W. Deng et al.
Applied Catalysis A, General 624 (2021) 118300
ray diffraction (XRD) and Raman spectra. The morphology and ele-
3. Results and discussions
ments’ distribution was observed using scanning electron microscopy
(
FE-SEM), scanning transmission electron microscopy (FE-S/TEM),
3.1. Characterization of catalysts
transmission electron microscopy (HR-TEM), and EDS mapping. The
surface component and oxidation state were analyzed by X-ray photo-
XRD patterns of the as-synthesized precursor are shown in Fig. S1,
whose diffraction peaks could be indexed to a structure of Co(OH)
electron spectra (XPS). N
2
adsorption-desorption experiments were
carried out to obtain the specific surface area, pore size, and pore vol-
ume of the catalysts. The redox and acidic properties of catalysts were
(OCH
cation of acetate ligands driven by heating in the presence of methanol
reaction of Co(CH COO) O → Co(OH)(OCH ) + CH CO CH
+ CH
O occurred during the solvothermal process and plate-like Co(OH)
OCH ) formed [32]. Moreover, the yield of the products was close to
100 % (as the residue solutions were colorless). As evidenced in Fig. S1
and Fig. S2, XRD patterns indicated that a spinel structure of Co
(JCPDS No. 42-1467) was obtained after calcination [33]. After loading
RuO species, the crystal phase of Co was not obviously affected. The
phases corresponding to RuO
3
) according to Zhu’s report [31]. As described, a typical esterifi-
studied by H
2
-TPR and NH
3
-TPD, respectively. More details could be
3
2
3
3
3
2
3
+
found in our previous report [24].
H
2
(
3
2
.3. Activity test
3 4
O
Catalytic activities of catalysts for VOCs oxidation were tested in a
quartz tube reactor with an inner diameter of 4 mm at atmospheric
pressure. Feed stream was prepared by delivering liquid VOCs (1, 2-DCE
or toluene) with a syringe pump (KDS 100, USA) and propane standard
gas (metered by a mass flow controller) at a given concentration into a
x
3 4
O
x
species were not detected due to their
◦
high dispersion (Fig. 1A). However, the diffraction peak at 36.9 shifted
to the lower angle (Fig. 1A, inset), which was an indication of the doping
of Ru3
+/4+
species into the octahedron centers of the Co
O
spinel
+/4+
(0.68 and 0.62 Å) was larger
dry gas mixture composed of 10 % O
2
and N
2
balance. The injection part
3
4
3
was electrically heated to ensure complete evaporation of liquid 1, 2-
structure because the ionic ratio of Ru
than Co3 (0.61 Å) and led to the lattice expansion [34]. Meanwhile, the
+
DCE or toluene, and 100 mg of catalyst (40–60 mesh) was used
ꢀ 1
ꢀ 1
h ). The effects of GHSV on 1, 2-DCE con-
(
GHSV was 60,000 mL g
lattice parameter of Co
3
O
4
increased from 8.082 Å to 8.088–8.093 Å
(Table 1), which further confirmed the incorporation
3+/4+
3 4
into the lattice of Co O . Additionally, the crystalline size of
version were investigated by changing the loading amount of RuO
x
/
after loading RuO
x
ꢀ 1
Co
3
O
4
-HP under the gas flow rate of 100 mL min . 3 vol. % water vapor
of Ru
(
when used) was added by a bubbling method. The reactants and
all the samples was about 19 nm based on Scherrer equation applied for
◦
products were analyzed online by gas chromatography (GC, FULI,
GC9790II, China) equipped with FID, TCD, and nickel converting
equipment. The conversion was measured by the average value of three
sampling analyses, and the carbon balance was up to 96 % or higher. Cl2
was detected by a chemical titration method as described in our previous
work [24]. Both external and internal diffusion limitations were
excluded by varying the particle size of catalysts and W/F (the ratio of
catalyst weight to the total flow rate). More details could be found in
Supplementary Materials. Usually, the mentioned mass transfer resis-
(311) at the 2θ angle of 36.9 (Table 1). Fig. 1.B further showed Raman
spectra of Co
3
O
4
and its supported RuO
x
samples. Five Raman-activated
modes could be detected on the Co
3 4
O
. In particular, the main band at
ꢀ 1
7
about 678 cm corresponded to the A1g species in the O
scopic symmetry from octahedral sites (CoO ) and the band at about 190
cm was assigned to the F2 g symmetry from tetrahedral sites (CoO ).
Meanwhile, the band located at about 477 cm was assigned to E
h
spectro-
6
ꢀ 1
1
4
ꢀ 1
g
-
1
ꢀ 1
symmetry and the bands at 521 cm accompanied with 613 cm were
2
x
assigned to the F2 g symmetry [35]. With the adding of RuO , no new
ꢀ 1
tance was eliminated with a linear velocity higher than 7.0 cm⋅s when
the catalyst particle size was diminished to 40–60 mesh [13].
bands appeared, but the intensity of the bands decreased and the posi-
tion shifted to the low wavenumbers (Fig. 1B, inset), indicating that Ru
species incorporated into the lattice of Co
consistent with XRD results.
3
O
4
. All the results were highly
2
.4. Temperature programmed surface reaction (TPSR)
The actual Ru content of all supported RuO
x
samples determined by
The temperature-programmed surface reaction was conducted: the
ICP-AES was approximately 0.90 wt. % (Table 1), which indicated that
Ru species could be effectively loaded by the adopted three methods.
The textural properties, such as the specific surface area, average pore
feeding containing 1000 ppm 1, 2-DCE and 10 % O
2
/Ar continuously
◦
flowed through 100 mg catalyst, was heated from 100 to 400 C at the
◦
ꢀ 1
heating rate was 2 C min in a temperature controlled-reactor. 1, 2-
DCE and products were analyzed online by mass spectrometer appa-
ratus (Hiden HPR-20EGA, England).
size, and pore size distribution, were measured by N
desorption as shown in Fig. 2 and Table 1. All the samples presented a
type IV sorption isotherm with an H -type hysteresis loop in the relative
pressure range of 0.75–1.0, which confirmed the existence of mesopores
Fig. 2A). Meanwhile, the pore size distribution calculated from the
adsorption isotherms branch based on the BJH model indicated that the
2
adsorption-
2
(
3 4 x
Fig. 1. XRD patterns (A) and Raman spectra (B) of Co O and its supported RuO catalysts.
3