D.P. Sobczyk et al. / Journal of Catalysis 219 (2003) 156–166
157
3
the OH species is the rate-determining step. These species
have also been detected at the platinum surfaces under UHV
conditions [1].
was then flushed with He (48 cm /min) for 20 min before
the reaction temperature was set.
A preoxidized platinum sponge is obtained by the fol-
lowing treatment: the reduced catalyst was pretreated with
1 vol% O /He flow (48 cm /min) for 1 h at 373 K followed
A suitable technique to study in situ transient and steady-
state phenomena at atmospheric pressure is positron emis-
sion profiling [19,20]. The PEP measurements offer a unique
possibility of studing the various processes at the catalyst
surface in a wide temperature range. PEP is a technique
3
2
3
by flushing with He (48 cm /min) for 1 h before the reaction
1
5
temperature was set. Additional [ O]O2 PEP experiments
indicated (not shown) that on preoxidized platinum sponge
oxygen is strongly bound and that oxygen adsorbs dissocia-
tively at this temperature, which is in line with earlier reports
−
15
in which minute (∼ 10
mol) quantities of radiolabeled
molecules emitting positrons are injected as pulses into the
feed of packed-bed reactors. The concentration distribution
of radiolabeled molecules can be measured as a function of
[
21–25].
time and position within a tubular reactor bed. In this study
we used 13N-labeled ammonia pulses.
2.2. Positron emission profiling
In this work, evidence for the activation of the ammo-
nia adsorption and dissociation promoted by oxygen on
platinum is provided by PEP pulse experiments. The con-
The 13N nucleus emits a positron upon decay. Positron
emission profiling is based on the detection of the two
1
3
version and product formation due to [ N]NH3 pulses on
preoxidized platinum have been studied as a function of
temperature. Here, we will demonstrate that the product se-
lectivity is temperature dependent and that a part of the
5
11 keV gamma photons which originate from the annihi-
lation of this positron with an electron. These two 511 keV
gamma photons are simultaneously emitted in opposite di-
rections and they travel typically a few centimeters in solid
matters. Coincidental detection of two photons by scintilla-
tion detectors (BGO) provides the position of the annihila-
tion. In practice, the tubular reactor is horizontally placed
between two arrays (upper and lower) of nine scintillation
detectors. In both arrays the detectors were tightly placed,
which results in the spatial resolution of 2.9 mm. The av-
erage concentration of all radiolabeled molecules within a
certain volume (length 2.9 mm) is measured at time inter-
vals of 0.5 s. The measurement of radiolabeled molecules
is simultaneous over the total detection length (5 cm), thus
within the 17 vol segments. In this way the concentration
distribution of the positron emitting molecules can be mea-
sured as a function of position and time [19,29].
1
3
injected [ N]NH3 remains at the preoxidized platinum sur-
face. In addition, the nature of the nitrogen species, which
remain after the ammonia pulse on preoxidized platinum
in the temperature range up to 423 K, is further investi-
gated with temperature-programmed desorption (TPD) and
temperature-programmed oxidation (TPO), and the removal
of the adsorbed species by H2, NH3, and NO reaction exper-
iments. Furthermore, we discuss the possible role of NO as
a reaction intermediate.
2
. Experimental
2
.1. Catalytic reactor
The Eindhoven 30 MeV cyclotron was used to irradi-
ate a water target with highly energetic protons of 16 MeV.
The irradiation time was 10 min and a typical beam cur-
rent of 500 nA was used. The target was a flowthrough
water target, with a total volume of 7 ml containing a dual
foil (Duratherm 600, thickness 15 µm). In this way formed
The platinum sponge was acquired from Johnson Mattey.
The sponge sample was of > 99.9% purity. The particle size
of the sponge was between 250 and 350 µm and the size of
the small non porous particles about 1.0–5.0 µm [18]. The
amount of platinum sites calculated via BET measurement
1
3
13
1
8
[ N]nitrate and [ N]nitrite were subsequently reduced to
is 3.0 × 10 sites/g and via the hydrogen chemisorption is
1
3
1
8
3
NH , using DeVarda’s alloy method [26,27]. The produc-
1
0
.3×10 sites/g. The metal surface area is determined to be
1
3
2
tion method of gaseous pulses of [ N]NH was described
3
.099 m /g. Atmospheric ammonia oxidation activity tests
elsewhere [28]. A pulse time of 10 s was used to inject a
were performed in a fixed-bed reactor setup equipped with
a quadrupole mass spectrometer (Balzers Instruments Om-
nistar GSD 3000), which was calibrated for on-line analysis
of reactants and products. A quartz tube with an internal di-
ameter of 4 mm was used as reactor. A sample of 1.8 g of
pure platinum sponge was used in a catalytic bed with a
length of 4.0 cm. The experiments were done at tempera-
tures between 323 and 673 K.
mix of 13NH3/ NH3 into the reactant stream, henceforth
14
1
3
14
−5
indicated as [ N]NH3. In this way NH3 (∼ 10 mol)
1
3
was measured with the mass spectrometer and NH3
−15
13
(
∼ 10
mol) was monitored with PEP. Since the NH3
concentration varies in each pulse, the absolute concentra-
tion of radiolabeled molecules in the various experiments
cannot be directly compared. However, the labeled species
are either introduced in a large flow of nonlabeled ammonia
or as trace amounts in ammonia-free flows. As such, these
variations will not affect the results between the various ex-
periments.
Prior to a catalytic experiment the platinum sponge was
reduced in situ by heating the sample in a 10 vol% H2/He
3
flow (40 cm /min) from 298 to 673 K. Subsequently the
sample was kept at this temperature for 2 h. The catalyst