  Let $\Omega$ be a bounded open set in $\mathbb{R}^2$. The aim of this article
is to describe the functions $h$ in $H^1(\Omega)$ and the Radon measures $\mu$
which satisfy $-\Delta h+h=\mu$ and $ div(T_h)=0$ in $\Omega$, where $T_h$ is a
$2\times 2$ matrix given by $(T_h)_{ij}=2\partial_ih\partial_jh- (|\nabla
h|^2+h^2)\delta_{ij}$ for $i,j=1,2$. These equations arise as equilibrium
conditions satisfied by limiting vorticities and limiting induced magnetic
fields of solutions of the magnetic Ginzburg-Landau equations as shown by
Sandier-Serfaty. Let us recall that they obtained that $|\nabla h|$ is
continuous in $\Omega$. We prove that if $x_0$ in $ \Omega$ belongs to $\supp
\mu$ and is such that $|\nabla h(x_0)|\neq 0$ then $\mu$ is absolutely
continuous with respect to the 1D-Hausdorff measure restricted to a
$\mathcal{C}^1$-curve near $x_0$ whereas $\mu_{\lfloor \{| \nabla
h|=0\}}=h_{|\{ |\nabla h|=0\}}$. We also prove that if $\Omega$ is smooth
bounded and star-shaped and if $h=0$ on $\partial \Omega$ then $h \equiv 0$ in
$\Omega$. This rules out the possibility of having critical points of the
Ginzburg-Landau energy with a number of vortices much larger than the applied
magnetic field $h_{ex}$ in that case.
