Abstract
This paper deals with an attraction–repulsion chemotaxis system {ut=∇⋅(D(u)∇u)−χ∇⋅(u∇v)+ξ∇⋅(u∇w),x∈Ω,t>0,τ1vt=Δv+αu−βv,x∈Ω,t>0,τ2wt=Δw+γu−δw,x∈Ω,t>0 under homogeneous Neumann boundary conditions in a smooth bounded domain Ω⊂RN (N≥2), where parameters τi(i=1,2), χ ξ α β γ and δ are positive, and diffusion coefficient D(u)∈C2(0,+∞) satisfies D(u)>0 for u≥0, D(u)≥dum−1 with d>0 and m≥1 for all u>0. It is proved that the corresponding initial–boundary value problem possesses a unique global bounded classical solution for m>2−[Formula presented]. In particular in the case τ1=τ2 and χα=ξγ the solution is globally bounded if m>2−[Formula presented]−[Formula presented]. Therefore, due to the inhibition of repulsion to the attraction, the range of m>2−[Formula presented] of boundedness is enlarged and the results of [21] is thus extended to the higher dimensional attraction–repulsion chemotaxis system with nonlinear diffusion.
| Original language | English |
|---|---|
| Pages (from-to) | 1066-1079 |
| Number of pages | 14 |
| Journal | Journal of Mathematical Analysis and Applications |
| Volume | 467 |
| Issue number | 2 |
| DOIs | |
| Publication status | Published - 15 Nov 2018 |
Keywords
- Attraction–repulsion
- Boundedness
- Chemotaxis
- Fully parabolic
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