A non-conventional discontinuous Lagrangian for viscous flow
Drawing an analogy with quantum mechanics, a new Lagrangian is proposed for a variational formulation of the Navier–Stokes equations which to-date has remained elusive. A key feature is that the resulting Lagrangian is discontinuous in nature, posing additional challenges apropos the mathematical tr...
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Online Access: | https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160447 |
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doaj-e40ca040a0b94be9bf06ff1fe929d93f2020-11-25T04:02:09ZengThe Royal SocietyRoyal Society Open Science2054-57032017-01-014210.1098/rsos.160447160447A non-conventional discontinuous Lagrangian for viscous flowM. ScholleF. MarnerDrawing an analogy with quantum mechanics, a new Lagrangian is proposed for a variational formulation of the Navier–Stokes equations which to-date has remained elusive. A key feature is that the resulting Lagrangian is discontinuous in nature, posing additional challenges apropos the mathematical treatment of the related variational problem, all of which are resolvable. In addition to extending Lagrange's formalism to problems involving discontinuous behaviour, it is demonstrated that the associated equations of motion can self-consistently be interpreted within the framework of thermodynamics beyond local equilibrium, with the limiting case recovering the classical Navier–Stokes equations. Perspectives for applying the new formalism to discontinuous physical phenomena such as phase and grain boundaries, shock waves and flame fronts are provided.https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160447potential fieldsvariational calculusnavier–stokes equationsnon-equilibrium thermodynamicsanalogiesfirst integrals |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. Scholle F. Marner |
spellingShingle |
M. Scholle F. Marner A non-conventional discontinuous Lagrangian for viscous flow Royal Society Open Science potential fields variational calculus navier–stokes equations non-equilibrium thermodynamics analogies first integrals |
author_facet |
M. Scholle F. Marner |
author_sort |
M. Scholle |
title |
A non-conventional discontinuous Lagrangian for viscous flow |
title_short |
A non-conventional discontinuous Lagrangian for viscous flow |
title_full |
A non-conventional discontinuous Lagrangian for viscous flow |
title_fullStr |
A non-conventional discontinuous Lagrangian for viscous flow |
title_full_unstemmed |
A non-conventional discontinuous Lagrangian for viscous flow |
title_sort |
non-conventional discontinuous lagrangian for viscous flow |
publisher |
The Royal Society |
series |
Royal Society Open Science |
issn |
2054-5703 |
publishDate |
2017-01-01 |
description |
Drawing an analogy with quantum mechanics, a new Lagrangian is proposed for a variational formulation of the Navier–Stokes equations which to-date has remained elusive. A key feature is that the resulting Lagrangian is discontinuous in nature, posing additional challenges apropos the mathematical treatment of the related variational problem, all of which are resolvable. In addition to extending Lagrange's formalism to problems involving discontinuous behaviour, it is demonstrated that the associated equations of motion can self-consistently be interpreted within the framework of thermodynamics beyond local equilibrium, with the limiting case recovering the classical Navier–Stokes equations. Perspectives for applying the new formalism to discontinuous physical phenomena such as phase and grain boundaries, shock waves and flame fronts are provided. |
topic |
potential fields variational calculus navier–stokes equations non-equilibrium thermodynamics analogies first integrals |
url |
https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160447 |
work_keys_str_mv |
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