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Notes and references
´
1 For reviews see: (a) A. M. Martın Castro, Chem. Rev., 2004, 104, 2939;
(b) The Claisen Rearrangement: Methods and Applications, ed.
M. Hiersemann and U. Nubbemeyer, Wiley-VCH, 1st edn, 2007, p. 591.
2 L. Claisen, Ber., 1912, 45, 3157.
3 (a) S. E. Denmark and M. A. Harmata, J. Am. Chem. Soc., 1982,
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Scheme 2 Transition state analysis.
4 (a) A. Wille, S. Tomm and H. Frauenrath, Synthesis, 1998, 305;
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The origin of the diastereoselectivity was also of interest as
data on alkyl substrates with this enol ether substitution pattern
is sparse. It was found that the products do not equilibrate under
the reaction conditions (eqn (2)), which is in agreement with the
fact that reactions employing isomeric allyl alcohols (4c/4d) do
not provide the same ratio of diastereomeric products.
optimized
ꢀ!
6d or 6e
6d or 6e
(2)
no epimerization
single diastereomer conditions
The observation that cis-allylic alcohols consistently yield pro-
ducts in higher dr than the corresponding trans-allylic alcohols
provides key insight into the relevant reaction pathways. Analysis
of the possible chair and boat transition states (cis-allylic alcohol: C1/
B1; trans-allylic alcohol: C2/B2) for thermal rearrangement reactions
reveals that both of the enol ether substituents are oriented in the
pseudoaxial positions in (Scheme 2). This is inherent to Claisen
substrates with the R1,R2-trans-enol substitution pattern. The chair
transition states (C1/2) would be predicted to be lower in energy than
the competing boat transition states (B1/2),12 and hence cis- and
trans-allylic alcohols lead to the syn and anti diastereomers, respec-
tively. The diastereoselectivity is likely higher for the cis-allylic alcohol
due to specific steric interactions between the alkene and enol ether
substituents. The 1,2-eclipsing interaction in B1 between R2 and R3
likely increases the TS‡ energy more substantially than the corres-
ponding 1,3-diaxial interaction between R1 and R3 in C1. This effect
is diminished in C2/B2 because R3 is equatorial and thus avoids
eclipsing interactions, leading to a smaller DDG‡ with trans-allylic
alcohol substrates. The boat-like transition state therefore becomes
more competitive, leading to the observed erosion in diastereoselec-
tivity. Although the allyl vinyl ether isolated above (Table 2, entry 5)
does undergo thermal rearrangement in the absence of catalyst,13
studies on the extent to which the cascade process is also catalyzed
are underway and will be reported in due course.
6 For reviews see: (a) M. Beller, J. Seayad, A. Tillack and H. Jiao, Angew.
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7 (a) B. D. Sherry and F. D. Toste, J. Am. Chem. Soc., 2004, 126, 15978;
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9 See: (a) A. S. K. Hashmi, Chem. Rev., 2007, 107, 3180; (b) J. Muzart,
Tetrahedron, 2008, 64, 5815; (c) Y. Fukuda and K. Utimoto, J. Org.
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Angew. Chem., Int. Ed., 1998, 37, 1415; (e) A. Corma, V. R. Ruiz,
´
A. Leyva-Perez and M. J. Sabater, Adv. Synth. Catal., 2010, 352, 1701;
¨
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´
R. S. Ramon, S. Gaillard and S. P. Nolan, J. Organomet. Chem., 2011,
In summary, we have reported an efficient new cascade
696, 7 and references therein.
reaction approach to the synthesis and rearrangement of allyl 10 Reactions often require temperatures in the range of 150–300 1C: see
ref. 1.
vinyl ethers that proceeds from simple compounds to form
ketone products in high yield and diastereoselectivity. The
11 For a-arylation: (a) D. A. Culkin and J. F. Hartwig, Acc. Chem. Res.,
2003, 36, 234; (b) C. C. C. Johansson and T. J. Colacot, Angew. Chem.,
concept of tandem intermolecular alkyne addition/[3,3]-sigma-
tropic rearrangement should be applicable in a variety of
different reaction constructs further enabling the rapid intro-
duction of complexity to simple substrates.
We thank the Herman Frasch Foundation (647-HF07) and
the James and Ester King Biomedical Research Program (09KN-
01) for their generous support of our programs.
Int. Ed., 2010, 49, 676. For oxidation of aryl ketones: (c) R. Gottlich,
K. Yamakoshi, H. Sasai and M. Shibasaki, Synlett, 1997, 971;
(d) P. A. Evans and M. J. Lawler, J. Am. Chem. Soc., 2004, 126, 8642.
12 For relevant reports that include computational analyses of the
transition states see: (a) R. L. Vance, N. G. Rondan, K. N. Houk,
F. Jensen, W. T. Borden, A. Komornicki and E. Wimmer, J. Am.
Chem. Soc., 1988, 110, 2314; (b) C. Uyeda and E. N. Jacobsen, J. Am.
Chem. Soc., 2011, 133, 5062.
13 See Scheme S1 in the ESI‡ for further details.
c
This journal is The Royal Society of Chemistry 2013
Chem. Commun., 2013, 49, 4157--4159 4159