A Sharp Global Boundedness Result for Keller--Segel--(Navier--)Stokes Systems with Rapid Diffusion and Saturated Sensitivities
Abstract
We investigate the Keller--Segel--(Navier--)Stokes system posed in a smooth bounded domain \( ⊂ RN\) with \(N = 2,3\): equation* cases nt + u · ∇ n = n - ∇ · ( n S(n)∇ c ), \\[2mm] u · ∇ c = c - c + n, \\[2mm] ut + (u · ∇) u = u - ∇ P + n ∇ φ, \\[2mm] ∇ · u = 0, cases equation* where \( ∈ \0,1 \ \), the given gravitational potential \(φ ∈ W2, ∞()\), and the chemotactic sensitivity function \(S ∈ C2([0,∞))\). 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: itemize If \(N = 2\), \( = 1\), and the sensitivity function satisfies \( ∞ S() = 0\), then the Keller--Segel--Navier--Stokes system admits a global classical solution that remains uniformly bounded in time. If \(N = 3\), \( = 0\), and \(S\) satisfies \[ |S()| KS ( + 1)-α for all 0, \] with some constants \(KS > 0\) and \(α > 13\), then the Keller--Segel--Stokes system possesses a global bounded classical solution. itemize Our results are optimal, since it is well established that, in the absence of fluid effects, blow-up can occur when S const in two dimensions, or when α < 13 in three dimensions.
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