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Cavity Growth from Crack-like Defects in Soft Materials

机译:软材料中裂纹状缺陷引起的空洞生长

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Failure of pressure sensitive adhesives are often preceded by the growth of interfacial or internal voids. The growth of these voids create a highly fibrillated micro-structure which is desirable since it enhances the toughness of the adhesive. There is a large literature on how cavities deform in a rubbery material, for example, see and the references within. The majority of these works focus on the growth of spherical or cylindrical cavities subjected to internal or external pressure since the problems can be reduced to a one dimensional one and therefore amendable to exact analysis. A well known result is that a spherical cavity in an infinite media consisting of an ideal rubber (i.e., a Neohookean material) will grow without bound when the applied hydrostatic tension P reaches a critical value of 2.5 μ, where μ is the infinitesimal shear modulus. However, this result seems to be at odd with experiments which showed that the critical hydrostatic tension depends on the cavity size. Specifically, smaller cavities require higher tension for rapid growth, whereas large cavities fail at a stress of approximately 2.5 μ. Since the Neohookean model typically underestimates the amount of strain hardening, one may argue that the higher critical stress required for rapid growth is due to hardening. This can not be the case for the following reason: since the cavity radius is the only length scale in the problem, the critical hydrostatic tension for cavity stability is independent of cavity size. In other words, strain hardening will increase the critical tension irrespective of cavity size. Therefore, it alone cannot explain why rapid growth of smaller cavities requires higher negative pressure. Gent suggested that the rapid growth of small cavities is not a deformation controlled process but a fracture process. Specifically, surface energy provides an additional restraint upon expansion, which becomes significant for small cavities with relative high surface areas. He started with the hypothesis that cavities grow from initial crack like defects. Gent's insight can be quantified by dimensional analysis: the energy release rate of a circular crack in an infinite medium must necessarily scales with the initial crack radius. Therefore, smaller defects have a smaller energy release rate for the same applied load. However, Griffith's fracture criterion dictates that crack growth occurs when the energy release rate reaches the fracture toughness G_c, which is a material constant. This explains the size dependence. In Gent's analysis, various approximations are made in order to obtain closed form expression for the energy release rate. In this work, we evaluate the energy release rate free of these approximations.
机译:压敏粘合剂的失效通常是在界面或内部空隙的增长之前。这些空隙的生长产生了高度原纤化的微结构,这是所希望的,因为它增强了粘合剂的韧性。关于空腔如何在橡胶质材料中变形的文献很多,例如,请参见及其中的参考文献。这些问题大部分集中在承受内部或外部压力的球形或圆柱形空腔的生长上,因为这些问题可以减少到一维,因此可以进行精确分析。一个众所周知的结果是,当所施加的静水压力P达到2.5μ的临界值时,由理想橡胶(即,新胡克材料)组成的无限介质中的球腔将无限制地生长,其中μ是无穷小的剪切模量。但是,该结果似乎与表明临界静水压力取决于腔尺寸的实验相矛盾。具体而言,较小的空腔需要较高的张力才能快速生长,而较大的空腔会在约2.5μ的应力下失效。由于Neohookean模型通常低估了应变硬化的数量,因此有人可能会认为,快速生长所需的更高的临界应力是硬化造成的。由于以下原因,情况并非如此:由于空腔半径是问题中唯一的长度尺度,因此用于空腔稳定性的临界静水张力与空腔尺寸无关。换句话说,无论腔尺寸如何,应变硬化都会增加临界张力。因此,仅凭这一点不能解释为什么小腔的快速生长需要更高的负压。根特指出,小腔的快速生长不是变形控制过程,而是破裂过程。具体地,表面能对膨胀提供了额外的限制,这对于具有相对高表面积的小腔体而言变得尤为重要。他从这样的假说开始,即空洞会从最初的裂纹(如缺陷)中生长出来。根特的洞察力可以通过尺寸分析来量化:无限介质中圆形裂纹的能量释放率必须与初始裂纹半径成比例。因此,对于相同的施加负载,较小的缺陷具有较小的能量释放率。但是,格里菲斯的断裂判据规定,当能量释放速率达到材料常数的断裂韧性G_c时,裂纹就会发生。这解释了尺寸依赖性。在Gent的分析中,为了获得能量释放速率的闭式表达式,进行了各种近似计算。在这项工作中,我们评估了没有这些近似值的能量释放率。

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