首页> 外文会议>Proceedings of International Conference on Structural Mechanics in Reactor Technology >DHC BEHAVIOUR OF IRRADIATED ZR-2.5NB PRESSURE TUBES UPTO 365°C
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DHC BEHAVIOUR OF IRRADIATED ZR-2.5NB PRESSURE TUBES UPTO 365°C

机译:高达365°C的辐照过的ZR-2.5NB压力管的DHC行为

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Under certain conditions, zirconium alloy pressure tubes in CANDU? reactors can be susceptible to amechanism of cracking called Delayed Hydride Cracking (DHC). The rate of initial crack penetration and propagation is typically low, and permits sufficient time for leak detection before an unstable crack length is obtained, termed Leak-Before-Break. Since the DHC velocity is temperature dependent, it is necessary to quantify the DHC velocity over the range of operating temperatures in order to confirm that the margins against unstable fracture are adequate to ensure Leak-Before-Break. The objective of the present work is to establish the DHC temperature dependence in irradiated material to a higher temperature than has been done previously. Theresults from an ex-service (irradiated) cold-worked Zr-2.5Nb pressure tube doped to a hydrogen isotope concentration of 153 wt ppm shows that between 150 and 325°C the DHC velocity follows an Arrhenius relationship. At temperatures higher than 325°C, the velocity deviates from the Arrhenius relationship, proceeding at much lower velocities until an upper temperature limit for DHC is achieved at about 365°C. Thephysical reason for the observed cessation temperature for DHC in this material, containing only 153 wt ppmhydrogen isotope, is thought to be due to insufficient hydrogen, making hydride nucleation at the crack tip impossible. It is expected that the strength-based DHC cessation temperature in irradiated material containing sufficient hydrogen would be higher.
机译:在一定条件下,CANDU中的锆合金压力管?反应堆可能容易受到 裂解的机理称为延迟氢化物裂解(DHC)。初始裂纹渗透和扩展的速率通常较低,并且在获得不稳定的裂纹长度(称为先泄漏后断裂)之前,有足够的时间进行泄漏检测。由于DHC速度与温度有关,因此有必要在工作温度范围内对DHC速度进行量化,以确认抗不稳定断裂的余量足以确保先泄漏后断裂。本工作的目的是建立被辐照材料中DHC的温度依赖性,使其达到比以前更高的温度。这 掺入氢同位素浓度为153 wt ppm的退役(辐射)冷加工Zr-2.5Nb压力管的测试结果表明,在150至325°C之间,DHC速度遵循Arrhenius关系。在高于325°C的温度下,速度偏离阿伦尼乌斯(Arrhenius)关系,以低得多的速度进行,直到在365°C左右达到DHC的最高温度极限为止。这 观察到该材料中DHC停止温度的物理原因,仅含有153 wt ppm 氢同位素被认为是由于氢不足而导致的,在裂纹尖端的氢化物成核不可能。可以预料,在含有足够氢的辐照材料中,基于强度的DHC停止温度会更高。

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