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Dynamic compression property of a low-carbon quenching and partitioning steel

机译:低碳调质钢的动态压缩性能

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The dynamic compression properties of a low carbon quenched and partitioned (Q&P) steel were investigated over the strain rate range of 500-2500 s~(-1) using split-Hopkinson pressure bar equipment. Traditional quenched and tempered (Q&T) steel with an identified composition was used for comparison. For both types of steel, the flow stress and yield strength gradually increased as the strain rate was increased from 500 to 2000 s~(-1), indicating that strain-rate hardening dominates the deformation behavior. At a higher strain rate (2500 s~(-1)), the flow stress and yield strength begin to decrease, indicating that the thermal softening of the martensite matrix caused by adiabatic heating begins to exceed the effect of the strain-rate hardening. Based on the Johnson-Cook equation, which describes the deformation behavior as well as the parameters calculated by this equation, the Q&P specimens exhibited less pronounced strain-rate dependencies than the Q&T specimens. In addition, the impact shearing tests demonstrated that adiabatic shear failure is less likely to occur in Q&P specimens than in Q&T specimens. Analysis revealed that a considerable amount of retained austenite in the Q&P specimen was responsible for these differences, and in turn, its stability was affected by the strain rate. At a relatively low strain rate, stress/strain induced martensitic transformations easily occur. With higher strain rates, martensitic transformations are suppressed because adiabatic heating decreases the driving force of martensitic transformations.
机译:利用分体式霍普金森压力棒设备研究了低碳淬火和分区(Q&P)钢在500-2500 s〜(-1)应变速率范围内的动态压缩性能。使用具有确定成分的传统调质钢(Q&T)进行比较。对于这两种类型的钢,流变应力和屈服强度都随着应变率从500 s〜(-1)的增加而逐渐增加,这表明应变率硬化主导着变形行为。在较高的应变速率下(2500 s〜(-1)),流动应力和屈服强度开始降低,这表明由绝热加热引起的马氏体基体的热软化开始超过应变速率硬化的作用。基于描述变形行为以及由该方程计算的参数的Johnson-Cook方程,Q&P试样比Q&T试样表现出较小的应变率依赖性。此外,冲击剪切试验表明,绝热剪切破坏在Q&P样品中发生的可能性小于在Q&T样品中。分析表明,Q&P试样中大量残留的奥氏体是造成这些差异的原因,而其稳定性受到应变率的影响。在较低的应变速率下,应力/应变诱发的马氏体相变容易发生。在较高的应变速率下,由于绝热加热降低了马氏体相变的驱动力,因此抑制了马氏体相变。

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