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Hydrogen Desorption Behavior of Pure Iron and Inconel 625 during Elastic and Plastic Deformation

机译:纯铁和Inconel 625在弹性和塑性变形过程中的氢解吸行为

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The hydrogen desorption behavior of pure iron with a body-centered-cubic (BCC) lattice and Inconel 625 with a face-centered-cubic (FCC) lattice was examined during tensile deformation using a quadrupole mass spectrometer in a vacuum chamber integrated with a tensile testing machine. Hydrogen and water desorption was continuously detected simultaneously under the application of a tensile load and strain to the specimens. Hydrogen desorption promoted by tensile deformation can be found by deducting both fragment hydrogen dissociated from H_(2)O and H_(2) desorbed under unloading from the total amount of hydrogen desorbed from hydrogen-charged specimens during tensile deformation. Hydrogen desorption from hydrogen-charged specimens was detected under various strain rates of 4.2×10~(?5)/s, 4.2×10~(?4)/s and 4.2×10~(?3)/s. Hydrogen desorption rarely increased under elastic deformation. In contrast, it increased rapidly at the proof stress when plastic deformation began, reached its maximum, and then decreased gradually with increasing applied strain for both pure iron and Inconel 625. This desorption behavior is closely related to hydrogen dragging by moving dislocations. The amount of desorbed hydrogen promoted by tensile deformation was measured by thermal desorption analysis (TDA). The TDA results showed that the amount of desorbed hydrogen differed at each strain rate. The largest amount of desorbed hydrogen promoted by tensile deformation was 16% of the initial hydrogen content in pure iron with a high hydrogen diffusion rate when the specimen was deformed at a strain rate of 4.2×10~(?4)/s. In contrast, that of Inconel 625 with a low hydrogen diffusion rate was 9% of the initial hydrogen content when the alloy was deformed at a strain rate of 4.2×10~(?6)/s. This difference in the amount of desorbed hydrogen transported by dislocations depends on the balance between the hydrogen diffusion rate and mobile dislocation velocity.
机译:在拉伸变形过程中,使用四极质谱仪在集成有拉伸力的真空室中检查了具有体心立方(BCC)晶格的纯铁和具有面心立方(FCC)晶格的Inconel 625的氢脱附行为。测试机。在向样品施加拉伸载荷和应变的同时,连续检测到氢气和水的解吸。拉伸变形促进的氢解吸可以通过从拉伸变形过程中从充氢试样中解吸的氢总量中减去从卸荷的H_(2)O和H_(2)解离的碎片氢中扣除。在4.2×10〜(?5)/s、4.2×10~(?4)/ s和4.2×10〜(?3)/ s的各种应变速率下检测到充氢样品中的氢解吸。在弹性变形下氢的解吸很少增加。相反,当纯铁和Inconel 625施加塑性应变时,当塑性变形开始时,它在屈服应力下迅速增加,达到最大值,然后逐渐减小。这种解吸行为与移动位错引起的氢拖动密切相关。通过热脱附分析(TDA)来测量由拉伸变形促进的脱附氢的量。 TDA结果表明,在每种应变速率下,脱附的氢量不同。当试样以4.2×10〜(?4)/ s的应变速率变形时,拉伸变形促进的最大脱附氢量为纯铁中初始氢含量的16%,且氢扩散率高。相反,当合金以4.2×10 6(s 6)/ s的应变速率变形时,具有低氢扩散率的Inconel 625的氢为初始氢含量的9%。通过位错传输的解吸氢的量的这种差异取决于氢扩散速率和移动位错速度之间的平衡。

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