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. Author manuscript; available in PMC: 2022 Jun 11.
Published in final edited form as: Rev Mod Phys. 2021 Jun 11;93(2):025008. doi: 10.1103/revmodphys.93.025008

FIG. 11.

FIG. 11

(A) A cartoon model of a (single-tailed) surfactant molecule. (B) A schematic of a spherical micelle with the thickness of the solvophobic core () and the area per head group (a) highlighted. A wedge-like portion of the micelle is cutaway to illustrate the interior packing of tails. (C) A spherocylinder model of a worm-like micelle, which has a cylindrical portion of length L capped by two hemispherical micelles of equal radius. (D) An energy landscape for spherocylinders described by the model in eq. (44) with P−1 = 2.25 and k¯=0.1. The dashed orange line shows the (L = 0) spherical micelle branch and the dashed pink line shows the (L = 0) worm-like micelle branch, whose corresponding energy as a function of reduced aggregation number is plotted in (E).