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. 2014 Aug 28;118(37):10874–10881. doi: 10.1021/jp505727w

Table 4. Conformational Free Energies from MMPB/SA Analysis for the Drew-Dickerson Dodecamera.

  Ab Bc canonical Ad (B – A) (B – Can.A)
E(gas)⟩e 2742.6 (5.8) 2812.8 (7.3) 2944.2 (5.3) 70.2 –131.4
⟨E(nonpolar)⟩f 26.9 (0.0) 26.7 (0.0) 26.2 (0.0) –0.2 0.5
⟨E(PB), ε = 80⟩g –5818.1 (3.9) –5931.7 (6.1) –6090.8 (4.6) –113.6 159.1
⟨E(total), ε = 80⟩ –3048.6 (5.5) –3092.3 (3.5) –3120.4 (2.0) –43.7 28.1
⟨ΔE(total), salt: 0.1 M⟩ –40.5 (0.0) –41.1 (0.1) –43.1 (0.0) –0.6 2.0
⟨ΔE(total), salt: 1.0 M⟩ –53.1 (0.1) –54.2 (0.1) –59.1 (0.1) –1.1 4.9
⟨ΔE(total), ε = 20⟩ 239.2(0.2) 245.0 (0.3) 260.4 (0.3) 5.8 –15.4
a

Standard errors are given in the parentheses.

b

100 snapshots selected from DD1 and DD1 clusters as in Table 3.

c

100 snapshots selected from DD3 cluster as in Table 3.

d

Snapshots from 1 ns restrained implicit solvent simulation of canonical A-DNA structure taken at 5 ps intervals starting from 0.5 ns.

e

CHARMM force field energy in vacuum.

f

Solvent-accessible surface area term: γ*SASA+β with γ = 0.00542 kcal/mol/Å2 and β = 0.92 kcal/mol.63,64

g

Solution of Poisson–Boltzmann equation using PBEQ module65 in CHARMM program with a grid spacing of 0.25 Å.