M. E. Jung, R. Salehi-Rad / Tetrahedron Letters 51 (2010) 4931–4933
4933
7. (a) Arimoto, H.; Nishiyama, S.; Yamamura, S. Tetrahedron Lett. 1990, 31, 5619–
5620; (b) Yamamura, S.; Nishiyama, S. Bull. Chem. Soc. Jpn. 1997, 70, 2025–
2037.
8. (a) Dess, D. B.; Martin, J. C. J. Org. Chem. 1983, 48, 4155–4156; (b) Dess, D. B.;
Martin, J. C. J. Am. Chem. Soc. 1991, 113, 7277–7287.
9. Inanaga, J.; Hirata, K.; Saeki, H.; Katsuki, T.; Yamaguchi, M. Bull. Chem. Soc. Jpn.
1979, 52, 1989–1993.
10. The structures of these two products were confirmed by protecting both
alcohols separately with the TES group. Only the corresponding silyl ether of
Finally, we attempted Crimmins cyclization conditions on the
diol 14, synthesized from the pyrone 9 in two steps, but did not ob-
serve any cyclized product (Scheme 4). A significant difference be-
tween our system and all the reported cyclizations by Crimmins
and co-workers is the presence of methyl substituents
a to the
ketone of the -pyrone, presumably increasing the steric conges-
c
tion of the transition state for cyclization. However, more experi-
ments are necessary to study the variables involved in this
reaction.
In conclusion, we have reported an efficient synthesis of the key
bis(pyrone) alcohol 3, a precursor for the Crimmins cyclization, to
accomplish a novel synthesis of auripyrone A 1. This approach
failed to provide the desired spiroketal natural product and rather
resulted in 1,5-acyl migration to give a mixture of the compounds
3 and 8. Similar treatment of structurally analogous compounds
also gave mostly acyl transfer.
the alcohol 12 exhibited identical spectral data with the
c-pyrone 11, thus
confirming the structure of 12. The minor isomeric alcohol 13 was
consequently assigned as the product of the acyl migration of the alcohol 12.
11. Hoffmann, R. W. Angew. Chem., Int. Ed. 2000, 39, 2054–2070.
12. Analysis of the relevant coupling constants in these systems indicates that a
local conformation such as I is likely. For example, in 12, Ha appears as a dd,
J = 9.0, 3.1 Hz while Hb is obscured. In 13, Ha appears as a dd, J = 8.5, 2.7 Hz and
Hb appears as a dd, J = 7.3, 3.5 Hz. Similarly in 3, Hb appears as a dd, J = 9.0,
3.0 Hz, while Ha is obscured. This pattern of one large and one small coupling
constant is consistent with the structures proposed since both Ha and Hb
should have one dihedral angle with a vicinal proton of about 180° and a
second of about 60°. Other related compounds in this series showed a similar
coupling constant pattern.
Acknowledgment
We thank the National Science Foundation (CHE 0614591) for
generous support of this work.
OR3
O
O
R1
O
O
OR4
Ha
Hb
Me
Me
Me
Me
Me
Me
Me
H
Me
R1 =
9
R1 =
R2 =
References and notes
11
Me
H
R2
O
Me
Et
1. Suenaga, K.; Kigoshi, H.; Yamada, K. Tetrahedron Lett. 1996, 37, 5151–5154.
2. Lister, T.; Perkins, M. V. Angew. Chem., Int. Ed. 2006, 45, 2560–2564.
3. Jung, M. E.; Salehi-Rad, R. Angew. Chem., Int. Ed. 2009, 48, 8766–8769.
4. Hayakawa, I.; Takemura, T.; Fukasawa, E.; Ebihara, Y.; Sato, N.; Nakamura, T.;
Suenaga, K.; Kigoshi, H. Angew. Chem., Int. Ed. 2010, 2401–2404.
H
OTBDPS
Me
R2
=
O
Me
3 R3 = H R4 = COCH2CHMe2
12 R3 = COCH2CHMe2 R4 = H
13 R3 = H R4 = COCH2CHMe2
5. Jung, M. E.; Chaumontet, M.; Salehi-Rad, R. Org. Lett. 2010, 12, 2872–2875.
6. Crimmins, M. T.; Omahony, R. J. Org. Chem. 1990, 55, 5894–5900.