薄铝材料韧性裂纹扩展的三维有限元模拟

A. Gullerud, R. H. Dodds, R. Hampton, D. Dawicke
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引用次数: 6

摘要

这项工作描述了一个三维模型的开发和验证,以预测薄韧性铝合金中稳定的I型裂纹扩展。该模型扩展了裂纹尖端张开角(CTOA)方法的标准二维形式,该方法通过获得裂纹尖端的临界角来确定裂纹扩展。当CTOA达到临界值时,沿电流三维裂缝前缘的所有节点同时释放,从而使裂缝以自相似方式扩展。CTOA的评估发生在裂纹尖端后的指定距离处;这将CTOA评估与网格细化解耦。基于ctoa的模型还包括自适应负载控制策略,以最小化离散负载增量对增长响应的影响。为了评估所述方法的有效性,本文描述了一项验证研究,该研究使用了NASA-Langley测试的2.3 mm厚Al 2024-T3试件的载荷裂纹扩展数据。测试基体包括C(T)和M(T)试样,具有不同的宽度(50至600 mm)、a/W比和抑制面外弯曲的约束水平。通过对比实验得出的载荷-裂纹扩展曲线和受约束的150-mm C(T)试样的分析,得出了校准后的临界CTOA值为5.1°。使用校准的CTOA值对有约束和无约束试样进行分析,提供了与实验值良好一致的峰值负荷预测。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
3-D Finite Element Modeling of Ductile Crack Growth in Thin Aluminum Materials
This work describes the development and verification of a 3-D model to predict stable, Mode I crack growth in thin, ductile aluminum alloys. The model extends the standard 2-D form of the crack tip opening angle (CTOA) methodology, which determines crack extension based on obtaining a critical angle at the crack tip. When the CTOA reaches the critical value, all the nodes along the current, 3-D crack front are released simultaneously, thereby growing the crack in a self-similar manner. Evaluation of the CTOA occurs at a specified distance behind the crack tip; this decouples CTOA evaluation from mesh refinement. The CTOA-based model also includes adaptive load control strategies to minimize the effects of discrete load increments on the growth response. To evaluate the effectiveness of the described approach, this work describes a validation study using load-crack extension data from 2.3-mm-thick Al 2024-T3 specimens tested at NASA-Langley. The test matrix includes C(T) and M(T) specimens, with varying widths (50 to 600 mm), a/W ratios, and levels of constraint to suppress out-of-plane bending. Comparisons of load-crack extension curves from experiments and analyses of a constrained 150-mm C(T) specimen provide a calibrated critical CTOA value of 5.1°. Analyses using the calibrated CTOA value for constrained and unconstrained specimens provide predictions of peak load in good agreement with the experimental values.
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