Engineering Papers⌕ Search

DOE OSTI · 1296870

Materials Data on Li3BiS3 by Materials Project

Abstract

Li3BiS3 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are twelve inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four S2- atoms to form a mixture of edge and corner-sharing LiS4 tetrahedra. There are a spread of Li–S bond distances ranging from 2.42–2.56 Å. In the second Li1+ site, Li1+ is bonded to four S2- atoms to form LiS4 trigonal pyramids that share a cornercorner with one LiS5 square pyramid, corners with two LiS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, a cornercorner with one LiS4 trigonal pyramid, an edgeedge with one LiS4 tetrahedra, and an edgeedge with one LiS4 trigonal pyramid. There are a spread of Li–S bond distances ranging from 2.40–2.66 Å. In the third Li1+ site, Li1+ is bonded to four S2- atoms to form distorted LiS4 tetrahedra that share a cornercorner with one LiS5 square pyramid, corners with two LiS4 trigonal pyramids, an edgeedge with one LiS4 tetrahedra, and edges with three LiS4 trigonal pyramids. There are a spread of Li–S bond distances ranging from 2.39–2.49 Å. In the fourth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to five S2- atoms. There are a spread of Li–S bond distances ranging from 2.45–3.21 Å. In the fifth Li1+ site, Li1+ is bonded in a distorted rectangular see-saw-like geometry to four S2- atoms. There are a spread of Li–S bond distances ranging from 2.43–2.77 Å. In the sixth Li1+ site, Li1+ is bonded to four S2- atoms to form distorted LiS4 trigonal pyramids that share a cornercorner with one LiS5 square pyramid, corners with three LiS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, a cornercorner with one LiS4 trigonal pyramid, an edgeedge with one LiS5 square pyramid, an edgeedge with one LiS4 tetrahedra, and an edgeedge with one LiS4 trigonal pyramid. There are a spread of Li–S bond distances ranging from 2.44–2.53 Å. In the seventh Li1+ site, Li1+ is bonded to four S2- atoms to form distorted LiS4 trigonal pyramids that share corners with two LiS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, corners with two LiS4 trigonal pyramids, an edgeedge with one LiS5 square pyramid, and edges with two LiS4 tetrahedra. There are a spread of Li–S bond distances ranging from 2.41–2.52 Å. In the eighth Li1+ site, Li1+ is bonded to four S2- atoms to form LiS4 tetrahedra that share a cornercorner with one LiS5 square pyramid, corners with four LiS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, corners with two LiS4 trigonal pyramids, and an edgeedge with one LiS4 tetrahedra. There are a spread of Li–S bond distances ranging from 2.42–2.54 Å. In the ninth Li1+ site, Li1+ is bonded to five S2- atoms to form LiS5 trigonal bipyramids that share corners with three LiS4 tetrahedra, corners with three LiS4 trigonal pyramids, edges with two equivalent LiS5 square pyramids, an edgeedge with one LiS4 tetrahedra, and an edgeedge with one LiS5 trigonal bipyramid. There are a spread of Li–S bond distances ranging from 2.60–2.88 Å. In the tenth Li1+ site, Li1+ is bonded to four S2- atoms to form LiS4 tetrahedra that share a cornercorner with one LiS5 square pyramid, a cornercorner with one LiS4 tetrahedra, a cornercorner with one LiS4 trigonal pyramid, edges with two LiS4 tetrahedra, an edgeedge with one LiS5 trigonal bipyramid, and an edgeedge with one LiS4 trigonal pyramid. There are a spread of Li–S bond distances ranging from 2.44–2.56 Å. In the eleventh Li1+ site, Li1+ is bonded to four S2- atoms to form LiS4 tetrahedra that share corners with three LiS4 tetrahedra, corners with two equivalent LiS5 trigonal bipyramids, a cornercorner with one LiS4 trigonal pyramid, an edgeedge with one LiS5 square pyramid, and an edgeedge with one LiS4 tetrahedra. There are a spread of Li–S bond distances ranging from 2.40–2.57 Å. In the twelfth Li1+ site, Li1+ is bonded to five S2- atoms to form LiS5 square pyramids that share corners with three LiS4 tetrahedra, corners with two LiS4 trigonal pyramids, an edgeedge with one LiS4 tetrahedra, edges with two equivalent LiS5 trigonal bipyramids, and edges with two LiS4 trigonal pyramids. There are a spread of Li–S bond distances ranging from 2.54–2.68 Å. There are four inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded in a distorted rectangular see-saw-like geometry to three S2- atoms. There are two shorter (2.53 Å) and one longer (2.62 Å) Bi–S bond lengths. In the second Bi3+ site, Bi3+ is bonded in a 3-coordinate geometry to three S2- atoms. There are a spread of Bi–S bond distances ranging from 2.54–2.58 Å. In the third Bi3+ site, Bi3+ is bonded in a distorted T-shaped geometry to three S2- atoms. There are two shorter (2.53 Å) and one longer (2.55 Å) Bi–S bond lengths. In the fourth Bi3+ site, Bi3+ is bonded in a 3-coordinate geometry to three S2- atoms. There are two shorter (2.53 Å) and one longer (2.62 Å) Bi–S bond lengths. There are twelve inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the second S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the third S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the fourth S2- site, S2- is bonded to four Li1+ and one Bi3+ atom to form distorted SLi4Bi trigonal bipyramids that share a cornercorner with one SLi5Bi octahedra and corners with two equivalent SLi4Bi trigonal bipyramids. The corner-sharing octahedral tilt angles are 46°. In the fifth S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the sixth S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the seventh S2- site, S2- is bonded to four Li1+ and one Bi3+ atom to form distorted SLi4Bi trigonal bipyramids that share corners with two equivalent SLi5Bi octahedra, corners with two equivalent SLi4Bi trigonal bipyramids, and an edgeedge with one SLi4Bi square pyramid. The corner-sharing octahedra tilt angles range from 25–68°. In the eighth S2- site, S2- is bonded in a 6-coordinate geometry to five Li1+ and one Bi3+ atom. In the ninth S2- site, S2- is bonded in a 6-coordinate geometry to five Li1+ and one Bi3+ atom. In the tenth S2- site, S2- is bonded to five Li1+ and one Bi3+ atom to form SLi5Bi octahedra that share corners with three SLi4Bi trigonal bipyramids, an edgeedge with one SLi5Bi octahedra, and edges with two equivalent SLi4Bi square pyramids. In the eleventh S2- site, S2- is bonded in a 5-coordinate geometry to four Li1+ and one Bi3+ atom. In the twelfth S2- site, S2- is bonded to four Li1+ and one Bi3+ atom to form distorted SLi4Bi square pyramids that share edges with two equivalent SLi5Bi octahedra and an edgeedge with one SLi4Bi trigonal bipyramid.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-28. Materials Data on Li3BiS3 by Materials Project. https://doi.org/10.17188/1296870

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↗