首页> 外文期刊>Journal of Mining and Metallurgy, Section B: Metallurgy >Evolution of secondary phases in 0.17C-16Cr-11Mn-0.43N austenitic stainless steel at 800 and 850°C: Thermodynamic modeling of phase equilibria and experimental kinetic studies
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Evolution of secondary phases in 0.17C-16Cr-11Mn-0.43N austenitic stainless steel at 800 and 850°C: Thermodynamic modeling of phase equilibria and experimental kinetic studies

机译:0.17C-16Cr-11Mn-0.43N奥氏体不锈钢在800和850°C下二次相的演变:相平衡的热力学模型和实验动力学研究

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The precipitation of secondary phases was investigated in the 0.17C-16Cr-11Mn-0.43N austenitic stainless steel during annealing at 800 and 850°C for times between 5 min and 100 h. Light microscopy, transmission electron microscopy, energy dispersive X-ray spectroscopy, scanning electron microscopy, and differential thermal analysis were used in experiments. Thermodynamic calculations were done by the ThermoCalc database software package. Cr2N and M23C6 were considered to be stable phases at the annealing temperatures. Cells consisting of alternating Cr2N and austenite lamellae were observed in the steel microstructure after sufficiently long annealing. The metastable chi phase was also found in all the annealed samples. After 100 h of annealing the equilibrium sigma started to precipitate. The thermodynamically predicted M6C was not confirmed experimentally in any of the annealed samples. DTA analysis showed the initial precipitation stage was followed by the phase dissolution. For the investigated steel the computational thermodynamics can be used only for qualitative interpretation of the experimental results as the measured endothermal peaks were found to be shifted of about 50 ÷ 70°C related to the computed results.
机译:研究了0.17C-16Cr-11Mn-0.43N奥氏体不锈钢在800和850°C退火5分钟至100小时之间二次相的沉淀过程。实验中使用了光学显微镜,透射电子显微镜,能量色散X射线光谱,扫描电子显微镜和差热分析。热力学计算是通过ThermoCalc数据库软件包完成的。 Cr2N和M23C6在退火温度下被认为是稳定相。经过足够长时间的退火后,在钢的显微组织中观察到由交替的Cr2N和奥氏体薄片组成的晶胞。在所有退火样品中也发现了亚稳态的χ相。退火100小时后,平衡西格玛开始沉淀。在任何退火样品中均未通过实验确定热力学预测的M6C。 DTA分析表明初始沉淀阶段之后是相溶解。对于所研究的钢,计算热力学只能用于定性解释实验结果,因为发现测得的吸热峰相对于计算结果有大约50÷70°C的偏移。

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