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Oxidation of FeCrAl alloy: influence of temperature and atmosphere on scale growth rate and mechanism

机译:FeCrAl合金的氧化:温度和气氛对氧化皮生长速率和机理的影响

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The oxidation behaviour of a FeCrAl alloy with little rare earth content (Y = 0.01 wt.%) was investigated. Specimens of this alloy were submitted to long-term oxidation treatments (up to 30 days) at 900 and 1200 degreesC, under gaseous atmospheres containing 21, 10 and 2 vol.% of O-2. The weight gain for unit area was measured vs. oxidation time. The alumina scale growth was found to occur, at least during the first days of treatment, according to Wagner's parabolic law. Afterwards, the layer rate growth decreases down to that expected on the basis of this law. The values of the parabolic rate constant for scale growth (K-p) chiefly depended on the treatment temperature, while only small variations of K-p, resulted from significant changes in treatment of atmosphere composition. The morphology and the composition of surface layers were studied by SEM-EDS and XRD analyses. Whatever the treatment temperature, the surface layer contained alpha -Al2O3 and non-negligible amounts of Cr and Fe. The metal/scale interface was always flat, while the morphology of the scale/gas interface changed greatly with temperature. At 900 degreesC an irregular scale/gas interface formed; this was characterised by the presence of long alpha -alumina whiskers protruding towards the gaseous atmosphere. Contrary, at 1200 degreesC a flat scale/gas interface was observed. These different morphologies can be attributed to different mechanisms of layer growth. (C) 2001 Elsevier Science B.V. All rights reserved. [References: 17]
机译:研究了稀土含量很少(Y = 0.01 wt。%)的FeCrAl合金的氧化行为。在含有21、10和2%(体积)O-2的气体气氛下,该合金的样品在900和1200℃下进行了长期氧化处理(长达30天)。测量单位面积的重量增加对氧化时间。根据瓦格纳的抛物线定律,至少在处理的第一天,氧化铝的生长就出现了。此后,层速率增长降低到根据该法则所预期的速度。垢生长的抛物线速率常数(K-p)的值主要取决于处理温度,而大气成分的处理发生显着变化则仅导致K-p的很小变化。通过SEM-EDS和XRD分析研究了表面层的形态和组成。无论处理温度如何,表面层均含有α-Al2O3和不可忽略的Cr和Fe。金属/水垢界面总是平坦的,而水垢/气体界面的形态随温度变化很大。在900摄氏度时,形成了不规则的水垢/气体界面;其特征在于存在向气体气氛突出的长α-氧化铝晶须。相反,在1200℃下观察到平坦的水垢/气体界面。这些不同的形态可以归因于层生长的不同机制。 (C)2001 Elsevier Science B.V.保留所有权利。 [参考:17]

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