On stationary motions of Prandtl-Eyring fluids in 2D

We prove the existence of weak solutions to steady Navier Stokes equations

$$\text{div}\, \sigma+f=\nabla\pi+(\nabla u)u.$$

Here $u:\mathbb{R}^2\supset \Omega\rightarrow \mathbb{R}^2$ denotes

the velocity field satisfying $\text{div}\, u=0$,

$f:\Omega\rightarrow\mathbb{R}^2$ and

$\pi:\Omega\rightarrow\mathbb{R}$ are external volume force and

pressure, respectively. In order to model the behavior of

Prandtl-Eyring fluids we assume

$$\sigma= DW(\varepsilon (u)),\quad W(\varepsilon)=|\varepsilon|\log

(1+|\varepsilon|).$$

A crucial tool in our approach is a modified Lipschitz truncation

preserving the divergence of a given function.