Anisotropic subloading surface Cam‐clay plasticity model with rotational hardening: Deformation gradient‐based formulation for finite strain
This study is aimed at developing an anisotropic elastoplastic constitutive model for geomaterials at finite strain and its stress calculation algorithm based on the fully implicit return‐mapping scheme. The Cam‐clay plasticity model is adopted as a specific prototype model of geomaterials. As a per...
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| Veröffentlicht in: | International journal for numerical and analytical methods in geomechanics Jg. 45; H. 16; S. 2321 - 2370 |
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| Format: | Journal Article |
| Sprache: | Englisch |
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Bognor Regis
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01.11.2021
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| ISSN: | 0363-9061, 1096-9853 |
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| Abstract | This study is aimed at developing an anisotropic elastoplastic constitutive model for geomaterials at finite strain and its stress calculation algorithm based on the fully implicit return‐mapping scheme. The Cam‐clay plasticity model is adopted as a specific prototype model of geomaterials. As a pertinent representation of deformation‐induced anisotropy in geomaterials, nonlinear rotational hardening is incorporated into the model in a theoretically reasonable manner by introducing the dual multiplicative decompositions of the deformation gradient tensor. In addition to the usual decomposition into elastic and plastic parts, the plastic part is decomposed further into a part contributing to the rotational hardening and a remainder part. The former part leads to a back stress ratio tensor related to the rotational hardening via a hyperelastic‐type hardening rule. The constitutive theory is thereby formulated on proper intermediate configurations entirely in terms of deformation‐like tensorial variables possessing invariance property, without resort to any objective rates of stress or stress‐like variables. Combining the Cam‐clay plasticity with the concept of subloading surface, a class of unconventional plasticity, enables the model to be capable of reproducing complex hardening/softening accompanied by volumetric contractive/dilative responses. Basic characteristics and predictive capability of the proposed model, as well as the accuracy of the developed numerical scheme, are verified through several numerical examples including monotonic and cyclic loadings. |
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| AbstractList | This study is aimed at developing an anisotropic elastoplastic constitutive model for geomaterials at finite strain and its stress calculation algorithm based on the fully implicit return‐mapping scheme. The Cam‐clay plasticity model is adopted as a specific prototype model of geomaterials. As a pertinent representation of deformation‐induced anisotropy in geomaterials, nonlinear rotational hardening is incorporated into the model in a theoretically reasonable manner by introducing the dual multiplicative decompositions of the deformation gradient tensor. In addition to the usual decomposition into elastic and plastic parts, the plastic part is decomposed further into a part contributing to the rotational hardening and a remainder part. The former part leads to a back stress ratio tensor related to the rotational hardening via a hyperelastic‐type hardening rule. The constitutive theory is thereby formulated on proper intermediate configurations entirely in terms of deformation‐like tensorial variables possessing invariance property, without resort to any objective rates of stress or stress‐like variables. Combining the Cam‐clay plasticity with the concept of subloading surface, a class of unconventional plasticity, enables the model to be capable of reproducing complex hardening/softening accompanied by volumetric contractive/dilative responses. Basic characteristics and predictive capability of the proposed model, as well as the accuracy of the developed numerical scheme, are verified through several numerical examples including monotonic and cyclic loadings. This study is aimed at developing an anisotropic elastoplastic constitutive model for geomaterials at finite strain and its stress calculation algorithm based on the fully implicit return‐mapping scheme. The Cam‐clay plasticity model is adopted as a specific prototype model of geomaterials. As a pertinent representation of deformation‐induced anisotropy in geomaterials, nonlinear rotational hardening is incorporated into the model in a theoretically reasonable manner by introducing the dual multiplicative decompositions of the deformation gradient tensor. In addition to the usual decomposition into elastic and plastic parts, the plastic part is decomposed further into a part contributing to the rotational hardening and a remainder part. The former part leads to a back stress ratio tensor related to the rotational hardening via a hyperelastic‐type hardening rule. The constitutive theory is thereby formulated on proper intermediate configurations entirely in terms of deformation‐like tensorial variables possessing invariance property, without resort to any objective rates of stress or stress‐like variables. Combining the Cam‐clay plasticity with the concept of subloading surface, a class of unconventional plasticity, enables the model to be capable of reproducing complex hardening/softening accompanied by volumetric contractive/dilative responses. Basic characteristics and predictive capability of the proposed model, as well as the accuracy of the developed numerical scheme, are verified through several numerical examples including monotonic and cyclic loadings. |
| Author | Higuchi, Masaki Hashiguchi, Koichi Machishima, Tomohiro Sato, Kiyoshi Sasaki, Tomohiro Iguchi, Takuya Yamakawa, Yuki Kawai, Tadashi |
| Author_xml | – sequence: 1 givenname: Yuki orcidid: 0000-0002-8519-2886 surname: Yamakawa fullname: Yamakawa, Yuki email: yuki.yamakawa.c7@tohoku.ac.jp organization: Tohoku University – sequence: 2 givenname: Koichi orcidid: 0000-0003-1830-7767 surname: Hashiguchi fullname: Hashiguchi, Koichi organization: Kyushu University – sequence: 3 givenname: Tomohiro surname: Sasaki fullname: Sasaki, Tomohiro organization: Obayashi Corporation – sequence: 4 givenname: Masaki surname: Higuchi fullname: Higuchi, Masaki organization: Obayashi Corporation – sequence: 5 givenname: Kiyoshi surname: Sato fullname: Sato, Kiyoshi organization: Obayashi Corporation – sequence: 6 givenname: Tadashi surname: Kawai fullname: Kawai, Tadashi organization: Tohoku University – sequence: 7 givenname: Tomohiro surname: Machishima fullname: Machishima, Tomohiro organization: Tohoku University – sequence: 8 givenname: Takuya surname: Iguchi fullname: Iguchi, Takuya organization: Tohoku University |
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| CitedBy_id | crossref_primary_10_1002_nag_3289 crossref_primary_10_1061_IJGNAI_GMENG_10709 crossref_primary_10_1007_s00707_025_04339_0 crossref_primary_10_1007_s11831_022_09880_y crossref_primary_10_1016_j_cma_2025_118038 crossref_primary_10_1016_j_cma_2023_116059 crossref_primary_10_1016_j_cma_2025_118164 crossref_primary_10_1038_s41598_025_08151_7 crossref_primary_10_1007_s11831_023_10022_1 crossref_primary_10_1016_j_sandf_2024_101532 crossref_primary_10_1038_s41598_022_26624_x crossref_primary_10_1016_j_compgeo_2021_104600 |
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| Notes | Present Address Current affiliation of T. Machishima: JIP Techno Science Corporation, Chiyoda‐ku, Tokyo, Japan. Current affiliation of T. Iguchi: Engineering Technology Division, Harumi Toriton Office, JSOL Corporation, Chuo‐ku, Tokyo, Japan. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
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| SubjectTerms | Algorithms Anisotropy cam‐clay plasticity Clay Constitutive models Decomposition Deformation Elastic deformation Elastoplasticity finite strain Geomaterials Hardening Mathematical models Plastic properties Plasticity Prototypes return‐mapping algorithm rotational hardening Strain Stress ratio subloading surface concept Tensors |
| Title | Anisotropic subloading surface Cam‐clay plasticity model with rotational hardening: Deformation gradient‐based formulation for finite strain |
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