1790
N. Raynal et al. / Tetrahedron Letters 48 (2007) 1787–1790
for the minor folded conformation of 2a. The low fre-
quency observed for 4a, in comparison with 2a, may
be the consequence of the double involvement, both of
its NH and CO groups in an H-bonding.18 Luppi
et al. raised such results with the oligomers of oxazolid-
inone derivatives.19 These data suggested that there is an
increase of hydrogen bonds with the oligomer size sug-
gesting that short oligomers of AMPA are able to fold
in an ordered structure. The propensity of short oligo-
mers to fold in organized structure was observed in
foldamers.1–4,19
References and notes
1. Gellman, S. H. Acc. Chem. Res. 1998, 31, 173–180.
2. Cheng, R. P.; Gellman, S. H.; Degrado, W. F. Chem. Rev.
2001, 101, 3219–3232.
3. Seebach, D.; Matthews, J. L. Chem. Commun. 1997, 2015–
2022.
4. Hill, D. J.; Mio, M. J.; Prince, R. B.; Hughes, T. S.;
Moore, J. S. Chem. Rev. 2001, 101, 3893–4011.
5. Gillespie, P.; Cicariello, J.; Olson, G. L. Peptide Sci. 1997,
43, 191–217.
6. Obrecht, D.; Altorfer, M.; Robinson, J. A. Adv. Med.
Chem. 1999, 1–68.
´
7. Amblard, M.; Martinez, J.; Berge, G. Patent 11/01/2000
However, as discussed before, in the absence of further
experimental data on the syn and anti orientations pres-
ent in the AMPA oligomer, we constructed the two pos-
sible helices (Fig. 1) and we compared their stability by
computational analysis. Among the conformations of
lowest energy, those presenting a syn orientation of
the amide group contained hydrogen bond between
the CO and NH of the same AMPA residue resulting
in an eight-membered ring. However, this computa-
tional prediction did not fit with the experimental IR
data showing a C@O–H–N hydrogen in the N- to C-ter-
minal direction forming a 10-membered ring. The helix
with a 10-membered ring hydrogen bond and a syn
amide group orientation observed in the transition state
(Fig. 1b), led after molecular modeling minimization to
an unstructured oligomer. These different results
prompted us to consider that the preferred structure
adopted a 10-helix with the amide groups in a trans
orientation.
sous le nꢁ 0000288, WO B0384.
8. Claridge, T. D. W.; Goodman, J. M.; Moreno, A.; Angus,
D.; Barker, S. F.; Taillefumier, C.; Watterson, M. P.;
Fleet, G. W. J. Tetrahedron Lett. 2001, 42, 4251–
4255.
9. Applequist, J.; Bode, K. A.; Appella, D. H.; Christianson,
L. A.; Gellman, S. H. J. Am. Chem. Soc. 1998, 120, 4891–
4892.
10. Experiments were performed on silicon graphics using
Discover Molecular Simulation program, Biosym/MSI.
We first performed a molecular dynamic at 1000 K and a
minimization of the monomer under its aldehydic form
H-AMPA-H. The conformer of the lowest energy was
selected and its corresponding Ac-AMPA-NH-Me was
subjected to a 45ꢁ variation of the four dihedral angles.
After minimization, we selected 10 conformations corre-
sponding to the predicted lower energy conformation
(34.33 kcal/mol) and those having an energy of 34.33 kcal
plus an increment equal to or less than 5 kcal/mol.
11. Zhilian, T.; Pelletier, J. C. Tetrahedron Lett. 1998, 39,
4773–4776.
12. Aubry, A.; Cung, M. T.; Marraud, M. J. Am. Chem. Soc.
1985, 107, 7640–7647.
In summary, we have shown by NMR and IR studies
that the short oligomers of 2-aminomethyl-phenyl-acetic
acid, selected by computational analysis for their possi-
bility to induce a well-defined secondary structure, could
adopt a 10-helical folding pattern. In the absence of chi-
ral center within the molecule and the difficulty of ana-
lyzing homo-oligomers, the availability of syn and anti
orientations of the amide was analyzed by molecular
modeling. The anti orientation of the amide group that
was also observed in the crystal of the AMPA derivative
seems to be the preferred conformation.
´
13. Jimenez, A. I.; Cativiela, C.; Aubry, A.; Marraud, M. J.
Am. Chem. Soc. 1998, 120, 9452–9459.
14. Crystal data 1b: C17H26N2O3, Mr = 306.40, colorless
3
˚
prism, crystal size 0.2 · 0.1 · 0.1 mm , a = 5.1411(4) A,
˚
˚
b = 11.5197(10) A, c = 15.236(2) A, a = 82.930(3)ꢁ, b =
3
˚
89.537(2)ꢁ, c = 78.520(7)ꢁ, V = 877.42(15) A , T = 293 K,
triclinic, space group P1, Z = 2, Dc = 1.160 g cmÀ3
,
ꢀ
l = 0.079 mmÀ1, k = 0.71073 A. 4323 reflections collected,
2474 independent (Rint = 0.0340) and 1394 observed
˚
reflections,
203
refined
parameters,
R = 0.064,
wR2 = 0.125. CCDC-633961 contains the supplemen-
tary crystallographic data for this paper. These data can
be obtained free of charge from the Cambridge Crystal-
request/cif.
This study suggested that computational analysis can al-
low us to establish a pre-selection of dipeptide mimetic
to construct new families of foldamers. The use of
AMPA oligomers as templates to design more function-
alized and soluble oligomers is under investigation in
our laboratory.
15. Aubry, A.; Vitoux, B.; Marraud, M. J. Chim. Phys., Phys.
Chim. Biol. 1985, 82, 933–939.
16. Muller, G.; Gurrath, M.; Kurz, M.; Kessler, H. Proteins
1993, 15, 235–251.
17. Due to the superposed proton resonances for the Ph–CH2
protons in 3a, and to the absence of Overhauser effects
across X motifs, the middle NHs in 3a could not be
discriminated.
18. Cung, M. T.; Marraud, M.; Neel, J.; Aubry, A. Biopoly-
mers 1978, 17, 1149–1173.
Supplementary data
Experimental procedures, NMR, HPLC, and mass spec-
trometry data, and 2b X-ray data. Supplementary data
associated with this article can be found, in the online
`
19. Luppi, G.; Soffre, C.; Tomasini, C. Tetrahedron: Asym-
metry 2004, 15, 1645–1650.