Search NASA⌕ Search

DOE OSTI · 1281746

Materials Data on Sc3Re2Si3 by Materials Project

Abstract

Sc3Re2Si3 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are six inequivalent Sc2+ sites. In the first Sc2+ site, Sc2+ is bonded in a 5-coordinate geometry to five Si4- atoms. There are a spread of Sc–Si bond distances ranging from 2.53–2.77 Å. In the second Sc2+ site, Sc2+ is bonded to six Si4- atoms to form ScSi6 pentagonal pyramids that share corners with five ScSi6 pentagonal pyramids, a cornercorner with one ScSi5 trigonal bipyramid, an edgeedge with one ScSi6 pentagonal pyramid, an edgeedge with one ScSi5 trigonal bipyramid, and faces with two equivalent ScSi6 pentagonal pyramids. There are a spread of Sc–Si bond distances ranging from 2.80–2.88 Å. In the third Sc2+ site, Sc2+ is bonded to six Si4- atoms to form distorted ScSi6 pentagonal pyramids that share corners with five ScSi6 pentagonal pyramids, corners with two equivalent ScSi5 trigonal bipyramids, an edgeedge with one ScSi6 pentagonal pyramid, and faces with two equivalent ScSi6 pentagonal pyramids. There are a spread of Sc–Si bond distances ranging from 2.77–2.95 Å. In the fourth Sc2+ site, Sc2+ is bonded in a 4-coordinate geometry to four Si4- atoms. There are a spread of Sc–Si bond distances ranging from 2.77–2.95 Å. In the fifth Sc2+ site, Sc2+ is bonded in a 4-coordinate geometry to four Si4- atoms. There are a spread of Sc–Si bond distances ranging from 2.68–3.08 Å. In the sixth Sc2+ site, Sc2+ is bonded to five Si4- atoms to form distorted ScSi5 trigonal bipyramids that share corners with three ScSi6 pentagonal pyramids, an edgeedge with one ScSi6 pentagonal pyramid, and an edgeedge with one ScSi5 trigonal bipyramid. There are a spread of Sc–Si bond distances ranging from 2.77–3.07 Å. There are four inequivalent Re3+ sites. In the first Re3+ site, Re3+ is bonded in a distorted square co-planar geometry to four Si4- atoms. There are a spread of Re–Si bond distances ranging from 2.45–2.50 Å. In the second Re3+ site, Re3+ is bonded in a 5-coordinate geometry to five Si4- atoms. There are a spread of Re–Si bond distances ranging from 2.40–2.52 Å. In the third Re3+ site, Re3+ is bonded in a bent 150 degrees geometry to two equivalent Si4- atoms. There are one shorter (2.45 Å) and one longer (2.47 Å) Re–Si bond lengths. In the fourth Re3+ site, Re3+ is bonded in a 6-coordinate geometry to six Si4- atoms. There are a spread of Re–Si bond distances ranging from 2.41–2.70 Å. There are eight inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 10-coordinate geometry to six Sc2+, two equivalent Re3+, and two equivalent Si4- atoms. There are one shorter (2.63 Å) and one longer (2.67 Å) Si–Si bond lengths. In the second Si4- site, Si4- is bonded in a 1-coordinate geometry to four Sc2+, three Re3+, and two Si4- atoms. There are one shorter (2.45 Å) and one longer (2.55 Å) Si–Si bond lengths. In the third Si4- site, Si4- is bonded in a 10-coordinate geometry to six Sc2+, two equivalent Re3+, and two equivalent Si4- atoms. In the fourth Si4- site, Si4- is bonded in a 9-coordinate geometry to six Sc2+, two equivalent Re3+, and one Si4- atom. In the fifth Si4- site, Si4- is bonded in a 8-coordinate geometry to four Sc2+ and four Re3+ atoms. In the sixth Si4- site, Si4- is bonded in a 9-coordinate geometry to four Sc2+, four Re3+, and one Si4- atom. In the seventh Si4- site, Si4- is bonded in a 10-coordinate geometry to six Sc2+, two equivalent Re3+, and two equivalent Si4- atoms. There are one shorter (2.63 Å) and one longer (2.66 Å) Si–Si bond lengths. In the eighth Si4- site, Si4- is bonded in a 10-coordinate geometry to six Sc2+, two equivalent Re3+, and two equivalent Si4- atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on Sc3Re2Si3 by Materials Project. https://doi.org/10.17188/1281746

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↗