Table 5.
Free loop | Bound loop | |||
---|---|---|---|---|
Bin size | nf (j) | |||
Δαk/15 | 250 (1) | 67.18 (4) | 68.72 (4) | −1.5 |
“ | 500 (2) | 66.48 (7) | 67.86 (8) | −1.4 |
“ | 750 (3) | 66.17 (4) | 67.58 (8) | −1.4 |
“ | 1250 (5) | 65.74 (4) | 67.19 (8) | − 1.4 |
Δαk/30 | 250 (1) | 67.04 (9) | 68.61 (7) | −1.6 |
“ | 500 (2) | 66.22 (7) | 67.61 (7) | −1.4 |
“ | 750 (3) | 65.77 (4) | 67.15 (8) | −1.4 |
“ | 1250 (5) | 65.19 (4) | 66.49 (3) | − 1.3 |
Δαk/45 | 250 (1) | 67.03 (4) | 68.60 (5) | −1.6 |
“ | 500 (2) | 66.17 (7) | 67.56 (7) | −1.4 |
“ | 750 (3) | 65.69 (4) | 67.08 (8) | −1.4 |
“ | 1250 (5) | 65.06 (4) | 66.36 (8) | − 1.3 |
TS QH | 78.6 (1) | 87 (6) | −.8 (7) | |
TS LS | 87.4 (1) | 90 (7) | −2.6 (8) |
The results are taken from Cheluvaraja et al., 2008. The bin sizes are δ=Δαk/l(equation (44)). nf denotes the sample size of the future chains used in the reconstruction process, nf = unit×j, where j is the number of simulations of unit size applied at each reconstruction step. Generation of the samples (of 600 conformations) and their reconstruction is based on the AMBER force field and 70 TIP3P water molecules. The statistical error in defined in Table 1; for the errors are smaller than ±0.1. SQH (equation (4)) is the quasi-harmonic entropy and SLS is obtained by the local states method using b=2 and the discretization parameter, l=10 (see Appendix). These results that were obtained from larger samples are strongly inaccurate. The entropy is defined up to an additive constant that is expected to be the same for both microstates. As anticipated, the results for decrease systematicallyas the approximation improves (i.e., as δ is decreased and nf is increased). The results for are stable converging to 1.3±0.2 kcal/mol.