We study the chemotaxis-fluid system \begin{align*} \left\{
\begin{array}{r@{\,}c@{\,}c@{\ }l@{\quad}l@{\quad}l@{\,}c}
n_{t}&+&u\cdot\!\nabla n&=\Delta n-\nabla\!\cdot(\frac{n}{c}\nabla c),\
&x\in\Omega,& t>0, c_{t}&+&u\cdot\!\nabla c&=\Delta c-nc,\ &x\in\Omega,& t>0,
u_{t}&+&\nabla P&=\Delta u+n\nabla\phi,\ &x\in\Omega,& t>0, &&\nabla\cdot
u&=0,\ &x\in\Omega,& t>0, \end{array}\right. \end{align*} under homogeneous
Neumann boundary conditions for n and c and homogeneous Dirichlet boundary
conditions for u, where Ω⊂R2 is a bounded domain with
smooth boundary and ϕ∈C2(Ωˉ). From recent
results it is known that for suitable regular initial data, the corresponding
initial-boundary value problem possesses a global generalized solution. We will
show that for small initial mass ∫Ωn0 these generalized
solutions will eventually become classical solutions of the system and obey
certain asymptotic properties.
Moreover, from the analysis of certain energy-type inequalities arising
during the investigation of the eventual regularity, we will also derive a
result on global existence of classical solutions under assumption of certain
smallness conditions on the size of n0 in L1(Ω) and in
LlogL(Ω), u0 in L4(Ω), and of
∇c0 in L2(Ω).Comment: 35 page