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Recrystallization and Grain Growth Behavior in Severe Cold-rolling Deformed SUS316L Steel under Anisothermal Annealing Condition

机译:等温退火条件下强冷轧变形SUS316L钢的再结晶和晶粒长大行为

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Ultrafine grained microstructure seems difficult to be obtained in austenite stainless steel by hot rolling process because the steel has a high recrystallization temperature and high grain growth rate. Instead of severe plastic deformation at medium temperatures, anisothermal annealing of cold-rolled steel could be an effective way to obtain the ultrafine microstructure in the steel. In order to clarify the recrystallization and grain growth in SUS316L stainless steel in anisothermal annealing condition, variations of hardness and average grain size of the steel at annealing temperatures ranging from 1 073 to 1 223 K and heating rates in the range of 0.031-9.3 K/s were systematically investigated, and the results were summarized in contour maps. The recrystallization finish temperature was recognized by a hardness criterion, which shows a linear relationship with the logarithm of the heating rate. Moreover, the average grain size at the critical temperature is approximately 2.2 μm at low heating rates, but decreases quickly with the increase of heating rates above 1 K/s. A proposed grain growth kinetics equation for anisothermal annealing is applied in the present investigated SUS316L steel. The proportional term, i.e., Π=(D~n-D_0~n)/(Γ_f-Γ_i), in the equation is calculated and is found to follow the equation Π=K·exp(0.5/θ). Meanwhile, the grain growth exponent, n, for the anisothermally annealed SUS316L steel is also determined and is found to lie between 2.5 and 3.0. On the other hand, EBSD analysis of the evolved microstructure at different heating rates indicates that low heating rate caused partial recrystallization with preferred orientations at the recrystallization finish temperature, while high heating rates above 1 K/s induced the homogeneously nucleated recrystallization microstructure with random orientations and a lognormal type grain size distribution.
机译:由于奥氏体不锈钢具有高的再结晶温度和高的晶粒生长速率,因此似乎很难通过热轧工艺获得超细晶粒的组织。代替中等温度下的严重塑性变形,冷轧钢的等温退火可能是获得钢中超细组织的有效方法。为了弄清楚SUS316L不锈钢在等温退火条件下的重结晶和晶粒长大,在退火温度为1073至1,223 K且加热速率为0.031-9.3 K的范围内,钢的硬度和平均晶粒度的变化/ s进行了系统的研究,并将结果汇​​总在等高线图中。再结晶结束温度通过硬度标准识别,该硬度标准与加热速率的对数呈线性关系。此外,临界温度下的平均晶粒尺寸在低加热速率下约为2.2μm,但随着加热速率在1 K / s以上的增加而迅速减小。在目前研究的SUS316L钢中,采用了建议的等温退火晶粒生长动力学方程。计算该方程式中的比例项即Π=(D〜n-D_0〜n)/(Γ_f-Γ_i),并发现其遵循方程Π= K·exp(0.5 /θ)。同时,还确定了经等温退火的SUS316L钢的晶粒长大指数n,位于2.5和3.0之间。另一方面,在不同加热速率下对演化组织的EBSD分析表明,低加热速率导致部分再结晶在重结晶完成温度下具有较好的取向,而高于1 K / s的高加热速率则诱导了具有随机取向的均相成核再结晶组织对数型晶粒尺寸分布。

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