Stability and exponential decay for the 2D anisotropic Boussinesq equations with horizontal dissipation

• Published in: arXiv.org 2021-05
• Main Authors: Dong, Boqing, Wu, Jiahong, Xu, Xiaojing, Zhu, Ning
• Format: Article
• Language: English
• Subjects: Astrophysics; Boussinesq equations; Computational fluid dynamics; Domains; Dynamic stability; Perturbation; Sobolev space; Thermal diffusion; Weather
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.2009.13445

The hydrostatic equilibrium is a prominent topic in fluid dynamics and astrophysics. Understanding the stability of perturbations near the hydrostatic equilibrium of the Boussinesq systems helps gain insight into certain weather phenomena. The 2D Boussinesq system focused here is anisotropic and involves only horizontal dissipation and horizontal thermal diffusion. Due to the lack of the vertical dissipation, the stability and precise large-time behavior problem is difficult. When the spatial domain is \(\mathbb R^2\), the stability problem in a Sobolev setting remains open. When the spatial domain is \(\mathbb T\times \mathbb R\), this paper solves the stability problem and specifies the precise large-time behavior of the perturbation. By decomposing the velocity \(u\) and temperature \(\theta\) into the horizontal average \((\bar u, \bar\theta)\) and the corresponding oscillation \((\widetilde u, \widetilde \theta)\), and deriving various anisotropic inequalities, we are able to establish the global stability in the Sobolev space \(H^2\). In addition, we prove that the oscillation \((\widetilde u, \widetilde \theta)\) decays exponentially to zero in \(H^1\) and \((u, \theta)\) converges to \((\bar u, \bar\theta)\). This result reflects the stratification phenomenon of buoyancy-driven fluids.