C. Lin et al.
CatalysisCommunications111(2018)64–69
aggregation of copper oxide [18]. For the unreduced Cu-Cr2O3/γ-
Al2O3 sample, the main peak shifted to 179 °C. The obvious low
reduction temperature peak was probably related to the reduction of
highly-dispersed CuO [19], and the disappearance of shoulder peak
indicated that the existence of Cr improves the dispersion of CuO
particles, which agreed well with the results of XRD. As for the
unreduced Cu-Cr2O3-CoO/γ-Al2O3 sample, the main peak further
shifted to lower temperature (146 °C), which meant that Co might
promote the dispersion of CuO or change its reduction. In con-
sideration of the similar Cu particle sizes with Cu-Cr2O3/γ-Al2O3
from XRD, properly the latter was the main reason. But it still
needed further verification by TEM. In addition, the new shoulder
peak may be ascribed to the reduction of Co3+ to Co2+ [20], while
the second broad peak around 300–500 °C was assigned to the re-
duction of the remaining Co2+ to Co0 [21,22]. Furthermore, no
peaks corresponding to the reduction of Cr species were identified.
Thus, under our experimental conditions, only the Cu specie was
reduced to metallic state, and the Cr and Co species still maintained
the oxidation state.
XPS. To further explore the chemical state of the elements at the
surface of catalysts, XPS analysis of three catalysts was carried out,
and the results are presented in Fig. S1 (Supporting Information).
The binding energies of Cu 2p3/2 for Cu/γ-Al2O3, Cu-Cr2O3/γ-Al2O3,
and Cu-Cr2O3-CoO/γ-Al2O3 were 932.4 eV, 932.2 eV, and 932.3 eV,
respectively. These were mainly ascribed to Cu 2p3/2 peaks of Cu0
[23]. This agreed well with the results of XRD pattern. The binding
energy of Cr 2p3/2 located at 576.7 eV, indicating the presence of
Cr3+ species as Cr2O3 or CuCr2O4 [19,24]. As for Co species in Cu-
Cr2O3-CoO/γ-Al2O3, the peaks at 780.6 eV was assigned to Co 2p3/2
with the shake-up satellite at 785.9 eV, while the peak at 796.3 eV
was assigned to Co 2p1/2 with the satellite peak at 802.7 eV [25].
The peaks and their shake-up satellites confirmed the presence of
Co2+ in the high-spin state [26]. The absence of the characteristic
peak at 778.1 eV indicated the nonexistence of Co metal. This result
declared that Co species exits as CoO phase, which is consistent with
Scheme 1. Reaction pathways for the hydrogenation of nitriles.
PNout, PAout, and BPAout were the concentrations of PN, PA, and BPA in
reaction fluid (including all products and unreacted reactants), re-
spectively. They were determined by GC with area normalization
method.
TEM. To further investigate the influences of Cr and Co on Cu/γ-
Al2O3 catalyst, these catalysts were characterized by TEM. The TEM
image of fresh Cu-Cr2O3-CoO/γ-Al2O3 catalyst is described in Fig. 4.
The needle-like γ-Al2O3 was clearly observed, and many black dots
were assigned to Cu metal particles, which were dispersed uniformly
on the support. Similar morphology was also observed on Cu/γ-
Al2O3 and Cu-Cr2O3/γ-Al2O3 (Fig. S2). For Cu-Cr2O3/γ-Al2O3, Cu
particles were also dispersed well on the support, and the particle
size was smaller. However, Cu particles aggregated severely on Cu/
γ-Al2O3 catalyst. This agreed well with the XRD results. EDS analysis
in the STEM image revealed that Cr was homogeneously dispersed
on the whole catalyst. It has been verified in our previous work that
γ-Al2O3 support modified by doping with Cr can enhance the dis-
persion of Cu metal particles [19,27]. Besides, the EDS map of Co
demonstrates that the CoO particles were strictly dispersed around
the Cu metal particles. Even though, CoO didn't further enhance the
dispersion of Cu, it changed the circumstance of Cu. That's why the
peak of Cu-Cr2O3-CoO/γ-Al2O3 in H2-TPR decreased 33 °C compared
with Cu-Cr2O3/γ-Al2O3. The CoO beside Cu particles played an
important role in the catalytic performances.
3. Results and discussion
3.1. Catalyst characterization
XRD. The X-ray diffraction patterns of supported Cu catalysts were
measured and the results are shown in Fig. 2. All catalysts showed the
characteristic diffraction peaks of γ-Al2O3 (located at 2θ = 37.6°, 45.8°,
and 66.7°) and the metallic Cu phase (located at 43.3°, 50.4°, and
74.1°). It was obvious that the Cu diffraction peaks of Cu-Cr2O3/γ-Al2O3
and Cu-Cr2O3-CoO/γ-Al2O3 were much weaker than Cu20/γ-Al2O3.
According to the Scherrer equation, the crystal sizes of Cu metal were
estimated to be 23.1, 14.0, and 13.7 nm for Cu/γ-Al2O3, Cu-Cr2O3/γ-
Al2O3, and Cu-Cr2O3-CoO/γ-Al2O3, respectively (Table S1). It was de-
monstrated that Cr enhanced the dispersion of Cu, which has been
verified in previous works [16,17]. No obvious diffraction peaks of
chromium and cobalt compounds were observed in the XRD patterns,
possibly attributed to their amorphous or small size.
H2-TPR. Fig. 3 showed the H2-TPR profiles for the precursors of
three samples. The first sharp peak, for Cu/γ-Al2O3, with the
maxima at 210 °C was ascribed to the reduction of well-dispersed
CuO to Cu0. The shoulder peak at 240 °C was corresponding to the
Fig. 1. Structures of PA, PN and BPA.
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