Table 3. Measured NMR and MD-Predicted 3J Couplings (hertz) at 278 K for Each Force Field with the A-Form (C3′-endo/anti) Starting Structure.
| torsion | NMR scalar couplinga | parm99b | parm99χb | parm99TORb,c | A-formd | angle (deg)e |
|---|---|---|---|---|---|---|
| C1 H1′–H2′ | ≤1.0 | 5.6 | 0.7 | 0.5 (0.6) | 0.0–1.0 | 91–104 |
| C2 H1′–H2′ | ≤1.0 | 4.6 | 0.5 | 0.5 (0.7) | 0.0–1.0 | 91–104 |
| C3 H1′–H2′ | ≤1.0 | 3.6 | 0.6 | 0.5 (0.6) | 0.0–1.0 | 91–104 |
| C4 H1′–H2′ | 2.6 | 6.7 | 1.5 | 1.8 (1.9) | 0.0–1.0 | 116 |
| C1 H2′–H3′ | 3.6 | 5.1 | 4.4 | 4.3 (4.3) | 3.8–4.8 | 50 |
| C2 H2′–H3′ | 4.3 | 5.0 | 4.4 | 4.4 (4.3) | 3.8–4.8 | 42 |
| C3 H2′–H3′ | 4.7 | 5.1 | 4.5 | 4.4 (4.4) | 3.8–4.8 | 38 |
| C4 H2′–H3′ | 4.9 | 5.1 | 4.7 | 4.9 (4.8) | 3.8–4.8 | 36 |
| C1 H3′–H4′ | 8.7 | 5.2 | 7.7 | 7.8 (7.8) | 7.6–8.6 | f |
| C3 H3′–H4′ | 8.8 | 5.8 | 7.7 | 7.9 (7.9) | 7.6–8.6 | f |
| C4 H3′–H4′ | 7.2 | 3.6 | 7.1 | 6.7 (7.0) | 7.6–8.6 | 205 |
| C2 H4′–H5′ | ≤1.0 | 2.5 | 2.6 | 2.8 (3.0) | 1.6–2.6 | f |
| C3 H4′–H5′ | 2.1 | 2.3 | 2.5 | 2.8 (2.8) | 1.6–2.6 | 63 |
| C4 H4′–H5′ | 2.0 | 2.3 | 2.5 | 3.7 (2.9) | 1.6–2.6 | 62 |
| C2 H4′–H5″ | ≤1.0 | 4.9 | 3.9 | 3.2 (3.1) | 2.9–4.4 | f |
| C3 H4′–H5″ | ≤1.0 | 3.8 | 3.5 | 3.1 (3.2) | 2.9–4.4 | f |
| C4 H4′–H5″ | 1.4 | 4.3 | 3.8 | 3.4 (3.5) | 2.9–4.4 | 292 |
| C1 H3′–C2 P | 8.8 | 5.1 | 8.7 | 7.1 (8.3) | 6.9–9.4 | 1 |
| C2 H3′–C3 P | 9.3 | 5.6 | 9.0 | 3.8 (5.2) | 6.9–9.4 | 3 |
| C3 H3′–C4 P | 9.3 | 5.8 | 8.6 | 4.7 (5.0) | 6.9–9.4 | 3 |
| C2 P–C2 H5′ | 3.8 | 3.1 | 3.8 | 4.2 (5.0) | 3.4–6.6 | 309 |
| C3 P–C3 H5′ | 3.9 | 3.8 | 3.8 | 3.7 (4.1) | 3.4–6.6 | 309 |
| C4 P–C4 H5′ | 3.8 | 2.7 | 3.6 | 6.2 (4.3) | 3.4–6.6 | 309 |
| C2 P–C2 H5″ | 1.2 | 3.0 | 2.3 | 2.6 (2.4) | 0.9–1.9 | 72 |
| C3 P–C3 H5″ | 0.5 | 2.4 | 2.2 | 2.5 (2.2) | 0.9–1.9 | f |
| C4 P–C4 H5″ | 1.1 | 3.3 | 2.4 | 4.2 (3.7) | 0.9–1.9 | 74 |
The error limit is ±0.5 Hz for scalar couplings of >1.0 Hz.
Marino et al.54 equations (Table S13 of the Supporting Information) were used to calculate 3J couplings for each time point of the MD trajectory, and then the couplings were averaged.
Parentheses indicate MD predicted 3J scalar coupling values calculated from 0 to 770 ns. After 770 ns, C1 intercalates between C3 and C4.
Range of values measured from four CC doublets in PDB entry 1QC0.57
Torsion angles determined via NMR (Table S13 of the Supporting Information). For scalar couplings of <1.0 Hz, an angle range covering 0–1 Hz is shown.
Could not be calculated with Marino et al.54 equations (Table S13 of the Supporting Information).