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W. Wang et al. / Catalysis Communications 11 (2010) 803–807
as Co–Ni–Mo–B or La–Ni–Mo–B. For comparison, Ni–Mo–B catalyst
containing no additive was also prepared as described above.
2.2. Catalyst characterization
Specific surface area was measured by a Quantachrome's NOVA-
2100e Surface Area instrument by physisorption of nitrogen at 77 K.
The morphology was obtained by scanning electron microscopy
(SEM) on a JEOL JSM-6360 electron microscopy. X-ray diffraction
(XRD) test was carried on a D/max2550 18KW Rotating anode X-Ray
Diffractometer with Cu Kα (λ 1.5418 Å) radiation (40 kV, 300 mA).
The 2θ was scanned over the range of 15–85° at a rate of 10°/min to
identify the amorphous structure. Bulk compositions were identified
by Inductively Coupled Plasma analysts (ICP) on a Varian VISTAMPX.
The surface composition and surface electronic state were analyzed by
X-ray Photoelectron Spectroscopy (XPS) using Kratos Axis Ultra DLD
instrument at 160 eV pass energy. Al Kα radiation was used to excited
photoelectrons.
2.3. Catalyst activity measurement
The catalyst activity tests were carried out in a 300-mL sealed
autoclave. The as-prepared catalyst (0.05 g), phenol (11.76 g) and
dodecane (88.24 g) were placed into the autoclave. Air in the
autoclave was evacuated by pressurization–depressurization cycles
with nitrogen and subsequently with hydrogen. The mixture was
heated at 10 K/min to desired temperature, then pressurized with
hydrogen to 4.0 MPa, stabilized the stirring speed at 700 rpm. During
the reaction, liquid samples were withdrawn from the reactor and
identified by Agilent 6890/5973 N GC–MS. The amounts of phenol and
products were analyzed by Agilent 7890 gas chromatography using a
flame ionization detector (FID) with a 30 m AT-5 capillary column.
3. Results and discussion
3.1. Characterization of the amorphous catalysts
Fig. 1 shows the morphologies of Ni–Mo–B, Co–Ni–Mo–B and La–
Ni–Mo–B samples. Ni–Mo–B showed eggshell morphology with
inhomogeneous particle size accompanied with agglomeration
phenomenon. The range of Ni–Mo–B particle size was 100 nm to
400 nm. The average particle diameters of Co–Ni–Mo–B and La–Ni–
Mo–B catalysts were both around 100 nm. But the agglomeration
phenomenon of Co–Ni–Mo–B was more obvious than that of La–Ni–
Mo–B. The corresponding surface areas of Ni–Mo–B, Co–Ni–Mo–B and
La–Ni–Mo–B, as shown in Table 1, were 38.42 m2/g, 52.67 m2/g and
116.64 m2/g, respectively, indicating that the additive Co or La could
decrease the particle size and increase the surface area of catalyst.
However, the addition of La increased two times the surface area
value in comparison with the addition of Co, which was related to the
agglomeration phenomenon of particles. La (r=2.74 Å), much larger
than Co (r=1.67 Å), was distributed in Ni–Mo–B amorphous catalysts
as dispersant agent and prevented agglomeration efficiently [22].
The XRD patterns of the fresh samples are shown in Fig. 2(a). A
broad diffraction peak was appeared around 2θ=45°, attributing to a
typical amorphous structure [19,20,23]. Another diffraction peak at
2θ=27° was mainly ascribed to boron oxides [15,24]. Compared with
Ni–Mo–B, the peaks of Co–Ni–Mo–B and La–Ni–Mo–B at 2θ=27°
were weaker, indicating that the additives Co or La could inhibit the
formation of boron oxide. As shown in Fig. 2(b), Co–Ni–Mo–B, heat-
treated at 548 K, showed three diffraction peaks at 2θ=38°, 44°, 52°,
corresponding to NiO, Ni (111) and Ni (200) [25], respectively, which
indicated that the amorphous state of Co–Ni–Mo–B catalyst began to
transform to crystalline state. However, La–Ni–Mo–B sample, heat-
treated at 548 K, showed only two small diffraction peaks at 2θ=44°
and 52° and the diffraction peak intensities of these two peaks were
Fig. 1. SEM images of (a) Ni–Mo–B, (b) Co–Ni–Mo–B and (c) La–Ni–Mo–B.
much weaker than that of Co–Ni–Mo–B(C) (heat-treated at 548 K),
suggesting that La–Ni–Mo–B also began to transform to crystalline
state. But the thermal stability of La–Ni–Mo–B was better than that of
Co–Ni–Mo–B.
The binding energies of metallic Ni combined with B in Ni–Mo–B,
Co–Ni–Mo–B and La–Ni–Mo–B, as shown in Fig. 3a, were 853.0 eV,
852.1 eV and 852.0 eV, respectively. The other peaks of each sample
were assigned to Ni2+ [16–19]. In Fig. 3b, all of the samples exhibited
two peaks. The low-binding energy (around 189.0 eV) was attributed
to B0 while the high-binding energy (around 193.0 eV) was attributed
to oxidized boron [16,26]. Notably, the binding energy of Ni0 in Ni–
Mo–B (853.0 eV) was higher than that of Co–Ni–Mo–B (852.1 eV) and
La–Ni–Mo–B (852.0 eV). Compared with the standard binding
energies of elemental nickel and boron, the binding energies of Ni0
shifted negatively while the binding energies of B0 shifted positively