Search NASA⌕ Search

DOE OSTI · 1742562

Materials Data on Ba4Cu11(Te4S)2 by Materials Project

Abstract

Ba4Cu11(Te4S)2 crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are four inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 2-coordinate geometry to six Te2- and two equivalent S2- atoms. There are a spread of Ba–Te bond distances ranging from 3.49–3.79 Å. Both Ba–S bond lengths are 3.20 Å. In the second Ba2+ site, Ba2+ is bonded in a 2-coordinate geometry to six Te2- and two equivalent S2- atoms. There are a spread of Ba–Te bond distances ranging from 3.49–3.82 Å. Both Ba–S bond lengths are 3.17 Å. In the third Ba2+ site, Ba2+ is bonded in a 2-coordinate geometry to six Te2- and two equivalent S2- atoms. There are a spread of Ba–Te bond distances ranging from 3.58–3.85 Å. Both Ba–S bond lengths are 3.16 Å. In the fourth Ba2+ site, Ba2+ is bonded in a 2-coordinate geometry to six Te2- and two equivalent S2- atoms. There are a spread of Ba–Te bond distances ranging from 3.50–3.84 Å. Both Ba–S bond lengths are 3.11 Å. There are eleven inequivalent Cu+1.09+ sites. In the first Cu+1.09+ site, Cu+1.09+ is bonded in a 4-coordinate geometry to four Te2- atoms. There are a spread of Cu–Te bond distances ranging from 2.71–2.86 Å. In the second Cu+1.09+ site, Cu+1.09+ is bonded to four Te2- atoms to form distorted corner-sharing CuTe4 tetrahedra. There are a spread of Cu–Te bond distances ranging from 2.69–2.87 Å. In the third Cu+1.09+ site, Cu+1.09+ is bonded to four Te2- atoms to form corner-sharing CuTe4 tetrahedra. There are three shorter (2.69 Å) and one longer (2.72 Å) Cu–Te bond lengths. In the fourth Cu+1.09+ site, Cu+1.09+ is bonded in a 4-coordinate geometry to four Te2- atoms. There are a spread of Cu–Te bond distances ranging from 2.63–2.85 Å. In the fifth Cu+1.09+ site, Cu+1.09+ is bonded in a distorted single-bond geometry to three Te2- and one S2- atom. There are one shorter (2.70 Å) and two longer (2.75 Å) Cu–Te bond lengths. The Cu–S bond length is 2.44 Å. In the sixth Cu+1.09+ site, Cu+1.09+ is bonded in a distorted single-bond geometry to three Te2- and one S2- atom. There are one shorter (2.70 Å) and two longer (2.74 Å) Cu–Te bond lengths. The Cu–S bond length is 2.44 Å. In the seventh Cu+1.09+ site, Cu+1.09+ is bonded in a 1-coordinate geometry to three Te2- and one S2- atom. There are one shorter (2.63 Å) and two longer (2.74 Å) Cu–Te bond lengths. The Cu–S bond length is 2.40 Å. In the eighth Cu+1.09+ site, Cu+1.09+ is bonded to three Te2- and one S2- atom to form distorted corner-sharing CuTe3S tetrahedra. There are two shorter (2.66 Å) and one longer (2.80 Å) Cu–Te bond lengths. The Cu–S bond length is 2.48 Å. In the ninth Cu+1.09+ site, Cu+1.09+ is bonded in a distorted trigonal non-coplanar geometry to three Te2- atoms. There are one shorter (2.63 Å) and two longer (2.64 Å) Cu–Te bond lengths. In the tenth Cu+1.09+ site, Cu+1.09+ is bonded in a distorted trigonal non-coplanar geometry to three Te2- atoms. All Cu–Te bond lengths are 2.63 Å. In the eleventh Cu+1.09+ site, Cu+1.09+ is bonded in a distorted trigonal non-coplanar geometry to three Te2- atoms. There are one shorter (2.62 Å) and two longer (2.63 Å) Cu–Te bond lengths. There are eight inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 8-coordinate geometry to four Ba2+ and four Cu+1.09+ atoms. In the second Te2- site, Te2- is bonded in a 8-coordinate geometry to four Ba2+ and four Cu+1.09+ atoms. In the third Te2- site, Te2- is bonded in a 7-coordinate geometry to four Ba2+ and three Cu+1.09+ atoms. In the fourth Te2- site, Te2- is bonded in a 8-coordinate geometry to four Ba2+ and four Cu+1.09+ atoms. In the fifth Te2- site, Te2- is bonded in a 6-coordinate geometry to two Ba2+ and four Cu+1.09+ atoms. In the sixth Te2- site, Te2- is bonded in a 8-coordinate geometry to two Ba2+ and six Cu+1.09+ atoms. In the seventh Te2- site, Te2- is bonded in a 8-coordinate geometry to two Ba2+ and six Cu+1.09+ atoms. In the eighth Te2- site, Te2- is bonded in a 8-coordinate geometry to two Ba2+ and six Cu+1.09+ atoms. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to four Ba2+ and two Cu+1.09+ atoms to form edge-sharing SBa4Cu2 octahedra. In the second S2- site, S2- is bonded to four Ba2+ and two Cu+1.09+ atoms to form edge-sharing SBa4Cu2 octahedra.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on Ba4Cu11(Te4S)2 by Materials Project. https://doi.org/10.17188/1742562

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↗