Engineering Papers⌕ Search

DOE OSTI · 1267661

Materials Data on Rb2LiNbS4 by Materials Project

Abstract

Rb2LiNbS4 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded to eight S2- atoms to form distorted RbS8 hexagonal bipyramids that share corners with two equivalent RbS8 hexagonal bipyramids, corners with two equivalent RbS7 pentagonal bipyramids, corners with two equivalent LiS4 tetrahedra, corners with two NbS4 tetrahedra, edges with two equivalent RbS8 hexagonal bipyramids, an edgeedge with one RbS7 pentagonal bipyramid, an edgeedge with one LiS4 tetrahedra, edges with three NbS4 tetrahedra, edges with three equivalent LiS5 trigonal bipyramids, and a faceface with one RbS8 hexagonal bipyramid. There are a spread of Rb–S bond distances ranging from 3.39–3.85 Å. In the second Rb1+ site, Rb1+ is bonded to seven S2- atoms to form distorted RbS7 pentagonal bipyramids that share corners with two equivalent RbS8 hexagonal bipyramids, corners with two equivalent RbS7 pentagonal bipyramids, a cornercorner with one LiS4 tetrahedra, a cornercorner with one NbS4 tetrahedra, corners with two equivalent LiS5 trigonal bipyramids, edges with four RbS8 hexagonal bipyramids, edges with two equivalent RbS7 pentagonal bipyramids, edges with three equivalent NbS4 tetrahedra, and an edgeedge with one LiS5 trigonal bipyramid. There are a spread of Rb–S bond distances ranging from 3.45–3.72 Å. In the third Rb1+ site, Rb1+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Rb–S bond distances ranging from 3.41–3.69 Å. In the fourth Rb1+ site, Rb1+ is bonded to eight S2- atoms to form distorted RbS8 hexagonal bipyramids that share corners with two equivalent RbS8 hexagonal bipyramids, corners with four NbS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, edges with three RbS8 hexagonal bipyramids, edges with three equivalent RbS7 pentagonal bipyramids, edges with two NbS4 tetrahedra, edges with three equivalent LiS4 tetrahedra, an edgeedge with one LiS5 trigonal bipyramid, and a faceface with one RbS8 hexagonal bipyramid. There are a spread of Rb–S bond distances ranging from 3.37–3.72 Å. There are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four S2- atoms to form LiS4 tetrahedra that share corners with two equivalent RbS8 hexagonal bipyramids, a cornercorner with one RbS7 pentagonal bipyramid, corners with two NbS4 tetrahedra, edges with four RbS8 hexagonal bipyramids, an edgeedge with one LiS4 tetrahedra, and an edgeedge with one NbS4 tetrahedra. There are a spread of Li–S bond distances ranging from 2.44–2.51 Å. In the second Li1+ site, Li1+ is bonded to five S2- atoms to form distorted LiS5 trigonal bipyramids that share a cornercorner with one RbS8 hexagonal bipyramid, corners with two equivalent RbS7 pentagonal bipyramids, corners with three NbS4 tetrahedra, edges with four RbS8 hexagonal bipyramids, an edgeedge with one RbS7 pentagonal bipyramid, an edgeedge with one NbS4 tetrahedra, and edges with two equivalent LiS5 trigonal bipyramids. There are a spread of Li–S bond distances ranging from 2.53–3.14 Å. There are two inequivalent Nb5+ sites. In the first Nb5+ site, Nb5+ is bonded to four S2- atoms to form NbS4 tetrahedra that share corners with three RbS8 hexagonal bipyramids, a cornercorner with one LiS4 tetrahedra, corners with two equivalent LiS5 trigonal bipyramids, edges with two RbS8 hexagonal bipyramids, edges with three equivalent RbS7 pentagonal bipyramids, and an edgeedge with one LiS5 trigonal bipyramid. There are a spread of Nb–S bond distances ranging from 2.28–2.30 Å. In the second Nb5+ site, Nb5+ is bonded to four S2- atoms to form NbS4 tetrahedra that share corners with three RbS8 hexagonal bipyramids, a cornercorner with one RbS7 pentagonal bipyramid, a cornercorner with one LiS4 tetrahedra, a cornercorner with one LiS5 trigonal bipyramid, edges with three RbS8 hexagonal bipyramids, and an edgeedge with one LiS4 tetrahedra. There are a spread of Nb–S bond distances ranging from 2.28–2.31 Å. There are eight inequivalent S2- sites. In the first S2- site, S2- is bonded to four Rb1+, one Li1+, and one Nb5+ atom to form distorted SRb4LiNb octahedra that share corners with four SRb4LiNb octahedra and edges with three equivalent SRb5Nb octahedra. The corner-sharing octahedra tilt angles range from 5–69°. In the second S2- site, S2- is bonded to five Rb1+ and one Nb5+ atom to form distorted SRb5Nb octahedra that share corners with four SRb5Nb octahedra and edges with seven SRb4LiNb octahedra. The corner-sharing octahedra tilt angles range from 3–23°. In the third S2- site, S2- is bonded in a 3-coordinate geometry to three Rb1+, two equivalent Li1+, and one Nb5+ atom. In the fourth S2- site, S2- is bonded in a 2-coordinate geometry to four Rb1+, one Li1+, and one Nb5+ atom. In the fifth S2- site, S2- is bonded in a 3-coordinate geometry to two Rb1+, two equivalent Li1+, and one Nb5+ atom. In the sixth S2- site, S2- is bonded to five Rb1+ and one Nb5+ atom to form distorted SRb5Nb octahedra that share corners with six SRb4LiNb octahedra and edges with four SRb5Nb octahedra. The corner-sharing octahedra tilt angles range from 3–69°. In the seventh S2- site, S2- is bonded in a 2-coordinate geometry to three Rb1+, two equivalent Li1+, and one Nb5+ atom. In the eighth S2- site, S2- is bonded in a 2-coordinate geometry to four Rb1+, one Li1+, and one Nb5+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Rb2LiNbS4 by Materials Project. https://doi.org/10.17188/1267661

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↗