二维 Keller-Segel-(Navier-)Stokes 系统中通过间接信号产生机制防止炸裂

Jiashan Zheng, Xiuran Liu
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引用次数: 0

摘要

本文讨论了二维平滑有界域中系统 $$\begin{aligned} 的初始边界值问题。\n_t+\textbf{u}\cdot n=\Delta n-\nabla \cdot (n\mathcal {S}(n)\nabla v),\quad x\in \Omega , t>;0,\v_t+textbf{u}\cdot \nabla v=\Delta v-v+w,\quad xin\Omega , t>0,\w_t+textbf{u}\cdot \nabla w=\Delta w-w+n,\quad xin\Omega , t>;0,\textbf{u}_t+\kappa (\textbf{u}\cdot \nabla )\textbf{u}+\nabla P=Delta \textbf{u}+n\nabla \phi , (四边形 xin \Omega , t>;0,\nabla\cdot \textbf{u}=0,\quad xin\Omega , t>0,\end{array}\right.\(*) (end{aligned}$$描述了化学运动的微生物与其周围不可压缩流体之间的相互作用、其中 \(\kappa \in \mathbb {R}\), 重力势能 \(\phi \in W^{2,\infty }(\Omega )\), 和 \(\mathcal {S}(n)\) 满足 $$\begin{aligned}|\mathcal {S}(n)|\le C_\mathcal {S}(1+n)^{-\alpha }\text{ for }\all }~~ n\ge 0,~~C_\mathcal {S}>0~~text{ and }~~\alpha >-1.\end{aligned}$$Under the boundary conditions $$begin{aligned} (\nabla n-n\mathcal {S}(n)\nabla v)\cdot \nu =\partial _\nu v=\partial _\nu w=0, \textbf{u}=0,\quad x\in \partial \Omega , t>;0,end{aligned}$本文表明,初始数据上合适的正则性假设导致以下结果:(i) 如果 \(\alpha >-1\) 和 \(\kappa =0/),那么简化的趋化-斯托克斯系统具有唯一的全局经典解,该解是有界的。(ii) 如果 \(\α \ge 0\) and\(\kappa \in \mathbb {R}\),那么完整的化合-纳维尔-斯托克斯系统就有一个唯一的全局经典解。
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Blow-up prevention by indirect signal production mechanism in a two-dimensional Keller–Segel–(Navier–)Stokes system

This paper deals with an initial-boundary value problem in two-dimensional smoothly bounded domains for the system

$$\begin{aligned} \left\{ \begin{array}{l} n_t+\textbf{u}\cdot \nabla n=\Delta n-\nabla \cdot (n\mathcal {S}(n)\nabla v),\quad x\in \Omega , t>0,\\ v_t+\textbf{u}\cdot \nabla v=\Delta v-v+w,\quad x\in \Omega , t>0,\\ w_t+\textbf{u}\cdot \nabla w=\Delta w-w+n,\quad x\in \Omega , t>0,\\ \textbf{u}_t+\kappa (\textbf{u}\cdot \nabla )\textbf{u}+\nabla P=\Delta \textbf{u}+n\nabla \phi , \quad x\in \Omega , t>0,\\ \nabla \cdot \textbf{u}=0,\quad x\in \Omega , t>0,\\ \end{array}\right. \qquad \qquad (*) \end{aligned}$$

which describes the mutual interaction of chemotactically moving microorganisms and their surrounding incompressible fluid, where \(\kappa \in \mathbb {R}\), the gravitational potential \(\phi \in W^{2,\infty }(\Omega )\), and \(\mathcal {S}(n)\) satisfies

$$\begin{aligned} |\mathcal {S}(n)|\le C_\mathcal {S}(1+n)^{-\alpha } \quad \text{ for } \text{ all }~~ n\ge 0,~~C_\mathcal {S}>0~~\text{ and }~~\alpha >-1. \end{aligned}$$

Under the boundary conditions

$$\begin{aligned} (\nabla n-n\mathcal {S}(n)\nabla v)\cdot \nu =\partial _\nu v=\partial _\nu w=0, \textbf{u}=0, \quad x\in \partial \Omega , t>0, \end{aligned}$$

it is shown in this paper that suitable regularity assumptions on the initial data entail the following: (i) If \(\alpha >-1\) and \(\kappa =0\), then the simplified chemotaxis-Stokes system possesses a unique global classical solution which is bounded. (ii) If \(\alpha \ge 0\) and \(\kappa \in \mathbb {R}\), then the full chemotaxis-Navier–Stokes system admits a unique global classical solution.

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Fractional wave equation with irregular mass and dissipation On a quasilinear two-species chemotaxis system with general kinetic functions and interspecific competition Multiplicity and concentration behavior of solutions for magnetic Choquard equation with critical growth Eventual smoothness in a chemotaxis-Navier–Stokes system with indirect signal production involving Dirichlet signal boundary condition Boundedness and finite-time blow-up in a Keller–Segel chemotaxis-growth system with flux limitation
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