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Eigenstrain modelling of residual stress generated by arrays of Laser Shock Peeing shots and determination of the complete stress field using limited strain measurements

机译:激光冲击射击阵列产生的残余应力的本征应变模型和使用有限应变测量确定完整应力场

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摘要

This paper presents a hybrid explicit finite element (FE) /eigenstrain model for predicting the residual stress generated by arrays of adjacent/overlapping laser shock peening (LSP) shots where the use of a completely explicit FE analysis may be impractical. It shows that for a given material, the underlying eigenstrain distribution (in contrast to the resulting stress field) representing a laser shock peen is primarily dependent on the parameters of the laser pulse and the number of overlays rather than the precise component geometry. Consequently the residual stress introduced by complex laser peening treatments can be built up by using static FE models and superposition of individual eigenstrain distributions without recourse to further computationally demanding explicit FE analyses. It is found that beneath a small patch of LSP array the magnitude of the compressive residual stress is higher than for a wider array of LSP shots and that with increasing numbers of layers the compressive stress increases as does the depth of the compressive zone. The model predictions for the eigenstrain distributions are compared well with experimental measurements of plastic strain (full-width-at-half-maximum) obtained by neutron diffraction. The eigenstrain method is also extended to construct the full residual stress field using measured residual elastic strains at a finite number of measurement locations in a component.
机译:本文提出了一种混合显式有限元(FE)/本征应变模型,用于预测由相邻/重叠激光冲击喷丸(LSP)镜头阵列产生的残余应力,而使用完全显式有限元分析可能是不切实际的。它表明,对于给定的材料,代表激光冲击点的潜在特征应变分布(与所得应力场相反)主要取决于激光脉冲的参数和覆盖层的数量,而不是精确的组件几何形状。因此,可以通过使用静态有限元模型和各个特征应变分布的叠加来建立由复杂的激光喷丸处理所引入的残余应力,而无需依靠进一步的计算要求进行明确的有限元分析。已经发现,在较小的LSP阵列块下,压缩残余应力的大小要比较宽的LSP散点阵列高,并且随着层数的增加,压缩应力会随着压缩区深度的增加而增加。本征分布的模型预测与通过中子衍射获得的塑性应变(半峰全宽)的实验测量结果进行了很好的比较。本征应变方法也扩展为使用在组件中有限数量的测量位置处测得的残余弹性应变来构建完整的残余应力场。

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