Engineering Papers⌕ Search

DOE OSTI · 1654543

Materials Data on Dy2Ga3Fe14 by Materials Project

Abstract

Dy2Fe14Ga3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are two inequivalent Dy sites. In the first Dy site, Dy is bonded in a 6-coordinate geometry to eighteen Fe atoms. There are a spread of Dy–Fe bond distances ranging from 2.90–3.26 Å. In the second Dy site, Dy is bonded in a 8-coordinate geometry to fourteen Fe and six Ga atoms. There are a spread of Dy–Fe bond distances ranging from 2.99–3.19 Å. There are four shorter (3.22 Å) and two longer (3.23 Å) Dy–Ga bond lengths. There are six inequivalent Fe sites. In the first Fe site, Fe is bonded to three Dy, seven Fe, and two Ga atoms to form FeDy3Ga2Fe7 cuboctahedra that share corners with five GaDy2Fe10 cuboctahedra, corners with ten FeDy3Ga2Fe7 cuboctahedra, edges with three GaDy2Fe10 cuboctahedra, edges with five FeDy3Ga2Fe7 cuboctahedra, faces with two GaDy2Fe10 cuboctahedra, and faces with eight FeDy3Ga2Fe7 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.46–2.68 Å. Both Fe–Ga bond lengths are 2.48 Å. In the second Fe site, Fe is bonded to three Dy, seven Fe, and two equivalent Ga atoms to form distorted FeDy3Ga2Fe7 cuboctahedra that share corners with five GaDy2Fe10 cuboctahedra, corners with ten FeDy3Ga2Fe7 cuboctahedra, edges with three GaDy2Fe10 cuboctahedra, edges with five FeDy3Ga2Fe7 cuboctahedra, faces with two equivalent GaDy2Fe10 cuboctahedra, and faces with eight FeDy3Ga2Fe7 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.49–2.68 Å. Both Fe–Ga bond lengths are 2.48 Å. In the third Fe site, Fe is bonded in a 2-coordinate geometry to one Dy, ten Fe, and three Ga atoms. There are a spread of Fe–Fe bond distances ranging from 2.29–2.89 Å. All Fe–Ga bond lengths are 2.64 Å. In the fourth Fe site, Fe is bonded in a 12-coordinate geometry to two Dy, eight Fe, and two equivalent Ga atoms. There are one shorter (2.51 Å) and one longer (2.78 Å) Fe–Fe bond lengths. Both Fe–Ga bond lengths are 2.50 Å. In the fifth Fe site, Fe is bonded in a 12-coordinate geometry to two Dy, eight Fe, and two equivalent Ga atoms. There are one shorter (2.52 Å) and one longer (2.77 Å) Fe–Fe bond lengths. Both Fe–Ga bond lengths are 2.50 Å. In the sixth Fe site, Fe is bonded in a 12-coordinate geometry to two Dy, eight Fe, and two equivalent Ga atoms. Both Fe–Ga bond lengths are 2.50 Å. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded to two equivalent Dy and ten Fe atoms to form GaDy2Fe10 cuboctahedra that share corners with four GaDy2Fe10 cuboctahedra, corners with ten FeDy3Ga2Fe7 cuboctahedra, edges with six FeDy3Ga2Fe7 cuboctahedra, faces with four FeDy3Ga2Fe7 cuboctahedra, and faces with six GaDy2Fe10 cuboctahedra. In the second Ga site, Ga is bonded to two equivalent Dy and ten Fe atoms to form GaDy2Fe10 cuboctahedra that share corners with four equivalent GaDy2Fe10 cuboctahedra, corners with ten FeDy3Ga2Fe7 cuboctahedra, edges with six FeDy3Ga2Fe7 cuboctahedra, faces with four equivalent FeDy3Ga2Fe7 cuboctahedra, and faces with six GaDy2Fe10 cuboctahedra.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-22. Materials Data on Dy2Ga3Fe14 by Materials Project. https://doi.org/10.17188/1654543

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related reports

Cyclic moisture reactivation of calcium sorbents for long duration thermochemical energy storage

The transition to a flexible and reliable energy infrastructure, using electro-thermal energy generation technologies such as geothermal, concentrated solar power, and nuclear, usually demands simultaneous advancement of thermal energy storage (TES) to support on-demand electricity generation and industrial applications while mitigating the inherent intermittency of renewable energy sources and power outages from direct energy generation. Among TES technologies, thermochemical energy storage (TCES) based on calcium looping emerges as a compelling high-power energy storage candidate due to its high reaction enthalpy, compatibility with elevated operating temperatures, and abundance of low-cost materials. However, the long-term durability of calcium-based sorbents for TCES is hindered by surface sintering and particle aggregation, leading to performance degradation over repeated thermal cycles. This study explores a moisture hydration-based strategy to regenerate a degraded calcium sorbent and mitigate performance degradation for long duration TCES. The addition of moisture transforms calcium oxide into calcium hydroxide and produces intercalation water layers, associated with a regenerated surface area and reduced calcium oxide crystallite size. Both these effects are beneficial in restoring the sorbents' reactivity for carbonization. Additionally, an optimized hydration-assisted reactivation protocol balances the recovered energy storage capacity with heating penalty required for moisture removal from hydrated samples, resulting in an enhanced energy storage capacity up to 176% compared to benchmark sorbents that undergo cycling without reactivation after 60 cycles. In conclusion, these results highlight the potential of hydration-assisted reactivation to enhance the long-term performance of TCES, providing an effective pathway to advancing electro-thermal storage technologies.

36 MATERIALS SCIENCE↗