Abstract
The coupled chemotaxis fluid system \begin{equation} \left\{ \begin{array}{llc} n_t=Δn-\nabla\cdot(n S(x,n,c)\cdot\nabla c)-u\cdot\nabla n, &(x,t)\in Ω\times (0,T), \displaystyle c_t=Δc-nc-u\cdot\nabla c, &(x,t)\inΩ\times (0,T), \displaystyle u_t=Δu-(u\cdot\nabla )u+\nabla P+n\nablaΦ,\quad \nabla\cdot u=0, &(x,t)\inΩ\times (0,T), \displaystyle \nabla c\cdotν=(\nabla n-nS(x,n,c)\cdot\nabla c)\cdotν=0, \;\; u=0,&(x,t)\in \partialΩ\times (0,T), n(x,0)=n_{0}(x),\quad c(x,0)=c_{0}(x),\quad u(x,0)=u_0(x) & x\inΩ, \end{array} \right. \end{equation} where , is considered in a bounded domain , , with smooth boundary. We show that it has global classical solutions if the initial data satisfy certain smallness conditions and give decay properties of these solutions.
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