can be estimated23 as 3.4 nm. The observed d = 1.8 nm peak
may be a second order reflection since it is highly unlikely this
peptide is folded.
In summary, ring-closing metathesis can be used to
create an intra-molecularly folded U-shaped peptide, whereas
inter-molecular ring-closing leads to extended a four-arm
‘‘branched’’ peptide dimer construct. The latter resembles in
some respects a cyclic peptide, although with a different
architecture (e.g. much larger branches than the side chains
on cyclic peptides) and with a distinct synthesis procedure.
Regions of these peptides must retain the b-sheet hydrogen
bonding pattern, consistent with the XRD results presented.
The conformational constraints introduced by ring-closing
hinder nanotube formation, observed for the parent uncross-
linked peptide. Instead, distinct fibrillar self-assembled nano-
structures are observed. The thickness of the fibril and ribbon
structures is related to the length of the peptides, whether
intra- or inter-molecularly ring-closed. Our results point towards
the use of ring-closing chemistries to create novel peptide
architectures, which are remarkably still able to form b-sheet
secondary structures.
Fig. 3 SAXS (and selected WAXS) data for peptide II and III in
0.5 wt% aqueous solutions. The inset shows an enlargement of the
WAXS profiles (in box) with linear intensity and q scales.
in ESI,w Fig. 14. ESI,w Fig. 15 shows typical intensity profiles
from equatorial sector averages for peptide I and peptide II.
This highlights certain features associated with the nanotube
structure of peptide I, in particular the presence of peaks at
d = 0.55 nm and d = 0.45 nm which are absent for peptide II,
the XRD pattern for which shows classical ‘‘cross-b’’ pattern
features, i.e. the 1.1 nm and 0.48 nm spacings (the same
features were observed for peptide III, data not shown). The
peaks observed for peptide I were previously observed in
oriented X-ray diffraction patterns (obtained by flow alignment)
for the heptapeptide A6K which forms nanotubes in concentrated
aqueous solution.22 A model for the origin of these peaks was
presented based on the helical wrapping of peptide dimers
(with a two-residue offset between adjacent dimers). An additional
feature noted in the fibre XRD is a d = 1.8 nm peak for both
peptides. For peptide I, it may be noted that a strong meridional
reflection presumably associated with the b-strand spacing, is
shifted such that the spacing is larger than usual, d = 0.49 nm.
The d = 0.45 nm peak is only present as a shoulder. The
d = 0.39 nm peak for peptide I is sharper and more intense than
the corresponding d = 0.38 nm peak observed for peptide II.
This peak is associated with the Ca–Ca backbone spacing.22
Molecular modeling (Cerius Molecular Dynamics using a
DREIDING force field) suggests a favored hairpin confor-
mation for peptide II, with a length approximately 1.8 nm
(Fig. 4a). This is in excellent agreement with the d spacing
observed in the fibre XRD pattern. The thickness of fibrils
observed by cryo-TEM suggests a width of three strands.
For peptide III, molecular dynamics simulations lead to a
conformation (Fig. 4b) with a planar arrangement in the cross-
linked region, and with a longest dimension approximately
3.5–4 nm. Detailed modeling of the aggregation of the peptides
into b-sheet fibrils will be the subject of future work. The length
of the decapeptide I in an antiparallel b-sheet configuration
Notes and references
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Fig. 4 Simulated conformations for (a) peptide II, (b) peptide III.
c
This journal is The Royal Society of Chemistry 2012
Chem. Commun., 2012, 48, 3757–3759 3759