Microstructure response of ferritic/martensitic steel HT9 after neutron irradiation: Effect of temperature

JOURNAL OF NUCLEAR MATERIALS

卷:528

Article

Zheng, Ce¹  Reese, Elaina R.²  Field, Kevin G.³  Liu, Tian²  Marquis, Emmanuelle A.²  Maloy, Stuart A.⁴  Kaoumi, Djamel¹ 

[1] North Carolina State Univ, Dept Nucl Engn, Raleigh, NC USA

[2] Univ Michigan, Dept Mat Sci & Engn, Ann Arbor, MI 48109 USA

[3] Oak Ridge Natl Lab, Mat Sci & Technol Div, Oak Ridge, TN USA

[4] Los Alamos Natl Lab, Mat Sci & Technol Div, Los Alamos, NM USA

关键词: Ferritic/martensitic steels;    Neutron irradiation;    Microstructure;    Swelling;    Precipitation;    Segregation;   

DOI  :  10.1016/j.jnucmat.2019.151845

来源: Elsevier

【 摘 要 】

The ferritic/martensitic steel HT9 was irradiated in the BOR-60 reactor at 650, 690 and 730 K (377, 417 and 457 degrees C) to doses between similar to 14.6-18.6 displacements per atom (dpa). Irradiated samples were comprehensively characterized using analytical scanning/transmission electron microscopy and atom probe tomography, with emphasis on the influence of irradiation temperature on microstructure evolution. Mn/Ni/Si-rich (G-phase) and Cr-rich (alpha') precipitates were observed within martensitic laths and at various defect sinks at 650 and 690 K (377 and 417 degrees C). For both G-phase and alpha' precipitates, the number density decreased while the size increased with increasing temperature. At 730 K (457 degrees C), within martensitic laths, a very low density of large G-phase precipitates nucleating presumably on dislocation lines was observed. No alpha' precipitates were observed at this temperature. Both a < 100 > and a/2 < 111 > type dislocation loops were observed, with the a < 100 > type being the predominant type at 650 and 690 K (377 and 417 degrees C). On the contrary, very few dislocation loops were observed at 730 K (457 degrees C), and the microstructure was dominated by a/2 < 111 > type dislocation lines (i.e., dislocation network) at this temperature. Small cavities (diameter < 2 nm) were observed at all three temperatures, whereas large cavities (diameter > 2 nm) were observed only at 690 K (417 degrees C), resulting in a bimodal cavity size distribution at 690 K (417 degrees C) and a unimodal size distribution at 650 and 730 K (377 and 457 degrees C). The highest swelling (%) was observed at 690 K (417 degrees C), indicating that the peak of swelling happens between 650 and 730 K (377 and 457 degrees C). Published by Elsevier B.V.

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