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首页> 外文期刊>Surface & Coatings Technology >Stability of expanded austenite, generated by ion carburizing and ion nitriding of AISI 316L SS, under high temperature and high energy pulsed ion beam irradiation
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Stability of expanded austenite, generated by ion carburizing and ion nitriding of AISI 316L SS, under high temperature and high energy pulsed ion beam irradiation

机译:AISI 316L SS的离子渗碳和离子渗氮在高温高能脉冲离子束辐照下产生的膨胀奥氏体稳定性

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摘要

Expanded austenite can be generated on austenitic stainless steels either by ion carburizing or ion nitriding. In both cases the resulting fcc crystal structure, supersaturated with nitrogen or carbon, is strongly hardened with improved wear-resistance, while maintaining the original resistance to corrosion. In this work, we have studied the stability of expanded austenite, generated by ion nitriding and ion carburizing on AISI 316L SS with N and C, under: a-high temperature (225 °C - 504 °C), and b-under irradiation with high energy (30 keV - 500 keV), high fluence (~10~(15) cm~(?2)), short duration (~400 ns) light (deuterium and helium) ion beams. It was found that expanded austenite is stable below 325 °C. Between 325 °C and 504 °C expanded austenite lattice parameter presents gradual reductionwith increasing temperature.We observedmicrostructural changes related only to the temperature treatment. We did not observe any microstructure change due to the duration of the heat treatment. Over 504 °C, the lattice parameter returns to the material's austenite original parameter. On the other hand,when irradiated with pulsed ion beams, a gradual reduction of the lattice parameter corresponding to the expanded austenite with the number of pulseswas observed. This behavior can be explained through the thermal shock induced on the surface by each beam, consisting in fast heating followed by fast cooling that induces the gradual exo-diffusion ofN(or C).Nevertheless, after 20 ion pulses, a final lattice parameter slightly higher than the corresponding to the original austenite was found as stable limit. This residual expansion can be attributed to partial amorphization of the first few micrometers that induces stresses on the crystals of austenite which are closer to the surface layers.
机译:奥氏体不锈钢可以通过离子渗碳或离子渗氮生成膨胀奥氏体。在这两种情况下,生成的fcc晶体结构都被氮或碳过饱和,在增强了耐磨性的同时,也得到了牢固的硬化,同时又保持了最初的耐腐蚀性能。在这项工作中,我们研究了在a-高温(225°C-504°C)和b-辐射下在AISI 316L SS上使用氮和碳进行离子渗氮和离子渗碳产生的膨胀奥氏体的稳定性。具有高能量(30 keV-500 keV),高通量(〜10〜(15)cm〜(?2)),短时间(〜400 ns)的光(氘和氦)离子束。发现膨胀奥氏体在325℃以下是稳定的。在325°C至504°C之间,奥氏体晶格参数随温度升高而逐渐减小。我们观察到仅与热处理有关的显微组织变化。由于热处理的持续时间,我们没有观察到任何微观结构的变化。在504°C以上,晶格参数返回到材料的奥氏体原始参数。另一方面,当用脉冲离子束照射时,观察到与扩展奥氏体相对应的晶格参数随着脉冲数而逐渐减小。这种现象可以通过每束电子束在表面上引起的热冲击来解释,包括快速加热然后快速冷却,引起N(或C)的逐渐外扩散。然而,在20个离子脉冲之后,最终的晶格参数略有下降高于相应的原始奥氏体被发现是稳定的极限。该残余膨胀可归因于前几个微米的部分非晶化,该非晶化在更接近表面层的奥氏体晶体上引起应力。

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