Theoretical Study on the Structure and Properties of Helium-Containing Zirconium Hydrides

Lü, Qi; Shi, Li; Wan, Jian Guo

doi:10.13182/fst13-648

Cited by 1 publication

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“…In the tritium storage period, helium is produced in UT 3 by the beta decay of tritium with a half-life of 12.3 years. The produced helium within UT 3 is not released immediately after the decay because of its small recoil energy. , Moreover, some of the generated helium does not leave the host material by heating even above the decomposition temperature of UT 3 , and a major release of helium requires heating at 800–1000 K. , Because the tritium delivery is planned to be conducted at 723 K in ITER-SDS to avoid high-temperature damage of devices, , helium will pile up in both UT 3 and alpha-U, which would affect the storage and delivery performance of U or UT 3 . Li et al reported that the effect of aging on the storage and delivery performance was negligible after one-time long-term aging (460–1720 days) .…”

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confidence: 99%

First-Principles Calculations of the Diffusivity of Interstitial Helium in Alpha-U Considering Anisotropy, Isotope Effects, and Quantum Effects

et al. 2021

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The interstitial migration of helium in alpha-U, which is planned to be used as a tritium storage material for nuclear fusion reactors and as a metallic fuel for advanced nuclear reactors, is studied by first-principles calculations. First, all migration paths are identified using the nudged elastic band method, and the migration barrier is determined for each path considering the thermal expansion of the lattice. In addition, the jump attempt frequencies are determined by applying harmonic transition state theory coupled with vibration analysis. Subsequently, the diffusion coefficient is evaluated numerically by kinetic Monte Carlo calculations using the determined migration barriers and jump attempt frequencies for all migration paths. Diffusion in the [010]-direction is found to be the most unlikely until sufficiently high temperature, while [001]-diffusion is the most dominant diffusion direction through the whole temperature range. The isotope effect, which is important because the beta decay of tritium produces helium-3, is not large and approaches the classical limit as the temperature increases. The quantum tunneling crossover temperature is computed to be approximately 100 K for helium-3 and 86 K for helium-4, which ensures the validity of the present calculation results over a wide temperature range. The diffusion coefficients are obtained as for helium-3 and for helium-4 over a temperature range from 200 to 900 K.

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