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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. 19.

FIG. 19

(A) Assembly ‘phase diagram’ for the capsid model (B → ∞ model of the fluid capsule model). The boundaries between the different kinetics regimes discussed in the text are shown as a function of capsid size and supersaturation Φ/Φs = eβΔμ. The calculation was performed using Eqs. 68, 5, 71 with α = 1, and C2. We set ϵmin = −15kBT and λ=ϵT/2a01/2 as in Fig. 18. (B), (C) TEM images of in vitro assembly of empty capsids from CCMV capsid proteins. (B) corresponds to productive assembly, while (C) corresponds to assembly of long-lived partial shells (the monomer starvation trap) that occurs under stronger subunit-subunit interactions. Images in (B) and (C) reproduced from (Zlotnick et al., 2000).