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3.3. Electro-oxidation of carbon monoxide
calculate the current density, the maximum value of
current density for the glycerol electro-oxidation was
determined for each platinum loading.
The differences observed between the Au/PAni–Pt
and GC/PAni–Pt electrodes can be attributed to the
differences in the active surface area of the dispersed
particles in the PAni. So, the electro-oxidation of an
adsorbed carbon monoxide monolayer [28,32] was per-
formed in order to evaluate the electrode active surface
area. These area values were determined from the
charges for CO electro-oxidation (QCO) on Au/PAni–Pt
Fig. 4 shows the evolution of the maximum current
density jmax for glycerol oxidation as a function of the
platinum loading. It can be observed that for both
electrodes (i.e. Au/PAni–Pt and GC/PAni–Pt), the cur-
rent density maximum increases with the amount of
platinum, but around 180 mg cm−2, significant differ-
ences appear. For the Au/PAni–Pt electrode the cur-
rent density jmax decreases after the maximum while for
the GC/PAni–Pt electrode a plateau is observed. Addi-
tionally, below 180 mg cm−2 of Pt, the value of jmax
increases faster with platinum loading for the Au/
PAni–Pt electrode than for the GC/PAni–Pt.
The efficiencies of the two types of electrode can be
evaluated from the initial slopes of the curves in Fig. 4.
The value obtained for the Au/PAni–Pt electrode is 3.8
A g−1 i.e. 50% of the value estimated for GC/PAni–Pt
electrode (7.6 A g−1). These values are at least one
order of magnitude lower than that estimated for
methanol oxidation [21].
Another interesting aspect is that, for glycerol oxida-
tion, the optimization of the electrode activity (maxi-
mum value) in the present case is observed for platinum
loading of 180 mg cm−2. This value is higher than that
usually reported (100 mg cm−2) for the same conditions
for the oxidation of small organic molecules such as
methanol, formaldehyde, formic acid and carbon
monoxide [21–25]. On the other hand, Kelaidopoulou
and GC/PAni–Pt electrodes containing 180 mg cm−2
.
It was also taking into account that the oxidation of a
full CO monolayer involves 420 mC cm−2 [28,34] and
that all the active sites occupied by CO molecules are
available, in the absence of CO, for the adsorption and
electro-oxidation of the glycerol molecules. This suppo-
sition is necessary in order to compare the results
obtained for glycerol. It is obvious that the number of
active sites for CO and glycerol molecules is different
but it is possible to have an idea about the ratio of the
real surface area of both modified electrodes.
From the cyclic voltammograms of Au/PAni–Pt and
GC/PAni–Pt with a platinum loading of 180 mg cm−2
in 0.1 M HClO4, in the absence of adsorbed CO and for
the electro-oxidation of a carbon monoxide monolayer
absorbed at 0.05 V, the values of QCO obtained were
14.46 and 8.27 mC for Au/PAni–Pt and GC/PAni–Pt,
respectively. These values (12 QCO) correspond to active
areas of 34.4 and 7.88 cm2, respectively. Considering
that the GC/PAni–Pt has a geometric surface area
equal to 0.4 cm2, its active area can be normalized
(divided by 0.4) in order to compare it with that
corresponding to the Au/PAni–Pt electrode. The nor-
malized active area for the GC/PAni–Pt is 19.7 cm2
and for the Au/PAni–Pt 34.4 cm2. The difference be-
tween the active surface area values of both electrodes
is ca. 43%.
On the basis of the active area values, the real current
densities for glycerol electro-oxidation on electrodes
with a platinum loading of 180 mg cm−2 were calcu-
lated and the resulting cyclic voltammograms for Au/
PAni–Pt and GC/PAni–Pt are shown in Fig. 5. Taking
into account the electrode active areas, the Au/PAni–Pt
electrode presents the higher electrocatalytic activity,
with current density values almost 30% higher than
those for GC/PAni–Pt. Additionally, glycerol oxida-
tion on Au/PAni–Pt starts at less positive potentials
than on GC/PAni–Pt. Also, there is a 100 mV potential
shift toward lower values between the Au/PAni–Pt
electrode and a smooth platinum electrode showing
that the modified electrodes are more active for glycerol
oxidation than the smooth platinum surface.
et al. [33] observed for the electro-oxidation of b-D-
(+)glucose using Pt/PAni–Pt electrodes that the maxi-
mum current densities, as well as the optimum platinum
loading (2.3 mg cm−2) are much higher than the values
observed in the present study. A possible explanation
for the higher values is the use of platinum as substrate
for the PAni electrosynthesis, which reinforces the re-
sults of this work showing the influence of the primary
substrate in the platinum microparticle distribution.
The platinum particle size (S) was estimated using
the procedure of Croissant et al. [28] and then, the
mean particle size (d) was determined assuming spheri-
cal particles of similar radius [35]. For the Au/PAni–Pt
Fig. 4. Maximum value of the electro-oxidation current of glycerol as
a function of platinum loading for (ꢀ) Au/PAni–Pt and (ꢁ) GC/
PAni–Pt electrodes.