Experimental data of Beltzner and Pollard (10) are fitted well assuming different limiting steps. Experimental results (symbols) and numerical solutions of Eq. 1 (curves) are shown for the following Arp2/3 concentrations (Table 2A): A0 = 100 nM (squares); 50 nM (circles); 20 nM (diamonds); 10 nM (triangles). (a) Simulations of nucleation kinetics limited by step 2: kbind = 4.5 × 10−4μM−1s−1, kon = 0.25 μM−1s−1, koff = kact = 1 s−1; E0 is a decreasing function of A0: E0 = 12, 18, 40, and 48 pM for A0=100, 50, 20, and 10 nM, respectively; (b) simulations of nucleation kinetics limited by step 3, kact = 1.45 × 10−4μM−1s−1, kon = kbind = 0.25 μM−1s−1, koff = 1 s−1, and E0 = 5.6, 6, 28, and 40 pM for A0 = 100, 50, 20, and 10 nM, respectively. In all simulations, kp = 10 μM−1s−1. Insets: Log-scale plots of Jcomplex_on, Jbinding, and Jactivation illustrate the presence of a rate-limiting step in the simulated kinetics.