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Russ.Chem.Bull., Int.Ed., Vol. 59, No. 8, August, 2010
Kadirov et al.
serving as the catalyst and grids of a thin Pt wire. The grids are
arranged at two sides of the catalystꢀcovered membrane and
serve as both electrodes and gas dividers.
(2)
First, fluoroplastic tube 3 is placed on a fluoroplastic cylinder,
which is mounted of body 1 and cap 2 with membrane—electrode
assembly 4 in the inner hole, thus transforming the components
into a single whole. The electrodes are connected to the external
circuit using thin silver connecting wires. Tubes, through which
hydrogen and oxygen are fed to the FC under low pressure and
their excess is removed, are connected to the channels. The side
of the membrane—electrode assembly, where hydrogen comes
through channels 1 and 2, serves as an anode, and the cathode is
the side where oxygen comes. The FC is placed in the ESR
spectrometer cavity in such a manner that the electric field lines
of the cavity standing waves would be perpendicular to the surface
covered with the catalyst of the membrane. Electrochemical
reactions of hydrogen oxidation and oxygen reduction occur on
the catalyst surface between the electrodes and membrane.
Hydrogen atoms split into the component electron and proton
on the catalyst surface in the negatively charged anodic part.
Protons diffuse to the cathode through the membrane, and
electrons move through the external circuit making useful work.
The electrons reach the cathodic side and reduce oxygen atoms
to bivalent ions. These ions form water and heat upon the
reaction with diffused protons. The FC performs the direct
conversion of the fuel energy to electricity, omitting poorly
efficient combustion processes that occur with high losses.
Experiments were carried out with H2/O2, viz., FC for
ESR with the surface density 0.2—1.0 mg cm–2 Pt/Nafion 117.
A 1 М solution of DMPO in water or alcohol (10 μL) was
uniformly deposited on the anodic or cathodic side. Spectra
were recorded 5 min after the beginning of the work of the FC
under the short circuit conditions. Conventionally high potentials
(>0.3 V) were used, and low potentials (<0.1 V) were also used
in particular experiments, which is additionally mentioned during
DMPO
DMPO/X
nearest the radical center. The large database on spin
adducts are available at the site.4
Experimental
The ESR method was used to study processes and products
in the FC.
By analogy to the prototype described earlier,5 we designed a
FC for ESR more reliable and simpler in operation.6 The scheme
of the FC for ESR is shown in Fig. 1.
The FC for ESR consists of body 1, cap 2, fluoroplastic tube
3, and membrane—electrode assembly 4. Channels providing
access of hydrogen and oxygen and removal of their excess are
made in the body and cap. Body 1 and cap 2 are connected in
such a way that metallic tubes 5, which are the ends of two
channels in the body, enter the corresponding two channels in
the cap, and the channels are joined into a single system. The
internal diameter of tube 3 is equal to the external diameter of
the cylindrical FC mounted of two parts. The body and cap have
holes for mounting of membrane—electrode assembly 4 consistꢀ
ing of the Nafionꢀtype membrane with supported Pt particles
5
a
the description. The flow rate of hydrogen was 14 cm3 min–1
and that of oxygen was 7 cm3 min–1
,
.
1
4
ESR spectra were detected on 3ꢀcm EMX (Bruker),
RadioPAN SE/Xꢀ2543, and REꢀ1306 radiospectrometers with
frequencies of 9.3—9.9 GHz. The former two spectrometers
are equipped with a rectangular cavity ТЕ102, and REꢀ1306 has
a cylindrical cavity ТМ110. The polarizing magnetic field was
modulated with a frequency of 100 kHz, and the sensitivity of
the spectrometers was (1—5)•1012 spin T–1. The polarizing
magnetic field induction was measured with ERꢀ035 and Sh1ꢀ1
NMR magnetometers and a Hall sensor. Frequencies in a
microwave cavity were measured with an EiP371 frequency
meter. The standard mode of ESR spectra detection was used
with autotuning of the klystron signal frequency by the measuring
cavity. The choice of detection modes was determined by
requirements of undisturbed recording of the first derivative of
the ESR signal. The measurement inaccuracy of magnetic
parameters depends mainly on inaccuracies of the frequency
meter and magnetometer, stability of resonance conditions, and
ESR linewidth, being 3•10–2 G for HFC constants and 1•10–4
for g factors.
2
4
b
5
1
2
c
Magnetoresonance parameters and relative intensities of
spectral components were determined, as a rule, by computer
simulation of experimental ESR spectra. The SimFonia (Bruker)
and WinSim (NIEH/NIH) simulation programs were used, and
the latter makes it possible to determine the basic parameters of
the isotropic spectrum by automatic fitting.
3
Fig. 1. Scheme of the fuel cell for ESR: a, front projection;
b, sagittal projection; c, fluoroplastic tube. For clarification,
see the text.