Search NASA⌕ Search

DOE OSTI · 1307183

Materials Data on Y6N2O5 by Materials Project

Abstract

Y6N2O5 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are six inequivalent Y sites. In the first Y site, Y is bonded to one N and five O atoms to form YNO5 octahedra that share corners with six YNO5 octahedra and edges with nine YN2O4 octahedra. The corner-sharing octahedra tilt angles range from 0–10°. The Y–N bond length is 2.39 Å. There are a spread of Y–O bond distances ranging from 2.36–2.44 Å. In the second Y site, Y is bonded to two N and four O atoms to form YN2O4 octahedra that share corners with five YN2O4 octahedra and edges with ten YNO5 octahedra. The corner-sharing octahedra tilt angles range from 0–9°. There are one shorter (2.36 Å) and one longer (2.48 Å) Y–N bond lengths. There are a spread of Y–O bond distances ranging from 2.33–2.40 Å. In the third Y site, Y is bonded to three N and three O atoms to form a mixture of corner and edge-sharing YN3O3 octahedra. The corner-sharing octahedra tilt angles range from 1–7°. There are two shorter (2.39 Å) and one longer (2.42 Å) Y–N bond lengths. There are a spread of Y–O bond distances ranging from 2.34–2.49 Å. In the fourth Y site, Y is bonded to three N and three O atoms to form a mixture of corner and edge-sharing YN3O3 octahedra. The corner-sharing octahedra tilt angles range from 1–7°. There are two shorter (2.39 Å) and one longer (2.42 Å) Y–N bond lengths. There are a spread of Y–O bond distances ranging from 2.34–2.49 Å. In the fifth Y site, Y is bonded to one N and five O atoms to form a mixture of corner and edge-sharing YNO5 octahedra. The corner-sharing octahedra tilt angles range from 0–10°. The Y–N bond length is 2.39 Å. There are a spread of Y–O bond distances ranging from 2.36–2.44 Å. In the sixth Y site, Y is bonded to two N and four O atoms to form a mixture of corner and edge-sharing YN2O4 octahedra. The corner-sharing octahedra tilt angles range from 0–10°. There are one shorter (2.35 Å) and one longer (2.49 Å) Y–N bond lengths. There are a spread of Y–O bond distances ranging from 2.33–2.41 Å. There are two inequivalent N sites. In the first N site, N is bonded to six Y atoms to form NY6 octahedra that share corners with two equivalent NY6 octahedra, corners with three OY5 square pyramids, edges with three equivalent NY6 octahedra, and edges with eight OY5 square pyramids. The corner-sharing octahedral tilt angles are 2°. In the second N site, N is bonded to six Y atoms to form NY6 octahedra that share corners with two equivalent NY6 octahedra, corners with three OY5 square pyramids, edges with three equivalent NY6 octahedra, and edges with eight OY5 square pyramids. The corner-sharing octahedral tilt angles are 2°. There are six inequivalent O sites. In the first O site, O is bonded to five Y atoms to form OY5 square pyramids that share a cornercorner with one NY6 octahedra, corners with five OY5 square pyramids, edges with five NY6 octahedra, and edges with three OY5 square pyramids. The corner-sharing octahedral tilt angles are 6°. In the second O site, O is bonded in a square co-planar geometry to four Y atoms. There are one shorter (2.36 Å) and one longer (2.37 Å) O–Y bond lengths. In the third O site, O is bonded to five Y atoms to form OY5 square pyramids that share corners with two NY6 octahedra, corners with five OY5 square pyramids, edges with three NY6 octahedra, and edges with four OY5 square pyramids. The corner-sharing octahedra tilt angles range from 0–1°. In the fourth O site, O is bonded to five Y atoms to form OY5 square pyramids that share a cornercorner with one NY6 octahedra, corners with five OY5 square pyramids, edges with five NY6 octahedra, and edges with three OY5 square pyramids. The corner-sharing octahedral tilt angles are 6°. In the fifth O site, O is bonded to five Y atoms to form OY5 square pyramids that share corners with two NY6 octahedra, corners with five OY5 square pyramids, edges with three NY6 octahedra, and edges with four OY5 square pyramids. The corner-sharing octahedral tilt angles are 1°. In the sixth O site, O is bonded in a square co-planar geometry to four Y atoms. There are one shorter (2.36 Å) and one longer (2.37 Å) O–Y bond lengths.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-22. Materials Data on Y6N2O5 by Materials Project. https://doi.org/10.17188/1307183

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↗