3
4
F. Mauriello et al. / Journal of Molecular Catalysis A: Chemical 328 (2010) 27–34
equilibrium pressures. Section A reports the O–H stretching region,
and section B that of C C stretching. In the former region, the two
been highlighted. Curiously, the IR technique affords information
on the overall reactivity and on the nature of the species adsorbed
on the silica support, but not on the metallic phases, because of the
metal/surface selection rule.
−1
bands at 3735 and 3715 cm (due to the isolated silanol and the
terminal species in a pair, respectively) decrease and a broad band
−1
at ca. 3390 cm increases, due these silanols species H-bonded to
−
1
2
,3-DHF molecules. The extent of the shift (ca. 350 cm ) is strongly
Acknowledgement
indicative of a coordination through the O atom. Indeed, this is the
order of magnitude of the shift imparted to the SiO–H stretching
mode by O-containing molecules like ethers [31].
Thanks are due to Regione Piemonte (projects B18 and E28) for
financial support.
As the double bond in 2,3-DHF is not directly engaged in the
interaction, its frequency coincides with the gas-phase molecule,
Appendix A. Supplementary data
−1
and is observed at 1624 cm (Fig. 6, section B). Also physisorbed
molecules contribute to this adsorption. A shoulder of the main
Supplementary data associated with this article can be found, in
the online version, at doi:10.1016/j.molcata.2010.05.011.
−1
band is observed at 1616 cm . Both the main component and
the shoulder are also observed in the interaction of 2,3-DHF with
the support alone. Comparison with the literature [32] shows that
interaction of silanol species SiO–H with the olefinic double bond
References
−
1
is weak and shifts the C C stretching mode by only 8–10 cm . The
[1] M.G. Musolino, C.M.S. Cutrupi, A. Donato, D. Pietropaolo, R. Pietropaolo, Appl.
Catal. A: Gen. 243 (2003) 333–346.
−1
interpretation of the 1616 cm band is therefore the double inter-
action of a 2,3-DHF molecule via both the oxygen atom and the
double bond, favoured by the relatively high silanol population.
The question arises of the modality of adsorption on the metallic
particles. A molecule with a C–C double bond may interact with a
metal surface in various ways, by forming -type adducts or dou-
bly -coordinated species, to leave aside more complex ethylidenic
species formed at higher temperatures [6–8]. In these two cases, a
substantial decrease in the C–C bond order takes place, so that the
related C–C vibration markedly decreases. In the present case, how-
ever, no bands related to metallic centres are present in the spectra
of 2,3-DHF adsorbed on the catalyst. This fact may be due to the
limited surface exhibited by the metallic phase, as indicated by the
TEM characterization of the catalysts.
[
2] M.G. Musolino, P. De Maio, A. Donato, R. Pietropaolo, Appl. Catal. A: Gen. 285
2005) 50–58.
[3] M.G. Musolino, G. Apa, A. Donato, R. Pietropaolo, F. Frusteri, Appl. Catal. A: Gen.
25 (2007) 112–120.
(
3
[
[
4] N. Sheppard, C. De la Cruz, Adv. Catal. 41 (1996) 1–112.
5] G. Busca, G. Ramis, V. Lorenzelli, A.J. Lavalley, J.-C. Lavalley, Spectrochim. Acta
A: Mol. Spectrosc. 4 (1987) 489–496.
[
[
6] M.A. Chesters, C. De La Cruz, P. Gardner, E.M. McCash, P. Pudney, G. Shahid, N.
Sheppard, J. Chem. Soc., Faraday Trans. 86 (1990) 2757–2763.
7] G. Shahidt, N. Sheppard, J. Chem. Soc., Faraday Trans. 90 (1994) 507–511.
[8] G. Shahidt, N. Sheppard, J. Chem. Soc., Faraday Trans. 90 (1994) 513–516.
9] G.D. Chukin, V.I. Malevich, J. Appl. Spectrosc. 26 (1977) 223–229.
10] B. Camarota, B. Onida, Y. Goto, S. Inagaki, E. Garrone, Langmuir C 23 (2007)
3164–13168.
[
[
1
[11] S. Bertarione, C. Prestipino, E. Groppo, D. Scarano, G. Spoto, A. Zecchina, R. Pel-
legrini, G. Leofanti, C. Lamberti, Phys. Chem. Chem. Phys. 8 (2006) 3676–3681.
[
12] L.M. Kustov, V.B. Kazansky, S. Beran, L. Kubelkova, P.J. Jiru, J. Phys. Chem. 91
1987) 5247–5251.
(
Another possible reason, though, is the orientation of the dou-
ble bond with respect to the surface. As shown by Sheppard and
De La Cruz, because, at the surface of a metal, the bulk electrons
respond to the oscillating dipoles of a molecule with a mirror image
dipole, the selection rule is different from those at the surface of
insulators, and in particular parallel vibrations become inactive
[13] N. Sheppard, C. De La Cruz, Catal. Today 70 (2001) 3–13.
[14] N. Sheppard, T.T. Nguyen, Adv. Infrared Raman Spectrosc. 5 (1978) 67–134.
[
[
[
15] C. Delacruz, N. Sheppard, J. Mol. Struct. 224 (1990) 141–161.
16] E. Ozensoy, D.W. Goodman, Phys. Chem. Chem. Phys. 6 (2004) 3765–3778.
17] S.G. Podkolzin, J. Shen, J.J. de Pablo, J.A. Dumesic, J. Phys. Chem. B 104 (2000)
4169–4180.
[
[
18] T.D. Klots, W.B. Collier, Spectrochim. Acta 50 (1994) 1725–1748.
19] F. Billes, H. Böhlig, M. Ackermannb, Matthias Kudra, J. Mol. Struct. (Theochem)
[
4].
The absence of C C stretching bands in the spectra seem to be
6
72 (2004) 1–16.
[20] M. Fleisher, V. Stonkus, L. Leite, E. Lukevics, Int. J. Quant. Chem. 88 (2002)
70–675.
21] S.K. Parida, S. Dashb, S. Patel, B.K. Mishra, Adv. Colloid Interface Sci. 121 (2006)
7–110.
[22] O.V. Dorofeeva, Thermochim. Acta 194 (1992) 9–46.
6
an indication of the fact that all molecules studied in the present
work lie flat on it, so that the metal-surface selection rule becomes
operative
[
7
[
[
[
[
[
[
[
23] J.R. Monnier, J.W. Medlin, Y.J. Kuo, Appl. Catal. A: Gen. 195 (2000) 463–474.
24] G.C. Bond, Heterogeneous Catalysis, Clarendon Press, Oxford, 1987.
25] Z. Dobrovolná, P. Kaèer, L. Èerven y´ , J. Mol. Catal. A: Chem. 130 (1998) 279–284.
26] K.I. Tanaka, Adv. Catal. 33 (1985) 99–104.
27] N.I. Shuikin, I.F. Belskii, R.A. Karakhanov, Russ. Chem. Bull. 11 (1962) 123–126.
28] A. Lifshitz, M. Bidani, J. Phys. Chem. 93 (1989) 1139–1144.
4
. Conclusion
The comparison between the reactivity of the catalyst with that
of the support alone has enabled a fairly complete characterization
of the vapour-phase interaction of C-2-OL with silica supported Pd
and Pt nanoparticles. The reaction network reported in Scheme 3
envisages a few steps, all of which fairly expected, the ensemble of
which, however, constitutes an original picture. The reason why the
chemistry of C-2-OL in ethanol solutions is drastically different has
29] A. Lifshitz, M. Bidani, S. Bidani, J. Phys. Chem. 90 (1986) 6011–6014.
[30] C.A. Wellington, W.D. Walters, J. Am. Chem. Soc. 83 (1961) 4888–4891.
[
[
31] A. Zecchina, S. Bordiga, G. Spoto, D. Scarano, G. Spanò, F. Geobaldo, J. Chem.
Soc., Faraday Trans. 92 (1996) 4863–4875.
32] G. Busca, G. Ramis, V. Lorenzelli, A. Janin, J. Lavalley, Spectrochim. Acta A: Mol.
Spectrosc. 43 (1987) 489–496.