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(b.p. 1628C).[8,9] However, harsh conditions and extended
reaction times, together with the requirement for high-boiling
solvents, which are difficult to remove from the product after
the reaction, make catalytic decarbonylation reactions gen-
erally incompatible with a high-yielding and sustainable
reaction procedure. Therefore, the majority of decarbon-
ylation protocols for the synthesis of complex molecules still
rely on stoichiometric or near-stoichiometric amounts of
a rhodium complex.[5]
Herein, we describe a unique biphasic gas–liquid contin-
uous-flow decarbonylation protocol that enables the efficient
decarbonylation of aldehydes in the presence of a catalytic
amount of a rhodium precursor within only 8–25 min. This
otherwise very challenging transformation is made possible
by inducing an annular flow regime in a coil-based micro-
reactor by using nitrogen as an inert carrier gas, which
efficiently removes CO from the equilibrium.
We chose 4-cyanobenzaldehyde (6a) as the model sub-
strate for initial optimization experiments (for optimization
details, see the Supporting Information). As it was clearly
evident from previously reported studies that a fast, catalytic
decarbonylation reaction would have to involve a high-
temperature regime, controlled sealed-vessel microwave
heating was used for process optimization.[10] The active
[Rh(dppp)]+ catalyst could be generated in situ from dppp
and various Rh sources, such as
pressure of the flow system was reduced, and the pressure
approached the vapor pressure of the solvent, did the
conversion increase from 30 to around 70% (see Table S5).
These experiments clearly demonstrate that the lack of
a headspace in the closed flow system, and the consequently
high concentration of CO in the liquid phase, inhibits the
decarbonylation reaction and prevents genuine catalysis. It is
well-known that, depending on temperature and the partial
pressure of CO, rhodium forms a range of different carbonyl
complexes, and the electronically depleted carbonyl com-
pounds generally do not participate in the decarbonylation
reaction.[1,13]
To prevent the poisoning of the catalyst by carbon
monoxide, we envisaged stripping the CO from the reaction
mixture with a stream of an inert gas fed into the flow system
(Figure 1).[14,15] Indeed, when N2 was fed into the flow reactor,
the conversion increased strikingly and approached or even
surpassed the results obtained under microwave batch con-
ditions on a small scale. Optimization of the process
parameters clearly illustrates that operation at the highest
temperature and lowest pressure is desired—namely, slightly
above the vapor pressure of the solvent at a given temper-
ature, to avoid its vaporization (Table 1; see also Tables S9–
S12).[14,16] Under such conditions, the experimentally deter-
mined residence time of the reaction mixture in the flow
RhCl3·3H2O or Rh(OAc)2 (see
Table S1 in the Supporting Informa-
tion). Initial optimization of the reac-
tion conditions provided best results
with 4 mol% of Rh(OAc)2 and
8 mol% of dppp in aprotic, inert
solvents, such as toluene. The reaction
was remarkably clean (ca. 95%
according to GC with a flame ioniza-
tion detector, GC–FID), and the only
detectable side product was 4,4’-dicya-
nobenzophenone, formed by a decar-
bonylative homocoupling of 4-cyano-
benzaldehyde.[11]
Figure 1. Gas–liquid continuous-flow decarbonylation of aldehydes with N2 as a stripping gas.
P=HPLC pump, SL=sample loop (poly(tetrafluoroethylene), 0.8 mm inside diameter), M=mixer
(1.0 mm i.d.), RT=residence tube (stainless steel, 1 mm i.d.), HE=heat exchanger (stainless
steel, 1 mm i.d.), BPR=back-pressure regulator).
Our initial batch experiments con-
firmed that the rhodium-catalyzed
decarbonylation of aromatic aldehydes
requires fairly high temperatures for
a reaction to occur at reasonable rates,
Table 1: Continuous-flow decarbonylation reactions at different temper-
or for the catalytic cycle to be completed at all. Furthermore,
even though a clean decarbonylation was possible at reaction
temperatures of around 2008C by sealed-vessel microwave
heating, the reaction rate greatly depended on the scale on
which the experiments were performed. With increasing
filling volume and consequently decreasing available head-
space in the sealed vessel, the reaction rate decreased
markedly. Whereas full conversion was observed on
a 0.6 mmol scale in a 10 mL microwave vial after 15 min at
1808C, the conversion gradually decreased to 26% when the
scale was increased to 1.4 mmol (see Table S4). Similarly,
conversions were around only 30% for initial continuous-flow
experiments in pressurized coil reactors, in which the head-
space is essentially eliminated.[12] Only when the back
atures and N2 flow rates (Figure 1; flow rate of liquid feed:
0.5 mLminÀ1).[a]
T/p
N2 [mLN minÀ1 [b]
]
[8C]/[bar]
8
15
25
180/6.8
200/9.1
220/12.5
65%
89%
92%
72%
93%
93%
89%
95%[c]
[a] The percentages given are the conversion of 6a into 7a under the
specified conditions of temperature, pressure, and nitrogen flow rate, as
determined by GC–FID. Flow reactions were performed in a 20 mL
stainless-steel reactor with a 0.2m solution of 4-cyanobenzaldehyde (6a)
in toluene (2 mL), Rh(OAc)2 (4 mol%), and dppp (8 mol%). [b] Gas flow
in mLN minÀ1 under normal conditions (Tn =08C and pn =1 atm). [c] The
pressure was increased from 9.1 to 9.7 bar.
2
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Angew. Chem. Int. Ed. 2014, 53, 1 – 6
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