Energy Conservation for the Generalized Surface Quasi-geostrophic Equation

IF 1.3 3区 数学 Q2 MATHEMATICS, APPLIED Journal of Mathematical Fluid Mechanics Pub Date : 2023-07-24 DOI:10.1007/s00021-023-00815-6
Yanqing Wang, Yulin Ye, Huan Yu
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Abstract

In this paper, we consider the generalized surface quasi-geostrophic equation with the velocity v determined by \(v=\mathcal {R}^{\perp }\Lambda ^{\gamma -1}\theta ,\) \(0<\gamma < 2\). It is shown that the \(L^p\)-norm of weak solutions is conserved provided \(\theta \in L^{p+1}\left( 0,T; {B}^{\frac{\gamma }{3}}_{p+1, c(\mathbb {N})}\right) \) for \(0<\gamma <\frac{3}{2}\) or \(\theta \in L^{p+1}\left( 0,T; {{B}}^{\alpha }_{p+1,\infty }\right) ~\text {for any}~\gamma -1<\alpha<1 \text { with} ~\frac{3}{2}\le \gamma <2\). Therefore, the accurate relationships between the critical regularity for the energy conservation of the weak solutions and the regularity of velocity for the generalized surface quasi-geostrophic equation are presented.

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广义地表准地转方程的能量守恒
本文考虑速度v由\(v=\mathcal {R}^{\perp }\Lambda ^{\gamma -1}\theta ,\)\(0<\gamma < 2\)决定的广义曲面准地转方程。证明弱解的\(L^p\) -范数在\(0<\gamma <\frac{3}{2}\)或\(\theta \in L^{p+1}\left( 0,T; {{B}}^{\alpha }_{p+1,\infty }\right) ~\text {for any}~\gamma -1<\alpha<1 \text { with} ~\frac{3}{2}\le \gamma <2\)为\(\theta \in L^{p+1}\left( 0,T; {B}^{\frac{\gamma }{3}}_{p+1, c(\mathbb {N})}\right) \)时是守恒的。因此,给出了广义曲面准地转方程弱解能量守恒的临界正则性与速度正则性之间的精确关系。
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来源期刊
CiteScore
2.00
自引率
15.40%
发文量
97
审稿时长
>12 weeks
期刊介绍: The Journal of Mathematical Fluid Mechanics (JMFM)is a forum for the publication of high-quality peer-reviewed papers on the mathematical theory of fluid mechanics, with special regards to the Navier-Stokes equations. As an important part of that, the journal encourages papers dealing with mathematical aspects of computational theory, as well as with applications in science and engineering. The journal also publishes in related areas of mathematics that have a direct bearing on the mathematical theory of fluid mechanics. All papers will be characterized by originality and mathematical rigor. For a paper to be accepted, it is not enough that it contains original results. In fact, results should be highly relevant to the mathematical theory of fluid mechanics, and meet a wide readership.
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