TABLE 1.
Experimental NOE | Range | Computed NOE | |||
---|---|---|---|---|---|
HC11 | G*6 | H1′ | G18 | [2.76, 4.76] | 4.37 (0.43) |
HC9 | G*6 | H1′ | C7 | [2.03, 3.23] | 2.31 (0.30) |
HC10 | G*6 | H1′ | C7 | [2.81, 4.41] | 4.24 (0.52) |
HC2 | G*6 | H4′ | A19 | [2.94, 4.54] | 3.16 (0.45) |
HC9 | G*6 | H1′ | G*6 | [4.00, 6.00] | 4.65 (0.49) |
HC10 | G*6 | H1′ | G*6 | [2.85, 4.45] | 3.74 (0.25) |
HC10 | G*6 | HN | G*6 | [2.50, 4.50] | 2.97 (0.06) |
HC8 | G*6 | HN | G*6 | [2.00, 4.00] | 2.37 (0.20) |
HC9 | G*6 | HN | G*6 | [3.00, 5.00] | 3.22 (0.17) |
HC8 | G*6 | H1 | G*6 | [2.68, 4.68] | 3.91 (0.23) |
HC9 | G*6 | H1 | G*6 | [3.53, 5.53] | 4.50 (0.20) |
HC8 | G*6 | H1 | G16 | [3.25, 5.25] | 4.69 (0.50) |
HC8 | G*6 | H1 | G18 | [3.30, 5.30] | 7.29 (0.37) |
1HC4 | G*6 | H5′1 | G18 | [3.17, 5.17] | 6.32 (0.72) |
1HC4 | G*6 | H5′2 | G18 | [3.17, 5.17] | 6.74 (0.73) |
1HC5 | G*6 | H5′1 | G18 | [3.17, 5.17] | 4.91 (0.52) |
1HC5 | G*6 | H5′2 | G18 | [3.17, 5.17] | 4.84 (0.57) |
2HC6 | G*6 | H5′1 | G18 | [2.13, 4.13] | 5.01 (0.46) |
2HC6 | G*6 | H5′2 | G18 | [2.13, 4.13] | 4.11 (0.41) |
3HC4 | G*6 | H4′ | G18 | [2.31, 4.31] | 4.46 (0.58) |
3HC4 | G*6 | H4′ | A19 | [2.31, 4.31] | 4.15 (0.93) |
3HC5 | G*6 | H4′ | G18 | [2.31, 4.31] | 2.93 (0.37) |
3HC5 | G*6 | H4′ | A19 | [2.31, 4.31] | 5.85 (0.86) |
4HC1 | G*6 | H4′ | A19 | [2.69, 4.69] | 4.09 (0.79) |
4HC3 | G*6 | H4′ | A19 | [2.69, 4.69] | 2.98 (0.64) |
NOEs for grouped proton pairs (groups 1, 2, 3, and 4) were assigned to any one of the pair members. Consequently they have identical bounds, as they could not be distinguished (Cosman et al., 1992).