It would appear that transmetallation of the 4-benzyloxy- and
4-hydroxy-pent-2-enylstannanes 1 (R2 = Bn, H) with tin(iv)
chloride gives the (3S,4S)-4-benzyloxy- and (3S,4S)-4-
hydroxy-pent-1-en-3-yl)tin trichlorides 3 (R2 = Bn, H) as
originally postulated. By analogy with the transmetallation of
the 5-alkoxypent-2-enylstannanes 5,5 it is likely that this
transmetallation is due to kinetic control. However only low
yields of products were obtained on attempted transmetallation
of the pent-1-en-3-ylstannane 6 using either tin(iv) chloride or
bromide, and so the interconversion of regioisomeric allyltin
trihalides could not be investigated in this case.
The formation of the 1,5-syn (Z)-products from the reactions
between the tin trichlorides 3 and aldehydes is consistent with
participation of chair-like transition structures akin to 4.
However, why does the C(3)–C(4) bond prefer to be axial rather
than equatorial, i.e. why are (Z)-alkenes obtained as the
dominant products from these reactions rather than their
(E)-isomers? To probe the factors involved in this ster-
eoselectivity, high level electronic structure calculations have
been carried out on the allyltin trichloride 16 and the transition
structures for its reactions with formaldehyde which would lead
to (E)- and (Z)-alkenols. A split valence basis was employed,9
with electron correlation included at the density functional
theory level (B3LYP), using GAUSSIAN94.10 Stationary
structures were identified as minima or saddle points by the
calculation of harmonic frequencies.
trans-isomer [Fig. 1(b)], which has a barrier of 12.0 kcal mol21
.
The favoured structure has a six-coordinated tin atom, with Sn–
C and Sn–O bond lengths in the range 2.2–2.4 Å. The transition
structure leading to the unfavoured trans-isomer has one of its
Sn–O bond lengths considerably longer than normal (3.3 Å), so
that the tin is effectively five-coordinated.
Two factors favour the transition structure shown in Fig. 1(a).
Firstly, there is greater steric repulsion between the C(3)–C(4)–
OMe entity and the chlorine atoms in the transition structure for
formation of the unfavoured trans-isomer. Secondly, the
different orientations of the C(3)–C(4) bond in the two
transition structures leads to the long Sn–O bond in the
disfavoured transition structure.
This work confirms the participation of the allyltin trich-
lorides 3 in tin(iv) chloride-promoted reactions of the allylstan-
nanes 1. The theoretical studies provide an insight into the
factors which favour the formation of cis-alkenes in reactions of
these allyltin trichlorides with aldehydes and complement
recently reported computational studies into reactions between
allylsilanes and aldehydes.11,12
We thank the University of Manchester and SmithKline
Beecham for support (to L. A. H.) under the CASE Scheme, Dr
M. Fedouloff of SmithKline Beecham for helpful discussions,
and the EPSRC for support.
Notes and References
We find two conformations of the allyltin trichloride 16,
corresponding to rotamers about the C(2)–C(3) bond, to be
energy minima with Sn–O bond lengths of 2.457 and 2.531 A.
Transition states for reactions of 16 with formaldehyde leading
† E-mail: e.j.thomas@man.ac.uk
1 E. J. Thomas, Chem. Commun., 1997, 411.
2 A. H. McNeill and E. J. Thomas, Synthesis, 1994, 322.
3 G. W. Bradley, D. J. Hallett and E. J. Thomas, Tetrahedron: Asymmetry,
1995, 6, 2579.
4 J. S. Carey and E. J. Thomas, Synlett, 1992, 585.
5 R. L. Beddoes, L. A. Hobson and E. J. Thomas, Chem. Commun., 1997,
1929.
3
4
Cl3Sn OMe
16
6 V. J. Jephcote and E. J. Thomas, J. Chem. Soc., Perkin Trans. 1, 1991,
429.
7 A. T. Bottini, R. L. VanEtten and A. J. Davidson, J. Am. Chem. Soc.,
1965, 87, 755.
8 L. D. Hall, P. R. Steiner and D. C. Miller, Can. J. Chem., 1979, 57,
38.
to both cis- and trans-double-bonded products have been
located and identified as saddle points on the potential energy
surfaces. These are summarised in Fig. 1.
9 W. J. Hehre, R. Ditchfield and J. A. Pople, J. Chem. Phys., 1972, 56,
2257; R. Ditchfield, W. J. Hehre and J. A. Pople, J. Chem. Phys., 1971,
54, 724; M. S. Gordon, Chem. Phys. Lett., 1980, 76, 163; P. C.
Hariharan and J. A. Pople, Theor. Chim. Acta, 1973, 28, 213;
A. Stromberg, O. Gropen and U. Wahlgren, J. Comput. Chem., 1983, 4,
181; an additional d-function with exponent 0.27 was used on tin.
10 M. J. Frisch, G. W. Trucks, H. B. Schlegel, P. M. W. Gill, B. G. Johnson,
M. A. Robb, J. R. Cheeseman, T. A. Keith, G. A. Petersson,
J. A. Montgomery, K. Raghavachari, M. A. Al-Laham, V. G.
Zakrzewski, J. V. Ortiz, J. B. Foresman, J. Cioslowski, B. B. Stefanov,
A. Nanayakkara, M. Challacombe, C. Y. Peng, P. Y. Ayala, W. Chen,
M. W. Wong, J. L. Andres, E. S. Replogle, R. Gomperts, R. L. Martin,
D. J. Fox, J. S. Binkley, D. J. Defrees, J. Baker, J. J. P. Stewart, M. Head-
Gordon, C. Gonzalez and J. A. Pople, GAUSSIAN 94, Revision A.1,
Gaussian, Inc., Pittsburgh, PA, 1995.
There are considerable differences in the transition state
structures and energy barriers leading to the two different
stereoisomers. The transition structure leading to the cis-
double-bonded product [Fig. 1(a)] has a considerably lower
barrier (1.9 kcal mol21) and different structure, particularly
about the tin atom, than the transition structure leading to the
(a)
(b)
Cl
Cl
Cl
Cl
Cl
Sn
Cl
Sn
2.222
2.182
1.284
3.297
2.380
O
1.267
O Me
C
O
C
O
C4
2.046
2.197
C3
C2
C3
C2
1.429
1.434
Me
C1
C1
1.388
2.374
1.376
C4
11 A. Bottoni, A. L. Costa, D. Di Tommaso, I. Rossi and E. Tagliavini,
J. Am. Chem. Soc., 1997, 119, 121131.
2.370
12 K. Omoto, Y. Sawada and H. Fujimoto, J. Am. Chem. Soc., 1996, 118,
1750.
∆E = 1.9 kcal mol–1
∆E = 12.0 kcal mol–1
Fig. 1 Transition structures leading to (a) cis and (b) trans products. Bond
lengths are in Å.
Received in Liverpool, UK, 28th January 1998; 8/00781K
900
Chem. Commun., 1998