This paper deals with the following chemotaxis–Stokes system $$\begin{aligned} \left\{ \begin{array}{ll} n_t+u\cdot \nabla n=\Delta n^m-\nabla \cdot (nS(x,n,c)\cdot \nabla c), &{}\quad x\in \Omega ,\,\, t>0,\\ c_t+u\cdot \nabla c=\Delta c-nf(c),&{}\quad x\in \Omega , \,\,t>0,\\ u_t=\Delta u+\nabla P+n\nabla \phi ,&{}\quad x\in \Omega , \,\,t>0,\\ \nabla \cdot u=0,&{}\quad x\in \Omega , \,\,t>0\\ \end{array} \right. \end{aligned}$$ under no-flux boundary conditions in a bounded domain \(\Omega \subset \mathbb {R}^{3}\) with smooth boundary, where \(m\ge 1\), \(\phi \in W^{1,\infty }(\Omega )\), f and S are given functions with values in \([0,\,\infty )\) and \(\mathbb {R}^{3\times 3}\), respectively. Here S satisfies \(|S(x,n,c)| \frac{7}{6}\), which insures the global existence of bounded weak solution. Our result covers completely and improves the recent result by Wang and Cao (Discrete Contin Dyn Syst Ser B 20:3235–3254, 2015) which asserts, just in the case \(m=1\), the global existence of solutions, but without boundedness, and that by Winkler (Calc Var Partial Differ Equ 54:3789–3828, 2015) which only involves the case of \(\alpha =0\) and requires the convexity of the domain.
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