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Russ.Chem.Bull., Int.Ed., Vol. 60, No. 6, June, 2011
Gerasimova et al.
potential was attained). The reversible hydrogen electrode was
used as a reference electrode, and a glassy carbon plate served as
a reference electrode. The measurements were carried out acꢀ
cording to the procedure described earlier.23
Experimental
Carbon nanofibers with a diameter of 100—200 nm, a length
of 1—5 μm, and a specific surface of the 100 m2 g–1 BET (N2)
were used as platinum supports.20 According to the elemental
analysis data, the oxygen content is lower than 0.5%.
Results and Discussion
Platinum was supported on carbon fibers by the reduction of
PtCl62– in an alkaline solution of ethylene glycol (pH 11) under
the action of microwave radiation (800 W, 1 min). The syntheꢀ
sized samples of the Pt/C catalysts were filtered and dried for
10 h at 105 °C in a desiccator. Thermogravimetric (TGA) and
differential thermal (DTA) analyses were carried out using an
STA 409 Luxx thermoanalyzer with the mass spectrometric atꢀ
tachment for analysis of gaseous products (Netzsch). The TGA
and DTA curves were recorded in the linear heating regime
at 10 °C min–1 from room temperature to 1000 °C in an air
flow (flow rate 50 mL min–1). Weighed samples (5—10 mg)
were placed in a corundum crucible, and the platinum
content was determined by the incombustible residue at the
end of experiment. The samples with the weight content of platꢀ
inum from 4% to 61% were obtained by the variation of the
Pt : C ratio.
The synthesized samples Pt/CNF with a weight conꢀ
tent of platinum of 4—61% were studied by transmission
electron microscopy. The microimages of the samples with
the platinum content 4, 12, and 49% are shown in Fig. 1.
The platinum particles are uniformly distributed over the
surface of carbon fibers. It is seen that the number of large
clusters increases with an increase in the platinum conꢀ
tent. The Pt cluster size distribution (Fig. 2) calculated by
the TEM data is described by the logꢀnormal distribution
typical of freely growing particles.24,25 The averageꢀmass
distribution is broader than the averageꢀnumerical one,
and this difference increases with an increase in the platiꢀ
num content. Assuming that the nanoparticles are spheriꢀ
cal, the specific surface Sgeom was calculated for all cataꢀ
lysts (Table 1).
The prepared catalysts were also characterized by powꢀ
der Xꢀray diffraction (Fig. 3). The platinum content in the
studied samples exerts a noticeable effect on the diffracꢀ
tion patterns. All reflections of platinum in the region
studied are well seen in the samples with a high platinum
content. For the samples with a low platinum content, the
reflection intensity from the carbon nanofibers is much
higher than that from the platinum nanoparticles, and only
one peak of platinum corresponding to the reflection [111]
is observed. Based on the Xꢀray diffraction patterns obꢀ
The specific surface of materials was determined by the BET
method on a Quadrasorb Sl instrument (Quantachrome). The
pore size distribution was constructed on the basis of the analysis
of the curves of nitrogen sorption/desorption.21,22
The platinum particle sizes were determined by transmission
electron microscopy (TEM) (Zeiss LEO 912B) and using powder
Xꢀray diffraction (Brucker D8 Advances, Kα monochromator,
1
1D detector, CuKα radiation). An analysis of the microimages
1
of the catalysts made it possible to construct the averageꢀnumerꢀ
ical particleꢀsize distributions for platinum (200—500 units), acꢀ
cepting that the particles were spherical and ignoring agglomerꢀ
ates. To obtain the averageꢀmass distribution, the weight was
calculated for each measured particle.
For electrochemical studies of the catalysts, the electrodes
were prepared as follows. Carbon nanofibers with supported platꢀ
inum were dispersed in water with the addition of dispersion
Nafion® DE1020 (DuPont, USA) in an amount of 25% of the
carbon weight and were supported in the surface of the gasꢀ
diffusion layer Toray® TGPꢀHꢀ060 (Toray Industries, Inc.,
Japan). The prepared electrode was used as a working electrode
in the threeꢀelectrode cell, and a reversible hydrogen electrode
(0.5 М H2SO4, 20 °C) served as a reference. Prior to measureꢀ
ments of carbon monoxide adsorption, background voltammoꢀ
grams were detected on the electrode under study in the potenꢀ
Table 1. Characteristics of the Pt/CNF catalysts with various
platinum contents
b
Conꢀ
ja/A (mg of Pt)–1SСО Sgeom DN
DM
DXRD
tent of Pt/
(wt.%)
(0.5 V)
m2 g–1
nm
c
4
7
0.32
3.05
2.61
0.75
1.08
0.31
0.60
30 250 1.0
90 120 2.1
120 125 2.0
90 155 1.7
1.2
2.6
2.5
2.1
6.3
3.8
4.3
—
2.5(40°)
c
tial range from 0.1 to 1.2 V with a potential sweep of 0.02 V s–1
.
12
23
34
49
61
—
The true surface of the electrodes was calculated by the surface
area of the desorption peak of carbon monoxide. For this purꢀ
pose, the solution in the cell was saturated with CO for 15 min
at an electrode potential of 0.1 V, then CO was removed by
blowing with argon, and cyclic voltammograms were detectꢀ
ed. All potentials are presented relatively to the reversible
hydrogen electrode taking into account ohmic losses, which
were determined by the impulse potentiostatic method (inacꢀ
curacy 3%).
The electrodes of fuel cells were studied in the reduction of
oxygen in a liquid gasꢀdiffusion halfꢀcell (1 M H2SO4) by cyclic
and stationary voltammetry (as stationary were taken the values
of current detected 30 min after the moment at which specified
2.3(40°)
6.3(67°)
3.4(67°)
3.7(67°)
25
30
40
50
85
70
4.1
2.4
2.6
a At a potential of 0.5 V.
b Calculation by the Sherrer equation, D = 0.9•0.5406/V cosθ,
the value of 2θ is given in parentheses.
c The reflections corresponding to Pt are comparable with the
background.
Note. DN and DM are the averageꢀnumerical and averageꢀmass
sizes of the platinum clusters; and DXRD is the size of the Pt
clusters determined by Xꢀray diffraction analysis.