.
Angewandte
Communications
tively, when the capping groups are omitted. The tetramer 3a
and the hexamer 3b exhibited tight right-handed 9-helix
…
=
structures stabilized by C O(i) HN(i+2) hydrogen bonds.
Notably only two residues were necessary to initiate the
folding into C9 hydrogen-bonded pseudocycles as observed on
dimer 2. The hydrogen-bonding patterns were homogenous
along the entire sequences in a forward direction, from N to
C. The average values of the dihedral angles for the ATC helix
were f= ꢁ76 ꢂ 168, q = 128 ꢂ 128, z = ꢁ6 ꢂ 58, and y =
ꢁ28 ꢂ 68 (Table 1). Only small distortions were observed on
the y angles of the C-terminal residues of each oligomer.
Table 1: Average backbone torsion angles for g-peptides adopting 9-
helical fold. The y angles of the last residue of the NMR and XRD
structures were omitted.
f
q
z
y
Balaram’s oligomers[9b]
Kunwar’s oligomers[9a]
Predicted Z-vinylogous
g-oligomers[13]
1098
1258
ꢁ79.88
ꢁ638
ꢁ688
122.88
ꢁ778
ꢁ658
888
978
ꢁ46.58
0.18
ATC oligomers
Average NMR values:
2, 3a, 3b
3d, 3e, 3 f
Figure 1. Superimposition of the NH/gCH region of the TOCSY (in
dark) and ROESY (in light) spectra of a) 3b recorded in CDCl3, b,c) 3 f
recorded in CD3OH and H2O/D2O, pH 6.5 at 2–10 mm. Typical strong
sequential NOE correlations of HN(i)/gCH(iꢁ1) are annotated. 1H
chemical shifts on both axes are given in ppm. HG corresponds to
gCH. d) Typical interresidue NOE pattern along the 3b and the 3 f
hexamers.
ꢁ76ꢂ168 128ꢂ128 ꢁ6ꢂ58 ꢁ28ꢂ68
ꢁ72ꢂ338 114ꢂ298 ꢁ5ꢂ68 ꢁ23ꢂ118
XRD structure of 3c
ꢁ78ꢂ38
127ꢂ148
0ꢂ38 ꢁ41ꢂ48
Importantly, we were able to crystallize the tetramer 3c by
solvent diffusion of diisopropyl ether into a solution of the
oligomer in toluene. Low-resolution X-ray diffraction data
were sufficient to show that ATC g-peptides adopt the same
helical structure in solid state and solution (Figure 2a,b). All
amide groups of the molecule form inter- or intrahelix
hydrogen bonds (Figure S7). The typical average dihedral
angles were comparable to those measured in NMR-spectro-
scopic experiments (f= ꢁ78 ꢂ 38, q = 127 ꢂ 148, z = 0 ꢂ 38
and y = ꢁ41 ꢂ 48, Table 1) with a notable deviation of the C-
terminal y torsion angle (y = ꢁ1658), which allowed the
packing of the molecules into infinite chains in the crystal.
Simulations of Hofmann and co-workers predicted that Z-
vinylogous g-oligomers could adopt a helical fold with nine-
membered hydrogen-bonded pseudocycles with close torsion
angles (f= ꢁ79.88, q = 122.88, z = 0.18, y = ꢁ46.58).[13] By
comparison, the C9 hydrogen-bonded helices reported by the
research groups of Balaram and Kunwar have values of f=
1098, q = ꢁ638, z = ꢁ778, y = 888 and f= 1258, q = ꢁ688, z =
ꢁ658, y = 978, respectively.[9] Considering the global shape of
the ATC oligomers, the edifice appeared to be close to a C3-
symmetric helix with three residues to achieve a complete
rotation with a pitch of 11.8 ꢀ. This helix had a rise-per-
residue of 3.9 ꢀ and exhibited six substitution patterns per
turn, which were distributed around a 608 angle all along the
axis (Figure 2c). We then solved the NMR solution structures
of the compounds 3d, 3e, and 3 f in water (pH 6.5) by using
12, 49, and 72 constraints, respectively, with the generalized
Born solvation model[18] in AMBER (Figure 3a and S5,
Table 1). As expected, since similar NOE sets were obtained
for the water-soluble series (Tables S20–22), comparable
typical (i, i + 2), (i, i + 3) medium-range NOEs were
detected.[15] Whatever the length of the oligomers and the
nature of the solvent, all the amide protons exhibited
remarkable downfield chemical shifts, for example, from
9.18 ppm for dimer 2 (Table S1) to 10.67 ppm for hexamer 3b
in CDCl3 (Table S5). As a comparison, Kunwar and co-
workers previously described a 9-helix for a g-peptide
oligomer in which amide resonances were found between
6.92 and 7.60 ppm in CDCl3.[9a] This marked unshielding of
the amide protons could be attributed to a highly stable
hydrogen-bonding pattern and/or to a ring-current effect of
the thiazole heterocycle. In addition, 3J(NH,gCH) values
smaller than 6 Hz (5.4 ꢂ 0.4 Hz) were typical of f values
around ꢁ608 (Table S19). Taken together, these data were
strong evidence of a well-organized system in solution for all
compounds whatever the solvent considered.
The ATC monomers were parameterized using the
Antechamber package[16] starting from the X-ray crystal
structure of 6b, which exhibited an extended conformation
with dihedral angles f= ꢁ1268, q = 1588, z = ꢁ48 and y =
1808 (Figure S6 and Table S25). NOEs were used as restraints
for calculations on the structure in solution determined by
NMR spectroscopy by using a simulated annealing protocol
with AMBER 10.[17] The solution structures of 2, 3a, and 3b in
CDCl3 were solved by using 39, 87, and 124 unambiguous
restraint distances, respectively. Figure S5 depicts a super-
imposition of the 20 lowest-energy structures calculated for
each compound. The root-mean-square deviation (RMSD)
values for the backbone are 0.11 ꢀ, 0.48 ꢀ, 0.63 ꢀ, respec-
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2013, 52, 6006 –6010