Engineering Papers⌕ Search

DOE OSTI · 1284080

Materials Data on V23Se40 by Materials Project

Abstract

V23Se40 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are twelve inequivalent V+3.48+ sites. In the first V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of distorted corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of V–Se bond distances ranging from 2.40–2.72 Å. In the second V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are a spread of V–Se bond distances ranging from 2.51–2.60 Å. In the third V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner, edge, and face-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 55°. There are a spread of V–Se bond distances ranging from 2.46–2.66 Å. In the fourth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner, edge, and face-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 54°. There are a spread of V–Se bond distances ranging from 2.47–2.62 Å. In the fifth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner, edge, and face-sharing VSe6 octahedra. The corner-sharing octahedra tilt angles range from 48–55°. There are one shorter (2.56 Å) and five longer (2.58 Å) V–Se bond lengths. In the sixth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 49°. There are five shorter (2.53 Å) and one longer (2.59 Å) V–Se bond lengths. In the seventh V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of V–Se bond distances ranging from 2.41–2.71 Å. In the eighth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form edge-sharing VSe6 octahedra. All V–Se bond lengths are 2.54 Å. In the ninth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner, edge, and face-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 55°. There are a spread of V–Se bond distances ranging from 2.46–2.62 Å. In the tenth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are a spread of V–Se bond distances ranging from 2.50–2.57 Å. In the eleventh V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of distorted corner and edge-sharing VSe6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of V–Se bond distances ranging from 2.39–2.71 Å. In the twelfth V+3.48+ site, V+3.48+ is bonded to six Se2- atoms to form a mixture of corner, edge, and face-sharing VSe6 octahedra. The corner-sharing octahedra tilt angles range from 48–55°. There are two shorter (2.54 Å) and four longer (2.58 Å) V–Se bond lengths. There are twenty inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a distorted T-shaped geometry to three V+3.48+ atoms. In the second Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the third Se2- site, Se2- is bonded in a 4-coordinate geometry to four V+3.48+ atoms. In the fourth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the fifth Se2- site, Se2- is bonded in a 5-coordinate geometry to five V+3.48+ atoms. In the sixth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the seventh Se2- site, Se2- is bonded in a distorted trigonal non-coplanar geometry to three V+3.48+ atoms. In the eighth Se2- site, Se2- is bonded in a 5-coordinate geometry to five V+3.48+ atoms. In the ninth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the tenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the eleventh Se2- site, Se2- is bonded in a distorted rectangular see-saw-like geometry to four V+3.48+ atoms. In the twelfth Se2- site, Se2- is bonded in a distorted trigonal non-coplanar geometry to three V+3.48+ atoms. In the thirteenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the fourteenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the fifteenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the sixteenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the seventeenth Se2- site, Se2- is bonded in a 3-coordinate geometry to three V+3.48+ atoms. In the eighteenth Se2- site, Se2- is bonded to four V+3.48+ atoms to form distorted corner-sharing SeV4 trigonal pyramids. In the nineteenth Se2- site, Se2- is bonded in a distorted trigonal non-coplanar geometry to three V+3.48+ atoms. In the twentieth Se2- site, Se2- is bonded in a 5-coordinate geometry to five V+3.48+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on V23Se40 by Materials Project. https://doi.org/10.17188/1284080

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↗