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S. Selvakumar et al. / Applied Catalysis A: General 372 (2010) 130–137
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Fig. 3(a) shows that the intensity of the 3740 cm band, arising
nature of the acid sites in a catalyst sample may depend
considerably on the cation associated with a metal triflate, as
can be seen clearly in Fig. 5(B). A pair of strong IR bands observed at
1614 and 1454 cm in the case of pyridine adsorption over zinc
triflate loaded SBA-15 [Fig. 5(B), (e)] arises due to well reported 8a
duetotheO–HstretchingoftheisolatedsilanolsinSBA-15,decreases
progressively with the increasing loading of the zinc triflate. No shift
was, however, observed in the frequency of this band as a result of
triflate loading (figure not shown). This behavior has been attributed
earliertotheinteractionoftriflatemoleculeswithsurfaceOHgroups;
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n(C–C) and 19b
n(C–C) vibrations of pyridine adsorbed at the Lewis
3 3
both the (SO ) and the (CF ) groups are shown to participate
acid (designated as L1) sites [15,25]. Another pair of bands
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1
individually in such interactions [19–22]. Various possible binding
observed at 1640 and 1546 cm in this figure is known to arise
due to the vibrations of pyridine molecules bound at bridge-
ꢁ
modes of triflate ion (CF
SO
3 3
) at the surface silanols, viz.
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monodentate, bidentate, tridentate and tetradentate, have also been
postulated in an earlier publication [4]. We may, however, point out
that an electronic interaction between the triflate ions with the
surfacesitesofSBA-15islikelytochangethefrequencyofthebonded
guestmolecules,ashasbeendiscussedinourearlierpublication[23].
bonded Br o¨ nsted (B) sites. The band appearing at 1491 cm is
attributed to the adsorption of pyridine at both the Lewis and
Br o¨ nsted acid sites. In the case of SBA-15 samples containing the
triflates of Y, La and Ce, instead of a pair of bands at 1614 and
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1
1454 cm
we observe two low intensity bands at 1597 and
1
Similarly, the
n(OH) frequency is expected to increase because of the
1447 cm [Fig. 5(B), (b–d)], similar to the IR bands observed for
pure SBA-15 [Fig. 5(B), (a)]. As discussed in our earlier paper in
detail [25], these bands are attributable to weak Lewis acid sites
(designated as L2), a characteristic feature of the siliceous
mesoporous silicates having a weak acid character. The higher
increased electron density along the hydroxyl group. Therefore, the
spectroscopyresultsofourstudycannotbeascribedtoanyelectronic
interactionbetweenthetriflateionsandthesurfacehydroxylgroups.
Ontheotherhand, theresultsreportedhereareakintothefindingsof
our previous studies on the occlusion of small molecules, such as
methanol, benzene and cyclohexane, in the channels of micro- and
mesoporous silicates [23,24]. Based on the detailed discussion
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intensity of the 1546 cm
band in curves (b–d) of Fig. 5(B)
indicates that the samples loaded with the triflates of La, Ce and Y
exhibit much higher Br o¨ nsted acidity and at the same time a lower
Lewis acidity, as compared to the zinc triflate containing sample.
The ratio B/L (L1 or L2) follows a trend La (9.5) > Y (4.7) > Ce
(3.0) = Zn (0.3), and this matches well with the catalytic activity
results of Fig. 7.
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presented in these references, the removal of 3740 cm band on
triflate or pyridine loading can be attributed to the physical
perturbation or the displacement of the –OH groups. This may
facilitate a weak van der Waals type interaction between the two
displaced hydroxyl groups, leading to the progressive removal of
The important role played by the metal cation in an occluded
triflate molecule becomes apparent when we compare the IR bands
in spectra (c–e) in Fig. 5(A) with the corresponding spectra of
pyridine in its vapor (curve (a)) and liquid (curve (b)) forms. In the
case of pyridine adsorption over pure SBA-15 [Fig. 5(A), (c)], the
two observed bands are quite broad and at the same time they lack
any splitting of the bands, a characteristic feature of the IR
spectrum of pyridine vapor [cf. Fig. 5(A), (a)]. Further, the full width
at half maximum (FWHM) of the IR bands seen in Fig. 5(A), (c) is
ꢂ15 cmꢁ , and this lies in between the FWHM values for IR bands
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1
3
740 cm bandandthedevelopmentofanewlowerfrequencyband
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at ꢂ3485 cm (Fig. 4). This is shown graphically in Fig. 8. This mode
of triflate occlusion in SBA-15 would thus enable a metal cation to
serve as a distinct Lewis acid site for the activation of a reactant
molecule, as shown in Fig. 8. The reaction mechanism for the
acylationofnaphthalenecanthusbeexpressedbytworeactionsteps.
The first step consists of an interaction of toluoyl chloride with the
metal triflate to form an acyl cation-zinc triflate activated complex.
This transient complex may promote the formation of some highly
active species, e.g. acylium ion. In the second step the acylium ion
mayreactwiththe naphthalene, givingrisetotheformationof 2-acyl
naphthalene and eventual regeneration of the catalyst.
1
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of vapor (ꢂ28 cm ) and liquid (ꢂ4 cm ) phases of pyridine. This
indicates that the pyridine molecules entrapped in SBA-15 may
exist in a non-equilibrium state, in between the vapor and the
liquid form. In this adsorbed state, the pyridine molecules are
likely to retain their rotational motion without any strong bonding
at the SBA sites. On the other hand, a considerable shift is observed
IR results in Fig. 5(A) confirm that the acid density in a catalyst
was directly related to the loading of a metal triflate. Moreover, the
in the frequencies of n8a and n19b C–C bands for the adsorption of
pyridine molecules in Zn-Tr/SBA samples [Fig. 5(A), (d and e)]. In
addition, significant narrowing of the peaks (FWHM ꢂ6 cmꢁ ) is
noticeable in spectra (d) and (e) of Fig. 5(A), as compared to the IR
bands of pyridine vapor [Fig. 5(A), (a)]. This represents an immobile
state of pyridine molecules having no rotational motion. It can thus
be concluded that the triflate metal cations may participate in the
direct binding of a guest molecule, a situation similar to that
presented schematically in Fig. 8. Further, the systematic increase
in the intensity of pyridine bands as a function of increasing triflate
loading in SBA-15 [Fig. 5(A), (d and e)] and the dependence of Lewis
acidity in the functionalized silicate samples on the nature of the
occluded metal cation [Fig. 5(B)] also serve as evidence for the
direct participation of the triflate cation in binding of the pyridine
molecules. Logically, other reactant molecules are likely to
undergo similar binding at the cation sites, as depicted in Fig. 8.
The binding of the pyridine molecules at triflate metal cations may
eventually lead to further perturbation of the surface hydroxyl
groups in the host matrix, thus giving rise to some synergistic
1
changes in the intensity of n(OH) band, as shown in Fig. 3(c). We
surmise that the perturbed –OH groups may give rise to certain
bridge bonded hydroxyl species with the participation of a triflate
metal cation, and these species may be associated with a broad IR
Fig. 8. Schematic presentation of the perturbation of –OH groups caused by the
confinement of a metal triflate molecule in a silicate channel, and the postulated
binding mode of a reactant molecule.
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band observed at 3485 cm
in Fig. 4. These bridge bonded