TABLE 4.
PwTBP
|
ΔΔG (kcal mol−1)
|
|||
---|---|---|---|---|
ID* | ΔΔGelec† | ΔΔHvdW‡ | Calculated§ | Experimental¶ |
WT | 0.0 | 0.0 | 0.0 | 0.0 |
E12A | −4.7 | 3.7 | −1.0 | −1.0 |
E42A | −5.7 | 4.3 | −1.4 | −0.3 |
D101A | 2.6 | 0.2 | 2.8 | −0.4 |
E128A | 0.6 | −3.2 | −2.8 | −0.5 |
E12AE128A | −2.9 | 1.5 | −1.4 | −1.3 |
E12AE42A | −9.7 | 9.4 | −0.3 | −1.1 |
3 | −7.9 | 5.8 | −2.1 | −1.8 |
4 | −8.2 | −4.0 | −12.2 | −1.9 |
Wild-type and mutant PwTBPs. Labels 3 and 4 represent mutants E12AE41KE128A and E12AE41KE42KE128A, respectively.
The electrostatic energy difference between the mutant and the wild-type PwTBP, ΔΔGelec, is computed from the nonlinear solution to the Poisson-Boltzmann equation.
The vdW energy, ΔΔHvdW, is the intermolecular DNA-TBP energy difference as computed from the empirical CHARMM 22/27 all-atom force field.
ΔΔG is approximated as ΔΔGelec + ΔΔHvdW for the mutant minus the wild-type.