S. Sitthisa et al. / Journal of Catalysis 284 (2011) 90–101
91
From the point of view of fuel production, neither hydrogena-
tion nor decarbonylation is desirable. While the former does not
remove O, the latter loses C in the process. Hydrogenolysis to 2-
methylfuran (via C1AO1 hydrogenolysis) would be the most desir-
able product, since not only has intrinsically good fuel properties
LaB6). Before TEM analysis, the samples were reduced ex situ in
pure H (100 ml/min) at 450 °C for 1 h. The reduced samples were
then mixed with 2-propanol, sonicated, deposited onto the TEM
(Cu) grids, and dried. The BET surface area (S ) was measured by
conventional N physisorption on a Micromeritics ASAP 2010 unit,
2
g
2
(
high octane number, RON = 131, low water solubility, 7 g/L [15])
after evacuation at 350 °C for 3 h.
but also can be considered an archetypical product of the desired
reaction paths in bio-oil upgrading, i.e., removing O while keeping
a high C yield.
2.2. Catalytic activity measurements
Therefore, one of the goals of this study was to find a catalyst
that is able to produce 2-methylfuran while suppressing the for-
mation of furan. Our recent study showed that bimetallic alloys
can greatly alter the furfural reaction paths. For example, we
showed that adding Cu to Pd and forming bimetallic PdACu alloys
greatly suppresses the production of furan from furfural. However,
only furfuryl alcohol, rather that 2-methylfuran, was observed
The vapor-phase conversion of furfural over the NiAFe catalyst
series was evaluated in a tubular quartz reactor. In each run, a pel-
letized catalyst sample (size range: 250–425 lm) was placed at the
center of the reactor tube between two layers of glass beads and
quartz wool and pre-reduced in H2 flow (60 ml/min, Airgas,
99.99%) for 1 h at 450 °C. After reduction, the catalyst was cooled
down to the selected reaction temperature (210–250 °C) under
the same H2 flow. Prior to the reaction, furfural (Sigma–Aldrich,
99.5%) was purified by vacuum distillation to remove residues
and any oligomers formed during storage. The purified liquid
was kept under He atmosphere until its use in the reaction test.
A 0.5 ml/h (0.006 mol/h) flow of liquid furfural was fed continu-
ously from a syringe pump (Cole Palmer) and vaporized into a H2
stream of 60 ml/min. The reaction products were analyzed by on-
line GC (Agilent model 6890), using an HP-5 capillary column
and a FID detector. The carbon balance was checked in every run
and found to be higher than 95% in every case. The product yield
and selectivity for each product were calculated as follows:
[
16]. In the present work, we have investigated the conversion of
furfural over NiAFe bimetallic catalysts. The effect of adding Fe
on the catalytic properties of silica-supported Ni is investigated.
Samples with different Ni/Fe ratios were prepared and characterized
by XRD, TEM, TPR, and BET techniques to evaluate the structural
changes and the extent of alloy formation. Structure–activity rela-
tionships were investigated by combining the results of catalytic
activity measurements with characterization and theoretical DFT
(
Density Functional Theory) calculations.
2
. Experimental
mol of the product produced
Yield ð%Þ ¼
ꢁ 100
mol of furfural fed
2.1. Catalyst synthesis and characterization
mol of the product produced
ꢁ 100
mol of furfural consumed
The NiAFe/SiO
co-impregnation, using an aqueous solution containing both metal
precursors, Ni(NO O (98%, Alfa Aesar) and Fe(NO
98% Sigma–Aldrich). Prior to impregnation, the silica support
SiO , Hisil 233) was dried overnight at 120 °C. Then, the aqueous
2
catalysts were prepared by incipient wetness
Selectivity ð%Þ ¼
3
)
2
ꢀ6H
2
3
)
3 2
ꢀ9H O
(
(
2.3. Density functional theory calculations
2
solution was added to the support, keeping an incipient wetness li-
quid/solid ratio of 1 cc/g. The Ni loading was kept constant at
All DFT calculations were performed with the Vienna ab initio
simulation package (VASP) [17,18]. A spin-polarized GGA PBE func-
tional [19], all-electron plane-wave basis sets with an energy cutoff
of 400 eV, and a projector augmented wave (PAW) method were
adopted [20,21]. The Brillouin-zone of the p(4 ꢁ 4) lateral supercell
was sampled at 3 ꢁ 3 ꢁ 1 k-points using the Monkhorst–Pack
scheme [21]. First-order Methfessel–Paxton smearing [22] of
0.2 eV was employed in the integration to speed up the conver-
gence. The conjugate gradient algorithm was used in the optimiza-
5
.0 wt.% on all samples, while the Fe loading was varied from 0.0
to 5.0 wt.%. After impregnation, the catalysts were first dried over-
night at room temperature and then placed in an oven at 120 °C for
1
2 h. The oven-dried catalysts were finally calcined for 4 h at
5
00 °C, with a linear heating ramp of 10 °C/min, under 100 ml/
min flow of pure air. The catalyst powders thus obtained were
pressed at 1500 psi, crushed, and sieved to 40–60 mesh.
ꢂ4
The reducibility of the calcined samples was determined by
temperature programmed reduction (TPR). In these measure-
ments, 20 mg of a sample was placed in a quartz reactor and
heated at 30 °C/min up to 500 °C under a He flow of 20 ml/min,
and held at this temperature for 1 h. The reactor was then cooled
tion. The convergence threshold was set to 10 eV in total energy
ꢂ2
and 10 eV/Å in force on each atom. All reported energies are
B
extrapolated to k T = 0 eV.
The Ni(111) surface was modeled by a three-layer slab with the
bottom two layers fixed at their equilibrium bulk phase positions
(calculated lattice constant = 3.522 Å), while the top layer was al-
lowed to relax. The two successive slabs were separated by a
10 Å vacuum region to ensure that the adsorbate (i.e., furfural)
and the subsequent slab would not interact. The p(4 ꢁ 4) supercell
has a dimension of 9.962 Å ꢁ 9.962 Å ꢁ 14.068 Å to ensure that the
effect of adsorbate–adsorbate interactions between adsorbed fur-
fural molecules is negligible.
2
down to 30 °C and the sample exposed to a stream of 5% H /Ar
at a flow rate of 20 ml/min. Subsequently, the sample was heated
up to 800 °C at a heating rate of 5 °C/min. The variation in hydro-
gen uptake was monitored on a TCD detector as a function of tem-
perature. The molar H uptake per gram of sample was quantified
2
from the peak area in the TPR profiles and calibrated with a CuO
standard.
Several physical techniques were employed to characterize the
The bimetallic NiFe(111) alloy surface [i.e., Ni0.5Fe0.5(111), sub-
script is omitted thereafter for simplicity] was cleaved from an
optimized NiFe fcc unit cell (calculated lattice constant
a = c = 3.553 Å, b = 3.582 Å) [22] and was modeled in the same
fashion as the pure Ni(111) surface. The p(4 ꢁ 4) supercell has a
dimension of 10.050 Å ꢁ 10.091 Å ꢁ 14.114 Å. Our calculations
show that NiFe fcc unit cell with lattice constant a = b = c = 3.553
or 3.582 Å is slightly higher in energy (0.10 and 0.12 kcal/mol,
respectively) than the one we employed in the calculations with
structure of the NiAFe/SiO
terns (XRD) for all the samples were collected on a D8 Series II X-
ray Diffractometer (BRUKER AXS), using Cu K radiation generated
at 40 kV and 35 mA. The samples were reduced ex situ under pure
(100 ml/min) at 450 °C for 1 h prior to the measurements. The
2
catalysts. X-ray powder diffraction pat-
a
H
2
scans covered the 2h range from 30° to 60°.
Morphology and size of the NiAFe clusters were characterized
by transmission electron microscopy (TEM, JEOL model JEM-2100