Global classical small-data solutions for a three-dimensional Keller--Segel--Navier--Stokes system modeling coral fertilization

preprint2019arXivOpen access

Abstract

We are concerned with the Keller--Segel--Navier--Stokes system \begin{equation*} \left\{ \begin{array}{ll} ρ_t+u\cdot\nablaρ=Δρ-\nabla\cdot(ρ\mathcal{S}(x,ρ,c)\nabla c)-ρm, &\!\! (x,t)\in Ω\times (0,T), \\ m_t+u\cdot\nabla m=Δm-ρm, &\!\! (x,t)\in Ω\times (0,T), \\ c_t+u\cdot\nabla c=Δc-c+m, & \!\! (x,t)\in Ω\times (0,T), \\ u_t+ (u\cdot \nabla) u=Δu-\nabla P+(ρ+m)\nablaϕ,\quad \nabla\cdot u=0, &\!\! (x,t)\in Ω\times (0,T) \end{array}\right. \end{equation*} subject to the boundary condition (∇ρ−ρS(x,ρ,c)∇c)⋅ν ⁣ ⁣= ⁣∇m⋅ν=∇c⋅ν=0,u=0(\nablaρ-ρ\mathcal{S}(x,ρ,c)\nabla c)\cdot ν\!\!=\!\nabla m\cdot ν=\nabla c\cdot ν=0, u=0 in a bounded smooth domain Ω⊂R3Ω\subset\mathbb R^3. It is shown that the corresponding problem admits a globally classical solution with exponential decay properties under the hypothesis that S∈C2(Ω‾×[0,∞)2)3×3\mathcal{S}\in C^2(\overlineΩ\times [0,\infty)^2)^{3\times 3} satisfies ∣S(x,ρ,c)∣≤CS|\mathcal{S}(x,ρ,c)|\leq C_S for some CS>0C_S>0, and the initial data satisfy certain smallness conditions.

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