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Oxidation Mechanism in Zircaloy-2-The Effect of SPP Size Distribution

机译:Zircaloy-2-的氧化机理SPP尺寸分布的影响

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The metal/oxide interface region in Zircaloy-2 oxidized in autoclave was studied with transmission electron microscopy (TEM) and atom probe tomography. In addition to waviness on the micrometer scale the metal/oxide interface was found to have irregularities on a finer scale, and metal islands were found especially at metal hills (delayed parts of the oxidation front). The thickness of the sub-oxide layer varies considerably along the interface in the same sample, from 100 to virtually 0 nm. The sub-oxide composition may vary on a very fine scale (down to 5nm), and it can sometimes be a mixture of sub-oxides with different oxygen content. The metal matrix in contact with the sub-oxide is saturated with up to 32 at. % oxygen, and the oxygen diffusion profile in the metal is in approximate agreement with literature data for pure Zr. However, the diffusion length appears to be somewhat larger at interface metal hills than under valleys, probably for both geometrical and stress state reasons. Hydride precipitates, hardly visible in conventional TEM, give a good image contrast when employing high angle annular dark field imaging. A model for the oxidation process is presented, where the creep deformation of the metal close to the interface and the formation of lateral cracks in the oxide are of highest importance. The effect of second phase particle (SPP) size is suggested to be twofold: Small and numerous SPPs give a stronger metal and therefore higher stress in the oxide. Small SPPs also nucleate many more lateral cracks in the oxide, which gives a weaker oxide. Together this leads to formation of large cracks associated with transition in the oxidation rate at an earlier time than for a material with larger and fewer SPPs, and thereby a higher oxidation rate.
机译:用透射电子显微镜(TEM)和原子探针层析成像技术研究了在高压釜中氧化的Zircaloy-2中的金属/氧化物界面区域。除了在微米尺度上起伏之外,还发现金属/氧化物界面在更细的尺度上具有不规则性,并且尤其在金属山丘(氧化前沿的延迟部分)上发现了金属岛。亚氧化物层的厚度沿同一样品中的界面变化很大,从100纳米到几乎0纳米。所述次氧化物组成可以在非常细的范围内变化(低至5nm),并且有时可以是具有不同氧含量的次氧化物的混合物。与低价氧化物接触的金属基质最多饱和32 at。 %的氧,并且金属中的氧扩散曲线与纯Zr的文献数据大致一致。但是,可能由于几何和应力状态的原因,在界面金属山丘上的扩散长度似乎比在山谷下更大。当采用大角度环形暗场成像时,氢化物沉淀物(在常规TEM中几乎不可见)可提供良好的图像对比度。提出了一种氧化过程的模型,其中靠近界面的金属的蠕变变形和氧化物中的横向裂纹的形成是最重要的。建议第二相粒子(SPP)大小的影响是双重的:小而众多的SPP产生更强的金属,因此氧化物中的应力更高。小型SPP还会使氧化物中更多的横向裂纹成核,从而产生较弱的氧化物。与具有更大和更少SPP的材料相比,这一起导致在较早的时间形成与氧化速率转变有关的大裂纹,从而导致更高的氧化速率。

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