displacement parameters, riding H atoms (with rotational freedom for
state, with very small vicinal coupling constants around the
ring, and significant long-range (W) coupling between H-2 and
H-4, and between H-3 and H-5 (indicating that each of these
protons was in an equatorial position). The corresponding
sulfone 5, prepared by oxidation of the sulfide 2a, exhibited
almost identical coupling constants and is therefore probably
also in the same conformation in solution.
methyl and hydroxy hydrogen atoms), and two-fold disorder for one silyl
1
2
2 2
group. Rw = [Sw(Fo 2 Fc2)/Sw(Fo ) ] = 0.223 for all data, conventional
2
R = 0.101 for F values of 5551 reflections with Fo > 2s(Fo2), goodness
2
of fit 1.129, absolute configuration indicated by refinement of enantiopole
parameter (ref. 9) to 20.3(2), residual electron density within ± 0.61 e Å23
.
The indicated absolute configuration was consistent with the known
absolute configuration of the starting material. The quality of data collection
and structure refinement are limited by the deformed nature of the crystals
(apparently slightly bent, giving distorted reflections) and the structural
disorder. Programs were standard Siemens control and integration software,
Siemens SHELXTL, and local programs. CCDC 182/580.
The ‘A value’ of the phenylthio group (4.60–5.19 kJ mol21 7
)
is not sufficiently large to force the other substituents axial, so
the most obvious explanation is that the adjacent tert-
butyldimethylsilyloxy groups at C-3 and C-4 are more sterically
encumbered when they are diequatorial than when they are
diaxial.‡ Eliel’s important report on the ‘A values’ of silyloxy
groups, which clearly showed (rather counter-intuitively) that a
tert-butyldimethylsilyloxy group had a smaller ‘A value’ than a
trimethylsilyloxy group,8 provides strong support for this idea.
The ease with which the tert-butyldimethylsilyl group at C-3 of
2b migrates to C-2 is probably another manifestation of this
same phenomenon.
It is clear that the pronounced conformational effects of tert-
butyldimethylsilyl ethers may have useful consequences in
control of reaction stereoselectivity.
We thank the EPSRC for a CASE award (C. L. W.) and for
equipment grants, Rhoˆne-Poulenc Rorer for support and Drs B.
Porter, A. J. Ratcliffe and M. Podmore (RPR) for helpful
discussions. R. F. W. J. also thanks the Nuffield Foundation for
a One Year Science Research Fellowship.
‡ This suggestion was first made by Suzuki (ref. 6). This type of behaviour
has been noted before in the case of glycals (ref. 10), and in b-lactams
derived from glycals by cycloaddition (ref. 11). It has also been suggested
as an influence on reactivity, but without direct evidence (ref. 4.).
1 R. L. Halcomb and S. J. Danishefsky, J. Am. Chem. Soc., 1989, 111,
6661.
2 C. H. Marzabadi and C. D. Spilling, J. Org. Chem., 1993, 58, 3761.
3 D. M. Gordon and S. J. Danishefsky, Carbohydr. Res., 1990, 206,
361.
4 For a related observation, see: T. Iimori, H. Takahashi and S. Ikegami,
Tetrahedron Lett., 1996, 37, 649.
5 A closely related migration of a tert-butyldimethylsilyl group has been
reported: R. W. Friesen and A. K. Daljeet, Tetrahedron Lett., 1990, 31,
6133. For an analogous migration of a trimethylsilyl group, see
V. Pedretti, A. Veyrie`res and P. Sina¨y, Tetrahedron, 1990, 46, 77.
6 T. Hosoya, Y. Ohashi, T. Matsumoto and K. Suzuki, Tetrahedron Lett.,
1996, 37, 663.
7 O. A. Subbotin, V. A. Palyulin, S. I. Kozhushkov and N. S. Zefirov,
J. Org. Chem. USSR (Engl. Transl.), 1978, 14, 196.
8 E. L. Eliel and H. Satici, J. Org. Chem., 1994, 59, 688.
9 H. D. Flack, Acta Crystallogr., Sect. A, 1983, 39, 876.
10 D. Horton, W. Priebe and O. Varela, Int. Carbohydr. Symp. XIIth,
Utrecht, July 1–7, 1984, Abstr. D8.35, p. 519.
11 M. Chmielewski, Z. Kaluza, H. Dodziuk, K. Suwinska, D. Rosenbaum,
H. Duddeck, P. D. Magnus and J. C. Huffmann, Carbohydr. Res., 1990,
203, 183.
Footnotes and References
* E-mail: r.f.w.jackson@newcastle.ac.uk
† Crystal data for 2a: C30H58O5SSi3, Mr = 615.1, orthorhombic, P212121,
a = 27.1719(17), b = 10.9754(7), c = 12.3479(8) Å, V = 3682.4(4) Å3,
Z = 4, Dc = 1.109 g cm 23, m = 0.22 mm21 (Mo-Ka, l = 0.71073 Å),
T = 160 K. Measurements were made on a Siemens SMART CCD area
detector diffractometer. Data were collected by narrow-frame w rotation.
19 575 reflections, 2q @ 50°, 6467 unique reflections, Rint = 0.091, semi-
empirical absorption correction, transmission 0.84–0.97. Structure solution
was by direct methods, refinement on F2 for all data, with anisotropic
Received in Liverpool, UK, 27th June 1997; 7/04534D
1856
Chem. Commun., 1997