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of the synthesis mixture was 1 TEOS : 0.27 TPAOH : 37 H2O. Aer
X-ray photoelectron spectroscopy (XPS) was conducted on an
being stirred for 3 h at 35 ꢀC, the resultant solution was heated at ESCALAB 250 (Thermo VG Corporation) using Mg Ka radiation
80 ꢀC in order to remove the ethanol generated during the (1253.6 eV, 15 kV, 10 mA, 150 W). The recorded spectra were
hydrolysis of TEOS and then water was added to maintain tted by a least square procedure to a product of Gaussian–
constant volume. Aer crystallization at 170 ꢀC for 3 days, the Lorentzian functions. The concentration of each element was
product was recovered by centrifugation and dried overnight at calculated from the area of the corresponding peak.
100 ꢀC. Finally, the template was removed by calcination in static
air at 540 ꢀC for 6 h.
The elemental analysis of catalysts was carried out on a
Perkin Elmer OPTIMA 2000DV ICP Optical Emission
Spectrometer.
2.2 Preparation of Pd@Hol S-1 and Pd–Cu@Hol S-1
2.4 Catalytic tests
Pd/S-1 was synthesized by the incipient-wetness impregnation
method. In brief, the calcined silicalite-1 was impregnated with
an aqueous solution of H2PdCl4, aer drying overnight at
All commercially available reagents (from Acros, Aldrich, Fluka)
were used without further purication. All reactions were
carried out in air. NMR spectra were recorded on a Brucker
AdvanceII 400 spectrometer using TMS as an internal standard
(400 MHz for 1HNMR). All products were isolated by short
chromatography on a silica gel (200–300 mesh) column using
petroleum ether (60–90 ꢀC). Compounds described in the
literature were characterized by 1H NMR spectra and compared
to reported data.
A mixture of aryl bromides (0.25 mmol), phenylboronic acid
(0.375 mmol), K2CO3 (0.5 mmol), catalysts (1.6 mol%), and
EtOH/H2O (1 mL/1 mL) was stirred at 80 C in air for the indi-
cated time. The reaction mixture was added to brine (15 mL)
and extracted with ethyl acetate (4 ꢁ 10 mL). The solvent was
concentrated under vacuum, and the product was isolated by
short column chromatography on silica gel.
ꢀ
100 ꢀC; the product was calcined in static air at 500 C for 4 h.
The Pd loading on the Pd/S-1 was 0.97 wt%, as measured by
inductively coupled plasma (ICP) mass spectrometry.
The as-prepared Pd/S-1 was treated with 0.3 M TPAOH
(20 mL of solution per gram of zeolite) at 170 ꢀC for 72 h, aer
dried overnight at 100 ꢀC and calcined in static air at 500 ꢀC
for 4 h, the Pd@Hol S-1 was obtained. The Pd loading on
the Pd@Hol S-1 was 1.3 wt%, as measured by ICP mass
spectrometry.
ꢀ
Pd–CuO binary metals (oxide) encapsulated in the hollow S-1
were prepared by the similar method with single metal, which
used H2PdCl4 and CuCl2 as Pd and Cu source, respectively, and
co-impregnation method to synthesize Pd–CuO/S-1. The as-
prepared Pd–CuO/S-1 was treated with 0.3 M TPAOH (20 mL
ꢀ
of solution per gram of zeolite) at 170 C for 72 h, aer drying
overnight at 100 ꢀC and calcining in static air at 500 ꢀC for 4 h,
the Pd–CuO@Hol S-1 was obtained. The Pd and Cu loading on
the Pd–CuO@Hol S-1 was 1.2 and 0.82 wt%, respectively, as
measured by ICP mass spectrometry.
3 Results and discussion
Fig. 1a shows a typical TEM image of the prepared Pd/S-1, which
clearly exhibits that palladium nanoparticles are located on the
crystal surface. Aer TPAOH treatment, a large regular hollow
void was created in the interior of the silicalite-1 and the
2.3 Characterization
Powder X-ray diffraction (XRD) patterns were recorded on a thickness of the shell was about 20 nm. The zeolite nanocubes
Rigaku Smartlab diffractometer using a nickel-ltered CuKa X- were still single-crystals and the palladium particles with 11.1
ray source at a scanning rate of 0.02ꢀ over the range between 5ꢀ nm in average particle size were encapsulated in the large cavity
and 80ꢀ.
(Fig. 1b). Fig. 1c and d are images of this sample with high
Transmission electron microscopy (TEM) images were taken resolution and the zeolite lattice fringes align clearly parallel to
on a Tecnai G2 20 S-twin instrument (FEI Company) with an each other, conrming the nanocubes are still single-crystals.
acceleration voltage of 200 kV. The samples for TEM analysis From Fig. 1d, it can be seen that the lattice fringes are not
were prepared by dipping the carbon-coated copper grids into aligned parallel to each other, conrming the Pd particle is
ethanol solutions of the samples and drying at ambient agglomerated from smaller clusters. The lattice spaces are
condition.
measured to be 0.194 and 0.225 nm, which matches the values
Ar isotherms were measured in a Quantachrome autosorb- of the d-spacing of Pd (200) and Pd (111), respectively (JCPDS:
iQ2 gas adsorption analyzer at 87 K. Prior to the measure- 46-1043). The energy-dispersive X-ray spectrometry (EDX)
ment, the samples were degassed in vacuum at 300 ꢀC for 10 h. elemental analysis along the line shown in Fig. 1e shows the
The Brunauer–Emmett–Teller (BET) method was applied to core rich in Pd and the shell rich in Si and O, thereby con-
calculate the total surface area (SBET), while the t-plot method rming that palladium is mainly located in the core of hollow
was used to discriminate between micro- and meso-porosity. In silicalite-1 (Fig. 1f).
the t-plot, the reported mesopore surface area (Smeso) consists of
contributions from the outer surface of the particles as well as During TPAOH treatment, the silicate oligomers are leached
mesopores and macropores. from interior of the crystal and recrystallize at the surface of
The Pd@Hol S-1 formation process is shown in Fig. 2.
Scanning electron microscopy (SEM) images were obtained silicalite-1 crystal. In this process, the palladium particles move
on a Hitachi S-5500 instrument with an acceleration voltage of from surface of the crystal to the interior of cavity, just like the
3 kV. Some samples were sputtered with a thin lm of gold.
process of cell phagocytosis (Fig. 2 step I and step II). During the
40298 | RSC Adv., 2015, 5, 40297–40302
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