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. Author manuscript; available in PMC: 2014 Oct 7.
Published in final edited form as: J Theor Biol. 2013 Jul 2;334:149–161. doi: 10.1016/j.jtbi.2013.06.020

Figure 2.

Figure 2

Bifurcation analysis and eigenvalues in the actin-wave model for s1 = 0.7, s2 = 0.7, ε̃ = 0.1 and other parameters at default values. Left panels: Analysis of well mixed (a) and LPA (c) ODE’s plotting steady states of A and Al respectively versus the basal activation rate k0 (Solid = stable, dashed = unstable). The well-mixed model has a single stable steady state (a). The LPA system (c) has the same global branch, and additional local branches. ■, BP = branch points, ●, H = Hopf bifurcation. Right panels: A comparison of maximal (with largest real parts) LPA (b) and Turing (d) eigenvalues versus k0. (Solid = real, dashed = imaginary parts). Symbols ■, ●, mark the corresponding k0 values in (c). Hopf points correspond to zero real part and branch points to zero imaginary parts of λLPmax. The eigenvalues in (b) and (d) are similar and the Hopf and BP bifurcations closely relate to bifurcations of the RDE model.