136
Table 1
Comparison of some parameters of the different CNTs supported Pt catalyst.
d
Catalysts
SBETa(m2/g)
SBJHb(m2/g)
Vmesobcm3/g
Vmicroccm3/g
Vtotalcm3/g
DBJH (nm)
Pt/CNTs
Pt/N-CNTs
Pt/O-CNTs
212.6
224.3
232.2
211.6
220.1
235.5
1.00
1.12
1.26
0.06
0.08
0.10
1.06
1.20
1.36
3.15
3.41
3.83
a
SBET: from the BET method.
SBJH and Vmeso: calculated from the BJH method.
Vmicro: calculated from the DFT methods.
b
c
d
DBJH: mesopore diameter calculated from absorption branch of nitrogen isotherms using BJH method.
Table 2
XPS surface Element content, binding energy values and relative concentration in the Pt4f7/2 for different CNTs supported Pt catalyst.
Catalysts
Element content (%)
Binding energy (eV)
Relative concentration (%)
C
N
O
Pt
Pt(0)
Pt(II)
Pt(IV)
Pt(0)
Pt(II)
Pt(IV)
Pt/CNTs
Pt/N-CNTs
Pt/O-CNTs
96.24
94.34
93.61
0.69
1.85
0.63
1.77
2.04
3.96
1.19
1.54
1.60
71.7
72.2
71.8
72.5
72.9
72.6
74.2
74.7
74.7
69.04
55.14
53.69
21.26
30.60
30.36
9.70
14.26
15.96
2.3. Characterization
the two treated samples had a broader full width at half maxi-
mum (FWHM) which was related to crystallite size, implying that
the treatment damaged the ordered crystal structure, resulting
in a decrease in crystallite size. This is also proved through the
Raman spectroscopy. The broad diffraction peaks at 40.2◦, 46.4◦
and 68.2◦ in good agreement with the metallic platinum (1 1 1),
(2 0 0), and (2 2 0) reflections (JCPDS card No. 04-0802), could be
observed in the Pt/CNT sample, which were consistent with the
face-centered cubic (fcc) structure of platinum [22]. However, the
peaks disappeared in the Pt/N-CNTs and Pt/O-CNTs due to the
smaller crystallite size of Pt, indicating functionalized CNTs support
favor the dispersion of metal nanoparticles. When the crystal-
lite size was less than 5 nm, the two adjacent peaks Pt(1 1 1) and
Pt(2 0 0) will broaden and overlap each other in amplitude rather
ance in peaks.
XRD patterns were measured at room temperature by using a
D8 Advance (Bruker, Germany) X-ray diffractometer with the Cu
K␣ radiation at 40 kV and 30 mA. Raman spectra of samples were
collected from 200 to 2000 cm−1 on a LabRAM HR800 Laser Confo-
cal Micro-Raman Spectroscopy (Horiba Jobin Yvon, Japan) using a
532 nm laser source. TEM was characterized by a by a FEI Tecnai G20
(USA) with an accelerating voltage of 200 kV. The textural proper-
ties of samples were performed by nitrogen sorption isotherms on
an ASAP 3020 instrument (Micromeritics, USA) at 77 K. The surface
area and pore volume were calculated using BET and BJH meth-
ods, respectively. XPS was measured with a K-Alpha XPS system
(Thermo Fisher Scientific, USA) using a monochromatic Al K˛ as the
excitation source (1486.6 eV). Survey (wide) scans spanned from
1000 to 0 eV binding energy, which were collected with an analyzer
pass energy of 100 eV at an interval of 1.00 eV.
Raman spectroscopy was employed to characterize carbona-
ceous materials for distinguishing ordered and disordered crystal
structures. All the materials in the Fig. 1b had same peak positions
of the G band (1576 cm−1), assigned to Raman-active E2 g mode for
the tangential in-plane stretching vibrations of the sp2-hybridized
of translational symmetry produced by the microcrystalline struc-
ture, and D’-band (1612 cm−1), attributed to a double-resonance
Raman feature induced by disorder, defects or ion intercalation
between the graphitic walls [23]. After the functionalization, the N
Therefore the lattice defect obviously increased and the D band
became strong for N-CNTs and N-CNTs. Typically, The ratio of the
integral intensities of the G and D bands (ID/IG) is used to probe the
degree of graphitization [24] and the in-plane crystallite size (equa-
tion: La = (2.4 × 10 − 10)ꢀ4laser(ID/IG)−1) [25] of samples. Among the
three samples, Pt/N-CNTs and Pt/O-CNTs have the higher ID/IG value
than Pt/CNTs and so they have the lower degree of graphitization
and smaller crystallite size, which is consistent with XRD.
2.4. Hydrogenation reaction
The hydrogenation reactions were carried out in a stainless
autoclave reactor with a 50 mL Teflon sleeve. In a typical pro-
cedure, 0.1 g catalyst was dispersed in 19 mL ethanol and then
8.2 mmol CAL was added into solution. The reactor was sealed,
purging with H2 for 3 times, respectively, and then pressurized
to 2.0 MPa. The reaction was conducted at 70 ◦C with a stirring
speed of 750 rpm for 2 h. The reaction mixture was analyzed by
Shimadzu GC-2010 gas chromatograph with a flame ionization
detector (FID) system equipped with a capillary column SE-54 [(5%-
phenyl)-95%dimethylpolysiloxane, 30 m × 0.32 mm × 0.5 m].
3.1. Catalysts characterization
Fig. 2 shows the TEM photographs and the corresponding his-
tograms of the particle size distribution of Pt NPs on the CNTs,
respectively. There was no obvious difference in the terms of
morphology and all the catalysts presented regular mesochannels
with the external diameter averaged 13 nm and inner diameter of
3.6 nm. It was observed that Pt NPs were highly dispersed on the
support with a narrow sizes distribution ranging from 2 to 6 nm,
regardless of the types of support. This was because NaBH4 reduc-
tion was able to produce small and uniform metal particles [26].
However, the maximum of Pt sizes present a slight difference for
these catalysts. The main Pt sizes in Pt/CNTs concentrated on 4-
Fig. 1a shows the powder XRD patterns of as-prepared catalysts.
The peaks at 26.1◦, 43.5◦, 54.1◦, 77.5◦ were attributed to the (0 0 2),
(1 0 1), (0 0 4) and (1 1 0) diffractions of hexagonal graphitic car-
bon (JCPDS 41-1487), respectively. The wide (0 0 2) peak showed
that the CNTs possess amorphous structure with small regions of
crystallinity and the regions of crystallinity are highly graphitic
[21]. The position and sharpness of the C (0 0 2) peak in the Pt/N-
CNTs and Pt/O-CNTs indicates that the graphite structure of the
CNTs was functionalized without significant damage. The lattice
structure (d) of region of crystallization was maintained well after
the functionalization. A puzzling phenomenon was observed that