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Lisachenko1983 ozone Al2O3

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React. Kinet. Catal. Lett., Vol. 23, Nos 1-2, 95-98 (1983)
INTERACTION OF OZONE WITH 7-A1203
SURFACE
A. O. Klimovskii, A. V. Bavin, V. S. Tkalich and A. A. Lisachenko
Institute of Physics, State Unversity, Leningrad, USSR
Received November 1, 1982
Accepted January 13, 1982
When contacting with dispersed ,y-A12 O~, ozone molecules were found to dissociate
with the efficiency r/ ~ 10 -4 . The reaction is accompanied by luminescence in the
350 ~ h ~< 600 nm region. Atwo-step model of the process is suggested implying the
occupation of surface sites by atomic oxygen and their subsequent regeneration.
HpH KOHTaKTe C g2elcIlepcHoi~l 3,-A120 a O3OH pacna~aeTca
c
aqbqbeKTl,
IBItocrhlO
n ~ 10 -4 9Peaxuna conpoBo~/~aeTc~I3nOMHHeCReHILqe!~IB o6JIac'rn350 ~<X~<600 HM.
Ilpe~nonaraeTcz nayxcra~m~Ha~ cxeMa npot~ecca, Bxmona~omaa nocne~oBaTen~qo
zanonnenne aTOMapHbIMKrIcnopo~oMH pereHepatteao noBepxHocTm,IXttenTpOB.
Studies on the mechanism of heterogeneous reactions of ozone are of great interest due to their possible role in the ozone balance in the upper layers of the
atmosphere /1/, the extremely high oxidizability of ozone and the necessity to
develop methods for the catalytic purification of gases from ozone admixtures.
Here we describe results on ozone decomposition over 3,-A1203 obtained by
several methods including manometry, mass- and thermal desorption spectroscopy
(TDS) and luminescence of the surface species.
EXPERIMENTAL
A stainless steel reactor was used equipped with a Pirani pressure gauge
(10 -3 N/m s sensitivity towards O2), a MX 1303 mass spectrometer, a photometric ozone pressure cell (1013 mol/cm 3 sensitivity), a programmed heating
device, a UV irradiation source and a luminescent measurement system. The experiment was aided by a D 3 - 2 8 computer.
130 mg batch of ~'-A1203 (S ~" 100 mS/g) was pretreated in 02 (5 N/m s)
at 850 K for 30 h and irradiated simultaneously with the UV irradiation of a
Hg-lamp. Ozone was produced by a microwave discharge in pure oxygen and then
distilled twice at 183 K.
95
KLIMOVSKII et al.: INTERACTION OF OZONE
RESULTS
Changes in the ozone concentration when contacting with the 7-A12Oa sample
are illustrated in Fig. 1 (curve 1). Taking the surface area of the sample to be
equal to the geometrical one, the portion of the active (i.e. resulting in ozone decomposition) collisions with the surface at 293 K is 10 -4. In the 1013 ~< [03] <~
~< 3 • 10 is molec 9 cm -3 region the ozone concentration decreases exponentially
with a simultaneous increase in the pressure of molecular oxygen (Fig. 1, curve 2).
Part of the oxygen molecules remains in the adsorbed state. The analysis of the
adsorbed phase indicates that the thermal desorption spectra of O2 after ozone
decomposition (Fig. 2, curve 3) differs from those of chemisorption (curve 1) or
photoadsorption (curve 2) of molecular oxygen in the total coverage and the much
P
tP
greater relative population of the phases at Tmax ~ 550 and Tmax ~ 715 K. The
high-temperature phases are generally ascribed to the dissociated species of o x y g e n / 2 /
It has been established that the admission of ozone to the sample leads to a flash
emission in the 350 ~< X ~< 600 nm region. This effect is partly reproduced if a new
doze of ozone is admitted, but for its complete restoration, heating at T/> 750 K
under high vacuum is necessary.
The estimated quantum yield was found to be not less than 10 -6 per one ozone
molecule dissociated.
Besides the short-time flash of luminescence (several seconds), a slowly decreasing (10 3 S) light emission was detected whose intensity sharply increases after the
evacuation of oxygen (Fig. 1, curve 3). This emission is accompained by Oxygen (O2) desorption.
Pumping-out
~
r-=
8
*03
~
//2 " " "
&
E
U
m
To
2
O
I
/~0
80
&O0
t (s)
800
1200
Fig. 1. Kinetics of the interaction of ozone with 7-AI~ O~: ozone concentration (1), oxygen
concentration (2), luminescence intensity (3)
96
KLIMOVSKII et al.: INTERACTION OF OZONE
r
2]
>
~5
3
7~
\
Z
"U
I
300
~.00
500
600
700
800
T I~()
Fig. 2. Thermal desorption of molecular oxygen: after chemisorption of molecular oxygen:
after ehemisorption of 02 (1), photoadsorption of 02 (2) and adsorption of 03 (3)
DISCUSSION
A two-step scheme of heterogeneous decomposition of ozone /3/ is:
o~ + ( ) ~ ( o )
+ o~
(1)
O3 +(o) K~ 202 + ( )
(2)
where ( ) are the active surface centers. Reaction (2) is supposed to be the ratedetermining step. On oxide surfaces, active sites can be the anion vacancies. The
analysis indicates that this scheme accounts for the kinetic peculiarities of the ozone
decomposition and the formation of high-temperature maxima in the thermal desorption spectra after contact with Oa. It can also account for the observed flash
luminescence. Actually, protons can be emitted after the insertion of atomic oxygen into the surface either directly by the transition complex or due to the surface defect, which consumed the released energy.
In order to explain the slowly decreasing light emission one must suppose that
the (O) centers are mobile enough to recombine via the scheme:
(0) + (0) K~ 2( ) + 0= + hz,
7
(3)
97
KLIMOVSKIIet al.: INTERACTIONOF OZONE
This reaction can also account for the desorption of 02. The quenching effect
of oxygen might be attributed to the blocking of emitting centers with the formation of three-atomic surface complexes, whose existence was reported in several
works/2/.
REFERENCES
1. R. D. Cadle, P. Crutzen, D. Enhalt: J. Geophys. Res., 80, 3381 (1975).
2. K. N. Spixidonov,O. V. Krylov: in Probl. Kinet. Katal., 16, 21 (1975).
3. G. I. Golodets: HeterogeneousCatalytic Reactions InvolvingMolecular Oxygen, Kiev 1977.
0
98
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