2020
DOI: 10.1007/s00603-020-02147-7
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Quasi-isotropic Biot’s Tensor for Anisotropic Porous Rocks: Experiments and Micromechanical Modelling

Abstract: HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L'archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d'enseignement et de recherche français ou étrangers, des labor… Show more

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Cited by 2 publications
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“…At the first-step homogenization, the rock block with the assumption of uniformly distributed penny-shaped cracks embedded is homogenized by the Eshelby solution-based upscaling procedure. Following the free energy of saturated cracked rocks (Chen et al 2013, Zhu 2016, the associated free enthalpy of rock block using the Mori-Tanaka homogenization scheme can be obtained by Legendre-Fenchel transform of the free energy (Zhu et al 2008 (2) where is the macroscopic strain contributed by the cracks, β and γ are the volumetric averaging of opening and sliding of cracks, is the unit sphere surface accounting for uniform randomly-distributed cracks, denotes the unit normal vector of randomly-distributed cracks; is the isotropic elastic compliance tensor of the solid matrix, which is characterized by its Poisson's ratio and Young's modulus ; H 0 and H 1 are two elastic parameters calculated by and ; is the second-order identity tensor; is the unit normal vector of bedding planes; is the microscopic damage variable defined by crack density, denotes the number of cracks per unit volume, a is the average radius; , B are the Biot modulus and Biot coefficient tensor of cracked rock blocks, they are related to the homogenized effective tensor of cracked rocks, with uniform randomly-distributed cracks in rock blocks an isotropic Biot coefficient tensor is used for simplification (Xie et al 2012, Hu et al 2020, , , and are the Biot coefficient and initial porosity for rock blocks.…”
Section: Free Enthalpy Of Saturated Layered Rocksmentioning
confidence: 99%
“…At the first-step homogenization, the rock block with the assumption of uniformly distributed penny-shaped cracks embedded is homogenized by the Eshelby solution-based upscaling procedure. Following the free energy of saturated cracked rocks (Chen et al 2013, Zhu 2016, the associated free enthalpy of rock block using the Mori-Tanaka homogenization scheme can be obtained by Legendre-Fenchel transform of the free energy (Zhu et al 2008 (2) where is the macroscopic strain contributed by the cracks, β and γ are the volumetric averaging of opening and sliding of cracks, is the unit sphere surface accounting for uniform randomly-distributed cracks, denotes the unit normal vector of randomly-distributed cracks; is the isotropic elastic compliance tensor of the solid matrix, which is characterized by its Poisson's ratio and Young's modulus ; H 0 and H 1 are two elastic parameters calculated by and ; is the second-order identity tensor; is the unit normal vector of bedding planes; is the microscopic damage variable defined by crack density, denotes the number of cracks per unit volume, a is the average radius; , B are the Biot modulus and Biot coefficient tensor of cracked rock blocks, they are related to the homogenized effective tensor of cracked rocks, with uniform randomly-distributed cracks in rock blocks an isotropic Biot coefficient tensor is used for simplification (Xie et al 2012, Hu et al 2020, , , and are the Biot coefficient and initial porosity for rock blocks.…”
Section: Free Enthalpy Of Saturated Layered Rocksmentioning
confidence: 99%