Kolmogorov's dissipation number and the number of degrees of freedom for the 3D Navier-Stokes equations
Proceedings of the Royal Society of Edinburgh Section A, Volume 149, Issue 2 April 2019 , pp. 429-446 Kolmogorov's theory of turbulence predicts that only wavenumbers below some critical value, called Kolmogorov's dissipation number, are essential to describe the evolution of a three-dimen...
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creator | Cheskidov, Alexey Dai, Mimi |
description | Proceedings of the Royal Society of Edinburgh Section A, Volume
149, Issue 2 April 2019 , pp. 429-446 Kolmogorov's theory of turbulence predicts that only wavenumbers below some
critical value, called Kolmogorov's dissipation number, are essential to
describe the evolution of a three-dimensional fluid flow. A determining
wavenumber, first introduced by Foias and Prodi for the 2D Navier-Stokes
equations, is a mathematical analog of Kolmogorov's number. The purpose of this
paper is to prove the existence of a time-dependent determining wavenumber for
the 3D Navier-Stokes equations whose time average is bounded by Kolmogorov's
dissipation wavenumber for all solutions on the global attractor whose
intermittency is not extreme. |
doi_str_mv | 10.48550/arxiv.1510.00379 |
format | Article |
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149, Issue 2 April 2019 , pp. 429-446 Kolmogorov's theory of turbulence predicts that only wavenumbers below some
critical value, called Kolmogorov's dissipation number, are essential to
describe the evolution of a three-dimensional fluid flow. A determining
wavenumber, first introduced by Foias and Prodi for the 2D Navier-Stokes
equations, is a mathematical analog of Kolmogorov's number. The purpose of this
paper is to prove the existence of a time-dependent determining wavenumber for
the 3D Navier-Stokes equations whose time average is bounded by Kolmogorov's
dissipation wavenumber for all solutions on the global attractor whose
intermittency is not extreme.</description><identifier>DOI: 10.48550/arxiv.1510.00379</identifier><language>eng</language><subject>Mathematics - Analysis of PDEs ; Physics - Fluid Dynamics</subject><creationdate>2015-10</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/1510.00379$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.1510.00379$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Cheskidov, Alexey</creatorcontrib><creatorcontrib>Dai, Mimi</creatorcontrib><title>Kolmogorov's dissipation number and the number of degrees of freedom for the 3D Navier-Stokes equations</title><description>Proceedings of the Royal Society of Edinburgh Section A, Volume
149, Issue 2 April 2019 , pp. 429-446 Kolmogorov's theory of turbulence predicts that only wavenumbers below some
critical value, called Kolmogorov's dissipation number, are essential to
describe the evolution of a three-dimensional fluid flow. A determining
wavenumber, first introduced by Foias and Prodi for the 2D Navier-Stokes
equations, is a mathematical analog of Kolmogorov's number. The purpose of this
paper is to prove the existence of a time-dependent determining wavenumber for
the 3D Navier-Stokes equations whose time average is bounded by Kolmogorov's
dissipation wavenumber for all solutions on the global attractor whose
intermittency is not extreme.</description><subject>Mathematics - Analysis of PDEs</subject><subject>Physics - Fluid Dynamics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNo1jztPwzAUhb0woMIPYMJbpxQ7rmt7ROUpKhjaPbqOr4NFExc7jeDfkwaYzkNHR_oIueJssdRSshtIX2FYcDkWjAllzknzEvdtbGKKwzxTF3IOB-hD7Gh3bC0mCp2j_Tv-x-ipwyYh5pP1o3GxpT6maSTu6CsMAVOx7ePHuMHP4_SWL8iZh33Gyz-dkd3D_W79VGzeHp_Xt5sCVsoUJXNKOBRGLg2uAMGW3pS1kkxbwZVWQhsulITa8lqXGiwKNADItJfSWzEj17-3E2l1SKGF9F2diKuJWPwAeoNSKg</recordid><startdate>20151001</startdate><enddate>20151001</enddate><creator>Cheskidov, Alexey</creator><creator>Dai, Mimi</creator><scope>AKZ</scope><scope>GOX</scope></search><sort><creationdate>20151001</creationdate><title>Kolmogorov's dissipation number and the number of degrees of freedom for the 3D Navier-Stokes equations</title><author>Cheskidov, Alexey ; Dai, Mimi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a679-20d73de39549e6aeab2f92c7508b317873891375acb1c828abe3e9aae08f55fb3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Mathematics - Analysis of PDEs</topic><topic>Physics - Fluid Dynamics</topic><toplevel>online_resources</toplevel><creatorcontrib>Cheskidov, Alexey</creatorcontrib><creatorcontrib>Dai, Mimi</creatorcontrib><collection>arXiv Mathematics</collection><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Cheskidov, Alexey</au><au>Dai, Mimi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Kolmogorov's dissipation number and the number of degrees of freedom for the 3D Navier-Stokes equations</atitle><date>2015-10-01</date><risdate>2015</risdate><abstract>Proceedings of the Royal Society of Edinburgh Section A, Volume
149, Issue 2 April 2019 , pp. 429-446 Kolmogorov's theory of turbulence predicts that only wavenumbers below some
critical value, called Kolmogorov's dissipation number, are essential to
describe the evolution of a three-dimensional fluid flow. A determining
wavenumber, first introduced by Foias and Prodi for the 2D Navier-Stokes
equations, is a mathematical analog of Kolmogorov's number. The purpose of this
paper is to prove the existence of a time-dependent determining wavenumber for
the 3D Navier-Stokes equations whose time average is bounded by Kolmogorov's
dissipation wavenumber for all solutions on the global attractor whose
intermittency is not extreme.</abstract><doi>10.48550/arxiv.1510.00379</doi><oa>free_for_read</oa></addata></record> |
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subjects | Mathematics - Analysis of PDEs Physics - Fluid Dynamics |
title | Kolmogorov's dissipation number and the number of degrees of freedom for the 3D Navier-Stokes equations |
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