278
SNYTNIKOV et al.
The X-ray powder diffraction patterns of the cata-
[CO] – [CO]
2 [O2]0 – [O2]out
1
0
out
----------------------------------------
S =
× 100%,
lysts for phase analysis were recorded on a DRON–
Seifert-RM4 diffractometer (CuKα radiation, graphite
monochromator in the reflected beam, amplitude-dis-
crimination scintillation detector, 2θ = 5°–135°, scan-
ning with 0.02° increments). The data obtained were
compared to JCPDS standard data (electronic version
PCPDFWIN) [25]. The diffraction data were processed
using the PowderCel 2.4 program, which allowed the
phase composition, unit-cell parameters, and the coher-
ent-scattering domain size (D) to be determined.
where [CO]0 and [O2]0 are the inlet CO and O2 concen-
trations and [CO]out and [O2]out are the outlet CO and O2
concentrations.
RESULTS AND DISCUSSION
The oxidation of CO in hydrogen-containing mix-
tures was initially studied for the Co–Pt powder.
Figure 1 shows the temperature dependences of the
outlet CO concentration, O2 conversion, and selectivity
for this system.
For the initial oxygen concentration 1.5 vol %, the
outlet CO concentration is 300 ppm at 100–110°C, the
O2 conversion is 100%, and S is about 30%. Raising the
O2 concentration in the reaction mixture to 2.5 vol %
makes it possible to reduce [CO]out to <10 ppm at 100–
110°C. In this case, the oxygen conversion is again
complete, but the selectivity is decreased to ~20%.
Thus, the Co–Pt powder is an active catalyst for selec-
tive CO oxidation in hydrogen-containing mixtures.
The phase composition of the Co–Pt powder before
and after the selective oxidation of CO in the presence
of H2 was determined by X-ray diffraction. The diffrac-
tion patterns for this powder and for some Co–Pt solid
solutions and intermetallides are presented in Fig. 2.
The strongest reflections from the Co–Pt powder before
the reaction (diffraction pattern 1) are broad and are
assigned to the fcc lattice of the solid solution with a
unit-cell parameter of a = 3.771(2) Å. This unit-cell
parameter implies that the mean volume per atom of the
Kinetic measurements for CO oxidation in hydro-
gen-containing gas mixtures were detailed in an earlier
paper [9]. The reaction was carried out at atmospheric
pressure in a flow quartz reactor. The reactor was a U-
shaped tube with a length of 40 cm, an inner diameter
of 8 mm, and a wall thickness of ~1 mm and had a ther-
mocouple well with an outer diameter of 3 mm at its
central axis. A weighed portion of the catalyst (granule
diameter, ≤1 mm) or the Co–Pt powder mixed with
powdered quartz (particle size, ~1 mm) was charged
into the reactor. The total height of the catalyst bed was
12 cm. The reactor inlet and outlet were fitted with a fil-
ter to prevent the small catalyst particles entrained by
the flowing gas from entering the gas inlet and outlet
capillary piping. The reaction temperature was mea-
sured with a chromel–alumel thermocouple placed in
the center of the catalyst bed. The catalyst was given no
pretreatment before the experiment.
The reactant and product concentrations at the reac-
tor inlet and outlet were identified using a Kristall-2000
chromatograph (Russia) equipped with a thermal-con-
ductivity detector, a flame-ionization detector, and a solid solution is Vmean = 13.41 Å3. This value coincides
methanizer accessory using a nickel catalyst (NKM-4 closely with the half-sum of the atomic volumes of
cobalt and platinum (VCo = 11.02 Å3, VPt = 15.09 Å3).
Therefore, the main phase of the Co–Pt powder is the
Co0.5Pt0.5 solid solution. The coherent-scattering
domain size of this phase derived from diffraction pro-
files is 50–70 Å.
brand). The combination of the methanizer and the
flame-ionization detector allowed any hydrocarbon
present in the gas mixture along with CO and CO2 to be
quantified with high sensitivity. The gas mixture being
analyzed was separated in a column packed with the
molecular sieve NaX (for the thermal-conductivity
detector) or with Porapak Q (for the flame-ionization
detector). The sensitivity of this method makes possible
measurement of CO, CH4, and CO2 concentrations
Along with the strong reflections from the Co0.5Pt0.5
phase, weak superstructure peaks are present in the dif-
fraction pattern of the Co–Pt powder before the reac-
tion. These peaks occur in nearly the same positions as
the reflections from the CoPt intermetallide (tetragonal
lattice with a = 3.803 Å and c = 3.701 Å, according to
JCPDS file no. 43-1358) [25]. However, their low
intensity and the absence of tetragonal splitting suggest
only that the solid solution is incompletely ordered.
Note that the main reflections are asymmetric and
broadened on their small-angle side. This is explained
by the fact that the Co–Pt powder before the reaction
contains a small amount of a solid solution with a
higher platinum content.
down to ~10–4 vol % and é2 concentrations down to
10−3 vol %. The oxidation of carbon monoxide in
hydrogen-containing mixtures was characterized in
terms of CO conversion (Xëé), é2 conversion (XO ),
2
and selectivity (S), which were calculated using the
equations
[CO]0 – [CO]out
--------------------------------------
XCO
=
× 100%,
[CO]0
The profiles and intensities of all reflections from
the Co–Pt powder after the reaction (diffraction pattern 2)
are nearly the same as the reflection profiles and inten-
sities observed before the reaction. Note only that the
[O2]0 – [O2]out
-----------------------------------
[O2]0
XO
=
× 100%,
2
KINETICS AND CATALYSIS Vol. 48 No. 2 2007