Table 2. Effect of structural noise on relative orientations and changes therein of the terminal regions of native and modified Dickerson dodecamers.
| DNA oligomer | α, ° | β, ° | γ, ° |
|---|---|---|---|
| Native† | 1.3 ± 3.2 | 1.0 ± 5.0 | –1 ± 14 |
| T8* | –2.4 ± 3.9 | 0.6 ± 3.8 | 10 ± 10 |
| T8*-native† | –3.7 ± 1.6 | –0.5 ± 2.9 | 11 ± 15 |
| Native† | 0.6 ± 3.0 | 1.3 ± 5.3 | 11 ± 22 |
| T7* | –8.6 ± 1.9 | 1.8 ± 3.8 | 2 ± 13 |
| T7*-native‡ | –9.3 ± 1.7 | 0.5 ± 2.7 | –9 ± 12 |
| Native† | 1.6 ± 3.2 | 1.6 ± 4.7 | 3 ± 24 |
| T7*T8* | –12.7 ± 3.5 | 0.9 ± 3.8 | 17 ± 9 |
| T7*T8*-native‡ | –14.2 ± 1.6 | –0.7 ± 3.0 | 14 ± 22 |
Average and standard deviation of RDC-derived rotation angles between the terminal domains of the structure of the native dodecamer (PDB entry 1NAJ) and a set of 20 noise-contaminated reference structures. Only RDCs in the terminal three base pairs (terminal four base pairs for T7*) that were measured in both the native and modified oligomer are used to define the rotation angles
Average and standard deviation of pairwise difference in rotation angles obtained from data measured for modified and native dodecamers, for a set of 20 noise-contaminated reference structures