H. Basch et al., A density functional study of the completion of the methane monooxygenase catalytic cycle. Methanol complex to MMOH resting state, J PHYS CH B, 105(35), 2001, pp. 8452-8460
In the final stage of the hydroxylation of methane to methanol by the metha
ne monooxygenase (MMO) enzyme, a binuclear iron-methanol complex (II), expe
ls the methanol and restores the resting state (RS) Fe-II-Fe-II form of the
hydroxylate (MMOH) component to complete the catalytic cycle. The overall
process, II --> RS, can include protonation, addition of water, expulsion o
f methanol, and ligand rearrangement, all in an unknown order of occurrence
. A model previously applied successfully to describe the hydroxylation mec
hanism that produces II is used here with the density functional theory to
examine a series of intermediate structures and reaction steps to find the
lowest-energy reaction path for II --> RS. Two different groups of structur
es and reaction steps are considered; those involving proton transfer from
the protein/environment to the complexes (group A) and those that are charg
e neutral with consideration of internal hydrogen atom migration among the
oxygen ligands of the diferric complexes (group B). The lowest-energy paths
for group A were found to be paths II - CH3OH --> III + H+ --> VII + H2O -
-> IX, II - CH3OH --> III + H2O --> V + H+ --> IX, and II + H+ --> VI - CH3
OH --> VII + H2O --> IX, with overall reaction energies of -19.9 ((9)A) and
-35.0 ((11)A) kcal/mol. The methanol dissociation step gives; a small ther
modynamic barrier to all these mechanisms. In group B, the preferred reacti
on path is II + H2O --> IV --> X {or XI} - CH3OH --> XII, as well as II - C
H3OH --> III + H2O --> V --> XII, with reaction energies of -15.7 ((9)A) an
d -18.8 ((11)A) kcal/mol. The IX and XIII structures have similar geometrie
s and can be identified with the RS of MMOH, depending on its actual charge
. The (11)A structures are consistently more stable than their (9)A counter
parts, as expected for Fe-III-Fe-III complexes, and the II --> RS process w
ill proceed entirely on the (11)A energy surface.