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. 2022 Apr 20;13:2162. doi: 10.1038/s41467-022-29804-5

Fig. 4. Coarse-grained model of self-assembling supramolecular polymers.

Fig. 4

a Molecular structure of a BTA monomer core (top), which can be decorated with generic (e.g., solvophilic) side chains. Bottom: CG model of a BTA-like solvophilic monomer (left), which interacts directionally with monomers of the same specie (right). b Snapshot of BTA fibres formed spontaneously after tCG = 20 μs of CG-MD, starting from 500 dispersed BTA monomers. A single fibre is highlighted and reported in the frame on the left. c Time evolution of the assembly-size populations (in percentage of monomers) for the BTA model at T = 320 K (top) and M model with ϵ = 45 kJ mol−1 (bottom) at the equilibrium. d Distribution of assemblies of different sizes (percentage over the average number of assemblies) for different BTA and M systems. e Cumulative molecular traffic (left) and flux (right)55 vs. time for different BTA and M systems at the equilibrium (same colours of (d)).