A Sharp Global Boundedness Result for Keller--Segel--(Navier--)Stokes Systems with Rapid Diffusion and Saturated Sensitivities

TL;DR

This paper proves that under certain conditions on diffusion and sensitivity functions, the Keller--Segel--(Navier--)Stokes systems in 2D and 3D have global bounded solutions, extending understanding of chemotaxis-fluid interactions.

Contribution

It establishes optimal boundedness results for Keller--Segel--(Navier--)Stokes systems with rapid diffusion and saturated sensitivities in 2D and 3D, improving previous blow-up criteria.

Findings

Global bounded solutions in 2D with vanishing sensitivity at infinity.

Global bounded solutions in 3D with decay rate of sensitivity exceeding 1/3.

Results are optimal given known blow-up scenarios.

Abstract

We investigate the Keller--Segel--(Navier--)Stokes system posed in a smooth bounded domain \(\Omega \subset \mathbb{R}^N\) with \(N = 2,3\): \begin{equation*} \begin{cases} n_t + u \cdot \nabla n = \Delta n - \nabla \cdot \big( n S(n)\nabla c \big), \\[2mm] u \cdot \nabla c = \Delta c - c + n, \\[2mm] u_t + \kappa (u \cdot \nabla) u = \Delta u - \nabla P + n \nabla \phi, \\[2mm] \nabla \cdot u = 0, \end{cases} \end{equation*} where \(\kappa \in \left \{0,1 \right \} \), the given gravitational potential \(\phi \in W^{2, \infty}(\Omega)\), and the chemotactic sensitivity function \(S \in C^2([0,\infty))\). Under no-flux boundary conditions for \(n\) and \(c\), together with the Dirichlet boundary condition for \(u\), we show that, provided the initial data satisfy suitable regularity assumptions, the following results hold: \begin{itemize} \item If \(N = 2\), \(\kappa = 1\), and the sensitivity function satisfies \(\lim_{\xi \to \infty} S(\xi) = 0\), then the Keller--Segel--Navier--Stokes system admits a global classical solution that remains uniformly bounded in time. \item If \(N = 3\), \(\kappa = 0\), and \(S\) satisfies \[ |S(\xi)| \le K_S (\xi + 1)^{-\alpha} \quad \text{for all } \xi \ge 0, \] with some constants \(K_S > 0\) and \(\alpha > \frac{1}{3}\), then the Keller--Segel--Stokes system possesses a global bounded classical solution. \end{itemize} Our results are optimal, since it is well established that, in the absence of fluid effects, blow-up can occur when $S \equiv \mathrm{const}$ in two dimensions, or when $\alpha < \tfrac{1}{3}$ in three dimensions.