Angewandte
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=
(EFC,R) and the driving force for the reaction (DErp),
C O p-bond move to the carbonyl oxygen atom. The
Equation (1), as defined in Figure 3.
resonance energy for the nucleophilic pathway is one-half of
ꢀ
ꢀ
the sum of the C O and Mn O bonds that are formed, while
a value of EPPA,p=184.7 kcalmolꢀ1 was estimated. Based on
first principles, we estimate the nucleophilic barrier to be
DE°VB,NA = 44.9 kcalmolꢀ1.
3
DEcross ¼ 1= EFC,R þ = DErp
ð1Þ
4
4
As shown previously using valence-bond curve-crossing
diagrams,[17] the actual transition state is below the curve
crossing energy by an amount B (the resonance energy), so
that we can predict the value of the transition state based on
estimates for EFC,R, DErp, and B with Equation (2).
The VB modeling, therefore, predicts that the side-on
manganese–peroxo will react with 2-PPA through preferen-
tial a-hydrogen-atom abstraction rather than via nucleophilic
addition. This is possible thanks to its small redox potential
that enables efficient electron transfer from peroxo to
manganese, which is a lower energy pathway than transferring
DE°
¼ DEcrossꢀB
ð2Þ
VB,HAT
an electron from peroxo to substrate carbonyl. Furthermore,
ꢀ1
We then analyzed the bond breaking and orbital changes
between reactants, transition states and intermediates for the
rate determining reaction step to predict the Franck–Condon
energy between R and R* and give details in Figure 3 in
a valence bond format. These VB schemes were used
previously to predict reactivities and rationalize reactivity
trends.[18,19] Thus, the hydrogen-atom abstraction is accom-
plished through the breaking of the sCH bond of the substrate
leading to atomic 2pC and 1sH orbitals, which energetically is
ꢀ
the C H bond strength of the substrate is only 80.3 kcalmol
and despite the fact that the side-on peroxo will give a weaker
ꢀ
ꢀ
O H bond, actually a strong Mn O three-electron bond is
formed, which gives the reaction to large driving force. By
5
5
ꢀ
contrast, the nucleophilic pathway gains a rather weak C O
bond probably due to stereochemical repulsions of the ligand
substituents interfering with the bond formation, so that this
process overall will cost more energy. Therefore, the side-on
manganese–peroxo with bispidine ligand system will prefer-
entially react via hydrogen-atom abstraction rather than
nucleophilic addition with aldehydes through its availability
of low-energy metal 3d orbitals that can pick up an electron
from the peroxo group. Further research will need to be done
on synthetic and enzymatic manganese and iron–peroxo
complexes, such as the aldehyde deformylating dioxyge-
nases,[20] to find out whether this is a general mechanism.
ꢀ
equal to the bond dissociation energy of the C H bond
2
(BDECH). On the oxidant side of the reaction the pOO,xy
2
p*OO,xy pair of orbitals revert back to atomic orbitals and
will cost an energy EO=O. This will generate two doubly
occupied 2p atomic orbitals, one on each oxygen atom. One of
those 2p electrons on the terminal oxygen atom will form
a bond with the incoming hydrogen atom, while the other
electron is transferred to the 3dyz orbital on Mn. Finally, the
other 2p orbital on oxygen atom O1 will form a three-electron
bond with the 3dxz orbital on manganese and form the pMnO,xz
and p*MnO,xz pair of orbitals. The Franck–Condon energy,
Acknowledgements
therefore, can be described as the sum of BDECH, EO O, and
=
Research support was provided by the Department of Science
and Technology (SERB), India (EMR/2014/000279) to C.V.S.
The National Service of Computational Chemistry Software
(NSCCS) is acknowledged for CPU time to S.d.V. A.S.F.
thanks the Tertiary Education Trust Fund Nigeria for
a studentship. D.K. is the Ramanujan Fellow of the Depart-
ment of Science and Technology, New Delhi (India).
EET. We calculate a BDECH value for the a-position of 2-PPA
of 80.3 kcalmolꢀ1, while the energy difference between the
pOO,xy and p*OO,xy was found to be 129.1 kcalmolꢀ1 in the side-
on manganese(III)–peroxo complex. Finally, the excitation
energy from p*OO,xy to 3dyz was estimated to be 96.6 kcal
molꢀ1. The resonance energy, as before,[17] was taken as one
half of the weakest bonds that are either broken or formed,
ꢀ
ꢀ
which in this case is the sum of the O H and Mn O bond. As
such, we estimate a hydrogen-atom abstraction barrier of
24.5 kcalmolꢀ1, which is in excellent agreement with the DFT
barrier reported above.
Keywords: biomimetic models · density functional theory ·
enzyme models · hydrogen-atom abstraction ·
reaction mechanisms
Subsequently, we investigated the bond breaking and
electron rearrangements for the nucleophilic addition reac-
tion of which we show the VB representation of the product
configuration in Figure 3. The reaction is initiated with the
breaking of the carbonyl p-bond (EPPA,p) as well as the
[1] a) Biomimetic Oxidations Catalyzed by Transition Metal Com-
plexes (Ed.: B. Meunier), Imperial College Press, London, 2000;
b) Cytochrome P450: Structure, Mechanism, and Biochemistry,
3rd ed. (Ed.: P. R. Ortiz de Montellano), Kluwer Academic/
Plenum Publishers, New York, 2005.
2
2
splitting of the pOO,xy p*OO,xy pair of orbitals on the peroxo
group into atomic orbitals, that is, EO O. Similarly to the
=
[2] a) D. J. Vinyard, G. M. Ananyev, G. C. Dismukes, Annu. Rev.
470; b) B. R. Streit, B. Blanc, G. S. Lukat-Rodgers, K. R. Lukat-
hydrogen-atom abstraction process the 2pO1 pair of electrons
form a three-electron bond with the 3dxz(Mn) electron.
ꢀ
Finally, a C O bond is formed between peroxo and carbonyl.
However, in contrast to the hydrogen-atom abstraction
process no electron transfer from peroxo to manganese
takes place. Instead, two electrons from the peroxo are
ꢀ
donated into the C O bond and the two electrons from the
4
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 1 – 6
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