Water-Free Proton-Conducting Membranes for Fuel Cells
NASA’s Jet Propulsion Laboratory, Pasadena, California
Jun 30 2007
Page 2 of 2
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Each of these preparations was
brushed onto an open mat of glass
fibers. The coated mats were dried in
flowing air at a temperature of 60 °C for
about an hour. The coated mats were
further dried in a vacuum oven at 60 °C
to remove traces of water.
The thermal stability of P4VPBS was evaluated
by differential scanning calorimetry.
The results showed that P4VPBS undergoes
a glass transition at a temperature of
about 182 °C and that it melts at about
298.7 °C, with no evidence of decomposition.
These thermal properties are consistent
with the requirements for stability
under operating conditions in fuel cells.
Cell Potential vs. Current Density was measured in a test of an experimental membrane/electrode assembly in a hydrogen/oxygen fuel cell at a temperature of 183.5 °C.
The coated mats were tested to determine
their ionic conductivities and to
quantify their performances as membranes
in hydrogen/oxygen fuel cells.
The ionic conductivity of the mat coated
with the P4VPBS/silica composite was
slightly greater than that of the mat coated
with P4VPBS: this was expected
because the composite contains additional
molecular groups that are presumably
available for forming hydrogen
bonds. On the basis of the observed temperature
dependence of the conductivity,
the activation energy for conduction
was estimated to be about 0.1 eV, suggesting
hopping-type conduction through
hydrogen bonds. While the measured
conductivity values were two orders of
magnitude lower than desirable for fuelcell
applications, the degree of solid-state
proton conduction was the highest
observed thus far in polymeric salts. It is
anticipated that the polymer backbone
could be modified to facilitate formation
of hydrogen bonds to obtain more sites
for proton hopping and, hence, greater
proton conductivity.
In preparation for the tests of fuel-cell
performance, the coated mats were further
coated with catalytic anode and cathode
layers to form membrane/electrode
assemblies. No attempt was made to optimize
the catalytic layers. In the fuel-cell
tests, stable maximum cell potentials of
0.85 V were attained. The anticipated
maximum cell voltage was 1.0 V. The
decrease from the expected maximum
value was attributed to some crossover of
hydrogen and oxygen through the membranes.
The figure shows some of the
data from the fuel-cell test of the mat
coated with the P4VPBS/silica composite.
The power density indicated by these
data is low for a fuel cell operating at the
indicated temperature — presumably
because of the lack of optimization of the
catalyst layers. Nevertheless, the data suggest
that optimization of catalysts and
enhancement of conductivity should
make it possible to realize high-temperature
fuel cells.
This work was done by Sekharipuram
Narayanan and Shiao-Pin Yen of Caltech for
NASA’s Jet Propulsion Laboratory. For more
information, download the Technical
Support Package (free white paper) at
www.techbriefs.com/tsp under the Materials
category.
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the contractor has elected to retain title to this
invention. Inquiries concerning rights for its
commercial use should be addressed to:
Innovative Technology Assets Management
JPL
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Refer to NPO-30873, volume and number
of this NASA Tech Briefs issue, and the
page number.
This Brief includes a Technical Support Package (TSP).
Water-Free Proton-Conducting Membranes for Fuel Cells (reference NPO-30873) is currently available for download from the TSP library.
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