12% CrMoV钢蠕变裂纹扩展及空化损伤

C. Wiesner, J.C. Earthman, G. Eggeler , B. Ilschner
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引用次数: 14

摘要

研究了一种12% CrMoV钢在650°C高温下的蠕变裂纹扩展,分别在接近平面应变和平面应力条件下,在带和不带侧槽的send试样中进行。实验在不同的加载条件下进行,包括恒定的C *, j积分速率参数。裂纹扩展行为的转变是在裂纹扩展的早期观察到的,当裂纹相对于试样宽度变长时观察到的。早期转变以裂纹尖端之前的空化损伤的初始发展为主。一旦这种转变完成,C *与裂纹扩展速率之间的相关性就变得有效。这种相关性与加载条件无关,它与理论预期相吻合,并且在第二次过渡之前是有效的,在第二次过渡中,损伤程度对裂纹尖端前面的应力场具有主要影响。在相同的C∗值下,我们观察到一个趋势,即在光滑面试件中裂纹的扩展比在侧槽试件中裂纹的扩展要慢。金相研究表明,裂纹扩展是通过裂纹尖端前面的空洞和微裂纹的形成和扩展而发生的。对光滑面和侧槽试件的损伤比较表明,在相同的C∗值下,平面应力条件下的蠕变损伤要比平面应变条件下的蠕变损伤广泛得多。这种差异是由于侧槽产生的多轴应力场影响了材料中的空化和微裂纹的形成。这也解释了光滑面试样中较小的裂纹扩展速率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Creep crack growth and cavitation damage in a 12% CrMoV steel

Creep crack growth of a 12% CrMoV steel has been investigated at 650°C in SENT specimens with and without side-grooves approaching plane strain and plane stress conditions respectively. Experiments have been conducted under different loading conditions including constant C, the J-integral rate parameter. Transitions in crack growth behaviour are observed early in the crack growth and later when the crack becomes long with respect to the specimen width. The early transition is dominated by the initial development of cavitation damage ahead of the crack tip. Once this transition is complete, the correlation between C and the crack growth rate becomes valid. This correlation is independent of loading conditions, it coincides with theoretical expectations and it is valid until the second transition where the extent of damage has a dominant influence on the stress field ahead of the crack tip. A trend has been observed that crack growth is slower in smooth-sided specimens as compared to the crack growth in side-grooved specimens for the same value of C. Metallographic investigations indicate that crack growth occurs by the formation and growth of cavities and microcracks ahead of the crack tip. A comparison of the damage in smooth-sided and side-grooved specimens shows that creep damage is much more extensive under plane stress conditions than under plane strain conditions for the same value of C. This difference is due to the multiaxial stress field, produced by the side-grooves, which influences cavitation and microcrack formation in the material. It also accounts for the smaller crack growth rates in smooth-sided specimens.

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