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Suppressing blow-up by gradient-dependent flux limitation in a planar Keller–Segel–Navier–Stokes system
Zeitschrift für angewandte Mathematik und Physik ( IF 1.7 ) Pub Date : 2021-03-22 , DOI: 10.1007/s00033-021-01508-8
Michael Winkler

The flux-limited Keller–Segel–Navier–Stokes system

$$\begin{aligned} \left\{ \begin{array}{lcl} n_t + u\cdot \nabla n &{}=&{} \Delta n - \nabla \cdot \Big ( n f(|\nabla c|^2) \nabla c\Big ), \\ c_t + u\cdot \nabla c &{}=&{} \Delta c - c + n, \\ u_t + (u\cdot \nabla ) u &{}=&{} \Delta u + \nabla P + n\nabla \Phi , \qquad \nabla \cdot u=0, \end{array} \right. \qquad \qquad (\star ) \end{aligned}$$

is considered in a smoothly bounded domain \(\Omega \subset {\mathbb {R}}^2\). It is shown that whenever the suitably smooth function f models any asymptotically algebraic-type saturation of cross-diffusive fluxes in the sense that

$$\begin{aligned} |f(\xi )| \le K_f\cdot (\xi +1)^{-\frac{\alpha }{2}} \end{aligned}$$

holds for all \(\xi \ge 0\) with some \(K_f>0\) and \(\alpha >0\), for any all reasonably regular initial data a corresponding no-flux/no-flux/Dirichlet problem admits a globally defined classical solution which is bounded, inter alia, in \(L^\infty (\Omega \times (0,\infty ))\) with respect to all its components. By extending a corresponding result known for a fluid-free counterpart of (\(\star \)), this confirms that with regard to the possible emergence of blow-up phenomena, the choice \(f\equiv const.\) retains some criticality also in the presence of fluid interaction.



中文翻译:

在平面Keller–Segel–Navier–Stokes系统中通过梯度相关的通量限制来抑制爆炸

通量受限的Keller–Segel–Navier–Stokes系统

$$ \ begin {aligned} \ left \ {\ begin {array} {lcl} n_t + u \ cdot \ nabla n&{} =&{} \ Delta n-\ nabla \ cdot \ Big(nf(| \ nabla c | ^ 2)\ nabla c \ Big),\\ c_t + u \ cdot \ nabla c&{} =&{} \ Delta c-c + n,\\ u_t +(u \ cdot \ nabla)u& {} =&{} \ Delta u + \ nabla P + n \ nabla \ Phi,\ qquad \ nabla \ cdot u = 0,\ end {array} \ right。\ qquad \ qquad(\ star)\ end {aligned} $$

被认为是在有界的域\(\ Omega \ subset {\ mathbb {R}} ^ 2 \)中。结果表明,只要适当的光滑函数f建模交叉扩散通量的任何渐近代数型饱和度,就意味着

$$ \ begin {aligned} | f(\ xi)| \ le K_f \ cdot(\ xi +1)^ {-\ frac {\ alpha} {2}} \ end {aligned} $$

对于具有\(K_f> 0 \)\(\ alpha> 0 \)的所有\(\ xi \ ge 0 \)成立,对于所有合理的常规初始数据,对应的无通量/无通量/ Dirichlet问题接受全局定义的经典解决方案,该解决方案除其他因素外,以\(L ^ \ infty(\ Omega \ times(0,\ infty))\)为界。通过扩展已知的(\(\ star \))的无液对应物的对应结果,这证实了关于爆炸现象的可能出现,选择\(f \ equiv const。\)保留了一些。在流体相互作用的情况下也具有临界性。

更新日期:2021-03-23
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