Search NASA⌕ Search

DOE OSTI · 1677378

Materials Data on Y11Ta5O28 by Materials Project

Abstract

Y11Ta5O28 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are six inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded to seven O2- atoms to form distorted YO7 pentagonal bipyramids that share corners with two equivalent TaO6 octahedra, a cornercorner with one YO7 pentagonal bipyramid, an edgeedge with one YO8 hexagonal bipyramid, edges with two equivalent TaO6 octahedra, and edges with two equivalent YO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 57°. There are a spread of Y–O bond distances ranging from 2.29–2.41 Å. In the second Y3+ site, Y3+ is bonded to eight O2- atoms to form distorted YO8 hexagonal bipyramids that share edges with six TaO6 octahedra and edges with two equivalent YO7 pentagonal bipyramids. There are a spread of Y–O bond distances ranging from 2.15–2.59 Å. In the third Y3+ site, Y3+ is bonded to seven O2- atoms to form distorted YO7 pentagonal bipyramids that share corners with three TaO6 octahedra, edges with two equivalent TaO6 octahedra, and edges with three YO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 46–54°. There are a spread of Y–O bond distances ranging from 2.20–2.45 Å. In the fourth Y3+ site, Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.32–2.61 Å. In the fifth Y3+ site, Y3+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.26–2.77 Å. In the sixth Y3+ site, Y3+ is bonded to seven O2- atoms to form distorted YO7 pentagonal bipyramids that share corners with two equivalent TaO6 octahedra, a cornercorner with one YO7 pentagonal bipyramid, edges with two equivalent TaO6 octahedra, and edges with three YO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 51°. There are a spread of Y–O bond distances ranging from 2.23–2.43 Å. There are two inequivalent Ta+4.60+ sites. In the first Ta+4.60+ site, Ta+4.60+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with four equivalent TaO6 octahedra, corners with two equivalent YO7 pentagonal bipyramids, and edges with two equivalent YO8 hexagonal bipyramids. The corner-sharing octahedral tilt angles are 39°. There are four shorter (1.98 Å) and two longer (2.06 Å) Ta–O bond lengths. In the second Ta+4.60+ site, Ta+4.60+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with three TaO6 octahedra, corners with three YO7 pentagonal bipyramids, an edgeedge with one YO8 hexagonal bipyramid, and edges with three YO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 39–63°. There are a spread of Ta–O bond distances ranging from 1.96–2.11 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded to two Y3+ and two equivalent Ta+4.60+ atoms to form distorted OY2Ta2 tetrahedra that share corners with seven OY2Ta2 tetrahedra, corners with two equivalent OY2Ta2 trigonal pyramids, and an edgeedge with one OY4 tetrahedra. In the second O2- site, O2- is bonded to two Y3+ and two equivalent Ta+4.60+ atoms to form distorted OY2Ta2 trigonal pyramids that share corners with four OY2Ta2 tetrahedra and edges with three OY3Ta tetrahedra. In the third O2- site, O2- is bonded in a 2-coordinate geometry to two Y3+ and two Ta+4.60+ atoms. In the fourth O2- site, O2- is bonded to four Y3+ atoms to form OY4 tetrahedra that share corners with eight OY4 tetrahedra, an edgeedge with one OY4 tetrahedra, and an edgeedge with one OY2Ta2 trigonal pyramid. In the fifth O2- site, O2- is bonded to four Y3+ atoms to form OY4 tetrahedra that share corners with nine OY2Ta2 tetrahedra, a cornercorner with one OY2Ta2 trigonal pyramid, and an edgeedge with one OY4 tetrahedra. In the sixth O2- site, O2- is bonded to three Y3+ and one Ta+4.60+ atom to form distorted OY3Ta tetrahedra that share corners with eight OY4 tetrahedra, a cornercorner with one OY2Ta2 trigonal pyramid, and edges with three OY3Ta tetrahedra. In the seventh O2- site, O2- is bonded to four Y3+ atoms to form a mixture of edge and corner-sharing OY4 tetrahedra. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to three Y3+ and one Ta+4.60+ atom. In the ninth O2- site, O2- is bonded to three Y3+ and one Ta+4.60+ atom to form distorted OY3Ta tetrahedra that share corners with nine OY2Ta2 tetrahedra, edges with two OY3Ta tetrahedra, and an edgeedge with one OY2Ta2 trigonal pyramid. In the tenth O2- site, O2- is bonded in a 4-coordinate geometry to three Y3+ and one Ta+4.60+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Y11Ta5O28 by Materials Project. https://doi.org/10.17188/1677378

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↗