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The Energetic Approach of Elastoplastic Fracture MechanicsApplied to the Problem of Unloading

机译:弹塑性断裂力学的能量学方法在卸荷问题中的应用

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In this paper, a cleavage parameter G_p, based on energetic considerations, is defined to characterise crack initiation in arnbrittle elastoplastic medium, and discussed in the context of the famous ? Rice’s paradox ?. We start from Francfort-Marigornelastic fracture theory, based on a minimum energy principle, which generalises Griffith’s theory. In this theory, the energyrndepends on the displacement field as well as the geometrical crack surface. The cleavage parameter is defined and determinedrnas the value of the discrete gradient of an incremental elastoplastic potential. For that purpose, it is necessary to compute twornsolutions : the solution of the problem with the initial crack, and the solution of the problem after a finite crack propagationrn?Δ1? taking into account the local unloading due to this propagation.rnThis parameter G_p is applied to the analysis of a centred cracked plate submitted to a loading first increasing (to open therncrack) and then decreasing (to close the crack). The constitutive law is elastoplastic with an isotropic hardening. A very finernmesh is used in the area of the crack tip, and a parametric analysis is realised to study the effect of this mesh and of the Δ1rnpropagation. Therefore an important result is obtained : the G_p parameter is neither mesh dependent, nor Δ1 dependent.rnDuring the unloading, G_p decreases very quickly from a maximum value to zero, and we can affirm then that no propagationrnis possible, although the value of the J-integral is non zero.rnThe G_p parameter can be related to the G~Δ parameter proposed by Kfouri & Miller in 1976. As suggested by Rice, thernvalue of this parameter seems to vanish to zero with the length Δ1 of the finite crack propagation. It means that, for anrnelastoplastic media, there would be no energy available for crack propagation. We will show that we would have obtained thernsame result for the G_p parameter with a standard mesh, but also that, if the mesh is sufficiently refined, the final result is notrnzero. Therefore, this G_p parameter can be used as a cleavage fracture parameter.
机译:在本文中,基于能量的考虑,定义了劈裂参数G_p来表征arnbrittle弹塑性介质中的裂纹萌生,并在著名的?赖斯的悖论?我们从基于最小能量原理的Francfort-Marigornelastic断裂理论开始,该理论推广了Griffith的理论。在这个理论中,能量取决于位移场以及几何裂纹表面。定义裂解参数并确定其为增量弹塑性势的离散梯度的值。为此,有必要计算两个解:具有初始裂纹的问题的解和有限裂纹扩展后的问题的解。考虑到由于这种传播而引起的局部卸荷。该参数G_p用于分析先加载后居中的开裂板,先增大(打开裂缝),然后减小(关闭裂缝)。本构定律是具有各向同性硬化的弹塑性。在裂纹尖端区域使用了非常精细的网格,并进行了参数分析以研究该网格和Δ1rn传播的影响。因此,获得了重要的结果:G_p参数既不依赖于网格也不依赖于Δ1.rn在卸载过程中,G_p从最大值迅速减小到零,因此可以确定,尽管J的值-integral非零。rn G_p参数可以与Kfouri&Miller在1976年提出的G〜Δ参数相关。正如莱斯所建议的那样,该参数的值似乎随着有限裂纹扩展的长度Δ1消失为零。这意味着,对于弹塑性介质,将没有能量可用于裂纹扩展。我们将显示,使用标准网格将获得与G_p参数相同的结果,而且,如果网格得到了充分细化,则最终结果将不为零。因此,该G_p参数可以用作劈裂断裂参数。

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