Construction of Lagrangians in continuum theories
For physical systems the dynamics of which is formulated within the framework of Lagrange formalism, the dynamics is completely defined by only one function, namely the Lagrangian. For instance, the whole conservative Newtonian mechanics has been successfully embedded into this methodical concept. I...
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Veröffentlicht in: | Proceedings of the Royal Society. A, Mathematical, physical, and engineering sciences Mathematical, physical, and engineering sciences, 2004-11, Vol.460 (2051), p.3241-3260 |
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description | For physical systems the dynamics of which is formulated within the framework of Lagrange formalism, the dynamics is completely defined by only one function, namely the Lagrangian. For instance, the whole conservative Newtonian mechanics has been successfully embedded into this methodical concept. In continuum theories, however, the situation is different: no generally valid construction rule for the Lagrangian has been established in the past. In this paper general properties of Lagrangians in non-relativistic field theories are derived by considering universal symmetries, namely space- and time-translations, rigid rotations and Galilei boosts. These investigations discover the dual structure, i.e. the coexistence of two complementary representations of the Lagrangian. From the dual structure, relevant restrictions for the analytical form of the Lagrangian are derived which eventually result in a general scheme for Lagrangians. For two examples, namely Schrödinger's theory and the flow of an ideal fluid, the compatibility of the Lagrangian with the general scheme is demonstrated. The dual structure also has consequences for the balances which result from the respective symmetries by Noether's theorem: universally valid constitutive relations between the densities and the flux densities of energy, momentum, mass and centre of mass are derived. By an inverse treatment of these constitutive relations a Lagrangian for a given physical system can be constructed. This procedure is demonstrated for an elastically deforming body. |
doi_str_mv | 10.1098/rspa.2004.1354 |
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For instance, the whole conservative Newtonian mechanics has been successfully embedded into this methodical concept. In continuum theories, however, the situation is different: no generally valid construction rule for the Lagrangian has been established in the past. In this paper general properties of Lagrangians in non-relativistic field theories are derived by considering universal symmetries, namely space- and time-translations, rigid rotations and Galilei boosts. These investigations discover the dual structure, i.e. the coexistence of two complementary representations of the Lagrangian. From the dual structure, relevant restrictions for the analytical form of the Lagrangian are derived which eventually result in a general scheme for Lagrangians. For two examples, namely Schrödinger's theory and the flow of an ideal fluid, the compatibility of the Lagrangian with the general scheme is demonstrated. The dual structure also has consequences for the balances which result from the respective symmetries by Noether's theorem: universally valid constitutive relations between the densities and the flux densities of energy, momentum, mass and centre of mass are derived. By an inverse treatment of these constitutive relations a Lagrangian for a given physical system can be constructed. 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From the dual structure, relevant restrictions for the analytical form of the Lagrangian are derived which eventually result in a general scheme for Lagrangians. For two examples, namely Schrödinger's theory and the flow of an ideal fluid, the compatibility of the Lagrangian with the general scheme is demonstrated. The dual structure also has consequences for the balances which result from the respective symmetries by Noether's theorem: universally valid constitutive relations between the densities and the flux densities of energy, momentum, mass and centre of mass are derived. By an inverse treatment of these constitutive relations a Lagrangian for a given physical system can be constructed. This procedure is demonstrated for an elastically deforming body.</description><subject>Average linear density</subject><subject>Constitutive equations</subject><subject>Constitutive Relations</subject><subject>Density</subject><subject>Energy</subject><subject>Flux density</subject><subject>Galilei Invariance</subject><subject>Geometric translations</subject><subject>Inverse Variational Problems</subject><subject>Lagrange Formalism</subject><subject>Lagrangian function</subject><subject>Mass</subject><subject>Mass density</subject><subject>Momentum</subject><subject>Universal Symmetries</subject><issn>1364-5021</issn><issn>1471-2946</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNp9UMtOwzAQjBBIlMKVE4f8QIIfm9cNWvGSIrgA4maZ1G5dWjuyHUH-HoegSj3AaXc1O7MzG0XnGKUYVeWldS1PCUKQYprBQTTBUOCEVJAfhp7mkGSI4OPoxLk1QqjKymIS4bnRztuu8cro2Mi45kvL9VJx7WKl48Zor3TXbWO_EsYq4U6jI8k3Tpz91mn0cnvzPL9P6qe7h_l1nTQAxCcFpxy_V0RIWeQYIMwZKkWOgJaUylwAyWkhBMfAJea8qgKwoAsJwFFTcTqN0lG3scY5KyRrrdpy2zOM2BCYDYHZEJgNgQOBjgRr-mDMNEr4nq1NZ3UY_2ZdjKy188bubgAGShANcDLCynnxtYO5_WB5QYuMvZbA6sd6lr1RwmZh_2rcX6nl6lNZwfbc_Bwffiq0Z5CjYCTDjBLATHabDWsXMkiQfyVM31rH99n0G4wRnAA</recordid><startdate>20041108</startdate><enddate>20041108</enddate><creator>Scholle, M.</creator><general>The Royal Society</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20041108</creationdate><title>Construction of Lagrangians in continuum theories</title><author>Scholle, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c442t-7a3a1b92eff761447a3508e6043833f6e42637eea14af1aa99438d3df44a0c9a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>Average linear density</topic><topic>Constitutive equations</topic><topic>Constitutive Relations</topic><topic>Density</topic><topic>Energy</topic><topic>Flux density</topic><topic>Galilei Invariance</topic><topic>Geometric translations</topic><topic>Inverse Variational Problems</topic><topic>Lagrange Formalism</topic><topic>Lagrangian function</topic><topic>Mass</topic><topic>Mass density</topic><topic>Momentum</topic><topic>Universal Symmetries</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Scholle, M.</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><jtitle>Proceedings of the Royal Society. A, Mathematical, physical, and engineering sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Scholle, M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Construction of Lagrangians in continuum theories</atitle><jtitle>Proceedings of the Royal Society. A, Mathematical, physical, and engineering sciences</jtitle><date>2004-11-08</date><risdate>2004</risdate><volume>460</volume><issue>2051</issue><spage>3241</spage><epage>3260</epage><pages>3241-3260</pages><issn>1364-5021</issn><eissn>1471-2946</eissn><abstract>For physical systems the dynamics of which is formulated within the framework of Lagrange formalism, the dynamics is completely defined by only one function, namely the Lagrangian. For instance, the whole conservative Newtonian mechanics has been successfully embedded into this methodical concept. In continuum theories, however, the situation is different: no generally valid construction rule for the Lagrangian has been established in the past. In this paper general properties of Lagrangians in non-relativistic field theories are derived by considering universal symmetries, namely space- and time-translations, rigid rotations and Galilei boosts. These investigations discover the dual structure, i.e. the coexistence of two complementary representations of the Lagrangian. From the dual structure, relevant restrictions for the analytical form of the Lagrangian are derived which eventually result in a general scheme for Lagrangians. For two examples, namely Schrödinger's theory and the flow of an ideal fluid, the compatibility of the Lagrangian with the general scheme is demonstrated. The dual structure also has consequences for the balances which result from the respective symmetries by Noether's theorem: universally valid constitutive relations between the densities and the flux densities of energy, momentum, mass and centre of mass are derived. By an inverse treatment of these constitutive relations a Lagrangian for a given physical system can be constructed. This procedure is demonstrated for an elastically deforming body.</abstract><pub>The Royal Society</pub><doi>10.1098/rspa.2004.1354</doi><tpages>20</tpages></addata></record> |
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subjects | Average linear density Constitutive equations Constitutive Relations Density Energy Flux density Galilei Invariance Geometric translations Inverse Variational Problems Lagrange Formalism Lagrangian function Mass Mass density Momentum Universal Symmetries |
title | Construction of Lagrangians in continuum theories |
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