Hydrogen accumulation around dislocation loops and edge dislocations: from atomistic to mesoscopic scales in BCC tungsten

In a fusion tokamak, the plasma interacts with the metallic wall and the divertor. Hydrogen isotopes penetrate and diffuse into the material and interact with defects where they are trapped. Neutrons produced by the fusion reactions in the plasma are stopped in the material, creating defects, includ...

Full description

Saved in:
Bibliographic Details
Published inPhysica scripta Vol. T170; no. 1; pp. 14073 - 14083
Main Authors De Backer, A, Mason, D R, Domain, C, Nguyen-Manh, D, Marinica, M-C, Ventelon, L, Becquart, C S, Dudarev, S L
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.12.2017
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:In a fusion tokamak, the plasma interacts with the metallic wall and the divertor. Hydrogen isotopes penetrate and diffuse into the material and interact with defects where they are trapped. Neutrons produced by the fusion reactions in the plasma are stopped in the material, creating defects, including vacancy and interstitial clusters, and dislocation loops. The trapping of hydrogen in vacancies has been extensively investigated. In our recent paper (De Backer et al 2017 Nucl. Fusion), we proposed a multi-scale model for H trapping and accumulation around interstitial defects, dislocation loops and dislocation lines. These defects create a long-range elastic field that attracts and may retain H atoms. A two-shell model with a short-range core region and a long-range elastic shell has been parameterized using a database of density functional theory (DFT) calculations. This model gives the number of H atoms forming the Cottrell atmosphere of a defect at finite temperature. In this paper, we present new DFT calculations of large dislocation loops decorated with up to 80 H, and explore our two-shell model in fusion relevant conditions. We conclude that large dislocation loops and edge dislocations can trap a significant number of hydrogen atoms in the core at temperatures up to 800 K, and also in the elastic field if the background hydrogen concentration is high.
Bibliography:Royal Swedish Academy of Sciences
PHYSSCR-106092.R2
ISSN:0031-8949
1402-4896
DOI:10.1088/1402-4896/aa9400