Steady Periodic Hydroelastic Waves
This is a study of steady periodic travelling waves on the surface of an infinitely deep irrotational ocean when the top streamline is in contact with a light frictionless membrane that strongly resists stretching and bending and the pressure in the air above is constant. It is shown that this is a...
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Veröffentlicht in: | Archive for rational mechanics and analysis 2008-08, Vol.189 (2), p.325-362 |
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description | This is a study of steady periodic travelling waves on the surface of an infinitely deep irrotational ocean when the top streamline is in contact with a light frictionless membrane that strongly resists stretching and bending and the pressure in the air above is constant. It is shown that this is a free-boundary problem for the domain of a harmonic function (the stream function) which is zero on the boundary and at which its normal derivative is determined by the boundary geometry. With the wavelength fixed at 2
π
, we find travelling waves with arbitrarily large speeds for a significant class of membranes. Our approach is based on Zakharov’s Hamiltonian theory of water waves to which elastic effects at the surface have been added. However we avoid the Hamiltonian machinery by first defining a Lagrangian in terms of kinetic and potential energies using physical variables. A conformal transformation then yields an equivalent Lagrangian in which the unknown function is the wave height. Once critical points of that Lagrangian have been shown to correspond to the physical problem, the existence of hydroelastic waves for a class of membranes is established by maximization. Hardy spaces on the unit disc and the Hilbert transform on the unit circle play a role in the analysis. |
doi_str_mv | 10.1007/s00205-007-0104-2 |
format | Article |
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π
, we find travelling waves with arbitrarily large speeds for a significant class of membranes. Our approach is based on Zakharov’s Hamiltonian theory of water waves to which elastic effects at the surface have been added. However we avoid the Hamiltonian machinery by first defining a Lagrangian in terms of kinetic and potential energies using physical variables. A conformal transformation then yields an equivalent Lagrangian in which the unknown function is the wave height. Once critical points of that Lagrangian have been shown to correspond to the physical problem, the existence of hydroelastic waves for a class of membranes is established by maximization. Hardy spaces on the unit disc and the Hilbert transform on the unit circle play a role in the analysis.</description><identifier>ISSN: 0003-9527</identifier><identifier>EISSN: 1432-0673</identifier><identifier>DOI: 10.1007/s00205-007-0104-2</identifier><identifier>CODEN: AVRMAW</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>Classical Mechanics ; Complex Systems ; Dynamics of the ocean (upper and deep oceans) ; Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Fluid dynamics ; Fluid- and Aerodynamics ; Fundamental areas of phenomenology (including applications) ; General theory ; Marine ; Mathematical and Computational Physics ; Mathematical methods in physics ; Numerical approximation and analysis ; Ordinary and partial differential equations, boundary value problems ; Physics ; Physics and Astronomy ; Physics of the oceans ; Solid mechanics ; Structural and continuum mechanics ; Studies ; Theoretical ; Vibration, mechanical wave, dynamic stability (aeroelasticity, vibration control...)</subject><ispartof>Archive for rational mechanics and analysis, 2008-08, Vol.189 (2), p.325-362</ispartof><rights>Springer-Verlag 2008</rights><rights>2008 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c378t-9166b76bedce029266abd7fe6f04be26ba4fd7feb59533353ba495f31c4a97e53</citedby><cites>FETCH-LOGICAL-c378t-9166b76bedce029266abd7fe6f04be26ba4fd7feb59533353ba495f31c4a97e53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s00205-007-0104-2$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s00205-007-0104-2$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=20431620$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Toland, J. F.</creatorcontrib><title>Steady Periodic Hydroelastic Waves</title><title>Archive for rational mechanics and analysis</title><addtitle>Arch Rational Mech Anal</addtitle><description>This is a study of steady periodic travelling waves on the surface of an infinitely deep irrotational ocean when the top streamline is in contact with a light frictionless membrane that strongly resists stretching and bending and the pressure in the air above is constant. It is shown that this is a free-boundary problem for the domain of a harmonic function (the stream function) which is zero on the boundary and at which its normal derivative is determined by the boundary geometry. With the wavelength fixed at 2
π
, we find travelling waves with arbitrarily large speeds for a significant class of membranes. Our approach is based on Zakharov’s Hamiltonian theory of water waves to which elastic effects at the surface have been added. However we avoid the Hamiltonian machinery by first defining a Lagrangian in terms of kinetic and potential energies using physical variables. A conformal transformation then yields an equivalent Lagrangian in which the unknown function is the wave height. Once critical points of that Lagrangian have been shown to correspond to the physical problem, the existence of hydroelastic waves for a class of membranes is established by maximization. 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π
, we find travelling waves with arbitrarily large speeds for a significant class of membranes. Our approach is based on Zakharov’s Hamiltonian theory of water waves to which elastic effects at the surface have been added. However we avoid the Hamiltonian machinery by first defining a Lagrangian in terms of kinetic and potential energies using physical variables. A conformal transformation then yields an equivalent Lagrangian in which the unknown function is the wave height. Once critical points of that Lagrangian have been shown to correspond to the physical problem, the existence of hydroelastic waves for a class of membranes is established by maximization. Hardy spaces on the unit disc and the Hilbert transform on the unit circle play a role in the analysis.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/s00205-007-0104-2</doi><tpages>38</tpages></addata></record> |
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subjects | Classical Mechanics Complex Systems Dynamics of the ocean (upper and deep oceans) Earth, ocean, space Exact sciences and technology External geophysics Fluid dynamics Fluid- and Aerodynamics Fundamental areas of phenomenology (including applications) General theory Marine Mathematical and Computational Physics Mathematical methods in physics Numerical approximation and analysis Ordinary and partial differential equations, boundary value problems Physics Physics and Astronomy Physics of the oceans Solid mechanics Structural and continuum mechanics Studies Theoretical Vibration, mechanical wave, dynamic stability (aeroelasticity, vibration control...) |
title | Steady Periodic Hydroelastic Waves |
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