330
F. Regali et al. / Applied Catalysis A: General 469 (2014) 328–339
Fig. 1. Simplified reaction network.
any other impurity may affect the NH3 adsorption and desorption
processes.
The contributions of the two possible routes of formation of
cracking products, i.e. bifunctional and hydrogenolytic, were esti-
mated by the simple reaction network model depicted in Fig. 1.
In this scheme, all reaction steps were considered first-order and
irreversible [22,26]. The equations describing the concentrations
profiles of the different product lumps as functions of the contact
time ꢀ (or the inverse of WHSV) are reported below.
Pyridine adsorption FTIR measurements were performed in an
ATI Mattson FTIR spectrometer. Approximately 0.20 g of sample
was pressed into a self-supporting thin wafer and placed in the FTIR
cell. The sample was pretreated in high vacuum (∼10−5 mmHg) at
450 ◦C for 1 h. The temperature was then lowered to 100 ◦C and
a background spectrum was recorded. Pyridine was adsorbed on
the sample at its ambient vapor pressure in flowing helium at
100 ◦C for 30 min. Spectra of adsorbed pyridine were recorded at
100 ◦C for 50 min; three measures were performed, after evacua-
tion for 1 h at 150, 250 and 350 ◦C, respectively. Spectral bands at
+k
)ꢀ
Cn-C16 = Cn-C160 e−(k
bif
hyd
ꢀ
ꢀ
ꢀ
−kbifCn-C160 (e−k
− e−k
)
2
bif
CMB
=
kbif − k2
Cn-C16 kbifk2e−k
Cn-C16 kbifk2(kbife−k − k2e−k
+ k3e−k
(kbif − k2)(kbif − k3)(k2 − k3)
− k3e−k
)
ꢀ
ꢀ
ꢀ
ꢀ
3
2
2
bif
bif
(kbif −0k3)(k2 − k3)
0
CDB
=
−
CCP = Cn-C16 − Cn-C16 − CMB − CDB
0
1545 cm−1 (Brønsted) and 1450 cm−1 (Lewis) were considered for
the estimation of acid site concentrations, using the molar extinc-
tion coefficients calculated by Emeis: 1.67 for the 1545 cm−1 band
and 2.22 for the 1450 cm−1 band [25].
Selectivity/conversion curves for the different product lumps
were obtained by non-linear regression of the experimental data.
First-order rate constants are given as kbif (bifunctional) and khyd
(hydrogenolysis), respectively.
The effect of H2 partial pressure was studied on a stable 1.2-
wt% Pt/Siral 40 catalyst. Experiments were performed at constant
n-hexadecane WHSV (18 h−1) and total pressure (30 bar), replacing
a part of the hydrogen feed with helium. The degree of vaporiza-
tion of n-hexadecane was considered to calculate hydrogen partial
pressure, which varied between 17.4 and 29.2 bar. The same set
of experimental points was repeated in the presence of pyridine,
mixed with n-hexadecane (0.8 wt%) in the feed vessel. The sys-
tem was run at the reference conditions until catalytic activity
reached steady state. Experimental points at reference conditions
were repeated to ensure that no further deactivation occurred
during the experiments with varying hydrogen partial pressure.
Apparent reaction orders with respect to hydrogen were calcu-
lated by linearization of the bi-logarithmic plot of reaction rates
versus inlet hydrogen pressure. Rates were approximated with
space–time yields, not considering the change in composition along
the reactor.
2.3. Catalytic testing
Hydroconversion of n-hexadecane (>99%, for synthesis, Merck
820633) was performed in a stainless steel tubular reactor, allow-
ing operation up to a pressure of 80 bar. The reaction and analysis
system has been described in detail elsewhere [26]. Briefly, the n-
hexadecane liquid feed was supplied by means of a HPLC pump, and
mixed with hydrogen prior to entering the reactor, which operated
in co-current downflow mode. The reaction products were sepa-
rated in a gas–liquid separator at room temperature. The product
gas was sent, through a downstream pressure control valve, to an
on-line gas chromatograph equipped with an Alumina PLOT col-
umn. The liquid products were sampled and analyzed off-line with
an HP-5 column.
Before each experiment, approximately 3 g of catalyst, previ-
ously sieved to a particle size of 90–200 m and dried overnight,
was loaded into the reactor. The catalyst was activated in situ in
hydrogen flow (50 N ml/min/gcat) at 400 ◦C for 2 h, by raising the
temperature with a heating ramp of 5 ◦C/min. Thereafter the system
was pressurized in hydrogen and stabilized at the desired reac-
tion temperature and pressure. The conditions used were T = 310 ◦C,
P = 30 bar, H2/n-C16H34 inlet ratio = 10 mol/mol. The total conver-
sion of n-hexadecane was varied by varying the weight hourly space
velocity (WHSV) between 0.25 and 18 h−1. Under these conditions
the distribution of cracking products was practically symmetric
throughout the full conversion range, i.e. overcracking was avoided.
Conversion of n-hexadecane is defined as 1 − Fn-C16,out/Fn-C16,in
where F is the molar flow. The hydroconversion activity is reported
as the pseudo-first-order reaction rate constant for the disappear-
ance of n-hexadecane, calculated assuming plug flow behavior.
Selectivities are reported on a carbon atom basis, as moles of C
in product per mole of C of converted n-hexadecane. The products
of n-hexadecane hydroisomerization/hydrocracking were grouped
into three main lumps: mono-branched hexadecanes (MB), di-
or multi-branched hexadecanes (DB), and cracking products (CP).
3. Results
3.1. Catalyst characterization
The textural properties of the catalysts are presented in Table 1.
Addition of platinum on the Siral 40 material caused a slight
were observed for varying platinum loading. The porous struc-
ture remained practically unaffected. On Siral 1, characterized by
a smaller surface area compared to the Siral 40 (227 m2/g vs.
440 m2/g), the effect of 0.33-wt% platinum was negligible.
Hydrogen-chemisorption analyses (Table 2) showed that plat-
inum particles were well dispersed on all catalysts, with dispersion
values ranging from 120% to 61%, with dispersion decreasing as
platinum loading increased. Values of dispersion higher than 100%
are of course physically impossible, and are due to the assump-
tion of a constant hydrogen adsorption stoichiometry coefficient
equal to 1. It has been shown that adsorption stoichiometry on