J. Shan et al. / Journal of Catalysis 383 (2020) 13–23
15
2
h, followed by evacuation at 10ꢁ2 Pa for 2 h. Finally, pyridine
moles of unreacted glycerol
moles of glycerol in the feed
Glycerol conversion ¼ ð1 ꢁ
Þ
vapor was introduced in the sample cell at 308 K for 1 h and the
spectra were recorded after evacuation at 423 K for 15 min.
ꢂ 100%
2
.3. In situ Fourier transform infrared experiments of glycerol
moles of 1; 2 ꢁ PDO
1; 2 ꢁ PDO selectivity ¼
ꢂ 100%
adsorption
moles of all liquid products
In situ FT-IR experiments of glycerol adsorption were conducted
TOF ðhꢁ
1
Þ
on a Bruker Tensor 70 FT-IR spectrometer equipped with a LN-MCT
Mid VP detector. A self-supported sample wafer was reduced with
conversion ꢂ moles of glycerol in the feed ðmolÞ
ꢁ1
¼
:
1
0 vol% H
2
/Ar flow (50 mL min ) at 593 K for 2 h. The spectra were
total Cu amount ðmolÞ ꢂ Cu dispersion ꢂ reaction time ðhÞ
collected at selected temperatures in the course of cooling down
and used as background. After cooling to room temperature,
2
0 mL 5 wt% glycerol tetrahydrofuran solution was dripped onto
3
. Results and discussion
the wafer homogeneously. The wafer was then heated, and the IR
spectra were recorded under vacuum at 323, 373, 423, and
4
3.1. Formation of CuAOASiAOA species and highly dispersed Cu
73 K. Tetrahydrofuran was used as a solvent because it can easily
be pumped out of the vacuum system at room temperature for its
low boiling point. The spectra of adsorbed species can be acquired
by subtracting the background spectra. The weight of the sample
wafer is about 10 mg for pure SBA-15, 10%Cu/SBA-15(IM), and
XPS analysis was used to determine the chemical states of cop-
per. The XPS spectra of calcined and reduced 10%Cu/SBA-15(G)
and 10%Cu/SBA-15(IM) are shown in Fig. 1A. For calcined 10%
Cu/SBA-15(G), two Cu 2p3/2 peaks (933.1 eV and 935.4 eV) can
be distinguished, corresponding to CuO and CuAOASiAOA spe-
cies, respectively [32,43–45]. As a comparison, the 935.4eV peak
of calcined 10%Cu/SBA-15(IM) is much smaller and enveloped
by the CuO peak at 933.1 eV, meaning fewer CuAOASiAOA spe-
cies in calcined 10%Cu/SBA-15(IM). These results are supported
by the green color of 10%Cu/SBA-15(G) and the gray color of
1
0%Cu/SBA-15(G). Cu+SBA-15 is a physical mixture of 50 wt%
metallic Cu (Alfa-Aesa) with particle size 0.5–1.5
and 50 wt% SBA-15.
lm diameter
2.4. Density functional theory calculations
First principles DFT calculations were carried out with the
1
0%Cu/SBA-15(IM) shown in Fig. S1 in the Supplementary Mate-
rial, because the colors of CuAOASiAOA and bulk CuO are green
and black, respectively [31].
Vienna ab initio simulation package (VASP) [38,39] with
projector-augmented wave (PAW) [40,41] pseudo-potentials. The
generalized gradient approximation (GGA)-type functional, param-
eterized by Perdew, Burke, and Ernzerhof (PBE), was implemented
to describe electron exchange and correlation energy [42]. The
plane-wave cutoff energy for the wave function was set to
From XPS spectra of reduced samples, it can be found that no
satellite peak appears at 940–947 eV, suggesting that almost all
2+
of the Cu species were reduced [46]. Additionally, the Cu2p2/3
binding energy of reduced 10%Cu/SBA-15(G) is higher than that
of the sample prepared by impregnation. The shift of the reduced
0%Cu/SBA-15(G) to higher binding energy indicates that a strong
4
00 eV. All structures were considered relaxed until the total
-5
energy was converged to 10 eV and all atomic forces were smaller
1
ꢁ1
than 0.05 eV Å . Spin-polarized calculations were performed. We
adopted a four-layer SiO (1 1 0) slab with a Cu adsorbing struc-
ture (Cu /SiO ) to investigate the CuAOASiAOA interface interac-
interaction exists between Cu and SiO resulting from formation of
2
2
4
CuAOASi bonds [47]. In contrast, only a few CuAOASi bonds were
formed in 10%Cu/SBA-15(IM), as indicated by the asymmetry of the
4
2
tion. More details concerning DFT methods and the calculated
model are described in the Supplementary Material.
Cu2p2/3 peak. The electron shift in CuAOASi bonds should result in
d+
the formation of Cu
sites. To confirm the existence of
CuAOASiAOA species and determine the surface content of Cu
species with different valence states, Cu LMM XAES spectra were
recorded for reduced catalysts (Fig. 1B). All samples presented
two peaks at kinetic energies of about 918.1 and 914.2 eV in the
Cu LMM XAES spectra, which could be ascribed to Cu0 and Cu
2
.5. Catalytic test
Glycerol hydrogenolysis to 1,2-PDO was carried out in a Teflon-
d+
lined stainless steel autoclave (NS-10-316 L, Anhui Kemi Machin-
ery Technology Co., Ltd.) equipped with an electromagnetic stirrer
and a temperature controller. The specific reaction conditions were
as follows: a certain amount of catalyst, 6.67 g n-butanol solution
of glycerol (12 wt%), 483 K, 4.0 MPa hydrogen pressure, and
sites
(CuAOASiAOA
species),
respectively
[3,37].
0
(CuAOASiAOA)/Cu was calculated by the area ratio of peaks cen-
tered at 914.2 and 918.1 eV. As clearly illustrated in Fig. 1B, the
0
(CuAOASiAOA)/Cu ratio of 10%Cu/SBA-15(G) (1.098) was much
5
00 rpm stirring speed. All the catalysts were prereduced in a flow
higher than that of 10%Cu/SBA-15(IM) (0.706), coincident with
XPS results.
ꢁ1
2
of 10 vol% H /Ar (50 mL min ) at 593 K for 2 h before reaction.
After designed reaction time, the reactor was cooled with an ice
water bath. Finally, the used catalyst was separated from the liquid
phase by centrifugation.
The TEM images of reduced 10%Cu/SBA-15(IM) and xCu/SBA-15
(G) are shown in Fig. S2. Initially, no obvious Cu nanoparticles
could be found in the general microstructure of reduced ground
samples (Figs. S2A, S2C, and S2E); the Cu nanoparticles are proba-
bly located inside the mesopores of SBA-15 [48]. After being
exposed to electron beam irradiation at high resolution for about
5 min, the ordered mesopores of SBA-15 were damaged and Cu
nanoparticles showed up (Figs. S2B, S2D, and S2F). The Cu
nanoparticles in xCu/SBA-15(G) are highly dispersed and the parti-
cle sizes are small. However, the large Cu particles could easily be
identified for 10%Cu/SBA-15(IM) (Fig. S2H), suggesting that small
Cu nanoparticles could be obtained more easily by grinding than
impregnation.
The collected liquid samples were analyzed on a Shimadzu GC-
2
010 Plus gas chromatograph equipped with a flame ionization
detector (FID), an HP-PONA capillary column, and an autosampler.
The gas phase was analyzed on an Agilent 7890A gas chro-
matograph equipped with two FIDs, a TCD, two capillary columns
(
2 3
DB-1 and GS-OxyPlot), and a Al O /KCl column. The gaseous prod-
ucts contain little CO . The contents of products and unreacted
2
glycerol were determined using an external standard method.
The conversion of glycerol, selectivity to identified products, and
turnover frequency (TOF) were calculated as follows: