铝化物
材料科学
铝化钛
涂层
扩散
正交晶系
氚
相(物质)
冶金
金属间化合物
单斜晶系
结晶学
复合材料
热力学
化学
晶体结构
合金
核物理学
有机化学
物理
作者
Michel Sassi,David J. Senor,Andrew M. Casella
标识
DOI:10.1021/acs.jpcc.3c01028
摘要
Surface coatings of steels used in extreme conditions and corrosive environments generally aim to provide protection and increased durability. In the case of tritium-producing burnable absorber rods (TPBARs) used in nuclear reactors, a 316 stainless steel has been coated with Al. Scanning transmission electron microscopy (STEM) characterization of the coating found three Al-rich (>60 atom % Al) iron aluminide alloys identified as hexagonal FeNiAl<sub>5</sub>, monoclinic Fe<sub>4</sub>Al<sub>13</sub>, and orthorhombic Fe<sub>2</sub>Al<sub>5</sub>. Density functional theory simulations using nudged elastic band have been performed to investigate the diffusion of interstitial tritium in each Al-rich iron aluminide phase. While FeNiAl<sub>5</sub> and Fe<sub>4</sub>Al<sub>13</sub> can be viewed as the stacking of two layers, the structural peculiarity of Fe<sub>2</sub>Al<sub>5</sub> is that channels of variable Al vacancy content are present along the c-axis. Therefore, three stoichiometries for Fe<sub>2</sub>Al<sub>x</sub> phase, namely, Fe<sub>2</sub>Al<sub>4</sub>, Fe<sub>2</sub>Al<sub>5</sub>, and Fe<sub>2</sub>Al<sub>6</sub>, have been considered to evaluate the impact of Al vacancy concentration on tritium diffusion behavior. Altogether, we found that at 600 K, tritium diffusion decreases from a faster rate in the channels of Fe<sub>2</sub>Al<sub>x</sub> phases (D<sub>T</sub> ≤ 10<sup>–11</sup> m<sup>2</sup>·s<sup>–1</sup>) to Fe<sub>4</sub>Al<sub>13</sub> (D<sub>T</sub> ≈ 10–12 m2·s–1), and finally in FeNiAl5 (D<sub>T</sub> ≈ 10<sup>–13</sup> m<sup>2</sup>·s<sup>–1</sup>). Here, we also find that interstitial tritium generally diffuses faster in Fe–Al coating phases than in the tritium breeding material γ-LiAlO<sub>2</sub> (D<sub>T</sub> ≈ 10<sup>–14</sup> m<sup>2</sup>·s<sup>–1</sup>) but slightly slower than in 316 stainless steel (D<sub>T</sub> ≈ 10<sup>–10</sup> m<sup>2</sup>·s<sup>–1</sup>).
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