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Slow Strain Rate Tensile Test Properties of Iron-Based Superalloy SUH660 in Hydrogen Gas

机译:铁基高温合金SUH660在氢气中的慢应变速率拉伸试验性能

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To investigate dependence of strain rate of tensile test for iron-based superalloy SUH660 (A286), tensile tests were conducted for the specimens in 70 MPa hydrogen gas and air at 150°C. Nominal stress-nominal strain curve of each strain rate in 70 MPa hydrogen gas showed same behavior to maximum load via yield point in comparison with that in air, however, each elongation at breaking point in 70 MPa hydrogen was a little shorter than that in air. The values of tensile strength didn’t depend on the strain rate in 70 MPa hydrogen as well as those in air. In addition, the difference in tensile strength wasn’t observed between that in 70 MPa hydrogen gas and that in air for the strain rate. However, it’s proved that relative reduction of area in 70 MPa hydrogen to that in air was significantly affected by strain rate of tensile test. Those values were 80%, 51%, and 32% in the case of strain rate 5.0×10~(?5), 7.5×10~(?6), and 1.25×10~(?6) s~(?1), respectively. The morphology of fracture surface also changed from dimple to quasi-cleavage (QC), with a decrease in strain rate. Simulation of hydrogen gas diffusion from surface to inside during experiment showed that the hydrogen diffusion layer of specimen with QC fracture surface (RRA 51%, strain rate 7.5×10~(?6) s~(?1)) was only 0.25 mm in depth. That implies that hydrogen content at crack tips is much higher than that of simulation due to hydrogen concentration by a couple of defects. That tendency seems to become stronger with a decrease in strain rate.
机译:为了研究铁基高温合金SUH660(A286)的拉伸试验应变速率的依赖性,在70 MPa的氢气和150°C的空气中对样品进行了拉伸试验。与空气相比,在70 MPa氢气中每种应变速率的标称应力-标称应变曲线通过屈服点对最大载荷具有相同的行为,但是,在70 MPa氢气中,断裂点的每个伸长率都比空气中的短。拉伸强度的值并不取决于在70 MPa氢气和空气中的应变率。另外,对于应变率,在70 MPa的氢气中与在空气中的拉伸强度之间没有观察到差异。但是,事实证明,拉伸试验的应变速率显着影响了70 MPa氢气相对于空气中氢气的相对减少量。在应变率5.0×10〜(?5),7.5×10〜(?6),1.25×10〜(?6)s〜(?1)的情况下,分别为80%,51%,32%。 ), 分别。断裂表面的形态也从酒窝变为准裂解(QC),应变率降低。在实验过程中氢气从表面到内部的扩散模拟表明,具有QC断裂表面(RRA为51%,应变率7.5×10〜(?6)s〜(?1))的试样的氢扩散层在0.25 mm内。深度。这意味着由于几个缺陷引起的氢浓度,裂纹尖端的氢含量比模拟的要高得多。随着应变率的降低,这种趋势似乎变得更加强烈。

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