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. Author manuscript; available in PMC: 2011 Mar 1.
Published in final edited form as: J Mol Recognit. 2010 Mar-Apr;23(2):153–172. doi: 10.1002/jmr.973

Table 5.

HSMD results (in kcal/mol) for the entropy, TSloopA (equation (46)) and TΔSloopA at T=300 K for the free and bound microstates of the loop of α-amylase in explicit watera

Free loop Bound loop
Bin size nf (j) TSloopA TSloopA TΔSloopA
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)
a

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 TΔSloopA the errors are smaller than ±0.1. SQH (equation (4)) is the quasi-harmonic entropy and SLS is ΔSloopA 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 TSloopA is defined up to an additive constant that is expected to be the same for both microstates. As anticipated, the results for TSloopA decrease systematicallyas the approximation improves (i.e., as δ is decreased and nf is increased). The results for TΔSloopA are stable converging to 1.3±0.2 kcal/mol.