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Microstructure evolution in an interstitial-free steel during cold rolling at low strain levels

机译:低应变水平冷轧过程中无间隙钢的组织演变

摘要

Microstructure development in an interstitial-free steel during cold rolling at low strain levels (ε ≤ 9.8%) has been investigated by using transmission electron microscopy. At a strain of 2.2%, {112} slip systems operate in addition to {110} slip planes. Dislocation reactions occur at this stage to produce immobile 100 segments in the scissors configuration and these segments are also found at higher strain in the dislocation walls of microbands. The formation of microbands starts at small reductions (ε ∼ 6.7%), and microbands are of lenticular shapes and have habit planes running approximately parallel to {110} planes. Two sets of dislocations comprise the microband walls; one is predominant and has its Burgers vector lying on the microband's habit plane. The secondary set is much less dense, and its slip plane is not coplanar with the microband habit plane. A considerable misorientation exists between the inner region of a microband and either of its two neighbouring matrices, rather than between the two matrices, which is consistent with Jackson's double cross-slip model. However, the growing end of a microband indicates the splitting of a dense dislocation sheet. In the specimen that was rolled to ε = 9.8%, some grains contain one or two sets of microbands, while some are microband-free. The crystallographic measurement and deformation geometry calculation reveal that the habit plane of an observed microband has the largest Schmid factor; and when one (111) slip direction is intensively activated in this plane, one set of microbands is formed on this plane. Two sets of microbands form if two (111) slip directions have high and nearly equal shear stresses. In the case of microband-free crystals, up to seven slip systems have similar Schmid factors and thus are activated concurrently. This leads to homogeneous deformation and as a result, no microbands form. Based on these results, a new mechanism is proposed for microband formation involving double cross-slip, dislocation wall splitting and dislocation exchange between the walls.
机译:利用透射电子显微镜研究了低应变水平(ε≤9.8%)冷轧过程中无间隙钢的组织发展。在{110}滑移面之外,{112}滑移系统在2.2%的应变下运行。在该阶段发生位错反应,以剪刀状结构产生固定的100个片段,并且在微带的位错壁中也以较高的应变发现了这些片段。微带的形成开始于小的减小(ε〜6.7%),并且微带为双凸透镜形状,并且具有与{110}平面大致平行的惯性平面。两组位错包括微带壁。一种是主要的,其Burgers向量位于微带的习惯平面上。次要集合的密度要小得多,并且其滑动平面与微带习惯平面不共面。微带的内部区域与其两个相邻矩阵中的任何一个之间都存在相当大的方向错误,而不是两个矩阵之间存在很大的方向错误,这与杰克逊的双重交叉滑移模型一致。然而,微带的增长端表明致密的位错片的分裂。在轧制到ε= 9.8%的样品中,一些晶粒包含一或两组微带,而有些则不含微带。晶体学测量和变形几何计算表明,观察到的微带的惯性面具有最大的施密德因子;当在该平面上强烈激活一个(111)滑动方向时,在该平面上形成一组微带。如果两个(111)滑动方向具有较高且几乎相等的剪切应力,则会形成两组微带。在无微带晶体的情况下,多达七个滑移系统具有相似的施密特因子,因此会同时被激活。这导致均匀变形,结果没有形成微带。基于这些结果,提出了一种新的微带形成机制,该机制涉及双交叉滑移,位错壁分裂和壁间位错交换。

著录项

  • 作者

    Chen QZ; Ngan AHW; Duggan BJ;

  • 作者单位
  • 年度 2003
  • 总页数
  • 原文格式 PDF
  • 正文语种 eng
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