs with no noise | RDCs with random noisea | |
---|---|---|
RDC R-factor (%)b | 19.0±0.4 | 19.6±0.7 |
RDC DaNH (Hz) | 11.1±0.2 | 11.1±2.4 |
RDC η | 0.59±0.02 | 0.58±0.06 |
SAXS/WAXSc | ||
q = 0.022 → 0.44 Å−1 | 0.58±0.09 | 0.58±0.13 |
q = 0.022 → 1.0 Å−1 | 0.76±0.16 | 0.78±0.19 |
Coordinate precision | ||
EIN domaind | ||
Cα rms displacement (Å) | 2.2 | 2.7 |
rotation (deg.) | 5.8 | 7.3 |
EINα subdomaine | ||
Cα rms displacement (Å) | 2.1 | 2.5 |
rotation (deg.) | 3.8 | 5.3 |
2% random noise added to experimental RDCs with a different distribution of random noise for each structure calculated. The values of the RDC R-factor, DaNH and η are reported with respect to the experimental RDCs (with no noise added). The RDC R-factor is calculated as Rinf = [<(Dobs-Dcalc)2>/(2<Dobs2>]1/2 where Dobs and Dcalc are the observed and calculated RDCs, respectively.18
The RDC data comprise 40×2 backbone N-H RDCs for the dimer, 20 for each subdomain of each EIN subunit.
Structures are refined against SAXS/WAXS data for q ≤0.44 Å−1 and the χ2 values reported for all the data (up to q = 1.0 Å−1) are obtained with the parameters from the fits to the data up to q = 0.44 Å−1; these χ2 values therefore report on how well the structures obtained using data up to q = 0.44 Å−1 predict the data from q = 0.44 to 1.0 Å−1.
The EIC domain is superimposed and fixed, and the position of the EIN domain compared.
The EINα/β subdomain is superimposed and fixed, and the position of the EINα subdomain is compared.