Mechanism of the decomposition of the surface oxide film on polycrystalline palladium
The decomposition of thin surface oxide films on polycrystalline palladium Pd(poly) at 500–1300 K was investigated by mathematical modeling. This process was analyzed in terms of a model including O 2 desorption from the chemisorbed oxygen layer (O ads ) and the passage of oxygen inserted under the...
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Veröffentlicht in: | Kinetics and catalysis 2016-03, Vol.57 (2), p.263-275 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The decomposition of thin surface oxide films on polycrystalline palladium Pd(poly) at 500–1300 K was investigated by mathematical modeling. This process was analyzed in terms of a model including O
2
desorption from the chemisorbed oxygen layer (O
ads
) and the passage of oxygen inserted under the surface layer of the metal (O
abs
) and oxygen dissolved in metal subsurface layers (O
dis
) to the surface. O
2
desorption was modeled on a surface with a square lattice of adsorption sites, with account taken of the energy of the lateral repulsive interactions between adjacent O
ads
atoms (ε
aa
). At ε
aa
= 10 kJ/mol and when the activation energy of O
2
desorption for a chemisorbed-oxygen surface coverage of θ ≈ 0 is
E
des
0
= 230 kJ/mol, the calculated spectra are in agreement with the oxygen temperature-programmed desorption (TPD) spectra obtained for Pd(poly) at θ ≤ 0.5. The passage of O
abs
and O
dis
atoms to the surface was calculated using a first-order equation, with account taken of the activation energy for these atoms coming out to the surface (
E
2
and
E
3
, respectively). As the oxide film is heated, O
2
desorption is accompanied by the passage of O
abs
and then O
dis
to the surface, which leads to an increase in the O
ads
surface coverage and, accordingly, to a buildup of lateral surroundings in the adsorbed layer. Owing to this fact and to the repulsive interactions between O
ads
atoms, the bonds between O
ads
and the surface weaken and
E
des
decreases. As a consequence, the O
2
desorption rate increases and a low-temperature peak with
T
max
≈ 710 K, which is due to the passage of O
abs
atoms to the surface, and then a high-temperature peak with
T
max
≈ 770 K, which is due to the passage of O
dis
atoms to the surface, appear in the TPD spectrum. At ε
aa
= 10 kJ/mol,
E
des
0
= 230 kJ/mol,
E
2
= 145 kJ/mol, and
E
3
= 160 kJ/mol and when the number of inserted oxygen monolayers is θ
abs
≤ 0.3 and the number of oxygen monolayers dissolved in subsurface layers is θ
dis
≤ 10, the TPD spectra calculated for the given model are in agreement with the O
2
TPD spectra that are observed for Pd(poly) and are due to the decomposition of surface oxide films. |
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ISSN: | 0023-1584 1608-3210 |
DOI: | 10.1134/S0023158416020129 |