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An implementation of the phase-field model based on coupled thermomechanical finite element solvers for large-strain twinning, explicit dynamic fracture and the classical Stefan problem

机译:基于耦合热机械有限元求解器的大应变孪晶,显式动态骨折与古典斯特凡问题的耦合热机械有限元求解器的实现

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摘要

The implementation of a phase-field model in finite elements usually requires significant expertise and involves the development of a user element with additional degrees of freedom. An alternative implementation of the phase-field model within a thermo-mechanical finite element simulation package was presented in (Cho et al 2012 Int. J. Solids Struct. 49 1973-1992), where the phase-field variable is treated as the temperature degree of freedom. However, this approach has only been used for small strain phase-field modelling of martensitic transformations and quasistatic phase-field modelling of fracture. In this work, we present a phase-field finite element implementation via the temperature degree of freedom for several additional cases from the literature: (i) the large-strain phase-field description of deformation twinning presented in (Clayton and Knap 2011 Physica D 240 841-858), (ii) phase-field description of brittle fracture with inertial effects based on the theory from (Molnar and Gravouil 2017, Finite Elem. Anal. Des. 130 27-38) and (Miehe et al 2010 Int. J. Numer. Methods Eng. 83 1273-1311) and (iii) the classical Stefan problem of solidification presented in (Mackenzie and Robertson 2002 J. Comput. Phys. 181 526-544). The last problem involves the temperature and phase-field variables as unknowns.
机译:在有限元中实现相位场模型通常需要具有重要专业知识,并且涉及具有额外的自由度的用户元素。介绍了热机械有限元模拟包中的阶段模型的替代实现(Cho等,2012 int。j.固体结构。49 1973-1992),其中相场变量被视为温度自由度。然而,这种方法仅用于马氏体转化的小应变相位模型和骨折的Quasistatic相位模型。在这项工作中,我们通过文献的几种额外情况的额外案例的温度自由度提出了一个相场有限元实现:(i)(i)呈现的变形孪晶的大应变相场描述(克莱顿和Knap 2011 Physica d 240 841-858),(ii)基于(Molnar和Gravouil 2017,有限的ELEM的理论,基于理论的易分骨折的相场描述脆性骨折。肛门。DES。130 27-38)和(Miehe等,2010 int。 J.数。方法ENG。83 1273-1311)和(iii)播放凝固的经典STEFAN问题(Mackenzie和Robertson 2002 J. Comput。物理。181 526-544)。最后一个问题涉及温度和相位场变量作为未知。

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