The Journal of Organic Chemistry
Article
transition states, we also employed the “Opt” keyword, but
additionally set the “Ts”, “Noeigentest”, and “Calcfc” options; see
the manual for GAUSSIAN 09 for the details of these descriptions.
(3) Koulouri, S.; Malamidou-Xenikaki, E.; Spyroudis, S. Tetrahedron
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1
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The 6-31G(d) basis sets were employed for H, C, and O, where a
diffuse function was added to each of O and a p-polarization function
was added to H. In all calculations, the solvation energy was evaluated
with the PCM method, where the UFF parameters were used to
determine the cavity size. It was ascertained that each equilibrium
geometry exhibited no imaginary frequency and each transition state
exhibited one imaginary frequency. In the case of homolytic cleavage
of the covalent O−O bond, the energy was evaluated using the
unrestricted-B3LYP (UB3LYP) method instead of the restricted-
B3LYP (RB3LYP) one.
Enthalpy, entropy, and Gibbs energy changes were calculated at
93.15 K. Zero-point energy, thermal energy, and entropy change were
2
evaluated with the DFT(B3LYP) method. The translational entropy in
1
3
water was computationally treated according to the literature. We
presented an example of the input file used for the geometry
optimization of TS3 in Supporting Information.
1
(
0, 3025.
5) Indirect quantification of acetic acid by using the ratio between
malonic acid and acetic acid is impossible in this case, since a
substantial part of the protons of malonic acid is deuterized by D O
during the degradation.
2
ASSOCIATED CONTENT
Supporting Information
Complete ref 11. Additional experimental details and results.
Cartesian coordinates of the optimized geometries. This
■
(6) We also optimized another transitions state connecting DHBQ to
*
S
I1k, in which only two water molecules are involved. However, the
calculated activation barrier (19.5 kcal/mol) was much higher than
that of TS1, indicating that at least three water molecules are necessary
to smoothly complete the nucleophilic addition; see also Figure S10 in
Supporting Information.
(
7) We did not calculated the transition states of this keto−enol
AUTHOR INFORMATION
interconversion, but the barriers in this process would be quite low,
since the keto form is much more stable than the enol counterpart.
■
*
⧧
(
8) One of the reasons for the discrepancy in the Δ S° is that we
used the gas phase rotational entropy without correction, though we
corrected the translational entropy.
Notes
The authors declare no competing financial interest.
(9) Siegel, B.; Lanphear. J. Org. Chem. 1979, 44, 942.
(
10) (a) Dagaut, P.; Wallington, T. J.; Kurylo, M. J. J. Phy. Chem.
1988, 92, 3836. (b) Vaghjiani, G. L.; Ravishankara, A. R. J. Phys. Chem.
989, 93, 1948. (c) Lightfoot, P. D.; Veyret, B.; Lesclaux, R. J. Phy.
Chem. 1990, 94, 708. (d) Lightfoot, P. D.; Lesclaux, R.; Veyret, B. J.
Phy. Chem. 1990, 94, 700. (e) Wallington, T. J.; Dagaut, P.; Kurylo, M.
J. Chem. Rev. 1992, 92, 667.
ACKNOWLEDGMENTS
■
1
We performed quantum chemical calculations on the work-
station of the Sakaki group, Fukui Institute for Fundamental
Chemistry at Kyoto University, Japan, and we thank them for
access. The financial support of the Austrian Christian Doppler
Research Society (CDG) through the CD-lab (Advanced
cellulose chemistry and analytics) and of the Austrian Research
Promotion Agency (FFG, project 829443) is gratefully
acknowledged.
(11) Frisch, M. J. et al. Gaussian 09, Revision A.1; Gaussian, Inc.:
Wallingford, CT, 2009. See Supporting Information for the complete
reference.
(12) (a) Becke, A. D. Phys. Rev. A 1988, 38, 3098. (b) Becke, A. D. J.
Chem. Phys. 1983, 98, 5648.
(13) Mammen, M.; Shakhnovich, E. I.; Deutch, J. M.; Whitesides, G.
M. J. Org. Chem. 1998, 63, 3821.
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