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Finite element analysis of thermomechanical behavior and residual stresses in cold flowformed Ti6Al4V alloy

机译:冷流量Ti6Al4V合金中热机械性能和残余应力的有限元分析

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Ti6Al4V alloy is very hard to flowform at room temperature due to its limited ductility. However, it retains excellent adiabatic heat trapping and thermal softening abilities, which can play an important role in improving the formability. In this paper, a 3-D finite element model of backward flowforming with three staggered rollers has been developed in Abaqus/explicit to study the thermomechanical behavior and the residual stress evolution. The model has been validated via flowforming experiments. The role of the heat generation due to plastic deformation is highlighted by comparing a thermomechanical analysis to a purely mechanical analysis without incorporating the additional heat input due to the plastic work. The maximum predicted temperature rise during cold flowforming is 911 degrees C, which significantly reduces the flow stress in the deformation zone. The two most important factors, which affect the temperature rise in the deformation zone, are friction coefficient and coolant heat transfer coefficient. Hence, a study has been done to assess the sensitivity of the thermomechanical behavior and the residual stresses towards these factors. The friction between the mating surfaces is helpful, but a friction coefficient higher than 0.1 causes through-thickness strain heterogeneity. An increase in the friction coefficient reduces the residual stresses, while an increase in the convective heat transfer coefficient causes a transition from compressive to tensile residual stress along the thickness of the tube.
机译:由于其有限的延展性,Ti6Al4V合金非常难以在室温下流动。然而,它保留了优异的绝热捕获和热软化能力,这可以在提高成形性方面发挥重要作用。在本文中,在ABAQUS /明确地开发了具有三个交叉辊的后向流量的3-D有限元模型,以研究热机械行为和残余应力进化。该模型通过流量实验验证。通过将热机械分析与纯机械分析进行比较,突出了由于塑性变形引起的发热引起的作用,而不将由于塑性工作引起的额外热输入。冷流量期间的最大预测温度升高为911摄氏度,这显着降低了变形区中的流量应力。影响变形区中温度升高的两个最重要的因素是摩擦系数和冷却剂传热系数。因此,已经进行了研究以评估热机械行为的敏感性和对这些因素的残余应力。配合表面之间的摩擦是有帮助的,但高于0.1的摩擦系数导致厚度应变异质性。摩擦系数的增加降低了残余应力,而对流传热系数的增加导致沿着管的厚度压缩到拉伸残余应力的过渡。

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