Search NASA⌕ Search

DOE OSTI · 1287954

Materials Data on Ba4Y2Cu4W2O17 by Materials Project

Abstract

Ba4Y2W2Cu4O17 is Orthorhombic Perovskite-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 11-coordinate geometry to eleven O2- atoms. There are a spread of Ba–O bond distances ranging from 2.69–3.21 Å. In the second Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.68–3.00 Å. In the third Ba2+ site, Ba2+ is bonded in a 12-coordinate geometry to twelve O2- atoms. There are a spread of Ba–O bond distances ranging from 2.70–3.35 Å. In the fourth Ba2+ site, Ba2+ is bonded in a 12-coordinate geometry to twelve O2- atoms. There are a spread of Ba–O bond distances ranging from 2.71–3.41 Å. There are two inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Y–O bond distances ranging from 2.24–2.71 Å. In the second Y3+ site, Y3+ is bonded to six O2- atoms to form distorted YO6 pentagonal pyramids that share a cornercorner with one CuO6 octahedra, a cornercorner with one CuO5 square pyramid, an edgeedge with one CuO6 octahedra, an edgeedge with one CuO5 square pyramid, and a faceface with one WO6 octahedra. The corner-sharing octahedral tilt angles are 73°. There are a spread of Y–O bond distances ranging from 2.17–2.50 Å. There are two inequivalent W6+ sites. In the first W6+ site, W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with five CuO6 octahedra. The corner-sharing octahedra tilt angles range from 11–27°. There are a spread of W–O bond distances ranging from 1.91–2.02 Å. In the second W6+ site, W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with five CuO6 octahedra and a faceface with one YO6 pentagonal pyramid. The corner-sharing octahedra tilt angles range from 6–19°. There are a spread of W–O bond distances ranging from 1.88–2.05 Å. There are four inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to six O2- atoms to form distorted CuO6 octahedra that share corners with five WO6 octahedra, a cornercorner with one YO6 pentagonal pyramid, a cornercorner with one CuO5 square pyramid, and an edgeedge with one YO6 pentagonal pyramid. The corner-sharing octahedra tilt angles range from 6–19°. There are a spread of Cu–O bond distances ranging from 1.97–2.60 Å. In the second Cu2+ site, Cu2+ is bonded to six O2- atoms to form distorted CuO6 octahedra that share corners with five WO6 octahedra and a cornercorner with one CuO5 square pyramid. The corner-sharing octahedra tilt angles range from 11–27°. There are a spread of Cu–O bond distances ranging from 1.94–2.75 Å. In the third Cu2+ site, Cu2+ is bonded in a 3-coordinate geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.88–2.68 Å. In the fourth Cu2+ site, Cu2+ is bonded to five O2- atoms to form distorted CuO5 square pyramids that share corners with two CuO6 octahedra, a cornercorner with one YO6 pentagonal pyramid, and an edgeedge with one YO6 pentagonal pyramid. The corner-sharing octahedra tilt angles range from 29–33°. There are a spread of Cu–O bond distances ranging from 1.91–2.33 Å. There are seventeen inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two Ba2+, one Y3+, and one Cu2+ atom. In the third O2- site, O2- is bonded in a 6-coordinate geometry to three Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+, one Y3+, and two Cu2+ atoms. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to four Ba2+, one W6+, and one Cu2+ atom. In the sixth O2- site, O2- is bonded in a distorted linear geometry to three Ba2+, one W6+, and one Cu2+ atom. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to three Ba2+, one W6+, and one Cu2+ atom. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to three Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the ninth O2- site, O2- is bonded in a 1-coordinate geometry to three Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the tenth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, one Y3+, and two Cu2+ atoms. In the eleventh O2- site, O2- is bonded in a 4-coordinate geometry to four Ba2+, one W6+, and one Cu2+ atom. In the twelfth O2- site, O2- is bonded in a 2-coordinate geometry to three Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the thirteenth O2- site, O2- is bonded in a 5-coordinate geometry to two Ba2+, one Y3+, and two Cu2+ atoms. In the fourteenth O2- site, O2- is bonded in a 2-coordinate geometry to three Ba2+, one W6+, and one Cu2+ atom. In the fifteenth O2- site, O2- is bonded in a 6-coordinate geometry to two Ba2+, two Y3+, and two Cu2+ atoms. In the sixteenth O2- site, O2- is bonded in a 6-coordinate geometry to three Ba2+, one Y3+, one W6+, and one Cu2+ atom. In the seventeenth O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ba2+, one Y3+, one W6+, and one Cu2+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-06-04. Materials Data on Ba4Y2Cu4W2O17 by Materials Project. https://doi.org/10.17188/1287954

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↗