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Implicit and explicit integration schemes in the anisotropic bounding surface plasticity model for cyclic behaviours of saturated clay
Institution:1. School of Civil Engineering, Tianjin University, Tianjin 300072, China;2. Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China;1. University of New South Wales, Canberra, Australia;2. School of Natural and Built Environments & Barbara Hardy Institute, University of South Australia, Australia;1. LTDS, Université de Lyon, UMR CNRS 5513, École Centrale de Lyon, Écully, France;2. Univ. Grenoble Alpes, 3SR, F-38000 Grenoble, France;3. CNRS, 3SR, F-38000 Grenoble, France;1. Univ Lille Nord de France, F-59000 Lille, France;2. Université Lille 1 Sciences et Technologies, Laboratoire de Mécanique de Lille (LML), UMR CNRS 8107, F-59650 Villeneuve d?Ascq, France;3. Université Lille 1 Sciences et Technologies, Laboratoire de Génie Civil et géo-Environnement (LGCgE), EA 4515, F-59650 Villeneuve d?Ascq, France;4. Université Lille 1 Sciences et Technologies, Unité Matériaux Et Transformations (UMET), UMR CNRS 8207, F-59650 Villeneuve d?Ascq, France;1. Université Paris-Est, Laboratoire Navier (UMR 8205), CNRS, ENPC, IFSTTAR, F-77455 Marne-la-Vallée, France;2. Department Argenco, University of Liège, Sart Tilman B52/3, Chemin des Chevreuils, 1, B-4000 Liege, Belgium;3. European Underground Research Infrastructure for Disposal of Nuclear Waste in Clay Environment, ESV EURIDICE GIE, Mol, Belgium;1. School of Transportation Science and Engineering, Beihang University, Beijing 100191, China;2. School of Civil Engineering, Tsinghua University, Beijing 100084, China
Abstract:Two integration algorithms, namely the implicit return mapping and explicit sub-stepping schemes, are adopted in the anisotropic bounding surface plasticity model for cyclic behaviours of saturated clay and are implemented into finite element code. The model is a representative of a series of bounding surface models that have typical characteristics, including isotropic and kinematic hardening rules and a rotational bounding surface to capture complex but important cyclic behaviours of soils, such as cyclic shakedown and degradation. However, there is no explicit current yield surface in the model to which the conventional implicit algorithm returns the stress state back or the sub-stepping integration corrects the drift of the stress state. Hence, necessary modifications have been made for both of the integration schemes. First, the image stress point is mapped or corrected to the bounding surface instead of mapping back or correcting the stress state to the yield surface. Second, the unloading–loading criterion is checked to determine the image stress point rather than checking the yield criterion after giving the trial stress state in a conventional way. Comparative studies on the accuracy, stability and efficiency of the two integration schemes are conducted not only at the element level but also in solving boundary value problems of monotonic and cyclic bearing behaviours of rigid footings on saturated clay. For smaller strain increments, there is no significant difference in the accuracy between the two integration schemes, but the explicit integration shows a higher efficiency and accuracy. For relatively larger increments, the implicit return mapping algorithm presents good accuracy and more robustness, while the sub-stepping algorithm shows deteriorating accuracy and suffers the convergence problem. With the tolerance used in the present model, the bearing capacity of the rigid footing predicted by the return mapping algorithm is closer to the available analytical and numerical solutions, while the bearing capacity predicted by the sub-stepping algorithm shows a marginal increase.
Keywords:Bounding surface plasticity model  Implicit integration  Explicit integration  Cyclic behaviour  Saturated clay
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