A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom

A thin-layer model for shallow viscoelastic free-surface gravity flows on slippery topographies around a flat plane has been derived recently in [Bouchut-Boyaval, M3AS (23) 2013]. We show here how the model can be modified for flows on rugous topographies varying ar...

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Main Author: Boyaval Sébastien
Format: Article
Language:English
Published: EDP Sciences 2014-09-01
Series:ESAIM: Proceedings and Surveys
Online Access:http://dx.doi.org/10.1051/proc/201445011
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spelling doaj-eea55465505240b482fb19700408af032021-07-15T14:07:21ZengEDP SciencesESAIM: Proceedings and Surveys2267-30592014-09-014510811710.1051/proc/201445011proc144511A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottomBoyaval Sébastien0Université Paris-Est, Laboratoire d’hydraulique Saint-Venant, Ecole Nationale des Ponts et Chaussées – EDF R&D – CETMEFA thin-layer model for shallow viscoelastic free-surface gravity flows on slippery topographies around a flat plane has been derived recently in [Bouchut-Boyaval, M3AS (23) 2013]. We show here how the model can be modified for flows on rugous topographies varying around an inclined plane. The new reduced model extends the scope of one derived in [Bouchut-Boyaval, M3AS (23) 2013]. It is one particular thin-layer model for free-surface gravity flows among many ones that can be formally derived with a generic unifying procedure. Many rheologies and various shallow flow regimes have already been treated within a single unified framework in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013]. The initial full model used here as a starting point is however a little different to one used in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], although the new thin-layer model is very similar to the one derived therein. Precisely, here, the bulk dissipation (due to e.g. viscosity) is neglected from the beginning, like in [Bouchut-Boyaval, M3AS (23) 2013]. Moreover, unlike in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], we perform here numerical simulations. The interest of the extension is illustrated in a physically interesting situation where new stationary solutions exist. To that aim, the Finite-Volume method proposed in [Bouchut-Boyaval, M3AS (23) 2013] needs to be modified, with an adequate discretization of the new source terms. Interestingly, we can also numerically exhibit an apparently new kind of “roll-wave” solution.http://dx.doi.org/10.1051/proc/201445011
collection DOAJ
language English
format Article
sources DOAJ
author Boyaval Sébastien
spellingShingle Boyaval Sébastien
A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
ESAIM: Proceedings and Surveys
author_facet Boyaval Sébastien
author_sort Boyaval Sébastien
title A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
title_short A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
title_full A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
title_fullStr A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
title_full_unstemmed A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
title_sort new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom
publisher EDP Sciences
series ESAIM: Proceedings and Surveys
issn 2267-3059
publishDate 2014-09-01
description A thin-layer model for shallow viscoelastic free-surface gravity flows on slippery topographies around a flat plane has been derived recently in [Bouchut-Boyaval, M3AS (23) 2013]. We show here how the model can be modified for flows on rugous topographies varying around an inclined plane. The new reduced model extends the scope of one derived in [Bouchut-Boyaval, M3AS (23) 2013]. It is one particular thin-layer model for free-surface gravity flows among many ones that can be formally derived with a generic unifying procedure. Many rheologies and various shallow flow regimes have already been treated within a single unified framework in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013]. The initial full model used here as a starting point is however a little different to one used in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], although the new thin-layer model is very similar to the one derived therein. Precisely, here, the bulk dissipation (due to e.g. viscosity) is neglected from the beginning, like in [Bouchut-Boyaval, M3AS (23) 2013]. Moreover, unlike in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], we perform here numerical simulations. The interest of the extension is illustrated in a physically interesting situation where new stationary solutions exist. To that aim, the Finite-Volume method proposed in [Bouchut-Boyaval, M3AS (23) 2013] needs to be modified, with an adequate discretization of the new source terms. Interestingly, we can also numerically exhibit an apparently new kind of “roll-wave” solution.
url http://dx.doi.org/10.1051/proc/201445011
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