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Examination of rate-controlling mechanisms for plastic deformation of pearlitic steel at low homologous temperatures

机译:低同源温度下珠光体钢塑性变形的速率控制机制研究

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The rate-controlling mechanisms of plastic deformation of pearlitic steel before and after cold drawing at low homologous temperatures (T/T-m) were explored because cold-drawn pearlitic steel is an important structural material that requires long-term sustainability at low T/T-m. Both the undrawn and the cold-drawn pearlitic steels were deformed plastically under constant loads at low T/T-m of 0.25-0.30. The strain rate-stress data were analyzed in terms of a power law model based on low temperature dislocation climb, a lattice friction controlled plasticity model, and an obstacle controlled plasticity model. The first two models were inadequate to explain low T/T-m plastic deformation of the present steels: (a) much higher activation energy than that for core diffusion resulted from the low temperature dislocation climb model, and (b) athermal stress comparable to that for pure alpha-Fe was estimated from the lattice friction controlled plasticity model, so the role of cementite on athermal stress in pearlite was unexplainable. By contrast, the obstacle controlled plasticity model estimated activation energy on the same order as that for overcoming forest dislocations which were regarded as the main obstacles in the present steels, as evidenced by microstructural observation. In addition, this model not only gave an estimate of the athermal stress for the present pearlitic steel that was higher than that of pure alpha-Fe (reflecting the effect of cementite on athermal stress), but also provided an estimate of the athermal stress of the cold-drawn steel that was higher than that of the undrawn steel (reflecting the effect of pre-existing dislocations caused by cold-drawing in the former). Therefore, it is probable that low T/T-m plastic deformation of the present pearlitic steels is rate controlled by dislocation glide overcoming forest dislocations generated by low T/T-m deformation and/or by cold drawing. (C) 2016 Elsevier Inc. All rights reserved.
机译:探索了珠光体钢在低同温(T / T-m)下冷拔前后塑性变形的速率控制机制,因为冷拔珠光体钢是一种重要的结构材料,需要在低T / T-m下具有长期可持续性。未拉伸和冷拉伸的珠光体钢都在恒定载荷下以0.25-0.30的低T / T-m塑性变形。根据基于低温位错爬升的幂律模型,晶格摩擦控制的塑性模型和障碍物控制的塑性模型,对应变率-应力数据进行了分析。前两个模型不足以解释当前钢的低T / Tm塑性变形:(a)低温位错爬升模型产生的活化能比堆芯扩散的活化能高得多,并且(b)无热应力可与根据晶格摩擦控制的可塑性模型估算了纯α-Fe,因此无法解释渗碳体对珠光体无热应力的作用。相比之下,障碍物可塑性模型估计的活化能与克服森林脱位的活化能相同,而微观结构的观察证明,森林脱位被认为是目前钢材中的主要障碍。此外,该模型不仅给出了目前珠光体钢的无热应力估算值,该值比纯α-Fe的高(反映了渗碳体对无热应力的影响),而且还提供了对碳素体钢无热应力的估算。冷拔的钢比未拔出的钢要高(反映了前者由于冷拔引起的先前存在的位错的影响)。因此,本珠光体钢的低T / T-m塑性变形很可能通过克服低T / T-m变形和/或冷拔产生的位错滑移克服森林位错来控制。 (C)2016 Elsevier Inc.保留所有权利。

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