2
4
L. Matachowski et al. / Applied Catalysis A: General 450 (2013) 19–27
−
synthesized’ Cs (Br) and Cs (I) samples were close to the stoichio-
metric ratio being near to 1. After annealing the samples at 353 and
be expected that interactions of Cl ions with the surface protons
2
2
−
of primary particles could be the strongest whereas those of I ions
573 K both atomic ratios decreased dramatically to about 0.046 and
0.012, respectively. It demonstrates that already during heating at
353 K almost all bromide or iodide ions were removed. These results
the weakest. It was previously showed that the addition of chloride
ions to the Cs (C) sample strongly influenced its structure [14]. The
2
presence of chloride ions in the colloidal solution of [Cs (C) + HCl] or
2
clearly confirm the previous conclusion that halogen ions play a
vital role in the formation of porous structure of studied samples
during their synthesis.
Cs (Cl) samples caused the formation of larger colloidal particles in
2
both cases [14]. This could be a result of interactions of chloride ions
with primary particles of these samples before aggregation process
or penetration of chloride ions into already formed colloidal parti-
The morphology of Cs (Br), Cs (I), [Cs (C) + HBr] and Cs2.5(C)
2
2
2
samples was studied by scanning electron microscopy technique
and obtained micrographs are displayed in Fig. 5. All samples, which
are characterized by mesoporous structure, form spherical par-
cles of the Cs (C) sample. Similar phenomenon was observed after
2
addition of HBr to the Cs (C) sample.
2
However, the addition of HBr to the colloidal solution of Cs (Cl)
2
ticles consisting of much smaller primary particles. The Cs (Cl)
sample also exhibits similar morphology, showing loosely aggre-
gated almost spherical particles composed of small nanocrystallites
sample practically did not change the specific surface area whereas
some changes in the porosity appeared, as was described above
(Table 2). Because the energy of H Cl bond is much higher than that
of H Br bond the exchange of chloride ions by bromide ions can be
2
[
14]. Hence, the morphology of all samples prepared with cesium
halides differ entirely from that of the Cs (C) sample but is similar
excluded. It seems that the results obtained for the [Cs (Cl) + HBr]
2
2
to that of the Cs2.5(C) salt [14,27]. According to the literature data
sample can indicate the co-absorption of bromide ions, when they
are present in the colloidal solution. This could be a result of
the penetration of bromide ions into colloidal particles. Such pro-
[
27] and our previous results, a highly compact structure of the
Cs (C) sample possesses smooth surface and any primary particles
2
cannot be noticed. However, the Cs (C) salt after addition of HBr
cess could change the porosity of [Cs (Cl) + HBr] sample, which is
2
2
can completely change its morphology because of the formation of
sphericalparticlescomposedof aggregatedprimaryparticleswhich
reflected by the increase of mesopores area accompanied by the
decrease of micropores area. However, this phenomenon seems to
be more complicated and its detailed explanation requires further
studies.
are observed in [Cs (C) + HBr] sample (Fig. 5). It can be supposed
2
−
that after the precipitation process of the Cs (C) sample, the Br
2
ions can penetrate and decompose its compact structure and after
self-organization process, can form mesoporous structure consist-
ing of spherical particles. This shows how halides ions can influence
Thus, it seems to be obvious that halide ions play an important
role in the aggregation of primary particles influencing the forma-
tion of mesoporous structure of the studied samples. On the other
hand, taking into account the ionic radius of halogens (Table 2), it
the formation of mesoporous structure of Cs HPW12O40 salt.
2
−
Our previous studies [14] showed that Cl ions were easily
is easy to explain how they influence the porous structure of the
−
removed from the ‘as synthesized’ Cs (Cl) sample. It was demon-
Cs HPW12O40 salt. The presence of the smallest Cl ions causes that
2
2
strated that this sample was ‘free’ of chloride ions after heating at
the structure with the highest contribution of micropores is formed.
−
−
4
53 K. The Cl atoms were also not detected by EDXS-SEM technique.
When Br or I ions interact with primary particles in Cs (Br) and
2
This suggested that vacuum pre-treatment of the sample prior to
microscopic studies caused the release of chloride ions. In the case
Cs (I) samples, the aggregated structure of the highest contribution
of mesopores is created (Table 2).
2
of Cs (Br) and Cs (I) samples expected values of Br and I atoms
After calcination of the Cs (Cl), Cs (Br) and Cs (I) samples at
2
2
2 2 2
were equal to about 5 and 8 wt%, respectively. However, their con-
tent detected by EDXS measurements was much lower. It has been
assumed that Br and I ions stayed to some extent in the structures
of both samples because their higher atomic masses compared to
chloride ions. This is consistent with the ICP-AES results presented
above which showed much higher content of halogens in the ‘as
synthesized’ samples and practically lack of halogens after their
annealing at 573 K.
573 K for 2 h, their specific surface area decreases and also some
changes in the pore distribution diagrams can be observed (Fig. 4).
Thermal treatment induces the most dramatic changes in the struc-
ture of the Cs (Cl) sample. Strong reduction in surface area (from
2
2
78.2 to 4.2 m /g) is accompanied by remarkable changes in the
porous structure. As Fig. 4 shows, wide mesopores with the max-
imum of about 6.2 nm in diameter vanish almost completely after
calcination, whereas some new narrower mesopores of 3.8 nm in
The role of halogen ions could be explained using a model
described by Okuhara et al. [27] which suggested that the pore
diameter are created. For the annealed Cs (Br) and Cs (I) samples,
2 2
the micropores structure (volume and area) practically does not
change and mesopores of 3.8 nm in diameter are preserved. The
contribution of the larger mesopores, of diameter within 6–10 nm
structure of CsxH3 PW12O40 salt precipitated with Cs CO3 was
−x
2
greatly dependent on the Cs/Keggin anion ratio. The final tex-
ture of these samples was formed via slow aggregation of primary
crystallites during heating and evaporation of the solution. The
crystalline sample of the Cs2.5H0.5PW12O40 was consisted of loosely
aggregated fine crystallites forming both micro- and mesopores.
In contrast, the Cs HPW12O40 salt (prepared with Cs CO ) was
range, decreases to some extent especially in the case of Cs (Br)
2
sample. For the latter sample, ca. two-fold decrease in surface
2
area appears (from 48.5 to 24.9 m /g). The changes are defini-
tively less pronounced for the Cs (I) sample as its surface decreases
2
2
only slightly from 39.3 to 30.0 m /g. The recrystallization process
2
2
3
consisted of dense aggregates of fine crystallites, what resulted in
a lack of porosity.
According to our previous results, at the beginning of acidic
cesium salts precipitation in water solution, primary particles are
formed and their surfaces are enriched by the protons [31,32].
resulting in the formation of larger crystallites (Table 1) may be
responsible for the observed structural changes. Alike, the meso-
pores of 3.6 nm in diameter are present in the Cs2.5H0.5PW12O40
salt (Fig. 4). As previously described, the mesoporous structure of
the Cs2.5(C) is stable under heating at 573 K in vacuum [27]. Data
presented by Zhang et al. [34] demonstrated that the mesoporous
When the Cs HPW12O40 salt is precipitated by Cs CO gaseous CO
2
2
3
2
is liberated from the colloidal solution, whilst when CsCl, CsBr or
CsI are used as the reagents, the HCl, HBr or HI may stay in the solu-
tion influencing the aggregation of primary particles. Therefore, the
structure of CsxH3 PW12O40 samples with x ≥ 2.2 did not change
−x
even after catalytic reaction performed at 653 K.
At this point, a question may be raised as to why the mesopores
of 3.6–3.8 nm in diameter are resistant for annealing at 573 K in
−
−
−
interaction of Cl , Br or I ions with surface protons of primary
particles should be taken into consideration. When ionic radius
Cs (Br), Cs (I) as well as in Cs2.5(C) samples. It was reported that in
2
2
−
−
increases from Cl to I (Table 2), the energy of H Cl > H Br > H
I
the structure of the Cs2.5H0.5PW12O40 salt the closest packed aggre-
gates formed the voids and necks, the latter with the size of about
bond decreases (432, 366 and 298 kJ/mol, respectively [33]). It can