Upper bounds on the dimension of the global attractor of the 2D Navier-Stokes equations on the $β-$plane

Aseel Farhat, Anuj Kumar, Vincent R. Martinez
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Abstract

This article establishes estimates on the dimension of the global attractor of the two-dimensional rotating Navier-Stokes equation for viscous, incompressible fluids on the $\beta$-plane. Previous results in this setting by M.A.H. Al-Jaboori and D. Wirosoetisno (2011) had proved that the global attractor collapses to a single point that depends only the longitudinal coordinate, i.e., zonal flow, when the rotation is sufficiently fast. However, an explicit quantification of the complexity of the global attractor in terms of $\beta$ had remained open. In this paper, such estimates are established which are valid across a wide regime of rotation rates and are consistent with the dynamically degenerate regime previously identified. Additionally, a decomposition of solutions is established detailing the asymptotic behavior of the solutions in the limit of large rotation.
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$β-$平面上二维纳维-斯托克斯方程全局吸引子维度的上界
本文建立了对$\beta$平面上粘性不可压缩流体的二维旋转纳维-斯托克斯方程全局吸引子维度的估计。此前,M.A.H. Al-Jaboori 和 D. Wirosoetisno(2011 年)在此背景下的结果证明,当旋转速度足够快时,全局吸引子会坍缩为一个仅取决于纵坐标的单点,即纵向流。然而,用 $\beta$ 来明确量化全局吸引子的复杂性仍然是个未知数。本文建立的这种估计值在很宽的旋转速率范围内都是有效的,并且与之前确定的动力学退化机制是一致的。此外,本文还建立了解的分解,详细说明了大旋转极限下解的渐近行为。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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