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首页> 外文期刊>鉄と鋼/Journal of the Iron and Steel Institute of Japan. >Shape, Size and Crystallographic Orientation of the Ferrite Grains Formed at Grain Boundaries of Deformed Austenite in a Low Carbon Steel
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Shape, Size and Crystallographic Orientation of the Ferrite Grains Formed at Grain Boundaries of Deformed Austenite in a Low Carbon Steel

机译:低碳钢中变形奥氏体晶界形成的铁氧体晶粒的形状,尺寸和晶体取向

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摘要

The influence of plastic strain on the shape, size and crystallographic orientation of ferrite (#alpha#) grains formed at the grain boundaries of the deformed austenite (#gamma#) was studied in a 0.l7C-0.3Si-l.5Mn steel. Specimens with a coarse #gamma# grain size of 300 #mu#m were compressed at 1023K and cooled at 10K/s. When the plastic strain increased to 0.4, the shape of #alpha# grains changed from plate like to equiaxed, and the average length of #alpha# grains decreased from 12 to 6 #mu#m. However, the average length did not change in the larger plastic strains up to 1.1. On the other hand, the average thickness of #alpha# grains was constant regardless of the plastic strain. The crystallographic orientations of the #alpha# grains formed at one #gamma# grain boundary were almost the same when the plastic strain was smaller than 0.2 and the #alpha# grain shape was plate like. However, the orientations were widely distributed (and most of the #alpha#/#alpha# boundaries were high angle ones, when the plastic strain was larger than 0.4 and the #alpha# grain shape was equiaxed. The shape change and #alpha# grain refinement by the deformation resulted from the wide distribution of crystallographic orientations of #alpha# grains rather than from the increase in the nucleation rate. The wide distribution of crystallographic orientation of #alpha# grains is closely associated with the serrated austenite grain boundaries induced by the deformation.
机译:研究了在0.L7C-0.3SI-L.5MN钢中研究了在变形奥氏体(#γ#)的晶界(#α#)颗粒的形状,尺寸和晶粒的影响(#α#)颗粒的影响。具有粗#γ#m的标本300#mu#m的标本在1023k中压缩并以10k / s冷却。当塑性应变增加到0.4时,#α#颗粒的形状从板式变为等轴,并且#α#谷物的平均长度从12到6#mu#m减小。然而,平均长度在较大的塑料菌株中没有变化,高达1.1。另一方面,无论塑性应变如何,#α#晶粒的平均厚度是恒定的。当塑性应变小于0.2时,在一个#γ#晶界处形成的#α#颗粒的晶体取向几乎相同。然而,当塑性应变大于0.4时,方向被广泛分布(大多数#Alpha#/#alpha#边界是高角度的。通过变形的晶粒改进是由#α#颗粒的晶状体取向的广泛分布而不是从成核速率的增加。#α#颗粒的晶体取向的广泛分布与锯齿状奥氏体晶界密切相关变形。

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