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The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow
Semi-continuum modelling of unsaturated porous media flow is based on representing the porous medium as a grid of non-infinitesimal blocks that retain the character of a porous medium. This approach is similar to the hybrid/multiscale modelling. Semi-continuum model is able to physically correctly d...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9090790/ https://www.ncbi.nlm.nih.gov/pubmed/35538096 http://dx.doi.org/10.1038/s41598-022-11437-9 |
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author | Vodák, Rostislav Fürst, Tomáš Šír, Miloslav Kmec, Jakub |
author_facet | Vodák, Rostislav Fürst, Tomáš Šír, Miloslav Kmec, Jakub |
author_sort | Vodák, Rostislav |
collection | PubMed |
description | Semi-continuum modelling of unsaturated porous media flow is based on representing the porous medium as a grid of non-infinitesimal blocks that retain the character of a porous medium. This approach is similar to the hybrid/multiscale modelling. Semi-continuum model is able to physically correctly describe diffusion-like flow, finger-like flow, and the transition between them. This article presents the limit of the semi-continuum model as the block size goes to zero. In the limiting process, the retention curve of each block scales with the block size and in the limit becomes a hysteresis operator of the Prandtl-type used in elasto-plasticity models. Mathematical analysis showed that the limit of the semi-continuum model is a hyperbolic-parabolic partial differential equation with a hysteresis operator of Prandl’s type. This limit differs from the standard Richards’ equation, which is a parabolic equation and is not able to describe finger-like flow. |
format | Online Article Text |
id | pubmed-9090790 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-90907902022-05-12 The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow Vodák, Rostislav Fürst, Tomáš Šír, Miloslav Kmec, Jakub Sci Rep Article Semi-continuum modelling of unsaturated porous media flow is based on representing the porous medium as a grid of non-infinitesimal blocks that retain the character of a porous medium. This approach is similar to the hybrid/multiscale modelling. Semi-continuum model is able to physically correctly describe diffusion-like flow, finger-like flow, and the transition between them. This article presents the limit of the semi-continuum model as the block size goes to zero. In the limiting process, the retention curve of each block scales with the block size and in the limit becomes a hysteresis operator of the Prandtl-type used in elasto-plasticity models. Mathematical analysis showed that the limit of the semi-continuum model is a hyperbolic-parabolic partial differential equation with a hysteresis operator of Prandl’s type. This limit differs from the standard Richards’ equation, which is a parabolic equation and is not able to describe finger-like flow. Nature Publishing Group UK 2022-05-10 /pmc/articles/PMC9090790/ /pubmed/35538096 http://dx.doi.org/10.1038/s41598-022-11437-9 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Vodák, Rostislav Fürst, Tomáš Šír, Miloslav Kmec, Jakub The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title | The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title_full | The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title_fullStr | The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title_full_unstemmed | The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title_short | The difference between semi-continuum model and Richards’ equation for unsaturated porous media flow |
title_sort | difference between semi-continuum model and richards’ equation for unsaturated porous media flow |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9090790/ https://www.ncbi.nlm.nih.gov/pubmed/35538096 http://dx.doi.org/10.1038/s41598-022-11437-9 |
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