Search NASA⌕ Search

DOE OSTI · 1203126

Materials Data on SrCuO3 by Materials Project

Abstract

SrCuO3 crystallizes in the orthorhombic Pmma space group. The structure is three-dimensional. there are two inequivalent Sr sites. In the first Sr site, Sr is bonded in a 11-coordinate geometry to eleven O atoms. There are a spread of Sr–O bond distances ranging from 2.59–2.92 Å. In the second Sr site, Sr is bonded to twelve O atoms to form SrO12 cuboctahedra that share corners with two equivalent SrO12 cuboctahedra, faces with two equivalent SrO12 cuboctahedra, and faces with eight CuO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.63–2.77 Å. There are three inequivalent Cu sites. In the first Cu site, Cu is bonded to six O atoms to form CuO6 octahedra that share corners with six CuO6 octahedra and faces with four equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–2°. There are a spread of Cu–O bond distances ranging from 1.93–2.00 Å. In the second Cu site, Cu is bonded to six O atoms to form CuO6 octahedra that share corners with four CuO6 octahedra, an edgeedge with one CuO6 octahedra, and faces with two equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–14°. There are a spread of Cu–O bond distances ranging from 1.94–1.96 Å. In the third Cu site, Cu is bonded to six O atoms to form CuO6 octahedra that share corners with four CuO6 octahedra, an edgeedge with one CuO6 octahedra, and faces with two equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 2–13°. There are a spread of Cu–O bond distances ranging from 1.94–1.96 Å. There are six inequivalent O sites. In the first O site, O is bonded to four Sr and two equivalent Cu atoms to form distorted OSr4Cu2 octahedra that share corners with twelve OSr4Cu2 octahedra, edges with four OSr3Cu2 square pyramids, and faces with eight OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–61°. In the second O site, O is bonded to three Sr and two equivalent Cu atoms to form distorted OSr3Cu2 square pyramids that share corners with eight equivalent OSr4Cu2 octahedra, corners with five OSr3Cu2 square pyramids, edges with two equivalent OSr4Cu2 octahedra, and faces with four equivalent OSr4Cu2 octahedra. The corner-sharing octahedral tilt angles are 58°. In the third O site, O is bonded to three Sr and two equivalent Cu atoms to form distorted OSr3Cu2 square pyramids that share corners with eight equivalent OSr4Cu2 octahedra, corners with five OSr3Cu2 square pyramids, edges with two equivalent OSr4Cu2 octahedra, and faces with four equivalent OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 58–59°. In the fourth O site, O is bonded to four Sr and two Cu atoms to form distorted OSr4Cu2 octahedra that share corners with eleven OSr4Cu2 octahedra, corners with four equivalent OSr3Cu2 square pyramids, edges with three OSr4Cu2 octahedra, faces with five OSr4Cu2 octahedra, and faces with two equivalent OSr3Cu2 square pyramids. The corner-sharing octahedra tilt angles range from 0–63°. In the fifth O site, O is bonded in a distorted L-shaped geometry to four equivalent Sr and two Cu atoms. In the sixth O site, O is bonded to four Sr and two Cu atoms to form distorted OSr4Cu2 octahedra that share corners with eleven OSr4Cu2 octahedra, corners with four equivalent OSr3Cu2 square pyramids, edges with three OSr4Cu2 octahedra, faces with five OSr4Cu2 octahedra, and faces with two equivalent OSr3Cu2 square pyramids. The corner-sharing octahedra tilt angles range from 0–63°.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-15. Materials Data on SrCuO3 by Materials Project. https://doi.org/10.17188/1203126

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↗