| Literature DB >> 31624265 |
Julia Y Rho1, Henry Cox2, Edward D H Mansfield1, Sean H Ellacott1, Raoul Peltier1, Johannes C Brendel1, Matthias Hartlieb1, Thomas A Waigh2,3, Sébastien Perrier4,5,6.
Abstract
Self-assembling peptides have the ability to spontaneously aggregate into large ordered structures. The reversibility of the peptide hydrogen bonded supramolecular assembly make them tunable to a host of different applications, although it leaves them highly dynamic and prone to disassembly at the low concentration needed for biological applications. Here we demonstrate that a secondary hydrophobic interaction, near the peptide core, can stabilise the highly dynamic peptide bonds, without losing the vital solubility of the systems in aqueous conditions. This hierarchical self-assembly process can be used to stabilise a range of different β-sheet hydrogen bonded architectures.Entities:
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Year: 2019 PMID: 31624265 PMCID: PMC6797743 DOI: 10.1038/s41467-019-12586-8
Source DB: PubMed Journal: Nat Commun ISSN: 2041-1723 Impact factor: 14.919
Fig. 1Self-assembling cyclic peptide-diblock polymer conjugates. The conjugation of carboxylic acid diblock co-polymer (pBA-b-pDMA, 1) with the diamine functionalised cyclic peptide. In aqueous conditions, the conjugated cyclic peptide-diblock conjugate (CP-(pBA-pDMA)2, 3) self-assembles to form a hydrophobic core around the peptide and a hydrophilic corona
Fig. 2Characterisation of cyclic peptide-polymer nanotubes. a Transmission electron microscopy (TEM) of the diblock conjugates prepared in water. b Small-Angle Neutron Scattering (SANS) of the diblock (12) and control (13) conjugates fitted to a cylindrical micelle model using SASfit software. The error bars plotted are standard error of the mean. c Table of the average length of the nanotubes measured via TEM, SANS and static light scattering (SLS), respectively
Fig. 3Dynamics of cyclic peptide-polymer nanotubes. The calculated length of the nanotubes from static light scattering over a range of concentrations (0.1–3.0 mg mL−1) before and after sonication
Fig. 4Kinetics of cyclic peptide-polymer nanotubes. a The orthogonal functionalization of cyclic peptide (CP) with two polymer arms and a donor or acceptor FRET dye. b Schematic of stable non-exchanging CP-polymer nanotubes. c Scheme of dynamically exchanging mixed CP-polymer nanotubes. d Graph to show the change in FRET ratio over time measured using fluorescence spectroscopy
Rate constants for FRET exchange, final and maximum FRET ratio and degree of mixing for the free dye, diblock (5 and 6) and control (7 and 8) dye conjugates
| Sample | k1/s−1 | k2/s−1 | Final FRET ratio | Maximum FRET ratio | Degree of mixing/% |
|---|---|---|---|---|---|
| Free dye | 0 | 0 | 0.14 | 0.14 | – |
| Diblock conjugate | 0.0961 | 0.314 | 0.39 | 0.96 | 41 |
| Control conjugate | 0.0272 | 5.35 | 0.54 | 0.61 | 89 |
Rate constants were determined by fitting to a second order decay function, see Supplementary Fig. 8. Final FRET ratio was reached for the diblock and control conjugates after 7 days and 60 min, respectively
Fig. 5Composition of cyclic peptide-polymer nanotubes. Schematic and stochastic optical reconstruction microscopy (STORM) of a co-injected and b premixed cyclic peptide-polymer-dye conjugates