取向硅钢冷轧剪切带与基体晶粒间的取向关系:晶体塑性计算与实验

  • 陈思昊 ,
  • 沙玉辉 ,
  • 张芳 ,
  • 程思飞 ,
  • 左良
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  • 东北大学 材料各向异性与织构教育部重点实验室  沈阳 110819

收稿日期: 2025-08-08

  修回日期: 2026-01-22

  录用日期: 2026-03-11

  网络出版日期: 2026-03-11

基金资助

立方金属板带晶界梯度区形变结构关联统计研究(52371022)

Orientation Relationship Between Cold-Rolling Shear Band and Matrix Grain in Grain-Oriented Silicon Steel: Crystal Plasticity Calculation and Experiment

  • Chen, Si-Hao
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  • Key Laboratory for Anisotropy and Texture of Materials, Ministry of Education, Northeastern University, Shenyang 110819, China

Received date: 2025-08-08

  Revised date: 2026-01-22

  Accepted date: 2026-03-11

  Online published: 2026-03-11

摘要

为了阐明取向硅钢冷轧时偏转{111}<112>取向基体与剪切带间的取向偏差角关系,本工作引入二维(2D)剪切面(剪切带与轧制横轴平行)和三维(3D)剪切面(剪切带与滑移面平行),采用粘塑性自洽模型计算偏转{111}<112>取向基体中形成的剪切带晶体取向转动过程。结果表明,当偏转{111}<112>取向基体的Euler角φ1 < 90°且Euler角φ2 < 45°时,剪切带取向转动过程中取向偏差角|Δφ1ʹ|减小、取向偏差角|Δφ2ʹ|先减小后增加或单调增加,相对于理想Goss取向,剪切带最终取向的|Δφ1ʹ|小于|Δφ2ʹ|。当偏转{111}<112>取向基体中φ1 < 90°且φ2 > 45°时,剪切带取向转动过程中|Δφ1ʹ|和|Δφ2ʹ|均减小,相对于理想Goss取向,剪切带最终取向的|Δφ1ʹ|大于|Δφ2ʹ|。在φ2 < 45°的偏转{111}<112>取向基体中,剪切带所在滑移面偏离最大剪切应力平面的角度大,剪切面更趋近于2D剪切面;在φ2 > 45°的偏转{111}<112>取向基体中,剪切带所在滑移面偏离最大剪切应力平面的角度小,剪切面更趋近于3D剪切面。

本文引用格式

陈思昊 , 沙玉辉 , 张芳 , 程思飞 , 左良 . 取向硅钢冷轧剪切带与基体晶粒间的取向关系:晶体塑性计算与实验[J]. 金属学报, 0 : 0 . DOI: 10.11900/0412.1961.2025.0224

Abstract

Superior magnetic properties of grain-oriented silicon steel arise from sharp Goss texture after secondary recrystallization. Shear band which is formed during cold rolling acts as preferential nucleation sites for recrystallization, and is a critical factor influencing accuracy of recrystallized Goss texture. The deviation angle of shear band φ1ʹ and Δφ2ʹ) from ideal Goss orientation ({110}<001>) is closely related to that of deformed matrix φ1 and Δφ2) from ideal {111}<112> orientation. Accordingly, it is essential to elucidate the relationship of orientation deviation between deviated {111}<112> orientation matrix and Goss shear band for precise orientation control of grain-oriented silicon steel. This study incorporates two-dimensional (2D) shear band plane (shear band parallel to transverse direction) and three-dimensional (3D) shear band plane (shear band parallel to slip plane) into a visco-plastic self-consistent (VPSC) model to calculate the crystal orientation rotation of shear bands within deviated {111}<112> orientation matrix, and simulated results are compared with experimental data. The findings indicate that both magnitude and mode of matrix orientation deviation significantly affect the corresponding shear band orientation deviation. When Euler angle φ1 of deviated {111}<112> orientation matrix is less than 90° and Euler angle φ2 is less than 45°, φ1ʹ| decreases while |Δφ2ʹ| either initially decreases and then increases or monotonically increases during shear band orientation rotation, and final shear band orientation exhibits a smaller |Δφ1ʹ| than |Δφ2ʹ| relative to ideal Goss. When φ1 of deviated {111}<112> orientation matrix is less than 90° and φ2 exceeds 45°, both |Δφ1ʹ| and |Δφ2ʹ| decrease during shear band orientation rotation, and final shear band orientation exhibits a greater |Δφ1ʹ| than |Δφ2ʹ| compared to ideal Goss. Shear band plane is also found to depend on direction of matrix deviation. For φ2 < 45°, the slip plane where shear band locates deviates significantly from the maximum shear stress plane, and shear band plane is more accurately represented by 2D shear band plane. For φ2 > 45°, the slip plane where shear band forms exhibits a smaller deviation from the maximum shear stress plane, and shear band plane is more accurately represented by 3D shear band plane. Identification of shear plane in deviated {111}<112> orientation matrix is thus fundamental to clarify the mechanism of shear band formation and to enable reliable crystal plasticity simulations of shear band orientation.


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