Despite border temperature coefficients in DMSO-d6,
small chemical shift variations (around 1 ppm) along the
DMSO-titration experiments indicated the participation
of these amide protons in an intramolecular hydrogen
bond. Finally, all measured parameters for the additional
NH(iPr) in 4, i.e. small temperature coefficient in CDCl3,
large value in DMSO-d6, and large chemical shift differ-
ence between CDCl3 and DMSO-d6 (ΔNH = 2.16 ppm),
indicated a solvent-accessible NH proton.
To gain further information on the hydrogen bond
network, FT-IR spectroscopy studies were undertaken.
As previously mentioned, frequencies of amide A and
amide I bands corresponding to NH and CO stretching
vibrations, respectively, depend on the involvement of
vibrators in hydrogen bonds.10 Typically, the frequencies
of stretching vibrations decrease with hydrogen bonding
formation. Those of the hydrogen bonded NH and CO
amide rise below 3400 and 1680 cm,À1 respectively, and
overlaps between “bound” and “free” bands are common
in the latter case. Moreover, with the time scale of infrared
spectroscopy being faster than that of NMR, an infrared
spectrum can contain the spectral contributions of all
components of a pool of conformers.11 Thus, for the same
CO or NH function, it should be possible to see both the
bonded and nonbonded forms.
band at a lower frequency (3295 cmÀ1) than 10, which
showed a major band at 3343 cmÀ1 and a shoulder at
3300 cmÀ1. Moreover, the ratio of the integrated intensity
of the hydrogen-bonded NH bands to free NH bands
(AH/AF)13 was much higher in the case of the ABOC
containing tripeptide (AH/AF = 1.94) than in the case of
the β-Ala analog (AH/AF = 0.89). This suggested a higher
involvement of NH groups in intramolecular interactions
in 4 compared to 10. Finally, in the amide I region (Figure
S1H), a free CO band at 1675 cmÀ1 was only observed for
10, which confirmed the previous observations of a higher
structuration level for 4.
In order to assign the positions of free NH and CO
vibrators of tripeptides 3 and 4, we first studied precursors
6, 7, 8, and 9 (Tables S1 and S2 and Figure S1AÀD). For
these precursors, we found no evidence of strong bonded
NH absorption bands as could be observed in the intra-
molecular reverse turn or in intermolecular interactions.12
However, the (S)-ABOC motif led to a new band at 3398
cmÀ1 in precursor 8, suggesting a certain contribution of
H-bonded species (Figure S1A). In the case of 4 a broad
band at 3295 cmÀ1 suggested the existence of a stronger
hydrogen-bonding interaction and therefore a higher level
of structuration (Figure S1A). No distinguishable band
around 3300 cmÀ1 was observed for 3, but an enlargement
ofthe signalsuggested anemergenthydrogen bond (Figure
S1B). Nevertheless for this tripeptide, a shoulder around
1655 cmÀ1 corresponding to a hydrogen bonded CO
stretch was present (Figure S1D). The study of CO stretch-
ing vibrations of all compounds showed either a global
shift of vibrators to lower frequencies or shoulders, both
related to bonded carbonyls. Both FT-IR amide A and
amide I band analyses of 3 and 4 confirmed the involve-
ment of NH and CO groups in hydrogen-bonding inter-
actions. In addition, comparison of 10 with 4 showed a
higher level of structuration for the latter. Indeed, in the
amide A region (Figure S1G), 4 revealed a NH bonded
Figure 2. ROE long-range distances (red arrows) in CDCl3 at
298 K for 3 and 4.
To gain more insight into the conformation of com-
pounds 3 and 4 in solution, we recorded CD spectra in
CD3CN and performed NMR studies based on ROESY
spectra (10 mM, 298 K) in CDCl3 and CD3CN. As no
signal could be detected for 2, the similar CD spectra of
3 and 4 with a maximum around 220 nm could indicate the
presence of comparable structuration (Figure S2). For
both compounds, ROE derived distances as upper bound
distances were used for structural calculations (Table S7).
The ROE long-range distances in CDCl3 are reported in
Figure 2. For the structure calculations using AMBER10,
21 and 19 distance restraints for 3 and 22 and 20 distance
restraints for 4 in CDCl3 and CD3CN respectively were
introduced. As expected, the set of ROEs observed on the
ROESY spectra were very close for 3 and 4 in both
solvents. The characteristic ROE long-range distances
between protons on each side of the ABOC residue sug-
gested a reverse turn scaffold for both compounds. The 15
lowest energy structures of 3 and 4 in CDCl3 and CD3CN
are reported in Figure S6. As indicated, the root-mean-
square deviations (rmsd) fit on backbone heavy atoms
were very low in the four calculated sets of structures and
decreased significantly when the terminal flexible moieties
were omitted (rmsd around 0.2). Indeed, we noticed that
the backbone trace of Ala-(S)-ABOC-Phe was particularly
(10) (a) Byler, D. M.; Susi, H. Biopolymers 1986, 25, 469. (b)
Arrondo, J. L. R.; Muga, A.; Castresana, J.; Goni, F. M. Prog. Biophys.
Mol. Biol. 1993, 59, 23. (c) Vass, E.; Hollosi, M.; Besson, F.; Buchet, R.
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(11) Vass, E.; Kurz, M.; Konat, R. K.; Hollosi, M. Spectrochim.
Acta, Part A 1998, 54, 773.
(12) (a) Chung, Y. J.; Huck, B. R.; Christianson, L. A.; Stanger,
H. E.; Krauthauser, S.; Powell, D. R.; Gellman, S. H. J. Am. Chem. Soc.
2000, 122, 3995. (b) Allix, F.; Curcio, P.; Quoc, N. P.; Pickaert, G.;
Jamart-Gregoire, B. Langmuir 2010, 26, 16818.
(13) (a) Benedetti, E.; Bavoso, A.; Di Baso, B.; Pavone, V.; Pedone,
C.; Crisma, M.; Bonora, G. M.; Toniolo, C. J. Am. Chem. Soc. 1982, 104,
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