论文标题

评估金属泡沫的J积分测试

An assessment of the J-integral test for a metallic foam

论文作者

Tankasala, H. C., Li, T., Seiler, P. E., Deshpande, V. S., Fleck, N. A.

论文摘要

通过将有限元(FE)仿真与实验相结合,对J积分测试程序进行了J积分测试程序,以对开铝合金泡沫的初始裂纹生长进行评估。在实验上发现,随机失败的支撑杆区域在主要裂纹尖端前发展,并且大小与塑料区域相当。因此,在主裂纹尖端启动裂纹生长时,没有裂纹尖端J场。这意味着,尽管样品大小符合J的有效性标准,但测量的J_IC值和J与裂纹扩展DA曲线不能被视为材料特性。韧性测试是在单边弯曲的弯曲试样上进行的,并通过数字图像相关和X射线计算机断层扫描来测量裂纹扩展。泡沫的裂纹生长抗性与两个不同的塑料耗散区域有关:(i)从裂纹尖端发出的块状塑料区域(包含一个随机失败的支撑杆),以及(ii)前进的裂纹尖端后面的裂纹桥梁。对于观察到的大规模桥梁的情况,探索了凝聚区模型预测断裂反应的适用性。为此,通过通过可压缩的,可压缩的弹塑性硬化固体替换开放电池金属泡沫的离散晶格来进行FE模拟,而泡沫中的断裂过程区则由粘性区域表示,其特征在于是由拉伸牵引力与分离法。对凝聚区模型与实验观测的详细比较表明,可以使用一组过程区参数捕获负载与位移响应,但不能捕获骨折过程区域的细节。

An assessment is made of the J-integral test procedure for initial crack growth in an open-cell aluminium alloy foam by combining finite element (FE) simulations with experiment. It is found experimentally that a zone of randomly failed struts develops ahead of the primary crack tip, and is comparable in size to that of the plastic zone. Hence, a crack tip J-field is absent at the initiation of crack growth from the primary crack tip. This implies that the measured J_IC value and the J versus crack extension Da curve cannot be treated as material properties despite the fact that the specimen size meets the usual criteria for J validity. The toughness tests were performed on a single-edge notched bend specimen, and crack extension was measured by the direct current potential drop method, by digital image correlation and by X-ray computed tomography. The crack growth resistance of the foam is associated with two distinct zones of plastic dissipation: (i) a bulk plastic zone emanating from the crack tip (containing a cluster of randomly failed struts), and (ii) a crack bridging zone behind the advancing crack tip. The applicability of a cohesive zone model to predict the fracture response is explored for the observed case of large scale bridging. To do so, FE simulations are performed by replacing the discrete lattice of the open-cell metallic foam by a compressible, elastic-plastic hardening solid while the fracture process zone in the foam is represented by a cohesive zone, as characterised by a tensile traction versus separation law. A detailed comparison of the cohesive zone model with experimental observations reveals that it is possible to capture the load versus displacement response but not the details of the fracture process zone using a single set of process zone parameters.

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