“…We show in appendix A that the average timescales of these phases for an individual capsid can be described by τ = τ nuc + τ elong , with and , where f is the subunit-subunit binding rate constant, C S is the concentration of free subunits, n nuc is the number of subunits in the nucleus. Because elongation requires N − n nuc assembly events, it introduces a minimum timescale for the overall assembly process, which is primarily responsible for the lag time in assembly kinetics reported in experiments [9,12,53], theory [21,48], and simulations [26,28,80], and results in a distribution of assembly times for an individual capsid that cannot be fit with a sum of pure exponential functions [81]. The observed assembly rate constant, f, can be considered an average quantity, since computational models [26,28] suggest that it varies for different intermediates and decreases due to excluded volume constraints as assembly nears completion.…”