The aim of this paper is to study the behaviour of a weak solution to Navier-Stokes
equations for isothermal fluids with a nonlinear stress tensor for time going to
infinity. In an analogous way as in [18], we construct a suitable function which
approximates the density for time going to infinity. Using properties of this
function, we can prove the strong convergence of the density to its limit state. The
behaviour of the velocity field and kinetic energy is mentioned as well.