Catalytic and physico-chemical properties of La1−xSrxCoO3 perovskites
Descripción
React.
Kinet.
Catal.
Lett.,
Vol.
53, No.
I, 223-229
(1994)
RKCL2506 CATALYTIC
AND P H Y S I C O - C H E M I C A L Lal_xSrxCoO3
L.A. S.V.
Isupova,
Tsybulya,
V.A.
M.P.
Boreskov
Institute
+Ural
Received Accepted
properties
num cobaltites
was
with the cobalt composition
cently.
Their
related
properties
and catalytic tention appear oxides,
differs
in oxidation
to correlate
(HCI, HF,
action of complex
cor-
on the surface;
to the den-
was noted.
of the catalytic
S02)
LaMnO3,
and simple oxides
and phys ~
have been published
(up to 1600 K)
[1,2] attract much at-
LaFeO3,
of ABO 3 per-
LaNiO3,
for transition
nature
LaCrO 3 metal
of the catalytic
[3]. Nevertheless,
turned out to depend on both the nature
re-
to that for Pt and Pdto heating
The order of activity
a similar
(3)
Under our experimental
with the same trend
which m a y evidence
com-
activity
from the bulk one;
(comparable
reactions
lanthaof CO oxiIt
is proportional
defects.
to studies
to these compounds.
ovskites
concentration
high resistance
poisoning
Russia
structure.
catalytic
of perovskites
high activity
containlng'catalysts),
Russia
the data about chemical
no role of point defects
Many papers ico-chemical
620083,
and bulk defect
activity
sity of bulk extended conditions
630090,
of strontium-substituted
(I) the initial
the steady-state
Petrov +
February 15, 1994 March 28, 1994
of the surface
(2) surface
Rar,
A.N.
Lal_xSrxCOO 3 in the reaction
found that
relates
A.A.
Novosibirsk
Ekaterinburg
dation were compared w i t h position
Ivanov,
Kolomilchuk,
Kononchuk +
of Catalysis,
State University,
Catalytic
V.P.
V.N.
and O.F.
OF
PEROVSKITES
Sadykov,
Andrianova,
PROPERTIES
of B cations Akad4miai
activity and the
Kiadd,
Budapest
ISUPOVA et al.:
presence
PEROVSKITES
of substituting
cations
in A sublattice.
data on the effect
of the degree
very c o n t r a d i c t i n g
[4,5], which may be explained
ence of the perovskite activity
of lanthanum
preparation
Literature
substitution
technique
are
by the influ-
on their catalytic
[1,2].
The aim of this work was to study the catalytic ico-chemical elucidate
properties
the reasons
of Lal_xSrxCOO3
perovskites
for the conflicting
and physand to
literature
data.
EXPERIMENTAL As starting pure),
La203
procedure perform
materials
Co304
(99.9% purity)
with repeated
the syntheses.
(pure),
were used.
intermediate
SrCO 3 (chemically
The solid-state
grindings
The final annealing
ceramic
was used to
was carried
out at
1373 K. The catalytic determined
activity
in a p u l s e / f l o w
with a v i b r o f l u i d i z e d position
was
in CO oxidation installation,
catalyst
bed.
1% CO + 1% 02 in He.
that,
the samples
The initial mixture
were
subsequent
first
termine
the initial
action mixture was analyzed
catalytic
after treatment
com-
activity.
was admitted
Steady-state
of the sample
for 1-2 h. Composition
cooling
at to
flushed with a helium
stream and then a pulse of CO + 02 mixture
were m e a s u r e d
K was
Samples were pretreated
673 K in the stream of dry oxygen with 413 K. After
at 373-500
using a mieroreactor
activities
in the flow of re-
of the reaction
by using gas c h r o m a t o g r a p h y
to de-
(thermal
mixture
conductivity
detector). The surface
chemical
composition
was analyzed
method using MS-7201 mass-spectrometer. Ar + ion beam was prevent were
supported
the dependences exposure ondary
the current during
onto high purity
density
indium
foil.
of Co + , La +, Sr + secondary
of the incident
beam were measured.
of corresponding
- 10-20 ~A/cm 2. To
ion bombardent,
ion yields of Co, La, Sr cations
the ratios 224
4 keV,
sample charging
by the SIMS
The energy of incident
ion currents
the samples In the experiments,
ion currents
on the
The relative
were determined
sec-
from
after attainment
of
ISUPOVA
the c o n s t a n t reference)
values
and were
and 3.6,
X-ray
patterns
using CuK
carried
of the r e l a t i v e
[6].
nickel
filter
and an a m p l i t u d e
specific
thermal
RESULTS
20 = of
In these
surface
desorption
experiments
was
of e x t e n d e d
X-Ray CuK
determined
Scattering
radiation
a n a l y z e r were
de-
with
a
used.
by the BET m e t h o d
of Ar.
AND D I S C U S S I O N
Initial Sr c o n t e n t tivities over,
a URD-63
on the d e g r e e
densities
out by the S m a l l A n g l e
(SAXS)
The
with
The scan r e g i o n was
of cell p a r a m e t e r s
Method
using
i (chosen as
(x) for La was also d e t e r m i n e d .
An e v a l u a t i o n fects was
0.ii,
were obtained
radiation.
4 ~ - 30 ~ . The d e p e n d e n c e Sr s u b s t i t u t i o n
to be
PEROVSKITES
respectively.
diffraction
diffractometer
found
et al.:
catalytic
increases
change
initial
tionary
activities (Fig.
values.
These
facts
centers
the d e g r e e
of d e a c t i v a t i o n
similar,
changes
composition
some
stability
found
imply while
to i n c r e a s e
i), w h i l e
manner
(Fig.
higher
that e i t h e r attaining
of t h e
2-5).
acMore-
than the sta-
the n a t u r e
of
the s t e a d y - s t a t e
of the same c e n t e r s
of the surface.
as the
steady-state
i, c u r v e s
are c o n s i d e r a b l y
the a c t i v e
the c h e m i c a l
i, curve
in a c o m p l e x
activities
are
depends
Since
steady-state
curves
centers
or
upon 2-5 are
up to 400 K
can be i n f e r r e d . The SIMS tration
s t u d y has
shown
does not c o r r e l a t e
that:
with
(i) s u r f a c e
the b u l k one;
cobalt
concen-
(2) l a n t h a n u m
and s t r o n t i u m
concentrations
change
(3) in c h a r g e
balance
at x > 0.I some a c c u m u l a t i o n
point O-)
defects
occurs
since
stant c o b a l t slow growth
in the
serious
analysis
of l a n t h a n u m
(Fig.
has r e v e a l e d
structural
changes.
structure
for x > 0.4 the s t r u c t u r e
with
directions;
(anion v a c a n c i e s ,
is c l e a r l y
of Sr c o n c e n t r a t i o n
ite has a h e x a g o n a l while
layer
a sharp decline
concentration
The X - r a y causes
terms, surface
in o p p o s i t e
of
Co 4+ or
content
not c o m p e n s a t e d
at conby the
2). that
Thus,
strontium pure
addition
lanthanum
cobalt-
a = 5.44 and c = 13.091,
is cubic.
The s a m p l e s
with 225
ISUPOVA
et al.:
PEROVSKITES
12
10
8 84
!
o x
_
_ i"
I
0
I
0l
~
0.4
gm~
I
06
0.8
X
Fig.
i.
Dependence
o f the
steady-state
X = 0.3
and
as c u b i c type of ~des
C O / m 2 s)
on the
strontium
0.4
of
expansion
226
The most
transition
of
strong
increase the
i) a n d
activities
(W.
1 - 413 K;
transient hexagonal of
the
and
c a n be
(increase the
For
content
each
pro-
o f c for h e x a g o n a l increase
o f the
de-
of the perovskite
structure
would
SAXS
demonstrate
data
defined
distortions.
strontium
in a c h a n g e
Indeed,
2 - 373 K;
5 - 500 K
Therefore,
disordered
region.
K;
lattice
results
2-5)
content:
4 - 458
structures).
substitution
structure. the
with the
(curve
for L a l _ x S r x C O O 3 p e r o v s k i t e s
structurally
structures
a n d a for c u b i c gree
are
structure,
some
(curves
molec.
3 - 413 K;
initial
be e x p e c t e d
in
a distinct
ISUPOVA et al.:
PEROVSKITES
0.6 ~
0.4 (J
02
I
I
J
02
04
0.6
r
X
Fig.
2.
Surface
concentration
thanum
[C3 of cobalt
(2) and strontium
(i), lan-
(3) cations
for
Lal_xSrxCOO 3 system
~
40
E 2o 0
I
'1
I
i
0.2
0.4
0.6
0.8
X
Fig.
3.
Integral
intensity
tended defects
of the scattering
(I, relative
units)
on ex-
versus
x
for Lal_xSrxCoO 3 maximum
of the integral
defects
at x = 0.3-0.4
intensity (Fig.
of scattering
on extended
3).
227
ISUPOVA et al.: PEROVSKITES
Hence,
Lal_xSrxCOO 3 samples
(oxygen vacancies, and extended
defects
Figures
catalytic
activity
activity.
So, one can expect
decline
perovskites.
to the steady-state
seems to be p r i m a r i l y in the number
also b y b i o c k i n g
that the ini-
surface)
varies
isolated
active
If this
value
determined
cobalt
of
the cations
sites on the clear
is so, the activity
caused by reaction by surface
of Co3+ cations),
of the surface
di-
Any variations
at x > 0.i do not influence
as c a t a l y t i c a l l y
of oxidized
crease
reconstruction.
cobalt concentration.
surface
incorporation
I) suggest
(clean oxidized
concentrations
(Co 3+) to function
by strontium
i) and 2 (curve
as the surface
point defects
contain both point defects
generated
caused by structural
1 (curve
tial catalytic rectly
etc.)
media
reduction
possibly
by strongly
(de-
accompanied
adsorbed
car-
bonates. On the other hand, ty correlates curves
2-5 and Fig.
concentration importance
in steady
cations defects
state clusters upon
function
surface
reduction) sites.
centers
reactive
forms of CO and oxygen,
bonates
due to a smaller
cobalt
thus making type
resistent number
ions,
at outlets
The reason
[7,83.
By that
localized
of extended
for high activity of weakly
possible These
to blocking
of basic
the
catalysis.
one can expect
to be the coordination
nism of the L a n g m u i r - H i n s h e l w o o d to be more
[7,8],
i,
i) suggests
for steady-state
oxides
activi-
(Fig.
w i t h the surface
2, curve
of low-charged
as active appears
(Fig.
of these
also expected
and SAXS data
3) and does not correlate
the pure cobalt
(or appearing defects
fact that the steady-state
structural
of cobalt
of extended
analogy with
the
well with
bound
a mecha-
clusters
by surface
Sr cations
are car-
as nearest
neighbors. The results
obtained
allow to explain
data on the effect of substitution for lanthanum. uncertainty
First, state).
caused by preparation
228
of alkaline
the discrepancies
in the conditions
or non-steady
Second,
the contradicting
of activity
measurements
an essential
procedure
earth cations
can be ascribed
determining
influence
to the (steady
may be
the bulk defect
ISUPOVA et al.: PEROVSKITES
structure and, hence,
the density of surface active centers
in
steady-state conditions.
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229
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