Communications
DOI: 10.1002/anie.200703928
Methane Oxidation
Direct Oxidation of Methane to Methanol at Low Temperature and
Pressure in an Electrochemical Fuel Cell
Atsuko Tomita, Junya Nakajima, and Takashi Hibino*
Methane is an abundantly available fuel whose use is mainly
limited to that of a primary energy source due to its low
reactivity. Methanol, on the other hand, is a useful inter-
mediate material in many chemical manufacturing processes
as well as a safe-to-handle liquid fuel for transportation and
storage. There is therefore a long-standing industrial interest
in producing methanol from methane effectively. The
conventional synthesis of methanol from methane involves
multi-step processes, including the steam reforming of
methane and subsequent catalytic reaction. These processes,
however, require high temperatures (< 7008C) and pressures
Although the direct oxidation of hydrocarbons has been
demonstrated in solid-oxide fuel cells (SOFCs) with stabilized
[
10,11]
[12]
zirconia
and perovskite-type oxide electrolytes, these
electrolytes require high temperatures above 5008C to show
high ionic conductivities. We have recently reported that
3
+
10 mol% In -doped SnP O (Sn In P O ) shows high
2
7
0.9
À1
0.1
À1
2
7
[1]
proton conductivities of above 10 Scm between 100 and
3508C under water-free conditions. This material has also
been used as an electrolyte in fuel cells, and herein we
report the selective oxidation of methane to methanol in a
hydrogen-oxygen fuel cell containing Sn In P O as electro-
[
13]
[14]
0
.9
0.1
2
7
(
200–300 atm) operations, respectively, which lead to high
running costs.
The direct oxidation of methane to methanol has received
lyte.
Sn In P O was prepared as reported previously. Pd/
[13]
0
.9
0.1
2
7
C, Pt/C, Rh/C, Au/C, and PdAu/C (10 wt.% metal) catalysts
were tested as the cathodes. The weight ratio of Pd to Au in
PdAu/C was in the range from 1 to 8. These catalysts were
prepared by an impregnation method starting from the
corresponding metal salts (PdCl , H PtCl ·6H O, RhCl , and
much attention as the next step in methanol production since
it avoids the above multi-step processes. However, this
oxidation is regarded as a very difficult reaction, especially
in the gas phase at low pressure, because of the need to
operate at high temperatures (> 4008C), where methanol is
2
2
6
2
3
HAuCl ·4H O). Thus, carbon powder (Black Pearls) was
4
2
[2–7]
quickly oxidized to formaldehyde and COx.
One approach
suspended in an ethanol/water solution and the metal salt
added at about 608C. After drying and grinding, the catalyst
powders were reduced under an H /Ar (10 vol.% H )
for oxidizing methane at lower temperatures is to apply an
electrochemical cell to the reaction system. Otsuka and
Yamanaka et al., for example, have reported the selective
oxidation of light alkanes to oxygenates by the electrochemi-
2
2
atmosphere at 4508C for 4 h. A commercial Pt/C anode
(60 wt.% Pt) was purchased from E-TEK inc.
[
8,9]
2
cally activated oxygen species
that are generated at the
The anode and cathode (area: 0.5 cm ) were attached on
cathode in polymer electrolyte (PEFCs) and phosphoric acid
fuel cells (PAFCs) [Eqs. (1) and (2)].
opposite sides of the electrolyte (thickness: 1.0 mm) and two
gas chambers were set up by placing the cell assembly
between two alumina tubes. The cathode and anode were
supplied with a 50 vol.% methane–50 vol.% oxygen mixture
and hydrogen, respectively, at a flow rate of 30 mLmin . Gas
analysis was performed with online flame-ionization detector
Anode : H ! 2 H þ 2 eÀ
þ
ð1Þ
ð2Þ
2
À1
Cathode : O þ 2 H þ 2 eÀ ! O* þ H O
þ
2
2
(FID) and thermal-conductivity detector (TCD) gas chroma-
tographs. The whole gas line and the alumina tube were
heated to a temperature of approximately 808C and the gas
concentrations were obtained after the reaction steady state
had been attained. Current/voltage curves for the fuel cell
were measured with a galvanostat.
The ability to produce methanol from methane was first
investigated with the Pd/C, Pt/C, Rh/C, and Au/C cathodes at
2508C. The common feature of these fuel cells is their open-
circuit voltage (OCV; 715–915 mV), which is lower than the
theoretical OCV of 1.1 V in all cases. This result is not due to
the presence of methane in the cathode gas, since there is no
difference in the OCVs in the presence and absence of
methane. At least two factors are responsible for the lower
OCVs: 1) physical leakage of gas through the electrolyte and
These active oxygen species can directly oxidize various
hydrocarbons, such as ethane and propane, to oxygenates at
low temperatures (< 808C), however, there has been no
report on the selective oxidation of methane to methanol in
fuel-cell systems. This is because the operating temperature is
too low to oxidize methane. Clearly, therefore, a fuel cell
capable of working above 808C is necessary for methane
oxidation.
[*] J. Nakajima, Prof. T. Hibino
Graduate School of Environmental Studies, Nagoya University
Fro-cho, Chilkusa-ku, Nagoya 464-8601 (Japan)
Fax : (+81)52-789-4206
E-mail: hibino@urban.env.nagoya-u.ac.jp
2
) partial electron/hole conduction in the electrolyte, which
A. Tomita
causes an internal short circuit. These fuel cells also show a
large difference in the short-circuit current (140–250 mA).
Materials Research Institute for Sustainable Development
National Institute of Advanced Industrial Science and Technology
Simosidami, Moriyama-ku, Nagoya, 463-8560 (Japan)
1
462
ꢀ 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2008, 47, 1462 –1464