Justification of the Benjamin–Ono equation as an internal water waves model

IF 2.4 1区 数学 Q1 MATHEMATICS
Martin Oen Paulsen
{"title":"Justification of the Benjamin–Ono equation as an internal water waves model","authors":"Martin Oen Paulsen","doi":"10.1007/s40818-024-00190-z","DOIUrl":null,"url":null,"abstract":"<div><p>In this paper, we give the first rigorous justification of the Benjamin-Ono equation: </p><div><div><span>$$\\begin{aligned} \\hspace{3cm} \\partial _t \\zeta + (1 - \\frac{\\gamma }{2}\\sqrt{\\mu }|\\textrm{D}|)\\partial _x \\zeta + \\frac{3{\\varepsilon }}{2}\\zeta \\partial _x\\zeta =0, \\hspace{2cm} \\text {(BO)} \\end{aligned}$$</span></div></div><p>as an internal water wave model on the physical time scale. Here, <span>\\({\\varepsilon }\\)</span> is a small parameter measuring the weak nonlinearity of the waves, <span>\\(\\mu \\)</span> is the shallowness parameter, and <span>\\(\\gamma \\in (0,1)\\)</span> is the ratio between the densities of the two fluids. To be precise, we first prove the existence of a solution to the internal water wave equations for a two-layer fluid with surface tension, where one layer is of shallow depth and the other is of infinite depth. The existence time is of order <span>\\({\\mathcal {O}}(\\frac{1}{{\\varepsilon }})\\)</span> for a small amount of surface tension such that <span>\\({\\varepsilon }^2 \\le \\textrm{bo}^{-1} \\)</span> where <span>\\(\\textrm{bo}\\)</span> is the Bond number. Then, we show that these solutions are close, on the same time scale, to the solutions of the BO equation with a precision of order <span>\\({\\mathcal {O}}(\\mu + \\textrm{bo}^{-1})\\)</span>. In addition, we provide the justification of new equations with improved dispersive properties, the Benjamin equation, and the Intermediate Long Wave (ILW) equation in the deep-water limit.</p><p>The long-time well-posedness of the two-layer fluid problem was first studied by Lannes [Arch. Ration. Mech. Anal., 208(2):481-567, 2013] in the case where both fluids have finite depth. Here, we adapt this work to the case where one of the fluid domains is of finite depth, and the other one is of infinite depth. The novelties of the proof are related to the geometry of the problem, where the difference in domains alters the functional setting for the Dirichlet-Neumann operators involved. In particular, we study the various compositions of these operators that require a refined symbolic analysis of the Dirichlet-Neumann operator on infinite depth and derive new pseudo-differential estimates that might be of independent interest.</p></div>","PeriodicalId":36382,"journal":{"name":"Annals of Pde","volume":"10 2","pages":""},"PeriodicalIF":2.4000,"publicationDate":"2024-11-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s40818-024-00190-z.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annals of Pde","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s40818-024-00190-z","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 0

Abstract

In this paper, we give the first rigorous justification of the Benjamin-Ono equation:

$$\begin{aligned} \hspace{3cm} \partial _t \zeta + (1 - \frac{\gamma }{2}\sqrt{\mu }|\textrm{D}|)\partial _x \zeta + \frac{3{\varepsilon }}{2}\zeta \partial _x\zeta =0, \hspace{2cm} \text {(BO)} \end{aligned}$$

as an internal water wave model on the physical time scale. Here, \({\varepsilon }\) is a small parameter measuring the weak nonlinearity of the waves, \(\mu \) is the shallowness parameter, and \(\gamma \in (0,1)\) is the ratio between the densities of the two fluids. To be precise, we first prove the existence of a solution to the internal water wave equations for a two-layer fluid with surface tension, where one layer is of shallow depth and the other is of infinite depth. The existence time is of order \({\mathcal {O}}(\frac{1}{{\varepsilon }})\) for a small amount of surface tension such that \({\varepsilon }^2 \le \textrm{bo}^{-1} \) where \(\textrm{bo}\) is the Bond number. Then, we show that these solutions are close, on the same time scale, to the solutions of the BO equation with a precision of order \({\mathcal {O}}(\mu + \textrm{bo}^{-1})\). In addition, we provide the justification of new equations with improved dispersive properties, the Benjamin equation, and the Intermediate Long Wave (ILW) equation in the deep-water limit.

The long-time well-posedness of the two-layer fluid problem was first studied by Lannes [Arch. Ration. Mech. Anal., 208(2):481-567, 2013] in the case where both fluids have finite depth. Here, we adapt this work to the case where one of the fluid domains is of finite depth, and the other one is of infinite depth. The novelties of the proof are related to the geometry of the problem, where the difference in domains alters the functional setting for the Dirichlet-Neumann operators involved. In particular, we study the various compositions of these operators that require a refined symbolic analysis of the Dirichlet-Neumann operator on infinite depth and derive new pseudo-differential estimates that might be of independent interest.

本杰明-奥诺方程作为内水波模型的合理性
在本文中,我们首次严格论证了本杰明-奥诺方程: $$\begin{aligned}\hspace{3cm}\partial _t \zeta + (1 - \frac{gamma }{2}\sqrt{\mu }|\textrm{D}|)\partial _x \zeta + \frac{3{\varepsilon }}{2}\zeta \partial _x\zeta =0, \hspace{2cm}\text{(BO)}(end{aligned}$$是物理时间尺度上的内水波模型。这里,\({\varepsilon }\) 是衡量波的弱非线性的小参数,\(\mu \)是浅度参数,\(\gamma \in (0,1)\) 是两种流体密度的比值。准确地说,我们首先证明了具有表面张力的两层流体的内部水波方程的解的存在性,其中一层为浅层,另一层为无限深层。对于少量表面张力,存在时间为 \({\mathcal {O}}(\frac{1}{{\varepsilon }})\令 \({\varepsilon }^2 \le \textrm{bo}^{-1} \),其中 \(\textrm{bo}\) 是邦德数。然后,我们证明这些解在相同的时间尺度上接近于 BO方程的解,其精度为 \({\mathcal{O}}(\mu + \textrm{bo}^{-1})\)。Lannes [Arch. Ration. Mech. Anal., 208(2):481-567, 2013]首次研究了双层流体问题在两层流体深度都有限的情况下的长时可求性。在此,我们将这一研究成果应用于其中一个流体域为有限深度,而另一个为无限深度的情况。证明的新颖之处与问题的几何形状有关,其中域的不同改变了所涉及的 Dirichlet-Neumann 算子的函数设置。特别是,我们研究了这些算子的各种组合,这需要对无限深度上的 Dirichlet-Neumann 算子进行精细的符号分析,并推导出可能具有独立意义的新的伪微分估计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Annals of Pde
Annals of Pde Mathematics-Geometry and Topology
CiteScore
3.70
自引率
3.60%
发文量
22
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信