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. 2020 Jan 22;6(3):413–419. doi: 10.1021/acscentsci.9b01216

Figure 2.

Figure 2

Hierarchical deformation. (a) LBL self-assembly is regulated by molecular (nbb, nsc, nL) and morphological (Rsc, DL, Rin, l) parameters, where Rsc - brush radius, DL - L-block domain diameter, and l - distance between neighboring side chains along the bottlebrush contour. (b) The cascade of deformation mechanisms during uniaxial extension of LBL networks: (1) unfolding of bottlebrush filaments limited by funfold < kBT/bKkBT/Rsc ≅ 0.5 pN (for nsc = 70), (2) stretching of backbones inside brush envelops ranging within kBT/Rsc < fstretch < kBT/l0 ≅ 20 pN, where l0 = 0.25 nm is the monomer projection length, and (3) pulling linear chains from microdomains creating a new interface between exposed linear block sections and the bottlebrush matrix. The two-head arrow indicates that chain pulling may overlap with backbone stretching. The pulling force is on the order of fpullγLBl0 ≅ 2.5 pN, where γLB ≅ 10 mN is the surface energy of the L–B interface. The actual fpull value may be higher due to kinetic barriers imparted by glassy L-domains.