Synergistic effect of helium and hydrogen for bubble swelling in reduced-activation ferritic/martensitic steel under sequential helium and hydrogen irradiation at different temperatures

被引:40
作者
Hu, Wenhui [1 ,2 ]
Guo, Liping [1 ,2 ]
Chen, Jihong [1 ,2 ]
Luo, Fengfeng [1 ,2 ]
Li, Tiecheng [1 ,2 ]
Ren, Yaoyao [3 ]
Suo, Jinping [4 ]
Yang, Feng [4 ]
机构
[1] Wuhan Univ, Minist Educ, Hubei Nucl Solid Phys Key Lab, Key Lab Artificial Micro & Nanostruct, Wuhan 430072, Peoples R China
[2] Wuhan Univ, Sch Phys & Technol, Wuhan 430072, Peoples R China
[3] Wuhan Univ, Ctr Electron Microscopy, Wuhan 430072, Peoples R China
[4] Huazhong Univ Sci & Technol, Inst Mat Sci & Engn, State Key Lab Mould Technol, Wuhan 430074, Peoples R China
基金
中国国家自然科学基金;
关键词
Reduced-activation ferritic/martensitic steel; Helium bubbles; Helium/hydrogen synergistic effect; Swelling; MECHANICAL-PROPERTIES; MARTENSITIC STEELS; DEUTERIUM; DYNAMICS; DEFECTS; ACCUMULATION; SIMULATION; DIFFUSION;
D O I
10.1016/j.fusengdes.2014.02.033
中图分类号
TL [原子能技术]; O571 [原子核物理学];
学科分类号
0827 ; 082701 ;
摘要
In order to investigate the synergistic effect of helium and hydrogen on swelling in reduced-activation ferritic/martensitic (RAFM) steel, specimens were separately irradiated by single He+ beam and sequential He+ and H+ beams at different temperatures from 250 to 650 degrees C. Transmission electron microscope observation showed that implantation of hydrogen into the specimens pre-irradiated by helium can result in obvious enhancement of bubble size and swelling rate which can be regarded as a consequence of hydrogen being trapped by helium bubbles. But when temperature increased, Ostwald ripening mechanism would become dominant, besides, too large a bubble could become mobile and swallow many tiny bubbles on their way moving, reducing bubble number density. And these effects were most remarkable at 450 degrees C which was the peak bubble swelling temperature for RAMF steel. When temperature was high enough, say above 450, point defects would become mobile and annihilate at dislocations or surface. As a consequence, helium could no longer effectively diffuse and clustering in materials and bubble formation was suppressed. When temperature was above 500, helium bubbles would become unstable and decompose or migrate out of surface. Finally no bubble was observed at 650 degrees C. (c) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:324 / 328
页数:5
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