D. Simon, B. Taylor / Journal of Catalysis 262 (2009) 127–133
129
phase composition by refinement of powder X-ray diffraction pat-
terns (Pan Analytical Xpert Pro, CuK ). Tungsten surface loading,
α
expressed in atoms per square nanometer, was calculated using
X-ray fluorescence data and BET surface area. X-ray refinements
◦
were performed on all materials following calcination at 500 C for
three hours and prior to activity testing.
The primary features of the X-ray diffraction patterns were
modeled using tetragonal zirconia and tungsten oxide. Monoclinic
zirconia, cubic zirconia and nickel tungstate were added to im-
prove the fit to the major features and account for peaks unas-
sociated with tetragonal zirconia. There was some difficultly in de-
termining the location of a predominance of the deposited nickel.
Since the nickel loading was known from X-ray fluorescence data,
an attempt was made to begin the refining of the complete pattern
containing nickel tungstate.
A significant amount of tungsten was not accounted for in the
tungsten oxide phase or the nickel tungstate phase. The exami-
nation of tungsten–zirconia materials (results not shown) showed
that in the absence of nickel, a zirconium tungstate phase was
present. The inclusion of this phase allowed for the accounting
of the deposited metal. In essence, the zirconium tungstate phase
modeled the interface between tungsten-containing phases and
the zirconia support. Similarly to the modeling of nickel phase,
X-ray fluorescence data provided starting compositions for the
structural refinements of the tungsten phases.
Fig. 1. Crystallographic phase content and initial n-hexane isomerization activity ver-
◦
◦
C
sus calcination temperature for catalysts Ni/WO3/ZrO2(Hf)-500 C through 800
◦
(288 C, 15 bar, LWHSV = 17 h−1, H2/HC = 0.7).
mote the formation of the more thermodynamically stable mon-
oclinic phase [4,5,7–12,14,15]. These literature accounts, however,
Despite a good overall fit to the experimental data, the three-
zirconia-phase model (tetragonal, monoclinic and cubic) did not
◦
generally refer to calcination temperatures above 800 C. The gen-
eration of tetragonal zirconia with increased calcination temper-
ature may also be an effect of tungsten surface loading. Sur-
face tungsten has been shown to stabilize the tetragonal zirconia
phase [14] and studies of hafnia/zirconia mixtures in the absence
of tungsten implied no regeneration of tetragonal zirconia follow-
ing formation of the monoclinic phase [16]. The elimination of
zirconia surface area due to sintering at high temperature may
result in a tungsten surface loading that ultimately stabilizes, in
this case, the tetragonal and cubic zirconia phases. The stabilizing
effect of tungsten is manifested in two respects. First, these materi-
als required higher calcination temperatures to produce crystalline
materials as compared to the tungsten-free case presented in refer-
ence [16]. Second, tungsten addition generated tetragonal zirconia
at the expense of monoclinic, but only with the aid of thermal
treatments.
◦
perfectly reproduce some of the small peaks (35–50 2θ) and
◦
shoulders (∼60 2θ) in the X-ray diffraction data. These minor dis-
crepancies led to the inclusion of an orthorhombic zirconia phase
and, in the case of amorphous materials, an additional monoclinic
phase. The data presented in this report utilizes X-ray fluores-
cence data coupled with X-ray diffraction data to assign nickel
tungstate (Space Group P12/c1) and zirconium tungstate (P213)
contents and includes up to five zirconia phases to fit the fea-
tures of the diffraction pattern (monoclinic = P121/c1, tetragonal =
P42/nm, orthorhombic = Pbc21 and cubic = P213). In an effort to
prevent over specification of the system, only the tetragonal phase
was modeled with Williamson–Hall strain.
3. Results and discussion
The orthorhombic phase appears as an intermediate phase dur-
ing the transition from monoclinic to tetragonal phase. Increases
in calcination temperature reduce the orthorhombic content in
favor of the catalytically active tetragonal phase. It is not clear
there is any real trend with calcination temperature in the cubic
phase content. Given the similar tungsten and nickel loadings for
each catalyst, the nickel tungstate and zirconium tungstate con-
centrations were constant. The appearance of tungsten oxide cor-
responded to calcination temperatures that resulted in a tungsten
surface loading of approximately two monolayers.
Catalytic activity increases with increasing tetragonal zirconia
content, a relationship previously asserted in the open literature
[4,5,7–12]. The initial isomerization rate appears to saturate at
tetragonal contents greater than approximately 40 wt%. Despite
being crystallographically distinct, the tetragonal and orthorhom-
bic phases are very similar. Their symmetry is essentially identical
except for a minor lengthening in one lattice parameter. A more
linear relationship between catalyst composition and activity can
be reproduced when initial isomerization activity is compared to
the sum of the tetragonal and orthorhombic phases. This makes a
case for the over specification of the model, given that orthorhom-
bic zirconia has not been identified as catalytically active in the
literature and activity has been shown previously to scale with
tetragonal content.
A number of Ni/WO3/ZrO2 catalysts, some containing hafnium
and/or aluminum and calcined at temperatures ranging from 500
to 900 C were prepared and are presented in Table 1. These cat-
alysts were prepared at essentially a constant weight of tungsten
with the surface tungsten concentration being set by the sintering
of the support at various calcination temperatures.
◦
3.1. The effect of hafnium
◦
◦
Catalysts Ni/WO3/ZrO2(Hf)-500 C through 800 C were pre-
pared from the comparatively inexpensive, hafnium-containing zir-
conia precursor. Shown graphically in Fig. 1, increasing calcination
temperature results in an increase in tetragonal zirconia content at
◦
the expense of the monoclinic. Ni/WO3/ZrO2(Hf)-500 C was best
fit using a short-range-ordered and a long-range-ordered mono-
clinic phase. If viewed as two separate monoclinic phases, the
long-range-ordered phase comprised 19.5% and the short-range-
ordered phase comprised 45.8% of the sample by weight. The
short-range-ordered monoclinic phase can be considered an amor-
phous phase given the low crystal domain size and its identifica-
tion only at the lowest calcination temperature. The elimination
of the monoclinic phase with thermal treatments is somewhat
contrary to literature accounts which show high temperatures pro-