Abstract
We study a free boundary problem for Fisher-KPP equation: \(u_t=u_{xx}+f(u)\) (\(g(t)< x < h(t)\)) with free boundary conditions \(h'(t)=-u_x(t,h(t))-\beta \) and \(g'(t)=-u_x(t,g(t))-\alpha \) for \(\alpha >0\) and \(\beta \in \mathbb {R}\). Such a free boundary problem can model the spreading of a biological or chemical species affected by the boundary environment. \(\beta >0\) means that there is a “resistance force” with strength \(\beta \) at boundary \(x=h(t)\). \(\beta <0\) (resp. \(\alpha >0\)) means that there is an enhancing force with strength \(\beta \) (resp. \(\alpha \)) at the boundary \(x=h(t)\) (resp. g(t)). There are many parts of \((\alpha ,\beta )\). In different parts, the asymptotic behavior of solutions are different. In the first part, we have a spreading-transition-vanishing result: either spreading happens (the solution converges to 1 in the moving frame), or in the transition case (the solution will converge to the compactly supported traveling wave), or vanishing happens (the solution converges to 0 within a finite time). In the second part, we also have a trichotomy result, but in transition case the solution will converge to the non-monotonous traveling semi-wave, and the vanishing case has three different types. For the third part, only spreading happens for any solution. In the fourth part (\(\alpha \) or \(\beta \) large), any solution will vanish, also there are three types of vanishing. For the case \(\alpha = \beta \), we have two different trichotomy results and a dichotomy result.
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This research was sponsored by NSFC (Nos. 11601225, 11701359) and Natural Science Foundation of Jiangsu (No. BK20161022).
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Cai, J., Gu, H. Asymptotic Behavior of Solutions of Free Boundary Problems for Fisher-KPP Equation. J Dyn Diff Equat 33, 913–940 (2021). https://doi.org/10.1007/s10884-020-09840-9
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DOI: https://doi.org/10.1007/s10884-020-09840-9
Keywords
- Fisher-KPP equation
- Free boundary problem
- Compactly supported traveling wave
- Non-monotonous traveling semi-wave