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A units, and for the first time isosteric C (carbamate[14]
)
The substitution of a CH2 for N’H at position P3 in 1a is
very conservative with little effect on the local geometry
(Figure 1). In addition, one aCH proton of the A unit behaves
as a hydrogen-bond donor and together with the amide NH
proton is in close contact with the carbonyl oxygen atom at
P5. This three-centered hydrogen bond is reminiscent of the
canonical hydrogen-bonding pattern of oligoureas.[19] Similar
bifurcated hydrogen bonds involving intermolecular CH···O
contacts have been observed previously in parallel sheet
structure arrangements formed by cyclopropane g-amino acid
derivatives.[20] The introduction of a carbamate unit into 2
replacements (1–5, Figure 1b). Although they share an
isosteric relationship, U, A, and C units are endowed with
different folding propensities. In solution and in the crystal,
aliphatic urea oligomers Un adopt well-defined right-handed
helical conformations stabilized by remote three-centered
hydrogen bonds.[7,15] The g4-peptide backbone An also shows
propensity to form helices, albeit of lower stability compared
to g2,4 and g2,3,4-substituted peptides.[3b,c,16,17] In contrast, there
is no evidence that the oligocarbamates Cn adopt a well-
defined fold.[18]
=
To assess the extent to which the canonical helical
structure of oligoureas can propagate across A and C units,
we first prepared analogues of uU5 containing one central
amide (1) or carbamate (2) linkage (P3 position). Crystals of
uU5, 1a, and 2b suitable for X-ray diffraction analysis were
obtained and structures were solved in the P212121 (uU5 and
1a) and P43212 (2b) space groups, respectively.[19] The crystal
structure of 2b contains two independent molecules (I) and
(II) in the asymmetric unit (ASU). All three oligomers are
fully helical in the solid state (Figure 2). A and C units
causes C O(5) to shift away from the main chain carbamate
oxygen atom [the distance between the two oxygen atoms is
3.7 ꢀ and 3.3 ꢀ in molecules (I) and (II), respectively] to
reduce the electronic repulsion between the carbamate and
carbonyl oxygen atoms. The carbamate NH at P3 nevertheless
=
remains within a hydrogen-bonded distance to C O(5) [D
(N···O) = 2.7 ꢀ (I and II), (N-H-O) = 155.28 (I) and 127.08
(II)]. Superimposition of the two independent molecules I
and II in the crystal structure of 2b is shown in Figure 2d. The
overall conformation of 2b(I) and 2b(II) is similar, but the
hydrogen-bonding scheme differs perceptibly between the
two independent molecules, thus reflecting backbone dynam-
ics. Complementary hydrogen-bonding sites are fully satisfied
in 2b(I) with NH and N’H of U units at positions P1, P2, and
P4 engaged in three-centered hydrogen bonds as in uU5. In
contrast, the carbonyl groups are slightly shifted in 2b(II) and
remaining hydrogen bonded to only one NH [i.e., N’H(U1),
N’H(U2), N’H(U4)].
The helical character of 1 and 2 was further investigated
by 1H NMR spectroscopy in CD3OH. As an indicator of
folding propensity, the diastereotopicity values of main chain
methylene protons (Dd) were measured and compared for all
three oligomers.[19,21]
The Dd values measured for backbone U methylene
protons in 1a (0.73 < Dd < 1.07 ppm) and 2a (0.60 < Dd <
0.97 ppm) compared to those of uU5 (0.81 < Dd < 1.31 ppm)
suggest folding, but also possible distortion from the original
helix geometry. This destabilization is likely to arise from the
loss of one hydrogen bond, an increased flexibility and/or
from local backbone rearrangement (e.g. as a result of
electronic repulsion in 2). The significant diastereotopicity
observed for methylene protons in the A and C units at P3
Figure 2. Structures of uU5, 1a, and 2b in the crystalline state. a) X-ray
crystal structure of uU5. b) X-ray crystal structure of 1a. c) Comparison
of helical conformations formed by the two independent molecules
2b(I) and 2b(II) in ASU. d) Overlay of 2b(I) and 2b(II) (side chains
are omitted). Carbon atoms in A and C units are depicted in orange
and green, respectively.
b
a
(Dd = 0.77 ppm and 1.09 ppm for CH2 in A unit and CH2
protons in C unit, respectively) is also indicative of a folded
b
accommodate the helix geometry with torsion angles f, q1,
and q2 (A unit in 1: À110.78, 55.08, 65.68; C unit in 2b:
À121.88, 54.38, 79.68), in the range of values measured for the
corresponding U unit in uU5 (À101.48, 54.48, 77.68). The mean
torsion angles f, q1, and q2 in U units do not vary significantly
between uU5, 1a (À108.88, 54.88, 77.18), and 2b [À111.58,
60.68, 78.98(I)) and (À107.68, 54.38, 87.08(II)]. An overlay of
the structures of 1a and 2b with that of uU5, by fitting the five
pairs of b-carbon atoms (U and C units) or g-carbon atoms
(A unit), indicated a close match between uU5 and 1a (root-
mean square deviation values (RMSD) of 0.150 ꢀ) and
pointed to larger differences between the backbone confor-
mations of uU5 and 2b [RMSD of 0.535 ꢀ (I) and 0.760 ꢀ
(II)].
conformation in 1a and 2a. The Dd value observed for CH2
in the Aunit of 1a compares favorably with that measured for
central residues in a helically folded g4 hexapeptide (ca. 0.43–
0.47 ppm in CD3OH).[16] Evidence that 1 adopts a helical
conformation akin to that of uU5 in solution came from the
observation of characteristic medium to strong i/(i+1) and
i/(i+2) nuclear Overhauser enhancements (nOes).[19]
Although a detailed NMR investigation of 2a was hampered
by resonance overlaps in the NH/CH fingerprint region,
several medium to weak inter-residue nOes consistent with
helical folding were unambiguously assigned in the ROESY
spectrum of 2a.[19] These results confirm that the 2.5-helix
geometry can accommodate discrete replacement of U units
by A and C units. Additional insight into the relative stability
4148
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2013, 52, 4147 –4151