Scheme 4 Reagents and conditions: i, O3, Et2O, 278 °C, 10 min; ii, NaBH4,
H2O, 0 °C, 1 h; iii, Mosher’s R-acid, DCC, DMAP, CH2Cl2, rt, 16 h.
Scheme 5 Reagents and conditions: i, Me2CuLi, THF, 278 °C, 1 h; ii,
TBDMSCl, HMPA, Et3N, 278 °C ? rt, 1 h; iii, EtCHO, TiCl4, CH2Cl2
278 °C, 2 h; iv, TsOH, toluene, reflux, 1 h; v, Me2CuLi, THF, 278 °C, 1 h;
vi, TMSCl, HMPA, Et3N, 278 °C ? rt, 1 h.
adjacent to the stereogenic centre carrying a silyl group has
undergone nucleophilic attack. All our work in the past has
involved electrophilic attack. Since the sense of attack, anti to
the silyl group 1, is the same, it may be that we have here some
indication that the stereocontrol is largely steric in origin. This
conclusion stems from the prejudice that nucleophilic attack and
electrophilic attack would take place in opposite senses if purely
electronic effects were operative.
Although this may be a little too simplistic, we can be sure
that the silyl group is an important component in ensuring the
high levels of diastereocontrol that we have seen, for we have
carried out a similar set of reactions with the C-5 methyl group
and the C-3 silyl group in 5 interchanged (Scheme 5). Starting
with the silicon-containing cyclohexenone 16,16 and using a
methylcuprate to set up the 1,3-related centres in the enone 17.
This time, the conjugate addition of the methylcuprate gave
both possible diastereoisomers 18 in equal amounts. Pre-
sumably a methyl group on C-3, although surely held axial,
shields the bottom surface from attack to the same extent as the
upturned methyl group on the side chain shields the top
surface.
bond. In consequence, even though a trimethylsilyl group has a
larger A-value than a methyl group (2.513 and 1.74, re-
spectively), the lower-energy conformation of the enone 3
probably has the methyl group equatorial and the silyl group
axial 12, where, in any case, it only has one 1,3-diaxial
interaction. With the silyl group held on the lower surface,
nucleophilic attack can be expected to take place on the top
surface anti to the bulky group 12 (arrow), and hence give the
silyl enol ether with the relative configuration 4.
To support this argument, we carried out molecular model-
ling calculations (Macromodel), which confirmed that the
conformation with the silyl group axial 12 had the lowest
energy,14 with the stereo drawings 13 giving a more accurate
We thank Avra Laboratories, Hyderabad, for a maintenance
grant (C. R.), and Setu P. Roday for help with the molecular
modelling.
Notes and references
1 Summarised in: I. Fleming, J.. Chem. Soc., Perkin Trans. 1, 1992,
3363.
2 I. Fleming and N. J. Lawrence, J. Chem. Soc., Perkin Trans. 1, 1998,
2679.
3 M. Ahmar, C. Duyck and I. Fleming, J. Chem. Soc., Perkin Trans. 1,
1998, 2721; I. Fleming and S. K. Ghosh, J. Chem. Soc., Perkin Trans.
1, 1998, 2733.
4 I. Fleming and C. P. Leslie, J. Chem. Soc., Perkin Trans. 1, 1996,
1197.
picture of the minimised structure. Looking at the space-filling
versions 14 (from above) and 15 (from below) illustrates the
difference between the two surfaces of the enone 3—the b-
carbon (darker grey) in the top view is exposed, but in the
bottom view it is hindered by the substituents on the silyl
group.15
5 G. Procter, A. T. Russell, P. J. Murphy, T. S. Tan and A. N. Mather,
Tetrahedron, 1988, 44, 3953.
6 C. E. Masse and J. S. Panek, Chem. Rev., 1995, 95, 1293.
7 N. L. Allinger and C. K. Riew, Tetrahedron Lett., 1966, 1269. For the
most recent discussion, see S. Mori and E. Nakamura, Chem. Eur. J.,
1999, 5, 1534. For the first application in synthesis, see G. Stork, R. A.
Kretchmer and R. H. Schlessinger, J. Am. Chem. Soc., 1968, 90, 1647;
G. Stork, Pure Appl. Chem., 1968, 17, 383.
8 I. Fleming, R. Henning, D. C. Parker, H. E. Plaut and P. E. J. Sanderson,
J. Chem. Soc., Perkin Trans. 1, 1995, 317.
9 R. A. N. C. Crump, I. Fleming and C. J. Urch, J. Chem. Soc., Perkin
Trans. 1, 1994, 701.
10 H. Nishiyama, K. Sakuta, N. Osaka, H. Arai, M. Matsumoto and K. Itoh,
Tetrahedron, 1988, 44, 2413.
11 D. Caine, K. Procter and R. A. Cassell, J. Org. Chem., 1984, 49,
2647.
12 H. Oikawa, I. Matsuda, T. Kagawa, A. Ichihara and K. Kohmoto,
Tetrahedron, 1994, 50, 13347.
Furthermore, the calculation for the second a,b-unsaturated
ketone 5 revealed why it suffered a lower degree of stereo-
control in the conjugate addition step—the methyl group of the
ethyl group was oriented upwards, hindering the top surface
more than the top surface of the a,b-unsaturated ketone 3 = 12
= 13.
The stereocontrol in this system is interesting from two points
of view. In the first place, it shows that the silyl group is not so
hindering that it cannot adopt the axial position, and yet
simultaneously it does hinder the approach of the incoming
nucleophile. The long Si–C bond takes the silyl group far
enough away from the cyclohexane ring to make 1,3-diaxial
interactions less severe than they would be for a carbon-based
group, and yet the length of the Si–C bonds to the three other
substituents on the silicon atom causes them to occupy much of
the space below the double bond. In the second place, this is the
first reaction that we have studied in which the double bond
13 W. Kitching, H. A. Olszowy, G. M. Drew and W. Adcock, J. Org.
Chem., 1982, 47, 5153.
14 The chair conformation with the silyl group equatorial is 46.5 kJ mol21
higher in energy, and there are two families of boat conformations in
between, at 13 and 40 kJ mol21 above the minimum.
15 Although the calculation places the phenyl group under the carbonyl
group, a methyl group would be nearly as much hindrance at the b-
carbon; we do not think that the high degree of selectivity is dependent
upon the presence of the phenyl group on silicon.
16 M. Laguerre, J. Dunogue`s R. Calas and N. J. Duffaut, J. Organomet.
Chem., 1975, 93, C17; M. Asaoka, K. Shima and H. Takei, Tetrahedron
Lett., 1987, 28, 5669.
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Chem. Commun., 2000, 2185–2186