C. Sepúlveda et al. / Applied Catalysis A: General 475 (2014) 427–437
429
The total acidity measurements of the carbon supports and cat-
alysts were carried out potentiometrically by titrating a suspension
of carbon in acetonitrile with n-butylamine using an Ag/AgCl elec-
trode [12].
900
750
600
450
300
150
0
GAC
CGran
X-ray photoelectron spectra (XPS) of sulfide catalysts were
obtained on an Escalab 200R electron spectrometer using Mg K␣
(1253.6 eV) as the excitation source. Spectra were recorded at 45◦
take-off angles by a concentric hemispherical analyzer operating in
the constant pass energy mode at 50 eV. Under these conditions the
Au 4f7/2 line was recorded with 1.34 eV FWHM at a binding energy
of 84.0 eV. The spectrometer energy scale was calibrated using Cu
2p3/2, Ag 3d5/2 and Au 4f7/2 photoelectron lines at 932.7, 368.3 and
84.0 eV, respectively. Charge referencing was done against adventi-
tious carbon (C 1s 284.8 eV). The catalyst samples were pre-sulfided
ex situ under flowing 15 vol.% H2S/N2 at 673 K for 4 h. The samples
were then cooled to room temperature, flushed with N2 and stored
in flasks containing N2, and then transferred to the pre-treatment
chamber of the spectrometer. Then, sulfide catalysts were mounted
on a sample holder and kept overnight in high vacuum in the
preparation chamber before they were transferred to the analy-
sis chamber of the spectrometer. The C1s, S2p and Re4f energy
regions were scanned with several sweeps until a good signal-to-
noise ratio was observed. The pressure in the analysis chamber was
maintained lower than 5 × 10−9 mbar.
0,0
0,2
0,4
0,6
0,8
1,0
Relative pressure (P/Po)
Fig. 1. N2 adsorption–desorption isotherms at 77 K of activated carbon supports.
taken periodically during the reaction and identified by Perkin-
Elmer Clarus 680 a coupled to GCMS-SQ8T equipped and quantified
by a Perkin-Elmer (Clarus 400) gas chromatograph equipped with
a Flame Ionization Detector (FID) and a CP-Sil 5 column (Agilent,
30 m × 0.53 mm × 1.0 m film thickness). The specific rate for the
total conversion of guaiacol was deduced from the initial slope of
conversion vs. reaction time plot. The intrinsic rate was calculated
from the specific rate according to the following equation:
Spectra were decomposed with the Casa XPS program (Casa
Software Ltd., UK) by using a Gaussian/Lorentzian (90/10) prod-
uct function after subtraction of a linear background. Atomic
ratios were calculated by using peak areas normalized on the
basis of acquisition parameters, sensitivity and transmission factors
provided by the manufacturer, and determined from the corre-
factors, with a precision of 7%.
The theoretical dispersion of the Re phase over the microporous
and micro–mesoporous catalysts were calculated according to the
model described by Kerkhof and Moulijn [13]. The model assumes
that the catalyst consists of sheets of the support of thickness t
with cubic crystallites of the supported phase of a dimension c in
between. For a monolayer dispersion of the supported metal phase,
the predicted XPS metal (Im) to support (Is) intensity ratio can be
expressed as in equation (1):
Sr
Ir =
× N
(2)
nRe
where Ir is the intrinsic rate (i.e. molecules of guaiacol transformed
per Re atom per second and expressed in molec. Re at−1 s−1), and Sr
is the specific rate (i.e. the moles of guaiacol−tr1ansformed per gram
of catalyst per second and expressed in mol gcat s
−1), nRe represents
the number of Re atoms per gram of catalyst, and N is the Avogadro
number. The deoxygenation (HDO) rate was calculated from the
conversion of guaiacol to O-free compounds (benzene, cyclohex-
ane, cyclohexene and methylated analogs). The HDO rate was also
calculated according to Eq. (2), where the specific activity repre-
sents the conversion of guaiacol into deoxygenated compounds.
On the other hand, the selectivities (%) were determined at 10% of
guaiacol conversion.
Im
Is
(m/s)(Dm/Ds)(ꢁm/ꢁs)(ˇs/2)[1 + exp(−ˇm)]
[1 + exp(−ˇm)]
=
(1)
where ˇs = t/ꢀs (ꢀs is the support photoelectron escape depth, t is
the thickness of the support), ˇm = t/ꢀm (ꢀm is the metal photoelec-
tron escape depth) and m/s is the metal/support atomic ratio. Ds and
Dm are the detector efficiencies, and ꢁs and ꢁm are the cross sections
for photoelectron emission of the support and metal, respectively.
The thickness of the sheets (t) can be estimated from the density
and the surface area of the support: t = 2/ꢂsS.
3. Results and discussion
3.1. Supports characterization
The nitrogen adsorption–desorption isotherms for the carbon
supports are shown in Fig. 1. The isotherms of the supports are
of microporous materials [14]. However, at high relative pres-
sure an increase in the amount of the nitrogen adsorbed, due to
is more prominent in the CGran support. Also, Fig. 1 shows that
both isotherms displayed a type H4 hysteresis loop, suggesting
lamellar-shaped pores. The textural properties of the supports are
summarized in Table 1: CGran support displayed higher surface
area than the GAC support. Also, the micropore volume (Vo) of the
volume.
2.3. Catalytic tests
The HDO of guaiacol was carried out in an autoclave reactor
operating in batch mode. The liquid reactant feed, consisting of
guaiacol (0.232 mol L−1) in n-dodecane (80 mL) with hexadecane
(0.0341 mol L−1) as an internal standard, was introduced into the
reactor. Then, approximately 0.200 g of freshly sulfided catalyst was
added. The system was closed, and to avoid any air contamination,
N2 was bubbled through the solution for 10 min. Still under N2 the
reactor was heated to the reaction temperature of 573 K under stir-
ring. When the reaction temperature was reached, the pressure was
adjusted to 5 MPa by H2 introduction into the reactor and kept con-
stant during the course of the experiment. Condensed samples were
Differences in the chemical nature of the oxygen functional
groups of the supports were determined by means of TPD profiles,
as shown in Fig. 2. The CGran support displayed a weak peak at