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CAVITY GROWTH SIMULATION OF 2.25CR-1MO STEEL UNDER CREEP-FATIGUE LOADING

机译:蠕变疲劳载荷下2.25Cr-1Mo钢的腔生长模拟

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High temperature components in thermal power plants are subjected to creep-fatigue loading where creep cavities initiate and grow on grain boundaries. Development of a quantitative evaluation method of cavity growth is important for reliable maintenance of these components. In this study, a creep-fatigue test was carried out at 600°C on 2.25Cr-1Mo steel in a scanning electron microscope, and continuous observation of cavity growth behavior on the surface during the test was made. Based on the cavity growth observation, existing cavity growth models were modified and a simulation result by the modified model was discussed by comparing with observed cavity growth behavior. From the observation, spherical shape cavities initiate and grow up to their length of 2μm on the grain boundaries at initial stage of damage, and then these cavities change their shape to crack-like to grow until their length reaches around 10μm. Finally, crack-like cavities coalesce each other to form one micro crack along a grain boundary. It can be concluded that cavity growth rates of these cavities are controlled by diffusion and power law creep under constrained condition based on theoretical consideration of cavity growth mechanism. Through these discussions, a new cavity growth model was proposed by modifying conventional models. Both spherical and crack-like cavity growth rate equations were derived from the modified cavity growth model. It was indicated that measured cavity growth rate was well predicted by the growth rate equations derived from the modified model, and a cavity growth simulation result corresponds to the change in the maximum cavity size with cycles under the creep-fatigue loading.
机译:热电厂中的高温分量经受蠕变 - 疲劳负荷,其中蠕变腔引发并在晶界上生长。腔生长的定量评估方法的发展对于可靠维持这些组件是重要的。在该研究中,在扫描电子显微镜下在2.25cr-1mo钢上在600℃下进行蠕变 - 疲劳试验,并在测试期间的表面上的腔生长行为的连续观察。基于腔生长观察,通过比较观察到的腔生长行为来修改现有的腔生长模型,并通过与观察到的腔生长行为进行讨论的模拟结果。从观察开始,球形形状腔在初始损伤阶段的晶界上启动并长长于2μm的长度,然后这些空腔将它们的形状改变为裂纹,直到它们的长度达到约10μm。最后,裂缝状腔彼此聚结,以沿晶界形成一个微裂缝。可以得出结论,基于腔生长机制的理论考虑,通过扩散和动力法蠕变来控制这些腔的腔生长速率。通过这些讨论,通过修改传统模型提出了一种新的腔生长模型。球形和裂纹状腔生长速率方程均来自改性腔生长模型。结果表明,测量的腔生长速率通过改性模型的生长速率方程预测,并且腔生长模拟结果对应于在蠕变疲劳负载下具有循环的最大腔体尺寸的变化。

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