碳钢在热塑性变形过程中组织的形成

I. Vakulenko, D. Bolotova, S. V. Proidak, H. Askerov, H. Çuğ, H. O. Tchaikovska
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引用次数: 0

摘要

目的。本工作的主要目的是确定碳钢奥氏体再结晶过程发展的特点,这取决于热塑性变形的程度,并提出改善铁路实轧车轮金属结构状态的建议。方法。以最小和最大含碳量分别为0.55和0.65%的两种铁路车轮碳素钢及60钢牌号组成内的其他化学元素为研究材料。在马弗炉中加热直径为20mm,高度为40mm的圆柱体样品,暴露一定时间以使样品横截面上的温度均匀。然后在Instron型试验机上进行热压缩试验。试样的热压缩温度区间为950 ~ 1100 oС,高度变形程度在10 ~ 40%之间。应变速率为10-3-10-2sec-1。采用标准刻蚀法检测奥氏体晶粒边界。结构研究是用Epikvant型光学显微镜进行的,其放大倍数足以确定奥氏体晶粒的结构。用定量金相法测定了奥氏体的晶粒尺寸。发现。在铁路车轮毛坯热压缩的情况下,仅提高钢的等级组成内的碳原子浓度就足以提高平均奥氏体晶粒尺寸,这证实了限制铁路车轮金属中碳含量的建议。铁路轮辋或轮毂横截面处形成一定程度的奥氏体组织非均质是由于再结晶过程的发展机制随变形值的变化而变化。在相同热塑性变形程度的条件下,用分数次压缩代替一次压缩会破坏再结晶核的形成条件。通过对热塑性变形方案的指定替换,得到了奥氏体晶粒尺寸的减小。创意。通过对铁路轮毂碳钢热压缩过程中集体再结晶过程发展的研究,确定了碳含量的增加有助于奥氏体晶粒的增大。轮坯热压缩后,奥氏体组织的不均匀性是由再结晶过程发展机制的改变决定的。在超过临界程度的变形过程中,再结晶核形成并不断长大,导致组织细化。当变形低于临界值时,奥氏体晶粒的生长遵循聚结机制,具有大取向角的晶界碎片逐渐消失。实用价值。对于铁路实轧轮毂大块零件的奥氏体晶粒细化,我们提出用分式热压缩代替一次热压缩。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
FORMATION OF CARBON STEEL STRUCTURE DURING HOT PLASTIC DEFORMATION
Purpose. The main purpose of the work is to determine the peculiarities of the development of recrystallization processes of carbon steel austenite depending on the degree of hot plastic deformation and to develop proposals for improving the structural state of the metal of the railway solid-rolled wheel. Methodology. Two carbon steels of a railway wheel with a minimum and maximum carbon content of 0.55 and 0.65 % and other chemical elements within the grade composition of the steel 60 were used as research material. Samples in the form of cylinders with a diameter of 20 mm and a height of 40 mm were heated in a muffle furnace, exposed for a certain time to equalize the temperature across the cross section of the sample. After that, the samples were subjected to hot compression on Instron type test machine. The temperature interval of hot compression of the samples was 950–1100 oС, with deformation degrees in height in the range of 10–40%. The strain rate was 10-3–10-2sec-1. A standard etching was used to detect the boundaries of the austenite grains. Structural studies were performed using Epikvant type light microscope at magnifications sufficient to determine the structure of austenite grains. The grain size of austenite was determined by the methods of quantitative metallography. Findings. In the case of hot compression of the railway wheel blank, increasing the concentration of carbon atoms only within the grade composition of the steel is sufficient to increase the average austenite grain size, which confirms the proposals to limit the carbon content in the metal of railway wheels. The formation of a certain degree of austenite structural heterogeneity at the cross section of the rim or hub of the railway wheel is due to a change in the development mechanism of recrystallization processes depending on the deformation value. Under conditions of the same degree of hot plastic deformation, the replacement of one-time compression by fractional one is accompanied by a violation of the conditions of formation of the recrystallization nucleus. As a result of the specified replacement of the scheme of hot plastic deformation we obtain reduction in the austenite grain size. Originality. Based on a study of the development of collective recrystallization processes during the hot compression of carbon steel of the railway wheel, it was determined that the increase in carbon content contributes to the austenite grain increase. After hot compression of the wheel blank, the structural inhomogeneity of austenite that occurs is determined by a change in the mechanism of recrystallization processes development. During deformations above the critical degree, the recrystallization nuclei are formed and successively grow, which leads to the structure refinement. In the case of deformations below the critical value, the growth of austenite grains occurs according to the coalescence mechanism, according to which fragments of boundaries with large disorientation angles consistently disappear. Practical value. For austenite grain refining in massive elements of solid-rolled railway wheel we offer to replace one-time hot compression by fractional one.
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