Dynamic Behavior of a Multi-Layer Quasi-Geostrophic Model: Weak and Time-Periodic Solutions
Zineb Hassainia, Haroune Houamed
TL;DR
The paper analyzes the QS2L two-layer quasi-geostrophic model, proving global weak (Yudovich) existence and uniqueness via flow-map stability despite lacking a velocity formulation. It introduces a contour-dynamics framework to construct time-periodic, $m$-fold V-states bifurcating from two rotating discs, using Crandall–Rabinowitz bifurcation in a setting where Euler and shallow-water kernels interact. A detailed kernel analysis based on Bessel functions and nonlocal operators underpins the existence, regularity, and spectral results; the bifurcation diagrams exhibit a two-dimensional pattern reflecting the multi-layer coupling. The study highlights parameter regimes where Crandall–Rabinowitz applies and identifies scenarios with spectral collisions, offering insights into the extension of V-state theory to multi-layer geophysical fluids and linking to both Euler and shallow-water dynamics.
Abstract
The quasi-geostrophic two-layer (QS2L) system models the dynamic evolution of two interconnected potential vorticities, each is governed by an active scalar equation. These vorticities are linked through a distinctive combination of their respective stream functions, which can be loosely characterized as a parameterized blend of both Euler and shallow-water stream functions. In this article, we study (QS2L) in two directions: First, we prove the existence and uniqueness of global weak solutions in the class of Yudovich, that is when the initial vorticities are only bounded and Lebesgue-integrable. The uniqueness is obtained as a consequence of a stability analysis of the flow-maps associated with the two vorticities. This approach replaces the relative energy method and allows us to surmount the absence of a velocity formulation for (QS2L). Second, we show how to construct $m$-fold time-periodic solutions bifurcating from two arbitrary distinct initial discs rotating with the same angular velocity. This is achieved provided that the number of symmetry $m$ is large enough, or for any symmetry $m\in \mathbb{N}^*$ as long as one of the initial radii of the discs does not belong to some set that contains, at most, a finite number of elements. Due to its multi-layer structure, it is essential to emphasize that the bifurcation diagram exhibits a two-dimensional pattern. Upon analysis, it reveals some similarities with the scheme accomplished for the doubly connected V-states of the Euler and shallow-water equations. However, the coupling between the equations gives rise to several difficulties in various stages of the proof when applying Crandall-Rabinowitz's Theorem. To address this challenge, we conduct a careful analysis of the coupling between the kernels associated with the Euler and shallow-water equations.
