Artigo Acesso aberto Revisado por pares

Existence of traveling wave solutions of parabolic–parabolic chemotaxis systems

2018; Elsevier BV; Volume: 42; Linguagem: Inglês

10.1016/j.nonrwa.2017.12.004

ISSN

1878-5719

Autores

Rachidi B. Salako, Wenxian Shen,

Tópico(s)

Evolution and Genetic Dynamics

Resumo

The current paper is devoted to the study of traveling wave solutions of the following parabolic–parabolicchemotaxis system, ut=Δu−χ∇⋅(u∇v)+u(a−bu),x∈RNτvt=Δv−v+u,x∈RN,where u(x,t) represents the population density of a mobile species and v(x,t) represents the population density of a chemoattractant, and χ represents the chemotaxis sensitivity. In an earlier work (Rachidi et al., 2017) by the authors of the current paper, traveling wave solutions of the above chemotaxis system with τ=0 are studied. It is shown in Rachidi et al. (2017) that for every 0<χ c∗(χ) and ξ∈SN−1, the system has a traveling wave solution (u(x,t),v(x,t))=(U(x⋅ξ−ct;τ),V(x⋅ξ−ct;τ)) with speed c connecting the constant solutions (ab,ab) and (0,0). Moreover, limχ→0+c∗(χ)=2aif0 1.We prove in the current paper that for every τ>0, there is0<χτ∗<b2 such that for every 0<χ c∗(χ,τ)≥2a satisfying that for every c∈(c∗(χ,τ),c∗∗(χ,τ)) and ξ∈SN−1, the system has a traveling wave solution (u(x,t),v(x,t))=(U(x⋅ξ−ct;τ),V(x⋅ξ−ct;τ)) with speed c connecting the constant solutions (ab,ab) and (0,0), and it does not have such traveling wave solutions of speed less than 2a. Moreover, limχ→0+c∗∗(χ,τ)=∞, limχ→0+c∗(χ,τ)=2aif0<a≤1+τa(1−τ)+1+τa(1−τ)++a(1−τ)+1+τaifa≥1+τa(1−τ)+, and limx→∞U(x;τ)e−μx=1,where μ is the only solution of the equation μ+aμ=c in the interval (0,min{a,1+τa(1−τ)+}). Furthermore, limτ→0+χτ∗=b2,limτ→0+c∗(χ;τ)=c∗(χ),limτ→0+c∗∗(χ;τ)=∞.

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