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Initiation of cracks with cohesive force models: a variational approach

机译:凝聚力模型引发的裂纹:一种变分方法

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In the spirit of the variational approach of Fracture Mechanics initiated in [Del Piero, G., 1997. One-dimensional ductile-brittle transition, yielding and structured deformations. In: P. Argoul, M. Fremond (Eds.), Proceedings of IUTAM Symposium "Variations de domaines et frontieres libres en mecanique", Paris, 1997, Kluwer Academic] and [Francfort, G.A., Marigo, J.-J., 1998. Revisiting brittle fracture as an energy minimization problem. J. Mech. Phys. Solids 46 (8), 1319-1342], we define the loss of stability of the elastic response of the body as the criterion of initiation of cracks. The result is very sensitive to the choice of the surface energy density. On one hand, if we adopt the Griffith assumption, then the elastic state is generally always stable. On the other hand, in the case of a surface energy of the Barenblatt type, i.e. a surface energy depending non-trivially on the jump of the displacement and inducing cohesive forces, the elastic response remains stable only if the stress field does not reach a critical value. In the full three-dimensional context of an isotropic material, we prove that this yield stress criterion is equivalent to a maximal traction criterion and a maximal shear criterion if the surface energy density is Frechet differentiable at the origin. When the surface energy density is only Gateaux differentiable, we obtain a yield stress criterion based on an intrinsic curve in the Mohr diagram. In any case, the domain of the admissible stress tensors is convex, unbounded in the direction of the hydrostatic pressures and depends only on the extreme eigenvalues of the stress tensor.
机译:本着[Dela Piero,G.,1997.一维延性-脆性转变,屈服和结构变形的断裂力学的变化方法的精神。在:P。Argoul,M。Fremond(编辑),IUTAM研讨会论文集《机械领域的变化与边界》,巴黎,1997年,Kluwer Academic]和[Francfort,GA,Marigo,J.-J., 1998年。重新探讨脆性断裂作为能量最小化的问题。 J.机甲物理固体[46](8),1319-1342],我们将主体弹性响应的稳定性损失定义为裂纹萌生的标准。结果对表面能密度的选择非常敏感。一方面,如果采用格里菲斯假设,那么弹性状态通常总是稳定的。另一方面,在Barenblatt类型的表面能(即表面能非常不依赖于位移跃变和产生内聚力)的情况下,只有在应力场未达到a时,弹性响应才能保持稳定。临界值。在各向同性材料的完整三维环境中,我们证明了这种屈服应力准则等效于最大牵引力准则和最大剪切准则,如果表面能密度在原点处是弗雷歇特可微的。当表面能密度只有Gateaux可微时,我们基于Mohr图中的本征曲线获得屈服应力准则。在任何情况下,容许应力张量的域都是凸的,在静水压力方向上是无界的,并且仅取决于应力张量的极限特征值。

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