Investigation of Methanol Oxidation
A R T I C L E S
Table 1. Some Physicochemical Properties of the Studied
Samples
interest to develop a process able to yield an ultra pure hydrogen
source for fuel cell applications. In this frame, intense investiga-
tions have been conducted during recent years, and especially
gold-containing materials were reported as very promising
catalysts to selectively convert CO into CO2 in the presence of
an excess of H2.1,18,19,21,22,24-29 In fact, gold has been for a
long time disregarded for any catalytic applications because this
noble metal is one of the most chemically inert element. The
very new life of gold in heterogeneous catalysis is due to
Haruta’s pioneer work30 who evidenced both a preparation
method to obtain Au supported nanoparticles (mean diameter
<5 nm) and the requirement of these nanosized gold particles
to generate highly active catalytic sites. More precisely, the new
coprecipitation method, which allows one to prepare gold
nanoparticles with an optimal size around 3 nm,31 even opened
the door to the low temperature catalytic oxidation, because it
appeared that CO could be converted into CO2 at temperature
as low as 200 K. From this discovery, the research on catalytic
properties for gold has increased exponentially. Nevertheless,
only a relative limited fraction of the reported studies deals with
mechanistic investigations, and the majority of them concern
CO oxidation at low temperature. These are the major reasons
why this study focuses on Au/CeO2 and Au/TiO2 nanosized
catalysts, aiming at understanding how they really work at the
molecular scale to provide information useful for extending their
efficiency to the oxidation of molecules more complex than CO,
that is, VOC compounds, represented by methanol in the present
case.
gold content/
wt %
specific area
(BET)/m2 g-1
gold particles
size/nm
sample name
TiO2
85
180
85
180
60
CeO2HSA
Au/TiO2
Au/CeO2HSA
Au/CeO2LSA
0.6
1
1
<3
<3
<3
the sample modifications and the methanol conversion, which was
also measured by online mass spectrometry.
Details on the operando system and the applied methodology
are reported in the Supporting Information. For this specific study
requiring efficient thermal regulation at temperatures close to room
temperature, a new reactor cell has been designed in our laboratory
(Figure 1). It is made of a stainless steel cylinder that carries a
toroidal sample holder in its center, where the catalyst is placed in
the form of a self-supported wafer of 10 mg cm-2. The thermo-
regulating system allows one to hold the sample at a fixed
temperature in a range from 263 to 373 K. The reaction chamber
hosting the sample is obviously tight with respect to the external
atmosphere, and its dead volume is extremely small allowing one
to obtain (i) time-resolved analysis, (ii) surface spectra without
superposition of the gas-phase signal, and (iii) fluid dynamics very
similar to that of a honeycomb system.
The reacting gas mixture composition was fixed to 700 ppm
CH3OH, 20 vol % O2 in argon, and the total flow was adjusted to
work with a constant gas hourly space velocity (GHSV) equal to
60 000 h-1. Before any experiment, each sample was simply treated
with argon and oxygen for a night at room temperature to stabilize
the surface state, without any thermal activation, to prevent metal
particle growth.
2. Experimental Section
Materials. The catalysts were prepared by depositing Au (via
trihydrated chlorauric acid) onto CeO2 and TiO2 commercial powder
materials with granulometry in the micrometer range. Two ceria
supports with pure fluorine phase having a high and a low level of
initial specific surface area and a pure anatase titania support were
chosen for this study. Details on the sample preparation are reported
in the Supporting Information.
In both cases, Au is finely dispersed onto the oxide supports
with a mean particle size below 3 nm as estimated by the X-ray
diffraction line broadening of Au. Furthermore, the specific surface
area of the oxides was unaffected by the Au deposition, as described
in Table 1.
3. Results and Discussion
3.1. Effect of the Support CeO2 or TiO2. The first aim of
this study was to investigate a potential activity of the support
oxides themselves. The evolution of the CH3OH conversion
(calculated from IR gas-phase analysis) with time on stream
(TOS) is given for CeO2-based samples in Figure 2. Focusing
on the CeO2HSA sample, a conversion loss to reach a plateau
without any catalytic activity was observed. Two hypotheses
are possible to explain this phenomenon of conversion drop:
(i) the catalysts deactivate with time on stream or (ii) the
disappearance of CH3OH is related to adsorption only and stops
when the surface is saturated.
Operando Tests. Operando IR studies were carried out using
the transmission technique to obtain quantitative data. Sample and
gas-phase IR spectra were alternatively collected to follow both
The upper part of Figure 2 indicates that during the first 30
min, the exposed surface cerium cations are saturated by
methoxy species coming from the dissociative methanol adsorp-
tion. According to abundant literature data,32-37 the band
evolving at 1102 cm-1 is associated with the formation of on
top methoxy species (type I) on Ce4+ cations, thus giving
evidence that after one night pretreatment under oxygen at room
temperature the main part of surface cations is oxidized. During
(21) Avgouropoulos, G.; Ioannides, T.; Papadopoulou, C.; Batista, J.;
Hocevar, S.; Matralis, H. K. Catal. Today 2002, 75, 157–167.
(22) Avgouropoulos, G.; Papavasiliou, J.; Tabakova, T.; Idakiev, V.;
Ioannides, T. Chem. Eng. J. 2006, 124, 41–45.
(23) Tabakova, T.; Boccuzzi, F.; Manzoli, M.; Sobczak, J. W.; Idakiev,
V.; Andreeva, D. Appl. Catal., A 2006, 298, 127–143.
(24) Avgouropoulos, G.; Manzoli, M.; Boccuzzi, F.; Tabakova, T.; Pa-
pavasiliou, J.; Ioannides, T.; Idakiev, V. J. Catal. 2008, 256, 237–
247.
(25) Ko, E.-Y.; Park, E. D.; Seo, K. W.; Lee, H. C.; Lee, D.; Kim, S.
Catal. Today 2006, 116, 377–383.
(32) Colo´n, G.; Pijolat, M.; Valdivieso, F.; Vidal, H.; Kasˇpar, J.; Finocchio,
E.; Daturi, M.; Binet, C.; Lavalley, J. C. J. Chem. Soc., Faraday Trans.
1998, 94, 3717.
(26) Luengnaruemitchai, A.; Osuwan, S.; Gulari, E. Int. J. Hydrogen Energy
2004, 29, 429–435.
(27) Panzera, G.; Modafferi, V.; Candamano, S.; Donato, A.; Frusteri, F.;
Antonucci, P. L. J. Power Sources 2004, 135, 177–183.
(28) Manzoli, M.; Avgouropoulos, G.; Tabakova, T.; Papavasiliou, J.;
Ioannides, T.; Boccuzzi, F. Catal. Today 2008, 138, 239–243.
(29) Wang, H.; Zhu, H.; Qin, Z.; Wang, G.; Liang, F.; Wang, J. Catal.
Commun. 2008, 9, 1487–1492.
(33) Finocchio, E.; Daturi, M.; Binet, C.; Lavalley, J. C.; Blanchard, G.
Catal. Today 1999, 52, 53.
(34) Daturi, M.; Binet, C.; Lavalley, J. C.; Galtayries, A.; Sporken, R. Phys.
Chem. Chem. Phys. 1999, 5717.
(35) Daturi, M.; Finocchio, E.; Binet, C.; Lavalley, J. C.; Fally, F.;
Perrichon, V.; Vidal, H.; Hickey, N.; Kasˇpar, J. J. Phys. Chem. B
2000, 104, 9186.
(30) Haruta, M.; Kobayashi, T.; Sano, H.; Yamada, N. Chem. Lett. 1987,
16, 405.
(36) Binet, C.; Daturi, M. Catal. Today 2001, 70, 155. 155.
(37) Binet, C.; Daturi, M.; Lavalley, J. C. Catal. Today 1999, 50, 207.
(31) Haruta, M. CATTECH 2002, 6, 102.
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