Critical points of the N-vortex Hamiltonian in bounded planar domains and steady state solutions of the incompressible Euler equations

Abstract

We prove the existence of critical points of the $N$-vortex Hamiltonian $H_{\Omega }(x_1,\dots ,x_N)=\sum _{i=1}^N{\Gamma }_i^{2}h(x_i)+\sum _{\genfrac{}{}{0ex}{}{i,j=1}{j\ne k}}^N{\Gamma }_i{\Gamma }_{j}G(x_i,x_j)+2\sum _{i=1}^N{\Gamma }_i{\psi }_0(x_i)$ in a bounded domain $\Omega \subset {\mathbb{R}}^2$ which may be simply or multiply connected. Here $G$ denotes the Green function for the Dirichlet Laplace operator in $\Omega$, more generally a hydrodynamic Green function, and $h$ the Robin function. Moreover ${\psi }_0\in C^1(\overline{\Omega })$ is a harmonic function on $\Omega$. We obtain new critical points $x=(x_1,\dots ,x_N)$ for $N=3$ or $N=4$ under conditions on the vorticities ${\Gamma }_i\in \mathbb{R}\setminus \{0\}$. These critical points correspond to point vortex equilibria of the Euler equation in vorticity form. The case ${\Gamma }_i=(-1{)}^i$ of counter-rotating vortices with identical vortex strength is included. The point vortex equilibria can be desingularized to obtain smooth steady state solutions of the Euler equations for an ideal fluid. The velocity of these steady states will be irrotational except for $N$ vorticFity blobs near $x_1,\dots ,x_N$.

References in corpus (1)

• Regularization of point vortices for the Euler equation in dimension two, part II