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. 2007 Dec 4;104(49):19181-6.
doi: 10.1073/pnas.0709471104. Epub 2007 Nov 28.

Axial ligand tuning of a nonheme iron(IV)-oxo unit for hydrogen atom abstraction

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Axial ligand tuning of a nonheme iron(IV)-oxo unit for hydrogen atom abstraction

Chivukula V Sastri et al. Proc Natl Acad Sci U S A. .

Abstract

The reactivities of mononuclear nonheme iron(IV)-oxo complexes bearing different axial ligands, [Fe(IV)(O)(TMC)(X)](n+) [where TMC is 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane and X is NCCH(3) (1-NCCH(3)), CF(3)COO(-) (1-OOCCF(3)), or N(3)(-) (1-N(3))], and [Fe(IV)(O)(TMCS)](+) (1'-SR) (where TMCS is 1-mercaptoethyl-4,8,11-trimethyl-1,4,8,11-tetraazacyclotetradecane), have been investigated with respect to oxo-transfer to PPh(3) and hydrogen atom abstraction from phenol O H and alkylaromatic C H bonds. These reactivities were significantly affected by the identity of the axial ligands, but the reactivity trends differed markedly. In the oxidation of PPh(3), the reactivity order of 1-NCCH(3) > 1-OOCCF(3) > 1-N(3) > 1'-SR was observed, reflecting a decrease in the electrophilicity of iron(IV)-oxo unit upon replacement of CH(3)CN with an anionic axial ligand. Surprisingly, the reactivity order was inverted in the oxidation of alkylaromatic C H and phenol O H bonds, i.e., 1'-SR > 1-N(3) > 1-OOCCF(3) > 1-NCCH(3). Furthermore, a good correlation was observed between the reactivities of iron(IV)-oxo species in H atom abstraction reactions and their reduction potentials, E(p,c), with the most reactive 1'-SR complex exhibiting the lowest potential. In other words, the more electron-donating the axial ligand is, the more reactive the iron(IV)-oxo species becomes in H atom abstraction. Quantum mechanical calculations show that a two-state reactivity model applies to this series of complexes, in which a triplet ground state and a nearby quintet excited-state both contribute to the reactivity of the complexes. The inverted reactivity order in H atom abstraction can be rationalized by a decreased triplet-quintet gap with the more electron-donating axial ligand, which increases the contribution of the much more reactive quintet state and enhances the overall reactivity.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Fig. 1.
Fig. 1.
Schematic structures of [FeIV(O)(TMC)(X)]n+ (1-X) and [FeIV(O)(TMCS)]+ (1′-SR).
Fig. 2.
Fig. 2.
Second-order rate constants determined in the reactions of [FeIV(O)(TMC)(X)]n+ (0.5 mM) at 0°C with PPh3 (a), 2,4-t-Bu2C6H3OH (b), and DHA (c). Blue diamonds indicate 1′-SR; black squares indicate 1-N3; green circles indicate 1-OOCCF3; and red inverted triangles indicate 1-NCCH3.
Scheme 1.
Scheme 1.
Scheme 2.
Scheme 2.
Fig. 3.
Fig. 3.
Correlations of reaction rates with BDE. (a) Plot of log krel of [FeIV(O)(TMC)(N3)]+ (1-N3) against Oformula imageH BDE of p-Y-2,6-t- Bu2C6H3OH in CH3CN at 25°C. (b) Plot of log k′2 of [FeIV(O)(TMC)(N3)]+ (1-N3) against Cformula imageH BDE of substrates. Second-order rate constants, k2, were determined at 25°C and then adjusted for reaction stoichiometry to yield k′2 based on the number of equivalent target Cformula imageH bonds of substrates (e.g., four for DHA and CHD and two for xanthene and fluorene).
Fig. 4.
Fig. 4.
Electrochemical comparisons. (a) Cyclic and differential pulse voltamograms of [FeIV(O)(TMC)(NCCH3)]2+ (1-NCCH3) in CH3CN at 25°C (Left) and [FeIV(O)(TMCS)]+ (1′-SR) in 1:1 CH3OH/CH3CN at −30°C (Right). (b) Plot of log k2 determined in the oxidation of DHA at 0°C against Ep,c values of [FeIV(O)(TMC)(X)]n+ complexes and [FeIV(O)(TMCS)]+ in 1:1 CH3CN/CH3OH measured at −30°C.
Fig. 5.
Fig. 5.
Key geometric features of 1-NCCH3, 1-OOCCF3, 1-N3, and 1′-SR optimized at the B3LYP/LACVP level (bond lengths in angstroms) in the triplet (quintet) states, along with the amounts of charge shifted from ligand to the (TMC)FeO moiety (ΔqCT) and the quintet–triplet energy gap (ΔEQ-T, in kcal/mol).
Fig. 6.
Fig. 6.
Plots of log k2 values for the reactions of 1-X and 1′-SR with DHA (red open circles), 2,4-t-Bu2C6H3OH (green filled triangles), and PPh3 (black filled squares) against the computed quintet-triplet energy gaps (ΔEQ-T) for 1-X and 1′-SR.

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