from the reduction of the pore size to 6.2 nm. The BET surface
area and pore volume of Pd/MSCN were calculated to be
345 m2 gÀ1 and 0.46 cm3 gÀ1, respectively. These phenomena
can be attributed to 5 wt% Pd supporting inside the channels
of the MSCNs, which leads to a partial blocking of the pores.
The 2-D hexagonal mesostructures of MSCN and Pd/MSCN
samples were confirmed by XRD (ESIw). For Pd/MSCN, the
face-centered cubic (fcc) Pd lattice is present, as confirmed by
several peaks at 2y = 40.1, 46.5, and 68.01 in wide-angle XRD
patterns (ESIw). It is interesting to find by TEM (Fig. 2(A)) a
narrow Gaussian distribution of Pd particle size of about
3.2 nm, which is consistent with the results either obtained
from H2 titration or estimated through the Scherrer formula.
Compared with the Pd particle size on Pd/AC, as shown in
Fig. 2(C), the dispersion of Pd on Pd/MSCN is much higher.
The possible reason for the high dispersion of small-size metal
particles is the unique hybrid nature of the carrier. In the
carrier, the silica and carbon components uniformly disperse
on the pore wall to construct a continuous framework.7 Pd ions
may be selectively adsorbed on the surface of hydrophilic SiO2,
whose silanol groups can interact with the Pd ions, while the
inert, hydrophobic component carbon possibly plays a role to
separate them. XPS results (ESIw) indicate that the intensity of
Pd for Pd/MSCN is much stronger than that for Pd/AC, which
can be ascribed to higher dispersion of Pd on Pd/MSCN and
more Pd atoms exposed to the surface.
Fig. 3 HDC of 4-CP over 5 wt% Pd/MSCN (Pd : Cl = 1 : 100 mol) at
258 and 278 K under ordinary hydrogen pressure (balloon) using Et3N
(1.0 equiv. vs. the number of chlorine atoms); 4-CP concentration:
5 mmol per 50 ml methanol solution; sp: the addition of 0.25 equiv.
Et3N vs. the number of chlorine atoms per 60 min.
of Pd/AC is low at low temperature, and the TOF is 1.9 minÀ1
at 278 K and 21.7 minÀ1 at 313 K.
The activity of Pd/MSCN for the HDC of 2,4-DCP is shown
in Fig. 4. Considering the conversion of 2,4-DCP to 2-CP and
4-CP, which, in turn, are converted into phenol, occurring on
Pd/MSCN, the corresponding TOF is related to the total number
of C–Cl bonds transformed and is estimated to be 3.2 minÀ1
(Table 1), higher than the TOF for the conversion of 4-CP to
phenol. This is in contradiction with the fact that the additional
Cl substituent is deactivating, 9 implying that there may be some
factor(s) that will affect the reaction process. The equivalence of
the initial 2,4-DCP consumption in the production of 2-CP
(5.9 mmol gÀ1 minÀ1) and phenol (2.7 mmol gÀ1 minÀ1) to the
HDC rate (8.6 mmol gÀ1 minÀ1) indicates that the reaction
proceeds predominantly in a stepwise fashion, converting first to
2-CP and then to phenol. However, a significant amount of 4-CP
was formed (with 10% selectivity) on Pd/AC, although its TOF
for 2,4-DCP is 1.1 minÀ1 (Table 1).
The evaluation of the activity of Pd/MSCN for the HDC
of 4-CP and 2,4-DCP was carried out under a hydrogen
atmosphere within the temperature range of 258–313 K
(ESIw). The conversion of 4-CP on Pd/MSCN at different
temperatures as a function of time is shown in Fig. 3, and the
turnover frequency (TOF) for the HDC of 4-CP is listed in
Table 1. At 258 K, the TOF for Pd/MSCN is 2.6 minÀ1, clearly
surpassing the TOF for Pd/AC of 0.9 minÀ1, and it takes
600 min for the HDC of 4-CP on Pd/MSCN to complete in the
presence of Et3N (1.0 equiv. vs. the number of chlorine atoms),
which can combine with the HCl formed during the reaction
so as to remove Cl species from Pd active sites. This result
confirms for the first time that nano-sized Pd particles
supported on MSCN are highly active for HDC in the liquid
phase at 258 K. Phenol was the only product, and no
formation of other species was observed. With raising
temperature, the activity of Pd/MSCN for HDC increases
obviously, and the TOF reaches 2.8 minÀ1 at 278 K and
25.0 minÀ1 at 313 K. Under similar conditions, the activity
Taking the solubility of H2, which has no significant change
within the range of 258–313 K, the temperature dependence of
the initial reaction rate can be used to generate apparent activa-
tion energies. The associated Ea value (with 95% confidence
limits; ESIw) of the HDC of 4-CP is 15.6 kJ molÀ1 within this
temperature range on Pd/MSCN, markedly lower than the value
(40.8 kJ molÀ1) obtained on Pd/AC (Table 1), and even lower
than the value (24.8 kJ molÀ1) that has been quoted for the HDC
of 4-CP promoted by Pd on carbon cloth over the temperature
range 303–358 K.10 This comparison indicates that nano-sized
Pd catalyst supported on MSCN is highly active for the HDC of
chlorophenols.
When Et3N is added in batches of 0.25 equiv. vs. the number
of chlorine atoms per 60 min for the HDC of 4-CP, the
conversion of 4-CP on Pd/MSCN is promoted greatly within
the range of the amount of Et3N added equivalent to the
formed HCl during the HDC, and the TOF at 258 K increases
up to 4.9 minÀ1 from 2.6 minÀ1. Meanwhile, the corres-
ponding Ea is 15.2 kJ molÀ1 within the range of 258–313 K
(ESIw), almost as same as the value for the HDC with one
batch addition of Et3N. This phenomenon indicates that Pd
atoms could interact with Et3N so as to be unavailable to
Fig.
2 TEM images of the mesoporous supported palladium
catalysts: fresh Pd/MSCN (A); used Pd/MSCN (B); Pd/AC (C).
ꢀc
This journal is The Royal Society of Chemistry 2009
Chem. Commun., 2009, 4438–4440 | 4439