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133
netic analyses indicate that the poor selectivities arise from
very high rates for propylene combustion (k3). It appears that
well-dispersed Cr species are not selective for propylene,
and that polymeric chromium oxides are preferred [33]. For
the nCrSiZr catalysts, an increase in the rate of propane
ODH (k1) and a decrease in the rate of propylene com-
bustion (k3) with increasing chromium content indicate that
different sites are at least partially responsible for these reac-
tions. Comparisons to previously reported Al2O3-supported
Cr catalysts synthesized via wet impregnation reveal that the
catalysts prepared here exhibit higher ODH activities, but
lower selectivities for propylene formation [33]. In addition,
comparisons of the Cr-based catalysts reported here with
previously reported V/Zr/O ODH catalysts synthesized via
thermolytic molecular precursor methods reveal that the cat-
alysts have comparable activities, but that selectivities for
propylene are superior for the vanadium-based species [30].
Propane DH reactions under mild conditions (723 K) us-
ing the nCrSiAl and nCrSiZr catalysts are characterized by
high selectivities at low propane conversions. The nCrSiZr
catalysts are generally more active than their nCrSiAl coun-
terparts. Lower Cr contents give rise to higher activities on
a per Cr basis, suggesting that isolated sites are preferred.
Detailed investigations using 2.5CrSiZr led to propane con-
versions greater than 35%, with propylene selectivities ap-
proaching 95%. These values are among the best reported
for propane DH catalysts, particularly at such a low reac-
tion temperature. Deactivation due to coking was observed
over the course of the reactions; however, calcination under
He/O2 at 773 K was effective for regeneration of the cata-
lysts. Therefore, for propane ODH, the best results seem to
be associated with chromate clusters, whereas for propane
DH, well-dispersed (and presumably isolated) chromium
species are most effective.
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Acknowledgments
We are grateful for the support of this work by the
Office of Basic Energy Sciences, Chemical Sciences Divi-
sion, of the US Department of Energy under Contract No.
DE-AC03-76SF00098. We also thank Prof. A. Stacy for the
use of instrumentation (PXRD, DRUV–vis), Dr. J. Male for
assistance with the XANES studies, and the Stanford Syn-
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