Communications
dize H . For CO oxidation in the presence of H , the TOF for CO
2
2
À2 À1
conversion was only 0.610
s
at 110 8C. Relative to that on
Pd/Al O , the TOF on CU-PdCl /Al O is almost 30-fold lower
2
3
x
2
3
under the same conditions. This inhibition indicates that it is
difficult to oxidize CO over CU-PdCl /Al O . On the basis of the
x
2
3
Arrhenius plots (Figure S5), we calculated the apparent activa-
tion energies (E ) of the CU-PdCl /Al O and Pd/Al O catalysts.
a
x
2
3
2
3
À1
The E value of 38.6 kJmol over CU-PdCl /Al O is one order
a
x
2
À1
3
of magnitude higher than that of 3.8 kJmol over Pd/Al O3
2
for CO oxidation. The high activation barrier of CU-PdCl /Al O
3
x
2
correlates well with its efficient inhibition of CO oxidation and
outstanding selectivity towards H oxidation.
2
Previous studies illustrated that the presence of CO usually
[
10,11]
has a negative effect on reactions in which H is involved.
2
To investigate the influence of a high concentration of CO on
the PrOx of H , we tested the adsorption behavior of the cata-
2
lysts by static chemisorption. In the individual tests, Table S2
shows that the adsorption of both H and CO on Pd/Al O is
2
2
3
more facile than on CU-PdCl /Al O . Relative to the amount of
x
2
3
CO adsorbed without competition of H , the amount of CO ad-
2
sorbed slightly decreased on both CU-PdCl /Al O (from 24.5 to
x
2
3
À1
À1
1
8.8 mmolg ) and Pd/Al O (from 43 to 34.6 mmolg ) after H
2 3 2
preadsorption. With a reverse order of CO/H adsorption, how-
2
ever, the behavior of these two catalysts was very different.
After CO preadsorption, a significant decrease (from 24.6 to
À1
5
.9 mmolg ) in the amount of H adsorbed was observed on
2
2
Figure 2. a) XANES spectra and b) k -weighted Fourier transform Pd K-edge
EXAFS spectra of the standard PdCl power (A), PdCl /Al (B), CU-PdCl
Al (C), Pd/Al (D), and standard Pd foil (E).
Pd/Al O . This indicates that a strong interaction between CO
2
3
2
2
2
O
3
x
/
and the Pd sites is established on Pd/Al O , and then the ad-
2
3
2
O
3
2 3
O
sorption of H is blocked. On the contrary, only a small de-
2
À1
crease (from 14.3 to13 mmolg ) in the amount of H adsorbed
2
was found on CU-PdCl /Al O . The coordination of Cl around
suggests that the PdÀCl bond increases in length as the
amount of excess Cl decreases and the configuration of PdClx
becomes coordinatively unsaturated. Besides that, no PdÀPd
bond can be detected in CU-PdCl /Al O , and consequently, no
x
2
3
the Pd sites should be responsible for this result, as this tends
to deplete backdonation from the d bands of Pd to the anti-
[12]
bonding 2p* orbitals of CO. Thus, the interaction between
x
2
3
CO and Pd is weakened. Such fragile adsorption of CO on the
metallic Pd particles are formed.
catalyst makes CO labile and commutable by H . Finally, the
Notably, the E values acquired from the Arrhenius plots are
2
a
adsorption gap between CO and H can be minimized over
apparent in that the diffusional effect was not eliminated;
therefore, an intrinsic investigation about the behavior of the
catalysts is essential. DFT calculations were performed to ex-
plore the inhibitory mechanisms of CO oxidation over the
PdCl structure. The chosen Pd (111) surface of Pd/Al O and
2
CU-PdCl /Al O by deliberately restricting access to CO, and
x
2
3
then the opportunity for H is maximized.
2
Both the electronic properties and the short-range local
structures of the discussed catalysts were determined from the
extended X-ray absorption fine structure (EXAFS) spectra and
X-ray absorption near-edge structure (XANES) spectra of the
Pd K-edge. As shown in Figure 2a, the XANES curve of PdCl2/
Al O fits well with the standard PdCl sample, but a slight de-
x
2
3
the defective PdCl (140) surface of CU-PdCl /Al O were iden-
x
x
2
3
tified through characterization by high-resolution transmission
electron microscopy, X-ray absorption fine structure, and X-ray
photoelectron spectroscopy (see Section S6 in the Supporting
Information). The comparable energetic landscapes of all the
pathways for CO oxidation on the surfaces are depicted in
Schemes S2 and S3. We propose two mechanisms for CO oxi-
2
3
2
viation is found in CU-PdCl /Al O , which suggests that the
x
2
3
local electron density of Pd increases as the coordination of
electron-withdrawing Cl becomes unsaturated. This verifies
that the intrinsic structure of PdCl is not intact. In contrast,
dation depending on whether H is involved or not.
x
2
the curve of Pd/Al O shows two metallic peaks at energies of
On Pd (111), pathway I is illustrated by a redox mechanism
2
3
[
13]
approximately 24367 and 24391 eV. These features are identi-
cal to those of a standard Pd foil sample.
in which H is only a spectator. As shown in Figure 3, ad-
2
sorbed CO* is directly attacked by O to yield a carbonate in-
2
2
The curves of the Fourier-transformed k -weighted Pd K-
termediate (CO *) with a barrier of 1.66 eV via transition state 1
3
edge EXAFS are shown in Figure 2b. The PdÀCl coordination
number (CN) of CU-PdCl /Al O (3.3Æ0.4) is markedly lower
(TS1), and it then decomposes to CO and O* via TS2. CO is
2
2
readily desorbed from the Pd surface and O* approaches an-
other adsorbed CO* species to produce another molecule of
x
2
3
than that of the standard PdCl sample and that of PdCl /Al O
3
2
2
2
(
5.3Æ0.9), and the PdÀCl distance (R) of PdCl is smaller, which
CO via TS3. Differing in the adsorption modes, other similar
x
2
ChemCatChem 2016, 8, 1909 – 1914
1911
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