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Formation of Austenite Grain After Peritectic Solidification in Hypo-and Hyper-Peritectic Carbon Steels

机译:次高碳和高贝氏体碳钢包晶凝固后奥氏体晶粒的形成

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A process from the occurrence of a delta dendrite(delta) to austenite(gamma) grain formation is investigated. When a hyper-peritectic carbon steel is unidirectionally solidified and quenched in water, three regions of delta dendrited, fine columnar grain and coarse grain are observed. The region of the delta dendrites is corresponding to (L+delta) phase. The regon of the fine columnar grain is (KL+delta+gamma) and (L+gamma) phases. The region of the coarse grain is (L+gamma) and gamma phases. The size of the narrow side of one fine columnar grain changes suddenly to the region of the coarse one when a liquid fraction in the (L+gamma) phases reduces below a certain value. On the other hand, in a hypo-peritectic carbon steel, three regions are observed, same as the hyper-peritectic carbon steel, The region of delta dendrites is correpsonding to (L+elta) phase, and fine columnar grain is (L+elta+gamma) and (delta+gamma) phases. The coarse grain is gamma phase. Furthermore, the region of the fine columnar grain changes suddenly the region of the coarse grain when the delta phase completely disappears. Likewise, the narrow size of the region of the coarse grain when the delta phase completely disappears. Likewise, the narrow size of the fine columnar grain coincides with the primary dendrite arm spacing. However, the gamma grain boundaries of the hypo-and hyper-peritectic carbon steels form at different location. That is ,they are formed in the skelecton of the delta dendrite and in the interspacing of the primary dendrite arm. Therefore, it seems that the liquid phase in the gyper-peritectic carbon steel and the delta phase in the hypo-peritectic carbon steel act as the prevention of the gamma grain growth.
机译:研究了从发生δ枝晶转变为奥氏体γ晶粒形成的过程。当过包晶碳钢在水中单向凝固并淬火时,观察到三个区域的δ树枝状,细柱状晶粒和粗晶粒。 δ树枝状晶体的区域对应于(L +δ)相。细柱状晶粒的区域是(KL +δ+γ)相和(L +γ)相。粗晶粒的区域是(L +γ)和γ相。当(L +γ)相中的液体分数降低到一定值以下时,一个细的柱状晶粒的窄边的尺寸突然变化到粗晶粒的区域。另一方面,在高包晶碳素钢中,观察到与高包晶碳素钢相同的三个区域,δ枝晶的区域与(L + elta)相对应,细的柱状晶粒为(L + Elta +γ)和(δ+γ)相。粗晶粒为γ相。此外,当δ相完全消失时,细的柱状晶粒的区域突然改变粗晶粒的区域。同样,当δ相完全消失时,粗晶粒区域的狭窄尺寸。同样,细柱状晶粒的窄尺寸与一次枝晶臂间距相吻合。但是,次包晶和超包晶碳钢的γ晶界在不同的位置形成。也就是说,它们形成在三角形枝晶的骨架中和初级枝晶臂的间隔中。因此,似乎似乎在银-白云母碳钢中的液相和在白云母碳钢中的δ相起到了防止γ晶粒长大的作用。

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