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Influence of Structure—Phase State of Nb Containing Zr Alloys on Irradiation-Induced Growth

机译:含Nb含Nb结构相位态的影响对辐照诱导的生长

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On account of the search for the optimal composition and structure-phase state of Zr alloys much attention is paid to upgrade the E110 (Zr-1%Nb) and E635 (Zr-1%Nb-0.35%Fe-1.2%Sn) alloys that have proved well in terms of irradiation-induced creep and growth, high strength characteristics, and corrosion. The difference between the alloy properties is determined by their states related to their compositions. The structure-phase state of the Zr-Nb and Zr-Nb-Fe-Sn systems has been studied after heat treatment in the α-- and α + β- regions and its influence on the irradiation-induced growth (IIG) during BOR-60 irradiation at T = 315-350°C was investigated. A substantial difference has been shown in the deformation effected by IIG of those alloys; it is less for Zr-Nb-Fe-Sn alloys in dissimilar structure-phase states. The incubation period of the accelerated growth stage is determined by the α-matrix composition, the phase state and the initial dislocation structure. Neutron irradiation leads to a redistribution of alloying elements between the matrix and the precipitates, and to changes in the α-solid solution composition. These changes affect accumulation and mobility of irradiation defects, anisotropy and formation of vacancy c-component dislocation loops. The appearance of c-loops usually correlates with an axial direction acceleration of the IIG of tubes conforming to their texture. The basic regularities of the phase transformation have been established: a) β-Nb precipitates in Zr-Nb alloys are altered in composition to reduce the Nb content from 85-90% to ~ 50%, fine precipitates likely enriched in Nb are formed; b) β-Zr precipitates are subject to irradiation-stimulated decomposition; c) Laves phase precipitates change composition (the content of Fe decreases) and crystal structure, HCP to BCC (β-Nb); d) (Zr,Nb)_2Fe precipitates having the FCC lattice retain their composition and crystal structure; e) no amorphization of any secondary phase precipitates is observable under the given conditions of irradiation (T = 315-350°C). Based on the dpa, the results were compared pertaining to Zr-alloy IIG deformation vs. fluence in various reactors at different energies of fast neutrons. The presented graphs enable comparison between the results of numerous experiments and enable predictions of Zr-material behavior in long-term operation and at high burn-up in commercial reactors.
机译:由于搜索Zr合金的最佳组合物和结构相位状态,因此支付了升级E110(Zr-1%Nb)和E635(Zr-1%Nb-0.35%Fe-1.2%Sn)合金的升高在辐照诱导的蠕变和生长,高强度特征和腐蚀方面已经证明了很好。合金特性之间的差异由它们与其组合物相关的状态确定。已经在α--α+β-区域的热处理后研究了ZR-NB和ZR-NB-FE-SN系统的结构相位状态及其对硼期间辐照诱导的生长(IIG)的影响研究了T = 315-350℃的60辐射。在该合金的IIG的变形中显示了显着的差异;对于不同结构相位状态的Zr-Nb-Fe-Sn合金,较少。加速生长阶段的孵育周期由α-基质组合物,相位状态和初始位错结构决定。中子辐射导致基质和沉淀物之间的合金元素的再分配,并在α-固溶溶液组合物中的变化。这些变化会影响辐射缺陷,各向异性和空位C组分位错环的积累和移动性。 C-LOOPS的外观通常与符合其纹理的管的IIG的轴向加速度相关。已经建立了相变的基本规律:a)β-nb在Zr-Nb合金中沉淀物在组合物中改变,将Nb含量从85-90%降低至〜50%,形成细沉淀物形成在Nb中形成; b)β-Zr沉淀物受到辐照刺激的分解; c)Laves相位沉淀的变化组合物(Fe降低的含量)和晶体结构,HCP至BCC(β-NB); d)(Zr,Nb)_2Fe沉淀,使FCC晶格保持其组成和晶体结构; e)在给定的照射条件下,没有任何二次相沉淀物的无态的无态化(T = 315-350℃)。基于DPA,将结果与Zr-Alloy IIG变形与快速中子的不同能量的各种反应器中的流量进行比较。所提出的图表能够在许多实验结果之间进行比较,并在长期操作中能够在长期操作中预测Zr材料行为,并且在商业反应器中的高燃烧。

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