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. Author manuscript; available in PMC: 2017 Nov 9.

Published in final edited form as: Soft Matter. 2016 Nov 9;12(44):8990–8998. doi: 10.1039/c6sm01498d

FIG. 6 — The number of faces in a circular geometry is plotted as a function of R_np for results from exact energy minimizing configurations (points) and the bead intercalation theory (red dotted line), and as a function of ψ for the theory (Eqs. (8), line, with δG set to unity). Snapshots from Monte Carlo simulations in which ϵ is gradually increased to 30 are shown on top, with rods colored blue and the nanoparticle in green. The rod length is n_b = 6.

FIG. 6 — The number of faces in a circular geometry is plotted as a function of R_np for results from exact energy minimizing configurations (points) and the bead intercalation theory (red dotted line), and as a function of ψ for the theory (Eqs. (8), line, with δG set to unity). Snapshots from Monte Carlo simulations in which ϵ is gradually increased to 30 are shown on top, with rods colored blue and the nanoparticle in green. The rod length is n_b = 6.

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