4
12
CHZHU et al.
particles of supported platinum, which, on the one defects in palladium crystallites, etc. [16]. We com-
hand, leads to the stabilization of the high dispersity pared palladium–aluminum catalysts calcined at the
and, on the other hand, to a decrease in the TON same temperature, but with different dispersities,
because of the enhanced deficiency of electron density
on the surface palladium atoms.
obtained by varying the concentration of palladium in
the catalysts.
The same but more pronounced trend is seen for pal-
ladium catalysts supported on pure modifying oxides in
the reaction of the complete oxidation of methane
It was found (Table 1) that for 1 and 2% palladium-
alumina catalysts calcined at 500°ë, an increase in the
concentration of palladium from 1 to 2 wt % leads to a
an increase in the average size of particles by a factor of
(Table 1), with the exception of palladium supported on
monoclinic ZrO for which the TON is the highest.
2
2
.2, and the TON decreases by a factor of 2.6. Proceed-
Thus, for methane oxidation, the TON decreases in the
ing from these data, we conclude that an increase in the
size of the supported palladium particles leads to an
increase in the TON. The explanation for such an effect
of particles size on the TON can be a hypothesis of a
decrease in the acceptor effect of the support on the
crystallites of supported palladium with an increase in
their size. On the other hand, the smaller the crystal-
lites, the more pronounced the acceptor effect of sup-
series: (Pd/ZrO , T
= 750°C
(Pd/Al O )
(Pd/CeO ) (2 wt % Pd).
2
2
calcin
2 3
(
Pd/ZrO , T
= 500°C)
2
calcin
For the 1 wt % palladium–alumina catalyst modified
by rare-earth element oxides and ZrO , the TON in the
2
complete oxidation of n-pentane decreases in the
series: (Pd/Al O )
(Pd/Al O –ZrO )
(Pd/Al O –CeO ).
2 3 2
2
3
2 3 2
(
Pd/Al O –La O )
2
3
2
3
A similar dependence of the TON on the nature of the port leading to the deficiency in the electron density on
modifier for platinum–alumina catalyst in the reaction of Pd(Pt) atoms, that is, to an increase in the oxidation
complete oxidation of n-butane was reported in [14].
state. At the same time, according to [17], the activation
As mentioned above, an increase in the TON in the of hydrocarbon molecules is determined by the concen-
reaction of the complete oxidation of hydrocarbons tration of the electron density on the active sites to be
with an increase in the metal particles size was noted by transferred to the antibonding orbital of the C–H bond.
many researchers. This was observed not only in the
An analysis of the data in Table 1 shows that, the
case of the aging of platinum-alumina and palladium–
concentration of palladium being the same and the dis-
persities being close, the TON is largely determined by
the nature of the supporting oxide; the stronger the
alumina samples in the reaction mixture at high temper-
atures [1, 2] but also upon sample calcination in air at
5
00–(850°C) 900°C (for platinum and palladium sup-
ported on Al O , ZrO , and SiO –Al O ) [6, 13]. For metal–support interaction the lower the TON.
2
3
2
2
2
3
the systems Pd/Al O and Pd/ZrO , an increase in the
2
3
2
Considerable changes are observed after calcination
at 600°C (Fig. 3a). As mentioned above, noncoherent
boundaries are formed by sintered species, which point
to the strong distortion in the particle structure, whereas
isolated particles are well ordered and cut. It is probable
that due to the strong interaction, the fragments of the
modifying oxide move together with the palladium par-
ticles interacting with them at an elevated temperature,
and do not allow the palladium particles to sinter. This
explains the existence of noncoherent boundaries
TON was also noted with an increase in the reaction
time [5].
It is quite possible that an increase in the TON (and
the specific catalytic activity) could be due to the
removal of admixtures from the catalysts during their
calcination in air or in the course of catalyst aging in the
reaction medium. Thus, it was shown in [15] that, when
the palladium catalyst supported on the lanthanum
oxide is prepared from H PdCl , the catalyst activity
2
4
increases for about 10 h in the reaction of n-butane oxi-
dation until it becomes constant due to the removal of between sintered particles. The existence of such struc-
the chloride ions that stabilize the palladium in the oxi- tural barriers stabilizes the dispersity of supported pal-
dized electron-deficient inactive state.
ladium and its activity.
The addition of a modifier stabilizes the dispersity
of palladium in the studied range of calcination temper-
atures (500–700°C), and this fact suggests that there is
an effect of dispersity on the TON of supported palla-
dium. On the other hand, a change in the dispersity with
an increase in the calcination temperature for the non-
modified palladium–alumina catalyst creates uncer-
tainties in the interpretation of the relationship between
the TON and dispersity because at elevated tempera-
tures, the processes of particle sintering and their
Thus, in this work we showed that, for palladium
catalysts supported on various oxides, the effect of ther-
mal activation (an increase in the TON of palladium
with an increase in the calcination temperature of the
samples from 500 to 700°C) is not observed in contrast
to supported platinum catalysts [9]. A comparison of
two palladium-alumina catalysts calcined at 500°C,
differing in the concentration of palladium and its dis-
persity shows that the TON of palladium is much higher
restructuring may occur: for instance, a decrease in the for palladium with a lower dispersity. All other condi-
fraction of a cluster and monatomic states of palladium tions being the same, the TON of supported palladium
on the support surface, a change in the structure of is determined by the support nature.
KINETICS AND CATALYSIS Vol. 45 No. 3 2004