Search NASA⌕ Search

DOE OSTI · 1733996

Materials Data on Ba14U2Fe4S25O by Materials Project

Abstract

Ba14U2Fe4S25O crystallizes in the tetragonal P4 space group. The structure is three-dimensional. there are eight inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten S2- atoms. There are a spread of Ba–S bond distances ranging from 3.29–3.58 Å. In the second Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten S2- atoms. There are a spread of Ba–S bond distances ranging from 3.30–3.57 Å. In the third Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Ba–S bond distances ranging from 3.09–3.32 Å. In the fourth Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Ba–S bond distances ranging from 3.11–3.59 Å. In the fifth Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine S2- atoms. There are a spread of Ba–S bond distances ranging from 3.18–3.59 Å. In the sixth Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine S2- atoms. There are a spread of Ba–S bond distances ranging from 3.18–3.56 Å. In the seventh Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Ba–S bond distances ranging from 3.14–3.48 Å. In the eighth Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Ba–S bond distances ranging from 3.14–3.49 Å. There are four inequivalent U6+ sites. In the first U6+ site, U6+ is bonded to five S2- and one O2- atom to form corner-sharing US5O octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.60 Å) and one longer (2.68 Å) U–S bond lengths. The U–O bond length is 2.16 Å. In the second U6+ site, U6+ is bonded to five S2- and one O2- atom to form corner-sharing US5O octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.60 Å) and one longer (2.68 Å) U–S bond lengths. The U–O bond length is 2.19 Å. In the third U6+ site, U6+ is bonded to five S2- and one O2- atom to form distorted corner-sharing US5O octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.61 Å) and one longer (2.68 Å) U–S bond lengths. The U–O bond length is 2.13 Å. In the fourth U6+ site, U6+ is bonded to five S2- and one O2- atom to form corner-sharing US5O octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.61 Å) and one longer (2.68 Å) U–S bond lengths. The U–O bond length is 2.16 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded in a tetrahedral geometry to four S2- atoms. There are two shorter (2.27 Å) and two longer (2.40 Å) Fe–S bond lengths. In the second Fe3+ site, Fe3+ is bonded in a tetrahedral geometry to four S2- atoms. There are two shorter (2.27 Å) and two longer (2.28 Å) Fe–S bond lengths. There are fourteen inequivalent S2- sites. In the first S2- site, S2- is bonded in a 1-coordinate geometry to five Ba2+ and one Fe3+ atom. In the second S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one Fe3+ atom. In the third S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one Fe3+ atom. In the fourth S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one Fe3+ atom. In the fifth S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one U6+ atom. In the sixth S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one U6+ atom. In the seventh S2- site, S2- is bonded in a 1-coordinate geometry to five Ba2+ and one Fe3+ atom. In the eighth S2- site, S2- is bonded in a 1-coordinate geometry to five Ba2+ and one Fe3+ atom. In the ninth S2- site, S2- is bonded to four Ba2+ and one Fe3+ atom to form distorted SBa4Fe trigonal bipyramids that share corners with two SBa4U2 octahedra, a cornercorner with one SBa4Fe trigonal bipyramid, and an edgeedge with one SBa4Fe trigonal bipyramid. The corner-sharing octahedral tilt angles are 57°. In the tenth S2- site, S2- is bonded to four Ba2+ and one Fe3+ atom to form a mixture of distorted edge and corner-sharing SBa4Fe trigonal bipyramids. In the eleventh S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one U6+ atom. In the twelfth S2- site, S2- is bonded in a 6-coordinate geometry to five Ba2+ and one U6+ atom. In the thirteenth S2- site, S2- is bonded to four equivalent Ba2+ and two U6+ atoms to form distorted corner-sharing SBa4U2 octahedra. In the fourteenth S2- site, S2- is bonded to four equivalent Ba2+ and two U6+ atoms to form distorted corner-sharing SBa4U2 octahedra. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two U6+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two U6+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Ba14U2Fe4S25O by Materials Project. https://doi.org/10.17188/1733996

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↗