To understand the polarization loss due to poisoning by
CO
of a porous Pt anode under various conditions, poisoning losses have been measured in a half‐cell in the temperature range 110°–190°C in 100 weight percent
H3PO4
for various mixtures of
H2
,
CO
, and
CO2
gases. At a fixed current density, the poisoning loss,
normalΔVnormalpois
, was observed to vary linearly with ln
false[COfalse]/false[H2false]
. Deviation from linearity was observed at lower temperatures and higher current densities for high
false[COfalse]/false[H2false]
ratios. Considering only the linear portions, it has been possible to derive a general relationship for
normalΔVnormalpois
with temperature,
CO
concentration, and current density. The surface coverage by
CO
was calculated at various temperatures and was found to bear a linear relationship with ln
false[COfalse]/false[H2false]
. From the experimental Temkin isotherms, a general adsorption relationship has been obtained. The standard free energies for
CO
adsorption were calculated and were found to vary from −14.5 to −12.1 kcal/mol in the temperature range 130°–190°C. The standard entropy for
CO
adsorption was calculated to be −39 cal/mol K. Interpretations of the data indicate that
CO
adsorption occurs through 1:1 replacement of H by
CO
through the process of selective site poisoning. Under conditions where a nonlinearity in the poisoning relationship occurs,
CO
molecules undergo some orientation, favored by the increasing positive charges on the Pt surface.
A study was undertaken to measure polarization losses due to the presence of
CO2
and
CO
in the
H2
fuel for a practical fuel cell Pt/C anode. A porous Pt anode (0.3 mg/cm2 Pt) was tested as a floating electrode in a half‐cell assembly to measure performance in 100 weight percent
H3PO4
at 190°C in presence of
H2
, and
H2
,
CO2
, and
CO
gas mixtures. The additional polarization loss over that of
H2
due to
CO2
dilution followed closely the expected loss from the Nernst equation in the range of current density 0–300 mA/cm2. The combined loss due to poisoning by
CO
and the dilution by
CO
and
CO2
was analyzed and found to be additive of the poisoning and dilution losses. The poisoning loss by
CO
was calculated by subtracting the dilution loss from the combined dilution and poisoning loss. Such data were found to be linearly dependent on the logarithm of
false[COfalse]/false[H2false]
ratio. This is consistent with
CO
poisoning by replacement of
H2
sites on the porous Pt electrode. The calculated values of surface coverage by
CO
ranged from 0.089 to 0.31 as the ratio
false[COfalse]/false[H2false]
varied from 0.01 to 0.025. The values of surface coverage were consistent with the dual site elimination model for the replacement of
H2
by
CO
molecules. The exchange current densities for
H2
oxidation varied from 309 to 142 mA/cm2 as the ratio
false[COfalse]/false[H2false]
changed from 0 to 0.025. By comparing the experimental isotherm for
CO
adsorption with the Temkin isotherm, the interaction parameter was calculated to be 3.83 kcal/mol, and the standard free energy of adsorption, −10.96 kcal/mol. The latter value indicated an adsorption of
CO
which is comparable to
H2
.
The polarization of a fuel cell Pt/ Canode has been mearsured under conditions similar to that of an operating fuel cell at atmospheric pressure (100 Wt.‐% H3PO4, 190°C) in the presence of H2 and mixtures of H2, CO2, and CO.
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