2021
DOI: 10.1016/j.camwa.2020.07.025
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Mathematical analysis and numerical approximation of a general linearized poro-hyperelastic model

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Cited by 17 publications
(27 citation statements)
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“…For this section we draw inspiration from the stability analysis of a system similar to (2.2), recently proved in [12]; and from the study of the linearised hyperelasticity equations, recently studied in [35]. We restrict the description to Neo-Hookean poroelastic solids with material parameters µ s , λ s , for which the effective first Piola-Kirchhoff stress tensor is…”
Section: Definition and Preliminariesmentioning
confidence: 99%
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“…For this section we draw inspiration from the stability analysis of a system similar to (2.2), recently proved in [12]; and from the study of the linearised hyperelasticity equations, recently studied in [35]. We restrict the description to Neo-Hookean poroelastic solids with material parameters µ s , λ s , for which the effective first Piola-Kirchhoff stress tensor is…”
Section: Definition and Preliminariesmentioning
confidence: 99%
“…Even if many numerical methods for the approximation of linear poroelasticity and their convergence analysis can be found in the recent literature (see [12,[16][17][18]52] and the references therein), much less attention has been given to formulations addressing large-strain poromechanics. In this regard, recent works include an enriched Galerkin framework [26], stabilised finite elements [15,77] and hybrid finite elements as well [76].…”
Section: Introductionmentioning
confidence: 99%
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“…The analysis of the well-posedness, stability and numerical approximation of this class of poromechanics models is still largely open. Among recent advances, we highlight the development and analysis of an implicit time discretization preserving the dissipation-energy identity at the discrete level [18]; an energy-preserving implicit-explicit time discretization incorporating a (non-iterative) operator splitting, decoupling solid and flow computations [19]; an energy-stable space and time discretization for a linearized model with focus on quasi-incompressible solids [20]; and finally, a space and time discretization for the same linearized model, exploiting a generalized saddle point structure and ultimately suggesting the use of Taylor-Hood type finite elements [21].…”
Section: Introductionmentioning
confidence: 99%
“…In addition to interactions between fluid networks, recently also the viscous forces acting within each network have come to the fore [6,14,12,31]. At its core, the effect of viscosity can be accounted for by replacing the Darcy approximation in the poroelasticity model by a Brinkman approximation [11,40].…”
mentioning
confidence: 99%