Search NASA⌕ Search

DOE OSTI · 1276827

Materials Data on Sr13Al6Si8O by Materials Project

Abstract

Sr13Al6Si8O crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are seven inequivalent Sr sites. In the first Sr site, Sr is bonded in a 7-coordinate geometry to two equivalent Al and five Si atoms. Both Sr–Al bond lengths are 3.36 Å. There are a spread of Sr–Si bond distances ranging from 3.29–3.39 Å. In the second Sr site, Sr is bonded in a single-bond geometry to four Al, four Si, and one O atom. There are two shorter (3.42 Å) and two longer (3.44 Å) Sr–Al bond lengths. There are two shorter (3.44 Å) and two longer (3.47 Å) Sr–Si bond lengths. The Sr–O bond length is 2.50 Å. In the third Sr site, Sr is bonded to eight Al and four Si atoms to form a mixture of edge and face-sharing SrAl8Si4 cuboctahedra. There are a spread of Sr–Al bond distances ranging from 3.44–3.48 Å. There are two shorter (3.57 Å) and two longer (3.61 Å) Sr–Si bond lengths. In the fourth Sr site, Sr is bonded in a 7-coordinate geometry to two equivalent Al and five Si atoms. Both Sr–Al bond lengths are 3.31 Å. There are a spread of Sr–Si bond distances ranging from 3.25–3.41 Å. In the fifth Sr site, Sr is bonded in a 7-coordinate geometry to two equivalent Al and five Si atoms. Both Sr–Al bond lengths are 3.29 Å. There are a spread of Sr–Si bond distances ranging from 3.29–3.40 Å. In the sixth Sr site, Sr is bonded in a distorted single-bond geometry to five Si and one O atom. There are four shorter (3.41 Å) and one longer (3.75 Å) Sr–Si bond lengths. The Sr–O bond length is 2.89 Å. In the seventh Sr site, Sr is bonded in a linear geometry to four Si and two equivalent O atoms. There are two shorter (3.41 Å) and two longer (3.42 Å) Sr–Si bond lengths. Both Sr–O bond lengths are 2.42 Å. There are three inequivalent Al sites. In the first Al site, Al is bonded in a 2-coordinate geometry to six Sr, one Al, and two Si atoms. The Al–Al bond length is 2.59 Å. There are one shorter (2.49 Å) and one longer (2.51 Å) Al–Si bond lengths. In the second Al site, Al is bonded in a 2-coordinate geometry to six Sr, one Al, and two Si atoms. The Al–Al bond length is 2.59 Å. There are one shorter (2.50 Å) and one longer (2.53 Å) Al–Si bond lengths. In the third Al site, Al is bonded in a distorted bent 120 degrees geometry to six Sr, one Al, and two Si atoms. There are one shorter (2.48 Å) and one longer (2.51 Å) Al–Si bond lengths. There are four inequivalent Si sites. In the first Si site, Si is bonded in a 2-coordinate geometry to seven Sr and two Al atoms. In the second Si site, Si is bonded in a 2-coordinate geometry to seven Sr and two Al atoms. In the third Si site, Si is bonded in a 9-coordinate geometry to eight Sr and one Al atom. In the fourth Si site, Si is bonded in a 9-coordinate geometry to eight Sr and one Al atom. O is bonded to six Sr atoms to form corner-sharing OSr6 octahedra. The corner-sharing octahedral tilt angles are 0°.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-22. Materials Data on Sr13Al6Si8O by Materials Project. https://doi.org/10.17188/1276827

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↗