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. 2022 Jun 22;144(24):10752-10767.
doi: 10.1021/jacs.2c01375. Epub 2022 May 10.

What Drives Radical Halogenation versus Hydroxylation in Mononuclear Nonheme Iron Complexes? A Combined Experimental and Computational Study

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What Drives Radical Halogenation versus Hydroxylation in Mononuclear Nonheme Iron Complexes? A Combined Experimental and Computational Study

Emilie F Gérard et al. J Am Chem Soc. .

Abstract

Nonheme iron halogenases are unique enzymes in nature that selectively activate an aliphatic C-H bond of a substrate to convert it into C-X (X = Cl/Br, but not F/I). It is proposed that they generate an FeIII(OH)(X) intermediate in their catalytic cycle. The analogous FeIII(OH) intermediate in nonheme iron hydroxylases transfers OH to give alcohol product, whereas the halogenases transfer X to the carbon radical substrate. There remains significant debate regarding what factors control their remarkable selectivity of the halogenases. The reactivity of the complexes FeIII(BNPAPh2O)(OH)(X) (X = Cl, Br) with a secondary carbon radical (R) is described. It is found that X transfer occurs with a secondary carbon radical, as opposed to OH transfer with tertiary radicals. Comprehensive computational studies involving density functional theory were carried out to examine the possible origins of this selectivity. The calculations reproduce the experimental findings, which indicate that halogen transfer is not observed for the tertiary radicals because of a nonproductive equilibrium that results from the endergonic nature of these reactions, despite a potentially lower reaction barrier for the halogenation pathway. In contrast, halogen transfer is favored for secondary carbon radicals, for which the halogenated product complex is thermodynamically more stable than the reactant complex. These results are rationalized by considering the relative strengths of the C-X bonds that are formed for tertiary versus secondary carbon centers. The computational analysis also shows that the reaction barrier for halogen transfer is significantly dependent on secondary coordination sphere effects, including steric and H-bonding interactions.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Scheme 1
Scheme 1. General Reaction Catalyzed by Nonheme Iron Halogenases, with αKG = α-Ketoglutarate and R–H as the Substrate
Scheme 2
Scheme 2. Iron Complexes, Carbon Radicals, and Reactions Studied in This Work
Figure 1
Figure 1
Top: 1H NMR spectra obtained in CDCl3 of isolated C6H5CH(Cl)CH3 from the reaction of 1Cl with C6H5CH(CH3)N=N(CH3)CHC6H5 (a), from the reaction of 2Cl with C6H5CH(CH3)N=N(CH3)CHC6H5 (b), and authentic C6H5CH(Cl)CH3 (c). Residual solvent signals are marked with a red asterisk (*). Bottom: Reactivity of 1Cl with tertiary and secondary carbon radicals.
Scheme 3
Scheme 3. Reactions of 1OTf with Tertiary and Secondary Carbon Radicals
Figure 2
Figure 2
UB3LYP/BS1-optimized geometries of the isolated reactants 61Cl/61Br as obtained in Gaussian with bond lengths given in Å. Relevant molecular valence orbitals are shown on the right.
Figure 3
Figure 3
Potential energy landscape for halogen versus hydroxyl transfer in complexes 1Cl/1Br/1F as obtained at UB3LYP/BS2//UB3LYP/BS1 level of theory with the solvent and zero-point corrections included. Energies relative to the reactant complexes are in kcal mol–1, while transition-state structures give bond lengths in Å, angles in degrees, and the imaginary frequency in cm–1.
Scheme 4
Scheme 4. Halogenated and Hydroxylated Product Complexes Showing Feasible Reverse Reactions for Br Transfer and Not for OH Transfer
Figure 4
Figure 4
Optimized geometries of TSCl2,2Cl and TSCl3,2Cl as obtained in Gaussian. Energies (ΔE + ZPE) are relative to the reactant complexes in kcal mol–1, while transition-state structures give bond lengths in Å, angles in degrees, and the imaginary frequency in cm–1.
Scheme 5
Scheme 5. Reactions of 2Cl with Tertiary and Secondary Carbon Radicals
Figure 5
Figure 5
Potential energy landscape for halogen versus hydroxyl transfer after isomerization of complex 1Cl into 2OH as obtained at UB3LYP/BS2//UB3LYP/BS1 level of theory with the solvent and zero-point corrections included. Energies are in kcal mol–1, while structures give bond lengths in Å, angles in degrees, and the imaginary frequency in cm–1. The constraint geometry scan for isomerization from 1Cl to 2OH is shown in the inset.
Figure 6
Figure 6
OH and Cl rebound barriers from 5Re1Cl and truncated models with steric or hydrogen-bonding interactions (or both) removed. Energies obtained at UB3LYP/BS2//UB3LYP/BS1 with zero-point and solvent corrections included. Data in kcal mol–1 with respect to the reactant complexes. Also shown are overlays of the Cl transfer and OH transfer transition states with the following color coding: full system (khaki), without sterics (pink), without H-bond (cyan), and without sterics/H-bond (light green).
Figure 7
Figure 7
Potential energy landscape for halogen versus hydroxyl transfer from complexes Re1Cl/Re1Br to the secondary radicals (C6H5)2CH (PP) and (C6H5)(CH3)CH (PM) as calculated at UB3LYP/BS2//UB3LYP/BS1 level of theory with the solvent and zero-point corrections included. Energies are in kcal mol–1. Values in parentheses are for the reaction from Re1Br.
Figure 8
Figure 8
Valence bond diagram for the prediction of OH and Cl-transfer barriers in 5Re1Cl. Dots are electrons and a bar between two dots is a chemical bond occupied with two electrons.

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