Search NASA⌕ Search

DOE OSTI · 1304483

Materials Data on BaY3F11 by Materials Project

Abstract

BaY3F11 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Ba2+ is bonded to four F1- atoms to form distorted BaF4 trigonal pyramids that share corners with four YF6 octahedra. The corner-sharing octahedra tilt angles range from 19–40°. There are a spread of Ba–F bond distances ranging from 2.45–2.52 Å. There are three inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded to six F1- atoms to form YF6 octahedra that share corners with five YF6 octahedra and a cornercorner with one BaF4 trigonal pyramid. The corner-sharing octahedra tilt angles range from 1–17°. There are a spread of Y–F bond distances ranging from 2.15–2.23 Å. In the second Y3+ site, Y3+ is bonded to six F1- atoms to form corner-sharing YF6 octahedra. The corner-sharing octahedra tilt angles range from 1–7°. There are a spread of Y–F bond distances ranging from 2.19–2.22 Å. In the third Y3+ site, Y3+ is bonded to six F1- atoms to form YF6 octahedra that share corners with three YF6 octahedra and corners with three equivalent BaF4 trigonal pyramids. The corner-sharing octahedra tilt angles range from 7–17°. There are a spread of Y–F bond distances ranging from 2.18–2.23 Å. There are eleven inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two Y3+ atoms. In the second F1- site, F1- is bonded in a linear geometry to two Y3+ atoms. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to one Ba2+ and one Y3+ atom. In the fourth F1- site, F1- is bonded in a linear geometry to two equivalent Y3+ atoms. In the fifth F1- site, F1- is bonded in a linear geometry to two Y3+ atoms. In the sixth F1- site, F1- is bonded in a linear geometry to two Y3+ atoms. In the seventh F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ba2+ and one Y3+ atom. In the eighth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ba2+ and one Y3+ atom. In the ninth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ba2+ and one Y3+ atom. In the tenth F1- site, F1- is bonded in a linear geometry to two Y3+ atoms. In the eleventh F1- site, F1- is bonded in a linear geometry to two Y3+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-29. Materials Data on BaY3F11 by Materials Project. https://doi.org/10.17188/1304483

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↗