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. 2021 May 10;22(5):2171-2180.
doi: 10.1021/acs.biomac.1c00253. Epub 2021 Apr 8.

Secondary Structure-Driven Self-Assembly of Thiol-Reactive Polypept(o)ides

Affiliations

Secondary Structure-Driven Self-Assembly of Thiol-Reactive Polypept(o)ides

Tobias A Bauer et al. Biomacromolecules. .

Abstract

Secondary structure formation differentiates polypeptides from most of the other synthetic polymers, and the transitions from random coils to rod-like α-helices or β-sheets represent an additional parameter to direct self-assembly and the morphology of nanostructures. We investigated the influence of distinct secondary structures on the self-assembly of reactive amphiphilic polypept(o)ides. The individual morphologies can be preserved by core cross-linking via chemoselective disulfide bond formation. A series of thiol-responsive copolymers of racemic polysarcosine-block-poly(S-ethylsulfonyl-dl-cysteine) (pSar-b-p(dl)Cys), enantiopure polysarcosine-block-poly(S-ethylsulfonyl-l-cysteine) (pSar-b-p(l)Cys), and polysarcosine-block-poly(S-ethylsulfonyl-l-homocysteine) (pSar-b-p(l)Hcy) was prepared by N-carboxyanhydride polymerization. The secondary structure of the peptide segment varies from α-helices (pSar-b-p(l)Hcy) to antiparallel β-sheets (pSar-b-p(l)Cys) and disrupted β-sheets (pSar-b-p(dl)Cys). When subjected to nanoprecipitation, copolymers with antiparallel β-sheets display the strongest tendency to self-assemble, whereas disrupted β-sheets hardly induce aggregation. This translates to worm-like micelles, solely spherical micelles, or ellipsoidal structures, as analyzed by atomic force microscopy and cryogenic transmission electron microscopy, which underlines the potential of secondary structure-driven self-assembly of synthetic polypeptides.

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Conflict of interest statement

The authors declare the following competing financial interest(s): Matthias Barz holds the patent Thiol-protected amino acid derivatives and uses thereof WO2015169908A1.

Figures

Scheme 1
Scheme 1. Synthesis of Block Copolypept(o)ides with Varying Secondary Structures
Figure 1
Figure 1
Analytical gel permeation chromatography in HFIP. (A) pSar-b-p(dl)Cys (P3–P6), (B) pSar-b-p(l)Cys (P7–P10), and (C) pSar-b-p(l)Hcy (P11–P14), with the respective pSar macroinitiators (P1 and P2).
Figure 2
Figure 2
Secondary structure analysis of pSar-b-p(dl)Cys, pSar-b-p(l)Cys, and pSar-b-p(l)Hcy. (A) FT-IR spectroscopy and (B) 1H NMR spectroscopy.
Figure 3
Figure 3
Influence of the secondary structure on the aggregation behavior. (A) Schematic illustration of the dynamic range. (B) Aggregation curve of polypept(o)ides (P3, P7, and P11) with sigmoidal fit.
Figure 4
Figure 4
Aggregation curves for copolymers P3–P14. (A) pSar-b-p(dl)Cys, (B) pSar-b-p(l)Cys, and (C) pSar-b-p(l)Hcy.
Figure 5
Figure 5
Self-assembly and core cross-linking. (A) Schematic illustration of secondary structure-driven self-assembly. (B) Single-angle DLS analysis of polymeric micelles (left: pSar-b-p(dl)Cys and pSar-b-p(l)Cys, right: pSar-b-p(l)Hcy). Morphological analysis of core cross-linked polymeric micelles by AFM and cryoTEM: (C) pSar-b-p(dl)Cys, (D) pSar-b-p(l)Cys, and (E) pSar-b-p(l)Hcy.

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