18 research outputs found
Substrate-Mediated Oxygen Activation by Homoprotocatechuate 2,3-Dioxygenase: Intermediates Formed by a Tyrosine 257 Variant
Homoprotocatechuate (HPCA; 3,4-dihydroxyphenylacetate
or 4-carboxymethyl
catechol) and O<sub>2</sub> bind in adjacent ligand sites of the active
site Fe<sup>II</sup> of homoprotocatechuate 2,3-dioxygenase (FeHPCD).
We have proposed that electron transfer from the chelated aromatic
substrate through the Fe<sup>II</sup> to O<sub>2</sub> gives both
substrates radical character. This would promote reaction between
the substrates to form an alkylperoxo intermediate as the first step
in aromatic ring cleavage. Several active site amino acids are thought
to promote these reactions through acid/base chemistry, hydrogen bonding,
and electrostatic interactions. Here the role of Tyr257 is explored
by using the Tyr257Phe (Y257F) variant, which decreases <i>k</i><sub>cat</sub> by about 75%. The crystal structure of the FeHPCD-HPCA
complex has shown that Tyr257 hydrogen bonds to the deprotonated C2-hydroxyl
of HPCA. Stopped-flow studies show that at least two reaction intermediates,
termed Y257F<sub>Int1</sub><sup>HPCA</sup> and Y257F<sub>Int2</sub><sup>HPCA</sup>, accumulate during the Y257F-HPCA + O<sub>2</sub> reaction prior
to formation of the ring-cleaved product. Y257F<sub>Int1</sub><sup>HPCA</sup> is colorless and is formed
as O<sub>2</sub> binds reversibly to the HPCAāenzyme complex.
Y257F<sub>Int2</sub><sup>HPCA</sup> forms spontaneously from Y257F<sub>Int1</sub><sup>HPCA</sup> and displays a chromophore at 425 nm (Īµ<sub>425</sub> = 10ā500 M<sup>ā1</sup> cm<sup>ā1</sup>). MoĢssbauer spectra of the intermediates trapped by rapid
freeze quench show that both intermediates contain Fe<sup>II</sup>. The lack of a chromophore characteristic of a quinone or semiquinone
form of HPCA, the presence of Fe<sup>II</sup>, and the low O<sub>2</sub> affinity suggest that Y257F<sub>Int1</sub><sup>HPCA</sup> is an HPCA-Fe<sup>II</sup>-O<sub>2</sub> complex with little electron delocalization onto the O<sub>2</sub>. In contrast, the intense spectrum of Y257F<sub>Int2</sub><sup>HPCA</sup> suggests the intermediate
is most likely an HPCA quinone-Fe<sup>II</sup>-(hydro)Āperoxo species.
Steady-state and transient kinetic analyses show that steps of the
catalytic cycle are slowed by as much as 100-fold by the mutation.
These effects can be rationalized by a failure of Y257F to facilitate
the observed distortion of the bound HPCA that is proposed to promote
transfer of one electron to O<sub>2</sub>
Spectroscopic and Theoretical Investigation of a Complex with an [Oī»Fe<sup>IV</sup>āOāFe<sup>IV</sup>ī»O] Core Related to Methane Monooxygenase Intermediate <b>Q</b>
Previous
efforts to model the diironĀ(IV) intermediate <b>Q</b> of soluble
methane monooxygenase have led to the synthesis of a
diironĀ(IV) TPA complex, <b>2</b>, with an O=Fe<sup>IV</sup>āOāFe<sup>IV</sup>āOH core that has two ferromagnetically coupled S<sub>loc</sub> = 1 sites. Addition of base to <b>2</b> at ā85
Ā°C elicits its conjugate base <b>6</b> with a novel Oī»Fe<sup>IV</sup>āOāFe<sup>IV</sup>ī»O core. In frozen
solution, <b>6</b> exists in two forms, <b>6a</b> and <b>6b</b>, that we have characterized extensively using MoĢssbauer
and parallel mode EPR spectroscopy. The conversion between <b>2</b> and <b>6</b> is quantitative, but the relative proportions
of <b>6a</b> and <b>6b</b> are solvent dependent. <b>6a</b> has two equivalent high-spin (<i>S</i><sub>loc</sub> = 2) sites, which are antiferromagnetically coupled; its quadrupole
splitting (0.52 mm/s) and isomer shift (0.14 mm/s) match those of
intermediate <b>Q</b>. DFT calculations suggest that <b>6a</b> assumes an anti conformation with a dihedral Oī»FeāFeī»O
angle of 180Ā°. MoĢssbauer and EPR analyses show that <b>6b</b> is a diironĀ(IV) complex with ferromagnetically coupled <i>S</i><sub>loc</sub> = 1 and <i>S</i><sub>loc</sub> = 2 sites to give total spin <i>S</i><sub>t</sub> = 3.
Analysis of the zero-field splittings and magnetic hyperfine tensors
suggests that the dihedral Oī»FeāFeī»O angle of <b>6b</b> is ā¼90Ā°. DFT calculations indicate that this
angle is enforced by hydrogen bonding to both terminal oxo groups
from a shared water molecule. The water molecule preorganizes <b>6b</b>, facilitating protonation of one oxo group to regenerate <b>2</b>, a protonation step difficult to achieve for mononuclear
Fe<sup>IV</sup>ī»O complexes. Complex <b>6</b> represents
an intriguing addition to the handful of diironĀ(IV) complexes that
have been characterized
Sc<sup>3+</sup>-Triggered Oxoiron(IV) Formation from O<sub>2</sub> and its Non-Heme Iron(II) Precursor via a Sc<sup>3+</sup>āPeroxoāFe<sup>3+</sup> Intermediate
We report that redox-inactive
Sc<sup>3+</sup> can trigger O<sub>2</sub> activation by the Fe<sup>II</sup>(TMC) center (TMC = tetramethylcyclam)
to generate the corresponding oxoironĀ(IV) complex in the presence
of BPh<sub>4</sub><sup>ā</sup> as an electron donor. To model
a possible intermediate in the above reaction, we generated an unprecedented
Sc<sup>3+</sup> adduct of [Fe<sup>III</sup>(Ī·<sup>2</sup>-O<sub>2</sub>)Ā(TMC)]<sup>+</sup> by an alternative route, which was found
to have an Fe<sup>3+</sup>ā(Ī¼-Ī·<sup>2</sup>:Ī·<sup>2</sup>-peroxo)āSc<sup>3+</sup> core and to convert to the
oxoironĀ(IV) complex. These results have important implications for
the role a Lewis acid can play in facilitating OāO bond cleavage
during the course of O<sub>2</sub> activation at non-heme iron centers
Upside Down! Crystallographic and Spectroscopic Characterization of an [Fe<sup>IV</sup>(O<sub>syn</sub>)(TMC)]<sup>2+</sup> Complex
Fe<sup>II</sup>(TMC)Ā(OTf)<sub>2</sub> reacts with 2-<sup>t</sup>BuSO<sub>2</sub>āC<sub>6</sub>H<sub>4</sub>IO to afford an oxoironĀ(IV) product, <b>2</b>, distinct
from the previously reported [Fe<sup>IV</sup>(O<sub>anti</sub>)Ā(TMC)Ā(NCMe)]<sup>2+</sup>. In MeCN, <b>2</b> has a blue-shifted near-IR band,
a higher Ī½Ā(Feī»O), a larger MoĢssbauer quadrupole
splitting, and quite a distinct <sup>1</sup>H NMR spectrum. Structural
analysis of crystals grown from CH<sub>2</sub>Cl<sub>2</sub> reveals
a complex with the formulation of [Fe<sup>IV</sup>(O<sub>syn</sub>)Ā(TMC)Ā(OTf)]Ā(OTf) and the shortest Fe<sup>IV</sup>ī»O bond
[1.625(4) Ć
] found to date
Structural, EPR, and MoĢssbauer Characterization of (Ī¼-Alkoxo)(Ī¼-Carboxylato)Diiron(II,III) Model Complexes for the Active Sites of Mixed-Valent Diiron Enzymes
To obtain structural and spectroscopic models for the
diironĀ(II,III)
centers in the active sites of diiron enzymes, the (Ī¼-alkoxo)Ā(Ī¼-carboxylato)ĀdiironĀ(II,III)
complexes [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā(O<sub>2</sub>CPh)Ā(NCCH<sub>3</sub>)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>3</sub> (<b>1</b>) and [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā(O<sub>2</sub>CPh)Ā(Cl)Ā(HOCH<sub>3</sub>)]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>2</b>) (<i>N</i>-Et-HPTB = <i>N,N,N</i>ā²<i>,N</i>ā²-tetrakisĀ(2-(1-ethyl-benzimidazolylmethyl))-2-hydroxy-1,3-diaminopropane)
have been prepared and characterized by X-ray crystallography, UVāvisible
absorption, EPR, and MoĢssbauer spectroscopies. Fe1āFe2
separations are 3.60 and 3.63 Ć
, and Fe1āO1āFe2
bond angles are 128.0Ā° and 129.4Ā° for <b>1</b> and <b>2</b>, respectively. MoĢssbauer and EPR studies of <b>1</b> show that the Fe<sup>III</sup> (<i>S</i><sub>A</sub> = 5/2) and Fe<sup>II</sup> (<i>S</i><sub>B</sub> = 2)
sites are antiferromagnetically coupled to yield a ground state with <i>S</i> = 1/2 (<i>g</i> <b>=</b> 1.75, 1.88, 1.96);
MoĢssbauer analysis of solid <b>1</b> yields <i>J</i> = 22.5 Ā± 2 cm<sup>ā1</sup> for the exchange coupling
constant (H = <i>J</i><b>S</b><sub>A</sub>Ā·<b>S</b><sub>B</sub> convention). In addition
to the <i>S</i> = 1/2 ground-state spectrum of <b>1</b>, the EPR signal for the <i>S</i> = 3/2 excited state of
the spin ladder can also be observed, the first time such a signal
has been detected for an antiferromagnetically coupled diironĀ(II,III)
complex. The anisotropy of the <sup>57</sup>Fe magnetic hyperfine
interactions at the Fe<sup>III</sup> site is larger than normally
observed in mononuclear complexes and arises from admixing <i>S</i> > 1/2 excited states into the <i>S</i> =
1/2
ground state by zero-field splittings at the two Fe sites. Analysis
of the ā<i>D</i>/<i>J</i>ā mixing
has allowed us to extract the zero-field splitting parameters, local <i>g</i> values, and magnetic hyperfine structural parameters for
the individual Fe sites. The methodology developed and followed in
this analysis is presented in detail. The spin Hamiltonian parameters
of <b>1</b> are related to the molecular structure with the
help of DFT calculations. Contrary to what was assumed in previous
studies, our analysis demonstrates that the deviations of the <i>g</i> values from the free electron value (<i>g</i> = 2) for the antiferromagnetically coupled diironĀ(II,III) core in
complex <b>1</b> are predominantly determined by the anisotropy
of the effective <i>g</i> values of the ferrous ion and
only to a lesser extent by the admixture of excited states into ground-state
ZFS terms (<i>D</i>/<i>J</i> mixing). The results
for <b>1</b> are discussed in the context of the data available
for diironĀ(II,III) clusters in proteins and synthetic diironĀ(II,III)
complexes
Structural, EPR, and MoĢssbauer Characterization of (Ī¼-Alkoxo)(Ī¼-Carboxylato)Diiron(II,III) Model Complexes for the Active Sites of Mixed-Valent Diiron Enzymes
To obtain structural and spectroscopic models for the
diironĀ(II,III)
centers in the active sites of diiron enzymes, the (Ī¼-alkoxo)Ā(Ī¼-carboxylato)ĀdiironĀ(II,III)
complexes [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā(O<sub>2</sub>CPh)Ā(NCCH<sub>3</sub>)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>3</sub> (<b>1</b>) and [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā(O<sub>2</sub>CPh)Ā(Cl)Ā(HOCH<sub>3</sub>)]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>2</b>) (<i>N</i>-Et-HPTB = <i>N,N,N</i>ā²<i>,N</i>ā²-tetrakisĀ(2-(1-ethyl-benzimidazolylmethyl))-2-hydroxy-1,3-diaminopropane)
have been prepared and characterized by X-ray crystallography, UVāvisible
absorption, EPR, and MoĢssbauer spectroscopies. Fe1āFe2
separations are 3.60 and 3.63 Ć
, and Fe1āO1āFe2
bond angles are 128.0Ā° and 129.4Ā° for <b>1</b> and <b>2</b>, respectively. MoĢssbauer and EPR studies of <b>1</b> show that the Fe<sup>III</sup> (<i>S</i><sub>A</sub> = 5/2) and Fe<sup>II</sup> (<i>S</i><sub>B</sub> = 2)
sites are antiferromagnetically coupled to yield a ground state with <i>S</i> = 1/2 (<i>g</i> <b>=</b> 1.75, 1.88, 1.96);
MoĢssbauer analysis of solid <b>1</b> yields <i>J</i> = 22.5 Ā± 2 cm<sup>ā1</sup> for the exchange coupling
constant (H = <i>J</i><b>S</b><sub>A</sub>Ā·<b>S</b><sub>B</sub> convention). In addition
to the <i>S</i> = 1/2 ground-state spectrum of <b>1</b>, the EPR signal for the <i>S</i> = 3/2 excited state of
the spin ladder can also be observed, the first time such a signal
has been detected for an antiferromagnetically coupled diironĀ(II,III)
complex. The anisotropy of the <sup>57</sup>Fe magnetic hyperfine
interactions at the Fe<sup>III</sup> site is larger than normally
observed in mononuclear complexes and arises from admixing <i>S</i> > 1/2 excited states into the <i>S</i> =
1/2
ground state by zero-field splittings at the two Fe sites. Analysis
of the ā<i>D</i>/<i>J</i>ā mixing
has allowed us to extract the zero-field splitting parameters, local <i>g</i> values, and magnetic hyperfine structural parameters for
the individual Fe sites. The methodology developed and followed in
this analysis is presented in detail. The spin Hamiltonian parameters
of <b>1</b> are related to the molecular structure with the
help of DFT calculations. Contrary to what was assumed in previous
studies, our analysis demonstrates that the deviations of the <i>g</i> values from the free electron value (<i>g</i> = 2) for the antiferromagnetically coupled diironĀ(II,III) core in
complex <b>1</b> are predominantly determined by the anisotropy
of the effective <i>g</i> values of the ferrous ion and
only to a lesser extent by the admixture of excited states into ground-state
ZFS terms (<i>D</i>/<i>J</i> mixing). The results
for <b>1</b> are discussed in the context of the data available
for diironĀ(II,III) clusters in proteins and synthetic diironĀ(II,III)
complexes
Enzyme Substrate Complex of the H200C Variant of Homoprotocatechuate 2,3-Dioxygenase: MoĢssbauer and Computational Studies
The
extradiol, aromatic ring-cleaving enzyme homoprotocatechuate 2,3-dioxygenase
(HPCD) catalyzes a complex chain of reactions that involve second
sphere residues of the active site. The importance of the second-sphere
residue His200 was demonstrated in studies of HPCD variants, such
as His200Cys (H200C), which revealed significant retardations of certain
steps in the catalytic process as a result of the substitution, allowing
novel reaction cycle intermediates to be trapped for spectroscopic
characterization. As the H200C variant largely retains the wild-type
active site structure and produces the correct ring-cleaved product,
this variant presents a valuable target for mechanistic HPCD studies.
Here, the high-spin Fe<sup>II</sup> states of resting H200C and the
H200Cāhomoprotocatechuate enzymeāsubstrate (ES) complex
have been characterized with MoĢssbauer spectroscopy to assess
the electronic structures of the active site in these states. The
analysis reveals a high-spin Fe<sup>II</sup> center in a low symmetry
environment that is reflected in the values of the zero-field splitting
(ZFS) (<i>D</i> ā ā 8 cm<sup>ā1</sup>, <i>E</i>/<i>D</i> ā 1/3 in ES), as well
as the relative orientations of the principal axes of the <sup>57</sup>Fe magnetic hyperfine (<b>A</b>) and electric field gradient
(EFG) tensors relative to the ZFS tensor axes. A spin Hamiltonian
analysis of the spectra for the ES complex indicates that the magnetization
axis of the integer-spin <i>S</i> = 2 Fe<sup>II</sup> system
is nearly parallel to the symmetry axis, <i>z</i>, of the
doubly occupied d<sub><i>xy</i></sub> ground orbital deduced
from the EFG and <b>A</b>-values, an observation, which cannot
be rationalized by DFT assisted crystal-field theory. In contrast,
ORCA/CASSCF calculations for the ZFS tensor in combination with DFT
calculations for the EFG- and <b>A</b>-tensors describe the
experimental data remarkably well
Spectroscopic and Theoretical Study of Spin-Dependent Electron Transfer in an Iron(III) Superoxo Complex
It was shown previously
(<i>J. Am. Chem. Soc.</i> <b>2014</b>, <i>136</i>, 10846) that bubbling of O<sub>2</sub> into a solution of Fe<sup>II</sup>(BDPP) (H<sub>2</sub>BDPP = 2,6-bisĀ[[(<i>S</i>)-2-(diphenylhydroxymethyl)-1-pyrrolidinyl]Āmethyl]Āpyridine)
in tetrahydrofuran at ā80 Ā°C generates a high-spin (<i>S</i><sub>Fe</sub> = <sup>5</sup>/<sub>2</sub>) ironĀ(III) superoxo
adduct, <b>1</b>. MoĢssbauer studies revealed that <b>1</b> is an exchange-coupled system, HĢex=JSĢFeĀ·SĢR, where <i>S</i><sub>R</sub> = <sup>1</sup>/<sub>2</sub> is the spin of the superoxo radical, of which the spectra were not
well enough resolved to determine whether the coupling was ferromagnetic
(<i>S</i> = 3 ground state) or antiferromagnetic (<i>S</i> = 2). The glass-forming 2-methyltetrahydrofuran solvent
yields highly resolved MoĢssbauer spectra from which the following
data have been extracted: (i) the ground state of <b>1</b> has <i>S</i> = 3 (<i>J</i> < 0); (ii) |<i>J</i>| > 15 cm<sup>ā1</sup>; (iii) the zero-field-splitting
parameters are <i>D</i> = ā1.1 cm<sup>ā1</sup> and <i>E</i>/<i>D</i> = 0.02; (iv) the major
component of the electric-field-gradient tensor is tilted ā7Ā°
relative to the easy axis of magnetization determined by the <i>M</i><sub><i>S</i></sub> = Ā±3 and Ā±2 doublets.
The excited-state <i>M</i><sub><i>S</i></sub> =
Ā±2 doublet yields a narrow parallel-mode electron paramagnetic
resonance signal at <i>g</i> = 8.03, which was used to probe
the magnetic hyperfine splitting of <sup>17</sup>O-enriched O<sub>2</sub>. A theoretical model that considers spin-dependent electron
transfer for the cases where the doubly occupied Ļ* orbital
of the superoxo ligand is either āinā or āoutā
of the plane defined by the bent FeāOO moiety correctly predicts
that <b>1</b> has an <i>S</i> = 3 ground state, in
contrast to the density functional theory calculations for <b>1</b>, which give a ground state with both the wrong spin and orbital
configuration. This failure has been traced to a basis set superposition
error in the interactions between the superoxo moiety and the adjacent
five-membered rings of the BDPP ligand and signals a fundamental problem
in the quantum chemistry of O<sub>2</sub> activation
A Long-Lived Fe<sup>III</sup>-(Hydroperoxo) Intermediate in the Active H200C Variant of Homoprotocatechuate 2,3-Dioxygenase: Characterization by MoĢssbauer, Electron Paramagnetic Resonance, and Density Functional Theory Methods
The extradiol-cleaving dioxygenase
homoprotocatechuate 2,3-dioxygenase (HPCD) binds substrate homoprotocatechuate
(HPCA) and O<sub>2</sub> sequentially in adjacent ligand sites of
the active site Fe<sup>II</sup>. Kinetic and spectroscopic studies
of HPCD have elucidated catalytic roles of several active site residues,
including the crucial acidābase chemistry of His200. In the
present study, reaction of the His200Cys (H200C) variant with native
substrate HPCA resulted in a decrease in both <i>k</i><sub>cat</sub> and the rate constants for the activation steps following
O<sub>2</sub> binding by >400 fold. The reaction proceeds to form
the correct extradiol product. This slow reaction allowed a long-lived
(<i>t</i><sub>1/2</sub> = 1.5 min) intermediate, H200C-HPCA<sub>Int1</sub> (<i>Int1</i>), to be trapped. MoĢssbauer
and parallel mode electron paramagnetic resonance (EPR) studies show
that <i>Int1</i> contains an <i>S</i><sub>1</sub> = 5/2 Fe<sup>III</sup> center coupled to an <i>S</i><sub>R</sub> = 1/2 radical to give a ground state with total spin <i>S</i> = 2 (<i>J</i> > 40 cm<sup>ā1</sup>) in Hexch=JSĢ1Ā·SĢR. Density functional theory (DFT) property calculations for structural
models suggest that <i>Int1</i> is a (HPCA semiquinone<sup>ā¢</sup>)ĀFe<sup>III</sup>(OOH) complex, in which OOH
is protonated at the distal O and the substrate hydroxyls are deprotonated.
By combining MoĢssbauer and EPR data of <i>Int1</i> with DFT calculations, the orientations of the principal axes of
the <sup>57</sup>Fe electric field gradient and the zero-field splitting
tensors (<i>D</i> = 1.6 cm<sup>ā1</sup>, <i>E</i>/<i>D</i> = 0.05) were determined. This information
was used to predict hyperfine splittings from bound <sup>17</sup>OOH.
DFT reactivity analysis suggests that <i>Int1</i> can evolve
from a ferromagnetically coupled Fe<sup>III</sup>-superoxo precursor
by an inner-sphere proton-coupled-electron-transfer process. Our spectroscopic
and DFT results suggest that a ferric hydroperoxo species is capable
of extradiol catalysis
Spectroscopic Identification of an Fe<sup>III</sup> Center, not Fe<sup>IV</sup>, in the Crystalline ScāOāFe Adduct Derived from [Fe<sup>IV</sup>(O)(TMC)]<sup>2+</sup>
The
apparent Sc<sup>3+</sup> adduct of [Fe<sup>IV</sup>(O)Ā(TMC)]<sup>2+</sup> (<b>1</b>, TMC = 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane)
has been synthesized in amounts sufficient to allow its characterization
by various spectroscopic techniques. Contrary to the earlier assignment
of a +4 oxidation state for the iron center of <b>1</b>, we
establish that <b>1</b> has a high-spin ironĀ(III) center based
on its MoĢssbauer and EPR spectra and its quantitative reduction
by 1 equiv of ferrocene to [Fe<sup>II</sup>(TMC)]<sup>2+</sup>. Thus, <b>1</b> is best described as a Sc<sup>III</sup>āOāFe<sup>III</sup> complex, in agreement with previous DFT calculations (Swart, M. Chem. Commun. 2013, 49, 6650.). These results shed light on the interaction of Lewis acids with
high-valent metal-oxo species