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Smirnov et al.
tion of all the substances under study coincide within the
experimental error with those obtained for the pure supꢀ
port. Thus, the nickel itself does not compete with the
support for sites of hydrocarbon adsorption. However,
being added into the composition of the mixed particles
(Au + Ni), nickel favors, most likely, the formation of
additional defects, which activate gold atoms. A possibilꢀ
ity of similar activation is indicated by literature data21 on
the bimetallic nanoparticles.
Let us attempt to compare the strength of adsorption
with the catalytic activity of the M/γꢀAl2O3 samples in
transformations of the corresponding unsaturated subꢀ
strates.
M = Au, Ni, Au + Ni; R = Ph, nꢀC5H11
Gold nanoparticles supported in approximately equal
amounts by the methods of anionic adsorption and metal
vapor synthesis possess similar adsorption properties. For
instance, the heats of adsorption on the catalysts, which
were obtained by anionic adsorption (0.4 wt.% Au) and
metal vapor synthesis (0.55 wt.% Au), are virtually
the same.
The heat of adsorption of allylbenzene on γꢀAl2O3,
which is catalytically inactive in reactions (1) and (2),
equals 51 kJ mol–1. The same values within the measureꢀ
ment error were obtained for Ni/γꢀAl2O3, which is also
catalytically inactive in these reactions. The increase in
the heat of adsorption of allylbenzene on all monoꢀ and
The heats of adsorption of alkanes on pure alumina
are somewhat lower than the published values.15,16 For
example, Q(nꢀC7H16) on γꢀAl2O3 is 32 kJ mol–1 (see
Table 1). The heats of adsorption of nꢀheptane on γꢀAl2O3
calculated from published data using extrapolation by the
additive scheme17 are 43.1 15 and 46.4 kJ mol–1 16
.
bimetallic goldꢀcontaining systems above 51 kJ mol–1
,
The data on adsorption of substances of other classes
agree with the known adsorption properties of γꢀAl2O3.
An increase in the basicity of the molecules upon the
introduction of alkyl or alkenyl substituents into the aroꢀ
matic ring determines a stronger adsorption of toluene
and allylbenzene as compared with unsubstituted benꢀ
zene. The lower (compared to that of octane) heat of
adsorption is caused by steric hindrance created by alkyl
substituents, which decrease the number of effective conꢀ
tacts of the methylene groups of alkane with active adꢀ
sorption sites of the surface.18,19
induces a measurable catalytic activity of these samples in
reactions (1) and (2). This activity changes in parallel to
the heat (see Table 1). A similar change in the catalytic
activity of M/γꢀAl2O3 (M = Au, Au + Ni) in the addition
of CCl4 to the multiple bond of C8H16 at different heats of
olefin adsorption is also observed for octꢀ1ꢀene.
Thus, the heats of adsorption can serve as indicators
of the activity of the goldꢀcontaining systems in the proꢀ
cesses including the step of activation of unsaturated comꢀ
pounds by the interaction with the metal.
Gold immobilization exerts no effect on the heats of
adsorption of chlorohydrocarbons, benzene, and toluene
but increases the heats for sorbates with long alkyl or
alkenyl groups, viz., alkanes, olefins, and isooctane (see
Table 1). Thus, the increase in the heat of adsorption
(∆Q), when small gold nanoparticles (average diameter
3 nm) appear on the support surface, is equal to 24, 23,
and 23 kJ mol–1 for hexane, heptane, and octane, respecꢀ
tively. For octꢀ1ꢀene containing both the methylene chain
and double bond, ∆Q = 36 kJ mol–1. The effect ∆Q of
alkanes is low for the samples with relatively large gold
crystallites (average diameter 23 nm). The probable exꢀ
planation of different adsorptions of alkanes on the
nanoparticles of different size is that the strong interacꢀ
tion between the metal and hydrocarbons occurs only
with special, coordinatively unsaturated metallic sites (verꢀ
tices, edges, cracks, and other "roughness").20 Undoubtꢀ
edly, the smaller is the size of the nanocluster, the higher
is the fraction of such strongly nonequilibrated areas on
the nanocluster surface .
The authors are grateful to the Ministry of Education
and Science of the Russian Federation for help in the
creation of the necessary instrumental basis for the work.
This work was financially supported by the Russian
Foundation for Basic Research (Project No. 05ꢀ03ꢀ33065)
and the Council on Grants of the President of the Russian
Federation (Program of State Support for the Leading
Scientific Schools of the Russian Federation, Grant
NSh 1275.2003.3).
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