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A much higher FA yield can be obtained in the presence of
DBU. A reaction at 658C leads to an AAR of 1.6 with a TOF of
36000 hꢀ1. In agreement with previous reports,[13b,16] the activi-
ty can be further enhanced at higher H2 partial pressures
(entry 3, Table 2). At a H2/CO2 molar ratio of 3:1 (Ptotal =40 bar),
a TOF of 65000 hꢀ1 was obtained at 658C, which increases to
1100000 hꢀ1 if the reaction is performed at 1208C (entry 4,
Table 2). This rate is nearly one order of magnitude higher than
the current record value reported for Nozaki’s Ir PNP-pincer
catalyst, which operates at a higher temperature and pressur-
e.[6a] In this high-temperature experiment, the kinetic trace fol-
lowed first-order behavior with respect to product formation
(Figure S11).
(40 bar) and low-pressure (5 bar) loading procedures, respec-
tively. The complete H2 liberation time did not exceed 1 h, at
which gas evolution peaked at over 160 mLminꢀ1, which corre-
sponds to TOF values higher than 150000 hꢀ1. H2/CO2 charging
times were less than 3 h, which depends on the temperature
program. The cyclic operation was performed without the ad-
dition of extra base between the cycles, which was necessary
for the stable performance of the amine-based system report-
ed previously.[5] No catalyst deactivation was observed in the
course of these experiments.
To conclude, we report the development of a highly active
system for the reversible hydrogenation of CO2. To the best of
our knowledge, the catalytic activities obtained for CO2 hydro-
genation and FA dehydrogenation reactions are the highest re-
ported to date. If used in combination with DBU, catalyst 1
allows the control of the hydrogen liberation activity in
a narrow temperature interval. Our results point to the key
role of the base strength to determine the H2 capacity of the
system under catalytically relevant conditions. Namely, strong
bases are required to generate high AARs at elevated tempera-
ture if the reaction times are short. Base strength was found to
affect the nature of the RDS in FA dehydrogenation. Although
the CꢀH cleavage step controls the rate in the presence of
weak bases, the initial H2 recombination determines the rate if
the reaction is performed in the presence of strong bases. The
reported system holds promise for the development of a practi-
cal H2 storage technology based on the reversible catalytic hy-
drogenation of CO2.
With the exceptional performance of 1 in DMF/DBU we
were able to hydrogenate CO2 at a relatively low pressure (en-
tries 5 and 6, Table 2). A high reaction rate of 60000 hꢀ1 was
obtained at a total pressure of only 5 bar of an equimolar
H2/CO2 mixture at 908C. This is superior to the TOF achieved
by the Fujita Ir catalyst[7] (Figure 1) at a comparable tempera-
ture of 808C and a 10-fold higher pressure. Unlike the DMF/
NEt3 system, the increase of the reaction temperature leads to
the stabilization of a higher AAR in DMF/DBU (Figure 4). The
H2 capacity of the DMF/DBU medium also depends strongly on
the total pressure. A stepwise increase of the pressure from 5
to 40 bar led to higher formate concentrations. A maximum
AAR of 2.1 was obtained at 908C and 40 bar. These data exem-
plify the crucial difference between DBU- and NR3-based sys-
tems. The high capacity of the latter can only be achieved at
low temperatures at the expense of the reaction rate. With
a molar volume similar to that of NEt3, DBU offers a nearly six-
fold higher FA loading capacity at 658C.
Experimental Section
All manipulations unless otherwise stated were performed using
Schlenk techniques. Catalytic hydrogenation tests and cycling ex-
periments were performed by using a 100 mL stainless-steel auto-
clave equipped with a gas compensation device and flowmeter for
evolved gas detection. CO2 hydrogenation was performed at a con-
stant pressure. Samples were withdrawn by using a dip tube instal-
lation and analyzed immediately by HPLC and GC with flame ioni-
zation detection (FID). The reaction was triggered by the addition
of the catalyst to a pressurized and preheated vessel. TOF values
were determined at the initial reaction stage if possible.
To further investigate the possibility of cyclic operation with
1 in DMF/DBU, we performed a series of hydrogen storage–re-
lease cycles over a week. Alternating high- and low-pressure
loading procedures were employed to evaluate the sensitivity
of the system to the variation of the operating conditions. The
results of these measurements are summarized in Figure 5. In
all cycles, the evolved H2/CO2 gas volumes were consistent
with AARs measured by direct sampling of the reaction mix-
ture. AAR values of 1.6 and 1.1 were observed for high-
Dehydrogenation reactions were performed by using a double-
lined glass reactor and syringe pump for FA supply. Gas evolution
was analyzed by using a Bronkhorst flowmeter or a foam flowme-
ter. The gas composition was analyzed by GC with thermal conduc-
tivity detection (TCD) and verified to be H2/CO2 =1:1 with no de-
tectible traces of CO. TOF values were estimated from the gas evo-
lution rate for both gas-detection methods.
Full experimental procedures for hydrogenation, dehydrogenation,
continuous storage, and activation energy determination are given
in the Supporting Information.
Acknowledgements
Figure 5. Total gas evolution in the H2 storage–release cycles with 1 in DMF/
DBU. Storage was performed at 658C under 40 bar (dark bars) and 5 bar
(light bars) H2/CO2 =1:1. Release was performed after decompression of the
system at 658C followed by heating to 908C (conditions: DMF/DBU=
30:5 mL, 1.42 mmol 1).
E.A.P. gratefully acknowledges the Technology Foundation STW
and the Netherlands Organization for Scientific Research (NWO)
for his personal VENI grant.
ꢀ 2014 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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