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Microstructure evolution in Alloy 617 B after a long-term creep and thermal aging at 700 ℃

机译:700℃长期蠕变和热时效后,合金617 B的组织演变

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摘要

Changes in the microstructure of heat-resistant materials may influence their long-term behaviour. For this reason, materials chosen for high temperature-based applications, e.g. advanced ultra-supercritical (A-USC) steam power plants, must exhibit long-term microstructure stability. Therefore, changes in the microstructure of frequently used materials must be determined and correlated with their creep behaviour to assure a reliable operation of components. In this work, a long-term study investigated the microstructure of a creep rupture specimen made of a nickel-based alloy 617 B. The creep tests were carried out at 700 ℃ for up to 45,148 h. By using optical microscopy (OM), scanning electron microscopy (SEM) and transmission electron microscopy (TEM) the virgin, thermal-loaded and creep states were characterized. The precipitate location, number and size have been determined. The experiment results were compared, discussed and correlated to the creep and failure behaviour. Furthermore, the long-term precipitation kinetics of Alloy 617 B was simulated, which considered its thermal history, using the MatCalc software. The simulated precipitates fraction and size were compared with the experimental data obtained in this study. The comparison between the experimental and simulation results demonstrated comparable gamma prime (γ~1) phases. The simulation results of the carbides identified at the grain boundaries were satisfactory. However, the size of the intragranular fine carbides M_(23)C_6 was not reproduced correctly.
机译:耐热材料的微观结构变化可能会影响其长期性能。因此,选择用于高温应用的材料,例如先进的超超临界(A-USC)蒸汽发电厂必须具有长期的微观结构稳定性。因此,必须确定常用材料的微观结构变化,并将其与蠕变行为相关联,以确保组件的可靠运行。在这项工作中,长期研究研究了由镍基合金617 B制成的蠕变断裂试样的微观结构。在700℃下进行了45,148 h的蠕变试验。通过使用光学显微镜(OM),扫描电子显微镜(SEM)和透射电子显微镜(TEM)来表征原始状态,热负荷状态和蠕变状态。确定了沉淀物的位置,数量和大小。对实验结果进行了比较,讨论并与蠕变和破坏行为相关联。此外,使用MatCalc软件模拟了合金617 B的长期析出动力学,并考虑了其热历史。将模拟的沉淀物分数和大小与本研究中获得的实验数据进行比较。实验结果和模拟结果之间的比较表明,可比较的伽马素数(γ〜1)相。在晶界处识别出的碳化物的模拟结果令人满意。然而,晶粒内细碳化物M_(23)C_6的尺寸没有正确地再现。

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