G.A.B. Mello et al. / Electrochemistry Communications 48 (2014) 160–163
161
knowledge about the influence of foreign atoms (like Rh and Sn) on the
ethanol electro-oxidation mechanism. In this context, despite the
unique characteristics ascribed to Pt–Sn–Rh combinations in the
literature, until now there are no works showing specifically how
The atomic compositions of the PtSnRh ternary electrodeposits were
estimated by energy dispersive X-ray analysis (EDX) using a Zeiss-
Leica/440 instrument provided with a SiLi detector. The mean values
were obtained from three points to each sample. Two samples were
prepared with PtSnRh compositions of (79:17:04) and (80:07:13). It is
worth noting that due to the penetration depth of the electron beam,
EDX analysis provides a bulk composition that does not necessarily
correspond to the surface atomic composition.
2
these catalysts act on the conversion of methyl groups to CO . This
issue is the main concern of the present work. Here we perform an in
situ FTIR study with isotopically labeled ethanol on ternary Pt–Sn–Rh
catalysts and investigate the ability of these surfaces to oxidize both
2 3 2
groups (–CH OH and –CH ) to CO .
3. Results and discussion
2
. Experimental
3.1. Analysis of polarization curves
4
+
Working electrodes were prepared by electro-reduction of Pt
Fig. 1 shows polarization curves obtained for both PtSnRh
compositions in 0.05 M ethanol solutions. Both curves show an
inflection in the current values at E ~ 0.25 V, which suggests that both
ternary compositions are active to electro-oxidize ethanol at very low
potentials. For both compositions, the oxidation profile is very similar
at low potentials, but the current densities become progressively higher
for that composition richer in Sn as the potential is increased. Such
behavior suggests that Sn plays a central role in the electro-oxidation
of ethanol and anticipates that PtSnRh (79:17:04) favors that pathway
responsible for the rising of currents at high potentials.
(
(
(
H
2
PtCl
SnCl
Sigma-Aldrich, ACS reagent, 70%) at 0.08 V vs. RHE for 10 min. A
6
—Sigma-Aldrich), Rh3 (RhCl
+
3
—Sigma-Aldrich) and Sn
2+
2
∙ 2H O—Merck) on a polished gold disk in 1.0 M HClO
2
4
platinum sheet of large area was used as a counter-electrode, and the
potentials were measured against a reversible hydrogen electrode
(
RHE) in a 0.1 M HClO
4
solution. For the spectroelectrochemical
experiments the solutions were prepared with Milli-Q water
13
13
(
—
18.2 MΩ cm) and 0.05 M ethanol (12CH
Isotec).
For the estimation of the surface areas we used the CO-stripping
procedure in a 0.1 M HClO solution, as described elsewhere [8]. The
3
–
CH
2
OH, 98 atom%
C
4
3.2. In situ FTIR characterization of isotopically labeled ethanol oxidation
charge involved in the oxidation of a monolayer of adsorbed CO was
used to estimate the surface areas, assuming a charge density of
Spectra of Fig. 2A and B were collected during the oxidation of
isotopically labeled ethanol on PtSnRh 80:07:13 and 79:17:04,
respectively. In these experiments, spectra were recorded from 0.05 V
up to 0.80 V with steps of 0.05 V. In Fig. 2A, at ~0.50 V two bands at
−
2
4
20 μC cm
.
For the electro-oxidation of ethanol the potential was kept at E =
0
.05 V and ethanol was admitted into the cell to reach the concentration
−
1
−1
of 0.05 M. Next, chronoamperometric experiments were performed by
monitoring the current vs. time response after the application of a
potential step of 0.05 V, from E = 0.05 to 0.80 V. For each step the
potential was kept constant for 50 s and the last current value before
the next step was taken to build the curves depicted in Fig. 1.
2343 cm
assigned to 12CO
bands shows that on PtSnRh catalysts, both methyl and alcohol carbon
and 2277 cm
rise simultaneously. These bands are
13
2
and CO , respectively [6]. The coexistence of both
2
groups are converted into CO
shows a band at ~1974 cm
2
1
in the same potential range. Fig. 2B
at 0.45 V (the exact wavenumber is
−
In situ FTIR spectra were acquired by using a FTIR spectrometer
equipped with a MCT detector. The electrochemical IR cell was fitted
potential-dependent) that is attributed to the stretching of linearly-
bonded CO [6]. Once both groups form CO it is expected that the
2
12
13
12
to a CaF
2
planar window. Further details of the spectroelectrochemical
dissociative adsorption of CH
COads. However, the band at low frequencies is not visualized in the
3
–
CH
2
OH yields both COads and
13
cell and setup can be consulted in [18]. Spectra were computed from
12
13
3
R
2 interferograms. Reflectance spectra were collected as the ratio (R/
) where R represents a spectrum at a given potential and R is the
present conditions, probably because COads and COads oscillators
are coupled and maximize that band located at higher frequencies
0
0
12
13
“
background” spectrum collected at E = 0.05 V. All the experiments
( COads signal) at the expenses of the lower frequency band ( COads)
were performed at room temperature. The same procedure of potential
steps described in the previous paragraph was adopted here.
[19]. Moreover, as previously noted by Vielstich et al., the use of
electrodeposited surfaces reduces the band intensities for adsorbed
species [20]. According to the authors, the reason for this effect probably
originates from the rough structure of such surfaces that imposes
important restrictions in the angles of incidence that can be perceived
by the detector [20]. Still, as the amount of COads coming from methyl
groups is lower [21], these effects combined can help to explain that a
single COads band is visualized in the present spectra. Other bands
0.04
0.03
0.02
0.01
0.00
PtSnRh (80:07:13)
PtSnRh (79:17:04)
−
1
at ~1378/1266 cm
can be attributed to the coupling of the
νC–OH + δO–H of \COOH groups of acetic acid [22]. Interestingly,
both bands can be visualized at 0.30 V (Fig. 2A–B) which indicates that
the formation of acetic acid is probably the responsible for the rising of
−
1
currents in Fig. 1. Finally, a large band at ~ 1108 cm corresponds to
C–H wagging vibrations [22] superimposed to the Cl–O stretching of
perchlorate [18]. Also, it is important noting that the magnitudes of the
bands cannot be compared between both series, once they were not
normalized by the corresponding areas of the electrodes.
3.3. PtSnRh facilitates the electro-oxidation of methyl groups
0.0
0.2
0.4
0.6
0.8
Potential vs. RHE/ V
2
New information on the selectivity towards the CO pathways
Fig. 1. Polarization curves for the oxidation of 12CH
–13CH
during the electro-oxidation of ethanol was afforded by taking the ratio
3
2
OH on PtSnRh electrodeposits
+ 0.05 M
12
(compositions indicated in the figure) between 0.05 and 0.80 V in 0.1 M HClO
4
of integrated band intensities extracted from Fig. 2, A( CO2, methyl)/
13
ethanol.
A( CO2, alcohol), as a function of the potential for both catalysts (Fig. 3).