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Finite element analysis of the Longitudinal Half Fixed Beam method for mode Ⅲ characterization

机译:纵向半固定梁法表征Ⅲ型的有限元分析。

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In this work, the Longitudinal Half Fixed Beam test (LHFB) for mode III characterization is analysed by means of Finite Element Analysis (FEA) and optical microscopy. The obtained results were compared with experimental data and analytical formulations obtained in previous works. The objective of this study is to determine the energy distribution across the crack front and to understand the micromechanics that give rise to the delamination failure in unidirectional carbon/epoxy composites.It was found that for samples with long initial crack lengths (i.e. a(0)=30 mm), pure mode III takes place in the central part of the delamination front. Nevertheless, these samples present a significant contribution of mode II at the edges of the specimen. As a(0) decreases, pure mode III increases in extension across the delamination front and mode II decreases at the sample edges. When the initial crack length (a(0)) is quite small, the sample presents pure mode III practically on the entire length of the crack front. Nevertheless, when the initial crack is very small, the applied force exercises a local influence on the tip of the crack at the edge of the sample and mode III distribution loses its uniformity across the crack front.The concordance between the analytical results and the numerical results obtained by the Finite Element Method (FEM) was variable depending on the length of the crack and if the comparison was made with G(III) or G(T) as reference.Intralaminar cracks at approximately 45 degrees with respect to the midplane were observed in planes perpendicular to the direction of delamination propagation (planes perpendicular to the fibre direction). Other authors also found this type of intralaminar cracks in other mode III test configurations.
机译:在这项工作中,通过有限元分析(FEA)和光学显微镜分析了用于模式III表征的纵向半固定光束测试(LHFB)。将获得的结果与先前工作中获得的实验数据和分析公式进行比较。这项研究的目的是确定整个裂纹前沿的能量分布,并了解引起单向碳/环氧树脂复合材料分层失败的微观力学。发现对于初始裂纹长度较长的样品(即a(0 )= 30 mm),纯模式III发生在分层前部的中央。然而,这些样品在样品的边缘呈现出模式II的重要贡献。随着a(0)的减小,纯模式III在整个脱层前沿的延伸量增加,而模式II在样品边缘减小。当初始裂纹长度(a(0))很小时,样品实际上在裂纹前沿的整个长度上呈现纯模式III。然而,当初始裂纹非常小时,施加的力会对样品边缘处的裂纹尖端产生局部影响,并且III型分布在整个裂纹前沿都失去了均匀性。分析结果与数值之间的一致性有限元方法(FEM)获得的结果因裂纹的长度以及是否以G(III)或G(T)为参考进行比较而变化。在垂直于分层传播方向的平面(垂直于纤维方向的平面)中观察到。其他作者也在其他III型测试配置中发现了这种类型的层内裂纹。

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