Search NASA⌕ Search

DOE OSTI · 1713722

Materials Data on Sr7Cu2HgBiSbO15 by Materials Project

Abstract

HgBiSr7Cu2SbO15 is (La,Ba)CuO4-derived structured and crystallizes in the orthorhombic Pmma space group. The structure is three-dimensional. there are three inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.62–2.79 Å. In the second Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.63–2.91 Å. In the third Sr2+ site, Sr2+ is bonded to six O2- atoms to form SrO6 octahedra that share corners with two equivalent SrO6 octahedra and corners with two equivalent SbO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Sr–O bond distances ranging from 2.47–2.70 Å. There are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to six O2- atoms to form CuO6 octahedra that share a cornercorner with one CuO6 octahedra and corners with three equivalent SbO6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. There are a spread of Cu–O bond distances ranging from 1.89–2.37 Å. In the second Cu2+ site, Cu2+ is bonded to six O2- atoms to form CuO6 octahedra that share a cornercorner with one SbO6 octahedra and corners with three CuO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Cu–O bond distances ranging from 1.89–2.46 Å. Hg2+ is bonded in a distorted linear geometry to four O2- atoms. There are two shorter (2.05 Å) and two longer (3.04 Å) Hg–O bond lengths. Bi5+ is bonded in a distorted see-saw-like geometry to four O2- atoms. All Bi–O bond lengths are 2.15 Å. Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with two equivalent SrO6 octahedra and corners with four CuO6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. There are a spread of Sb–O bond distances ranging from 1.97–2.04 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four equivalent Sr2+, one Cu2+, and one Hg2+ atom. In the second O2- site, O2- is bonded to four equivalent Sr2+, one Cu2+, and one Sb5+ atom to form distorted OSr4CuSb octahedra that share corners with two OSr4Cu2 octahedra, edges with two equivalent OSr4Cu2 octahedra, and faces with four OSr5Sb octahedra. The corner-sharing octahedral tilt angles are 0°. In the third O2- site, O2- is bonded in a distorted linear geometry to four Sr2+, one Cu2+, and one Sb5+ atom. In the fourth O2- site, O2- is bonded to four equivalent Sr2+ and two Cu2+ atoms to form distorted OSr4Cu2 octahedra that share corners with six OSr4CuSb octahedra, edges with two equivalent OSr4CuSb octahedra, and faces with two equivalent OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–59°. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to three Sr2+, one Hg2+, and one Bi5+ atom. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Cu2+, and one Bi5+ atom. In the seventh O2- site, O2- is bonded to four equivalent Sr2+ and two equivalent Cu2+ atoms to form distorted OSr4Cu2 octahedra that share corners with six OSr5Sb octahedra and faces with four OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–57°. In the eighth O2- site, O2- is bonded to five Sr2+ and one Sb5+ atom to form distorted OSr5Sb octahedra that share corners with ten OSr4Cu2 octahedra and faces with two OSr4CuSb octahedra. The corner-sharing octahedra tilt angles range from 2–59°. In the ninth O2- site, O2- is bonded to four equivalent Sr2+, one Cu2+, and one Sb5+ atom to form distorted OSr4CuSb octahedra that share corners with six OSr4CuSb octahedra, edges with two equivalent OSr4CuSb octahedra, and faces with two equivalent OSr5Sb octahedra. The corner-sharing octahedra tilt angles range from 0–57°. In the tenth O2- site, O2- is bonded in a distorted square co-planar geometry to four Sr2+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Sr7Cu2HgBiSbO15 by Materials Project. https://doi.org/10.17188/1713722

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↗