English

Multiple Vortices for the Shallow Water Equation

Analysis of PDEs 2013-01-29 v1

Abstract

In this paper, we construct stationary classical solutions of the shallow water equation with vanishing Froude number FrFr in the so-called lake model. To this end we need to study solutions to the following semilinear elliptic problem {cases} -\varepsilon^2\text{div}(\frac{\nabla u}{b})=b(u-q\log\frac{1}{\varepsilon})_+^{p},& \text{in}\; \Omega, u=0, &\text{on}\;\partial \Omega, {cases} for small ε>0\varepsilon>0, where p>1p>1, div(qb)=0\text{div}(\frac{\nabla q}{b})=0 and ΩR2\Omega\subset\mathbb{R}^2 is a smooth bounded domain,. We showed that if q2b\frac{q^2}{b} has mm strictly local minimum(maximum) points zˉi,i=1,...,m\bar z_i,\,i=1,...,m, then there is a stationary classical solution approximating stationary mm points vortex solution of shallow water equations with vorticity i=1m2πq(zˉi)b(zˉi)\sum_{i=1}^m\frac{2\pi q(\bar z_i)}{b(\bar z_i)}. Moreover, strictly local minimum points of q2b\frac{q^2}{b} on the boundary can also give vortex solutions for the shallow water equation. As a further study we construct vortex pair solutions as well. Existence and asymptotic behavior of single point non-vanishing vortex solutions were studied by S. De Valeriola and J. Van Schaftingen.

Keywords

Cite

@article{arxiv.1301.6420,
  title  = {Multiple Vortices for the Shallow Water Equation},
  author = {Daomin Cao and Zhongyuan Liu},
  journal= {arXiv preprint arXiv:1301.6420},
  year   = {2013}
}

Comments

27 pages. arXiv admin note: text overlap with arXiv:1208.3002

R2 v1 2026-06-21T23:16:06.917Z