J. Am. Chem. Soc. 1998, 120, 1523-1527
1523
+
Radiolytic Silylation of Alkenes and Alkynes by Gaseous R Si Ions.
3
Stereochemical Evidence for the â-Silyl Effect
Barbara Chiavarino, Maria Elisa Crestoni, and Simonetta Fornarini*
Contribution from the Dipartimento di Chimica e Tecnologia delle Sostanze Biologicamente AttiVe,
UniVersit a` di Roma “La Sapienza”; P.le A. Moro 5, I-00185 Roma, Italy
ReceiVed September 30, 1997
Abstract: Carbocation intermediates stabilized by a â silyl group have been characterized, using the silylation
+
of alkenes by R3Si ions as a route of formation. Neutral silylated products have been obtained from the
+
reaction of R3Si ions, generated in a gaseous medium at atmospheric pressure by a radiolytic technique, with
selected alkenes, alkynes, and allene, thereby indicating the occurrence of electrophilic silylation. Notable
features of the charged silylated intermediates emerge from the isomeric product distribution. The silylation
of cis- and trans-2-butene shows a high degree of retention of configuration, as expected if a bridged species
(I) were the reaction intermediate. Alternatively, the intermediacy of an open structure (II), whereby C-C
bond rotation is inhibited by the hyperconjugative interaction between the â silyl group and the vacant p
orbital, should be inferred. The charged intermediates from the silylation of alkenes and alkynes are found to
be unreactive toward conceivable isomerizations to more stable species, such as the ones bearing the positive
charge on silicon. Stereoelectronic factors affect the deprotonation of the silylated intermediates, which may
involve loss of the proton from either the R or the γ position with respect to the silylated carbon. A comparison
of the reactivity of alkenes and alkynes in the cationic silylation reaction is presented.
One of the salient features of organosilicon chemistry is the
stabilizing effect exerted on a carbenium ion by a silyl group
in a position â to the carbon bearing the formal charge, the
that include species I/II as possible isomers, have been generated
from different precursors, and their unimolecular and bimo-
lecular reactivity has been investigated by mass spectrometric
techniques. These experimental studies have been accompanied
by MO calculations, providing a fairly comprehensive picture
of the relative stabilities of isomeric structures and their
1
so-called â effect. A remarkable number of reactivity studies
in solution, mainly focused on solvolytic processes, have
reported on the stabilization of a positive charge by â silicon,
which gives rise to low energy transition states and/or inter-
3
interconversion pathways. However, the question of whether
12
mediates, causing rate enhancements of up to 10 with respect
I or II should be favored remains open. We have used the R -
3
2
+
to model systems. An open question regards the structure of
Si reaction with alkenes as an entry to I/II type species,
+
the postulated intermediate species. It may in fact be described
either as a bridged structure (I), where the Si atom exploits the
ability to expand its coordination, or as a â silylated carbenium
ion (II). The magnitude of the developing â-silicon effect
depends in a crucial way on the p-σCSi hyperconjugation, which
is maximized when the 2p orbital developing on the cationic
carbon and the C-Si σ bonding orbital are aligned in the same
plane. However, the actual involvement of structure I vs II is
hard to prove.2
because the reaction of Me Si ions with alkenes was known
3
to yield abundant adduct ions in a high-pressure ion source.4
The equilibrium constants for the association reactions (eq 1)
were studied as a function of temperature, and thermodynamic
data were derived.
+
+
Me Si + R R CdCR R f [Me Si-CR R CR R ] (1)
3
1
2
3
4
3
1
2
3 4
e
(2) Recent examples include: (a) Lambert, J. B.; Wang, G.; Finzel, R.
B.; Teramura, D. H. J. Am. Chem. Soc. 1987, 109, 7838. (b) Lambert, J.
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Gong, Y. J. Am. Chem. Soc. 1994, 116, 5963. (d) Gabelica, V.; Kresge, A.
J. J. Am. Chem. Soc. 1996, 118, 3838. (e) Lambert, J. B.; Liu, X. J.
Organomet. Chem. 1996, 521, 203. (f) Surya Prakash, G. K.; Reddy, V.
P.; Rasul, G.; Casanova, J.; Olah, G. A. J. Am. Chem. Soc. 1992, 114,
3
076. (g) Siehl, H.-U.; Kaufmann, F. P.; Apeloig, Y.; Braude, V.; Danovich,
D.; Berndt, A.; Stamatis, N. Angew. Chem., Int. Ed. Engl. 1991, 30, 1479.
e) Siehl, H.-U.; Kaufmann, F. P.; Hori, K. J. Am. Chem. Soc. 1992, 114,
343.
3) (a) Hajdasz, D.; Squires, R. J. Chem. Soc., Chem. Commun. 1988,
(
9
In principle, the study of naked ions in the gas phase should
provide the most objective description of ion structures and
energetics. Gaseous ions of the general formula CnH2n+3Si ,
(
+
1212. (b) Drewello, T.; Burgers, P. C.; Zummack, W.; Apeloig, Y.; Schwarz,
H. Organometallics 1990, 9, 1161. (c) Bakhtiar, R.; Holznagel, C. M.;
Jacobson, D. B. J. Am. Chem. Soc. 1992, 114, 3227. (d) Ciommer, B.;
Schwarz, H. J. Organomet. Chem. 1983, 244, 319. (e) Apeloig, Y.; Karni,
M.; Stanger, A.; Schwarz, H.; Drewello, T.; Czekay, G. J. Chem. Soc.,
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Lett. 1988, 29, 4159.
(1) (a) Fleming, I. Chem. Soc. ReV. 1981, 10, 83. (b) Lambert, J. B.
Tetrahedron 1990, 46, 2677. (c) Apeloig, Y. In The Chemistry of Organic
Silicon Compounds; Patai, S., Rappoport, Z., Eds.; Wiley: New York, 1989;
chapter 2. (d) Bassindale, A. R.; Taylor, P. G. The Chemistry of Organic
Silicon Compounds; Chapter 14. (e) Eaborn, C.; Bott, R. W. In Organo-
metallic Compounds of the Group IV Elements; MacDiarmid, A. G., Ed.;
Marcel Dekker: New York, 1968; Vol. 1, Part 1. (f) Nguyen, K. A.; Gordon,
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Published on Web 02/06/1998