2
88
W. Li, H. Cheng / Journal of Alloys and Compounds 448 (2008) 287–292
◦
2
. Experimental
tor temperature was increased from room temperature to 260 C with a rate of
3
◦
C/min. The variation of CO2 concentration in the final gases was detected by
a SQ-206 gas chromatograph equipped with a Porapak-Q column.
2
.1. Materials synthesis
2
.1.1. Preparation of monodisperse Bi2O3 nanoparticles
A typical synthetic procedure the monodisperse spherical Bi2O3 nanoparti-
3. Results and discussion
cles is described in detail in Refs. [14,15], and briefly shown as follows: 0.01 mol
3
.1. Analysis of phase structures
Bi(NO3)3·6H2O was dissolved in 30 mL of 0.005 M HNO3 to form a transpar-
3
+
ent solution. The 20 mL PEG8000 was slowly added into the Bi solution in
◦
a 90 C water bath under thorough stirring. After being further stirred for ca.
Fig. 1 presents XRD patterns of the as-synthesized core/shell
3
0 min, 50 mL of 4 M NaOH solution was poured into the above solution, in
nanoparticles before and after calcinations. It can be seen that the
precursors before calcinations are mainly composed of Bi2O3
which a light yellow suspension would be formed immediately. After being vig-
◦
orously stirred for 2 h in a 90 C water bath, the resulting light yellow precipitates
(JCPDS: 712274 and 501088) as core and copper ammonium
were collected by centrifugation at a rotation rate of 24,000 r/min, followed by
successive washing with absolute ethanol, acetone, and deionized water for sev-
eral times. The final products were obtained after dried in a vacuum oven for
chromate as shell, and the chemical formula of the shell mate-
rials was found to be (NH4)0.78Cu1.04(NH ) CrO (OH)
according to JCPDS-420072 (Fig. 1a). The XRD pattern of the
3 0.14
4
0.86
5
h.
◦
samples after calcined at 500 C for 5 h in argon atmosphere is
2
.1.2. Preparation of CuCr2O4–CuO nanocomposites
shown in Fig. 1b, indicating that only diffraction peaks for Bi2O3
can be observed. This may be due to the thermal decomposition
of (NH4)0.78Cu1.04(NH3)0.14CrO4(OH)0.86, resulting in the for-
mation of amorphous or poorly crystallized CuCr O inorganic
In comparison, the CuCr2O4–CuO nanocomposites were also prepared by a
complexing-coprecipitation method as described in the following: ammonia was
added dropwise into 100 mL of 0.5 M Cu(NO3)2 under strongly stirring until a
◦
dark blue solution was obtained. The resulting solution was put in a 90 C water
2
4
bathandstirredfor30 min. Then, 100 mLof0.5 MCr(NO3)3 solutionwasslowly
dropped into the above solution under stirring, in which brown precipitates were
gained. Next, ammonia was used to adjust the pH value of the solution to be
around 8. After being stirring for another 6 h, the dark brown precipitates were
filtered out and dried in an oven for 24 h to obtain the dark brown precursors.
Some of the precursors were used for DTA analysis to investigate the thermal
decomposition procedure. Black CuCr2O4–CuO composite nanomaterials can
component. The diffractions of peaks referring to CuCr2O4 are
too weak to be seen as compared with Bi2O3. When the anneal-
ing temperature is elevated to 800 C, the XRD pattern indicates
◦
that the as-prepared samples mainly consist of Bi2O3 and spinel
CuCr O , accompanying by trace of CuO as shown in Fig. 1c.
2
4
◦
If the calcinations temperature is further increased to 1000 C,
reflections referring to CuCrO2, Cr2O3, and CuO phases can be
seen in the XRD pattern in Fig. 1d, in addition to Bi2O3 and
CuCr2O4. As reported, CuCr2O4 will decompose to CuCrO2
and Cr2O3 at high temperature [16]. As a result, although the
XRD results are fairly ambiguous, the aforementioned observa-
tions imply that the copper chromite component is successfully
coated on the surfaces of Bi2O3 core materials, which will be
further discussed in detail in the following sections.
◦
be obtained after the precursors are annealed at 800 C for 5 h.
2
.1.3. Fabrication of monodisperse Bi2O3/CuCr2O4–CuO core/shell
nanoparticles
A certain amount of the as-prepared monodisperse Bi2O3 nanoparticles were
washed with deionized water several times, then placed into 100 mL isopropyl
alcohol and sonicated for 1 h, resulting in a light yellow colloidal suspensions.
Next, 20 mL of 5% ammonia and 20 mL deionized water were added into the
◦
mixed suspensions under vigorous stirring under a 60 C water bath to adjust
its pH value to be ca. 8. The suspension was further stirred for 1 h at constant
temperature, followed by aging for 5 h at room temperature. Thereafter, a cer-
tain amount of 0.05 M Cu(NO3)2 solution was dropped slowly into the above
3.2. Fourier transformation infrared (FTIR) analyses
◦
suspension under continuous stirring in a 60 C water bath, during which 5%
ammonia was used to keep the pH of the solution to be about 8. After the addi-
tion of Cu(NO3)2 solution, the resultant suspension was mildly stirring in a
bath for 5 h and then allowed to age for 5 h at room temperature. Next, an equal
amount of 0.05 M Cr(NO3)3 solution was added into the suspensions in a similar
way to that of Cu(NO3)2 solution except that the aging time is 36 h. Finally, the
brown black precursors were collected by filtering. The dark black samples were
obtained by calcining the precursors at 300 C for 2 h and then 800 C for 5 h in
air. The molar ratio of CuCr2O4 to Bi2O3 in the whole preparation process was
controlled to be 1:4.
The FTIR spectrum of monodisperse spherical Bi2O3
nanoparticles employed as core materials (templates) is pre-
sented in Fig. 2a. Four characteristic bands can be clearly seen
−
1
from Fig. 2a, in which the band at ∼3449 cm corresponds to
−1
the stretching vibration of OH , while the band appearing at
1633 cm represents the stretching mode of absorbed H2O.
◦
◦
−
1
∼
−1
In addition, the band located at ∼1381 cm can be ascribed to
−
−1
the bending vibration of NO3 , and the band at ∼444 cm is
2
.2. Materials characterization
attributed to the stretching mode of Bi–O. The FTIR data reveal
−
thatthereareabundantOH groupslocatedonthesurfacesofthe
The phase structures of the as-prepared samples were characterized by X-
ray diffraction (XRD) taken on a Germany Bruker D-8 Diffractometer (Cu K␣
radiation, λ = 1.5418 A˚ ). The surface structures were analyzed by Fourier trans-
Bi2O3 nanoparticles [17,18], which would play a critical role in
the following reactions for the formation of core/shell structures
2+
3+
via the interactions between Bi2O3 particles and Cu /Cr [19].
Fig. 2b depicts the FTIR spectrum of the CuCr2O4–CuO com-
posites obtained by complexing-coprecipitation method. Two
formation infrared spectra (FTIR). The microscopic morphologies and grain
sizes were observed with a Japan Hitachi H-800 transmission electron micro-
scope operated at an accelerating voltage of 200 kV. The catalytic activities of
the products on the conversion of CO were evaluated with a fixed-bed and quartz
glass reactor. The 0.2 g of the as-prepared products was used as the catalysts.
The volume percentages of CO and O2 in the mixed gases were 1.0% and 16%,
respectively. N2 was adopted as balanced gas in the catalytic process. The veloc-
ity of gas was controlled with a D07-7A mass flowmeter, and the total flux of
the mixed gases was 100 mL/min. During the whole reaction process, the reac-
−
1
−1
strong absorption bands at ∼615 cm and ∼515 cm can be
seen in the short-wave region, which corresponds to the vibra-
tion absorption of Cu–O–Cr in CuCr2O4 [20,21]. As to the
samples after coating, the characteristic absorption bands for
−
1
−1
−1
)
Bi–O (∼444 cm ) and Cu–O–Cr (∼605 cm , ∼515 cm