(1. State Key Laboratory of Geomechanics and Geotechnical Engineering,Institute of Rock and Soil Mechanics,Chinese Academy of Sciences,Wuhan,Hubei 430071,China;2. Geotechnical and Structural Engineering Research Center,Shandong University,Jinan,Shandong 250061,China;3. Belgian Nuclear Research Centre,Mol 2400,Belgium)
Abstract:The definitions of overconsolidation state parameter and structural property state parameter is further perfected firstly and a more popular derivation of this model is offered. Then the numerical implementation is completed based on the semi-implicit algorithm and the constitutive subroutine is compiled by using UMAT in ABAQUS for the improved model considering the cohesion. Finally,the complicated mechanical properties of the overconsolidated and undisturbed soil are simulated under different conditions and various loading types. The result implies that the model owns excellent simulation capabilities and the UMAT subroutine ensures sufficient accuracy and stability. Therefore,the key step to apply this constitutive model into engineering practice has been successfully accomplished.
[1] 姚仰平,侯 伟. 土的基本力学特性及其弹塑性描述[J]. 岩土力学,2009,30(10):2 881–2 901.(YAO Yangping,HOU Wei. Basic mechanical behavior of soils and their elastoplastic modeling[J]. Rock and Soil Mechanics,2009,30(10):2 881–2 901.(in Chinese))
[2] 张 锋. 计算土力学[M]. 北京:人民交通出版社,2007:31. (ZHANG Feng. Computational soil mechanics[M]. Beijing:China Communications Press,2007:31.(in Chinese))
[3] HASHIGUCHI K. Plastic constitutive equations of granular materials[C]// Proceedings of US–Japan Seminar Continuum Mechanics and Statistical Approaches in the Mechanics of Granular Materials. Sendai:JSSMFE,1978:321–329.
[4] HASHIGUCHI K. Constitutive equations of elastoplastic materials with elastoplastic transition[J]. Journal of Applied Mechanics,1980,47(2):266–272.
[5] HASHIGUCHI K. Subloading surface model in unconventional plasticity[J]. International Journal of Solids and Structures,1989,25(8):917–945.
[6] NAKAI T,HINOKIO M. A simple elastoplastic model for normally and over consolidated soils with unified material parameters[J]. Soils and Foundations,2004,44(2):53–70.
[7] 孔 亮,花丽坤,王燕昌. 次加载面理论及其在土体循环塑性模型中的应用[J]. 宁夏大学学报:自然科学版,2003,24(1):50–56.(KONG Liang,HUA Likun,WANG Yanchang. The subloading surface theory and its application to the cyclic plastic model for soil[J]. Journal of Ningxia University:Natural Science,2003,24(1):50–56.(in Chinese))
[8] 孔 亮,郑颖人,姚仰平. 基于广义塑性力学的土体次加载面循环塑性模型(I):理论与模型[J]. 岩土力学,2003,24(2):141–145.(KONG Liang,ZHENG Yingren,YAO Yangping. Subloading surface cyclic plastic model for soil based on generalized plasticity(I):theory and model[J]. Rock and Soil Mechanics,2003,24(2):141–145.(in Chinese))
[9] 詹云刚,袁凡凡,栾茂田. 基于次加载面理论改进的ALPHA模型及其数值实施[J]. 岩土力学,2010,31(2):407–415.(ZHAN Yungang,YUAN Fanfan,LUAN Maotian. A modified ALPHA model based on subloading surface theory and its numerical implementation[J]. Rock and Soil Mechanics,2010,31(2):407–415.(in Chinese))
[10] 黄 雨,周子舟. 下负荷面剑桥模型在ABAQUS中的开发实现[J].岩土工程学报,2010,32(1):115–119.(HUANG Yu,ZHOU Zizhou. Numerical implementation for subloading Cam-Clay model in ABAQUS[J]. Chinese Journal of Geotechnical Engineering,2010,32(1):115–119. (in Chinese))
[11] ASAOKA A,NAKANO M,NODA T,et al. Delayed compression/ consolidation of naturally clay due to degradation of soil structure[J]. Soils and Foundations,2000,40(3):75–85.
[12] ASAOKA A,NAKANO M,NODA T. Superloading yield surface concept for highly structured soil behavior[J]. Soils and Foundations,2000,40(2):99–110.
[13] 袁克阔,陈卫忠,于洪丹,等. 考虑拉压不等效应的修正剑桥模型及数值实施[J]. 岩石力学与工程学报,2012,31(8):1 574–1 579. (YUAN Kekuo,CHEN Weizhong,YU Hongdan,et al. Modified Cam-Clay model considering cohesion and S-D effect and its numerical implementation[J]. Chinese Journal of Rock Mechanics and Engineering,2012,31(8):1 574–1 579.(in Chinese))
[14] ASAOKA A,NODA T,YAMADA E,et al. An elastoplastic description of two distinct volume change mechanisms of soils[J]. Soils and Foundations,2002,42(5):47–57.
[15] 康国政. 非弹性本构理论及其有限元实现[M]. 成都:西南交通大学出版社,2010:78–100.(KANG Guozheng. Inelastic constitutive theory and its finite element implementation[M]. Chengdu:Southwest Jiaotong University Press,2010:78–100.(in Chinese))
[16] BORJA R I,LEE S R. Cam-Clay plasticity,part I:implicit integration of elastoplastic constitutive relations[J]. Computer Methods in Applied Mechanics and Engineering,1990,78(1):49–72.
[17] BERNIER F,VAN CAUTEREN L. Instrumentation programme near the face of an advancing tunnel in Boom Clay[C]// The Geotechnics of Hard Soils-Soft Rocks. Rotterdam:Balkema,1998:953–959.
[18] FRANÇOIS B,LALOUI L,LAURENT C. Thermo-hydro-mechanical simulation of ATLAS in situ large scale test in Boom Clay[J]. Computers and Geotechnics,2009,36(4):626–640.
[19] 于洪丹. Boom Clay渗流–应力耦合长期力学特性研究[博士学位论文][D]. 武汉:中国科学院武汉岩土力学研究所,2010.(YU Hongdan. Study on long-term hydro-mechanical coupled behavior of Belgium Boom Clay[Ph. D. Thesis][D]. Wuhan:Institute of Rock and Soil Mechanics,Chinese Academy of Sciences,2010.(in Chinese))