This paper deals with a two‐competition‐species chemotaxis‐Navier‐Stokes system with two different consumed signals
false(n1false)t+boldu·∇n1=d1normalΔn1−χ1∇·false(n1∇cfalse)+μ1n1false(1−n1−a1n2false),in3.0235ptnormalΩ×false(0,∞false),ct+boldu·∇c=d2normalΔc−α1cn2,in3.0235ptnormalΩ×false(0,∞false),false(n2false)t+boldu·∇n2=d3normalΔn2−χ2∇·false(n2∇vfalse)+μ2n2false(1−a2n1−n2false),in3.0235ptnormalΩ×false(0,∞false),vt+boldu·∇v=d4normalΔv−α2vn1,in3.0235ptnormalΩ×false(0,∞false),boldut+false(boldu·∇false)boldu=normalΔboldu+∇P+false(β1n1+β2n2false)∇ϕ,in3.0235ptnormalΩ×false(0,∞false),∇·boldu=0,in3.0235ptnormalΩ×false(0,∞false),
in a smooth bounded domain
normalΩ⊂double-struckR3 under zero Neumann boundary conditions for
n1,n2,c,v, and homogeneous Dirichlet boundary condition for
boldu, where the parameters
di (
i=1,2,3,4) and
χj,μj,aj,αj,βj (
j=1,2) are positive. This system describes the evolution of two‐competing species which react on two different chemical signals in a liquid surrounding environment. Recently, the boundedness and stabilization of classical solutions to the above system under two‐dimensional case have been derived in the previous works. However, to the best of our knowledge, the well‐posedness problem of solutions for the above system is still open in the three dimensional setting, because of the difficulties in the Navier‐Stokes system. The aim of this paper is to construct global weak solutions and show that after some waiting time, these weak solutions become eventually smooth.