Volume 105, Issue 5 e70064
ORIGINAL PAPER

Global boundedness of solutions for a quasilinear chemotaxis-Stokes system with nonlinear production

Wei Wang

Corresponding Author

Wei Wang

School of Mathematical Sciences, Dalian University of Technology, Dalian, P.R. China

Correspondence

Wei Wang, School of Mathematical Sciences, Dalian University of Technology, Dalian 116024, P.R. China.

Email: [email protected]

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First published: 22 April 2025

Abstract

In this paper we study the global boundedness of solutions to the quasilinear chemotaxis-Stokes system with nonlinear production

n t + u · n = · ( D ( n ) n n S ( n ) c ) , c t + u · c = Δ c c + n β , u t + P = Δ u + n ϕ , · u = 0 , $$\begin{equation} {\left\lbrace \begin{aligned} &n_t+u\cdot \nabla n=\nabla \cdot (D(n)\nabla n-nS(n)\nabla c),\\ &c_{t}+u\cdot \nabla c=\Delta c-c+n^{\beta },\\ &u_{t}+\nabla P=\Delta u+n\nabla \phi, \nobreakspace \nabla \cdot u=0, \end{aligned} \right.} \end{equation}$$ ( $\star$ )
subject to no-flux/no-flux/Dirichlet boundary conditions in a smoothly bounded domain Ω R N $\Omega \subset \mathbb {R}^N$ with N { 2 , 3 } $N\in \lbrace 2,3\rbrace$ , where β 0 $\beta \ge 0$ , ϕ W 2 , ( Ω ) $\phi \in W^{2,\infty }(\Omega)$ , and D , S C 2 ( [ 0 , ) ) $D,S\in C^2([0,\infty))$ generalize the prototypes D ( s ) = k D ( s + 1 ) m $D(s)=k_D(s+1)^{-m}$ and S ( s ) = K S ( s + 1 ) α $S(s)=K_S(s+1)^{-\alpha }$ for all s 0 $s\ge 0$ with k D , K S > 0 $k_D,K_S>0$ and m , α R $m,\alpha \in \mathbb {R}$ . It is shown that if α > m + β 2 N $\alpha >m+\beta -\frac{2}{N}$ for N = 2 $N=2$ , or α > m + ( β 2 N ) + $\alpha >m+(\beta -\frac{2}{N})_{+}$ for N = 3 $N=3$ , then for any reasonably regular initial datum, the corresponding initial-boundary value problem of ( $\star$ ) possesses a unique globally bounded classical solution. Compared to the global boundedness condition α > m + β 2 N $\alpha >m+\beta -\frac{2}{N}$ for N { 2 , 3 } $N\in \lbrace 2,3\rbrace$ in the relevant fluid-free system [J. Differ. Equ. 268 6729–6777 (2020)], the present result indicates that the slow fluid motion described by the Stokes equation might possibly be adverse to the global solvability in the case that β < 2 N $\beta <\frac{2}{N}$ with N = 3 $N=3$ . What is more, this paper provides for the quasilinear problems with general signal production a universal approach capable of deriving the boundedness of solutions in the optimal range of parameters.

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