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A three-dimensional Keller-Segel-Navier–Stokes system involving subquadratic logistic degradation: global generalized solutions and eventual smoothness

  • Yu Tian,
  • Zhaoyin Xiang

摘要

In this paper, we consider a Keller-Segel-Navier–Stokes system involving subquadratic logistic degradation: \(\begin{aligned} \left\{ \begin{array}{ccl} n_t + {\textbf{u}}\cdot \nabla n & =& \Delta n-\nabla \cdot (n\nabla c)+\rho n- \mu n^{\alpha }, \\ \, c_t + {\textbf{u}}\cdot \nabla c & =& \Delta c -c+n, \\ {\textbf{u}}_t+ ({\textbf{u}}\cdot \nabla ) {\textbf{u}}& =& \Delta {\textbf{u}}+ \nabla P + n\nabla \phi , \\ \nabla \cdot {\textbf{u}}& = & 0 \end{array} \right. \end{aligned}\) n t + u · n = Δ n - · ( n c ) + ρ n - μ n α , c t + u · c = Δ c - c + n , u t + ( u · ) u = Δ u + P + n ϕ , · u = 0 in a three-dimensional smoothly bounded domain along with reasonably mild initial conditions and no-flux/no-flux/Dirichlet boundary conditions, where \(\rho \in {\mathbb {R}}\) ρ R and \(\mu >0\) μ > 0 . The purpose of the present work is to firstly establish the generalized solvability for the model under the subquadratic exponent restriction \(\alpha \ge \frac{4}{3}\) α 4 3 , which indicates that persistent Dirac-type singularities can be ruled out, and to secondly exhibit the eventual smoothness of these solutions under the stronger restriction \(\alpha > \frac{5}{3}\) α > 5 3 whenever \(\rho \) ρ is not too large in the sense of \(\begin{aligned} \big (\rho _++1\big )^{\alpha -1}{\rho _+}\le \delta _0\mu ^{\alpha },\qquad \big (\rho _++1\big )^{\min \{1,\,\alpha -1\}}{\rho _+}^{\max \{1,\,3-\alpha \}}\le \delta _0\mu ^{2},\qquad \rho _+\le \delta _0\mu \end{aligned}\) ( ρ + + 1 ) α - 1 ρ + δ 0 μ α , ( ρ + + 1 ) min { 1 , α - 1 } ρ + max { 1 , 3 - α } δ 0 μ 2 , ρ + δ 0 μ for some \(\delta _0=\delta _0(\alpha )>0\) δ 0 = δ 0 ( α ) > 0 . These results especially extend the precedent works due to Winkler (J Functional Anal 276: 1339-1401, 2019; Comm Math Phys 367: 439–489, 2022), where, among other things, the corresponding studies focus on the case \(\alpha =2\) α = 2 of quadratic degradation.