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. 2019 Sep 4;475(2229):20190378. doi: 10.1098/rspa.2019.0378

Figure 2.

Figure 2.

Numerical solutions of the Fisher–KPP and the Fisher–Stefan models. (a) Numerical solutions of the Fisher–KPP equation evolving into a travelling wave solution with the minimum wave speed, c = 2. (b) Numerical solutions of the Fisher–Stefan model evolving into a travelling wave solution with c = 1.2. (c) Numerical solutions of the Fisher–Stefan model leading to extinction. (d) Magnified region of the solution in (c), for 0≤x≤2, to clearly show the dynamics of the extinction behaviour. For the Fisher–Stefan model, we set κ = 20 in (b) and κ = 0.45 in (c). Numerical solutions of the Fisher–Stefan model are obtained with Δξ = 1 × 10−4, whereas numerical solutions of the Fisher–KPP model are obtained with Δx = 1 × 10−4. For both, the Fisher–KPP and Fisher–Stefan models, we set Δt = 1 × 10−3 and ϵ = 1 × 10−8. For all results presented here, the initial condition is equation (2.4) with α = 0.5 and β = 1.