Search NASA⌕ Search

DOE OSTI · 1688164

Materials Data on Sr12Ti4Si16O61 by Materials Project

Abstract

Sr12Ti4Si16O61 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are nine inequivalent Sr sites. In the first Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.50–2.90 Å. In the second Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.50–2.90 Å. In the third Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.50–2.88 Å. In the fourth Sr site, Sr is bonded to eight O atoms to form distorted SrO8 hexagonal bipyramids that share corners with four SiO4 tetrahedra and edges with two equivalent SiO4 tetrahedra. There are a spread of Sr–O bond distances ranging from 2.47–2.78 Å. In the fifth Sr site, Sr is bonded to seven O atoms to form distorted SrO7 pentagonal bipyramids that share corners with four SiO4 tetrahedra and edges with two equivalent SiO4 tetrahedra. There are a spread of Sr–O bond distances ranging from 2.46–2.77 Å. In the sixth Sr site, Sr is bonded to seven O atoms to form distorted SrO7 pentagonal bipyramids that share corners with four SiO4 tetrahedra and edges with two SiO4 tetrahedra. There are a spread of Sr–O bond distances ranging from 2.42–2.82 Å. In the seventh Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.63–2.80 Å. In the eighth Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.63–2.82 Å. In the ninth Sr site, Sr is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Sr–O bond distances ranging from 2.61–2.80 Å. There are two inequivalent Ti sites. In the first Ti site, Ti is bonded to six O atoms to form TiO6 octahedra that share corners with two TiO6 octahedra and corners with four SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 14°. There are a spread of Ti–O bond distances ranging from 1.94–2.04 Å. In the second Ti site, Ti is bonded to six O atoms to form TiO6 octahedra that share corners with two TiO6 octahedra and corners with four SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 13–14°. There are a spread of Ti–O bond distances ranging from 1.94–2.05 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SrO7 pentagonal bipyramids, and corners with two SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 47°. There are a spread of Si–O bond distances ranging from 1.60–1.67 Å. In the second Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one SrO8 hexagonal bipyramid, a cornercorner with one TiO6 octahedra, a cornercorner with one SrO7 pentagonal bipyramid, and corners with two SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. In the third Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one SrO8 hexagonal bipyramid, a cornercorner with one TiO6 octahedra, a cornercorner with one SrO7 pentagonal bipyramid, and corners with two SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Si–O bond distances ranging from 1.61–1.66 Å. In the fourth Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SrO7 pentagonal bipyramids, and corners with two SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Si–O bond distances ranging from 1.62–1.66 Å. In the fifth Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SiO4 tetrahedra, and an edgeedge with one SrO7 pentagonal bipyramid. The corner-sharing octahedral tilt angles are 50°. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. In the sixth Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SiO4 tetrahedra, and an edgeedge with one SrO8 hexagonal bipyramid. The corner-sharing octahedral tilt angles are 50°. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. In the seventh Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SiO4 tetrahedra, and an edgeedge with one SrO7 pentagonal bipyramid. The corner-sharing octahedral tilt angles are 49°. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. In the eighth Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two SiO4 tetrahedra, and an edgeedge with one SrO7 pentagonal bipyramid. The corner-sharing octahedral tilt angles are 51°. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. There are thirty-six inequivalent O sites. In the first O site, O is bonded in a distorted T-shaped geometry to one Sr and two equivalent Ti atoms. In the second O site, O is bonded in a distorted T-shaped geometry to one Sr and two equivalent Ti atoms. In the third O site, O is bonded in a distorted T-shaped geometry to one Sr and two Ti atoms. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to one Sr and two equivalent Si atoms. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to one Sr and two equivalent Si atoms. In the sixth O site, O is bonded in a distorted bent 150 degrees geometry to one Sr and two Si atoms. In the seventh O site, O is bonded in a 2-coordinate geometry to one Sr, one Ti, and one Si atom. In the eighth O site, O is bonded in a 2-coordinate geometry to one Sr, one Ti, and one Si atom. In the ninth O site, O is bonded in a 2-coordinate geometry to one Sr, one Ti, and one Si atom. In the tenth O site, O is bonded in a 2-coordinate geometry to one Sr, one Ti, and one Si atom. In the eleventh O site, O is bonded in a distorted bent 150 degrees geometry to two Sr atoms. In the twelfth O site, O is bonded in a distorted bent 150 degrees geometry to two Sr atoms. In the thirteenth O site, O is bonded in a distorted bent 150 degrees geometry to two Sr atoms. In the fourteenth O site, O is bonded in a 1-coordinate geometry to two Sr and one Si atom. In the fifteenth O site, O is bonded in a 3-coordinate geometry to two Sr and one Si atom. In the sixteenth O site, O is bonded in a distorted single-bond geometry to two Sr and one Si atom. In the seventeenth O site, O is bonded in a 1-coordinate geometry to two Sr and one Si atom. In the eighteenth O site, O is bonded in a distorted bent 150 degrees geometry to one Sr and two Si atoms. In the nineteenth O site, O is bonded in a distorted bent 150 degrees geometry to one Sr and two equivalent Si atoms. In the twentieth O site, O is bonded in a distorted linear geometry to one Sr and two equivalent Si atoms. In the twenty-first O site, O is bonded in an L-shaped geometry to two Sr atoms. In the twenty-second O site, O is bonded in an L-shaped geometry to two Sr atoms. In the twenty-third O site, O is bonded in an L-shaped geometry to two Sr atoms. In the twenty-fourth O site, O is bonded in a 1-coordinate geometry to three Sr and one Si atom. In the twenty-fifth O site, O is bonded in a 1-coordinate geometry to three Sr and one Si atom. In the twenty-sixth O site, O is bonded in a 1-coordinate geometry to three Sr and one Si atom. In the twenty-seventh O site, O is bonded in a 4-coordinate geometry to three Sr and one Si atom. In the twenty-eighth O site, O is bonded in a distorted bent 120 degrees geometry to one Sr and two Si atoms. In the twenty-ninth O site, O is bonded in a distorted bent 120 degrees geometry to one Sr and two Si atoms. In the thirtieth O site, O is bonded in a distorted bent 120 degrees geometry to one Sr and two Si atoms. In the thirty-first O site, O is bonded in a distorted bent 120 degrees geometry to one Sr and two Si atoms. In the thirty-second O site, O is bonded in a 4-coordinate geometry to two Sr, one Ti, and one Si atom. In the thirty-third O site, O is bonded in a 4-coordinate geometry to two Sr, one Ti, and one Si atom. In the thirty-fourth O site, O is bonded in a 4-coordinate geometry to two Sr, one Ti, and one Si atom. In the thirty-fifth O site, O is bonded in a 4-coordinate geometry to two Sr, one Ti, and one Si atom. In the thirty-sixth O site, O is bonded in a single-bond geometry to one Sr atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Sr12Ti4Si16O61 by Materials Project. https://doi.org/10.17188/1688164

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↗