Abstract

Abstract This paper is concerned with a chemotaxis system u t = Δ u m − ∇ ⋅ ( χ 1 ( w ) u ∇ w ) + μ 1 u ( 1 − u − a 1 v ) , x ∈ Ω , t > 0 , v t = Δ v n − ∇ ⋅ ( χ 2 ( w ) v ∇ w ) + μ 2 v ( 1 − a 2 u − v ) , x ∈ Ω , t > 0 , w t = Δ w − ( α u + β v ) w , x ∈ Ω , t > 0 , \left\{\begin{array}{ll}{u}_{t}=\Delta {u}^{m}-\nabla \cdot \left({\chi }_{1}\left(w)u\nabla w)+{\mu }_{1}u\left(1-u-{a}_{1}v),& x\in \Omega ,\hspace{0.33em}t\gt 0,\\ {v}_{t}=\Delta {v}^{n}-\nabla \cdot \left({\chi }_{2}\left(w)v\nabla w)+{\mu }_{2}v\left(1-{a}_{2}u-v),& x\in \Omega ,\hspace{0.33em}t\gt 0,\\ {w}_{t}=\Delta w-\left(\alpha u+\beta v)w,& x\in \Omega ,\hspace{0.33em}t\gt 0,\end{array}\right. under homogeneous Neumann boundary conditions in a bounded domain Ω ⊂ R 3 \Omega \subset {{\mathbb{R}}}^{3} with smooth boundary, where μ 1 , μ 2 > 0 {\mu }_{1},{\mu }_{2}\gt 0 , a 1 , a 2 > 0 {a}_{1},{a}_{2}\gt 0 , α , β > 0 \alpha ,\beta \gt 0 , and the chemotactic sensitivity function χ i ∈ C 1 ( [ 0 , ∞ ) ) {\chi }_{i}\in {C}^{1}({[}0,\infty )) , χ i ′ ≥ 0 {\chi }_{i}^{^{\prime} }\ge 0 . It is proved that for any large initial data, for any m , n > 1 m,n\gt 1 , the system admits a global weak solution, which is uniformly bounded.

Highlights

  • Chemotaxis refers to the effect of chemical substances in the environment on the movement of species

  • This can lead to strict directional movement or partial orientation and partial tumbling movement

  • Chemotaxis is an important means of cellular communication

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Summary

Introduction

Chemotaxis refers to the effect of chemical substances in the environment on the movement of species. When D(u) ≡ 1, in the three-dimensional case, Zheng et al proved that the system (2) with a logistic type source μu(1 − u) admits a unique global classical solution if the initial data of w are small in [5]. If N ≤ 2, if N ≥ 3, where λ0 is a positive constant which is corresponding to the maximal Sobolev regularity, for any sufficiently smooth initial data there exists a classical solution which is global in time and bounded. Global existence and boundedness 951 if χi (w) = χi are positive constants They considered asymptotic behavior of solutions to the system: when a1, a2 ∈ (0, 1), u(⋅, t) → 1 − a1 , v(⋅, t) → 1 − a2 , w → α(1 − a1) + β(1 − α2) in L∞(Ω) as t → ∞;.

Some preliminaries
Global existence and boundedness of weak solution
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