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Non-coaxial plasticity of similar weakly cemented soft rock under directional shear stress path.
Liu, Jiashun; Zheng, Zhiyong; Zhou, Hui; Zhu, Kaixin; Wang, Yang; Zhou, Ni; Wang, Siyu; Sun, Mengyao.
Affiliation
  • Liu J; School of Civil Engineering, Liaoning Technical University, Fuxin, 123000, People's Republic of China. liujiashun000@163.com.
  • Zheng Z; State Key Laboratory of Geomechanics and Geotechnical Engineering, Institute of Rock and Soil Mechanics, Chinese Academy of Sciences, Wuhan, 430071, China. liujiashun000@163.com.
  • Zhou H; School of Mechanics and Civil Engineering, China University of Mining & Technology, Beijing, 100083, People's Republic of China. liujiashun000@163.com.
  • Zhu K; School of Civil Engineering, Liaoning Technical University, Fuxin, 123000, People's Republic of China.
  • Wang Y; State Key Laboratory of Geomechanics and Geotechnical Engineering, Institute of Rock and Soil Mechanics, Chinese Academy of Sciences, Wuhan, 430071, China.
  • Zhou N; School of Civil Engineering, Liaoning Technical University, Fuxin, 123000, People's Republic of China.
  • Wang S; School of Civil Engineering, Chongqing University, Chongqing, 400044, People's Republic of China.
  • Sun M; School of Civil Engineering, Liaoning Technical University, Fuxin, 123000, People's Republic of China.
Sci Rep ; 14(1): 21108, 2024 Sep 10.
Article de En | MEDLINE | ID: mdl-39256416
ABSTRACT
The plastic flow behavior of soft rock exhibits non-coaxial features under complex stress paths, while traditional plasticity theories are ill-equipped to adequately represent this, which leads to the mechanism of soft rock failure still unclear. To investigate the evolution law of strain increments and non-coaxial characteristics of weakly cemented soft rock, the directional shear tests are conducted using the hollow cylinder apparatus (HCA). The results show that non-coaxiality does not occur when α is distinct from 0° or 90°. The oscillation of the non-coaxial angle is significantly more variable in soft rock experiencing combined tension-torsion (45° < α < 90°), as opposed to those under the influence of combined compression-torsion (0° < α < 45°). The non-coaxiality swiftly dissipates when the sample is approaching the failure state. The stress rate is decomposed into stress magnitude and direction to describe non-coaxial features of plastic strain. And a new method for non-coaxial stress rate is proposed which can express the plastic strain increment directions. The spherical interpolation coefficient method is utilized to describe the continuous change in non-coaxial plastic flow direction between tangential and normal directions of the yield surface. The non-coaxial parameter (Δ) is introduced to quantify the non-coaxial characteristics of soft rock and its validity is confirmed through test results. This method effectively captures the principal stress direction influence on non-coaxial behavior of soft rock and have significance for rock mechanics.
Mots clés

Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Langue: En Journal: Sci Rep Année: 2024 Type de document: Article Pays de publication: Royaume-Uni

Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Langue: En Journal: Sci Rep Année: 2024 Type de document: Article Pays de publication: Royaume-Uni