R.J. Kalbasi et al. / Catalysis Communications 12 (2011) 955–960
957
1
so, a pure product was obtained. The product was identified with H
1
3
NMR, C NMR and FT-IR spectroscopy techniques.
3
. Results and Discussion
3
.1. Catalyst Characterization
The powder X-ray diffraction patterns of mesoporous silica SBA-
5, PVAm/SBA-15 and Ni-PVAm/SBA-15 samples are shown in Fig. 1.
1
Typically, the low angle diffraction pattern shows three peaks at 2θ
values of 0.5°–3°, including one strong peak (100) and two weak
peaks (110) and (200) (Fig. 1a)‚ which corresponded to a highly
ordered hexagonal mesoporous silica framework [17]. The PVAm/
SBA-15 and Ni-PVAm/SBA-15 samples showed the same patterns at
2θ values of 0.5°-3°, indicating that the long-range order of the SBA-15
framework was well retained after the immobilization (Fig. 1b, c).
In the amorphous Ni-PVAm/SBA-15, Ni peak could not be seen in
XRD due to the homogeneity of the composite and Ni-PVAm/SBA-15
showed an amorphous pattern at 2θ values of 20°–40° (Fig. 1d). In order
to prove the existence of the Ni nanoparticles in the composite, the
composite catalyst was exposed to temperature (200 °C and 400 °C). On
heating, amorphous Ni- changed to crystalline, thus appearing as a peak,
the intensity of which increased at higher temperature. The XRD
patterns of Ni-PVAm/SBA-15 sample at two temperatures (200 °C and
Fig. 2. FT-IR spectra of (a) PVAm/SBA-15 and (b) Ni-PVAm/SBA-15.
1436 cm− is the bending vibration absorption of the N–H bond.
1
−1
Moreover, the presence of peaks at around 2800–3000 cm
corre-
sponds to the aliphatic C–H stretching in PVAm/SBA-15. According to
our previous study [14], the characteristic band at 1089 cm− is due to
the Si–O stretching in Si–O–Si structure of SBA-15. The appearance of
the above bands shows that PVAm was attached to the surface of SBA-
15, and the PVAm/SBA-15 composite was obtained.
1
4
2
00 °C) can be seen in Fig. 1e and Fig. 1f, respectively. After calcining at
00 °C (Fig. 1e), XRD patterns of residue showed that the broadening
and low intensity of peaks could be attributed to nano size of Ni particles
described in later section). Nevertheless, the peaks at 2θ=44.29,
(
−1
corresponding to the plane (111) of fcc nickel, could be observed. The
same procedure can be seen in Fig. 1f, nickel nanoparticles peak is
shown at 2θ=44.29.
As shown in Ni-PVAm/SBA-15 spectrum, the band around 1090 cm
−1
was shifted to lower wavenumbers (999 cm ) (red shift). This might be
due to the introduction of the Ni groups. The peak intensity of the
−1
Fig. 2 shows the FT-IR spectra of PVAm/SBA-15 and Ni-PVAm/SBA-
spectrum of Ni-PVAm/SBA-15 at 1346 cm is lower than that of PVAm/
SBA-15 and also the peak is shifted to lower wavenumbers. These might
result from interaction between the Ni particles and N–H groups.
1
5. In the FT-IR spectrum of PVAm/SBA-15 (Fig. 2a), the band at
2+
Fig. 3a shows the DRS-UV of PVAm/SBA-15, Ni -PVAm/SBA-15
and Fig. 3b shows the DRS-UV of Ni-PVAm/SBA-15. DRS UV of Ni2+
-
PVAm/SBA-15 is shown because we want to show the difference
between DRS UV of Ni2 -PVAm/SBA-15 and Ni-PVAm/SBA-15. There
is no characteristic peak in PVAm/SBA-15. In the case of Ni(II) amin
complex, there are no LMCT transitions at wavelengths longer than
+
2
50 nm, so the peaks involve in this case are d–d transitions only
(
Fig. 3a). Assuming octahedral coordination of Ni(II), the observed
3
absorption bands can be attributed to the electronic transitions of T1g
(
(
3
3
3
1
3
P)← A2g (F) (365 nm), T1g (F)← A2g (F) (592 nm), E
g
(D)← A2g
F) (745 nm) (Fig. 3a) [18]. As shown in Fig. 3b, Ni-PVAm/SBA-15
shows the feature around 250 nm [19] due to the Ni nanoparticles. So
2+
comparing the two spectra, it can be found that all peaks of Ni
disappeared as a result of the reduction of Ni2 to Ni .
+
0
The TEM micrographs of SBA-15 and Ni-PVAm/SBA-15 were
depicted in Fig. 4. The TEM micrographs of SBA-15 materials
(
Fig. 4a) showed the well-ordered hexagonal arrays of pores with
one-dimensional channel indicating 2-D hexagonal mesopores.
In order to reveal the morphology and structure for Ni nanopar-
ticles, TEM experiment is carried out for the Ni-PVAm/SBA-15 (Fig. 4b,
c). As shown in Fig. 4b, spherical nickel nanoparticles (average
diameter of ~3 nm) were seen to be dispersed mainly inside the pores
of SBA-15. TEM images of Ni-PVAm/SBA-15 confirm that the
hexagonally arranged mesopores of SBA-15 are retained and no
damage of the periodic structure of the silicate framework was
observed. Fig. 4b clearly shows the uniform dispersion of nickel
nanoparticles inside the SBA-15 channels. Fig. 4c shows Ni particles
with a spherical shape and relatively narrow size distribution in the
range of 2–5 nm.
EDX analysis from area shown in Fig. 4c, confirmed the presence
Fig. 1. XRD patterns of (a) mesoporous silica SBA-15 (b) PVAm/SBA-15 (c) Ni-PVAm/
SBA-15 (2θ=0.5–5) (d) amorphous Ni-PVAm/SBA-15 (2θ=15–70) (e) Ni-PVAm/SBA-
of nickel nanoparticles and Na which attributed to NaBH
reducing agent.
4
used as a
15 burned in 200 °C for 2 h and (f) Ni-PVAm/SBA-15 burned in 400 °C for 2 h.