N. Ungvári et al. / Inorganica Chimica Acta 363 (2010) 2016–2028
2027
(1) is the source for Co2(CO)6(CHCO2Et) in the second cycle. The for-
5.4. Computational details
mation of the latter connects cycle A with cycle B. From the compo-
sition of the catalytic reaction mixtures and the observed kinetics of
the individual steps in the cycles we conclude that using sufficient
high concentration ratio of [N2CHCO2Et]/[CO] ꢅ 0.1, the rate-deter-
mining steps at low (1 bar) or high (50 bar) pressure of carbon mon-
oxide are the reactions of Co2(CO)7(CHCO2Et) (1) and
Co2(CO)6(CHCO2Et)2 (2) with carbon monoxide. Complex 2 is 66-
times more effective than complex 1 in this reaction. At low concen-
tration ratio [N2CHCO2Et]/[CO] < 0.1, the reactions of the catalyst
precursors Co2(CO)8 and complex 1 with ethyl diazoacetate become
rate determining, in which reactions the carbon monoxide concen-
tration has a negative effect. If the low concentration ratio of
[N2CHCO2Et]/[CO] is combined with a high CO concentration (for
example at 150 bar pressure), more diethyl malonate is produced
in catalytic cycle A than in catalytic cycle B.
Full geometry optimizations have been performed at the den-
sity functional level of theory without any symmetry constraints
using the GAUSSIAN 03 suite of programs [21]. For all the calculations
the gradient-corrected exchange functional developed by Becke
[22] was utilized in combination with a correlation functional
developed by Perdew [23] and denoted as BP86. For cobalt the va-
lence triple-f SDD basis set following the (8s7p6d1f) ? [6s5p3d1f]
contraction pattern is utilized with the corresponding relativistic
effective core potential [24]. For the other atoms the 6-31G(d,p)
basis set [25] was used. The density fitting basis sets were gener-
ated automatically from the AO primitives by the GAUSSIAN 03 pro-
gram. The stationary points were characterized by frequency
calculations in order to verify that they have zero imaginary fre-
quencies for equilibrium geometries and one imaginary frequency
for transition states. Thermochemistry corrections were taken
from frequency calculations at 298.15 K and 1 atm. Intrinsic reac-
tion coordinate (IRC) analyses [26] were carried out throughout
the reaction pathways to confirm that the stationary points are
smoothly connected to each other. For charge decomposition anal-
yses (CDA) the AOMIX software was used [27].
Computational studies on the ketene formation step have
shown that the coupling of the bridging carbene ligand with a
terminal CO ligand takes place via a low barrier resulting in a
coordinative unsaturated ketene complex, which is converted to
a (l2
g
–g –
2) ketene complex by an uptake of external CO. The (l2
2) complex quickly transforms to a (l1 2) species which
–g
releases ethoxycarbonylketene via a small barrier resulting in the
dibridged heptacarbonyl-dicobalt which reforms complex 1 after
reacting with ethyl diazoacetate.
Acknowledgements
The authors thank the Hungarian Academy of Sciences and the
Hungarian Scientific Research Fund for financial support under
Grant Nos. OTKA NK 71906 and F046959 and also thank the Super-
computer Center of the National Information Infrastructure Devel-
opment (NIIF) Program as well as Flextra Lab KFT. The support of
Bolyai Grant of the Hungarian Academy of Sciences for T.K. is also
acknowledged.
5. Experimental
5.1. General comments
Handling of the carbonyl cobalt complexes was carried out in an
atmosphere of dry (P4O10) and deoxygenated (BTS contact, room
temp.) argon or carbon monoxide utilizing standard Schlenk tech-
niques [17]. Methylene chloride were dried and distilled under an
atmosphere of argon or carbon monoxide according to standard
procedures [18]. IR spectra were recorded on Thermo Nicolet Ava-
tar 330 and Bruker Tensor 27 FTIR spectrometers using 0.00265,
0.00765, 0.0218 or 0.05097 cm CaF2 solution cells, calibrated by
the interference method [19]. Octacarbonyl dicobalt [20] and the
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The reactions of Co2(CO)8, complex 1 and complex 2 with ethyl
diazoacetate and ethanol at atmospheric pressure was performed
in a thermostatted glass reactor connected to a gas burette under
an atmosphere of carbon monoxide or argon. The gas volume
change was followed by reading the gas burette in appropriate
time intervals (usually 8–15 readings for calculation of the initial
rates). The concentration of diethyl malonate, Co2(CO)8, complex
1 and complex 2 in samples of the reaction mixture was calculated
from the IR spectrum using the molar absorbances of diethyl mal-
onate eM (CH2Cl2, 1749 cmꢁ1) = 579 cm2/mmol and eM (CH2Cl2,
1732 cmꢁ1) = 666 cm2/mmol, Co2(CO)8 eM (CH2Cl2, 2022 cmꢁ1) =
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697 cm2/mmol, complex
1
eM (CH2Cl2, 1853 cmꢁ1) = 953 cm2/
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Gomperts, R.E. Stratmann, O. Yazyev, A.J. Austin, R. Cammi, C. Pomelli, J.W.
Ochterski, P.Y. Ayala, K. Morokuma, G.A. Voth, P. Salvador, J.J. Dannenberg, V.G.
Zakrzewski, S. Dapprich, A.D. Daniels, M.C. Strain, O. Farkas, D.K. Malick, A.D.
Rabuck, K. Raghavachari, J.B. Foresman, J.V. Ortiz, Q. Cui, A.G. Baboul, S.
Clifford, J. Cioslowski, B.B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I.
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mmol, complex 2 eM (CH2Cl2, 2080 cmꢁ1) = 3768 cm2/mmol.
5.3. Measurements at higher than atmospheric pressure
Reactions above the atmospheric pressure using CO pressures
were performed in a thermostatted stainless steel autoclave of
20 cm3 capacity. The concentration of the components in the reac-
tion mixture was determined from samples by quantitative infra-
red spectroscopy (see above).