首页> 外文会议>EPRI s International Conference on Advances in Materials Technology for Fossil Power Plants;International 123HiMAT Conference on High-Temperature Materials >EXPERIMENTAL AND COMPUTATIONAL STUDY ON GRAIN BOUNDARY AND GRAIN INTERIOR PRECIPITATION OF FE_2NB LAVES PHASE IN FE-CR-NI-NB AUSTENITIC HEAT RESISTANT STEELS
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EXPERIMENTAL AND COMPUTATIONAL STUDY ON GRAIN BOUNDARY AND GRAIN INTERIOR PRECIPITATION OF FE_2NB LAVES PHASE IN FE-CR-NI-NB AUSTENITIC HEAT RESISTANT STEELS

机译:Fe-Cr-Ni-Nb奥氏体耐热钢Fe_2NB熔化液晶界和晶粒内部沉淀的实验与计算研究

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The precipitation behavior of Fe_2Nb Laves phase (C14 structure) on grain boundary (GB) and grain interior (GI), and Ni_3Nb metastable γ" phase and stable 8 phase on GI in the austenitic heat-resistant model steels is studied experimentally in different temperatures, and it is reproduced by thermo-kinetic calculation. The steel studied was prepared by arc melting, and cold rolled by 65%. Then, the sample was solution treated at γ single phase region, in order to control the grain size to approximately 150 μm. Solution-treated sample was subsequently aged at 973 K to 1473 K for up to 3600 h. Microstructure was observed by FE-SEM and the chemical composition of y matrix and precipitates of Laves and δ phase was analyzed by EPMA. The precipitation modeling was performed using MatCalc software. The thermodynamic database constructed in our research group was used for the calculation of chemical potential of each phase. Classical nucleation theory was used for the nucleation, and SFFK model was used for the growth and coarsening stages. Grain boundary and grain interior Laves phase is defined as different phases, and morphology of all precipitates is assumed as spherical in the calculation. Precipitation start time is defined as the time when the precipitate fraction is reached to 1%. Experimental results show that, above 973 K, the Laves phase firstly nucleates on grain boundaries and then nucleates within the grain interior. The nose temperature is located at around 1273 K. In order to reproduce the experimentally determined TTP diagram, first, interaction parameters among elements is modified. Then, by introducing the lower interfacial energy between γ matrix and Laves phase, TTP diagram is reproduced by calculation, suggestion that the interface is relatively stable.
机译:在不同的温度下,研究了谷晶界(GB)和谷物内部(GI)和谷物内部(GI)和晶粒内部(GI)和晶粒内部(GI)和稳定的8相的沉淀行为,并在不同温度下进行了奥氏体耐热模型钢的GI上的稳定8相,它是通过热动力学计算再现的。通过电弧熔化制备的钢,冷轧65%。然后,在γ单相区域处理样品,以控制晶粒尺寸至约150 μm。随后在973k至1473k时,溶液处理的样品可达3600小时。通过Fe-Sem观察微观结构,通过EPMA分析了y矩阵的化学组成和雷击和δ相的沉淀物。降水模拟使用MATCALC软件进行。我们的研究组中构建的热力学数据库用于计算每个阶段的化学潜力。古典成核理论用于核心,以及SFFK模型用于生长和粗化阶段。晶界和谷物内部疏浚阶段定义为不同的阶段,并且所有沉淀物的形态被认为是在计算中的球形。降水开始时间定义为沉淀级分达到1%的时间。实验结果表明,高于973 k,Laves阶段首先对晶界进行成核,然后在谷物内部成核。鼻温位于1273k左右。为了再现实验确定的TTP图,首先,修改元件之间的交互参数。然后,通过在γ矩阵和疏浚阶段之间引入较低的界面能量,通过计算再现TTP图,建议界面相对稳定。

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