Phase transition in yttrium under shock compression by atomistic simulations

•A new reliable F-S potential of Y is developed and further validated under static and dynamic conditions.•The atomistic mechanism of HCP → Sm-type → DHCP → FCC phase transition is characterized by the minimum energy path for shock along the [10−10] direction.•Amorphization mediates the phase transi...

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Veröffentlicht in:International journal of mechanical sciences 2023-07, Vol.250, p.108330, Article 108330
Hauptverfasser: Liu, Beibei, Chen, Yangchun, Guo, Long, Li, Xiaofan, Wang, Kun, Deng, Huiqiu, Tian, Zean, Hu, Wangyu, Xiao, Shifang, Yuan, Dingwang
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Sprache:eng
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Zusammenfassung:•A new reliable F-S potential of Y is developed and further validated under static and dynamic conditions.•The atomistic mechanism of HCP → Sm-type → DHCP → FCC phase transition is characterized by the minimum energy path for shock along the [10−10] direction.•Amorphization mediates the phase transition process for the [0001] and [−12−10] shock directions, and then rapidly annihilates and recrystallizes to FCC lattices.•The uniaxial compression strains in the [0001] and [−12−10] shock directions inhibit the formation of Sm-type and DHCP phases. The insightful understanding of phase transition in rare earth elements under shock compression is significant to the future development of materials science. In this work, a new reliable Finnis-Sinclair interatomic potential for hexagonal close-packed (HCP) single crystal yttrium (Y) is developed and validated. The potential reproduces the phase transition sequence of HCP → Sm-type (samarium-type) → DHCP (double hexagonal-close-packed) → FCC (face-centered-cubic) of Y observed in high-pressure experiments. Further, large-scale NEMD simulations are conducted to study shock compression behaviors of Y. For the [10−10]HCP shock direction, the HCP → Sm-type phase transition occurs via an intermediate metastable BCC structure, which is accomplished by atomic shuffles and shear. Then, a pure-shear along the [10−10]Sm-type direction transforms the Sm-type to DHCP structure. Besides, we find FCC phase can be generated by shifting the atoms at two layers in opposite directions on {0001} planes in the DHCP lattice. Combined with the transition state theory, we confirm these transition pathways follow the minimum energy path. For shock along the [0001]HCP and [−12−10]HCP directions, the HCP → FCC phase transition is mediated by the amorphization which subsequently annihilates and turns to recrystallize to be FCC lattice. The results suggest that the uniaxial compression strain along the [0001]HCP and [−12−10]HCP directions hinders the formation of Sm-type and DHCP phases. Our findings provide essential insights into the phase transition behavior of Y under shock loading. [Display omitted]
ISSN:0020-7403
1879-2162
DOI:10.1016/j.ijmecsci.2023.108330