Cargando…
A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones
Earthquake fault zones are more complex, both geometrically and rheologically, than an idealized infinitely thin plane embedded in linear elastic material. To incorporate nonlinear material behaviour, natural complexities and multi-physics coupling within and outside of fault zones, here we present...
Autores principales: | , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society Publishing
2021
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8059614/ https://www.ncbi.nlm.nih.gov/pubmed/33715407 http://dx.doi.org/10.1098/rsta.2020.0130 |
_version_ | 1783681215740510208 |
---|---|
author | Gabriel, A.-A. Li, D. Chiocchetti, S. Tavelli, M. Peshkov, I. Romenski, E. Dumbser, M. |
author_facet | Gabriel, A.-A. Li, D. Chiocchetti, S. Tavelli, M. Peshkov, I. Romenski, E. Dumbser, M. |
author_sort | Gabriel, A.-A. |
collection | PubMed |
description | Earthquake fault zones are more complex, both geometrically and rheologically, than an idealized infinitely thin plane embedded in linear elastic material. To incorporate nonlinear material behaviour, natural complexities and multi-physics coupling within and outside of fault zones, here we present a first-order hyperbolic and thermodynamically compatible mathematical model for a continuum in a gravitational field which provides a unified description of nonlinear elasto-plasticity, material damage and of viscous Newtonian flows with phase transition between solid and liquid phases. The fault geometry and secondary cracks are described via a scalar function ξ ∈ [0, 1] that indicates the local level of material damage. The model also permits the representation of arbitrarily complex geometries via a diffuse interface approach based on the solid volume fraction function α ∈ [0, 1]. Neither of the two scalar fields ξ and α needs to be mesh-aligned, allowing thus faults and cracks with complex topology and the use of adaptive Cartesian meshes (AMR). The model shares common features with phase-field approaches, but substantially extends them. We show a wide range of numerical applications that are relevant for dynamic earthquake rupture in fault zones, including the co-seismic generation of secondary off-fault shear cracks, tensile rock fracture in the Brazilian disc test, as well as a natural convection problem in molten rock-like material. This article is part of the theme issue ‘Fracture dynamics of solid materials: from particles to the globe’. |
format | Online Article Text |
id | pubmed-8059614 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | The Royal Society Publishing |
record_format | MEDLINE/PubMed |
spelling | pubmed-80596142022-02-02 A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones Gabriel, A.-A. Li, D. Chiocchetti, S. Tavelli, M. Peshkov, I. Romenski, E. Dumbser, M. Philos Trans A Math Phys Eng Sci Articles Earthquake fault zones are more complex, both geometrically and rheologically, than an idealized infinitely thin plane embedded in linear elastic material. To incorporate nonlinear material behaviour, natural complexities and multi-physics coupling within and outside of fault zones, here we present a first-order hyperbolic and thermodynamically compatible mathematical model for a continuum in a gravitational field which provides a unified description of nonlinear elasto-plasticity, material damage and of viscous Newtonian flows with phase transition between solid and liquid phases. The fault geometry and secondary cracks are described via a scalar function ξ ∈ [0, 1] that indicates the local level of material damage. The model also permits the representation of arbitrarily complex geometries via a diffuse interface approach based on the solid volume fraction function α ∈ [0, 1]. Neither of the two scalar fields ξ and α needs to be mesh-aligned, allowing thus faults and cracks with complex topology and the use of adaptive Cartesian meshes (AMR). The model shares common features with phase-field approaches, but substantially extends them. We show a wide range of numerical applications that are relevant for dynamic earthquake rupture in fault zones, including the co-seismic generation of secondary off-fault shear cracks, tensile rock fracture in the Brazilian disc test, as well as a natural convection problem in molten rock-like material. This article is part of the theme issue ‘Fracture dynamics of solid materials: from particles to the globe’. The Royal Society Publishing 2021-05-03 2021-03-15 /pmc/articles/PMC8059614/ /pubmed/33715407 http://dx.doi.org/10.1098/rsta.2020.0130 Text en © 2021 The Authors. https://creativecommons.org/licenses/by/4.0/Published by the Royal Society under the terms of the Creative Commons Attribution License http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) , which permits unrestricted use, provided the original author and source are credited. |
spellingShingle | Articles Gabriel, A.-A. Li, D. Chiocchetti, S. Tavelli, M. Peshkov, I. Romenski, E. Dumbser, M. A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title | A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title_full | A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title_fullStr | A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title_full_unstemmed | A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title_short | A unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
title_sort | unified first-order hyperbolic model for nonlinear dynamic rupture processes in diffuse fracture zones |
topic | Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8059614/ https://www.ncbi.nlm.nih.gov/pubmed/33715407 http://dx.doi.org/10.1098/rsta.2020.0130 |
work_keys_str_mv | AT gabrielaa aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT lid aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT chiocchettis aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT tavellim aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT peshkovi aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT romenskie aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT dumbserm aunifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT gabrielaa unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT lid unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT chiocchettis unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT tavellim unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT peshkovi unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT romenskie unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones AT dumbserm unifiedfirstorderhyperbolicmodelfornonlineardynamicruptureprocessesindiffusefracturezones |