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γ相预变形及α相回火00Cr12钢中的011/011近奇异晶界

011/011 near singular boundary in 00Cr12 steel pre-deformed at γ region followed by tempering at α region

  • 摘要: 011/011近奇异晶界腐蚀抗力显著优于随机晶界,通过晶界工程优化并提高此类晶界的比例,有望成为提高体心立方金属,特别是低铬铁素体不锈钢晶间腐蚀抗力的有效途径。本文选用热锻态00Cr12钢为试验材料,5个平行试样在γ相区(960 ℃)进行厚度减缩量为35%的1道次轧制后,迅速放入700 ℃的马弗炉中分别回火0.5、1、2、3、4 h,然后水淬至室温。为了定量化计算各试样中011/011近奇异晶界的比例,采用了基于电子背散射衍射(electron backscatter diffraction,EBSD)技术结合5参数分析的晶界界面匹配表征方法。结果显示,随着回火时间的延长,011/011近奇异晶界的比例并非单调变化,而是呈先增加后减少的规律,并在700 ℃回火2 h时达到极大值10.97%。离线原位EBSD结果进一步揭示,011/011近奇异晶界的形成主要有2种机制,一是原本不相邻但具有〈011〉/θθ为取向差旋转角)取向差关系的晶粒,在700 ℃回火过程中通过吞并中间晶粒而最终碰撞形成011/011近奇异晶界;二是相邻晶粒在回火过程中发生取向差调整及晶界面再取向,生成011/011近奇异晶界。在700 ℃回火超过2 h后,发生晶粒异常长大,大角度晶界的迁移吞并了部分011/011近奇异晶界,导致该晶界比例下降。

     

    Abstract: The corrosion resistance of 011/011 near singular grain boundaries is significantly better than that of random grain boundaries. Optimizing and increasing the proportion of such grain boundaries through grain boundary engineering may become an effective way to improve the intergranular corrosion resistance of body centered cubic metals, especially low chromium ferritic stainless steel. In this study, hot forged 00Cr12 steel was used as the test material. Five parallel samples were subjected to one pass rolling with a thickness reduction of 35% in the γ phase region at 960 ℃, and then quickly placed in a muffle furnace at 700 ℃ for tempering for 0.5, 1, 2, 3, and 4 h respectively, followed by water quenching to room temperature. To quantitatively calculate the proportion of 011/011 near singular grain boundaries in each sample, a grain boundary inter-connection characterization method based on electron backscatter diffraction (EBSD) technology combined with five parameter analysis was adopted. The results show that with increasing tempering time, the proportion of 011/011 near singular grain boundaries does not change monotonically. It first increases and then decreases, reaching a maximum value of 10.97% after tempering at 700 ℃ for 2 h. Offline in situ EBSD results further reveal that there are two main mechanisms for the formation of 011/011 near singular grain boundaries. One is that grains that are not originally adjacent but have an orientation relationship of 〈011〉/θ collide with each other by swallowing intermediate grains during tempering at 700 ℃, thus forming 011/011 near singular grain boundaries. The other is that adjacent grains undergo orientation difference adjustment and grain boundary plane reorientation during tempering, generating 011/011 near singular grain boundaries. When tempering at 700 ℃ for more than 2 h, abnormal grain growth occurs. The migration of high angle grain boundaries swallows part of the 011/011 near singular grain boundaries, leading to a decrease in the proportion of such boundaries.

     

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