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首页> 外文期刊>Metallurgical and Materials Transactions, A. Physical Metallurgy and Materials Science >Fatigue-Crack Growth in Ti-6A1-4V-0.1Ru in Air and Seawater: Part I. Design of Experiments, Assessment, and Crack- Growth-Rate Curves
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Fatigue-Crack Growth in Ti-6A1-4V-0.1Ru in Air and Seawater: Part I. Design of Experiments, Assessment, and Crack- Growth-Rate Curves

机译:空气和海水中Ti-6A1-4V-0.1Ru的疲劳裂纹扩展:第一部分。实验设计,评估和裂纹扩展速率曲线

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摘要

Fatigue-crack growth rates for different simulated ocean environments and loading conditions have been investigated for beta-annealed Ti-6A1-4V-0.lRu (extra-low interstitials, (ELI)), a candidate material for oil production risers; the focus was on uncovering whether certain combinations of conditions could produce unexpectedly high crack growth rates. A two-level, one-quarter-fraction factorial design-of-experiments (DOE) approach was used to ascertain which testing variables and environmental conditions warranted further study. This study used eight different combinations of variables: parent/deformed material, 27 deg C/85 deg C temperature, 2 Hz/20 Hz loading frequency, 0.1/0.6 load ratio (R = #sigma#_(min)/#sigma#_(max), where #sigma#_(min) is the minimum and #sigma#_(max) is the maximum stress during a fatigue cycle), and aerated/deaerated seawater. Comparisons were based on crack growth rates at #DELTA#K = 17 MPa m~(1/2), roughly the middle of the Paris portion of the da/dN vs #DELTA#K curves. The da/dN vs #DELTA#K curves were also examined, and conclusions based upon these data were compared with those from the DOE. Consideration of the microstructure's influence on the crack path is postponed until Part II of this article. Samples tested at the higher load ratio showed a statistically significant increase in the crack propagation rate compared to those tested at R = 0.1; the same was true of specimens tested at 20 Hz vs those tested at 2 Hz, but the level of significance was lower. The parent material had somewhat higher crack growth rates than the deformed samples. Changes in environmental conditions other than frequency produced little effect on the crack growth rate. Comparison of crack growth rates over the #DELTA#K range measured revealed details that would have not been uncovered in comparisons at a single #DELTA#K value. The Paris exponent ranged between 3.7 and 6.7, and the only systematic variation observed was an increase in the exponent with increasing test frequency. In seawater, cold work (a 5 pct reduction in thickness by rolling) reduced fatigue-crack growth rates by a factor of 2 (compared to the parent material) at intermediate and high #DELTA#K values. There was a crossover of crack growth rates for low #DELTA#K values: below 10 MPa m~(1/2), growth rates were lower for the parent material than for the cold-rolled material, suggesting a higher #DELTA#K_(th) for the parent material, while above this value, fatigue cracks grew more rapidly in the parent material than in the cold-rolled material. Crack growth rates were slightly higher in seawater than in air, but only slightly more than the sample-to-sample variation of crack growth rates, and cold work reduced fatigue-crack growth rates in air by about the same amount as in seawater. Somewhat more scatter was observed for the R = 0.1 tests than for the R = 0.6 tests. Differences in temperature (27 deg C, 53 deg C, and 85 deg C) do not appear to affect fatigue-crack growth rates. For #DELTA#K < 20 MPa m~(1/2), crack growth rates were similar for 0.2 and 2 Hz but were higher for 20 Hz; above 20 MPa m~(1/2) the crack growth rates were similar for all three frequencies.One explanation for the unusual frequency dependence relies on the possibility that the environment produces different amounts of closure for different test frequencies. According to this view, closure is effective in air and in seawater at 0.2 and 2 Hz but not at 20 Hz: perhaps the higher loading rate breeches the passive layer at a rate more rapid than it can reform. Because the crack growth rate appeared independent of temperature, it is unlikely that there is a significant influence of thermally activated corrosion-fatigue mechanisms for the conditions tested.The results demonstrate that beta-annealed Ti-6V-4A1-0.lRu (ELI) possesses a robust response to the combinations of environment and loading expected in oil production riser service. The value of the DOE approach was clear, and supple
机译:已经对β-退火的Ti-6A1-4V-0.lRu(极低间隙,ELI)(一种石油生产立管的候选材料)进行了研究,研究了不同模拟海洋环境和载荷条件下的疲劳裂纹增长率。重点在于揭示某些条件的组合是否会产生出乎意料的高裂纹增长率。实验采用两级,四分之一分数阶乘设计(DOE)方法来确定哪些测试变量和环境条件值得进一步研究。这项研究使用了八种不同的变量组合:母体/变形材料,27摄氏度/ 85摄氏度温度,2 Hz / 20 Hz加载频率,0.1 / 0.6加载比率(R = #sigma #_(min)/#sigma# _(max),其中#sigma #_(min)是最小值,而#sigma #_(max)是疲劳周期中的最大应力),以及充气/脱气的海水。比较是基于在#DELTA#K = 17 MPa m〜(1/2)时的裂纹扩展速率,大约在da / dN与#DELTA#K曲线的巴黎部分的中间。还检查了da / dN与#DELTA#K曲线,并将基于这些数据的结论与DOE的结论进行了比较。微观结构对裂纹路径的影响的考虑被推迟到本文的第二部分。与在R = 0.1的情况下进行测试的样品相比,在更高的负载比下进行测试的样品显示出裂纹扩展速率的统计显着提高。在20 Hz下测试的标本与在2 Hz下测试的标本相同,但显着性水平较低。母材具有比变形样品更高的裂纹扩展速率。除了频率以外,环境条件的变化对裂纹扩展速率的影响很小。在#DELTA#K范围内测量的裂纹扩展速率的比较揭示了在单个#DELTA#K值的比较中未发现的细节。巴黎指数介于3.7和6.7之间,观察到的唯一系统变化是随着测试频率的增加,指数增加。在海水中,冷加工(通过轧制可将厚度降低5%)在#DELTA#K中值和较高值下,疲劳裂纹的生长速度降低了2倍(与母材相比)。低#DELTA#K值存在裂纹扩展速率的交叉:低于10 MPa m〜(1/2),母材的生长速率低于冷轧材料,表明#DELTA#K_较高(th)对于母材,尽管高于该值,疲劳裂纹在母材中的增长比在冷轧材料中更快。海水中的裂纹增长率比空气中的裂纹增长率稍高,但仅比裂纹增长率的样品间差异稍大,而冷作则使空气中的疲劳裂纹增长率与海水中的裂纹增长率几乎相同。 R = 0.1测试比R = 0.6测试观察到的散射更大。温度差异(27摄氏度,53摄氏度和85摄氏度)似乎不会影响疲劳裂纹的生长速度。当#DELTA#K <20 MPa m〜(1/2)时,裂纹扩展速率在0.2和2 Hz时相似,但在20 Hz时更高。在20 MPa m〜(1/2)以上时,所有三个频率的裂纹扩展速率都相似。一种对异常频率依赖性的解释取决于环境对于不同测试频率产生不同封闭量的可能性。根据这种观点,封闭在空气和海水中在0.2和2 Hz时有效,但在20 Hz时则无效:也许更高的负载速率使钝化层以比其能够重新形成的速率更快的速度使钝化层变质。由于裂纹扩展速率似乎与温度无关,因此热活化腐蚀疲劳机理不太可能对测试条件产生重大影响。结果表明,β退火Ti-6V-4A1-0.lRu(ELI)对石油生产立管服务中预期的环境和负荷的组合具有强大的响应能力。 DOE方法的价值是清晰而柔软的

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