H. Li et al. / Journal of Catalysis 259 (2008) 104–110
105
adjusted by changing the amount of oil phase in the microemul-
sion. During liquid-phase hydrogenation of CMA to CMO, the as-
prepared Co–B exhibited better catalytic performance (activity, se-
lectivity, and durability) than the Co–B prepared by direct reduc-
using the ideal gas equation. The RSH should represent the intrinsic
activity, because the effect of metal dispersion has been ruled out.
During the reaction, samples were withdrawn from the reaction
mixture every 30 min for product analysis using a gas chromato-
graph (GC 102) with a flame ionization detector. The stationary
phase was 15% Apiezon (L)/Gas Chrom (red) at 523 K with N2 as
carrier gas. All results have been reproduced, and the errors were
limited within 5%.
−
tion of Co2+ with BH4 or even by ultrasound-assisted reduction of
−
Co(NH3)2+ with BH4 . The correlation of the catalytic performances
to the st6ructural properties has been tentatively established.
2. Experimental
3. Results and discussion
2.1. Catalyst preparation
3.1. Structural and electronic characteristics
In a typical run of catalyst synthesis, CoCl2·6H2O (5.0 mmol,
1.2 g) and polyethylene glycol (Mw = 20,000, 5.0 g) were first dis-
solved in deionized water (40 ml), then an appropriate amount
of cyclohexane was added to this solution. The mixture thus ob-
tained was treated under ultrasonic radiation at 293 K for 30 min,
with an oil-in-water microemulsion formed. Then a 2.0 M KBH4
aqueous solution (10 ml) was added dropwise under vigorous stir-
ring at 293 K. After reaction was complete, the black precipitate
The TEM images (Fig. 1a) show that Co–B-0 displayed irreg-
ular, broadly dispersed particles, apparently due to the particle
−
agglomeration, because the reaction between Co2+ and BH4 is
strongly exothermic [12]. In contrast, the Co–B nanoparticles syn-
thesized in an oil-in-water microemulsion were spherical and rela-
tively uniform, and the particle size decreased from 20 to 6 nm
as the cyclohexane/water volume ratio was increased from 0.1
to 0.25 (Figs. 1b–1d), which was obviously much smaller than the
Co–B-50-30 synthesized through ultrasound-assisted reduction of
−
+
was washed free from Cl or K ions with deionized water until
a pH ∼7 was achieved, followed by three washings with abso-
lute alcohol (EtOH). Finally, the mixture was stored in EtOH until
use. The as-prepared Co–B samples were designated Co–B-x, with
x representing the volume ratio of cyclohexane to water. The di-
rect reduction of CoCl2 with KBH4 in pure aqueous solution re-
sulted in the regular Co–B sample [21] and was designated Co–B-0.
The Co–B-50-30 was prepared by ultrasound-assisted reduction of
−
Co(NH3)2+ with BH4 [14]. The relatively narrow distribution for
6
the as-prepared nanoparticles can be attributed mainly to the dis-
persing effect of oil droplets in microemulsion, which can restrict
particle growth and even prevent aggregation of the Co–B nanopar-
ticles. An increase in the cyclohexane content may enhance the
dispersing effect, leading to decreased particle size (Figs. 1b–1d);
however, a further increase in the amount of cyclohexane could in-
duce significant agglomeration due to the extremely high surface
energy in small Co–B nanoparticles (Fig. 1e).
−
Co(NH3)2+ with BH4 in aqueous solution [14], where 50 and 30
6
refer to the ultrasound power (W) and ultrasonication time (min),
respectively.
ICP analysis revealed that the bulk compositions in all Co–B-x
samples were very close (Table 1). The higher B content in Co–
B-x compared with in Co–B-0 may be due to the inhibition of
2.2. Characterization
−
BH4 hydrolysis in the microemulsion, which would enhance the
The bulk composition was analyzed by inductively coupled
plasma optical emission (ICP; Varian VISTA-MPX). The amor-
phous structure was determined by both X-ray diffraction (XRD;
Rigaku D/Max-RB with CuKα radiation) and elective area elec-
tronic diffraction (SAED; JEOL JEM-2010). Surface morphology and
particle size were observed by transmission electron microscopy
(TEM; JEOL JEM2010). The size distribution was evaluated from
about 300 randomly selected particles. Thermal stability was deter-
mined by differential scanning calorimetry (DSC; Shimadzu DSC-
60) under N2 atmosphere, at a heating rate of 10 K min−1. The
active surface area (SCo) was measured by hydrogen chemisorption
acidity of the reaction solution and the formation of B-enriched
amorphous alloys [24]. Table 1 also shows that the SCo of Co–
B-x samples initially increased and then decreased with increas-
ing cyclohexane content in the microemulsion. The maximum SCo
was obtained for Co–B-0.25, obviously due to the smallest par-
ticle size (see Fig. 1). Co–B-50-30 displayed a higher SCo than
Co–B-0, due to the ultrasound effect, which can clean the cata-
lyst surface and also inhibit the particle agglomeration. Co–B-0.25
showed even higher SCo than Co–B-50-30, obviously due to its
smaller particle size. The XRD patterns presented in Fig. 2 show
that, similar to the Co–B-0 and Co–B-50-30 [14], all Co–B samples
synthesized in oil-in-water microemulsion (e.g. Co–B-0.25) exhib-
on a Quantachrome CHEMBET 3000 system, assuming H/Co(s) = 1
−20
and a surface area of 6.5 × 10
m2 per Co atom [22]. The hy-
◦
ited a single broad peak around 2θ = 45 indicative of amorphous
drogen temperature-programmed desorption (H2-TPD) curves were
obtained on the same instrument in argon flow at a ramping rate
of 20 K min−1. The surface electronic states were investigated by
X-ray photoelectron spectroscopy (XPS; Perkin-Elmer PHI 5000C
ESCA using AlKα radiation), and all Co–B samples were dried in
pure Ar atmosphere before measurements. The binding energy (BE)
values were calibrated using C 1s = 284.6 eV as a reference.
structure [25], which can be further confirmed by a successive
diffraction halo in an attached SAED image [26]. Treatment of the
fresh Co–B-0.25 sample (at 673 K in N2 for 2 h) resulted in the
appearance of various diffraction peaks corresponding to metallic
Co and crystalline Co–B alloy. The appearance of Co–B crystalline
phases during the crystallization process verified the formation of
an alloy between Co and B for the as-prepared Co–B. In addition,
our previous work also demonstrated the presence of Co–B bond
through EXAFS analysis [21]. The presence of a shoulder peak at
around 1.7 Å at the radial distribution functions obtained from the
Co χ(k)k3 edge by fast Fourier transformation suggests the forma-
tion of a Co–B bond. Furthermore, calculations based on the EXAFS
reveal that the Co–B bond length was much shorter than the sum
of Co radius and B radius, which also suggests the formation of
Co–B alloy. We infer that except for the crystallization, partial de-
composition of a Co–B amorphous alloy may occur in this process.
The DSC analysis (Fig. 3) reveals that the crystallization of the Co–
B-0 sample involved two steps: rearrangement of Co–B amorphous
2.3. Activity test
Liquid-phase hydrogenation of CMA was carried out in
a
200-ml stainless autoclave containing 0.30 g of catalyst, 4 ml of
CMA, 40 ml of EtOH, and 1.0 MPa of H2 at 373 K. The reaction
system was stirred vigorously (1000 rpm) to eliminate the diffu-
sion effects [23]. According to the PH drop with the reaction time,
2
both the specific activity [i.e., H2 uptake rate per gram of cobalt,
RmH (mmol h
g
−1)] and the areal activity [i.e., H2 uptake rate per
−1
Co
−1
m2 of the active surface area, RSH (mmol h
m
−2)] were calculated
Co