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 γ Channel Thickness in Single Crystal Nickel-based Superalloy, CMSX-4
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Relation between Creep Rate during Accelerating Creep Stage and γ Channel Thickness in Single Crystal Nickel-based Superalloy, CMSX-4

机译:CMSX-4单晶镍基高温合金蠕变阶段蠕变速率与γ通道厚度的关系

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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 γ' channel was investigated by using the single crystals crept at 1273K in a wide stress range of 100-400 MPa. The shape of γ' phase and the thickness of γ 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 γ' phase turns its shape to a rafted one. While at the stresses less than 160 MPa the rafted γ' phase appears before the onset of accelerating creep. At the stresses higher than 250 MPa, the cuboidal γ' phase still remains. The correlation between the thickness of γ channel, λ{sub}γ, and the creep rate during the accelerating creep stage, ε, was evaluated, and the following equation, ε{top}.∝(λ{sub}γ){sup}4 is proposed and confirmed in a wide stress range of 100-400 MPa, independent of the shape of γ' phase. In addition, it was also confirmed that the radius of dislocation curvature within γ channel of the crept specimens was proportional to the thickness of γ 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 γ channel, λ{sub}γ.
机译:为了阐明单晶镍基高温合金CMSX-4加速蠕变的起源,通过使用蠕变速率为5%的单晶研究了加速蠕变阶段蠕变速率与γ'通道厚度之间的相关性。在100-400 MPa的宽应力范围内为1273K。随着应力的减小,加速蠕变开始时的γ'相形状和γ通道厚度会变为不同的形状。在160 MPa的应力下,长方体γ'相的形状变成筏状。当应力小于160 MPa时,在加速蠕变开始之前就出现了γ'筏相。在高于250 MPa的应力下,仍然存在长方体γ'相。评估了γ通道的厚度λ{sub}γ与加速蠕变阶段ε的蠕变速率之间的相关性,并通过以下方程ε{top} .∝(λ{sub}γ){sup提出并证实了44,其应力范围为100-400 MPa,与γ'相的形状无关。另外,还证实了蠕变样品的γ通道内的位错曲率半径与TEM确定的γ通道的厚度成比例。因此,单晶镍基高温合金中加速蠕变开始的原因是由于γ通道λ{sub}γ的厚度增加而引起的抗蠕变性的降低。

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