TABLE 2.
Parameter | Valuea found for crystal: |
|
---|---|---|
MolA | PuhB | |
Space group | I212121 | P2 |
Unit-cell parameters | ||
a (Å) | 126.43 | 77.37 |
b (Å) | 226.32 | 100.52 |
c (Å) | 265.38 | 238.55 |
β (°) | 90, 90, 90 | 90, 90.37, 90 |
Wavelength (Å) | 0.9537 | 0.9537 |
Resolution range (Å) | 48.94–2.29 (2.33–2.29) | 39.60–2.96 (3.02–2.96) |
No. of unique reflections | 170,085 | 75,147 |
Completeness (%) | 99.9 (99.0) | 99.2 (99.8) |
Multiplicity | 20.3 (13.5) | 5.6 (5.4) |
Rmerge(I)b | 0.182 (2.201) | 0.201 (0.683) |
Rpimc | 0.059 (0.893) | 0.135 (0.474) |
Mean I/σ(I) ratio | 16.3 (1.6) | 8.3 (2.6) |
CC1/2d | 0.998 (0.564) | 0.981 (0.752) |
Refinement | ||
No. of reflections used | 170,085 | 75,147 |
Resolution range (Å) | 48.94–2.29 (2.33–2.29) | 39.60–2.96 (3.02–2.96) |
RWork/RFreee | 0.1761/0.2032 (0.2917/0.3272) | 0.2438/0.2806 (0.3510/0.4233) |
RMS deviations | ||
Bond length (Å) | 0.008 | 0.015 |
Bond angle (°) | 1.18 | 1.76 |
PDB ID | 4WGX | 4WHB |
Values in parentheses are for the highest-resolution shell.
Rmerge(I) = Rmerge(I) = (Σhkl Σj |Ihkl,j − 〈Ihkl〉|)/(Σhkl Σj Ihkl,j), where 〈Ihkl〉 is the average intensity of j symmetry-related observations of reflections with Miller indices hkl.
Rpim = (Σhkl Σj |Ihkl,j − 〈Ihkl〉|)/(Σhkl Σj Ihkl,j).
CC1/2 = percentage of correlation between intensities from random half-data sets.
RWork = Σhkl|F(obs) − F(calc)|/Σhkl|F(obs)|; 5% of the data that were excluded from the refinement were used to calculate RFree.