Table V.
Calculation of the free energy cost of moving a protonated water from solvent water to the highest point (barrier) in the proton translocation pathway (D channel) of the D132N mutant of CcO (a).
| ΔGnp→crg | ΔΔGw→p |
|
ΔG#=12.0+ ΔΔGw→p | ||
|---|---|---|---|---|---|
| In water (ΔGw) | −92.9 | --- | |||
| In protein (ΔGp) (procedure A) | −68.9 | 24.0 | 36.0 | ||
| In protein (ΔGp) (procedure B) | −86.7 | 6.2 | 2.3 | 20.5 |
Energy values are reported in kcal/mol. A weak constraint of 0.3 kcal/mol was used to keep the LRA/MC generated water molecules in place. The results reported were obtained from microscopic FEP calculations using two different procedures. Procedure A corresponds to using standard solvation approach while including water molecules resolved by X-ray, whereas Procedure B corresponds to using our water flooding LRA/MC screening approach. All of these molecular dynamics simulations are performed using the polarizable ENZYMIX force field [36].