首页> 外文期刊>鉄と鋼/Journal of the Iron and Steel Institute of Japan. >Relation between Creep Rate during Accelerating Creep Stage and gamma Channel Thickness in Single Crystal Nickel-based Superalloy, CMSX-4
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Relation between Creep Rate during Accelerating Creep Stage and gamma Channel Thickness in Single Crystal Nickel-based Superalloy, CMSX-4

机译:单晶镍高超合金中加速蠕变阶段和伽马通道厚度蠕变率的关系,CMSX-4

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摘要

To elucidate the origin of the Onset of accelerating creep in a single crystal nickel-based superalloy, CMSX-4, the correlation between the creep rate during the accelerating creep stage and the thickness of gamma channel was investigated by using the single crystals crept at 1273K in a wide stress range of 100-400 MPa. The shape of gamma' phase and the thickness of gamma channel at the time of the onset of accelerating creep turn to different ones with decreasing the Stress. At the stress of 160 MPa, the cuboidal gamma' phase turns its shape to a rafted one. While at the stresses less than 160 MPa the rafted gamma' phase appears before the onset of accelerating creep. At the stresses higher than 250MPa, the cuboidal gamma' phase still remains. The correlation between the thickness of gamma channel, lambda _r, and the creep rate during the accelerating creep stage, d epsilon, was evaluated, and the following equation, d epsilon propor. to lambda _(gamma)~4 is proposed and confirmed in a wide stress range of 100-400 MPa, independent of the shape of gamma' phase. In addition, it was also confirmed that the radius of dislocation curvature within gamma channel of the crept specimens was proportional to the thickness of gamma channel defined by TEM. Consequently, the origin of the Onset of accelerating creep in a single crystal nickel-based superalloy was interpreted by the loss of creep resistance due to an increase in the thickness of gamma channel, lambda _(gamma).
机译:为了在单晶镍基超合金中阐明加速蠕变的起点,CMSX-4在加速蠕变阶段期间的蠕变率与γ通道的厚度之间的相关性进行研究,通过使用1273K悄悄进行在100-400 MPa的宽应力范围内。伽马相的形状和伽马通道的厚度在加速蠕变的开始时转向不同的曲线,随着减小的应力而转向不同的蠕变。在160MPa的应力下,立方体伽马相位将其形状转向褶皱。虽然在小于160MPa的压力下,在加速蠕变开始之前出现椽子的伽马相。在高于250MPa的压力下,立方体伽玛阶段仍然存在。评估γ通道,λ_R和蠕变率,D epsilon,D epsilon的蠕变率之间的相关性,以及以下等式,D epsilon求解器。提出并确认在100-400MPa的宽应力范围内并确认λ_(γ)〜4,与γ相似的形状无关。此外,还证实,爪式标本的γ通道内的位错曲率半径与由TEM定义的伽马通道的厚度成比例。因此,通过由于γ频道厚度的增加,抗蠕变性,抗蠕变性,抗蠕变性,抗蠕变性的超合金中的加速蠕变的起点。

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