Inorganic Chemistry
Article
a
of FA solution (Figure 5). The resulting high-pressure gas was
composed of H2 and CO2 in the same molar ratio, whereas no
Table 5. Continuous DFA using the Ir Complexes
b
c
entry complex pressure /MPa stability /h CO /vol. ppm TON80%
d
1
2
3
4
5
6
7
1a
1a
1b
1b
1c
1d
PYIM
0.1
20
0.1
20
20
20
20
60
10
120
60
40
30
n.d.
n.d.
n.d.
n.d.
n.d.
n.d.
n.d.
66500
5829
402000
72400
50300
39100
45800
e
30
a
Reaction conditions: temperature = 50 °C, catalyst amount = 16
μmol, initial FA solution = 5 M, 40 mL. FA was added at a rate of 0.6
mL/h over 10 h using a plunger pump and then stopped for several
b
hours. This process was repeated several times. Time elapsed from
c
the beginning until a decrease in the gas generation rate. Calculated
value when the gas flow rate had decreased by 80% of the initial rate.
d
e
Below the detection limit (<6 vol. ppm). Data taken from the
literature.22
< 6 vol ppm, Figure S28). From 20 to 30 h of FA addition, the
gas flow rate was measured as 0.62 L/h (13 mmol-H2/h), and
the corresponding FA flow rate was 0.4 mL/h (11 mmol/h).
However, the gas flow rate gradually decreased over time
during FA addition. When the gas flow rate had decreased by
80% from the initial rate, a TON of 66500 (TON80%, Table 5,
entry 1) was calculated from the volume of H2. In the case of
1b, the average gas flow rate from 10 to 20 h of FA addition
was 0.80 L/h (16 mmol-H2/h). When the gas flow rate had
decreased by 80% and 50% from the initial rate, TONs were
402000 (TON80%, Table 5, entry 2) and 515000 (TON50%),
respectively. The TON80% for complex 1b (402000) was
therefore 6-fold larger than that for 1a (TON80% = 66500,
solution, the gas generation continued even after the addition
of FA had been stopped. Finally, when the FA decomposition
had reached completion, a TON of 974000 was calculated
from the total gas volume of H2.
Next, the catalytic stability of the complexes was studied
during continuous DFA at 20 MPa and 50 °C, and the
generated gas flow rate was measured. Complex 1a became
deactivated after the system reached 20 MPa (entry 2 in Table
5) owing to the formation of polymeric compounds with the
generated H2 which indicated limited stability under high
pressure.21 As determined using the stop and flow method,
complex 1b was able to generate the high-pressure gas with a
constant pressure of 20 MPa over six cycles of FA addition,
although the pressure gradually decreased thereafter (Figure
6). Complex 1b retained its stability for 60 h under high
pressure and afforded a TON80% value of 72400 (entry 4 in
Table 5). Complexes 1c and 1d also allowed a constant flow
rate of the generated gas to be maintained for six and three
cycles of FA addition, respectively, and the TON80% for 1c
(50300, Figure S30) was greater than that for 1d (39100,
Figure S31). In addition, we also observed that the resonance
associated with the amine and pyridine groups, which increases
with increasing electron density of the pyridine nitrogen atom,
had less effect on the stability than on the activity of the
catalyst. As mentioned above, we observed the highest pressure
of 153 MPa during DFA using the Ir-PYIM catalyst, although
the PYIM ligand lost its stability after 30 h at 20 MPa with a
TON80% of 45800. Thus, the incorporation of amino groups at
the para positions of pyridine improves the catalytic activity (=
TOF) and stability (= TON80%) during high-pressure DFA. It
should be noted that during the continuous-flow measure-
Figure 5. Time course of the generated pressure by the DFA at 80 °C
in highly concentrated FA solution using the Ir complexes (2 mM): ×
○
, 1a in 20 M FA; , 1c in 21 M FA.
CO (<6 vol ppm) was detected by GC analysis (Figure S25).
Under similar conditions, a maximum gas pressure of 123 MPa
was obtained using 1a owing to catalyst deactivation.22
Furthermore, we compared the reaction rates for complexes
1a, 1b, 1c, and 1d and an Ir complex bearing 2-(2′-
pyridyl)imidazoline (PYIM) to reach a pressure of 40 MPa
(Table 4), as PYIM was previously reported to generated the
a
Table 4. High-Pressure DFA using the Ir Complexes
complex
initial
reaction
time /h
residual FA
conc. /M
b
entry complex conc. /mM TOF /h−1
1
2
3
4
5
6
1a
1b
1c
1d
PYIM
PYIM
0.4
0.2
0.2
0.2
0.2
0.4
1900
8500
14600
16900
6500
14.0
5.2
3.7
2.2
18.2
2.4
0.55
0.42
0.40
0.37
9.99
0.40
9000
a
Reaction conditions: temperature = 80 °C, pressure = 40 MPa,
catalyst amount = 8 or 16 μmol, initial FA solution = 16 M, 40 mL.
b
Average value over the initial 10−30 min.
highest pressure of 153 MPa from DFA.22 The highest TOF
(16900 h−1) was obtained in 16 M FA solution using 1d at 80
°C. The flow rate of the high-pressure gas (H2 and CO2)
generated by DFA increased gradually with time during the
reaction (Figure S26) and might be correlated with the FA
concentration. Under these conditions, the equilibrium
concentration of FA was estimated as 0.37
0.01 M. This
high-pressure reaction was performed using the low concen-
trations of 1b, 1c, and 1d, and a high concentration of PYIM.
Based on the residual FA concentration after the reactions, the
complexes were arranged in descending order of catalytic
stability (1d ≅ 1c ≅ 1b > PYIM > 1a).
To assess the long-term reactivity, the Ir complexes were
subjected to continuous-flow measurements at 50 °C (Table
5). We first studied the decomposition of FA using 1a and 1b
at atmospheric pressure by adding neat FA to the solution at a
constant rate via a liquid pump. In the case of 1a, FA was
continuously and selectively decomposed into H2 and CO2
gases over 200 h without any detection of CO (detection limit
F
Inorg. Chem. XXXX, XXX, XXX−XXX