A number of short peptide amphiphiles consisting of dipeptides linked to fluorenylmethoxycarbonyl spontaneously form fibrous hydrogels under physiological conditions (see figure). The structural and physical properties of these gels are dictated by the amino acid sequence of the peptide building blocks, and the gels support the three‐dimensional cell culture of chondrocytes.
Bovine insulin has long been known to self-assemble in vitro into amyloid fibrils. We have observed a further higher-order selfassociation of the protein into spherical structures, with diameters typically around 50 m but ranging from 10 to 150 m. In a polarizing light microscope, these structures exhibit a ''Maltesecross'' extinction pattern typical of spherulites. Spherical structures of a similar size distribution can be observed in the environmental scanning electron microscope, which also reveals the presence of significant amounts of water in the structures. The spherulites contain a large quantity of well defined amyloid fibrils, suggesting that they are formed at least in part as a consequence of the self-assembly of preformed fibrils. Similar structures also have been observed in the tissues of patients suffering from amyloid disorders. The ability of amyloid fibrils to form such higher-order assemblies supports the hypothesis that they represent a generic form of polypeptide structure with properties that are analogous to those of classical synthetic polymers.
A thermoreversible fibrillar hydrogel has been formed from an aqueous lysozyme solution in the presence of dithiothreitol (DTT). Its physical properties and potential as a tissue engineering scaffold have been explored. Hydrogels were prepared by dissolving 3 mM protein in a 20 mM DTT/water mixture, heating to 85 degrees C and cooling at room temperature. No gel was observed for the equivalent sample without DTT. The elastic nature of the gel formed was confirmed by rheology, and the storage modulus of our gel was found to be of the same order of magnitude as for other cross-linked biopolymers. Micro differential scanning calorimetry (microDSC) experiments confirmed that the hydrogel was thermally reversible and that gelation and melting occurs through a solid-liquid-like first-order transition. Infrared spectroscopy of the hydrogel and transmission electron microscopy studies of very dilute samples revealed the presence of beta-sheet-rich fibrils that were approximately 4-6 nm in diameter and 1 mum in length. These fibrils are thought to self-assemble along their long axes to form larger fibers that become physically entangled to form the three-dimensional network observed in both cryo-scanning electron microscopy (cryo-SEM) and small-angle neutron scattering (SANS) studies. The hydrogel was subsequently cultured with 3T3 fibroblasts and cells spread extensively after 7 days and stretched actin filaments formed that were roughly parallel to each other, indicating the development of organized actin filaments in the form of stress fibers in cells.
Self-assembling peptide-based hydrogels have The formation of hydrogels by self-assembling peptides 44 involves two distinct processes; the self-assembly of the 45 peptides themselves to form thin fibrillar structures and the 46 entanglement and association of these fibrils into a threef1 47 dimensional percolated network (Figure 1). Developing a 48 fundamental understanding of these two processes at all length 49 scales is crucial as the properties of the final materials will not 50 only depend on the intrinsic properties of the fibers, but also on In this work we were interested in understanding how 77 network topology affects the mechanical properties of the 78 hydrogel and how it can be used to design materials with 79 tailored properties. For this purpose we decided to use a family 80 of octapeptides based on the same design that are known to 81 self-assemble into β-sheet rich fibrils. This approach allowed us 82 to keep the fiber structure identical across all the systems and 83 focus on the effect of network topology on the mechanical 84 properties of the hydrogels formed. As mentioned above due to 85 the design chosen interfiber interactions are controlled mainly 86 by the hydrophilic residues. Of particular interest to us was 87 arginine, which is a residue that has a guanidine side group. 88 were assessed in an oscillatory mode, using a stress-controlled ) < 2.4, with q = 171 (4π/λ) sin(θ/2), where θ is the scattering angle. The collected data 172 was corrected for the detector efficiency and dark current background. 173 Counter normalization was achieved by using the incoherent scattering 174 of an amorphous hydrogenous poly(methyl methacrylate) secondary 175 standard. After ensuring the scattering was isotropic, the data were 176 radially averaged to obtain a one-dimensional scattering curve. Under 177 these conditions, the normalized intensity scattered by a sample is
The effect of peptide charge on the self-assembly, gelation behavior, and model drug release profiles has been explored here for three octa-peptides, VEVKVEVK (VEK2), VKVKVEVK (VEK3), and VEVEVKVE (VEK1), that carry a net charge of 0, +2, and -2 at neutral pH, respectively. Transparent, self-supporting hydrogels were found to form above a critical concentration when the peptide charge modulus was >1 and this was independent of the sign of the charge. TEM, SAXS, and shear rheology revealed that there were no differences in hydrogel structure or mechanical properties when the peptides were at the same concentration and carried the same charge modulus. All peptides were found to form dense fibrillar networks formed by β-sheet rich single fibers where lateral aggregation of the fibers occurred and increased with decreasing charge modulus. Such behavior was found to correlate with an increase in hydrogel mechanical properties, demonstrating that fiber lateral aggregation is inextricably linked with the mechanical properties of these hydrogels. Two hydrophilic model drug molecules, namely napthol yellow (NY) and martius yellow (MY), were subsequently incorporated within the VEK1 and VEK3 hydrogels at pH 7 and although they did not effect the self-assembly of the peptide at a molecular level, they did effect the level of lateral fiber aggregation observed and, therefore, the mechanical properties of the hydrogels. The release of each molecule from the hydrogels was monitored over time and shown to be controlled by Fickian diffusion where the diffusion rate, D, was dependent on the ratio between the overall effective charges carried by the peptide, i.e., the fibrillar network, and the overall charges carried by the guest molecules, but independent from the hydrogel concentration and mechanical properties within the ranges investigated. This work highlights the possibility of controlling the rate of release of small drug molecules by manipulating the charges on the guest molecules as well as the charged state of the self-assembling peptide.
We investigate the possibility of using the protease thermolysin to drive the synthesis and gelation of ionic-complementary peptides from nongelling precursors. In this system, short peptide fragments are continuously interconverted to form a dynamic peptide library, which eventually favors synthesis of peptides that are thermodynamically stabilized by molecular self-assembly. Thermolysin was added at a fixed concentration (0.3 mg mL(-1)) to solutions (0-300 mg mL(-1)) of the short tetrapeptide FEFK. Initially, the protease partially hydrolyzed the tetrapeptide into dipeptides in all samples. Subsequently, longer peptide sequences were found to form through reverse-hydrolysis. The stability of the different sequences was found to be dependent on their self-assembling properties. The sequences that self-assembled into antiparallel beta-sheet rich fibers became the stable products for the reverse hydrolysis reaction, while the others formed were unstable and disappeared with increasing incubation time. Ultimately, the main product of the system was octapeptide, which suggests that it represents the thermodynamically favored product of this dynamic library. Its concentration dictated the gelation behavior of the sample, and gels with moduli up to 25 kPa where obtained depending on the initial concentration of tetrapeptide.
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