Table 1: The conditions and properties of the nucleopeptidic hydrogelators and corresponding supramolecular nanofibers and hydrogels.
Sample
1A
1G
1T
1C
3A
3G
3T
3C
concentration [wt%]
pH
2.0
5.0
2.0
5.0
2.0
5.0
2.0
5.0
2.0
7.4
2.0
7.4
2.0
7.4
2.0
7.4
optical images
width of nanofibers [nm]
critical strain [%]
16
1.0
8090
>500
15
0.8
12613
>500
9
1.2
6346
>500
10
0.6
26
>500
20
0.4
2082
>500
14
2.0
682
>500
9
5[a]
–
8.0
2.9
>500
storage modulus G’ [Pa]
–
IC50 [mm][b]
>500
[a] These thin nanofibers have low quantity and coexist with nanoparticles, thus fail to result in a hydrogel. [b] Concentration required for 50 %
inhibition of cell viability.
storage moduli of hydrogels of 1A, 1G, 3A, and 3G may stem
from purine bases that favor the formation of Hoogsteen base
pair,[12] in addition to strong p–p interactions of purine
nucleobases that contain two fused five- and six-membered
heterocyclic rings. Moreover, the lower storage moduli of the
hydrogels of 3 relative to those of the corresponding hydro-
gels of 1 suggest that the presence of tyrosine may reduce the
efficiency of the noncovalent interactions required for the
stabilization of self-assembled nanostructures, thus resulting
in a relatively weak viscoelastic property of those hydrogels.
Furthermore, the addition of an oligomeric deoxyadeno-
sine (A10) to the hydrogel of 1Tor 3Tresults in a more stable
hydrogel (see Figures S3 and S6 in the Supporting Informa-
tion), as demonstrated by the increase of storage modulus
(G’) from 6.3 KPa (of hydrogel 1T) to 14.3 KPa (of the
hydrogel of 1T and A10), or from 2.9 Pa (of hydrogel 3T) to
12.0 Pa (of the hydrogel of 3T and A10; see Figure S6 in the
Supporting Information). This result suggests that Watson–
Crick interactions between the self-assembly of 1T (or 3T)
and A10 favor molecular aggregation and enhance the
mechanical strength of the hydrogels. To further examine
Watson–Crick H-bonding between complementary nucleo-
bases among the hydrogelators, we use hydrogelators of 1T
and 1A (or 3Tand 3A) to prepare a mixed hydrogel and find
that the storage modulus (G’) increases from 6.3 KPa (of
hydrogel 1T) to 18 KPa (of the hydrogel of 1T and 1A), or
from 2.9 Pa (of hydrogel 3T) to 150 Pa (of the hydrogel of 3T
and 3A). The mixed hydrogel of the mismatched nucleobases
(i.e. 1T and 1G or 1T and 1C) exhibits, however, little
increase of the storage moduli (see Figure S8 in the Support-
ing Information) in comparison to that of hydrogel 1T. These
results indicate that these nucleopeptidic hydrogelators
preserve Watson–Crick interactions of the nucleobases.
We used circular dichroism (CD) to study the super-
structures of these nanofibers of self-assembled nucleopep-
tides in the gel phase. The hydrogels of 1 have the common
feature of b-sheet structure according to the CD spectra with
a positive peak near 195 nm and a negative peak around
210 nm (see Figure S3 in the Supporting Information),
suggesting that these nucleopeptides arrange into b-sheet-
like configurations. The hydrogels of 3A, 3G, and 3T display
the common feature of CD spectra with a positive peak near
195 nm and a negative peak around 210 nm, which also
suggests that the nucleopeptides adopt b-sheet-like config-
urations. The CD spectrum of the 3C solution exhibits a
positive peak near 203 nm and a negative peak around
215 nm, which red-shifts relative to the signals of typical b-
sheet configuration. The red-shifted signal related to b-sheet-
like configurations is likely associated with a structure, which
is twisted relative to the standard planar b-sheet structure,
agreeing with the fact that the increase in b-sheet twisting
causes disorder and results in short nanofibers and nano-
particles, which leads to weak mechanical strength.[13] Overall,
the signals of b-sheet structures (i.e. transitions at 195–
225 nm) of 1 are stronger than those of 3, following the trend
that the storage modulus of 1 is larger than that of 3. The CD
signals with broad bands around 300 nm among the hydrogels
1 and 3 likely originate from the formation of mesophases of
hydrogelators because they locate far from the chromophoric
absorption region (ca. 270 nm) of the hydrogelators (see
Figure S4 in the Supporting Information).
Similar to other nucleobase-containing small molecules
that bind with nucleic acids through Watson–Crick interac-
tion,[14] hydrogelators 1T or 3T also bind to oligomeric
deoxyadenosine (e.g. A10), which results in distinctive
changes in the CD spectra. For example, comparing to the
CD of hydrogel 1T, the CD of the 1T–A10 mixed gel (see
Figure S5 in the Supporting Information) exhibits the
decreased ellipticity of positive bands at 192 and 228 nm
and negative bands around 205, 247, and 287 nm. The CD
spectrum of the 3T–A10 mixed gel (see Figure S5 in the
Supporting Information) shows that the addition of A10 both
changes the intensity of the bands at 195 and 205 nm and
creates a new band at 303 nm that possibly is a result of the
conformational change of the self-assembled structures of 3T
induced by A10.[14a–c] In addition, compared to the solution of
1T or 2T, the CD spectra of the mixed solution of A10 with
hydrogelator 1T (or precursor 2T) shows slight changes in the
band shape, indicating the relatively weak interaction in the
solution state (see Figure S5 in the Supporting Information).
We also used molecular mechanical (MM) calculations to
evaluate noncovalent interactions[15] and simulate the width
of the nanofibers of 1. As shown in Figure 3a, the simulated
widths of the nanofibers are 15, 16, 9, and 11 nm for
nucleopeptides 1A, 1G, 1T, and 1C, respectively, which
correlate well with experimental observations (Figure 2).
Angew. Chem. Int. Ed. 2011, 50, 9365 –9369
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim