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. 2018 Oct 19;10(2):576-586.
doi: 10.1039/c8sc03980a. eCollection 2019 Jan 14.

Mechanism of hydrogen peroxide formation by lytic polysaccharide monooxygenase

Affiliations

Mechanism of hydrogen peroxide formation by lytic polysaccharide monooxygenase

Octav Caldararu et al. Chem Sci. .

Abstract

Lytic polysaccharide monooxygenases (LPMOs) are copper-containing metalloenzymes that can cleave the glycosidic link in polysaccharides. This could become crucial for production of energy-efficient biofuels from recalcitrant polysaccharides. Although LPMOs are considered oxygenases, recent investigations have shown that H2O2 can also act as a co-substrate for LPMOs. Intriguingly, LPMOs generate H2O2 in the absence of a polysaccharide substrate. Here, we elucidate a new mechanism for H2O2 generation starting from an AA10-LPMO crystal structure with an oxygen species bound, using QM/MM calculations. The reduction level and protonation state of this oxygen-bound intermediate has been unclear. However, this information is crucial to the mechanism. We therefore investigate the oxygen-bound intermediate with quantum refinement (crystallographic refinement enhanced with QM calculations), against both X-ray and neutron data. Quantum refinement calculations suggest a Cu(ii)-O-2 system in the active site of the AA10-LPMO and a neutral protonated -NH2 state for the terminal nitrogen atom, the latter in contrast to the original interpretation. Our QM/MM calculations show that H2O2 generation is possible only from a Cu(i) center and that the most favourable reaction pathway is to involve a nearby glutamate residue, adding two electrons and two protons to the Cu(ii)-O-2 system, followed by dissociation of H2O2.

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Figures

Fig. 1
Fig. 1. The active site of AA10-LPMOs with the histidine brace and the nearby Phe164 residue, numbering according to PDB 5VG0. The figure also shows to the employed quantum system in the quantum-refinement calculations. (A) and (B) refer to chain A and B, respectively.
Fig. 2
Fig. 2. Structure and nuclear density maps of the active site after joint refinement. The m2FoDFc maps are contoured at 1.0σ and the mFoDFc maps are contoured at +3.0σ (green) and –3.0σ (red). (A) – subunit A, ND2; (B) – subunit B, ND2; (C) – subunit A, ND, (D) – subunit B, ND. RSZD– values for the N-terminal atom are given for the ND2 states to highlight if there are any extra atoms in the model. RSZD+ values for the N-terminal atom are given for the ND states to highlight if there are any missing atoms in the model.
Fig. 3
Fig. 3. Structure and nuclear density maps of the active site after quantum refinement. m2FoDFc maps are contoured at 1.0σ and mFoDFc maps are contoured at +3.0σ (green) and –3.0σ (red) (A) – subunit A, ND2; (B) – subunit B, ND2; (C) – subunit A, ND, (D) – subunit B, ND.
Fig. 4
Fig. 4. Active sites of the original crystal structure (entry 5VG0) (blue), calculated/quantum-refined structures with peroxide oxygen species (red) or superoxide oxygen species (green). (A) – QM/MM structure, subunit A; (B) – QM/MM structure, subunit B; (C) – quantum-refined structure, subunit A; (D) – quantum-refined structure, subunit B.
Fig. 5
Fig. 5. Protonation of the superoxide moiety. (A) – reactant, proton on Glu-201 (triplet); (B) – product with the superoxide protonated (open-shell singlet).
Fig. 6
Fig. 6. Second protonation of the superoxide moiety starting from (A) – Cu(ii)–HO2 or (B) – Cu(i)–O2H. Relative energies of the reactants, products and transition state (for Cu(ii)–O2H) are depicted above each structure.
Fig. 7
Fig. 7. Release of the dioxygen moiety after reduction of the copper center to Cu(i). (A) – optimised Cu(i)–HO2 system; (B) – optimised Cu(i)–H2O2 system.

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