One of the assumptions of Linear Elastic Fracture Mechanics is that the crack faces are traction-free or, at most, loaded by bounded tractions. The standard Irwin's crack closure integral, widely used for the computation of the Energy Release Rate, also relies upon this assumption. However, there are practical situations where the load acting on the crack boundaries is singular. This is the case, for instance, in hydraulic fracturing, where the fluid inside the crack exerts singular tangential tractions at its front. Another example of unbounded tractions is the case of a rigid line inclusion (anticrack) embedded into an elastic body. In such situations, the classical Irwin's crack closure integral fails to provide the correct value of the Energy Release Rate. In this paper, we address the effects occurring when square-root singular tractions act at the boundary of a line defect in an elastic solid and provide a generalisation of Irwin's crack closure integral. The latter yields the correct Energy Release Rate and allows broad applications, including, among others, hydraulic fracturing, soft materials containing stiff inclusions, rigid inclusions, shear bands and cracks characterized by the Gurtin-Murdoch surface stress elasticity. We present the results in the most general form, where six Stress Intensity Factors are present: three of them are classical SIFs corresponding to the modes I-II-III and computed under the assumption of homogeneous boundary conditions at the defect surfaces, while the other three SIFs are associated with singular admissible tractions (those that lead to a finite ERR value). It is demonstrated that this approach resolves an ambiguity in using the same SIF's terminology in the cases of open cracks and rigid inclusions, among other benefits.
翻译:线性 Elastic Fracture Mechanic 的假设之一是,裂纹面部是没有牵引的,或者最多是被绑定的牵引。标准的Irwin 的裂缝封闭部分是用来计算能源释放率的,也依据这一假设。然而,有些实际情况是,裂缝边界上产生的负负负是奇特的。例如,液压裂变就是这种情况,裂缝内流的液压在其前端产生奇异的正正正正正正正的分流。另一个非正向偏斜的角是嵌入一个弹性的地平面体。在这种情况下,古典Irwin的裂缝封闭部分无法提供能源释放率的正确值。在本文中,当平面的单向线缺陷的边界移动时,当Irwin 的液压断裂变时, 后者产生正确的能源释放率,并允许广泛的应用,包括,在其它情况下, 液压的三直流、软的直径直径直的直截面的内置部分, 当我们用直径直径的平面的平面的平面的内压的内压的内压, 直径的内压的内压的内压的内压的内压, 。